EP1694942A4

EP1694942A4 - Retrorotating, post-rotating and birotating prime movers (second part: general conclusion)

Info

Publication number: EP1694942A4
Application number: EP04821233A
Authority: EP
Inventors: Normand Beaudoin
Original assignee: Individual
Current assignee: Individual
Priority date: 2003-09-24
Filing date: 2004-09-03
Publication date: 2006-12-20
Also published as: WO2005073512A1; CA2481427A1; CN1922387A; JP2007506902A; EP1694942A1; AU2004314945A1

Abstract

The present invention aims at completing the work concerning prime movers by generalizing some support methods, such as poly-induction machines, through hoop gearing, as well as by generalizing the criteria for manufacturing prime movers, essentially showing that the degrees of mechanical rotativity thereof can be achieved horizontally, thereby ensuring the manufacture of so-called rotary-circular prime movers, with differential dynamics or on the contrary, said prime movers enabling the chromatic ranges of prime movers to be completed and the levels of dynamism to be differentiated; and the degrees of material, virtual and real embodiments. It will be demonstrated moreover that the mechanical generalizations correspond to the dynamic generalizations of figures.

Description

RETROROTATIVE, POST ROTATING AND TWO-ROTATING DRIVING MACHINES (second part: conclusive generalization)

Disclosure

Fields of the present invention

The present invention can be considered as the second part of our work relating to the driving machines, work of which we will find the first part summarized in our patent application filed internationally under the title retro rotary, post rotary and birotative driving machines.

Furthermore, this patent application summarizes all of the patent applications filed in advance thereof. In contrast to the figurative plane, developed in the first part, in which we have shown a certain number of criteria making it possible to describe the degrees of the figures and the mechanics of the machines, the present invention will determine the main ones making it possible to determine, from a cutting precise made possible by certain units of the first part, the various degrees this time dynamico-mechanical of the machines, and by a new set of the possible machines on this plan, in particular the rotary and circular rotary differential machines, and the rotary machines on the contrary.

In addition, it will be shown that the degrees of the machines can simultaneously belong to the two planes. Finally, we will show that machines also have degrees of figurative reality, namely the material, virtual, and Real degrees.

In summary, therefore, the present invention therefore aims to complete our first work and show that we can restore to rotary machines, geometrically and dynamically, degrees of achievement ensuring them not only a motor capacity, but also a versatility of realization and distinction of types of machines appreciable. This versatility will find its theoretical form in a vast set of conceptual criteria allowing to determine any machine.

This new set of machines, much larger, and meeting a much broader set of precise and sophisticated criteria, will therefore allow a new synthesis, much broader and encompassing, which will be expressed in the various chromatic ranges of motor machines. This new set of machines will also be important since it will make rotary-circular machines with blade or cylinder dynamics in Clokwise appear not only as the primary cutting point for the various types of machine dynamics forming the chromatic range, but also, from the point from a practical point of view by its fundamental original realization of rotary machines, in that this is the only machine in which we find, as in turbines, no acceleration deceleration of any of the parts, and as in piston engines, equal and complete thrust on the compressive parts. From the point of view of the marketing capacity of the present invention, while the machines of mechanical and dynamic configuration of the prior art have remained faced with significant problems, and have fallen into commercial abandonment, we believe that some of the machines rotary-circular on the contrary, the first version of which was provided in our previous works, we really seem to be a type of machine which, by their qualities, allows us to envisage a renewed commercial capacity for rotary machines.

More specific content and objects of the present invention

The first part of the present invention will consist in generalizing certain parts or methods of supporting the first part. In particular, the concepts of poly induction, hoop gears and polycamation will be extended.

The purpose of the second part of the present invention will be to generalize the basic rotational circular figure, with clokwise blade movement, presented in the first part of the present invention. In particular, we will show that this realization is mechanically original, since it is the perfectly birotative dynamic realization. We will indeed show that birotativity, which we had figuratively highlighted in our first part, is also presented there dynamically, in the form of the circular rotary machine with clokwise movement. We will explain here the immense advantages of this type of machine and we will generalize the horizontal support methods allowing to ensure a correct support of the compressive parts.

We will show, moreover, that the Rotativo-circular motor machines, generally produced by coordination of the compressive part of circular movement and clokwise movement are important not only from the point of view of their original specific qualities, but also theoretically, since they make it possible to determine with precision a birotative cutting point, this point subsequently allowing the completion of a complete system of engine dynamics, which will be represented by the chromatic scales. "

In other words, we will show that the mechanical degrees, which we defined in the first part, and which made it possible to figuratively produce machines of different degrees, by curvatures of different and more sophisticated cylinders, will also allow, when they are carried out horizontally by the use of semi transm tive inductions, to dynamically differentiate the degrees of the machines, according to whether they are in clokwise dynamics, in retro-rotary differential dynamics, or post rotary, or according to whether they are in dynamic contrario.

In summary, it will therefore be shown that all the advancements relating to the degrees and the birotativity of the machines that we have made on the vertical plane in the first part of this work, will be able, starting from the unit of rotary-circular machine by Clokwise blade in movement also shown in this part, that we can generalize this dynamic and develop the complete plan of the machines, this time from the dynamic and horizontal point of view. We will complete this work by also showing that these two plans can be produced in the same machine.

All of these dynamics will make it possible to constitute a complete system of the driving machines, including the chromatic ranges, and a completed criteriology allowing us to define any machine.

More precisely a) we will show the rules allowing to regroup under a same design the mechanical multiples of these machines b) we will show the differentiation between material figures, virtual figures and real figures of machines, which will allow to show different machines with opposite movement, including those with Slinky movement c) we will generalize rotary-circular machines to all machines, such as for example polyturbines or Quasiturbines d) we will show that the notions of degrees not only figurative but also dynamic surplus can be applied machines in general and poly turbines e) we will show that we can realize chromatic ranges of general machines, and that these apply in post, retro or fixed cylinder, or planetary cylinder in movement Clokwise f) we will show that circular rotary machines are also general from the point of view of their pa the, namely that they can be produced by sets of single-cylinder blades, standard poly-faced blade, palic structure. g) we will suggest more adequate types of segmentation h) we will suggest supports by crankpins and their means of realization

I) we will show that the circular rotary machines can not only be carried out by any induction, but also that they can be raised in degrees by all the methods of elevation already listed for the machines with fixed cylinder, notions of figurative and figurative degrees , like for example polycamed gears, degrees of induction.

Work plan of the present invention

To achieve these objectives, the following disclosure steps are therefore carried out

1) Summarize the prior art, before Wankle and at Wankle, 2) Show the main practical shortcomings of Wankle, and the mechanical difficulties which result from it. 3) Show how our different contributions greatly improve the thrust, even in first degree rotary machines 4) Show the clokwise dynamics 5) Summarize a general system of machine understanding, eliminating Wankle's difficulties 6) Extend to their limit the notions of mono induction and poly induction 7) Suggest adequate segmentation of the machines 8) Suggest support for compressive parts by crankpins. 9) Show Wankle's semantic gaps

All of these achievements, linked to those already produced by ourselves, will show all the mechanical and theoretical shortcomings of Wankle and how a more total, more extensive, more inclusive and final system can respond.

The stages of realization of this second part of our work will be the following a) we will summarize the data relating to the prior art relating to mainly rotary motor machines, with compressive part with blade or piston b) we will summarize l Wankle's contribution to the matter. c) We will state the various basic difficulties of the Wankle system (It should be noted that we will show, subsequently several errors of design and meaning thereof) d) We will carry out a brief recapitulation of the first part of the present invention, and in particular, we will show how we have, in this one overcome the difficulties thereof, which will have made it possible to carry out the characterization of degrees, of these, as well as of the compressive, neutral, motor aspect "e) We will generalize some of these achievements, for example the achievements by hoop gear, the realization by poly induction f) We will show that one of our previous achievements, either that by dynamic in clokwise movement of blade, is not a simple achievement among others, but a strategically important achievement, since not only it implements an original degree of dynamization of these machines, but also park e qu, it will make it possible to complete the dynamic chromatic range of these machines, and to carry out new characterizations, such as the contrario machines, and the virtual figuration and real figuration machines. It will also be shown that these types of machine are fundamentally original from the point of view of their quality, in particular by their thrust also distributed over the entire surface of the pistons, and by their total absence of acceleration and deceleration of all their driving parts. and compressive. g) Realizing a point missing from the previous systems making it possible to create the chromatic scales of the machines, differentiated into dynamic differential post or retro rotary machines, and into machines with Clokwise or contrario movement. h) We will show below the generalizing quality of machines with dynamic dynamics called circular rotativo, in that they can not only apply to any machine, whether it is retro-rotary, post rotary, or birotative, but also in all dynamics, first, second third degree or other. i) It will then be shown that all these machines can also be made by combinations of simple blades, by standard multifaceted blades, or by palic structures j) It will be shown that machines can also achieve higher degrees dynamically or figuratively, in particular by the methods of correction of the figure already commented on, such as for example by polycamed gears. k) We will determine the general principles of association of the support methods of these machines, the notions of self-induced induction, rising induction, descending induction.

1) We will finally show that starting from these new skills, we can differentiate the virtual and real material levels of the machines, and thus make Slinky motion machines m) We will show that all the mechanical skills already achieved by ourselves can be applied to circular rotary machines, which guarantees the specifically generative character of these machines. To do this, we will define the semi-transmissions already commented on by ourselves as inductions transferred onto themselves n) We will list all the characterizations allowing to specify the nature of a given machine includes and exceeds by far the simple determinations of the prior art, and allows maximum versatility of machines and an exhaustive understanding of each. To this end, we will show the semantic errors of several machines of the prior art. o) It will be shown that all of these characterizations form a synthetic unit by which a number of machines, which cannot be understood by the simple classifications of the prior art, can now enter it correctly p) We will show that the corrective methods, by slides, staggerings, polycamed gears, can also be applied to circular rotary machines, by poly crankpins q) It will be shown that circular rotary machines can also be realized by rotary blades and circular rotary cylinder, creating thus the chromatic counter ranges r) We will show various types of simplified segmentation for these machines s) We will show the possibilities of suspension by crankpins

Summary of the prior art before and at Wankle

The art before and after Wankle excluding our works

We can summarize the period prior to Wankle of work relating to motor machines, mainly rotary as the period in which we gradually discovered a set of figuration of blades and cylinders, allowing the planetary movement of these blades in their cylinder respectively.

The basic figures were discovered by a group of inventors including Fixen, Coole, Maillard and several others. (Fig.l a)

We can say, excluding our own work that the prior art in general relating to particularly rotary motor machines, seems to have experienced its greatest expansion before Wankle and at Wankle. Developments subsequent to those of Wankle are very fragmented, and even today, in the industry, the method of support by mono induction, invented by Wankle, is used. This is mainly due to the great opacity of the Wankellian theory, which leaves little room for restructuring. But, as we have already shown and will finish showing here, a fairly large number of machine characteristics, and the serialization, semantic cutting of these, allows the development of a large number of new machines, of a broader and more general theory, and above all, new types of machines totally excluding the whole of the defects of machines prior to Wankle, and of Wankle machine.

Wankle's contributions

As we have already mentioned in our previous work, Wankle's contributions can be classified into three main categories: 1) that of historical indexing, 2) that of mechanization, and finally 3) segmentation on a blade, and a series of these new figures

At the limit, one could add the variant contribution. But this last bet contains errors in dynamic semantics and is deprived of mechanical support methods, which prevents knowing its maturity and actual composition.

The contribution of Wankle's historical indexing The consultation of Wankle's main patent, titled Eintellung der rotationskolbermachinen. Rotations kolbenmachinen mit parrallelen drehaschsen unt arbeitshramumwandungenaus starrem werstoff with number xb02204164 allows to take cognizance of the faithful exposure, by Wankle of the state of the motorology of machines of its time and prior art.

In truth, many of these machines, and even the vast majority, remain non-mechanized, however, and non-mechanizable by strictly using the two induction methods proposed by the inventor. This is why we will only consider here machines that can be mechanized, that is to say machines whose driving parts can be mechanically supported.

Rationalization of figures at Wankle

Wankle's most important theoretical contribution is certainly to have organized the initial figurations of the prior art in such a way that the segmentations in these new machines can no longer be carried out on the corners of the cylinders, but rather on the points blades. Subsequently, Wankle, like Fixen and Cooley, produced the series of these machines, retro and rotary. These logical series similar to the figures of machines of the prior art, we allowed to group the machines into two categories, which we later called retro-rotary, and post rotary, according to whether their blade, observed by an outside observer, moves in the same direction as its eccentric, or in the opposite direction to it. (Fig. 1 b)

The second part of Wankle's rationalization consists of specific series of each of these categories, put in series to rationalize the ratio of number of sides of the blades and cylinders of each of these categories. Wankle therefore enacts the rule that the rotary machines have a blade side number of one less than that of their respective cylinder, while the post rotary machines have a blade side of one greater than that of their respective cylinder. (Fig. 1 b)

Mechanization

The theoretical contributions of Wankle would certainly not be known to the general public today if it had not been for its mechanical contributions, which had the result of allowing autonomous support of the blades relative to their respective cylinders and consequently of removing friction undue blades on the cylinder, causing premature wear of the segments.

These types of mechanical support are limited to two at Wankle. These are supports by mono induction, and by intermediate gear. (Fig. 1 c) Support by mono induction is the type of support generally used in industry. variants

The only dynamic variant for which Wankle provides support methods is the rational double action variant. This variant is still used today in the production of pumps. Wankle provides two support methods for this one. (Fig. 1 d)

Mechanization by mono induction and triangular blade

It should be noted from the start that the crankshaft of rotary, and mainly retro-rotary, machines must be made of very small dimension to allow the achievement of an acceptable compression ratio. Similarly, the greater the number of faces of the blades and cylinders of the machines, the smaller their eccentric. It is for these reasons that the industry has concentrated almost exclusively on post rotary machines with triangular blades.

As for the mechanizations proposed by Wankle, in mechanization by intermediate gear, it turns out to be more difficult to carry out the segmentation, and to carry out with full assurance the exact positioning of the blade. The industry has therefore restrictively recognized the mono induction method as a reliable method of support allowing commercial production of this type of machine.

Period subsequent to the Wankle period excluding our work The opacity and rigor of the Wankle system made subsequent conceptual developments difficult. The rational organization of the driving machines includes only very few rationalization criteria, characteristic distinguishing criteria of the machines, which will have made the design not only narrow, theoretically but also, insufficient and erroneous in several places, notably those from the analysis perspective, and those relating to the compressor and motor characteristics of the machines. The excess purification of the components by Wankle made lose a large part of the rotary capacities of the machines. Among the works subsequent to those of Wankle, whose contribution relating to motive machines is significant, we should note those of Wilson and St Hilaire. The first shows that we can make a motor machine whose blade will be a flexible set of blades, which we have called a palic structure. The second uses this palic structure as a support structure for a set of upper blades. Each of these inventors was only able to suggest adequate support structures for these machines.

We have abundantly shown that these machines constitute machines of the second degree, and of the third degree, and that they can, like the machines of the first degree, be put in series. We also mounted that the same mechanics as the first degree machines, but this time put in combination allowed to support the compressive parts.

Very concise summary of the preliminary course and this work

At first, like many researchers, we found that rotary machines, especially when they had their compressive parts supported by methods conventional ones producing a lot of friction, which is the direct consequence of contradictory thrusts on the blade. We therefore first proposed several new support methods to overcome these difficulties, such as, in particular, the poly induction, hoop gear, active central induction, semi transmission and so on. (Fig. 2) We subsequently realized that the mechanical deconstruction carried out during the expansion was more interesting in retro rotary machines than in post rotary machines. In order to take advantage of this important advantage, we have worked extensively to correct the weak point of these machines, trying to show methods capable of increasing the compression of retro-rotary machines. To achieve this, we were led to understand that it was necessary to correct the stroke of the blade, and the curvature of the cylinder, so that it sinks less deeply into the tips of the cylinders and more deeply into in the sides. As this work progressed, we became interested in machines with palic structures, the first compressive structure of which was produced by Wilson. We found there that the curvature of the cylinder of this one was specific in that it comprised at the same time n retro rotary aspect, and a post rotary aspect what was corroborated by the various methods of mechanical support which we produced for bear in parts. We concluded, moreover, that certain machines by their nature had a higher degree of rotativity proven by a higher number of rotary structures. It has therefore been shown that the mechanics of these machines could then be applied to retro rotary or post rotary machines, which gave them a higher mechanical degree, a more subtle cylinder representation, and finally, a partially rotary character. These methods have therefore made it possible to increase not only the compression of the retro-rotational machines, but also to increase the torque of the post-rotary machines. The main methods of realizing birotativity were therefore that of adding geometry rod, polycamed gears, stepping, poly induction. (Fig.3)

The reasons for the results obtained, both in the rotary and post rotary machines consisted in the fact that these machines were restored to their bi rotativity, the number of degrees of mechanization allowing the correct motricity of these.

The difficulty of carrying out the mechanical layering subsequently led us to propose other original solutions for carrying out dual induction. Poly induction made it possible to carry out horizontally the cutting that we had produced there. We have therefore also gone further by showing that birotativity could also be achieved horizontally and dynamically, by making machines with blades in clokwise movement, which must be considered, as we will show, as the most theoretically important; circular rotary machines (Fig. 4)

Very concise summary of the present invention.

In the present invention, first of all, a first part will be devoted to a generalization of certain methods of our previous previous work. We will show in particular the concepts of poly induction in descending inking, or alternative poly induction. We will broaden the concepts of polycamed gears, and method of support by hoop gear. In the second time, we will specify our thought relative to the basic rotary-circular machines, and will specify the bi inductive nature with clokwise movement of blade. We will show the great mechanical relevance of these machines.

Subsequently, in a third step, we generalize the support methods for these types of machines, by showing in particular that there is always the participation of at least two mechanics, by rising induction, by falling induction, or by semi transmission, and that the parts are linked by the blade, by the crankshaft, or by the support gear.

Thirdly, we will generalize circular rotary machines to their limit. We will show in fact that, starting from the clokwise dynamic, we can realize, this time on a horizontal plane, all the degrees of the machines, together that we had figuratively and vertically in the first part of our work. We will more precisely realize this: 1) by showing that the number of degrees in these, is expressed dynamically, by post rotary differential action, retro rotation, or by action in contrario 2) that the types of corrective methods, for example by polycamerous gears, by increasing degrees of rotativity can also be applied to them 3) that the various types of blades, simple, standard polyfaciated, by palic structure can be applied 4) that the horizontal plane on which they are made can be combined with vertical plane of the previous machines 5) that any rotary-circular machine is both the expression of a material figuration of pale cylinder ratio, of a virtual figuration expressing the movement of the blade, and of a Real figuration, expressing the correct location of machine times 6) That rotary-circular machines can also be produced with a differential dimension or a d imension a contrario 7) That machines with clokwise movement can be produced virtually, in reverse mirror, either by clokwise cylinder and rotational blade, 8) That machines with clokwise movement can also be produced in bifunctionality.

All of these new generalizations will complete our work and will make it possible to achieve a general theory of criteria for determining any driving machine.

More precise summary of our previous work and the subject of the present invention of our previous work

Our previous work therefore achieved the following aspects:

A) we have added several first level mechanics to the two Wankle mechanics, which will have made it possible to determine a vast mechanical assembly comprising the following support methods, (Fig. 2): - by mono induction (Wankle) - by intermediate gears (Wankle) - by poly induction (Beaudoin) - Method by semi transmission (Beaudoin) - Method by hoop gear (Beaudoin) - Method by intermediate gear (Beaudoin) - Method by heel gear (Beaudoin) - Method by juxtaposed internal gears (Beaudoin) - Method by superimposed internal gears (Beaudoin) - Method by post active central gears (Beaudoin) - Method by gear structure (Beaudoin) - Method by unitary gears (Beaudoin)

We have subsequently produced all of the following advancements (Fig. 3) a) We have shown that we could increase the compression of retro-rotary machines, the torque of post-rotary machines b) We have therefore shown that could realize rotary machines of various degrees, these machines realizing new forms of more subtle cylinder and being supported increasing the number of induction c) we showed that one could produce accelero-decelerative actions of the compressive parts, increasing by there their oscillatory effect, and thus improving the race of the compressive parts and the shape of the cylinders being relative to it d) we showed the rules of combination of the mechanics in staging e) we generalized the shapes of cylinder of the poly turbines f) we have showed the methods of modifying the degrees and cylinders of machines g) we showed the dynamic degrees of rotor cylinder machines at piston h) we have shown the effects of poly crankpin on rotary machines i) we have shown the different types of cylinders obtained Square, ovalized etc. j) we showed that the machines could be built by sets of unitary blades, standard polyfaces blades, palic structures k) showed us the perfectly birotative dynamics of pay in movement Clokwise, and the rotativo-circular dynamics that this movement implied.

Retrospective of the art prior to Wankle and of Wankle We can summarize the art prior to Wankle by saying that it is the progressive and non-rationalized expression of the various figures of rotary machines. The main inventors to whom we owe the basic geometric figures of rotary machines are Fixen, Cooley, Maillard and several others. These inventors have shown that blades of various number of sides can be produced so as to produce an inner planetary stroke at one cylinder, when mounted on an eccentric. (Fig. 1 a) Wankle's contributions

Wankle's contributions can be viewed from three particular points of view.

First of all, we owe to Wankle an important historical part, since in his invention, he made a more exhaustive inventory of the driving machines of the prior art.

The second Wankle contribution should rather be classified from the point of view of its theoretical value. Indeed, Wankle establish a classificatory rationalization of these figures, and of segmentation figures on the blades, which allows him on the one hand to divide them into post rotary figures and retro-rotating figures, and on the other hand to fill the said classes missing figures. (Fig. 1 b)

The third contribution of Wankle consists in having to realize two methods of orientational support of the blades of the machines, methods which we have named by mono induction and by intermediate gear. (Fig. 1 c) The main effect of these methods was to make the blade completely independent, mechanically, from the cylinder in which it travels. Consequently, the use of these methods allowed a correct separation of the mechanical and compressive parts of the rotary machines. It is mainly for this reason that one of these methods, the mono induction method, was adopted by the industry, with the result that rotary motors are often also called Wankle motors, named after the inventor of these methods.

First part

In this first part, we more specifically determine the most fundamental shortcomings of the prior art and in particular that of Wankle and we will produce an extension by precision of methods which we previously proposed. .

General shortcomings of the Wankle system

It is a point of consensus to consider rotary machines before Wankle as very little resistant to premature wear of the segments, and Wankle machines as having a high coefficient of friction and a very low torque. "

To truly be able to correct these faults, one must have a full awareness of their causes. It is known that the segments of the machines of the prior art to Wankle, underwent premature wear caused in the fact that the orientational support of the blade is achieved by its anchoring to the cylinder. The segments then undergo significant mechanical pressure for which they were not designed.

We can classify the shortcomings of the Wankle system into three main categories: mechanical, semantic and incomplete. We will only study the semantic and incompleteness gaps at the end of the present invention, and will consider, for the purposes of this section only the mamamic gaps. Wankle mechanical deficiencies

Segmentation

The positive effects of the new Wankle segmentations were to allow segmentation on the blades, and softening of the cylinders, which had the effect of minimizing the wear of the segments. Furthermore, the main negative effect was to produce the explosion, so to speak, on a blade placed horizontally, and not a blade in righting, as was the case in the machines of the prior art. The price to pay for securing the segmentation therefore initially has that of considerably reducing the extent of the extension, reduced in Wankle machines to the sole extension of the crankshaft.

Mechanical

Wankle's mechanical contributions have therefore fulfilled their objectives of securing the orientation of the blade independently of the cylinder, and therefore of achieving complete separation of the mechanical action from the compressive action. In addition, it is obvious that the realization of these methods of orientational support caused other difficulties, almost as important, theoretically mechanically.

Since we intend in the first part of the present application, to extend some of our previous solutions, namely poly induction, induction by hoop gear, and by polycamered gear, and in the second part, generalize the dynamic dynamo-mechanical plane of machines, we will discuss here the Wankle errors, and show that all our solutions are not fragmented, but on the contrary form an original systematic corpus making it possible to fully account for the machines. It will therefore be easier for the reader to take into account the originality, the efficiency, the flexibility of the variability, and the generality of the global synthesis that we propose for this purpose.

The set of Wankle gaps and the set of solutions that we have brought and bring to it are the following a) An achievement, by means of two mechanics, namely mono inductive mechanics and by intermediate gear, of contradictory thrust on the same blade, part of these thrusts being in the opposite direction to the rotation of the machine (solutions: hoop gear inductions, semi transmission, post active central gear) b) A mechanical embodiment lowering the number of components to a number less than that strictly necessary for achieving motor skills (layering solution, poly crankpins) c) Counter-rotating mechanization, resulting from the reverse observation of machine mechanics, from the outside to the inside of the machine system ( solution: constructed observation, and poly induction) d) an exaggeration in the regularity of the rotary movement of the blade polycamed gear) First gap of Wankle: centralization of the anchoring resulting in contradictory thrusts on the blade

The element constituting without question the major difficulty of any rotary machine, when the orienting action of this one is carried out by one of the methods of Wankle, that is to say in the center of the machines, is certainly that of the contradictory thrust of the explosive power on the blade. By contradictory thrust, we mean on the one hand that a part of the blade has an orientation induction not only contrary to the other part of the same blade, but also contrary to the system of the machine. This is exactly what happens in Wankle’s two main induction mechanics, mono induction, and intermediate gear induction, and this is most certainly the main reason for the lack of motricity of these machines when made in these ways. (Fig. 5 b)

To better understand the cause of this shortcoming, we can use more easily understandable examples by comparing several piston engines, of different types. One can indeed compare standard piston engines with piston motors with a sliding rod, and with poly induction piston engines. (Fig. 5 c)

It can be seen in this figure that the power of the piston on the crankshaft, during descent, is given in the standard piston engine by the vertical thrust thereon, and b by the lateral support thereof and of the connecting rod transforming into lateral thrust.

The two combined effects, thrust and rod effect combine to achieve the circular movement of the crankshaft. The thrust on the surface of the piston is fully used. Indeed, whether it is anterior or posterior to its support point, it transforms into a lateral and vertical thrust directed in one direction.

In the sliding rod engine, the lateral action of the thrust is lost, and the rod effect is subtracted. The machine therefore only has its vertical effect.

In the poly induction motor with a straight rod, from our patent titled Poly induction energy machine, the power is increased this time by the strictly vertical action of the thrust, added to that of the lever of the superimposed crankshafts.

In rotary engines of the prior art to Wankle, it was possible to achieve a thrust, even uneven over the entire surface of the blade and therefore an appreciable thrust effect on the crankshaft (fig. 5 a)

The crankshaft and the blade participate in carrying out their compressive action in mechanical action, the end of the blade achieving a certain inking in the cylinder and allowing a lever action of the blade on the crankshaft. Unfortunately, such a procedure makes the commercial production of these machines difficult, since mechanical parts produced in the same way with compressive parts necessarily result in premature wear of the latter. He therefore fell in an absolute way to realize support methods that are not only positional, that is to say from the center of the blade, friends also, orientation of the latter, in such a way as to make its action completely independent. of the cylinder and thus allow the realization of a strictly floating segmentation.

Wankle's methods: induction by mono induction and intermediate gear

As we have just shown, it can be said that the orientation anchoring in rotary machines is the equivalent of the effect of the connecting rod in piston machines.

It can therefore be said that the displacement of the anchor from the outside towards the center of these machines produces a similar effect if not worse than that of the removal of the rod effect by making the sliding transmission previously shown in the piston engine.

Indeed, by inking the orientational aspect of the blade in the center of the machine, one divides, necessarily, this so-called blade in two parts which will carry out the explosion push in a contradictory way, in opposite direction.

The thrusts on each of the parts of the blade will therefore be opposite, and this will result in a reduced thrust on the crankshaft, since the thrust on the latter will only be the difference of the contradictory thrusts. In the case of mono induction machines, which is the first Wankle support method, the rear of the blade will undergo a negative thrust while the front will undergo a positive thrust. On the contrary, in the case of the application of the intermediate gear method, it is the front part of the blade which will carry out a negative thrust, and the rear part which will carry out a positive thrust. (Fig. 5 b 1, 5 b 2)

The explanations relating to these mechanics can be found in more detail in the present application for earlier patents.

Details of solutions already provided

We will take care to read our previous work relating to power machines, to take care of the various methods of support and correction of the races of the blades of machines, and to better understand the concepts of degrees of these. For the purposes of this document, we will only recall those that we intend to expand. We will therefore generalize more

A) hoop gear inductions, performing them with chains or belts B) polycamed gear methods, this time performing them circularly, with alternately spaced and closely spaced teeth C) semi-transmissions with vertical compression and electrified structure D) poly induction methods 1) at their induction 2) at the support locations 3) at their alternation As we have already mentioned, we have already shown several solutions to these problems. We will limit here however our presentation to the solutions which will receive in the present invention and generalization.

We have demonstrated several solutions to these difficulties could be achieved without changing the level of the machine, that is to say, keeping the machine at its first degree level. These solutions all have in common the objective of realizing this time mechanically the externalization of the anchoring of these machines. These solutions already commented on in our previous work are mainly, the mechanical ones by the solutions by hoop gear, by polycamation, by i tra mission, the mechanical ones by poly crankpins

To this end, we can reread our previous work, as well as the considerations on the thrust that these solutions bring, and which we show in our patent application in antecedence titled Retro-rotating, post rotary, and birotating machine (conclusion)

These mechanics for the purposes of the present application must be completed in the following way: A) the hoop gear mechanics must also include their production with chain, belt (FIG. 6). B) The camshaft gear components must also include the round gears in which the accelerations and decelerations already commented on are carried out by bringing the teeth closer or further away. (Fig. 7) C) Mechanics by semi transmission apply to all machine dynamics, whether the driving parts are the cylinder or the blades, whether these machines are post rotary or retro-rotary, or that these retro-rotary machines are side explosion on the blade, or vertical explosion. (Fig.8)

Hoop gear mechanics

The mechanical hoop gears are produced when the support and induction gears of the external type are coupled together by a gear that is rotatably and planetarily mounted together. We then successfully activated the blade, this time mounted on a crankpin, by its top. Which gives it a great fluidity of induction. We have already shown that, in hoop gear mechanics, one could increase the chord effect of the hoop gear, and the angulation of the thrust by performing these mechanics with a third gear. Furthermore, in our bicycle pedals we have shown that this mechanism could also be applied by making the hoop gear in the form of a chain. The present simply has the effect of stating, for motive machines, that the mechanical ones, called by hoop gears, the hoop gear can materially be produced by a belt, or even by a chain (Fig. 6) As before, in these embodiments, the rope effect prevents the realization of the contradictory forward thrust effect on the blade. The forward thrust is therefore rotatable in the direction of machine, and adds to the back push, which is also positive. The chain can also be produced in the form of a belt.

Indeed, as in the realizations with three gears, the mechanical hoop gears, when carried out with chain or belt, will achieve an additional chord effect, this effect canceling the contradictory thrust before and consequently allowing a thrust, although uneven, positive on the entire surface of the blade.

The thrust on the blade will therefore no longer be contradictory and since all the thrusts on the blade are offensive and, moreover, respects the uneven nature of the opening of the blade during expansion.

Accelero-decelerative mechanics and polycamation techniques.

We have shown in our previous work that the realization of decelerative accelerating parts in the motor machines could allow the realization of previously impossible machines, and allowed machines of higher degree of motricity. These machines were made from gears which we have said polycamed gears. In particular, these machines, when produced by such gears, in addition to admitting a thrust acceleration compatible with the thermodynamics of the explosion, allowed a variation of the anchoring points reducing the negative counter-thrust on the blade. We can hereby extend the notion of polycammed gears by stating that standard gears or polycammed gears can be produced in such a way as to produce acceleration deceleration by producing distanciations of variable teeth. A gear, the teeth of which will not be equally arranged, and which consequently will be in places closer together and by others more distant, will produce, even if they are circular, accelerations and decelerations similar to those of gears polycamés. (Fig.7)

In addition, two gears designed in this way can achieve alternative or similar accelerations and decelerations with each other over time.

We will then produce the same accelerating and decelerating effects of the parts which are fixed to them, and, moreover, different cylinder shapes, more curved, or more acute, which we can moreover realize in symmetry.

Generalization of the semi-transmission method

As it appears in our work filed before this, the semi-transmission method applies to any rotary machine, and in the case of retro-rotary machines, to vertical explosion machines (Fig. 8 a) This method will allow a verticalizing action of the thrust on the crankshaft

In addition, it is important to mention here that the semi-transmission method can be carried out in a subdivided manner, by the conjunction of a rising support induction, and a falling rotation axis induction. (Fig.8) Finally, we must mention, as we will specify later, elicited in a semi transmittive way to adequately support the blades in clokwise birotary movement.

Solutions for increasing the number of vertical rotational degrees: stepping inductions and poly induction

It can certainly be summed up by saying that the first Wankle deficiency consists in an excessive reduction in the number of parts of the machine. This lowering makes it possible to realize the machine in its Compressive nature, but not in its Driving nature.

This statement is also understandable with regard to the examples of piston machines already presented. In the piston machine with sliding rod, rod and pistons are made in the same way. There therefore remain only two constituent elements of the machine, the compression part, produced by including therein in a fixed manner the ligating part and the mechanical part. The machine will be powerful in compression, but will be less efficient when used as an engine.

The way to give it its power will be to restore the ligator part, the connecting rod, separate from the piston.

It must be clearly stated that the centering of the inking in the rotary machines is equivalent to the subtraction from the subtraction of the connecting rod itself. When the connecting rod is made in the same way as the piston, the machine is deprived of its connecting rod effect. A similar loss is realized when the inking of the machine is brought back to the center of it.

We affirm that, for internal combustion machines, the following three elements must be realized for any machine either in its Engine form - a compressive part, - a mechanical part -. a ligating part

must be carried out jointly and cooperatively to produce the machines in their neutral or motor form.

We believe that power machines, whether piston or rotary, can be made in two main ways, either in their compressive, motor, or neutral form. They are produced in their neutral form when they are deprived of their connecting rod effect and are produced with combined parts. They are neutral and motive when their connecting rod effect is restored, and moreover when a lever effect is added to it, as in engines with rectilinear connecting rods.

We have shown and will show here again that one of the major errors in the realization of any machine of the prior art is to have made the rotary machines as first degree machines, that is to say as being machines with only one degree of peripheral rotativity. All the machines have therefore been produced in their Compressive nature, not Motor.

Mechanical staging as a step elevation solution

During our previous work, we have shown that the mechanical staggering, which firstly aimed to make retro-rotary machines with an acceptable compression ratio, was actually of much more general value since one could realize any motor using this method. More specifically for machines of the post rotary type, it made it possible to produce an extremely more powerful torque considerably improving the angles of attack of the blade on its crankshafts. As for the machines of the bi-rotary type, since the mechanical degree allowed the support of the blades was already of second degree, these mechanical by staging allowed a correct support of the compressive parts, which the prior art had not been in able to realize nature These machines of the second degree were therefore more powerful and their nature was of the Motor type, while the machines of the first degree, produced with a single stage, remained machines of the Compressive type, the ones with two stages became of the type neutral or driving.

In the layered embodiments, the driving parts of the machines are not confused. Indeed, the achievements by staging have restored in whole and in a distinct but coordinated manner, the driving parts of the machines, and have therefore produced them in their Motor form.

For more information we will take care to read our previous work on this subject. The brief recall here of these concepts is only intended to prepare the ground for a better understanding of the combinations of mechanics, which in the present will be carried out, for circular rotary machines, horizontally. We are not limited here to a few machines.

The most obvious examples of these achievements are made in triangular retro-rotary motors, with and the post-rotary triangular blade, (Fig. 9)

In these machines, the displacement of the center of the blades, in other words the displacement positions! blades, is no longer simply circular, but is itself planetary. The mechanics of these machines all assume a superior mechanics whose support gear is dynamic and peripheral, since it is fixedly positioned at the height of the crankpin, or else polycamed and disposed in the side of the engine. The upper crankshaft of these machines performs an action similar to the action of the connecting rod of a piston engine. There are more than two hundred possible combinations of mechanics.

Second Wankle gap and second solution for increasing vertical degrees: poly induction

We have abundant work on the concept of poly induction To better understand not only the originality but also the scope of the concept of poly induction, and this, not only from the mechanical point of view but also at the conceptual level it is necessary to make room for an understanding of rotary machines from an observation point of view. As we said before, the shapes of the cylinders of rotary machines as well as their strictly positional support appeared before the development of the various types of orientation of the blades. Therefore, it can be said that in the field of rotary machines, experience and practice have preceded theory. Starting from blades simply supported positionally by an eccentric and arranged in a cylinder, we were able to make two types of observations, observations which subsequently enabled the composition of mechares ensuring, moreover, the autonomous orientation of the blades.

Types of observation

One must necessarily think that to obtain the result of the mechanics by mono induction and by intermediate gear, one had to precede the observation of the blade in two different ways. We will say that the first type of observation is an observation by an absolute point, from outside the machine, (Fig.10 a) and we will say that the second observation is dynamic and internal, since it can be performed from a hypothetical observer positioned on the crankshaft during rotation. (Fig. 10 b)

Observation by general external observation.

In the first type of observation, said by absolute external observation, we assume an observer located outside the machine and observing the movement of the blade and the crankshaft. In post rotary machines, this one will observe that the blade acts in the same direction as that of the crankshaft which supports it, but but more slowly than this one. Conversely, in retro-rotary machines, the latter will note that the blade acts in the opposite direction of rotation than that of the crankshaft which supports it. It is from these observations that the first mechanical Wankle mechanics must necessarily have been built, which we have subsequently called induction by mono induction.

In the case of post rotary machines, the need to produce a blade movement slower than that of the eccentric has been realized by the use of a blade induction gear of the reducing type, that is to say of the internal type, to an external type support gear. In the second case, that is to say, retro-rotary figuration, since the blade must rotate in the opposite direction to that of the crankshaft, the blade gear is of the external type, while the support gear is of the internal, which will force a sufficiently accelerated back rotation of the blade so that the observer can observe, observed the opposite movement of the latter relative to that of the crankshaft. (Fig. 10 a)

Observation by positioning on the crankshaft.

The second type of observation gives rise to all the other first degree mechanics, including the mechanics by intermediate gear, from Wankle, as well as our first degree mechanics, including for example by semi transmission, and by hoop gear, by central gear. active,

This type of observation is possible if it is assumed that an observer is positioned on the crankshaft of the machine and compares the direction of its own movement with that of the blade. This one will note that contrary to what happens in the first case, the blade always acts with against the direction of the crankshaft. There is no contradiction between the two observations. Indeed, even if the blade always rotates in the opposite direction to the crankshaft, its reverse rotation speed varies depending on whether it is a post rotary or retro rotary machine. Thus, if its speed of rotation is lower than that of rotation of the crankshaft, as it is the case in post rotary machines, the outside observer will continue to observe that the planetary rotation is carried out in the same direction as that of the crankshaft. Furthermore, if its reverse rotation speed is higher than that of its crankshaft, as is the case in retro-rotary machines, the outside observer will continue to observe a movement opposite of it relative to that of the crankshaft.

We can deduce from these assertions that the mechanics to be constructed from an observation on the crankshaft, will not directly seek to perform an action in the same or opposite direction of the blade, as in the case of the first observation, but a rotation in opposite direction to that of the crankshaft, but with different speeds however, thus realizing post rotary or retro-rotating machines. (Fig. 10 b)

Again, by way of example, Wankle's intermediate gear induction mechanically produces this observation. The blade is activated not in a direct relation to the body of the engine, but by means of a gear mounted on the crankshaft, in such a way as to be activated by its relation to it.

As we have already mentioned, the mechanics by hoop gear, by central active gear by semi transmission, and several others of our design are mamcic works resulting from this same perspective and observation.

It is from these types of observation that we were able to construct the consequent mechanics, which we can call first degree mechanics with front prominence, and first degree mechanics with rear prominence, depending on whether it is the front or rear part of the blade which produces a thrust, the opposite part producing, as we have already shown, a counter-thrust.

External observation of displacement points.

A third type of observation can be made, and this type of observation will be the rational source for the realization of mechanics by poly induction. In this type of observation, it is again a question of carrying out an observation starting from an external fixed point., However, here, it is not a question of observing the movement of the blade in general or of compare it with that of the crankshaft, as in the case of the first type of observation. It is rather to observe the course of various points of the blade for a rotation. This type of dynamic observation will be called. (Fig. 10 c)

This observation will make it possible to realize that any point located on a line starting from the centers with the points of blades traverses the caricatural form of the cylinder in which it strolls. Secondly, this observation will show that any point located on a line joining the center of the sides to the center of the blade crosses a shape similar to the shape of the cylinder, but this time in the opposite direction to it. The observer will thereafter note that the points of the two forms are always equidistant from each other, which will make it possible to attach a rigid blade to mechanics performing these two points.

On the basis of this observation, two planetary mechanics working, however, working in opposition, will therefore be carried out, what will be called poly induction. (Fig. 1)

The original and fundamental theoretical aspect of poly induction

Again, the poly induction method is much more than a support method. It is, in a way, a dynamic geometric understanding quite contrary to that of the thinkers of the prior art including Wankle. Indeed, for Wankle and his predecessors, the geometric realization of any shape of cylinder is produced by subtraction of movements, that is to say, a rapid central movement, that of the crankshaft and a slow external movement and in opposite direction, that of the blade. As we saw previously, there is inversion and realization in a combined way of the mechanical parts. The subtraction of these movements made by the central eccentric and by the blade, produces the curvature of the cylinder. (Fig. 12)

However, poly induction shows that the production of the curvature of the cylinder can be carried out in a completely different way by the production in an additive and non-subtractive manner, of two positive movements, one, master produced by the central crankshaft and the second, secondary. , produced by a subsidiary crankshaft. In addition, the slow movement, therefore master, is this time carried out at the center of the machine, and by the crankshaft, and not at the periphery, and in a manner confused with the blade.

In addition to carrying out in a dissociated way the compressive, ligaturai and mechanical elements of the machine, poly induction shows beyond any doubt that the curvature of the cylinder can be achieved by the sum of two positive dynamic circular actions, and not, as in inventors of the prior art by the sum of contradictory actions.

But there is much more to consider. As we will see later, the type of dissection of the movement in under movement carried out by. poly induction will allow to realize on this basis, a new dynamic organization of the most important and determining, as much mechanically as theoretically, is the dynamic rotary-circular organization with blade movement in Clokwise.

Before going to this step, however, we will generalize here some notions of poly induction.

Poly induction: generalization of methods and horizontal distribution of under movement: circular rotary machines

We intend to generalize the poly induction method in the following four ways:

A) mention that any induction can be used to control each post rotary subsidiary induction of a poly induction B) that any location of the crankpin connection points can be chosen, and will make it possible to distinguish the compressive, neutral and motor aspects of the machine in poly inductive mode. 1) that when producing with more than two subsidiary crankshafts, it is possible to keep the Slinky hinge effect by performing poly induction dynamically, that is to say alternately

A) poly induction by all inductions

In standard poly induction, in double or in several parts, each subsidiary induction is comparable to a mono induction however post rotary, comprising a gear of induction post rotatijÇ of external type, and a gear of support also of external type, common to each induction.

1) We simply intend to state here that the post inductive action of each sub-induction can be carried out by any induction of first degree, this being however carried out in a post rotary manner. For example, each induction gear can be activated by hoop gear, by intermediate gear, and so on. (Fig. 13)

2) the second clarification that we intend to make here is that any point on the blade produces the shape of the cylinder, but with different orientations depending on its situation. As we noted previously, the points in the axis of the points, and the points in the axis of the sides, produce complementary shapes of the cylinder. Note also that the intermediate points produce the shape of the cylinder, but this time oblique. The machine can therefore be supported not by double articulation, but by tri-articulation. In this case, the supports by the sides will produce a descending inking, supports them in the intermediate position, a late or precipitated descending inking, and supports them by the tips, a superior inking. It will therefore be said that in the first two cases, the machine is of the motor or neutral type. The supports in the sides carry out a reverse stroke of the crank pins, vertical, and the parts of the blades joining these support points to the blade points must be considered as geometric additions whose effect will be to restore, despite these positions, and stroke, the expected initial curvature. During a point support, the machine is of the Compressive type. Note that the latter type was carried out by Muelling. It is therefore evident here that even poly induction can be carried out in a negative manner.

The positioning of these induction will allow, as is partially achieved in poly induction in double part, an inking and a hinge effect during descent, which will allow to realize the machine in its motor version

2) When produced with more than two supports, a large part of the hinge effect Slinky produced in two parts disappears. However, it is important to keep this mega effect, which makes the inductions interact between them, and not to keep them in isolated reports of mini inductions. Furthermore, but it is also important to provide a balanced support which is also distributed between the various inductions of the faces of the blades of the machines, as is possible with the embodiments with triple parts. (Fig. 13 b) The solution to this dilemma is to perform a Slinky induction alternately and successively. To do this, we will subtract teeth either on the support gear, exit on the induction gear so that never more than two inductions, except during their alternative transitions, work together.

Each induction is therefore alternately motivated by its direct connection to poly inductive mechanics, or even by its strict connection to the blade.

Consequently, the blade is always held minimally by two inductions and the third induction is mechanically free and driven by the blade itself.

In this way, not only is the Slinky effect ensured, but also the contradictory induction is suppressed, producing any counter or half-thrust.

As we have just shown by the poly induction mechanics, the dynamic geometric design of Wankle machines is not only faulty because, as we said, it lowers the number of parts making up the machine, but also because, in doing so, it also reverses them.

Wankle reversal gap

To better understand this idea, we will use as an example, again strictly piston engines. We will indeed compare standard piston engines to orbital piston engines and rotor cylinder engines, the latter being taken from our Canadian patent In the standard and orbital engines offered, each compressive, ligaturai and mechanical assembly taken in isolation is exactly the same, in that the purely rectilinear action of the piston is transmitted by the connecting rod to the crankshaft rotatably mounted in the machine. The differences between these machines are only relative to the initial positioning of certain parts, such as the piston cylinder assemblies and the crankshaft pin. In the case of standard machines, several successive explosions are established by placing several crankpins in different dials of the crankshaft, each set of cylinders being found on the same line. In orbital engines, it is rather the connecting points of the connecting rods which are on the same line, since these are connected to the same crankpin. Conversely, the cylinders are arranged in different dials. Again, the dynamics of construction or deconstruction of the compression is exactly the same for these two machines, since the internal ratios of crankshaft, connecting rod and pistons are maintained.

The dynamics of the piston rotor cylinder engine are very different.

The connecting rods and pistons are all attached to the same fixed, off-center axis, and the rotor cylinder is rotatably mounted in the center of the machine. (Fig. 15)

The rectilinear action of the piston in its specific cylinder is therefore the result of the circular double action of the cylinder and piston from different centers. This machine is much less powerful than the two other versions previously commented on, and this is explained because the power is partly transmitted from the center to the periphery before returning to the central motor axis. There is therefore a loss of energy. A second way to understand the reason for the power deficiency of this type of machine, when used as an engine, is to understand that power is obtained, similarly to the result obtained between the keel and the sail of a sailboat, by a very low torque angle, even halfway through expansion.

If we seek to determine the geometric cause of this insufficient energy production, we realize that the functions usually granted to the crankshaft have been deconstructed and subdivided, then granted to different parties. In fact, it can be seen that the crankpin of the crankshaft is produced in the form of the fixed secondary axis, while the rotary part of the crankshaft is granted to the rotor cylinder. There is therefore both dismantling of the crankshaft and carrying out part of the dismantling thereof in a manner identical to the cylinder. In effect, the rotor cylinder produces both the crankshaft components and part of the compressive components of the machine. We thus see, thus clarified, more precisely the contradiction, which consists in finding that a strictly rectilinear cylinder can transmit only little energy when it is produced as a crankshaft. In summary therefore, in the rotor cylinder machines, piston rod and cylinder are present in the machine. It is is the crankshaft which is not produced in its standard form, but is rather produced in part with the cylinder. The crankshaft is therefore found at the periphery.

In the case of the aforementioned machines, the strong knowledge of the basic provisions, when this is carried out in a standard manner and of the orbita type, make it fairly easy to understand that the role play performed in the rotor cylinder machines is a constructed version .

In rotary machines, taking charge of the construction mistake is more difficult, since these machines have, from their origin, been rendered in an inverted arrangement. "

L We must indeed assume that in any rotary machine the master crankshaft, unbeknownst to the inventors of the prior art, was produced in a manner coincident with the blade, and that, starting from the observations that Von can draw from our poly inductions , the central eccentric is nothing other than the expression of a subsidiary crankshaft, placed in place and center of the crankshaft.

As we said before, the first shortcoming of rotary machines rotary machines do not have connecting rods, and for this reason they have lost the connecting rod effect. Now, in the light that what we have just demonstrated, it could be affirmed that if certain parts of standard rotary machines were produced in a confused way, they are not, as in sliding motors, connecting rods and pistons, but rather, as in rotor cylinder engines, the crankshaft and the compressive part, the cylinder. We believe that standard rotary machines are rather machines in which, as in the example mentioned above, the master crankshaft was produced in one of the compressive parts, here the blade. If this turns out to be justified, one could say that what is generally understood to be the crankshaft of a rotary machine, when produced by first degree induction, is in fact only the subsidiary crankshaft thereof, the master crankshaft being produced in a manner coincident with the blade.

The fully formed rotary machines, such as, for example, the layering machines and the poly induction machines already commented on, would include the correct arrangement of the compressive, motor and ligating parts.

If this assumption is true, we can say that in all standard embodiments, namely first degree, of rotary machines, the master crankshaft is removed from its central position, to be replaced by the subsidiary crankshaft. From then on, the master crankshaft is made in the same way as the blade. It can therefore be seen here that the second fundamental shortcoming of the machines, namely that the master crankshaft of these is produced at the periphery, in a manner coincident with the blade, is completely corollary of the first, in which the 'We recognized an excessive lowering of the machine parts and the confused realization of certain elements.

Wankle's third fundamental flaw: the post-rotary differentiation of machines.

In the previous discussion, we used examples of piston engines, to show that first degree engines invert the parts of the machine in a certain way. But the main example, that of the rotor cylinder engine, remains imperfect. In this one, effectively, the crankshaft is moved in the cylinder, while in the rotary engine, it is in the blade.

We must therefore go further to give a valid image, when produced as piston engines, of the rotary engine. This image will make it easier to realize the third gap we are talking about here.

To make the reader understand our point, we will once again use an example taken from piston engines, standard and rotary. "

As we have already shown, standard piston engines, the best mounting when made with a fixed cylinder, and when when made with a rotor cylinder, as shown in our Canadian patent already cited and examples already cited

However, in the rotor cylinder machine, the crankshaft, as we have shown above is subdivided, and one of its parts, the crankpin is produced by the support axis of the connecting rods and pistons, and the other l 'central axis of rotation, by the rotor cylinder. It is possible, as shown in our comments to the Canadian patent application entitled Energy machine with poly crankpins and Simple induction machine, to achieve a movement of contraction and expansion of the cylinder and the piston by increasing the degree of machine by splitting the crankshaft, so to speak, while keeping the part which has been allocated to the cylinder, by completely rebuilding the initial crankshaft The result will be a hybrid engine, made up of both a standard engine , and a rotor cylinder engine. (Fig.16.2) As can be seen in the same figure, the opposite action or in the same direction of two pistons can be obtained with a fixed cylinder and poly crankshafts in opposite dials and in the same dial.

The action of this new crankshaft can therefore be determined in both directions. We can indeed increase the post rotary speed of the latter and make it higher than that of the cylinder, or even reverse it relative to that of the cylinder. In doing so, the power of the machine will be further reduced or increased. Indeed, in the first case, the thrust on the piston is achieved against an element, the cylinder, which travels, although more slowly, in the same direction as the latter. The developed power is therefore partly contradictory. It is produced only by the difference of the real thrust, minus the counter thrust by the reaction on the cylinder. This is why we will speak of simply differential thrust.

Conversely, when the crankshaft is activated in the opposite direction to the rotor cylinder, the two parts travel on the contrary, and the expansion takes place at the same time on these two parts. As in the two cases of semi transmissions coordinate parts, the power, in the second case is not differential, but additional, since it is the result of the contrario movements of the parts.

We can therefore deduce more given examples than the most relevant comparable of rotary machines, and particularly post rotary machines when produced with piston, the rotor cylinder engine with post rotary induction, when produced with a straight rod. In this engine, the force is only differential, and moreover the connecting rod effect is obliterated by the use of sliding rod.

summary

These three fundamental shortcomings would explain the lack of power of these machines, and would open the door to a set of new solutions which gradually would end up determining the best position for the crankshaft and other elements.

Our staging and poly induction solutions indeed show that it is possible to advantageously correct these shortcomings. A third type of solution, original and extremely. advantageous in several respects consists in the solution by movement of blade in clokwise and rotational cylinder, the dynamics of which has been shown in the first part of this work. In this part we will generalize this dynamic and show the relevance of this generalization under the name of rotary-circular machines. (Fig. 17)

In the next part, we will go further, by generalizing a dynamic of our first works that it is possible to carry out it in a central and independent way, in particular in the methods by poly induction and by staging of induction, and that its realization confused this time with the cylinder, in the circular rotary engines, is certainly the realization which cuts off all the design errors already commented on, and which is the realization implementing the deep nature of these machine. Summary of this first part

In summary of this first part, we can therefore state that the deep nature of rotary presses would therefore be contrary to that of piston engines.

In standard engines, it is quite easy and obvious to realize the veracity of this statement, since one can easily compare standard machines to their dynamic derivatives, machines with rotor cylinder and one can notice quite easily where the elements have gone.

In rotary machines, the same observation is much more difficult because these machines were made by use, by experience, and therefore mechanical history has designed them from the start in reverse, in the 'absence of representation benchmark allowing to gauge this counter orientation. Poly induction and induction staging allow this understanding. We therefore worked as if, in piston engines, standard engines were invented after rotor cylinder engines.

In summary, and as surprising as it may seem, we must understand that in rotary engines in their standard form, what plays the funny central crankshaft is similar to a rotary connecting rod, or even a subsidiary crankshaft centrally arranged and that the real crankshaft is produced externally, in a hidden way and confused with a peripheral and compressive component, the blade.

Second part

Horizontal reintegration of the rod effect: Machines with clokwise movement / rotational cylinder, and horizontal dynamic generalization: rotary circular or rotary-orbital machines

We now know that the three previous shortcomings are present in all Wankle machines. Not only is there an excessive lowering of the constituent parts of a motor machine, by the confused realization of some of eues, but also that this confused realization is moreover reversed, in that it is not , as in the case of engines with sliding rods, the rod which is produced in a confused manner with the compressive part, but the crankshaft, and in addition post differential, which reduces the power of the machine.

The motive power is therefore subtracted as much vertically as horizontally. It is, simultaneously carried out, these entrenchments and inversions of the parts which are the root causes of the non-realization of the explosive power of the machine.

Furthermore, as will have been noted, even if the stepped and poly induction mechanics largely correct the fundamental shortcomings of the prior art already stated, they are not themselves perfect. The staggered mechanics will certainly offer some resistance to marketing. It will be argued that to control the movement of a blade supported by the rotation of two superimposed crankshafts, may indeed cause certain very material difficulties. Furthermore for poly induction, it could be argued that the use of three subsidiary crankshafts for one blade does not represent an economy compared to that, in a standard engine, of using three pistons for a crankshaft

Moreover, by showing that the position of the crankshaft confused with the blade is not relevant, we must also ask the question of whether to bring the position of the latter as central master crankshaft as in the machines with piston is the best arrangement for rotary machines.

Observation from the master crankshaft of poly inductive machines And realization of the clokwise birotative movement of the machine (figl8)

Note from the start that we have shown the sequences for a tour of the Clokwise mechanics, first, second and third level in the first part of this work. In this part, we will provide more in-depth theoretical explanations, we will generalize these achievements and we will rationally determine the rules of composition of mechanical assemblies allowing them to adequately support the compressive parts

To answer the above-mentioned objections and questions, a new type of observation will be relevant, a type of observation which will be made possible by the mechanical realization of the poly induction method.

In poly induction machines, the rotation of the master crankshaft corresponds to a rotation equal to the relative speed of the blade. One supposes, in this type of observation, an observer positioned on this master crankshaft, and observing, as in the previous cases, the behavior of the cylinder, of the blade and, in addition of the subsidiary crankshafts. We must deduce that even if for us, external observers, this master crankshaft is in rotation, for the observer being positioned there, awaiting its constant speed, the reference frame will give very different results. Indeed, the observer will clearly see the components of the circular rotary movement with blade in full Clokwise

Indeed, by considering the movement of the blade, the observer will note on the one hand that the movement position rotational of this one is circular, and moreover that unchanging orientation aspect, that is to say that the orientation of it does not vary, despite the circular action of its center. Similar to the turning hands of a watch, the figures of this watch always remain at the same angle, that is to say perpendicular. This is why we called this specific movement of the blade, the Clokwise movement.

Conversely when the observer directs his gaze towards the cylinder, he will no longer perceive it as we see from the outside, namely as a fixed element, a fixed element, but rather as an element rotatably activated in the opposite direction of movement positional circular of the blade. The observer will therefore be virtually opposite, from the first expression of the rotary rotary birotative machine, the clokwise blade / rotational cylinder movement machine (Fig. 18) Another construction making it possible to carry out the Clokwise movement, and showing that it comes from poly induction cutting, unknown to Wankle t these predecessors, is to enclose the crankshaft of a poly inductive machine, for example in a vice and activate the remaining elements. We will then see that the blade produces exactly the clokwise movement and that the cylinder produces the rotational movement on the contrary. (Fig. 18)

Concrete realization of the clokwise machine

The Clokwise realization of the machine will be produced when the observations of the observer are physically carried out as previously positioned.

It emerges from these explanations that the most obvious concrete realization of the machine, will result from a revitalization of the very mechanics which made it appear. One can indeed imagine, starting from this observation, that since the crankshaft is without movement relative to the observer, the latter will be stationary, and could therefore be produced in a manner confused with the side of the machine. The secondary crankshafts will be fitted with induction gears and will be rotatably mounted in the side of the machine. They will be joined by a means such as a third gear, ensuring the similarity of their rotations. The blade, which will be mounted on these crankshafts will therefore carry out a strict circular movement, without directional movement, a so-called Clokwise movement. The gear uniting the induction gears will be the dynamic support gear, and will also be coupled to the cylinder, which will ensure the back rotation. (Fig. 19) The same procedure can be carried out for machines of the retro-rotary type but using a dynamic support gear of the internal type. Let us note that the machines in movement clokwise of post rotary figuration carry out, a movement of the compressive parts on the contrary, and the machines of retro-rotary figuration carry out, when they are assembled with the initial degree, a movement in the same direction. We will come back to these types of criteria which are most important for driving machines.

Specificity and originality of the clokwise movement and circular rotary dynamics.

If we continue to understand the driving machines as we started them, we will realize that the blade movement machines in clokwise are original and important, for several reasons, as much mechanical as theoretical. These machines completely correct all the defects and shortcomings of the rotary machines of the prior art, and this is understandable since the latter

Go beyond the normal categories of these machines to realize both the qualities of piston machines and turbines. As we will show later * the specific movement in Clokwise can be obtained by a large set of combinations of mechanics. However, the previous embodiment, by fixed polyinduction already makes it possible to understand the following. The clokwise movement has the following major mechanical and theoretical originalities. (Fig. 17) A) the machine, unlike any machine of the prior art, is, dynamically, perfectly birotative. Indeed, as can be seen, the blade has no orientational rotation. It is neither post rotary nor retro rotating. It has a derotation with respect to the crankshaft very exactly located between the post rotary and retro rotational derotation. It is therefore perfectly birotative, It therefore has a similar nature not to the machine of the prior art, but rather that of poly turbines. By its nature, it will always require two inductions to activate the parts correctly.

B) the machine consequently does not, unlike any machine of the prior art, perform any counter-thrust on the blade. Similarly and even higher than that of a piston, the thrust is produced not only over the entire surface of each face of the blade, but also in a perfectly distributed manner on each side of the poly inductive support points in mono inductive these (Fig. 20) This feature allows once and for all to compare advantageously the thrust of rotary machines with those of piston engines.

C) the machine, unlike any rotary or post machine of the prior art, and similarly to turbines, the movement of the clokwise blade, as well as the mechanical parts do not produce any acceleration or deceleration of any of the parts

D) the machine distributes the layers of poly induction or stepped inductions, this time horizontally, which removes any vibration in the machine

E) the curvature of the cylinder will cause its back rotation, and this back rotation will achieve an effect similar to the effect of connecting rods of piston engines, and an additional force to the machine.

F) the parts restore horizontally the minimum number of constituent parts allowing the machine to be produced in its driving nature.

G) finally, the blade and cylinder are in opposite movement, which is not found anywhere in the prior art, except in our realizations of simple induction machines, made with pistons, and rocker pistons.

Circular rotary motors with a clokwise movement blade therefore comprise both the qualities of piston engines, rotary machines of orbital engines and turbines, while having only a few of their respective faults.

Indeed, if we compare these machines to piston engines, we see that the blade of these machines accepts a thrust equally distributed as in piston engines. We can see that any point on the blade and therefore on its surface, travels at the same speed. In a way, we can even say that the thrust is greater than that of piston engines, since, the blade being directly connected to the crankshafts, makes the angulation of the connecting rod non-existent. This will result in an absence of friction and energy expenditure caused by your negative counter pushes.

Furthermore, if we compare these machines to rotary machines, we see that they can use the same figures, and therefore produce combustion chambers. closed. Furthermore, the rotationality of the parts can allow the use of light valves.

Finally, if we compare these machines to the turbines, we see that like the turbines, except that they will be made with the help of polycammed gears, all the parts without exception travel at a constant speed, and that there is no acceleration and deceleration of any mechanical or compressive parts.

It is therefore a kind of driving machine situated at the confluence of driving machines of totally different categories from the prior art, which recovers the most essential qualities of each of these but recovers only a few of their faults. The thrust should give them power, figuration a minimum number of parts and rotatability a maximum and unequal velocity and longevity in terms of motor machines (fig. 21).

It should be noted that the geometrical dynamics of the opposite poly induction, as we have shown to that of Wankle, is the dynamic which makes it possible to carry out a just and valid cutting of the movements entering into the composition of the planetary movement of the blade. , in two specific movements, and thereafter, to restore them horizontally by the dynamic clokwise / rotational cylinder.

If our reasoning is correct, this will allow us to answer now the question that we had previously left hanging. We showed indeed that the geometric designs of Wankle and thinkers of the prior art had reversed the composition of the parts by arranging the crankshaft, in a manner confused with the blade, in a peripheral and planetary manner, which deprived the machine of all its motor substance. We then restored a vision

So to speak "piston" of the machine by making it by master and secondary crankshaft, asking us if it really was the most relevant arrangement.

In the light of what we have just shown, it appears that the most relevant arrangement consists in making the machine horizontally, by making the crankshaft confused, this time with the cylinder,

As surprising as it may seem, therefore, while the least relevant provision for piston engines is that of rotor cylinder machines, it turns out to be the most relevant for rotary machines.

Machines with blades in clokwise movement and rotary-circular machines in general: generalization

In the next section we will apply ourselves to show that the circular rotary machines constitute a specific determined type of machine, realizing as it were the motor machines in their horizontal plane, as opposed to the vertical plane whose existence we have shown in the first part.

To do this, we will show mainly that circular rotary machines can be produced with all existing inductions, to the extent that the concepts of semi transmissions, up and down induction are specified.

We will then show that they can receive all types of blades from standard machines. We will then show that they can establish different degrees of achievement by dynamics. We will then show that a correct understanding of these machines requires distinguishing their material, virtual and real aspects. Finally, we will show that all of these generalizations will allow us, by the combination of the two vertical planes and horizontal, to produce a synthesis of the global and a relevant criteria of any driving machine.

More specifically we will deal with the following points:

Mechanical generalization a) Clokwise movement by central induction. b) the semi-transmission methods by considering them as a shifted induction from center to center, called horizontal induction c) the methods by rising induction and descending induction and horizontal induction d) and we will show that the combinations of stepped induction can be produced horizontally, and allow the support of the compressive parts of rotary-circular machines

Figurative generalization e) that any rotary-circular machine has all the variants of any other machine, namely that it applies 4) just as much to post rotary as to retro-rotary machines, 5) that they apply to these machines any number of sides 6) that they apply to rotary machines, such as poly turbines 7) that they can be produced as accelero-deceleratively 8) that they can also be produced with combinations of single cylinder blades, blades simple, standard poly faces blade, blade structures

Dynamic generalizations 9) that they can be carried out in degree, by movement of clokwise blade of first degree, of second degree, these degrees being able to be carried out horizontally or vertically ”10) that they can have various degrees of differential mechanical retro and post rotary, and on the contrary 1 l) that they can, when realized on the contrary, realize at the same time material, virtual, and real cylinder figures 12) That they can, like static cylinder machines be made in bifunctional compressive parts

These additions will allow us to globalize our whole company and show: 13) that the set of all possible machines can be arranged in chromatic ranges 14) that the determining characteristics of all machines can be specified by a set of very broad generic criteria, encompassing the criteria of the prior art 15) that several semantic difficulties of the prior art can be correctly specified: mechanics suitable for dynamics with a rotor cylinder, machine direction 16) That mechanics by polycamation can also be able to contain the upright forms of retrotrotative machines 17) that they can be made in center-periphery inversion, by rotary clokwise cylinder / blade

Mechanical generalizations

Clokwise movement by central induction.

Another very interesting characteristic of clokwise dynamics should be noted right now. In it, any point of the blade describes exactly the clokwise movement, and even the central point of the blade. Therefore, the blade can be supported by its center. In addition, it is important to reiterate the character and perfectly birotative nature of this movement. Starting from these two ideas, we will see that, to ensure support by the center of the blade in Clokwise movement, we can use any induction resulting from an observation by the crankshaft, taking care, however, to carry out original bimechanical support and induction gear ratios, i.e. one-to-one support and induction gear ratios. Indeed, in the prior art, as we have specified, it is always intended to rotate the blade in such a way that it has a distinctive orientational character, post rotary or retro rotary. Consequently, the gear ratios are always produced either by larger support gears, during the retro-rotary productions, or even by smaller support gears, for the post-rotary productions. The Clockwise realizations of blades and the one-to-one induction ratios that their support requires are not in the order of thought of the initiators of the prior art. This report requirement, original to the realization of the Clokwise movement is explained by the fact that to achieve an orientational non-rotation of the blade, it must undergo a rotation perfectly equal to the post rotation of the crankshaft. Since the central crankshaft of these machines is equivalent to the subsidiary crankshafts of poly induction concentrated in one and that all the inductions are possible for this one, the same methods all apply here, respecting the ratios mentioned above. It is therefore possible to realize the orientational support of the blade by intermediate gear, by hoop gear, by central gear actiζ and so on, respecting the clokwise ratio of one on one. Furthermore, the use of simple mono-inductive induction is impossible, which clearly shows the originality of this machine. It is necessary to carry out the clokwise movement, by this induction, to use the semi transmittive method of this one, method by which the retro-rotation of the support gear will accelerate the orientational retro-rotation of the blade at the speed equal to that of the crankshaft. (Fig.22)

We now know that it is possible to achieve the clokwise movement of the blade by fixed poly induction, the induction gears being driven in the same direction by means of an external, internal, chain gear, or even that the clokwise movement of the blade can be achieved by central induction with a ratio of one to one. But like step machines and poly induction machines, Clokwise movement machines restore your rotational levels necessary for full motor action. Like poly turbines, by their nature, Clokwise movement machines are second degree machines since they always require two inductions, this time horizontally arranged. It is indeed necessary, in addition to the retro-rotary, or post-rotary control, depending on whether there is a post-rotary or retro-rotary machine, of the rotational cylinder.

To do this, three concepts must first be specified, which are those of horizontal or semi-transmittive induction, then of rising and falling induction. (Fig. 18 b)

Semi-transmittive induction or horizontal induction

We have shown on several occasions the importance of semi-transmissions, these making it possible to modify the initial figures of the machines, or even, to make these machines capable of restoring their retro-rotary and post-rotary power of the same blade.

It can be said that there are mainly two types of semi transmission, accelerating or decelerating transmissions, and reverse transmissions. It could also be said that each of the semi transmissions could be produced with standard gears, external or internal, or pinion gears. (Fig.23)

In circular rotary machines, it will often be necessary to achieve both reverse and accelerative semi-transmissions. This will happen mainly when the action of the cylinder is activated by activated compared to that of the eccentric. Since the cylinder acts in contrast to the blade, and at a speed different from the latter, it will require a semi transmission realizing both these two necessities.

Poly inductive semi transmittive induction is very simple from this aspect. This involves rotating the gearbox known as reversing gears in the machine block. It will then be provided with which, if necessary, the crankshaft of the gear of an external type coupled to these gears, and the rotary cylinder of the machine will be provided with a gear of the internal type. This gear will also be coupled to the reversing gears. The result of such an arrangement will condensed way to achieve the anti-rotation and reduction of speed of the cylinder relative to that of the crankshaft. Note that on some occasions the speed of the parts may be equal, and in other cases that of the rotational cylinder will be higher. We can also proceed by pinion gears. One of the pinion gears will be coupled to the crankshaft and the other to the cylinder. We will couple these two gears via a double of inversion gears, taking care to choose one of the two gears with a dimension greater than the other. Each of these gears being coupled to the vtfebrequin or cylinder gear. This will get both anti-rotation and the necessary speed difference required. (Fig.23)

Generalization: we state that all the inductions can thus be transformed into semi transmission, and for this reason, semi transmissions will be able for the purposes of present to be named adjusts horizontal induction title. We will find, in our previous patent applications as well as in the patent applications placed on the list, several examples, which all meet these definitions.

Up and down induction

The term “rising inductions” is understood to mean all the first inductions of the prior art as of our art and of higher degrees, the support gear of which is disposed centrally, and the induction gear of which is disposed at the periphery . For example, inductions by mono induction, by hoop gear, by poly induction are rising inductions.

Conversely, if there is a support gear, this time at the periphery, either rigidly fixed on the crankpin of the crankshaft, or else, for example on the blade of a machine, and that starting from this gear, l 'one activates a central gear one by descending induction. The use of these two inductions in combination in a standard machine can make it possible to create a blade support different from the motor axis which will be activated by the blade. This would be, at the limit of an electrified semi-transmission method. (Fig. 23)

In the case of n circular rotativo chines, one will be able by one side of the blade, to activate the movement in Clokwise of this one, and on the other side, to fix to the blade a gear of peripheral support, and by the recourse to an induction, for example by hoop gear, hindering the rollback of the cylinder. (Fig. 23)

The three main methods of supporting circular rotary machines of the first degree with clokwise movement

As we have shown for the staging of inductions in height, since there are more than fifteen first degree induction, and each can be combined with a second first degree induction, this being however peripheral, we have a very impressive total of inductions.

In the same way, if we accept the simplification that we have previously produced to the effect that all semi transmission is a horizontal induction, or in other words, an induction neither rising or falling, but rather transferred to the same center, or on itself, and qùé consequently any induction can be transformed into semi transmission, and of other by that the circular rotary machine always require, two confused and coupled induction, one realizes that there exists here again an impressive number of possible induction combinations which it would be difficult to list in full.

A rational and synthetic regulation of the organization of these will make it possible not to have to expose all, and at the same time to encircle them correctly. This rule is as follows

One can realize the combined support of any rotary rotary machine by using, like combinatory part, (fig. 24) a) of the blade, b) of the crankshaft, c) or of the induction gear of the cylinder, each of the rising, falling or semi transmittive inductions being combined with this same element which will have been determined.

To better understand the reason for this last statement, it is enough to grasp the idea that the movement of the cylinder and that of the blade must be perfectly coordinated and synchronized. Consequently, their inductions must also be, which means that they must have a characteristic of dependence on one another. In other words, there will have to be at least one of the parts of their respective action, which is shared, which is the same for the two inductions. These parts will be either the blade, the crankshaft, or the induction gear.

Combinatorial interdependence by blade.

As a general rule, we will achieve the interdependence of the systems by means of the blade by activating, as we have previously shown, the Clokwise movement of the blade by one of the induction, with ratio of one on one of the gears of support and induction, and one activates, inversely the cylinder, again from the blade, by a descending induction, by placing on the blade a peripheral support gear, and on the rotational cylinder a gear induction. (Fig. 24)

In this way, when the blade is activated by the crankshaft, by the use of its rising induction, it will activate the cylinder, and conversely when it is activated by the cylinder, by the use of its descending induction, it will activate the crankshaft Any induction can therefore serve as a rising or falling induction.

Combinatorial interdependence by the crankshaft

In the methods of combination of induction by the crankshaft, one will realize starting from the crankshaft a rising induction of one on one which will ensure the correct movement in Clokwise of the blade. Furthermore, as shown above, the cylinder and the crankshaft will be connected by means of an inverso-accelerative semi-transmission. Therefore the movement of the blade and the cylinder will be fully coordinated. To carry out this type of induction, one will be able to use, for the blade, any induction, and for the cylinder of any semi transmission. Several combinations are therefore possible. We will consult our work, in antecedents, and our previous work, to be aware of several examples to this effect. (Fig.24,55,56,57)

Combinatorial interdependence by blade support gear.

As already shown previously, the ratio of the support and blade gears must be carried out in an order of one on one to ensure the Clokwise movement thereof. Furthermore, we know that we can, as long as we adequately modify the size ratio of the support and induction gears, we can energize the support gear of any induction, the thus making it semi transmittive, without modifying the directional rotation ratios of the blade relative to its initial dynamics. It is therefore possible, starting from the crankshaft, to perform a retro-rotary and semi-transmittive management of the support gear of a rising blade induction, which we have done several times in our work

In the case of circular rotary machines, it will be necessary to motivate the dynamic support gear in such a way that while allowing the respect of the characteristics one on of the Clokwise movement, it activates, being rigidly fixed to it, the roll back of the cylinder, consequently l 'We can say that the same semi transmission, will activate the dynamic support gear of the blade, and that this dynamic support gear of the blade, will be confusedly the induction gear of the cylinder. The two systems will therefore, in a broad sense, be connected by the same semi transmission, and in a direction restricted by the gear, serving as a support gear for one and an induction gear for the other. (Fig. 24)

As before, several configurations are possible, since there are several semi transmissions, but the logic will remain the same.

Figurative generalization

Machines in Clokwise movement of post rotary and retro rotary blades.

Although original dynamics, recalling as we said the qualities of piston engines and turbines, circular rotary machines use again the geometric figures of blades and cylinders of the prior art. The rotary rotary blade movement machines in Clokwise can therefore be made just as much of type of retro-rotary figuration as post rotary. It should however be noted that their dynamics are different in that, while the machines with Clokwise post rotary movement carry out a movement of compressive parts on the contrary, the machines of the retro-rotary type, carry out a movement of blade and cylinder in the same direction. (Fig. 25)

Rotary circular machines with blade movement in Clokwise and number of sides.

As we have already observed, the figurations of the compressive parts of circular rotary machines are similar to those of standard rotary machines, when these are performed in the first degree. It is therefore necessary to specify that all the figures of retro-rotating or post-rotary machines can therefore be produced in circular rotary rotation mecha, with blade in clokwise movement. In fact, for example, in a post machine with a triangular cylinder and a four-sided blade, the blades will always have its Clokwise movement and the cylinder will always have anti-rotation. Similarly, in the retro-rotary figures, the blade on three sides will have a Clokwise movement in the same direction as its cylinder, strictly rotational. (Fig. 25) Rotary circular machines with blade movement in clokwise and birotative machines

The polyturbine type machines, whose cylinder and pale compression structure were invented by Wilson and for which we provided the adequate mechanics when the cylinder was fixed, can also be produced in their rotary-circular form. In these cases, the subsidiary crankshafts, added with connecting rods of geometry will strictly carry out only a circular action, which will carry out the losango squareoid driving of the palic structure. Their induction gear will be coupled to the cylinder gear which, in rotation, will complete the system. It will be noted here, that even if the induction crankshafts and the cylinder have no acceleration deceleration, the pale structure, more complex, achieves its oscillatory aspect, an aspect to which we will return later for any machine. (Fig. 26) It should also be noted, as we will see below that several degrees of circular rotary dynamics will be possible for all machines, including poly turbines.

Rotary circular machines with blade movement or decelerative accelerating cylinder

One can, as for any machine, in the assembly of rotary rotary machines of polycamed or polycamés derivative gears, which will produce modifications of the forms of cylinders resulting from accelerated decelerative movements of the parts. We will use mechanics similar to those that we have already described in our differential turbines, in which the cylinder will be supported by polycamera gears, producing a support with strictly circular action, but accelero-decelerative.

One could for example decide to keep the rotational movement of the cylinder its regularity but grant the Clokwise movement a certain accelerating decelerative irregularity. This will modify the cylinder and thereby achieve a higher thermodynamics, as when applied in standard machines. In circular rotary machines, one can inversely realize the movement of the rotational cylinder in decelerated accelerated. (Fig. 27)

Rotary circular machines with blade movement in Clokwise: types of blades

We can make circular rotary machines with the three types of blades that can also be used in standard machines.

First, we can use a combination of unitary blades to the cylinder and produce explosions either between each of them and the cylinder, or between them and the cylinder. (Figl28) In these two ways the combustion chambers can be common, which will have the effect of multiplying the crankshaft span by two. This will considerably increase the compression ratio and make these machines with diesel gas management.

Of course, these machines can be made with blades with several faces, ie standard blades, or as we have previously determined with blade structures, (Fig. 28) Rotary circular machines with blade movement in Clokwise and number of degrees,

The Clokwise movement in its most natural state is achieved by positional movement of a circular blade. It can, as we have also shown in the first part, be non-circular, for example rectilinear. (Fig. 29 b) It can also, when the range of the central crankshaft is wide, be part of a cylinder movement not rotational but itself planetary. In these last two cases, it is necessary to increase one of the degree inductions to make the machine (Fig. 29 c, d) The movement of the Clokwise rectiligo blade indeed requires an induction step. Furthermore, planetary driving also requires a higher degree of induction than simply rotational driving. .

Rotary circular machines with blade movement in Clokwise and symmetrical oscillatory movement and in contrast with blade

It is also possible to perform the blade movement in an oscillating Clokwise manner with the use of polycameral inductions. Indeed, the ratios of one on one will remain maintained for one revolution, but, with the use of polycamed gears, the perfectly orientationally fixed movement will now be variable, alternatively. (Fig. 30,31)

This will make it possible to produce the machine figures with odd cylinders and with movement of opposite unit blades, and to realize the oscillatory nature of the poly turbines.

Rotary circular machines with Clokwise blade movement and Clokwise cylinder and rotational blade movement

We have, before present, shown that we can make machines with fixed blades and planetary cylinder. In these cases, the figure produced is a virtual figure corresponding to the real induction of the machine. For example, a triangular type figuration, in which the cylinder is planetary and the blade fixed, requires a post rotary machine mechanical of figure from three sides of the blade to two sides of the cylinder. This means that the apparently retro-rotating figure is the virtual figure of the real post-rotating figure, in the complementary position.

Likewise, Clokwise figures can also be reversed from center to periphery. To achieve these reversals in a perfect way, it is necessary, as in the case of standard figures, to arrange the figures in their complementary direction, and to use the mechanical support of the real figure and not of the virtual figure. (Fig. 33) Thus, Ton can make machines with a dynamic cylinder in Clokwise movement and a perfectly rotational blade dynamic. Of course, as before, this cylinder can be a set of unitary cylinders, in standard polyfaciated cylinders, or in palic-cylinder structure (Fig. 26)

Likewise machines with Clokwise cylinder movement can be produced in bi-functionality, these cylinders of one being simultaneously used as blades of others. (Fig. 56) These procedures allow powerful turbines or two-stroke or backflow management.

Dynamic generalizations

Circular rotary machines and dynamic degrees

We have shown previously, the circular rotary machines can be increased by degrees by modifying the stroke of the center of the blade, while keeping intact the fixity of the orientational aspect of the blade of the machine. The degree of the machines has been increased, so to speak, figuratively, and not dynamically. The purpose of the next remarks will be to show that the rotary-circular machines can be dynamically increased by degrees this time. We will therefore broaden the notion of Clokwise movement machine by that of rotary-circular machines

We will see in the next comments that the Clokwise dynamics are not only important from the practical point of view, and this with regard to the qualities that we have already stated, but also, from the theoretical point of view. We will show indeed since they constitute a major segmentation axis allowing to delimit areas of dynamisms of machines and to realize the understanding of motive machines on a completely different plane, ie from the angle of the degrees of dynamisms. These understandings will make it possible to create a plan of the complete ranges of rotary machines, and to correct several semantic errors in machines of the thinkers of the prior art, while including them in a much more general theory, possessing much more powerful machine characterizations. and effective.

The next remarks will show that we can achieve similar dynamics in rotary machines of the rotary-circulatory type, than in the mechanical cylinder with piston rotor that we have previously exposed by way of example. I

Indeed, so far, we have only commented on rotary-circular machines with blade movement in Clokwise. However, it is possible to make machines whose blade movement will not be. We can for example suppose a machine whose blade movement, a blade on two sides will move in a cylinder on one side, this cylinder being however not fixed, but rotational. (Fig. 33)

In this first case, it will be considered that the blade has a back rotation allowing it to produce three faces. The cylinder feedback will compensate for the figures. It will then be seen that the machine can be made in such a way that the blade and the cylinder act in the same direction. The push from then on, between your parts will only be differential.

Conversely, we can assume, for the same type of figure, a slower retro-rotational movement of the blade, and a post-rotational movement of the cylinder making it possible to fill this alteration. (Fig. 34) Again, but this time actively post, blade and cylinder will act in the same direction, but differentially from each other.

Finally, we suppose the mechanics with fixed cylinder, (34) where the force produced is neutral, and the dynamics with Clokwise movement, (Fig. 34) in which the movement of the blade and the cylinder are conversely, thus developing lot of energy. In the very last Heu, one will be able, as Wankle did, to realize strictly rotationally blade and cylinder (Fig. 34) One thus sees that for the same figure, five very different dynamics are possible.

Comprehension

To better understand the rationality of the last examples, we will state a formula which can later be applied to any machine. We will say that this formula is the dynamical mechanical regularization formula, or formula of cylindrical counterpart. This formula can be stated as follows.

In any machine, it is possible for the same figure of a cylinder blade, to move the next place of compression by anticipating or delaying it relative to the standard time of next compression, this standard place being produced when the cylinder of the machine is fixed . On the other hand, a mechanical regularization will be carried out and the cylinder will have to be dynamically moved.

Let's give an example. We know that during standard dynamics, for example a triangular blade and a cylinder on both sides, we can measure the difference in angulation between the various highlights of the blade, corresponding to the locations of successive explosions, and that in this case, we make an angle of one hundred and four twenty degrees. In the triangular engine, one hundred and twenty degrees separate each place of explosion (Fig. 34, 35)

We can determine for a figure, in any case, any new place of perpendicularity to the eccentric of the successive surface of each face of the blade. Consequently, this planned point of new expansion will not achieve the standard angulation provided for the new blade straightening. For example, if you want to adjust the new compression point not to a hundred and eighty degrees, but rather to sixty degrees, you will realize that the wire lacks a paddle movement of one hundred and twenty degrees to re-align standard. One will therefore have to compensate for and must therefore compensate for this difference by mechanical regularization by applying the difference in angulation of this new point of maximum expansion and that of standard expansion to the cylinder. Consequently, one will make realized: here in the cylinder a reversion of one hundred and twenty degrees.

As we can see, if this point is earlier than the standard explosion point, it will have to be compensated by a retro rotation of the cylinder, equivalent to the same angle separating these two points. Furthermore, if it exceeds the standard explosion point, a post-rotary action must be printed on the cylinder, the angle of which will be equivalent to this difference in order to maintain.

For example here, if we intend to produce the next explosion at two hundred and forty degrees, we will calculate an additional sixty degrees at the standard position. The cylinder will therefore have to actively post activate sixty degrees. However, this one rule fails to make a correct and complete rendering of all mechanical possibilities in this area. To fully understand the types of rotary-circular machines thus created, it is necessary to appeal to the concept of retrorotativity of the blade.

As we have already mentioned, in any rotary machine, the blade has a retro-rotating action with respect to its eccentric. We also determined that the more or less pronounced retro-rotating action made it possible to determine whether the machine was of post or retro mechanical nature. In the two preceding examples, it will have been noted that we, by anticipating or delaying the moment of explosion, increased or decreased the derotation speed of the blade of the machine. By analyzing the examples in more detail, these examples show that when the blade of the machine reaches its next compression after only sixty degrees, it thus produces six explosions per revolution. The retro-rotation will therefore be accelerated to such an extent that a retro-rotary type induction must be used, for example a single induction with internal support gear and external induction gear. In the second case, the speed of the rotary rotation of the blade will remain low and the machine will remain of the post rotary type.

We therefore see that, for the same figuration, the dynamico-mechanical alterations of the machine make it go from post rotary to retro rotary.

It is here that once again, the mechanics with clokwise movement of the blade turns out to be important, since its dynamic nature which is perfectly birotative, makes it possible to consider it here as a most important segmentation terminal. We can still give an image of this birotativity of the machine in Clokwise by saying that the blade reappears explosions in the same places as its inverted figure, for example here triangular. The Clokwise dynamics is therefore an important mechanical hinge. Indeed, we can accelerate the derotation of any post rotary blade, without changing its nature, to the Hmite Clokwise point. If the rotor rotation is further accelerated, the machine becomes retro-rotating.

Figurative and mechanical proofs.

Mechanics is certainly the best proof that a machine belongs to one class or another.

Here, in Clokwise mechanics, the mechanical realizations, in a one to one ratio, are proof of the perfect bimechanicity of the machine. It does not pour either on the side of post inductive or retro inductive machines. When using mechanics of this kind, particularly in mono, induction, they must be corrected by semi transmission to achieve a bi-mechanical rendering. Similarly, if we consider the definitions of blade movement compared to that of the crankshaft, observed from the outside to define the post or retro rotary character of the machines, we can see that here again, the blade does not rotates neither in the same direction as its crankshaft nor in opposite direction, since it rotates only positionally.

As for the capacity of dynamic retro-rotary refactorings, we can understand it in that, as we said, in retro-rotary machines, the derotation of the blade relative to its crankshaft is more accentuated than in the post rotary figures . By understanding that this is the consequence, for the same blade of a greater number of sides of cylinder and by Consequently of a greater approximation of these, it is understood that this approximation, even produced artificially, likewise requires an accelerated blade rotation and a rotary mechanics.

If we strictly observe the movement of the blade movement of a circular rotary machine whose blade has been accelerated beyond the clokwise birotative dynamic, we will see that it will describe a virtual figure different from the material figure, this time retro-rotating.

It must therefore be clear that the mechanical realizations of circular rotary machines must take these points into account and that one must take into account the virtual figure of the blade to determine the adequate blade mechanics of the blade, and the nature of this machine. .

We will return later to these notions of material and virtual figures and show that he was also adding to them those of real figure. But before that, it is necessary to deal with another important subject, that of differential movements and on the contrary

Differential movements and conversely as compressive or motor movements

We can determine important differences between the various machines with rotary-circular movement, which this time are not related to post rotativity or retro-rotativity, but rather related to the realization of these machines in their compressive form. , or in their motor form.

Once again, your Clokwise movement machines will be of great use and relevance in determining this point. Indeed, in this section it is necessary to conclude by stating clearly that if the machines with rotary-circular movement can be subdivided into classes of machines, they can also carry out another subdivision, of the most relevant, either in compressive or motor machines.

The following can be stated. Any machine whose place of next compression will be located between the place of standard compression and the place of Clokwise compression, will have an action in contrast to the compressive parts, which will assure it a motive power. (Fig.45,47,4.2))

We can also state the following, any machine whose place of next expansion is after the time of next standard expansion will see its compressive action supplemented by an action of the cylinder in the same direction. (Fig. 47,49) The machine will therefore remain post rotary, but will become rotary-circular and in its Compressive nature, since the resulting force will only be differential.

In the final analysis, we can state the following. Any machine giving the retro-rotational movement will be accelerated beyond the clokwise movement, and which consequently will react its next expansion time before the next expansion time of this machine will not only become retro-rotating, but will also lose its capacity on the contrary, and will become different. . The machine will therefore be a differential rotary rotary. Indeed, as in the piston rotor cylinder machines that we have previously presented as an example, the rotary-circular machines can be subdivided into motor skills class, that is, the contrario classes, and the anterior or posterior differential class. If we then intend to make a visual image of all of these possibilities, we will determine the following pivotal points (Fig. 49.2) a) the fixed position, in unison: this is the representation strictly figurative of machines of various degrees, when not in motion b) the straight position: this is the position of first compression when the machine is carried out by fixed cylinder, planetary blade c) the third position: it is the position of first deceleration of the decelerative dynamics d) the octave position: this is the position of the parts when any movement when the next compression position is at the same point as that of unison We can by then create circular rotary machine areas.

We will therefore find: a) between the unison position and the Clokwise position, the machines of the anterior differential type b) between the Clokwise positions and the straight position, standard, the rotary-circular machines in contrario c) and between the positions of standard fifth and octave position, the rotary-circular circular differential posterior

It should be noted that we make these distinctions here for post rotary machines. We will show that these distinctions are made, by regularizing them, also obviously to retro-rotary machines, and to machines with a planetary cylinder / fixed blade, or birotatives.

These distinctions are still insufficient to fully describe any machine. In the next section we will show how, with the help of virtual figures and real figures, we can complete this last table, and produce a correct rendering of more complex machines.

Material figures and virtual figures

In our last examples we applied a general rule of regularization of the displacement of next explosion allowing to counterbalance this material positional change by a correct rotational activation of the cylinder. We will have noticed that we randomly chose the new compression position, and moreover that we made the corrections statically and only for this new compression. It will however be noted that even if the rule which we have given is applicable to any new position, the production of the machine obtained will pose problems when these new positions will produce more complex angles. For example, for a machine standard, if the new compression is found at thirty seven degrees, it will take several turns to the machine before returning to the initial position.

In addition one will also realize that one can determine certain new positions which have a semantic mechanical value. The most obvious, for example for a machine of a given type of rotativity, for example post rotary, consists in giving to a given blade, the new compression position of its counterpart, for example here rotary.

For example, since we know that a blade on two sides can feed a post rotary cylinder on one side just as much, or a rotary one on three sides, we can take a blade on two sides and cylinder a post rotary side, and determine the point of next explosion at the same points as in a triangular rotary engine. We will compensate for this change by a ^• rotation of the cylinder, mechanically organized in the same way as for machines with Clokwise movement. (Fig.35.4)

It is therefore reaaHser that the mechanics supporting the blade is exactly the same as the mechanics of a triangular rotary machine, and that for this reason, if we follow the movement of the blade, we realize that It describes exactly this form. Furthermore, since the cylinder is rotational and this arrangement has been obtained by changing the position of new compression of a post rotary machine, the material shape of the blade and of the cylinder will remain post rotary.

Let us give a second example, this time starting from a retro-rotating form, more precisely with a triangular blade and a square cylinder. Normally, each new compression of this machine occurs at all four comes ten degrees. (37.3) We can however hear this new explosion determined at one hundred and four come degrees. According to the rule given above, we will proceed to a regularization by a post activation of the cylinder of four came ten degrees, the difference between the degrees of these two positions, standard and projected. In doing so, it will be seen that the control of the blade must be ensured by the same mechanics as that of a post rotary blade of a machine with a triangular blade and a cylinder of two arcs, while retaining the crankpin span length of the material form. This will be confirmed by an observation, in an isolated way, of the action of the blade. Furthermore, the rotation of the cylinder makes it possible to conserve the material cylinder of the first machine.

We can therefore see that it is absolutely necessary and relevant to determine concepts capable of enabling us to account for these situations. Consequently, we will call the shape of the blades and cylinder before alteration, material form, or material figures. Furthermore, as the shape described by the blade alone allows not only to prescribe the mechanics, but also to determine the location of accessories such as candles, supply and outlet lights, we will say that the shape of the blade and visually produced cylinder will be called virtual figure or shape.

We can then give other examples which are not simple counterpart. We could for example reaHser a figure of a blade on two sides, cylinder of one, post rotary, in a retro-rotary machine of virtual cylinder on four sides, explosion every ninety degrees. A post rotary machine with a triangular blade can be set up, the explosions of which will take place every sixty degrees, thus setting up a retro-rotary machine with a virtual cylinder. six sides. We will take care to consult our patent application prior to taking into account several other examples on this subject. (Fig. 35-50)

Let us simply note here, moreover, the originality of the Clokwise movement machine from this point of view. The blade movement is effected there as if one wanted to react the explosion exactly in the same places as its counterpart not by mechanical, but rather reversive, mirror, either that of the triangular motor, or every hundred and twenty degrees. The rotation of the blade is therefore accelerated, and the rotation of the cylinder is produced accordingly.

In summary, we can therefore enact the following that any rotary-circular machine is composed of a material figuration and a virtual figuration and that the blade mechanics and the positioning of the elements and accessories can be carried out according to this virtual form.

Linked virtual figures and independent virtual figures

As we have seen, in the standard figures, with a fixed cylinder, the same blade can be activated in a cylinder on one side more, in the case of rotary machines, and on one side less, in the case of post rotary machines. The realization of a machine having both a material form and a most obvious virtuefle form therefore consists in realizing a machine of a given material cylinder and blade shape, and of a virtual cylinder shape of the opposite rotating part. For example, we can reaHser a blade machine on two sides, rotating in a material cylinder on one side, therefore post rotary, and a virtual cylinder on three sides, giving it its retro-rotating substance. It will also be possible to readjust a blade on three sides, rotating in a cylinder of two, this machine therefore being of post rotary material representation, and simultaneously a blade machine on three sides rotating in a virtual universe on four sides, recalling the rotary machine. (Fig. 35.5, 37.3)

It is important to note here that one of the originalities of the virtual-material machines consists in that in their virtual aspects, these machines are not subjected to the rules of dimensions. In fact, the machine can be made in such a way that a blade, for example on three sides, makes a virtual cylinder with four, five, six sides, and so on. (Fig. 38, 39.1, 39.2)

These possibilities will give an increased Hberté for a réaUsation of various rotary machines, since they will not be any more subjected to a rigid rule of dimensions.

In summary, the standard even blade figures lead to odd cylinder figures and vice versa. Virtual figures introduce freedom since numbers and their even or odd characters can all be used.

Material and virtual figures, versus Real Figure

Slinky movements and Real forms

The last concepts which we have just described must now be put in correspondence with the concepts of machines of compressive type and of motor type, these the latter being expressed, in rotary-circular machines under the idea that we have also commented on, of differential machines and of contrario machines.

In all the examples already given, we have only talked about machines whose next compression will occur, for standard machines on the next face of the cylinder, and for rotary-circular machines, on the next face of the virtual cylinder

This single dynamic arrangement deprives us of interesting developments. Indeed, it will be understood that the contribution of rotary-circular machines is to be able with a cylinder with a fairly low number of counties, for example a triangular blade and a cylinder on two sides, to produce a machine with a high degree of compression, and at the same time react this machine with a high number of explosions, as if it were a machine with several faces of blade and cylinder. For example, by realizing the machine with a material cylinder on two sides and a virtual cylinder on six sides, Fon obtains six compressions per revolution, whereas one would normally obtain only two.

Furthermore, as we have shown, we will have to retroactivate the blade of this machine beyond the Clokwise point of birotativity, and consequently the machine will pass, not only from post rotary to retro-rotary, but also from thrust machine standard with a simply differential thrust machine, which will further reduce the engine power, and will perform in its dynamic Compressive form.

It is therefore important to adjust the dynamics of the machine in such a way that it benefits both from its material figuration, from its virtual figuration, but also from you so that the machine not only preserves, but even increases its motor capacities. It is therefore necessary that the machine can simultaneously perform the contrario movements.

This is where the Slinky dynamics come to the rescue, which we have beforehand, shown for your piston engines. We will therefore once again use reactions from our previous corpus, however with pistons, to give an example of the next subject.

As we have already shown here, it is possible to rotate a piston machine, under the idea of a rotor cylinder machine. In the Slinky dynamics, it is a question of making work the same piston from edge to edge of the cylinder (fig.34) This type of realization is impossible in the works of the prior art, since the mechanics allowing to rehash this machine requires either a semi-transmission combined with a rectilinear action obtained by poly induction, or the recourse to polycamed gears, which will make it possible to modify the form of the induction of first degree, or even the speed of the rotor, so that induction and rotor can be combined. We will not dwell more extensively on these statements, as far as this is concerned, and we will content ourselves with mentioning that this procedure allows, compared to standard rotor cylinder machines, firstly to achieve compressions alternately on each face of the same piston, and secondly to perform compression "by jumps". the sum of all compressions is therefore done in two or more turns. (Fig. 41.1 and following) We can clearly see in the unfolding of the figures that the piston acts in the manner of a Slinky, hence the name of this machine. We can understand this solution differently by saying that compared to standard machines, we can produce successive explosions that do not correspond to material successions or virtual successions. This type of realization seems at first sight impossible in rotary machines. In fact, this type of implementation is not only possible, but also desirable.

One can indeed determine the location of new expansion at a location which is neither determined by the successive material position thereof when it is produced in its standard form, nor in the successive virtual position thereof. when we consider the next expansion. It is indeed possible, as in the case of Slinky piston engines, to produce this new compression by jumps, and to carry out subsequent sequences of these jumps which will gradually pass through all the faces of this new figure, in two, three turns. , or even more. It is from this new feçon of realizing the continuation of the compressions that we will therefore have to establish the new locations of the spark plugs, supply and exhaust systems, and this is why we will say that the figure covered by these jumps constitutes h.figure Real of the machine. We will say this figure réeHe, because it is on eHe that we will have to lean to reaHser reeHly the machine, namely, to correctly determine the locations of the candles, exhaust and fuel inlets.

Therefore we will therefore have for the machine a material figure, consisting of the figure of the side ratios of the blade and cylinder at rest, a virtual figure, which corresponds to the embodiment of the number of faces and therefore total of the machine, and the actual figure corresponding to the path traveled by the blade to completely read out this number of faeces.

It will therefore be seen that for a material figure and the same virtual figure, several real figures will be possible. If the number of faeces of the virtual figures is high, some of these real figures will perform their first compression, even non-successive, prior to the Clokwise point. The machines will therefore remain prior differentials, despite these contributions. Certain Real figures will also have their first compression beyond the standard Er of first compression. They will also remain differential, however later. . "

But what really interests us is to consider that the Heu of the first jump, of the first compression on non-successive material and virtual face will be carried out between the Heu of first compression Clokwise and the place of first standard compression. The machine will then have dynamic contrario, and therefore in its Motor form and not in its differentiated or Compressive form.

As before, for the same material figure, several virtual figures are possible, and for the same set, several real figures are possible. By way of example, we will note, for a triangular blade and cylinder figure on two sides, a virtual figure on eight sides, and a jump procedure on three sides, which will allow the blade to perform eight compressions in Slinky movement. (Fig. 42 to 49) We will take care to read more carefully our patent application filed in anticipation of this to take into account the multiple possibilities and varieties of this contribution. For the purposes of the present, it is however an absolute necessity to say why this type of figure is necessary, and to realize that the contribution of these criteria of reaHsation and distinction is essential to rotary-circular machines, This contribution is necessary since it allows to realize figures on the contrary by determining the point of next explosion of any figure, independently of its material or virtual characteristics,

This contribution will therefore make it possible, from material figures producing a good conφression, for example figures three of two, to create virtual figures producing a significant number of explosions, for example figures with eight, twelve sides, but in addition to the to make starting from a sequential figure having several Real faces, this having as a consequence that each explosion will be on the contrary, since it will not carry out the next successive explosion material or virtual, and is inside the Clokwise / standard terminals of production .

It is therefore important to note here that not only are the virtual figures independent of the dimension rules of the material figures, but moreover that the real, synthetic figures are themselves partly independent of the material and virtual figures.

Mechanical support processes

Non-clokwise circular rotary machines can be supported by the same technical procedures as clokwise moving machines. It is important here however to specify that this will have a hybrid character, which will respect both the virtual and real hardware aspects of the machine. Indeed, it is by the length of range of the crank pin or the eccentric that the material figuration will remain efficient. The mechanics chosen will include this length.

When the figures are virtueHes, but Hées, we will use the mechanics of orientational retro-rotation of the figure virtueHe. For example a post rotary figuration machine of triangular blade and cylinder in two, will have a crankpin of standard length. But if this machine has a virtual form of a retro-rotary machine with a triangular pale square cylinder, the mechanics will be of the retro-rotary type.

In the case of machines with successive compressions of the virtual figures, not in slinky, but whose number of sides of the virtual cylinder is not higher than that of the blade, an induction corresponding to the virtual figure is carried out, taking account for the differences in angulation on the sides of the material figure and those that a virtual figure should have. For example, a triangular blade figure rotating in a virtual figure of six sides will rotate twice on itself per turn. It will therefore be given a retro-rotary mechanism using an induction gear half the size of the internal support gear.

In the case of machines with a slinky contrario movement, it will be necessary, as previously, while preserving the length, to calculate the back rotation of the blade so as to achieve the desired jumps, most often achieving all of the virtual sides on more of a turn. Consequently, in the case of even virtual figures, the real figures will generally be in pairs, and conversely in the case of odd virtual figures, the real figures will be even. Vertical and figurative plans of machines and horizontal and dynamic plans of machines

We can therefore summarize the first part of our work by saying that we have exposed, so to speak, the vertical plane of the machines, in other words the ways of raising the degree of the machines by staggering or other methods of modifying cylinder, such as the use of polycamera gears.

In this work, we show the machines can be modified in their degrees, but this time in a dynamic way. We show that the Clokwise dynamics, presented in the first part has a value not only by its immense birotative qualities, but also has a systematic value since it allows to carry out a cutting between the differential machines, anterior and ^' posterior, consequently of type compressive, and contrario type machines, of which the Clokwise unit is the first representative.

So we have a vertical plane and a horizontal section of machine development. In this section, we want to add that these two planes are not incompatible, One can indeed increase figuratively the degree of a rotativo-circular machine, as one can conversely increase rotativo circularly a standard machine.

This is, for example, what is produced when the degree of a circular rotary machine with clokwise movement is increased by, for example, making an oscillating blade, by polycamed gears from one to one. (Fig. 35 a) We then figuratively increased the degree of the machine.

One can increase for example the degree of a rotary-circular machine with Clokwise movement of blade by realizing it with a cylinder not simply rotational, but this time planetary. This procedure can be very interesting, moreover, if this cylinder is bifunctional, that is to say, if it is also intended to be used as an outer blade. This will allow, in particular, the re-setting of retro-rotary machines in the clokwise way, on the contrary, this time by eccentrics on the contrary.

Counter machines: planetary cylinder / fixed blade, and Clokwise cylinder / planetary blade machines

It should be mentioned here that the forms of the machines in their inverted state, which we call counter forms are reachable, in the standard way by making the cylinder and blade in the orientation opposite to the original orientation, and by granting the cylinder , the same mechanics as the original mechanics.

For example, a triangular machine shape, is, when the cylinder is the planetary and the fixed blade, has an orientation opposite to a post rotary machine with three sides of the blade, two sides of the cylinder and uses the same mechanics as that. cl This is why, despite its shape, this machine remains post rotary. (Fig. 50)

This is also why, the rotary cylinder can both be produced in a bifunctional manner, and on its outer surface produce the blade of a standard machine. The same procedure can be performed for your rotary-circular machines, and in particular for Clokwise blade movement machines, (Fig. 56,57)

The machine can be made the machine this time with a Clokwise movement of the cylinder, orientationally opposite to its initial position, and a rotational movement of the blade. The outside surface of the cylinder can then be used as a Clokwise blade for a higher system.

Let's finish by saying that the chromatic scales already shown for standard dynamics are also true for figurative counterparts. So, we can place the machines in a series of dynamics, in double rotational at the zero point, in cylinder Clokwise, then in cylinder planetary, and to reaHser rotatvo-circular differential sets and on the contrary between these parts.

Wankle semantic gaps overcome

As we specified at the beginning of this work, Wankle effectively rationalizes the retro-rotary and post-rotary machines of the prior art, when these are made with planetary blade and fixed cylinder. For these figures, it is rather the only two mechanics that Wankle offers that are lacking, always realizing, as we have shown counter forces harmful to the motor skills of the machine. In several other places, however, this one seems to us to be mistaken by inversion or omission, semantically, which literally prevents it from systematizing the planes of the machine. We believe that all of these shortcomings are corrected here and the corrections made are part of a superior understanding of machines.

We summarize these errors in the following way A) in relation to planetary cylinder machines, H there is error of meaning and omission or contradiction of mechanization. Indeed, the correct direction of these machines is complementary to the sense of their counterpart, and the mechanics must not be that of the figure, but that of the counterpart. A correct understanding of these elements allows, as we have shown, to realize the cylinder in a bifunctional manner. B) Relative to machines with blades and rotational cylinder, the sense of this must be reversed since, according to the rule that we have given, the next expansion taking place in the same place, the blade must carry out a rotation of one hundred and twenty degrees, and the rotational cylinder must undergo a rotation of one hundred and four twenty degrees. This reorientation of the machine makes it possible to consider it as the octave machine for the chromatic scales C) The rotor cylinder machine realizes a virtual figuration blade of a machine with a square cylinder, and thereby becomes differentiated retro-rotating, which lowers the motor skills of the machine. machine. The understanding of this machine is incomplete, not only by the absence of a general rule, but also by the absence of a Clokwise movement machine, and by the absence of the establishment of virtual figures and RéeHes. Like the figures of Fixen, Cooley, and Malaird, this figure is an isolated realization, and is not systematized. In addition, as before, there is an absence of mechanization of this figure, which would have shown this retro-rotating character, and the need for semi transmission, or descending inductions. D) the ignorance of bi inductive, figurative figures, either poly turbines, and dynamic, or machines with Clokwise movement of blade or cylinder E) the absence of establishment or determination of mechanical levels of figuration or dynamics F ) the absence of mechanized accelerator-decelerative dynamics G) The absence of knowledge and the use of polycamerous gears, which allows the support of machine figures impossible at Wankle, such as different turbines, Slinky machines, blade machines and endorsed, square cylinders and so on.

Machine determinations

One of the quaHties of the advancement of any theory, science, art or language is the increase in the capacity of criteria for determining the object on which or by which eu is directed. We are gradually moving from a universe of signs to a more subtle and complex articulated language.

To keep our main examples in the arts or science, we can say for example that to analyze a phrase of the ancient melody, we needed only few criteria. This sentence was generally a psalmody with some intonations and some alternations of voice and of siïence, and with the limit some frettings. Likewise, from the point of view of harmony, women sang with an octave and it was even thought that it was the same note.

It is quite different to analyze a work by Bach, and subsequently by Beethoven, Ravel or Rachmaninov. One notes in the course of the history an increase of the musical procedures intervening in the same musical phrase, and of this feit, an explanatory rendering of this one requires the knowledge of these characters and their combination. The same is true of science. The concept of weight in ancient Greece was established by the scale. In antiquity, there were few criteria for understanding a falling body. With Newton, a weight is referred to a rational attraction. It falls not only at a certain speed, but also invariable, according to a set of criteria. With Einstein, we know that if this body is an atom, and that its speed is close to that of light, the rules of understanding will have to be widened, and widened so as to respect both these borderline cases , and to corroborate Newton's theory in non-cosmic spaces. In the same way here, if we compare Wankle's work to that of the inventors of the prior art, we see that, from this level, Wankle's contribution has been to bring new criteria rational and generative understanding of machines.

While indeed for the inventors of the prior art, each machine in its autonomous figuration, and remains without mechanical modus vivandi relative to the orientation aspect, at Wankle, we are witnessing the renunciation of rationalization criteria which are those of first-degree machine breakage and mechanization breaks.

We can therefore say that we find in Wankle the elaboration of two criteria, one of figure and the other of mechanics. The criteria of figures allows a classification into types of figures that we have called post rotary and retro rotative.

As for the criteria of orientational suspension, we see that they remain in the order of the criteria of the figures, on the one hand, namely that the proposed mechanizations are strictly retro-rotating, or post rotary, and that on the other hand, They are limited to two, either post or retro rotary mono induction, and post or retro rotary intermediate gear mechanics.

Still relative to the figures, one can, from Wankle, logically determine the figurative situation of a machine of a class to that of a machine of the same class by comparing the number of sides according to the rule of sides,

It will therefore be said that it is a 3: 2, 4: 5, 7 machine: these values correspond to the number of sides of the blades and cylinder.

Using these criteria, we can analyze standard machines. For example, in the case of commercial type engines, we will say that it is:

Motors 1) of post rotary class H) of blade characteristics of the cylinder 3: 2 I) of orientational support method by post rotary mono induction, or 'reductive

As a second example, we can assume that a machine with a blade of the same number of sides is made, but this time if the cylinder has four sides. It would therefore be a machine 1) of retro-rotary class 2) of 4: 3 side characteristics 3) of orientational support method by mono induction 4) of retro rotary or reverse type support

As we have shown, an almost unlimited number of machines can be produced which cannot be fully understood by the criteria, all in all quite limited and limiting of the prior art. We believe that a correct understanding of these machines requires a set of criteria which is sometimes much broader. These criteria are sufficient to understand some of the machines, even from the first stages. If we suppose for example a 3: 2 figuration machine, but supported by a hoop gear produced in the form of a chain, the mechanics of the machine will remain unexplained, if we only have the criteria of prior art.

We will determine the machine in the following way:

Standard cylinder blade 3: 2

Mechanical hoop gear, in its chanie form

We can also suppose the realization of a machine with compression assembly by unitary blades, in opposite direction, retro-rotating and supported by mechanical of hoop gear with third gear of deflection

We will therefore determine this machine in the following way a. retro-rotary class b. characteristic 2 X 3: 2 virtual c. internal explosion in compression lining d. hoop gear support e. bi rotary support

Let's give another example.

In this example, a triangular type machine is produced with stage support, and in addition with accelerating decelerative action of the blade. The machine is therefore characterized in the following manner

A) retro-rotary class B) degree of rotativity 2 c) in height d) support methods Mono induction master and by peripheral or secondary hoop gear 'e) domed cylinder e) mono induction by polycamera gears, accelerodecelerative f) cylinder domed in shapes and against forms

Let's give another example. In this case, we realize a machine whose compressive figure comes from our generalization of the basic Wilson figure, and whose retro-rotary mechanics with geometric addition is ours

The machine can therefore be described in the following way A) birotative class B) compressive part by structure paHque C) number of sides 6: 3 D) birotative mechanics, E) by first degree mechanics by F) modifying mechanics by and geometric addition

Let’s give one last example. It will appear here of a rotary rotary machine on the contrary, with blade and material cylinder three of two and Real cylinder of eight sides. The machine is therefore of type: a) post rotary material class b) circular rotary type on the contrary c) slinky dynamics d) material figurations 3: 2 virtueHe jump of three ReeHe 3: 8 e) mechanics by Combinatorial house by the support gear f) mechanical by semi transmission by pinion gears

As can be seen, in addition to the mechanics before the regularization structure, that is to say the mechanics by retro-rotation, there are no criteria belonging to the criteria of Wankle or his predecessors, and he could not achieve a correct rendering of this machine.

The number of example machines being partially or totally determined by criteria not belonging to the prior art is almost limited.

It is almost impossible to list all the possible machines, which cannot be described by the systemic as we can see, very limited by Wankle and his predecessors. The way to encompass all these possible machines is that of their determination from a descriptive and rational support grid for all the constitutive characters of the machines, as Wankle gave the basis, and as we have completed them. as we work.

This determination factor will only include generative criteria which can be applied to all machines, which will ensure that each of these criteria is generally necessary to consider them as such.

These criteria are: a) the class of the machine, post rotary (Wankle, Beaudoin), retro-rotating (Wankle, Beaudoin), birotating (Beaudoin) b) the number of side blades of the cylinder Retro-rotating (Wankle) post rotary (Wankle) Bi rotary Beaudoin) c) the first degree mechanics used: mono induction (Wankle) intermediate gear (Wankle) hoop gear (Beaudoin) with third gear, chain, belt (Beaudoin) - by poly induction (Beaudoin) • Semi transmission method (Beaudoin) - Hoop gear method (Beaudoin) - Intermediate gear method (Beaudoin) - Gear method heel (Beaudoin) - Method by juxtaposed internal gears (Beaudoin) - Method by superimposed internal gears (Beaudoin) - Method by post active central gears (Beaudoin) - Method by gear structure (Beaudoin) - Method by unitary gears (Beaudoin) d) the type of blade: standard (Wankle, Beaudoin. Fixen, Cooley); in a single blade and cylinder assembly (Beaudoin) in a Paque structure (Wilson, Beaudoin, St-Hilaire) e) the type of regular dynamics (Wankle Beaudoin) f) decelerative acceleration (Beaudoin) g) the degree of the machine (Beaudoin) vertical figurative (Beaudoin) dynamic (Beaudoin) Mixed (Beaudoin)

H) the type of second degree mechanics by By poly induction In double parts in tripla part (Beaudoin) inking in the points (MulHng) in triple part in descending inking, by support in positioning in the side centers, or in the intermediate parts (Beaudoin) »I) the type of corrective mechanics allowing the realization of degrees obtained: By couHsse (Beaudoin), by geometric addition (Beaudoin) by osciUement (Beaudoin), by induction staging (Beaudoin)

J) the type of machine type Planetary blade - fixed cylinder (Wankle, Beaudoin) Planetary cylinder - fixed blade (Wankle, Beaudoin) Bifunctional cylinder blade (Beaudoin) K) The dynamic type Standard (Wankle, Beaudoin) Rotativo circular differential retro (Wankle) Beaudoin) or post rotary (Beaudoin) A contrario (Beaudojn) "clokwise movement (Beaudoin) and planetary movement (Beaudoin)

L) The Material degree (Wankle, Beaudoin) Virtual (Beaudoin) Real (Beaudoin)

M) The type of compressive part with blade, (Wankle, Beaudoin) with pistons (Beaudoin) N) With slinky dynamics (Beaudoin)

O) The type of material figure used Standard figure Cooley Fixen Wankle Beaudoin) Bulging (Beaudoin), rectangularized (Beaudoin)

P) Counterpart figure Planetary cylinder / fixed blade (Beaudoin) Clokwise cylinder / rotational blade (Beaudoin) Bifunctional figure (Beaudoin)

Conclusion

At first glance, for a good number of researchers, it is obvious that Wankle's indexations, rationalizations and mistreatments are offered as an opaque, hermetic and insurmountable material. The key elements are reduced to their greatest simplicity, and we do not see that it is precisely this simplicity that is itself lacking.

As we check you frequently however, over time however, as with any theory and any system, we see one after the other errors of assessment, mechanical shortcomings and finally the rational contradictions and the various limitations of the business.

Gradually, as we will finish showing here, these gaps and their corrections will give way to new perspectives, and the exceptions will gradually show their qualities of hidden rules, generalizing so generalize that they result in new motor things, many more perfect. We can therefore proceed to rationalizations allowing to understand more machine characteristics, more machines, more mechanics, more variant of basic machines. In addition, the new units, resulting from the correction concepts will allow the realization of more reliable, more powerful, more fluid machines, and therefore, what is most important to you, privileged machine units, which we have called rotativo -circular, realizing qualities at the same time of piston machines, rotary machines and turbines, but without realizing the faults.

A bit like the musical system or the physics system, the general theory of any motor machine has not developed all at once, but rather its developmental history, which goes in unison, fifth, seventh and so on octaves, or a diatonic system gradually incorporating a chromatic system. Likewise in physics, what appeared only as exceptions in Newton's theory, turns out to be, from the point of view of cosmology, a new law.

We can therefore say that compared to Bach and Newton, we can say that Wankle laid the foundations for a first rationaHsation of rotary machines, his system, as theoretical as mechanical as it is, has several shortcomings, both mechanical and semantic. These shortcomings, overcome in a coherent manner, will make it possible to establish a larger and encompassing machine system, this system having superior figurative, mechanical and dynamic cutting criteria, more manageable and variable, from which will be able to hatch both types of more complex machines, but also, surprisingly simpler and more efficient.

The new system will not only offer more machines, but also machines with better propensity. 10) Suggest adequate segmentation of the machines 11) Suggest supports for the compressive parts by crankpins.

Brief description of the figures

Figure 1 comments on the figures of the prior art, in terms of rotary machines.

Figure 2 shows all of Wankle's first-degree methods, as well as those that we developed beforehand.

Figure 3 a) shows the main methods of mechanical degree increase as we do. have elaborated before the present.

Figure 4 recalls, also from our first part, the three main types of bi-inductive machines, namely, in a) the straight rod machine, in b) the poly turbine type machine, and in c) the blade machine in motion these / rotational cylinder.

Figure 5a shows that the thrust in the engines prior to Wankle We notice that these machines are efficient, from the point of view of the thrust, firstly because their explosion takes place at the top of the crankshaft ascent and straightening of the blade.

Figure 5b shows the two Wankle inductions, namely the induction by mono induction and the induction by intermediate gear.

FIG. 5 c shows, by way of example, the differences between engines with standard piston and with connecting rod. Figure 6 shows the details provided by the present invention relating to induction by hoop gear.

FIG. 7 shows the details provided by the present invention relating to induction by polycamed gears

FIG. 8 shows the details provided by the present invention relating to induction by semi transmission.

Figure 9 rappeUe for the two post and retro rotary base figures, the shape and torque corrections made previously by ourselves by adding degrees by staging of induction.

Figure 10 shows two types of observations leading to specific induction.

Figure li a shows the specific external observation method This method consists in observing, by an external observer, the movement of a specific point on the blade during its planetary rotation.

Figure 12.1 shows, in a), that understanding the geometrical dynamics of the blade produced by poly induction is completely contrary to that of the prior art. In b of the same figure, it can be seen that, whatever the position of the subsidiary centers of crankshafts during their total elevation, the explosive thrust on the blade remains, in spite of the poly induction in two parts, always equally distributed.

FIG. 13 shows the details provided by the present invention relating to induction by poly induction.

Figure 14 shows the dynamics for a lap of such an arrangement. Note that here the induction has been placed on the sides of the blades, but as we have said. They could be placed anywhere on the blade.

Figure 15 in a) three dynamics of different piston engines. In c), in the same figure, we see the staging dynamics that we produced in the first part of the present invention. It can be seen that the blade is not mounted on a central eccentric but rather on a crankshaft staging, the second of which plays the role of a rotating shaft.

Figure 16.1 shows how, starting from a standard piston machine, in a) one can produce between two dynamic compressive parts, here two pistons, actions in contrario in b, in the same direction, in c.

Figure 16.2 shows, from examples of machines with a piston rotor cylinder, how one can grasp the third fundamental shortcoming of the machines of the prior art, this time dynamic.

Figure 17 is a reminder of the Clokwise dynamics of a post rotary blade figuration machine with three sides and cylinder of two. Figure 18 shows by what type of observation we can see the Clokwise movement. We named this observation, observation starting from the master crankshaft of poly inductive machines.

Figure 20 summarizes the mechanical difficulties and weaknesses of standard rotary machines, resulting from the pre-stated shortcomings

Figure 21 shows that the Clokwise dynamics is midway between your standard piston, rotary, orbital and turbine dynamics and rotor cylinder. This is why they were called rotary-circular machines, or rotativo turbiniques, or finally rotary-orbital.

FIG. 22 shows that any first degree induction obtained by observation on the crankshaft, if it is carried out in a ratio of support gear and induction gear of one on one, can react the guidance in Clokwise of the blade through the center.

Figure 23 a) differentiates the rising and falling inductions. The rising inductions are standard first degree inductions, or, as we have seen in the induction stages, the edge inductions, ensuring the orientational support of the blade.

Figure 23b summarizes the two main types of semi-transmission, accelero-decelerative, and shows how to reactivate them in a combined manner.

Figure 24 summarizes the three main methods of supporting circular rotary machines. We can consider that circular circular machines are the horizontal expression of machines with stepped support structures already presented by ourselves. In b of the same figure, the induction of the blade is carried out by an induction in intermediate gear. In c of the same figure, the elements will this time be shown by the same gear, which will serve as both a dynamic support gear for the blade and a gear or induction axis for the cylinder

Figure 25 specifies the contrario movements and in the same direction for machines with Clokwise movement / rotational cylinder post rotary and retro rotary.

FIG. 26 specifies that even the birotative type machines, such as for example the polyturbines in a and in b and the Qjuasiturbines in c) are reachable in the manner of a circular rotary machine. In d), we also see that these machines are also workable for everything. number of sides. Here the rotary circular poly turbine has a six-sided structure in a triangular rotational cylinder. FIG. 27 shows that the rotary-circular dynamics can also be, from the correction mechanics already commented on by ourselves, in particular by using polycammed gears, for standard machines, be carried out in an accelero / decelerative manner. In these cases the curvatures of the cylinders will be modified.

Figure 28 shows that rotary-circular machines can be made with different types of blades. Figure 29 recalls our first dynamics on this subject and shows that Clokwise blade movement machines can have various degrees,

FIG. 30, it is shown that the polycamation of the induction or support gears can be carried out not to accelerate and decelerate the positional movement of the blade, but to alternately modify the orientational movement of the blade, thus rendering it in oscillatory Clokwise

Figure 31 shows that, as with standard machines, the machine can be made with inversion of the dynamics of the compressive parts at the periphery.

FIG. 32 shows that even inversely, the cylinder can, like the blade, be in a single multifaceted piece, in a) in several plain faceted pieces, in b) and in external paHque structure. In c)

Figure 33.1 shows the three dynamics by planetary blade / fixed cyHndre, in a, rotational blade / cylinder, in b, and clokwise blade / rotational cylinder in c)

Figure 33.2 shows that we can go further by varying the dynamics of such a way of carrying out explosions and expansion in locations different from those of the previous figures.

Figure 30 gives other examples, this time with a blade on three sides and a cyHndre of two, of the rule which we will call the rotational counterpart rule.

Figure 33.3 shows for the same material figure of a blade on three sides of two, such as shown in a) anterior differentiated dynamics in b, posterior differential dynamics in c.

Set of figures relating to rotary circular or orbital rotary machines.

Figure 33.4 shows that another dynamic is possible, and that this dynamic makes it possible to react a contrario movement of the cylinder and the compressive part, as we had previously shown for rotor cylinder machines.

Figure 34 shows what we will call the cylindrical counterpart rule.

Figure 35 shows that this counterpart rule is general, and is applicable regardless of the time of a new projected explosion

Figure 35.4 gives a first example of a more complete dynamic making it possible to reveal these figures which one will name, as opposed to the so-called material figures, the virtual figures

Figure 35.5 gives a second example of a material and virtual figure. Figure 35.6 shows the rest of the positions of a Clokwise movement machine. As you can see, the origin of this type of machine is to describe a limit point between two areas of the chromatic range of rotary machines.

Figure 36 shows that we can conversely reduce the number of sides of the virtual figure compared to the standard figure, which implies, insofar as the compressions will be successive, that we will achieve a different virtual shape later.

Figure 37.1 shows that consequently we can by adding or subtracting on one side the virtual cylinder, transfer a post rotary machine, into a retro-rotary machine and vice versa

Figure 37.2 shows that this is true for all forms of figures. Here we have, by way of example, in a, a triangular blade machine, in b a square blade machine, in c) a five blade machine.

Figure 37.3 shows that the realizations of synthetic figures are as true for retro rotary as post rotary machines.

FIG. 38 shows that the realizations, for the same material figure, of virtual figures are not limited to the figures with a number of sides less than or greater than one.

Figure 39.1 shows that in reality, you can reaHser, for the same material figure, all your basic geometric figures as virtual figures.

Figure 39.2 shows that this is true for all the figures, and gives the example of a post rotary material figure with square blade.

Figure 40 shows that one can realize the virtual cylinder of a machine by réaHsation of each face of the latter in a non-successive manner, by jumps.

For example, for a triangular blade machine of the post-rotary type, it is possible to realign this machine by locating each compression by jumping from eluded faeces

Figure 40.1 gives the following, for one turn <of all the blade compression and expansion positions. It is important here to make the following few comments. .

Figure 41.1 recalls the dynamic slinky for a rotor cylinder machine, this dynamic realizing a jump race of the parts.

Figure 41 2 shows that, since the races of non-successive faeces are possible, the sequences of synthetic races, which we will also call real races, are multiple for the same virtual figure.

The figure 42.1 thus widens the rule of construction of the rotativity of the cylinder by deciding that one must take into account not the figure virtueHe, but well the virtueHe race of réaHsation of this figure. Figure 42.2 realizes a synthetic, real, non-successive race, the jumps of which are made in such a way as to be located in the contrario area of the machine. Here, we therefore erect a virtual fece with each compression.

Figure 42, 3 shows the same real and virtual forms, but, again with a different synthetic race. Here, the jump is two so the sequence is as follows, 1: 1, IN: 2, H: 3, N 4, III 5

Figure 43 summarizes the previous three figures and concisely puts He in the synthetic race and the belonging of a réaHsation to one area or another. .

Figure 44 shows that certain figures, the number of sides of which is even and quite low, lead to lower figures.

Figure 45 shows various real strokes of a virtual figure of seven sides for a post rotary material figure of a three-sided blade. One can find there, from one to seven for each figure, the continuation of the cuts.

Figure 46 shows various real strokes of a virtual figure of eight sides for a post rotary material figure of a three-sided blade.

Figure 47.1 shows that the more the number of sides increases, the more the number of possible races increases, and consequently of contrario races.

Figure 47.2 recalls that each material blade figure has its specific area and that the more sides the blade has, the smaller the area on the contrary.

Figure 48.1 summarizes the last figures, and shows, in a single figure that several virtual figures are possible for the same material figure, and that several synthetic strokes are possible for each virtual figure.

The figure 48.2 shows, for a turn, this time, a post rotary material figure of four of three sides of blade and cylinder, carried out on a virtual structure of. ten sides.

Figure 49.1 shows, conversely, that several material figures are possible for the same virtual figure, and that each will have a preferable area.

Figure 49.2 shows the chromatic scale of a material figure machine with a blade on three sides and a cylinder with two. We can see the anterior differential areas there, realizing when the explosion occurs before the clokwise moment of the machine.

Figure 50.1 shows the specifics of the mechanics of these machines.

Figure 50.2 shows, as with standard machines, clokwise machines can not only be done in reverse fashion, but also in a bi-functional fashion. Figure 50.3 distinguishes, for all the realizations, your retro-rotary differential, post-rotary and conversely differential chromatic ranges for a machine that is itself virtual.

FIG. 51 shows the qualities of a machine with a virtual cylinder in eight and a jump of two, consequently of movement in contrast.

Figure 52 summarizes the four possible types of mechanization for circular rotary machines: Either: a) by real mechanics of the virtual movement of the blade by semi-tranmittive mechanics of the rptational cylinder b) by real mechanics of the virtual movement of the blades by mechanics downward rotation of the cylinder c) by semi transmittive mechanics of the blade by semi ttansmittive mechanics combined with the cyHndre d) by semi transmittive mechanics of the blade by descending mechanics of the rotational cyHndre

Figure 53 shows that each of these mechanical and semi transmission can be standard, or poly inductive type.

FIG. 54 shows that the efficiency of differential piston machines can be increased by realizing them with rotor cylinders or the perforated upper pistons.

FIG. 55 is an example of mechanization of a circular rotary machine in which a poly inductive semi transmission in a is used, and a mono inductive downward induction in b

Figure 56 shows some other combinations, among the hundreds possible.

Figure 57 shows that the clokwise movement is also possible peripherally.

FIG. 58 shows that the clokwiuse movement can be carried out in a bifunctional manner, the external cylinder and the internal sub-blade being strictly rotational, and the blade in clokwise movement.

Figure 59 shows in a that one can reaHser in a simplified way the segmentation of rotary machines by the use of U-shaped segments. In b of the same figure, one shows how to reaHser the machine with the use of a crankshaft rather than an eccentric. In c of the same figure, it is shown that the rotational blade of machines with a clokwise movement cylinder can be realized by constructing it in the manner of a turbine blade. Figure 60 shows three other additional mechanical combinations

Figure 62 shows, in addition to the mechanical shortcomings already stated, your semantic shortcomings overcome by our work in relation to planetary cylinder inachines. There is an error in meaning and an omission or contradiction in mechanization.

Detailed description of the figures

Figure 1 a) shows the main retro-rotating figures of machines of the prior art, in particular of Cootey. In 1 b, we see the work of Wankle, Herman, Fixen, who mainly carried out a modification of the basic forms of your way of making the machines with a segmentation this time on the blades 1, as opposed to a segmentation on your cyHndre 2, as in the machines of the prior art. In b) of the same figure, we see the post rotary figures of the art prior to Wankle, eHes also segmented on the cylinders. In the second part of b), we see the figures of Wankle and Fixen, in which, as in a 2) the latter have rather arranged the segments on the blades. In 1 c, We see the two unique Wankle mechanics for planetary vane machines, namely by mono induction 3 and by intermediate gear 4 In 1, d), we see the only dynamic variant for which Wankle has supplied with mechanical support. In e) we show the two compressive structures of the prior art, after Wankle. These are the Wilson 5 Polyturbine and the St-HHaire 6 Quasiturbine

Figure 2 shows all of Wankle's first-degree methods, as well as those that we developed beforehand. In 7, we find the method by mono induction of Wankle, in 8 the method by poly induction in double part, in 9, the method by semi transmission, in 10, the method by hoop gear, in 11, the method by internal gear stages, at 12, the Wankle intermediate gear method, at 13, the juxtaposed internal gear method, at 14, the intermediate gear internal gear method, at 15 the unitary gear method, at 16, the heel gear method, in 17, the central dynamic gear method, in 18 the gear structure method.

These methods have all already been commented on by us even before the present. We recall them because they will enter into composition with other methods to support the compressive parts of the machines disclosed herein.

Figure 3 a) shows the main methods of mechanical degree increase that we developed before the present. It is the method by staged combination of central and peripheral inductions, 19, the polycamed gear method, 20 the geometric addition method 21, the semi transmittive poly induction method, 22 the poly method crank pins 23.

In b of the same figure, it is simply recalled that these methods generally result in an increase in torque and an improvement in the curvature of the figures of the machines, 24, 25. In c of the same figure, we recall your generalizations of sides that we have produced for machines with palic structure, namely your Polyturbines. .

By these processes of increasing degrees by modifying the couse of the blades, we have shown that we could increase the compression of the retro-rotary machines, the torque of the post-rotary machines. We have also shown that we could realize rotary irachines of In various degrees, these machines, for example poly turbines, producing new, more subtle and sustained cyhndre shapes increasing the number of induction. We have shown that one could produce, with the use of polycamed gears, accelero-decelerative actions of the compressive parts, thereby increasing their oscUlatory effect, and thus improving the stroke of the compressive parts and the shape of the cylinders relating thereto. . We have shown the rules for combining mechanics in stages. We have generalized the cylinder shapes of poly turbines. We have shown the effects of poly crankpins on rotary machines. We have shown that the machines could be built by sets of unitary blades, standard polyface blades, Easter structures. We showed the perfectly birotative dynamics of blade in Clokwise movement, and the rotational-circular dynamics that this movement implied.

FIG. 4 recalls, also from our first part, the three main types of bi-inductive machines, namely, in a) the rectiHgne bieUe machine, in b) the poly turbine type machine, and in c) the vane machine in motion these / rotational cUindre.

Figure 5a shows that the thrust in the engines prior to Wankle We notice that these machines are efficient, from the point of view of the thrust, firstly because their explosion takes place at the top of the crankshaft rise and straightening of the blade. 25. Secondly, we note that the downward thrust on the blade 26 takes place with an arming of this one to the cylinder, this arming making it possible to achieve, so to speak, a lever effect.

In addition, it is precisely this armament that will have been the cause of premature wear of the segments, and this is why Wankle will have implemented two blade support methods making segmentation possible on this one.

FIG. 5 b shows your two Wankle inductions, namely the induction by mono induction and the induction by intermediate gear. We will explain more abundantly, during the present disclosure, the fundamental shortcomings which contributed to the mechanical deficiencies of these inductions. For the moment let us simply mention that each of them produces a high proportion of counter pushes harmful to the motricity of the machine. In the mono induction method, while the explosive thrust on the front of the blade achieves motricity, 29, the thrust on the rear part of the blade produces a counterforce 30, reducing the motricity of the machine.

In mechanics by intermediate gear on the contrary, the thrust in the direction of rotation is reacted by the rear part of the blade, 31 and the negative thrust is produced on the front part. 32. FIG. 5 c shows, by way of example, the differences between the standard piston 33 and the sliding twin 34 motors. Whereas in the first case, in the course of the descent, inking the piston on the cylinder 35 is produced, what U is common to call the rod effect, we see that by the use of a rod of the slide type, we lower the number of constituent parts of the machine, and the we lose the so-called connecting rod effect. In both cases, it can be seen that a first major shortcoming of the two Wankle mecanisms consists in the fact that this one, by moving the anchor of the machine, was to lose the peripheral anchor at the origin the leverage of the explosion surge over the entire surface of the blade. .

Figure 6 shows the details provided by the present invention relating to induction by hoop gear. In a, we find the hoop gear mechanism in its original form. An external type induction gear 36 is rigidly fixed to the center, of the blade, and a support gear, also of external type 37, is rigidly fixed to the body of the machine. A hoop gear 38 is rotatably planetary mounted to the support gear such that it is both coupled to the induction gear. The rotation of the hoop gear, during rotation, causes the rotation of the blade.

In b), it can be seen that a third tension gear 39 has been added, which allows both offset of the attack of the hoop gear on the induction gear, and also a more powerful rope effect, preventing the push before turning into a retro rotation.

In c), the hoop gear is made in the form of a chain.40 The front thrust on the blade is again transformed into a rope effect 41, which causes the post rotation of the blade, in addition to the rear thrust . Contrary to Wankle's inductions, the two surges are therefore positive.

In d), the chain is produced in the form of a belt 42 and produces the same effects.

FIG. 7 shows the details provided by the present invention relating to induction by polycamed gears As we have already commented on several occasions, the polycamed gears 43 make it possible to produce several machines requiring acceleration and deceleration of the parts. The present simply has the effect of mentioning that the rotation of gears, round, or themselves polycamed, with teeth at variable distances from the teeth 44 may produce the same accelero-decelerative effects.

FIG. 8 shows the details provided by the present invention relating to induction by semi transmission. It is simply a matter of adding that semi transmission applies to all forms of rotary machines, including explosion machines at the top of the blade straightening, and to all induction.

In these cases, the thrust on the active support gear 45 is in straight Kgne with the drive of the machine, and is added to the thrust on the eccentric

Figure 9 rappeUe for the two post and retro rotary base figures, the shape and torque corrections made previously by ourselves by adding degrees by staging of induction. It is clear that the induction stage, from a 1 to a 2, has enabled a much better compression capacity 46. By authors of b 1 to b 2, we see that the position of the master and subsidiary crankshafts is much more favorable to a systemic deconstruction 47. The figure also shows in c that The application of polycammed gears to figurations whose segmentation is located in the cylinder corners allows a softening of the blades and an improvement of the longevity of the segments. We will consult, at the end of this presentation the segmentation proposals that we present.

Figure 10 shows two types of observations leading to specific induction. In the first type of observation, in a) that we will laugh from the comparative outside, the observer, positioned outside the machine, 49 is able to note that what defines post rotary machines is that in this latter the blade travels in the same direction as the crankshaft, but at reduced speed 50, while what is defined as the rotary machine consists in that the blade travels in the opposite direction of its crankshaft. 51 It is from this type of observation that the mono induction method may have been constructed.

In b) of the same figure, shows Y observation by the crankshaft. In this type of observation, the observation can be produced from an observer, this time positioned on the eccentric of the machine 52, will note that, whether the machine is post rotary, or retro-rotating, the blade always has a retro-rotating action with respect to that of the crankshaft 53, and that what differentiates the machines, from this point of view, is a difference in degree, in that the retro-rotation of the retro-rotating machine is more accentuated 54.

It is from this type of observation that all the methods in which the induction of the blade can be carried out with a view to carrying out a retro induction with respect to that of the crankshaft can be carried out.

Figure li a shows the specific outside observation method This method consists in observing, by an external observer, 55, the movement of a specific point on the blade during planetary rotation of the latter. This type of observation is the basis for understanding the poly induction method. In a) we can see that any point located on a line starting from the center of the blade at one of its ends 56, realizes a similar race to that of the blade, and slightly more obtuse. 57. by authors, if the point chosen is located on the Hgne starting from the center and the reKant at the center of one of the sides, 58, the race carried out will be similar to the first, but in the opposite direction to this one 59.

Furthermore, if the point chosen is located in an intermediate space between these two lines, either posteriorly 60 or previously, 61, the shape produced by these points will be as similar to the first, but this time in half orientational path between the first, either posteriorly 62, or anteriorly 63.

During these observations, one will moreover observe a constant between the reaHsation of these curvatures, and this despite their totally different specific orientations. If we indeed draw a Hgne between the lowest point of one of the figures, at y and the highest point you of the other figure x, and that we follow pale the sequence of these figures, we will see that the displacement of these points forming a Hgne will be equidistant. Throughout the creation of additional figures. It will subsequently be possible to rehase, as shown in e), a poly induction with two parts, in lacquering of the secondary crankshafts 64, are rotatably mounted on a master crankshaft 65, their crankpins being initially disposed of you. ways of realizing these complementary forms. These subsidiary crankshafts will support the compressive parts. More details of these statements can be found in our Russian Patent Poly-Induction Energy Machines, Number 200200979, May 14, 2001.

Figure 12.1 shows, in a), that the understanding of the geometrical dynamics of the blade produced by poly induction is completely contrary to that of the prior art. Indeed, at a 1, we can see that we can express the geometric dynamics of the prior art, by saying that the shape d of the sought-after cylinder is reacted from a rapid geometric circular movement 66, produced by the central eccentric and by the réaHsation on the periphery, of a circular rotary movement, 67, produced by the blade. The final form is therefore subtractive, since the upper movement is negative, and subtracts from the speed of the central movement. This is the first fundamental shortcoming of Wankle and his predecessors. In poly induction, the dynamic reaction of the projected shape 69 is on the contrary produced by a slow movement in the center 70, and by a rapid and accelerated movement in the periphery 71. The form is therefore created from the addition of these two positive movements, hence the power of the machine.

In b of the same figure, it can be seen that, whatever the position of the subsidiary centers of crankshafts during their total elevation, the explosive thrust on the blade remains, in spite of the poly induction in two parts, always equally distributed. Indeed, when the line formed by the two crankshafts is perpendicular to the explosion, 72, the blade is also divided, 73 of course. Likewise, when these are angularly arranged, 74 the blade is still equally divided, since the front and rear parts are equal 75, and the central part is well centered 76.

FIG. 13 shows the details provided by the present invention relating to induction by poly induction. In a) it is shown that poly induction can be carried out by any induction, each induction being carried out in a post-rotary fashion. In the example given in a) the induction of the subsidiary crankshafts are actuated by induction by hoop gear. 77

In double induction poly induction, we supported the idea that stopping the previous induction during descent produced an arming of descent. Finally, it is shown that poly induction can be carried out in three parts while retaining the descending anchorage by positioning the support points in the sides, 78. Each crankshaft will therefore carry out a vertical cyHndre stroke 79.

In c, the position of the support points is both in intermediate zones 80 and, moreover, carried out in such a way that during the explosion, two of the crankshafts are perpendicular to the attack 81. One of the three crankshafts will therefore always be partly subtracted from neutral, the neutral being divided between your two perpendicular crankshafts. It should moreover be noted that the displacement of the crankshafts will be obHque 82 and the inking will be in part a descent inking and is diagonal 83.

In d), it is shown that it is simultaneously possible to react the double and triple part poly induction by reacting the inductions in an alternative manner. In this type of induction, certain teeth are partially or totally cut off from the support gear 84, or from the induction gears, so that except for the transition periods of the effective inductions, only two out of three inductions work. Consequently, the hinge effect around an anchoring point, specific to double-induction poly induction is ensured here, in an evenly distributed manner for all of your blade feces. When realizing k power, the inductions will therefore be in double part, and the more negative induction k will be neutralized. This induction will be actuated not by the crankshafts, but by its simple connection to the blade.

Figure 14 shows k dynamic for a lap, of such an arrangement. Note that here the induction has been placed in the sides of the blades 85, but as we said. They could be placed anywhere on the blade. It will be noted in addition that, as for all our inductions, this type of mechanics is valid for all, figure, rotary, and for all dynamics, like for example dynamics with planetary cylinder and rotativo-circular.

In this figure we notice that, as we said above, the teeth of the support gear have been partially cut off 86. Consequently, except in the transitional periods 87 only two inductions work 88. Consequently, k power does not simply result from k rotation of the subsidiary crankshafts, but is also constructed from the rotation of one assembly around the other, in partial stop 89. Consequently, a mega-rotation takes place around this center point, which is called descending armament, and produces mega energy. This is what we call the Slinky movement. The interest of k present specification consists in constructing an identical descent for each part of k blade. We therefore see, following k figures that U occurs a relay between active and passive inductions.

Figure 15 in a) three dynamics of different piston engines. In a 1) we find k standard dynamics. In a 2) we find k orbital-type dynamics and in a3) k rotor cylinder dynamics of our Canadian patent for this purpose titled Energy machine II. In the first dynamic, we find your three constituent elements of any machine when we hear k reacting under its so-called motor form, that is the compressive part 90, here produced in the form of a piston and a cyHndre , k transmitting Hgatrice part 91, here réaHsée in the form of a connecting rod, and finally the mechanical part, carried out in the form of the crankshaft. 92 In k dynamic known as orbital, the arrangement of several of these systems is different, since they are not on k same Hgne, but rather arranged in periphery. However, each system is complete, and includes all the elements already described. 90,91,92. In the rotor cylinder machine, however, the crankshaft is no longer active. The latter has in fact been dissected, and only its crankpin is made in a non-dynamic manner by an off-center fixed axis rigidly disposed in the side of the block. 100. Unlike the orbital engine, the general cylinder of this machine is rotatably rotated 101 about a central axis 102. Pistons and cylinders therefore travel through different circumferences 103, which provide the expansions and compressions.

From the point of view of the constitution of the elements, it can therefore be seen that k reaHsation of the crankshaft of the previous examples was made in a confused manner with another element, here, the cylinder. There has therefore been a deportation of k central position thereof which results in a great loss of energy.

In c), of k same figure, we see k dynamic by staging that we produced in the first part of k present invention. We see that k pale is not mounted on a central eccentric but rather on a crankshaft staging, the second of which acts as a rotating rod.

All of these examples, in addition to the examples by poly induction already discussed in the previous figures, lead us to point the finger at the fundamental seconds of Wankle and his predecessors, which consists in having unwittingly moved the crankshaft subsidiary from the periphery to the center, and to have produced the central crankshaft, as in the above-mentioned example, in a manner confused with a peripheral element, namely the blade, which constitutes the second fundamental shortcoming of these machines.

Figure 16.1 shows how, starting from a standard piston machine, in a) one can produce between two dynamic compressive parts, here two pistons, actions in contrario in b, in the same direction, in c. To rehase the contrario machines, a crankshaft is used, coupled to pistons mounted one inside the other, the crank bearings of which will be located in opposite parts. The pistons will therefore have an opposite action. Conversely, if we have the crankpins in the same dial and this with different length spans, as shown in c, we will simply react a differential action between the pistons.

FIG. 16.2 shows, from examples of machines with a “piston rotor cylinder”, how one can grasp the third fundamental shortcoming of the machines of the prior art, this time dynamic. As we have seen in the example of a rotor cylinder machine mentioned above, we completely subtracted the action of the crankshaft. In our patent application, simple induction machine, we showed that we could revitalize it, either retro-rotatively , or post rotationally, and thus produce expansions and compressions at a rate greater than one per all per cylinder.

At a of k this figure we thus find k basic arrangement, without dynamics of crankshaft already exposed. In b, of k same figure, it is supposed that the crankshaft 104is reinserted in k figure, while preserving the rotational movement of the cylinder 105. It is supposed that the crankshaft acts in retro-rotation 106. One will thus note an expansion faster compressive parts, and a contrario action of the mechanical parts which will increase k power of k nmchine. In c), of the same figure, we suppose that this cylinder has closed chambers. In addition, it is assumed on the contrary that the crankshaft is driven in the same direction as that of the cylinder, and moreover, but at accelerated speed 107, which will also produce expansions and compressions. This will be seen when the crankshaft acts more quickly and joins the next expansion 108, as in the rotary engine, U joins the next fece 109.

It will be noted that, on the contrary, that on the contrary, this dynamic is only differentiated, since the force on the crankshaft is therefore built by pressing on a part from a part. This very clearly constitutes the third Wankle gap, the third fundamental gap, which consists in having performed a simply differentiated action between the crankshaft and the blade. As we have already shown, the birotative dynamics, by staging of inductions and by poly induction do not address these gaps. In the next figures, we will show that the birotative dynamic by compressive part in Clokwise movement also realizes the machines without these three fundamental gaps. FIG. 17 is a reminder of the dynamic Clokwise 110 of a post rotary blade figuration machine with three sides and cyHndre of two. In this dynamic we suppose a very specific blade movement in that its orientation aspect remains unchanged, observed from the outside during k rotation of its center, and that consequently, as for the hands of a watch, despite movement of the hands, the orientation of the numbers does not change. This is why we named this payroll movement Clokwise movement.

In a machine, if a blade is produced with this type of movement, the cylinder will have to be made in a rotational fashion 112, and in the more specific case of post-rotary machines, so as to contrast the circular movement with center of k pale.

Figure 1b shows by what type of observation we can see the Clokwise movement. We named this observation, observation starting from the master crankshaft of poly inductive machines. This type of observation was obviously not possible for the inventors of the prior art. In this type of observation, an observer is supposed to be placed on the master crankshaft 113 of a poly induction machine. This crankshaft as its stability frame, it will note the following. First of all he will observe the Clokwise movement of the blades that U observes, and that each part of it performs a strictly circular, not rotational, movement. 114. Secondly, when he observes the cylinder, it will no longer be for him, as for a fixed external observer, but rather in movement, and read precisely in reverse movement to that of the Clokwise movement of pale.

The Clokwise rotaivocular movement can also be carried out mechanically and constructively by gripping the master crankshaft of a poly inductive machine in a vice 115 and activating the rest of the machine. Therefore, in fact, if we turn the assembly, we will see that the subsidiary crankshafts can still be activated and therefore produce the Clokwise movement of the blade, 116, and that the support gear, preakably non-dynamic will activate, causing the cylinder to rotate with it. 117. It is therefore possible, by this stratagem, to observe from the outside a perfect rotary-circular machine of the blade type in Clokwise.

Figure 19 b) shows, as a deduction from k previous experience, k basic mechanics used to concretely re-support the support of k machine in Clokwise. It is a poly induction so to speak dynamically reversed. One simply rotates two subsidiary crankshafts 118 fitted with support and induction gears 119 in the side of k

Machine. The blade 119 is installed on the crankpin of these crankshafts. A k axis 120 of the machine 120 is then rotatably mounted in k machine to which the Hen gear is joined, joining the crankshaft gears 121 and the cylinder 122. The Clokwise movement of the blade will therefore cause k back rotation of the 'central gear and consequently the cylinder.

FIG. 20 summarizes the mechanical difficulties and weaknesses of standard rotary machines, consequent on the shortcomings pre-stated in a), and shows that all these difficulties and shortcomings are overcome in the Clokwise arrangement. The theoretical shortcomings mentioned above result in very real difficulties, the main ones of which are as follows: a) a negative counter force on the rear part of the blade during the descent 123 b) an uneven speed of systemic deconstruction 124 c) over-control of the crankshaft, a third of a turn of the blade, requiring a full turn of the latter 125 d) increased friction in derotation of the k blade on its crankshaft, 126 caused by the use of an eccentric

In summary, therefore, k blade works positively only over a part of its length, and this work remains unevenly distributed. In addition, this work carries out a work whose k resulting force is reduced by k speed of the crankshaft and k great friction.

The machine is not very efficient. In the dynamic with clokwise / rotational cylinder blade All these gaps are cut off and replaced by quantities.

We note: a) a power over any length of k blade 127 b) a descending speed equal at all points 128 c) a significant decrease in the over-command of the crankshaft: a number of three explosions per revolution of the crankshaft by opposition with two 129 d) a rod effect found by the turbine thrust on the cylinder 130 e) a systemic deconstruction on the contrary between the cylinder and the blade 131 f) the absence of any acceleration and deceleration of any part 132 g) the cylinder rotational can be fitted with a blade and ensures the cooling and reactivation of the machine's dynamic light valves.

Figure 21 shows that k Clokwise dynamics is midway between standard piston, rotary, orbital and turbine dynamics and rotor cylinder. This is why they were called rotary-circular machines, or rotativo turbiniques, or finally rotary-orbital.

First of all, note that your rotary rotary blade engines in Clokwise have a frank and equal thrust on the blade, not only sembkble, corn even equal to that of piston engines 133. Next, it must be said that these machines derive their geometric figuration from the rotary machines of the prior art 134. It should then be added that these machines, unless they are produced on purpose with polycammed gears, have, like your turbines, no acceleration or deceleration of both mechanical and compressive parts, 136. Then, as in the counter-rotor rotor cylinder machines, the induction combination was made the crankshaft horizontally, which implies that the crankshaft was not placed at the periphery, but centrally but also that the parts are conversely, 137. Finally, the descent of the piston is fairly vertical and peripheral, and recalls that of the orbital motors in a single blade 138.

Im, / It is almost true to say that this new machine has the qualities of all these machines combined without having the respective faults.

FIG. 22 shows that any induction of first degree obtained by observation on the crankshaft, if it is carried out in a ratio of support gear and induction gear of one on one, can carry out the guidance in Clokwise of the blade by the center. In a 1, a 2, a 3, there are respectively first-of-gear induction by intermediate gear, by hoop gear, by heel gear, all mounted with gear ratios of one on one. This gear ratio clearly shows, in addition to the perfectly equal action on each part of k blade, the birotative aspect of blade machines in Clokwise, an aspect which is found, in other figurative forms, only in poly turbines, and in straight-line motors.

In 22 b, we show that your mono induction, or poly induction induction must, like any induction from which you would not have changed the gear ratio, to be carried out in their semi transmittive form 139, in a manner of their subtract their propensity either retro-rotating or post-rotating.

Figure 23 a) differentiates the rising and falling inductions. The rising inductions are standard first degree inductions, or, as we have seen in the induction stages, the edge inductions, ensuring the orientational support of the blade. As we can see here, in 140, there is a rising induction of the mono induction type. We define an induction as descending when it on the contrary of an element on the periphery to activate a lower or central element In these cases, it is the upper gear, most often of blade which becomes the gear of support of induction 141, while the lower gear, most often of the central axis is the induction gear 142 of this axis and of the elements, commonly the cylinder which are attached to it. In this figure, for the sake of simplification, the downward induction is also a mono induction induction, but it could be a poly induction, a hoop gear induction or any other induction.

Figure 23 b 1) summarizes the two main types of semi-transmission, accelero-decelerative, and in b 2 shows how to achieve them in the same way.

One can react acceleration or deceleration of parts by semi transmission transmitted with the help of an internal and external gear 143, or even by the coupling of two gears to a double gear 144 of different sizes. In addition, the reversal can be carried out either by pinion gears 145 or by a combination of external gears 146.

As these two mechanical actions will frequently be necessary in rotary-circular machines, it will be advantageous to react these reverse-accelerating semi-transmissions together, such as in b 1, or even in b2.

Figure 24 summarizes the three main methods of supporting circular rotary machines. We can consider that circular rotary machines are the horizontal expression of machines with stepped support structures already presented by ourselves. Therefore one To achieve them, there will always be a need for two inductions in combination, very often one of a semi transmittive type. We therefore define semi transmission as inductions transferred to eHes themselves, from center to center. It will have been understood, awaiting the number c of the first degree induction that we have provided, and the number of semi transmittive induction, that the possible permutations are vast and cannot be presented here. This is why we will give the generating rules for combining these inductions.

The logic of these rules is as follows. It will be understood that one of the inductions will control the rotation of the cylinder and the other the Clokwise or planetary movement of the blade, and that consequently these two inductions must be perfectly synchronized. They must therefore communicate by a third party, will allow coordination. The support methods, uplink, downlink or transmission may be semi réaHsées by a part common ^• either by k blade vUebrequin you, support the gear. In k part a) of this figure, we therefore find an example of the first type of combination. On one side, the blade is supported by a hoop gear method, one on one ratio ensuring the Clokwise movement, By the way, on its second part, it is provided with a descending induction ensuring the rotation of the axis of the cylinder. The two systems are therefore combined by k pale.

In b of k same figure, the induction of k blade is carried out by an induction in intermediate gear. EU communicates with the crankshaft, by the way, from this same element, we attach a semi transmission which will rotate the cylinder. Blade and cylinder will therefore be converging because coupled to the same element that is the crankshaft.

In c of k same figure, the elements will this time be connected by the same gear, which will serve k times as a dynamic support gear with a blade and as gear or axis of induction to the cylinder. Indeed, we can see that k blade is activated by a semi transmittive mechanism, and that its support gear is dynamic. By authors, if we realize k reverse rotation of the cyHndre, starting from the crankshaft, we can use a reverse semi transmission, realized in a totally confused with k first, which allows to say that the gear cylinder is an induction gear, is the same gear as the dynamic blade gear.

We now understand better the advantage of mounting by poly induction presented in our first mounting figures. In this setting, the rising induction of the blade is exactly the same, in the opposite direction as the semi transmittive and reverse induction of the cylinder, which makes the number of parts very limited. There are others at the end of this talk. examples of combinations which all respect the same underlying assoc tive idea, namely that the inductive parts are necessarily determined by one or the other of the mechanical components of the machine, blade, crankshaft or support gear.

Figure 25 specifies the contrario movements and in the same direction for the machines with Clokwise / rotary rotary rotary and retro rotary movement. Likewise it shows that blade movement machines in Clokwise are feasible for any machine figure In a) we have the post rotary blade figuration machine in three sides, cyHndre in two.

In b) we find k triangukire retro-rotary machine. It is noted that in the case of rotary machines, the cylinder remains rotational, but works on the same side as the movement.

Clokwise blade.

Figure c) shows a Clokwise movement of the blade from four sides and rotational to the opposite of the cylinder in three

Figure d) shows a Clokwise blade machine on three sides, but this time in a cylinder of four, therefore of retro-rotary figuration. Cylinder and blade therefore work in the same direction.

In e) we see a post rotary rotary blade figure in Clokwise from five sides, and a moving cylinder in contrast from four sides.

In f), a retro-rotating figure with movements in the same direction, of Clokwise blade on four sides, cylinder of five.

Figure 26 specifies that even the birotative type machines, as for example the polyturbines in a and in b and the Quasiturbines, in c) can be made in the manner of a rotary rotary machine. In d), we also see that these machines are also reachable for any number of sides. Here the rotativo-circular poly turbine has a six-sided palic structure in a triangular rotary cyHndre.

In addition, if we observe the sequences present in a) and b), it will be noted that, as for standard machines, various levels of rotativity can intervene for the same inachine. In a), the structure is not rotational, it simply realizes its losango squareoid alternately, and is completed by rotation of the cylinder.

In b, we will note your two crankshafts supporting the paHque structure are strictly rotational, which forces the reacation of the losango-square alternating passage of k pale structure to reachase through a certain rotation, not planetary however. This rotation is completed by k rotation of the cyHndre. I

Figure 27 shows that the rotary-circukires dynamics can eUes also, from the correction mechanics already commented by ourselves, in particular by the use of polycamed gears, for the standard machines, to be carried out in acceleration / decelerative manner. In these cases the curvatures of the cylinders will be modified.

Figure 28 shows that rotary-circulating machines can be made with different types of blades. In a), we find the standard blade figures.

In b) the compressive structure consists of unitary blades with Clokwise movement acting in combination with the cylinder to form compression either between them and the outside, or between them and the cyndre at the center of the machine. In the latter case, the compression achieved by this assembly will be double the normal compressions and the machine will consequently be able to establish diesel gas management. In c), it is simply a matter of recalling that k compression structure can also be of PaHque structure, as shown in the previous figure.

Figure 29 recalls our first dynamics on this subject and shows that Clokwise blade movement machines can have various degrees,

In a) the blade without orientational action, and consequently has a clokwise movement, the positional action of the latter being circular. In b) k pale has a Clokwise and rectilinear positional action, In c) it has a Clokwise and almost triangular positional action. Finally in d) its orientational action remains Clokwise, but its positional action, since the crankshaft is more elongated, is coupled not to a simply rotational cylinder action, but to a planetary cylinder action.

All these machines are therefore the same generation of machine, sometimes increased by degree by k rectUignisation or geometrization here, by triangularization of k positional stroke of the blade, such as in b and c, sometimes by an increase in the degree of the cylinder .

All of these dynamics of different degrees, shows that circular rotary machines form a category of machines with generative characteristics of their own. In all these machine cases, the master crankshaft is the same as the cylinder.

In k figure 30, it is shown that k polycamation of the induction or support gears, can be carried out not to accelerate and decelerate the positional movement of the blade, but to alternately modify the orientational movement of k blade, k rendering thus in Clokwise oscUlatoire. This is possible by a relation of support and induction gears always in a ratio of one on one but, this time, of polycamed nature.

Furthermore, in this figure, it is shown that it is possible, by set of unitary blades, to achieve the compression of machmes with odd cylinders. Here, while one of the blades is in compression, the other will be in depression. Note also the opposite oscillating action of the blades.

Figure 31 shows that as for the. standard machines, we can realize k machine with inversion of k dynamic of the compressive parts center periphery. Consequently, here it will be the cylinder will be in Clokwise movement and k blade in rotational movement. It should be noted that, as we will show more abundantly at the end of the present invention, the orientation of the parts will be complementary and that k mechanical will be that of the material counterpart.

A second consequence of this inversion will be that the post rotary figures thus produced, in addition to requiring retro-rotating mechanics, will achieve dynamics in the same direction, while the retro-rotating figures, as shown in b, will perform dynamics a contrario .

FIG. 32 shows that even in an inverted manner, the cyndre can, like the pale, be in a single multifaceted piece, in a) in several united faceted pieces, in b) and in external paHque structure. In c) Figure 33.1 shows your three dynamics by pknetary blade / fixed cylinder, in a, rotational blade / cylinder, in b, and clokwise moving blade / rotational cylinder in c)

Figure 33.2 shows that we can go further by varying your dynamics in such a way as to create explosions and expansion in different places from those in the previous figures. In a) standard blade dynamics on two cylinder sides in one.

In b), k blade of this machine does not however carry out a Clokwise movement. Here the explosion takes place in three different places, bl, b2, b3 and not in one as in standard dynamic k.

Conversely, in b) k figure shows that we can suppose, for the same type of figure, a slower retro-rotational movement of k pale than in b, but faster than in a) a post-rotational movement of the cylinder to fill this alteration. The explosion will therefore take place here in cl and c 3

Finally, in c) we assume k mechanical with fixed cylinder, where k reacted force is neutral

Figure 30 gives other examples, this time with a blade on three sides and a cyndre of two, of k rule which we will call rotational counterpart rule.

Figure 33.3 shows for the same material figure of a blade on three cylinder sides of two, as shown in a) anterior differentiated dynamics in b, posterior differential dynamics in c. In a, the explosion moment is in a 1 In b, the successive explosions are in bl, b2, b3, b4, and in c, cl, c2,, c3, c4. we will note in b, as in c, that the cylinder is moving in the same direction as the blade, one retro-rotating, and the other post rotary, and this is why we will say these dynamics of compressive type. This is why we will say that the machine produces only a differentiated force between these parts. However as, the time of k next compression will be exceeded that of k next standard compression, one will say that this machine is posterior differential.

Set of figures relating to rotary-circular machines with orbital rotary.

Figure 33.4 shows that another dynamic is possible, and that this dynamic makes it possible to react a contrario movement of the cylinder and of the compressive part, as we had previously shown for rotor cylinder machines. Each figure corresponds to k following successive compressions of the machine. One will indeed note in this figure a planetary postrotative movement of k blade and a retro-rotational movement of the cylinder, and that consequently these two parts carry out a movement which will be called Motor, or on the contrary.

Figure 34 shows what we will call the cylindrical counterpart rule. This rule shows how all these mechanics of different appearance are understandable from the same logic. This rule can be stated in k as follows: for any machine d, a given number of sides, U exists, during its standard setting, with planetary blade and fixed cylinder, a number of degrees of rotation of the eccentric for each Heu of new expansion. Any alteration in reduction of this number of degrees must be compensated for by counterpart by a rotation or a back rotation of the cyHndre. In other words, the cyHndre must itself be in relation to the blade in a position identical to that which U would have had without these alterations.

Let’s give an example. We know that the explosion in a standard machine with a three-sided blade and a cylinder of two will take place after one hundred and eighty degrees of turning the crankshaft. Now if we determine that the next explosion will have Happ at only a hundred and twenty degrees, we will have to calculate the difference of the angles corresponding to the standard explosion, and that of the new projected explosion. We arrive here at sixty degrees a month. It will therefore be necessary to carry out a mechanical regularization and to print to the cylinder a back rotation of sixty degrees. If one reacts in this way following the explosions, one arrives at the clokwise movement.

La.figure 35 shows that this counterpart rule is general, and is applicable whatever the time of the planned new explosion. For example in a) the Heu of new projected explosion is at one hundred degrees, which is eighty degrees less than the standard place. The mechanical regularization will thus be to print that cyHndre a retro-rotation of eighty degrees.

In b) the projected location of new compression is 270 degrees, which is ninety degrees more than the standard. The regularization rule will therefore enact a correction of dynamic k of the cylinder by giving it a post rotation of ninety degrees.

Figure 35.4 gives a first example of more complete dynamics making it possible to reveal these figures which one will name, as opposed to the figures known as material, the virtual figures. In the first case, the real figure is of the post-rotary type with a blade on two sides, the whole rotating and producing a virtual rotary figure with a triangular cylinder.

As we have shown in the previous figures, U is possible to react the new compression Heu at any new angle, and to correct it by a cylindrical regularization. However, since it is a question here of driving machines, it is important to specify for these new machines, types of mechanics which will be used to support the blades, and cylinders, as well as the location of the mouths of entry and exit gases, as well as fixing candles or other accessories. To do this, U is therefore relevant to observe the behavior of the blade, independently of the cylinder. ,

In doing so, we will see that the attribution of a new explosion explosion will necessarily force a dynamic representation of the blade different from its material representation. This new figuration, for the reasons that we have previously given, can be established in such a way that it can be done in one, two or three turns.

It will therefore be seen that by determining the time of the next explosion of you so that this new projected angle can be a fairly simple fraction of three hundred and sixty degrees, for example one in three, one in four, in five, six, we will allow the k blade to create a virtual figure equivalent to one of the basic figures of rotary machines.

In the example given here, an explosion is projected at each hundred and twenty degrees. And we therefore realize the blade in such a way that it achieves this virtual figure, here triangular, while realizing the dynamic regularization of the cylinder. We must therefore necessarily distinguish material figures from virtual figures. In this example, as we said, the blade and the material cylinder, give a figure of post rotary type of blade on two sides, cylinder on one side, as shown in a). In b, we see that k virtual figure that k pale will realize will be that of a triangular motor. Driven exactly by the same mechanical mechanism as this retro-rotating figure, the blade will move in an identical fashion.

To compensate for this planetary rotation figure of k blade, the material cylinder will be actuated by adjusting each angle and at each moment according to k procedure set out in k previous figure. The cylinder will therefore rotate by two thirds of turns for each third of a blade revolution. This procedure therefore makes it possible to readjust the machine with a retro-rotary mechanism, and simultaneously with a real post-rotary figuration, the compression of which will be better.

As can be seen, the blade and the cylinder rotate in the same direction, which makes the machine simply differential, here posterior.

Figure 35.5 gives a second example of a physical and virtual figure. We must perform the machine with a specification of k virtual figure, since, as we will see, on the one hand, the mechanics will be that of k virtual figure, and on the other hand, k position of the candles and inputs and outputs k machines will also be produced while respecting the virtual figure. In this example, the physical figure will be that of a post rotary machine with a triangular blade and double arc cylinder, as shown in a) However, as shown in b) k virtual figure will be that of a retro rotary machine.

As we have already mentioned, if we understood k thing from the mechanical point of view, we could on the contrary say that k material figure is k second, since k mechanical allowing to support k blade will necessarily be that of k figure virtueUe. As before, if we adjust the cycle with the corrected angulation at each phase of its progress, we will obtain a rotational cylinder which will allow the conjunction of real and virtual figures, which we will call synthetic race. A material figure of a post rotary machine of a triangular blade with a double arc cylinder will be produced simultaneously with a virtual form of a triangular retro-rotating machine. As in the first case, this figure is located in the area of previous differential machines.

Figure 35.6 shows again the positions of a motion machine in Clokwise. As can be seen, the originality of this type of machine is to describe a limit point entered two areas of k chromatic range of rotary machines. At this point, we find k following characteristic that the number of sides of the blade is identical to that of the virtual cylinder. Explosions or compressions are in effect, for example here, on each side of a virtual triangle for a virtual blade. We see for each figure in a and b, that the number of real sides of k pale is equal to the number of sides of the virtual cylinder, which constitutes the originality of k machine, this being not strictly achievable réeUement.

Figure 36 shows that, conversely, we can decrease the number of sides of the virtual figure compared to the standard figure, which implies, as long as your compressions are successive, that we will achieve a different virtual form later. Here, therefore, we realize a real post rotary machine with triangular blade and cyHndre in double arcs, in a way that you can virtually set up a post rotary machine on one side. This réaHsation allows, for all practical purposes to subtract the crankshaft, realizing the compressive parts only by strict rotary action.

Figure 37.1 shows that therefore one can by adding or subtracting on one side the virtual cylinder, transfer a post rotary machine, into a retro-rotary machine and vice versa. Here, the same post rotary machine with a triangular blade can become a synthetic post rotary machine with a virtual side on one side, or a synthetic retro rotary machine with a virtual cylinder with four sides.

Figure 37.3 shows that the realizations of synthetic figures are as true for retro rotary as post rotary machines. In a) we can see a post rotary machine realizing a retro rotary shape of virtual cylinder whereas in b, we see a material retro rotary machine realizing a virtual post rotary shape.

FIG. 38 shows that your realizations, for the same material figure, of virtual figures are not limited to the figures with a number of sides less than or greater than one. Here, we realize, for example, a post rotary machine of triangular blade with a virtual cylinder shape of five sides.

In k column of a) we can see k list of explosions, and there, we can see that k blade is compatible simultaneously with k real shape and the virtual shape of the cylinder. In the column of b, one can see the various moments of passage, in which the blade tips pass simultaneously through the tips of real and virtual cylinders. Here, the rotation of the blade is accelerated, which produces a rotation thereof in the same direction as the cylinder, and for this machine k is located in the area of the previous differential machines.

Figure 39.1 shows that in reality, one can reaHser, for the same material figure, all the basic geometric figures as virtual figures. For example, here, for a post rotary machine with triangular blade, we can realize, as we have already shown, a figure with a smaller number of sides, i.e. posterior differential, or with more sides, triangular, square, hexagonal and so on.

Figure 39.2 shows that this is true for all your figures, and gives the example of a post rotary material figure with square blade.

FIG. 40 shows that it is possible to carry out the virtual cyHndre of a machine by réaHsation of each face thereof in a non-successive manner, by jumps.

For example, it will be possible, for a triangular blade machine of the post rotary type, to make this machine by locating each compression by jumping from eluded faces. In the present example, we organize k dynamics of k pale in such a way that not only does it achieve a virtual figure in eight sides, but moreover that it does not spank it pale by successive feces, but rather by jumping two faces evaded at k times. The blade will therefore react here of its virtual figure starting from k following the following faeces: I, IN, VII, π, N, VIII, III VI.

Figure 40.1 gives the following, for a turn of all the blade compression and expansion positions. It is important here to make your following comments. The first consists in mentioning that the creation of this virtual figure allows several explosions per turn, which would normally only be possible with an eight-sided figure, and which therefore would only give small explosions. The second consists in saying that this pretending, one succeeds in placing each successive compression in the zone on the contrary. Indeed, if we observe the unfolding of the sequence of the blade and the cylinder, we notice that they work in opposite directions, which gives the machine, by a contrario force, a significant motive power. A third observation consists in noting that the movement of each of the compressions and expansion is alternative and is comparable to the movement in Skliny, or even to a movement in successive multi Clokwise, movements already commented by ourselves for the piston machines, and which here is its layout for rotary machines. This movement, comparable to a successive Clokwise movement, allows more expansion towards the center than in standard rotary machines, the expansion of which pivots around the center before reshaping it. The expansion here, moreover, will not take quarter-turn holes, as in rotary machines, but only a quarter-turn. The machine can therefore easily be re-type four third time by choosing the even sequences for the explosion and the odd sequences for the evacuation and admission or vice versa.

Figure 41.1 recalls k slinky dynamics for a rotor cylinder machine, this dynamic realizing a jump race of the parts.

Figure 41 2 shows that, since the races of non-successive faeces are possible, the sequences of synthetic races, which we will also call real races, are multiple for the same virtual figure. For example, here, we show that various virtual strokes of the k blade make it possible to realize a virtual figure of five sides for a post rotary material figure of a three-sided blade.

In your following figures, we will show that, according to the synthetic course chosen for the same real and virtual figures, we can set up very different machines, since some of them will be located in the area of previous differential machines, others in the contrario machine area, and others in the posterior differential machine area.

Figure 42.1 therefore widens the construction rule of k reflectivity of the cyHndre by deciding that one must take account not of the virtual figure, but of the virtual race of realization of this figure. Consequently, the difference in degree of the first successive material and virtual compressions, and the angle thereof, will be applied to the cylinder.

In the example of k in this figure, k virtual figure of five sides is successively carried out, which forces the displacement of k blade and cyHndre in the same direction, and realizes an anterior differentiated machine.

Figure 42.2 realizes a synthetic race, real, not successive, and whose jumps are realized in such a way as to be located in the contrario area of the machine. Here, we build by therefore a virtual fece with each compression. As shown in b, the machine follows the sequence, 1: 1, 111: 2, V: 3 R: P 4, IV: 5

We must therefore characterize the machine according to its criteria of real form, virtual form, and synthetic sequence. We could say that this machine is of type P 3/2; 5; 1: contrario, which will be understood to mean that k machine is a rotary post of three sides on two, of virtual cylinder of 5 sides, and of jump of one side eluded. We can even specify it on the contrary.

Figure 42, 3 shows the same real and virtual forms, but, again with a different synthetic race. Here, the jump is two k sequence is therefore k following, 1: 1, IV: 2, π: 3, V 4, III 5

As we can see, it is no longer so much the virtual form which will define the area of the machine, but the synthetic course on this form. Here, k synthetic course appears k first explosion located in an area in deca of the point of explosion during k standard realization, and anterior to the zero point, k thing is therefore posterior differential, and as we can note it, since the cylinder and k blade act post rotary in the same direction, the power is reduced, since there is a mechanical contradiction with the one direction that an explosion must have.

Figure 43 summarizes the previous three figures and concisely puts He in the synthetic race and the belonging of a réaHsation to one area or another. . In a we have a successive course, of which k first compression is located in the anterior differential area,

In b, k synthetic race realizes a machine of the chromatic area said on the contrary, and will be of the Motor category.

In c, k machine realizes a synthetic stroke whose k first compression is located in the posterior differential area. The machine will be Compressive.

Figure 44 shows that certain figures, the number of sides of which is even and quite low, lead to lower figures. For example here, k virtual figure in six sides, allows a sequence of successive faces in a) In b, however the sequence with a jump, we fall back on the Clokwise dynamics, while k sequence with two jumps in c), we fall back on standard dynamics.

Figure 45 shows various real strokes of a virtual figure of seven sides for a post rotary material figure of a three-sided blade. One can find there, from one to seven for each figure, following the compressions. As before, the first synthetic runs will give Heu to anterior differential machines, the sequence with two eluded faces will give Heu to a contrario type machine, and the other sequences, posterior differential machines.

Figure 46 shows various real strokes of a virtual figure of eight sides for a post rotary material figure of a three-sided blade. As in the previous figure, we can

Here is a virtual figure of fourteen to fourteen sides for a post rotary real figure of a three-sided blade.

Figure 48.1 summarizes your last figures, and shows, in a single figure that several virtual figures are possible for the same material figure, and that several synthetic strokes are possible for each virtual figure.

Figure 48.2 shows, for a turn, this time, a post rotary material figure of four of three sides of the blade and cylinder, carried out on a virtual structure of ten sides. The synthetic race by jumping from three sides makes it possible to react to the first compression and explosion, and the following ones, in a contrario part of the machine. As can be seen, 10 compressions are carried out for each half turn of the blade, and a third of a turn, therefore, if the machine is carried out in four stages, ten explosions per revolution of the blade, which corresponds to a motor with a piston in V of twenty pistons, that is practically three good old V 8, or two good old V 12.

Figure 49.2 shows the chromatic scale of a machine with a material figure with a blade on three sides and a cylinder with two. We can see there the differentiated previous areas, occurring when the explosion occurs before the clokwise moment of the machine. We can see there the so-called posterior differentiated areas, realizing when the moment of explosion is later than the moment of standard explosion. Lastly, we can see the contrario areas there, realizing when the first explosions happen between clokwise and standard Heux.

Figure 50.1 shows the specifics of the mechanics of these machines. We can generally say that these machines can be activated by mechanics similar to the mechanics of circular rotary machines with clokwise movement, and taking into account, however, to carry out the movement of the blade so that it produces the movement at times. real and material figurations, if the machine is produced in Slinky and virtual and material if it produces successive compressions.

In both cases, the crank pins carried by the machines will be produced in such a way that their length is equivalent to that of the material figures, when carried out in a standard manner, and also in such a way that they carry out the reports of turning and back-rotation. virtual or real figures as the case may be. For example, in the case of k mechanization of k figure 42.2 and 33.4, the machine will be made with the same lengths of crankpins as k figure material is rotating blade three sides and cylinder two.

By the way, we orient k mechanical orientational of k figure 42.2 with the help of a retro-rotating mechanics, imitating that of a cylinder machine of five sides, increased by number of additional degrees to be filled by the triangular shape and not square of the blade.

In your two cases, it will be noted that this pretending one greatly improves k poly induction, and increasing k range of this one, which has the effect of making positive even k rear part of the blade movement, which will not remain more so by simple blocking, but will act dynamically

Figure 50.2 shows, as with standard machines, clokwise machines can not only be done in reverse fashion, but also in a bi-functional fashion.

Figure 50.3 distinguishes, for all of the realizations, the retro-rotary differential chromatic ranges, differentiated post rotary and on the contrary, for a machine which is itself virtual. This chromatic range is made up of the following main points: cylinder and rotating blade machines, Clokwise cylinder machines, planetary rotor cylinder machines. The interphases between these points constitute the differential, contrario, or differentiated posterior parts of these machines. These observations constitute a definite advancement in the knowledge of these machines, which previously consisted only of two polar possibilities, namely the octave point, and the standard point, which will be called the fifth point. The addition of the clokwise point, which we call the third point, not only makes it possible to constitute the areas of these machines, but also to achieve a rational progression between them, as in the range of colors, the range of musical tone , or in other ranges. The parts no longer understand each other successively, discreet and isolated, but rationally, by their relationships to the same fundamental, the zero point. In addition, from the dynamic point of view, the creation of a machine according to its synthetic course, therefore, not only simultaneously virtual and real, but moreover, by jumps, makes it possible to derive ranges from the melodic relationships which give the machine its vivance, a deeper dynamic, less mechanical and more real, rationally speaking, and in the Hegelian or Cartesian sense of the term. In these cases, mechanical logic k resembles the arts, since it makes it possible to realize understanding Hens from material data, which ultimately are more real than these data itself.

FIG. 51 shows the qualities of a machine with a virtual cylinder in eight and a jump of two, consequently of movement in contrast. As we can see, here, your parties work on the contrary. Second, as in Clokwise movement machines, the connecting rod effect is achieved by rotation of the cylinder. Third, as can be seen in c, k end of the expansion is fairly vertical compared to the expansion of a standard machine, which better respects the explosion amorphism.

Figure 52 summarizes the four types of mechanization possible for circular rotary machines, either in a) by real mechanics of the virtual movement of k pale by semitransmittive mechanics of the rotational cylinder, in b) by real mechanics of the virtual movement of the blade by descending mechanics of rotation of the cylinder, in c) by semi transmittive mechanics of the blades by confused semi transmittive mechanics of the cyHndre, by d) by semi transmittive k blade mechanics by descending mechanics of the rotational cyHndre

FIG. 54 shows that the efficiency of different piston machines can be increased by making them with rotor cylinders or the perforated upper pistons. In the same way one can perforate the rotational cylinder towards the fixed external cylinder. In this way k compression is feigned from three parts, and the power on the blade is therefore achieved by pressing on the outer cylinder which eliminates the contradictory effect of k strictly differentiated thrust.

Figure 55 is an example of mechanization of a rotary circukire machine in which a poly inductive semi transmission in a is used, and a mono inductive downward induction in b

Figure 56 shows some other combinations, among the hundreds possible. It is therefore important to note that these induction assemblies are exemplary. Any induction of these may be replaced by any other induction, as the case may be, standard, semi-transmittive, rising or falling. In al, we have a poly inductive semi transmission controlling the retro rotation of the cyHndre, carried out in a confused way with a fixed poly induction bl, controlling the clokwise action of k pale.

In a 2, we have a poly inductive action of k pale, and in b 2.1 a mono inductive downward action of the cylinder In b2.2, the action controlling the cyHndre is semi transmittive with pinions.

In a 3, the semi-transmittive poly inductive action controls both the cylinder and the dynamic support gear of the rising blade induction poly, in b 3,.

In a4, k rising poly induction of blade causes a descending poly induction of cyHndre in b 4. In a 5, a semi transmittive induction with pinion gear simultaneously drives the cylinder and the support gear of the semi tranmittive rising induction by gear hoop in b 5 At a 6, k split double transmission drives both the cyHndre and the dynamic central gear d the rising induction by dynamic central gear in b 6

Figure 57 shows that clokwise movement is also possible peripherally.

FIG. 58 shows that the clokwise movement can be carried out in a bi-functional manner, the external cylinder, and k under the internal blade being strictly rotational, and k blade in clokwise movement.

FIG. 59 shows in a that we can simplify the segmentation of rotary machines by the use of U-shaped segments, 300 inserted in the tips of the blades, you way that their end parts 301 touch each other, or you, that at 2, touch a central circular segment 302. In 1 3, we see that these U-shaped segments can also be arranged in the cyHndre, of teHe so as to partially coat k pale ,. In these cases, these will be supplemented by segments 304 corresponding to the shape of the blade stroke, arranged in your sides of these ^: ci

In b of the same figure, we show how to make the machine with the use of a crankshaft rather than an eccentric, by cutting out the paddle with a kisser to pass through the crankpin of the stem and re-extruding it by an additional part blade 505

In c of the same figure, it is shown that the rotational blade of clockwise moving machines can be realized by constructing it in the manner of a turbine blade. The entry of materials through the center 306 will therefore produce a first rotation of the blade in the manner of a turbine, and the substances escaping therefrom 307 will entrain the clokwise cylindrical parts of it.

Conversely, if the substances are inserted from the outside 308, the turbine will then act as a strong material concentrator 409, and as a propellant.

Figure 60 shows other possible mechanics, which again fall under the composition rules already shown. It is therefore important to repeat that these induction assemblies are exemplary. Any induction of these can be replaced by any other induction, depending on the case, standard, semi transmittive, rising or falling Here, in all three cases, the rising induction is a polyinduction. In a, the induction gears 400 are supported on their support gear 401 and are coupled to a second series of gears which will be peripheral support gears 402. The crankpins, 403, supporting the blade 404, will therefore be coupled to the induction gears by the use of this second series of gears. These will retroactively activate the cylinder induction gear 405.

In b, k poly induction activates the blade, 406 and is connected to a semi transmission by inverted pinion 407, activating the cylinder. In c, the original cyhndre gear 408 is coupled to an internal gear 408, which will allow the cylinder to be re-planed.

Figure 62 shows the semantic gaps overcome by our work in relation to planetary cylinder machines, there is an error in meaning and an omission or contradiction in mechanization. Indeed, the correct direction of these machines is complementary to the sense of their counterpart, and mechanical k must not be ceUe of k figure, but well that of k against part. A correct understanding of these elements makes it possible, as we have shown, to readjust the cylinder in a bifunctional fashion. J) Relatively to machines with blades and rotational cyHndre the direction of this one must be reversed since according to k rule which we gave, k next expansion pretending in the same place, k pale must carry out a retrorotation of one hundred and twenty degrees, and te rotational cylinder must undergo a rotation of one hundred and four twenty degrees. This reorientation of the k machine makes it possible to consider k as the octave machine for the chromatic scales K) The rotor cylinder machine realizes a virtual figuration blade of a machine with a square cylinder, and thereby becomes a retro-rotary differential, which lowers the motor skills of the machine, k understanding of this machine is incomplete, not only by the absence of a general rule, but also by the absence of a clokwise movement machine, and by the absence of the establishment of virtual and real figures. As before, there is an absence of mechanization of this figure, which would have shown this retro-rotational character and k necessity of semi transmission, or of descending inductions. This figure is out of its chromatic fields and remains isolated, anterior differential, without mechanics. Like most attempts in terms of rotary machines, it evokes the machine in compressive and non-motor capacity, which gives it lower power, even with standard machines.

L) the ignorance of bi inductive, figurative figures, either poly turbines, and dynamic, or machines with Clokwise movement of blade or cylinder

M) the absence of establishment or determination of mechanical levels of figuration or dynamics

N) the absence of mechanized accelerator-decelerator dynamics

O) the absence of establishment of the chromatic fields

Claims

claims

1 Any machine which simultaneously realizes a compressive material figuration of the post rotary, retro rotary or birot type, a virtual figuration and a synthetic figuration, this machine being able to be located on the chromatic range of rotary machines, with the exception of retro type machines rotary and post rotary whose material, virtual and real figures are identical, mechanized by mechanics of the same kind, respectively rotary and post rotary, when the mechanics are, for these strict cases, mechanics by mono induction and by intermediate gear , attributable to Wankle.

2 Any machine for dynamic standard compressive parts, of which k mechanical by hoop gear is produced with a third gear allowing k desangulation of the support and induction gears in rektion with the hoop gear.

3 Any machine for dynamic standard compressive parts, of which k mechanical by hoop gear is produced with the use of a chain or belt to replace the hoop gear

4 Any machine for dynamic standard compressive parts, of which k mechanical by poly induction is produced, when k three-sided blade with the use of more than two support crankshafts, these being arranged outside the lines connecting the center and the blade corners

5 Any machine for dynamics of standard compressive parts, whose mechanics by poly induction is produced with a so-called alternative poly induction, alternately realizing the induction of two subsidiary crankshafts by mechanics, and of the other induction by simple attachment to a blade, this being possible by partial or total removal of teeth from the support or induction gears

6 Any machine of dynamics of the standard compressive parts of which k mechanical by poly induction is produced an induction of each subsidiary crankshaft by one of all the first degree inductions already listed by ourselves

7 Any machine for dynamic standard Compressive parts including k mechanical by poly induction is produced by polycamed gear, these gears being produced by reciprocating and distancing their teeth alternately this producing the desired decelerative accelerating effect.

8 Any machine called rotativo circukire, whose retro-rotational action of k blade has been modified in such a way as to produce a place of next expansion different from that of its standard position, and produces a virtual figuration different from k material figuration, k counterpart of this modification is carried out by a rotational or planetary dynamization of the cyHndre 9 Any machine such as described in, known as Clokwise blade movement, whose orientational blade movement, observed from the outside, is nuL and whose cylinder is rotational, this dynamic producing a new compression identical to its rotary counterpart .

10 Any rotary rotary machine with blade in Clokwise movement of the rotary post type, whose cylinder is rotatably rotated on the contrary. ¹

11 Any rotary rotary machine with Clokwise blade in retro rotary type, whose cylinder is rotated in the same direction

12 Any machine such as. defined in 1, 8, 9, the mechanics of which support the compressive parts, is carried out with the use of two or more of the following elements: - a rising induction - a falling induction - a semi transmission activating the cylinder and / or the blade induction support gear

13 Any machine such as defined in 12, of which the mechanics rising generally but not limitatively is one of the following mechanics: by mono induction, by intermediate gear, by poly induction, by hoop gear, by double internal gears, by heel gear, by gear structure, by unitary gear, by central active gear

! 4 Any machine such as defined in 12, including k downward mechanical, defining itself as a mechanical whose support gear is dynamic and peripheral, usually arranged on k blade, and the induction gear is central and activates the cylinder , is generally but not limited to is one of the following mechanics: by mono induction, by intermediate gear, by poly induction, by hoop gear, by double internal gears, by heel gear, by gear structure, by unitary gear, by active gear central

15 Any machine whose k semi transmission is invertive, and most often accelerative inyerivo, and which is carried out - either from inversion by coupling of external gears, and acceleration by coupling of internal and external gears - or from d pinion gears and double d pinion gears

16 Any machine such as defined in 1 and 15, the mechanics of which activate the blades and cylinder compressive parts are combined and synchronized by their coupling to the same element, either the eccentric blade, or the crankshaft the support / induction gear 17 Any machine such as defined in 1, which will have a different Heu for next expansion, anterior or posterior to the standard Heu, and of which this difference will be bridged by a mechanical counterpart dynamically rotating the cylinder.

18 Any machine, such as defined in 1, whose action of k pale will simultaneously realize a virtual cylinder shape, this shape can be retro or rotary post its on the chromatic scale.

19 Any machine machine, such as defined in 1, the inductions and semi transmission of which can be carried out in the same way, this having the result that the support gears of one will be the same gears as the induction gears of the other, or vice versa.

20 Any machine such as defined in 1, whose next explosion time is on the successive face of a virtual figure prior to the next explosion time Clokwise, this machine then being called anterior differential rotary-circular

21 Any machine such as defined in 1, whose next explosion time is on k successive of a virtual figure posterior to the next standard explosion time, this machine being then said rotary-circular differentiated posterior

22 Any machine such as defined in 1, whose next explosion time is on k successive face of a virtual figure is posterior to the next Clokwise explosion location, and prior to the next standard explosion time, this machine then being called rotativo- circular to contrario

23 Any machine of which k mechanics is the mechanics of k virtual figure of k machine, that is to say k mechanics of k stroke of k blades relative to the fixed body of k machine, and not in relation to k material representation of the compressive parts.

24 Any machine whose k mechanical k blade will be corresponding to k virtual form of the cyndre that it produces, and which will be carried out by the induction corresponding to this form, in a standard or semi-transmittive way,

25 Any machine such as defined in 1, whose next compression hours in virtual form will occur by jumping, thus requiring more than one revolution of the machine to carry out all the faeces, and thus allowing a next compression time. on the contrary, • in spite of a virtual figure on more sides than your material figures, k figuration produced by all the compression suites being known as the real figure of the machine.

26 Any machine whose k blade will be mechanically activated by a mechanism corresponding to the real figure of the machine,

27 Any machine having a material figure, a virtual figure and a real figure, whose Next Expansion Heux is anterior to this Clokwise Heu of this one, between this one and the standard Heu, and posterior to the standard Heu, thus realizing, as the case may be, an anterior differential, contrario, or posterior differential RéeUel machine. 28 Any machine such as defined in 1, of which the material compressive structure will be retro-rotary, post-rotary, or birotative, of the Polyturbine or polyturbine stage type.

29 Any machine, such as defined in 1, whose blades will be - of standard type, - as a combined set of single blades - in a single structure

30 Any machine such as defined in a, the degrees of which will be increased - by vertical elevation of degree, - by planetization of the positioning of the blade, - by acceleration / decelerative reaction of the piston, - by acceleration / deceleration or oscillation of the blades.

31 Any machine whose dynamics of the compressive parts have been reversed, from center to periphery, as well as rearranged in opposite orientations, these machines being supported by the mechanics of their forms before inversion

32 Any machine such as defined in 1, whose cylinder is planetary, and k blade is fixed, the cyHndre being activated by k mechanics of k figure of opposite nature

33 Any machine in the cylinder is in Clokwise movement and the blade is in rotational movement, this machine using mechanical counter part

34 Any machine with a cylinder in planetary motion and a blade in rotational motion

35 Any machine peripherally and orientationeUement inverted, whose movement of the parts will be anterior differential, posterior differential, on the contrary.

36 Any machine in which one of the compressive parts will be bifunctional, performing at once k a cylindrical function of one of the compressive systems, and a palic function of the second system.

37 Any rotary rotary machine with clokwise blade movement, comprising in composition - subsidiary crankshafts rotatably mounted in the side of the cylinder and fitted with gear, and supporting the blade, these crankshafts having the same stroke since combined with the same third element, a blade mounted on these crankshafts whose movement is a Clokwise movement a central axis of the machine to which is fixed a gear coupling the gears of subsidized crankshafts, as well as the rotational cylinder The crankshaft gears playing both the role of induction gears of the upward induction of blade, and of support of the downward induction of cyHndre, and conversely, the blade gear playing the role of gear of support of upward induction of blade and induction of downward induction of cylinder.

38 Any machine comprising in composition a blade, governed by a semi transmittive induction, a semi transmittive induction, comprising three crankshaft pinion gears and the support gear, this same semi-transmission driving the cylinder, fixed to the same axis as the support gear, k semi transmission of the blade support gear and induction of cyHndre being consequently made in the same way.

39 A machine comprising in composition - a blade governed by an induction, exemplarily but nono Hmitatively a mono induction, - on its other side, a descending induction, for example also a mono induction governing the cylinder.

40 Any machine in Clokwise movement, whose positional action of k blade is non-circular.

41 Any machine such as claimed in I, the segmentation of which is carried out - by U-shaped segments angularly arranged in the tips of you so that their end portions are supported on the complementary U-shaped segments - by U-shaped segments angularly arranged in the tips so that their end parts are supported on a complementary circular segment arranged in the side of the blades

42 A nrachine of the rotary type whose eccentric is realized in the form of a crankshaft, the blade in which the latter will be disposed both provided with an extrusion allowing its arrangement and with a completely fixed part subsequently closing this extrusion and possibly crossed out by any standard process. .

43 Any machine claimed here, used as a pump, motor, compressor, capture machine, compressor, artificial heart.

44 Any machine whose k blade mechanics is made in such a way as to make, by its length the material aspect of k figure, and by its orienting mechanics, k intentional virtual form. 45 Any machine whose blade mechanics is made in such a way as to realize, by its length the material aspect of k figure, and by its orientational mechanics, k defined virtual form, through a definite real synthetic path

46 Any machine whose cylinder mechanics is carried out by descending induction from the blade

47 Any machine whose mechanical k of cylinder is realized by semi transmittive induction leaving from eccentric

48 Any machine of which k mechanical cylinder is realized by semi transmittive induction outgoing out of the dynamic blade support gear

49 Any machine in which k span length is rektive to k material figure and k mechanical, semi transmittive or not, rektive to k virtual or RéeUe figure.

50 Any machine whose k rotationality of the cyHndre allows an equivalent angulation, according to k rule of mechanical counterpart, with k difference of angulation of k new blade position in total expansion and k standard position.

51 Any machine having at least one of the following descriptive parameters a) having a first degree induction of the present inventor b) having a descending induction c) having a semi transmittive rising induction d) having a semi transmittive cyHndre induction e) having a oscillating blade action f) having an increase in degrees by addition of induction, by polycamation g) having a horizontal combination of inductions

52 Any clokwise, or slinky movement machine whose blade or cylinder is increased by degrees.

53 any machine possessing, in addition to the material character, a virtual character, or virtual Real