JP2010523868A - A machine that works on the principle of centrifugal force utilization - Google Patents

Abstract

A machine that operates on the principle of utilizing centrifugal force and typically on the principle of potential energy gain for generating mechanical energy.
Based on the principle of utilizing the centrifugal force of a mass (M) that generates mechanical energy and is moved along a closed dynamic circuit (12) over at least a curved portion of the circuit (12). Provided is a machine (10) that functions. This machine is also optionally under the influence of gravity in a closed circuit (12) that is permanently maintained in dynamic unbalance using a continuous or discontinuous input of external energy (W0, Wmag). It functions on the principle of energy gain generated by the falling mass (M).
[Selection] Figure 12

Description

  The present invention relates to the functional principle of a machine that generates mechanical energy from the centrifugal force of a mass in a closed dynamic circuit (closed mechanical circuit), which optionally includes the earth's gravity. Under the influence of the field, the state of permanent imbalance is maintained using the fall of the mass body.

ここで、（Ｖ）は、高さ（ｈ）から落下した後に質量体（Ｍ）によって達成される速度であり、（ｇ）は、地球の重力場に起因する質量体（Ｍ）の加速度、すなわち９．８１ｍ／ｓ^２（または３２．２ｆｔ／ｓ^２）である。 As is well known, a mass body (M) (an object of mass M) located at a given height (h) has a stored potential energy (PE): PE = M * g * h (PE = M × g × h). When the mass body (M) is in a free-fall state, the potential energy (PE) is converted into kinetic energy, and the following equation is obtained by the energy conservation law.

Where (V) is the velocity achieved by the mass (M) after falling from height (h), and (g) is the acceleration of the mass (M) due to the earth's gravitational field, That is, 9.81 m / s ² (or 32.2 ft / s ² ).

  However, in order to maintain the falling motion of the mass body (M), after the mass body (M) falls, the mass body (M) again reaches the start point of the falling motion of the mass body (M), that is, the height (h). It is necessary to lift up. This lifting requires the supply of energy (ie, [M * g * h] without considering resistance) to the mass (M), so that when M, g and h are all the same value, the gain of energy There is no. That is, M * g * h = M * g * h.

  The fall of any mass in the Earth's gravitational field is considered to be in a state of dynamic imbalance (the sum of external forces acting on the mass (M) during the fall is not null (ie, not 0)). Note that this is different from any machine that exists today.

  To date, no machine can continuously generate more mechanical energy (positive gain, greater than 1 energy efficiency ratio) than the amount of energy input from the outside (eg, a human).

  Accordingly, there is a need for a machine that functions based on the principle of potential energy gain for generating mechanical energy, based on the principle of utilizing centrifugal force.

  Accordingly, it is an object of the present invention to provide a machine that functions on the principle of utilizing centrifugal force and typically on the principle of potential energy gain for generating mechanical energy.

  The advantage of the present invention is that a machine functioning on the principle of centrifugal force utilization can be used in different ways and with different magnitudes for different output gains while utilizing centrifugal force on at least one curve. It can be realized.

  Another advantage of the present invention is the energy efficiency ratio defined by the ratio of the sum of all external energy inputs (including energy input from humans) supplied to a machine greater than 1 to the mechanical energy generated by the machine. A machine that also functions on the basis of the principle of potential energy gain to have a system that utilizes centrifugal force, while maintaining a permanent dynamic imbalance.

  Another advantage of the present invention is that a machine functioning on the principle of potential energy gain, in different magnitudes for different output gains, can be realized in a number of different ways.

  In accordance with one aspect of the present invention, a machine for generating mechanical energy is provided that is closed at least temporarily around an at least one rotating freewheel by the input of external energy. A closed circuit that is selectively mounted so that a plurality of mass bodies move along the closed circuit, and the mass body is moved so that the mass can move along the circuit. Mass located in at least one curvilinear section of the closed circuit for applying energy to the circuit different from the external energy input from the system for guiding along the circuit and the centrifugal force of the mass And a system for utilizing the centrifugal force of the body.

  In one embodiment, a system for utilizing the centrifugal force of a mass is typically substantially free and substantially radially movable when the mass is on the at least one curve. Like that.

  In one embodiment, the mass is selectively mounted in a closed circuit between its relative upper point and its lower point, while falling from an upper point to a lower point in the Earth's gravitational field. The kinetic energy resulting from the transformation of the mass energy of the mass is supplied to the closed circuit, and the guidance system is desorbed from the closed circuit using at least its own kinetic energy at the lower point while the mass is Including a mass track adapted to move from point to upper point, the machine being adjacent to the lower point to selectively maintain the closed circuit in a permanent dynamic unbalanced state A system for detaching the mass from the closed circuit at a position, and the mass at the position adjacent to the upper point to selectively maintain the closed circuit to a permanent dynamic imbalance. System for wearing and And a said at least one curved section of the closed circuit which is located between the at least partially the upper point and the lower point.

  Conveniently, the mass track includes a substantially arcuate portion extending between the upper and lower points.

  Typically, the mass track includes a generally semi-circular portion that extends between a lower point and an upper point.

  Conveniently, the closed circuit includes a lower portion ending at the lower point, and the mass track has a lower track portion that selectively and movably supports the mass along it before reaching the lower point. Including.

  In one embodiment, the mass track is immediately after the system for utilizing the centrifugal force of the mass and is oriented substantially tangential to the trajectory of the mass exiting the system for utilizing the centrifugal force. It is attached.

  In one embodiment, the guidance system includes a subsystem for selectively holding a mass along a closed circuit at least between an upper point and a lower point.

  Conveniently, the guidance system can be moved around at least one wheel for selectively receiving a mass body internally along a closed circuit between an upper point and a lower point. The holding subsystem maintains a mass in each of the carts between an upper point and a lower point.

  Conveniently, each carriage includes a fixed part movable along at least one wheel along a closed circuit between an upper point and a lower point, and a movable part, the movable part being a fixed part The movable part is movable in the radial direction with respect to the fixed part between a closed form in which the movable parts are close to each other and a deployed form in which the movable part is separated from the fixed part.

  Typically, the movable part of the carriage is selectively and freely radially movable from a closed configuration to a deployed configuration when the carriage is on the at least one curved section.

  Conveniently, the desorption system includes a release mechanism for selectively desorbing masses from each of the carriages near the lower point.

  Conveniently, the closed circuit includes an upper portion starting from an upper point and ending at the upper end point, and the mounting system mounts the mass in the closed circuit at a position between the upper point A and the upper end point.

  Typically, the mounting system includes a mass storage (magazine) for receiving mass desorbed from the lower point near the upper point, the mass storage between the upper point and the upper endpoint. The at least one desorbed mass body temporarily including the at least one desorbed mass body so that each mass body of the desorbed mass body reaches an upper point. Attach to an empty cart of individual carts.

  Conveniently, the system for mounting the mass recovers at least a portion of the kinetic energy of the mass that has been desorbed from the lower point upon reaching the containment.

  Alternatively, a system for mounting mass bodies uses a work input outside the circuit to allow each mass to have at least the speed of the circuit when mounted.

  Alternatively, the mounting system accepts a mass that has been desorbed from a lower point near the upper point and of the desorbed masses, the mass of the mass that has been desorbed between the upper point and the upper end point. It includes a mass transport mechanism that is mounted on an empty cart among the plurality of carts so that each mass reaches the upper point.

  Conveniently, the release mechanism is selectively activated when the velocity of the mass at the lower point is greater than or equal to a predetermined value, so that the mass reaches the upper point. Ensure that you have sufficient kinetic energy.

  In one embodiment, the masses are equally spaced from each other along the closed circuit.

  Conveniently, the kinetic energy supplied to the closed circuit is consumed by the frictional forces of the masses at each relative displacement along it, and each mass is mounted near the upper point. Is greater than resistance work (work that resists resistance), including work consumed by the mass mounting system.

  Conveniently, the system for mounting the mass accelerates the mass to a speed approximately equal to the speed of the circuit using external energy input when the upper point is reached.

  Typically, a system for desorbing a mass, a system for mounting a mass, and a system for utilizing the centrifugal force of a mass are only activated when the circuit reaches a predetermined speed. The

  In accordance with another aspect of the present invention, a machine for generating mechanical energy is provided, which is a closed circuit located around one or more rotating freewheels and is moved along therewith. Having a plurality of masses and movably driven until a predetermined speed is reached that is equal to or greater than the minimum speed using at least temporarily maintained input of external initial energy. A closed circuit, a system that guides the mass body along their displacement along the closed circuit, and an energy different from the external initial energy input from the centrifugal force of the mass body. A system enabling the use of the centrifugal force of the mass located in at least one curved section of the closed circuit.

  In one embodiment, the mass body supplies kinetic energy due to the transformation of the mass energy of the mass body to the closed circuit while falling in the earth's gravitational field, and the machine makes the closed circuit permanent. A system that allows the mass body to be desorbed from the closed circuit at its lower point in order to maintain a dynamic unbalanced state, a system that attaches the mass body to the closed circuit at its upper point, and a lower point from the closed circuit And a system for adding the mass body to the closed circuit at an upper point using kinetic energy from its own velocity when desorbed from the closed circuit when desorbed.

  Conveniently, a system for attaching a mass to a closed circuit uses an external energy input to allow the mass to reach the speed of the circuit when installed.

  Typically, a system that allows a mass to be mounted in a closed circuit includes a system that allows recovery by circulation of the mass's kinetic energy when the upper point is reached.

  In one embodiment, the shape of the circulation path causes a tangential reaction due to centrifugal force to add positive work to the moving component.

  Alternatively, the shape of the circulation path may have a large amount of energy due to the centrifugal force when the mass body desorbs from the circulation path at a lower point in addition to the kinetic energy generated by the speed of the circulation path. It can be so.

  Other objects and advantages of the present invention will become apparent upon careful reading of the detailed description herein with reference to the appropriate accompanying drawings.

1 is a schematic elevation view of a machine that operates on the principle of potential energy gain without a system for utilizing centrifugal force according to an embodiment of the present invention, the basic having an empty carriage defined by four wheels A typical closed circuit. FIG. 2 is a schematic elevation view showing the circulation path of FIG. 1 in which the mass body is shown in its original position in the carriage. FIG. 3 is a schematic elevation view of FIG. 2 with some mass bodies removed and detached from a cart that moves upward (from point G to point A). FIG. 4 is a schematic elevation view of FIG. 3 with an off-circulation bypass track for an upwardly moving mass that is detached from the carriage. The schematic elevation view of other embodiment of a basic circuit form. The schematic elevation view of other embodiment of a basic circuit form. The schematic elevation view of other embodiment of a basic circuit form. The schematic elevation view of other embodiment of a basic circuit form. In addition to the two systems of external input work W0 (at the height of the circuit) and in this version Wmag (at the height of the system for mounting the mass on the circuit at its upper point A) FIG. 5 is a schematic elevational view of FIG. 4 with a containment feed for placing mass in an empty cart and receiving mass leaving the mass track. FIG. 5 is a schematic elevation view of FIG. 4 with an alternative embodiment of a mass transport mechanism. FIG. 3 is a schematic elevation view illustrating a method used by a system for utilizing centrifugal force for centrifugal force acting on a mass body according to an embodiment of the present invention. FIG. 3 is a schematic elevation view illustrating a method used by a system for utilizing centrifugal force for centrifugal force acting on a mass body according to an embodiment of the present invention. The expanded schematic elevation which shows the example of the different part of the trolley | bogie in a closed form. The expansion schematic elevation which shows the example of the different part of the trolley | bogie in the expand | deployed form. FIG. 7 is a schematic elevation view of FIG. 6 in which a system for utilizing the centrifugal force of the mass body is located immediately after the upper end of the circuit. FIG. 7 is a schematic elevation view of FIG. 6 in which a system for utilizing the centrifugal force of the mass is located just before the lower point of the circuit. FIG. 12 is a schematic elevation view of FIG. 6 combined with a system for utilizing the centrifugal force of the mass body of FIGS. 10 and 11.

  In the following paragraphs, the following corresponding machine examples are considered to explain the functional principle and purpose of the present invention.

  In the following description, the machine of the present invention is able to operate on a generally horizontal surface where only frictional forces will be considered, but in a configuration oriented vertically to take advantage of the potential energy of the mass. Note that this indicates that it may have parts.

  The functional principle is that the moving mass generated by the falling mass body (M) due to the earth's gravitational field generates a closed dynamic circuit without using the law of conservation of energy. The goal is to maintain a permanent dynamic imbalance with the selective input of energy.

  The present invention is described step by step in the following paragraphs so that it can be easily understood.

  A-Basic system (not using centrifugal force)

  Referring to FIGS. 1-4, based on the principle of energy gain provided by a mass M falling under the influence of gravity in a closed dynamic circuit 12 that is permanently maintained in a dynamic unbalanced state. A functioning machine 10 is shown.

  The closing dynamic circuit 12 has at least one of the initial external energy W0 and the four rotating freewheels R1, R2, R3, R4 shown in FIGS. 1-4 arranged in the corners of a substantially rectangular configuration. It is driven by the potential energy of one surrounding mass body M. Any of the wheels R1, R2, R3, R4 is used to recover the acquired mechanical energy and to other machines (not shown), for example to convert this mechanical energy into electrical energy, for example. Can communicate. Typically, the circulation path 12 includes a mass guidance system that includes a plurality of carriages 14 as shown in the drawing, including an inner rail Ri or truck that can be moved in a counterclockwise direction. A guidance subsystem is included.

  Preferably, each carriage having a mass (M) rolls on the inner rail Ri, typically by a bearing 16, although any other friction mitigation mechanism is conceivable. As shown in FIG. 1, the carts 14 are preferably equidistant and connected to each other by a flexible mechanical connecting portion 18 such as a chain.

  The circulation path 12 shown in FIG. 1 has a dynamic balance, and a mass body M is added to each carriage 14. Conveniently, the mass M selectively selects the mass M along the outer rail Re or the closed circuit 12 on the bearing 20 or similar friction reducing mechanism, at least between the upper point A and the lower point F. Slide along a track that forms part of another subsystem of the mass guidance system.

  Even if the mass body M is added, the circulation path 12 remains in a dynamic balance as shown in FIG. 2 (the sum of the external forces becomes zero).

  The circuit 12 typically has a substantially horizontal upper portion 22 extending between a relatively upper point A and an upper end point B of the circuit, and a lower start point E and a relatively lower point F of the circuit. A similar substantially horizontal lower portion 24 extending therebetween. Circuit 12 also defines a descending portion 26 between points B and E and an ascending portion 28 between points F and A. Although all of the portions 22, 24, 26, 28 are shown as being substantially straight, those skilled in the art will appreciate that any other shape would not depart from the scope of the present invention. .

  Dynamic imbalance is introduced into the circuit 12 according to the following conditions.

  1-circulation path 12 is rotated (operated) around wheels R1, R2, R3, R4 at initial speed V0 using input energy W0 supplied from the outside.

  2- Mass M is removed from its corresponding carriage 14 (and thus circuit 12) near lower point F by the release mechanism of the mass detachment system (such as the shape of the mass container of the carriage 14 or any other mechanism). Desorbed, pulled apart or released.

  3—Additional mass M is mounted or attached to circuit 12 (or empty cart 14) at upper point A by the mass mounting system each time an empty cart 14 is placed adjacent to upper point A. It is done. Typically, the mass M is accelerated at the mass mounting system level using external energy Wmag to a speed equal to the speed or speed Vcir of the circuit (the influence of the additional mass M and the additional mass M's The source is explained below).

  The guidance system, mounting system and desorption system are typically mechanical systems, although they can be easily made at least partially electrical, electronic, etc.

  The periodic distance P separating two adjacent carriages 14 represents the period (i), that is, the distance that the carriage 14 has moved to reach the position of the carriage just before it.

  At that time, the balance of energy over each period (i) is as follows.

ここで、ＲＭは質量体Ｍの質量体中心の変位の半径であり、ｈは、ホイール間（Ｒ２、Ｒ３及びＲ４、Ｒ１；すなわち点Ｃと点Ｄの間（循環路下降部分２６）及び点Ｇと点Ｈの間（循環路上昇部分２８））で摩擦が生じないような質量体（及び台車）が移動する垂直距離であり、ｇは地球の重力場の加速定数である。 1-potential work

Here, RM is a radius of displacement of the mass body center of the mass body M, and h is between the wheels (R2, R3 and R4, R1; that is, between point C and point D (circulation path descending portion 26) and point G is the vertical distance traveled by the mass (and the carriage) that does not cause friction between G and point H (circulation path rising portion 28), and g is the acceleration constant of the earth's gravitational field.

ここで、Σ（Ｍ＋ｍ）_１２は循環路１２に沿って存在する全ての質量体の合計であり、Ｃｆはベアリングの摩擦係数である（異なる位置に対して異なる摩擦係数が考えられるが、この例では全て同じであると仮定する）。 2- resistance work (friction between points; the carriage 14 assumes that there is no internal rail Ri from point C to point D and from point G to point H (although it cannot), from point H Friction to point C and from point D to point G; then added to the following equation):

Here, Σ (M + m) ₁₂ is the sum of all mass bodies existing along the circulation path 12, and Cf is the friction coefficient of the bearing (although different friction coefficients can be considered for different positions, this example Let's assume all are the same).

  This simplified formula (without considering the integrals due to centrifugal forces to be considered for accurate prediction) is a different parameter (M, m, Cf) that can fall within the resistance work calculation. , P, etc.) are given as examples. Actually, the calculation formula for resistance work varies depending on the circuit configuration, for example, the closed circuit is supported by the inner rail Ri between all points A, B, C, D, E, F, G, and H. Or only along the part from point H to point C, the weight of the mass (M + m) is supported by the external rail Re between points C, D, E, F, or h And according to the shape of the closed circuit (see FIG. 5) determined by the actual value of L. The goal of the resistance work Wres equation above is to show that the parameters used in the equation (M, m, Cf, P, etc.) can be selected to minimize the resistance work.

である。この仕事Ｗ（＋）は、Ｍ、ｍ、Ｃｆ、ｈ、Ｌ、ｒ及びＲＭのサイズの選択次第で正になり得る。 At this time,

It is. This work W (+) can be positive depending on the choice of size of M, m, Cf, h, L, r and RM.

  L is between wheels (R1, R2 and R3, R4; that is, between point A and point B (circulation path upper part 22) and between point E and point F (circulation path lower part 24). )) Horizontal distance, and r is the radius of the wheel (R1, R2, R3, R4).

  3-At the beginning of each cycle (i), the circulation path 12 is attached to the circulation path 12 at the upper point A, and due to the attachment / detachment of the mass body M near the lower point F, [(1 / 2) Lose a large amount of energy equal to * M * Vcir (i-1) ^ 2], and the circulation path becomes [(1/2) * M * Vcir (i) ^ 2] during period (i). An equal amount of energy is supplied to the mass body. The mass M has its own kinetic energy (WMA (i): the energy of the mass M at point A during period (i)) so as to be mounted on the empty carriage 14, and the upper point A To reach. The mass energy WMA (i) will be subtracted from the energy supplied by the circulation path 12.

  The mass body M leaves the carriage 14 at a lower point F as shown in FIG. 3 while maintaining the same speed Vcir as the speed of the circulation path 12. As shown in FIG. 4, by having a mass track 30 of the mass guidance system for upward displacement outside the circuit 12, the mass M is typically returned to the upper point A. It follows a substantially circular arc of radius R, preferably a semicircular curve.

  The mass body M takes the mass track 30 in a function of the speed of the mass body M when leaving the lower point F, that is, in a function of the speed Vcir of the circulation path when the mass body M is detached from the carriage 14. Thus, the height up to the upper point A of the circulation path 12 can be obtained. Therefore, when the mass body M is desorbed, the mass body M can reach the upper point A at a speed VMA larger than [√ (g * R)] ([SQUARE ROOT (g * R)]). The speed Vcir of the circulation path needs to exceed a predetermined value necessary for this.

Actually, in order for the mass body M to reach the upper point A, the velocity of the mass body M at the lower point F is at least the gravitational weight of the mass body M at the upper point A (gravity of the earth). It must be allowed to have a centrifugal force equal to.

の質量体Ｍの離脱運動エネルギーが得られるように、十分なエネルギーを加えることによって、少なくとも［（１／２）*Ｍ*ｇ*Ｒ］に等しい運動エネルギーを有して質量体Ｍが上方点Ａに到達しなければならないということである。 What this means is to raise the mass M by [2 * M * g * R] as a height equal to (2 * R), ie its potential energy increase, and the curve R of the mass track 30 In order to include the amount of energy WfM required to counter friction along the friction (friction due to the weight of the mass and centrifugal force), therefore

By adding sufficient energy so that the detachment kinetic energy of the mass body M is obtained, the mass body M has the kinetic energy at least equal to [(1/2) * M * g * R] A must be reached.

に等しくなければならない。 Therefore, the speed of separation of the mass body M from the lower point F, that is, the speed VMF of the mass body M when the mass body M desorbs from the circulation path 12 at the lower point F is at least

Must be equal to

ここで、Ｎｈは、点Ｃと点Ｄの間及び点Ｇと点Ｈの間の周期的距離Ｐの数であり、Ｖｃｉｒ（ｉ−Ｎｈ−２）は、下方点Ｆで循環路から脱着されるときの質量体Ｍの速さ（ＶＭＦ）である。 From there, in general,

Here, Nh is the number of periodic distances P between point C and point D and between point G and point H, and Vcir (i−Nh−2) is desorbed from the circulation path at the lower point F. This is the speed (VMF) of the mass body M at the time.

  While the mass body M returns to the upper point A, the mass body M does not affect the behavior of the circulation path 12. That is, when the mass body M is detached from the circulation path 12 at the lower point F, the mass body M and the circulation path are completely independent from each other.

4- Input of external energy to the circulation path:

5- (Another Embodiment) External energy Wmag (i) to the mass M at the height of the storage unit 40 (details will be described later) when mounted on the circulation path at the upper point A during the period (i) Input.

と書ける。 The energy balance equation for the circuit is

Can be written.

  Note: This equation is true when there is a large amount of energy equal to Wmag (i) supplied to the mass M when mounted on the carriage 14 at the upper point A.

とも書ける。ここで、Ｗｃｉｒ（ｉ）は、周期（ｉ）の終わりの循環路のエネルギーの総量である。 The equation for the energy balance of the circuit (depending on the cycle) is

You can also write. Here, Wcir (i) is the total amount of energy in the circulation path at the end of the period (i).

  Actually, because the circulation path 12 is removed from the circulation path at the lower point F by W0 and returns to the circulation path at the upper point A, and these mass bodies M return to the mass track 30 (see FIG. 6). When the speed V0 exceeding the minimum speed Vcir (min) required to start following the reference is reached, the work W0 is no longer supplied to the circuit as long as W (+) is positive (greater than 0).

  W (+) = Wpot−Wres, and Wpot is equal to [M * g * RM] when the first mass body M is desorbed, and [M * g when the second mass body M is desorbed. * (RM + P)], equal to [M * g * (RM + (2 * P))] when the third mass M is desorbed, and Wpot = M * g until Wpot reaches the maximum value. Recall that * (h + (2 * RM)) [h = Nh * P].

  In the functional principle of the machine 10 (the subject of the present invention), W (+) must be positive and it is possible to hold or change the value of W0 in order to increase the energy gain.

とする。 Less than,

And

に等しい多量のエネルギーを質量体Ｍに供給しなければならなかったことを忘れてはならない。 Therefore, in each cycle (i), a large amount of energy equal to W (+) is added to the circuit 12, but to apply this condition, at the beginning of cycle (i)

Remember that a large amount of energy equal to must have been supplied to the mass M.

  Wmag (i) is then equal to the energy lost by circuit 12 when mass M is desorbed at lower point F, which is desorbed from the circuit in period (i-Nh-2) Less than the kinetic energy WMA (i) recovered by the system for mounting the mass body at the upper point A of the circulation path 12 from the mass body M reaching the storage unit 40 [(1/2) * M * Vcir (i− 1) Equal to ^ 2].

  Therefore, a large amount of energy equal to Wmag must be input to the circuit in each period (i) so that the circuit 12 can acquire each period (i) due to the potential energy from the mass M. However, after a certain number of cycles, the total amount of energy Wmag supplied exceeds the amount of energy stored in the circulation path 12. This means that during each period (i), the amount of energy W (+) applied to the circuit 12 during each period (i), which increases the circuit speed Vcir, is constant. This is explained by the fact that the amount of energy Wmag supplied to the circulation path 12 increases with its speed. Further, Wmag reaches the value of Wpot by its own kinetic energy when the speed of the circulation path 12 reaches the minimum value necessary for the mass M to travel along the mass track 30 all the time. From there, it is required to intervene the existing centrifugal force (the value of which depends on the speed of the circuit) to add additional energy to the circuit, which leads to the next.

  B-System for utilizing centrifugal force

  Referring to FIG. 8a, the mass M following the circular trajectory tends to naturally follow a linear trajectory that is the tangent of the circle it describes, and the mass M is then between the mass M and the center of rotation (o). It is well known that due to the centripetal force due to physical links, it is forced to follow a circular orbit.

  When this link breaks, there is no centripetal force and the mass M is no longer forced to follow a circular trajectory. This is explained by the fact that the mass, when free, follows a straight orbit that is tangent to the circle because of its stored energy.

  Here, referring to FIG. 8b in which the frame ox-y is connected to the rod (ab), the mass M has an angular velocity [Vy (M (a)) / r] and an angle Ψ. An example of free-sliding is shown along a rotating rod (ob) indicated by, where the first position is indicated by a dotted line and the second position is indicated by a solid line. Thus, between points (a) and (b), without physical connection to be held radially with respect to the center of rotation so as to eliminate centripetal force with respect to the center of rotation (o), There is a mass M. Conversely, the mass M will have to follow its rotation for its sliding attachment to the rod (ob), which moves from point (a) to point (b). It will be subjected to a centrifugal force pulling it along the rod (ob). This centrifugal force is the axis (o-x) (x = o-M is the distance from the center (o) to the mass M), and the position of the mass M along the straight line (tangent line). ) Because it depends on the velocity Vy (M (x)), it is variable and the two parameters vary between point (a) and point (b).

  To better explain, in the more specific case, the following calculation is obtained from the schematic of FIG.

  When Ψ = 0, the straight line (tangential) velocity of the mass M is equal to Vy (M (a)). Accordingly, the mass M has a tangential kinetic energy of [Ecy (M (a)) = (M * Vy (M (a)) ^ 2) / 2]. The mass M also has only one degree of freedom (translation along the rod (ob)), so at the point (A) [Ecx (M (a)) = (M * Vy (M (a)) ^ 2) / r], where (r) is the distance (oa) along the axis (ox).

になり、その直線速度は

になる。というのも、角速度Ｖｙ（Ｍ（ａ））／ｒは一定のままであるからである。この増分変位の間、質量体Ｍに運動エネルギーが加えられる。そのときこの点で、質量体Ｍの運動エネルギーは、

でなければならない。 The mass M under the influence of the centrifugal force Fcx (M (a)) moves Δx (delta (x)) toward the point (b) with respect to the rotation increment of ΔΨ (delta (Ψ)). Then the radius of rotation is

The linear velocity is

become. This is because the angular velocity Vy (M (a)) / r remains constant. During this incremental displacement, kinetic energy is applied to the mass M. At this point, the kinetic energy of the mass M is

Must.

の点ｘ＝（ｒ＋Δｘ）で遠心力を受けることを示唆している。 This is because the mass M is then

It is suggested that the centrifugal force is received at the point x = (r + Δx).

と書くことができる。ここで、Ｇ（ｘ）は、ロッド（ｏ−ｂ）またはフレーム（ｏ−ｘ−ｙ）内の軸線（ｏ−ｘ）に沿った遠心力に起因する質量体Ｍの加速度である（図８ｂを参照）。従って、

At this time,

Can be written. Here, G (x) is the acceleration of the mass M caused by the centrifugal force along the axis (ox) in the rod (ob) or the frame (ox) (FIG. 8b). See). Therefore,

  Since the tangential velocity Vy (M (a)) is constant, it is possible to obtain the amount of time necessary to produce a rotational increment of ΔΨ.

が与えられる。 Generally, since [V = L / t], [t = L / V],

Is given.

The position x (M (x)) of the mass M and its velocity Vx (M (x)) along the axis (ox) are obtained as a function of ΔΨ.

である。 Since the radial velocity Vx (M (a)) of the mass M at point (a) (at angle ψ = 0) is null [Vx (M (a)) = 0], the first angular increment of Δψ for

It is.

である。 And for the next angle increment,

It is.

になる。 Using these two equations, following the mass M's trajectory for a determined rotation angle, its velocity at the longitudinal tip of the rod (ob) and when it is detached from the rod. Can be calculated one by one. The velocity of the mass is therefore the vector sum of its tangential velocity Vy (M (b)) and the normal or radial velocity Vx (M (b)):

become.

になる。 And the kinetic energy of the mass body is

become.

の運動エネルギーの量として質量体Ｍに供給されなければならなかった。 To keep the angular velocity constant, a large amount of tangential energy is

Must be supplied to the mass M as the amount of kinetic energy.

  This amount of energy is part of the mass energy at point (b), and is the kinetic energy Ecx (M) of the mass M along the axis (y) [Energy conservation law] Furthermore, there is kinetic energy Ecx (M) due to centrifugal force.

  The kinetic energy Ecx (M) resulting from this excess centrifugal force will be utilized in the circuit 12 of the present invention in two different ways, which will be described later, and is therefore shown schematically in FIGS. 9a and 9b. Such a carriage 14 is considered.

  Figures 9a and 9b are in a closed and unfolded form, respectively (of many possible other embodiments) of a carriage 14 made up of two main parts, a fixed part 14f and a movable part 14m. ) An embodiment. The fixed portion 14f is typically provided with a bearing 16 that allows it to follow the track of the inner rail Ri, and the movable portion 14m is typically telescopic (or nested) or similarly. As a single degree of freedom, each fixed portion 14f is moved by a parallel movement substantially perpendicular to the axis 16a passing through the rotation center of the bearing 16f of the fixed portion 14f of the carriage and substantially perpendicular to the track at a specific location of the inner rail Ri. Connected. The movable portion 14m is a portion that selectively receives the mass body M attached to it by a mechanical system or the like (not shown). A mechanical mounting system such as an external rail Re (shown in FIGS. 9a and 9b for illustration only) or the like, on which the bearing 16m of the moving part 14m of the carriage and / or the bearing of the mass M 20 (which depends on the position of the carriage or movable unit (cart + mass M) along the circulation path 12) rolls the two parts 14f, 14m of the carriage in close proximity to each other, Further, in a predetermined curved portion of the circulation path 12, it is possible to freely expand the fixed portion 14f along the trajectory determined in advance by calculation of the mass body M and / or the movable portion 14m. .

  Example embodiments of a system for utilizing centrifugal force

  In the next paragraph, each of the different points A, B, C, D, E, F, G, H of the circuit is marked with “i” and “e”, respectively. The corresponding height (level) of the inner rail Ri and the outer rail Re can be identified at a point A) including Ai and Ae.

  FIG. 10 shows an example embodiment of a system for utilizing centrifugal force according to the present invention incorporated on the circuit of FIG. Immediately after the upper part 22 of the circuit 12, in the upper zone Zs at the end point B, the system for utilizing the centrifugal force has a typical angle of 180 ° (π radians) that is part of the system (any other angle is It is placed in a circular part that utilizes the centrifugal force of the mass M on the curved part of the circuit 12. Therefore, the external rail Re has the shape Be-Ce (the trajectory is calculated one by one so that the component Rt of the reaction R on the mass M caused by the centrifugal force Fc that is tangent to the trajectory is as large as possible. Can be changed). Centrifugal force Fc is based on a mass body unit (Mcm + M) movable in the radial direction (mass body + mass body M of movable part 14m of carriage 14), a separation distance from the rotation center to the mass body, and a circulation path speed Vcir. It is. The only requirement is that this trajectory is in a trajectory that the mass unit (movable part 14m + mass M) can follow without any radial (normal) obstacles. That is. This condition ensures a permanent contact with the outer rail Re, which causes a reaction Rc therefrom that acts on the mass unit. This reaction R can be decomposed into a normal (radius) direction force Rn that opposes the deployment of the movable portion 14m of the carriage with respect to the corresponding fixed portion 14f, and another tangential force Rt. The force Rt is in the same direction as the direction of movement of the circulation path 12 that will generate work in addition to the work from the weight force of the mass M along the descending portion 26 of the circulation path 12. is there.

  註:

  -The centrifugal force is the part Bi-Ci (of the inner rail Ri) as well as the work it generates and the work caused by the displacement of the mass unit (movable part 14m + mass body M) relative to the fixed part 14f of the same carriage 14. Is always perpendicular to the track of the inner rail Ri of the circuit 12, so that this work is completely independent of the work of the circuit 12.

  -The separation of the mass unit from the center of rotation of the wheel R2 increases the mass unit tangential speed and thus its kinetic energy. This energy is taken from the circuit energy, but from the law of conservation of energy, it is returned to the circuit from the beginning of the descending portion 26 from the point Ci to the point Ce.

  -Since the generated work is null between the points B and C, the force due to the weight of the mass unit is not taken into consideration.

  Along the descending portion 26, the external rail Re brings the mass unit once again into contact with the fixed part 14f of the carriage, while adding the mass M to the mass of the movable part 14m of the carriage, and the gravitational acceleration constant of the earth Multiply (g) by the friction coefficient Cf and absorb a large amount of energy due to friction equal to the horizontal distance between points Ce and De.

  Other examples of embodiments of systems for utilizing centrifugal force

  FIG. 11 shows another example of an embodiment of a system for utilizing centrifugal force according to the present invention incorporated on the circuit of FIG. Immediately after the lower part 24 of the circuit 12, in the lower zone Zi at the lower point F, the system for utilizing the centrifugal force is typically part of the system in such a way as to extend the lower point F to the point G. It is placed in a circular part that utilizes the centrifugal force of the mass M on the curvilinear portion of the circuit 12 at an angle of 180 ° (π radians) (any other angle is possible). Thus, to release the mass unit that is accelerated due to centrifugal force, the outer rail Re ends at point Fe (point F is at the height of the outer rail Re) and it is removed from the center of rotation of the wheel R4. keep away. This displacement remains generally perpendicular to the trajectory of the inner rail Ri between the points Fi and Gi, so that the work caused by this displacement does not depend on the work of the circuit 12, and under these conditions the mass unit Of point Fe and point Ge under the action of two velocities: tangential velocity V′cir [V′cir = Vcir * r (Mmc + M) / r] and normal velocity or radial velocity Vc due to centrifugal force. Move along the trajectory between. At the point Ge ′ near the point Ge at the beginning of the mass track 30, the mass unit desorbs the mass M from the movable part 14m of the carriage without restriction on the displacement of the mass (mass body). The desorption system passes through a machine base or the like.

When the mass M is desorbed, it is at the beginning of the mass track 30 that its inlet portion has always been maintained, typically automatically, tangential to the direction of motion of the mass M. The direction of motion of the mass M is a function of the direction of its velocity VMGe ′ at the point Ge ′ when it is detached from the movable part 14m, ie a vector of two velocities V′cir and Vc that are always perpendicular to each other. It is sum.

に等しい運動エネルギーを有して質量体トラック３０に入る。 At this time, the mass M is

Enters the mass track 30 with a kinetic energy equal to.

  When the mass body M is detached from the movable portion 14m of the carriage, the movable portion 14m is in contact with the external rail Re by the bearing 16m at the point Ge (this contact occurs after the mass body M is removed therefrom). There must be). When rising along the rising portion 28 of the circulation path 12 between the point Ge and the point He, the outer rail Re brings the movable portion 14m into contact with the corresponding fixed portion 14f again, and the outer rail Re is rotated by one cycle (i ) The mass of the movable part 14m is multiplied by the gravitational acceleration constant (g) of the earth, the coefficient of friction Cf, and the energy resulting from friction equal to the product of the horizontal distance between the point Ge and the point He is absorbed. To do.

となり、

となる。ここで、Ｗｒｅｓは循環路１２に沿った摩擦力によって浪費されたエネルギーであり、Ｗ［Ｆｃ（Ｂｅ−Ｃｅ）］は点Ｇｅと点Ｃｅの間の遠心力によって発生するエネルギーであり、

である。ここで、ＷｆＭは、質量体トラック３０に沿って摩擦力によって浪費されたエネルギーである。 Both embodiments of the system for utilizing centrifugal force described herein can also be used on the same circuit as schematically shown in FIG. 12, where the work balance of the machine 10 is

And

It becomes. Here, Wres is the energy wasted by the frictional force along the circulation path 12, and W [Fc (Be-Ce)] is the energy generated by the centrifugal force between the points Ge and Ce,

It is. Here, WfM is energy wasted due to frictional force along the mass track 30.

  In all cases shown in FIGS. 10, 11 and 12, as soon as [Wcir (i) −Wcir (i−1)] becomes positive and remains positive, the external energy W0 is temporarily input. Can be stopped.

  Operation of the machine of the present invention

  Step a:

  With the input of the external energy W0, the speed of the circuit 12 is a predetermined value greater than the required minimum speed Vcir (min) that allows the value [Wcir (i) −Wcir (i−1)] to be positive. The speed is increased to Vpre (in function of different physical parameters of the machine 10 and the closed circuit 12).

  Step b:

  In the embodiment shown in FIG. 10, when the circuit 12 reaches a predetermined speed Vpre, the mass body desorption system is typically activated automatically, and the mass body at a lower point F of the circuit 12. M is detached from the carriage 14 and the movable part 14m of the carriage is detached from the fixed portion 14f only between the points Be and Ce.

  In the case of the embodiment shown in FIG. 11 and partly in FIG. 12, every time the mass unit reaches the point Ge ′ at the beginning of the mass track 30 when the circulation path 12 reaches a predetermined speed Vpre. The mass body desorption system is typically activated automatically to desorb the mass body M from the movable part 14m of the carriage 14. Typically, in these cases there is no need for a special system for connecting and disconnecting the fixed part 14f and the movable part 14m of the carriage from each other, which is typically provided by the outer rail Re. .

  Step c:

  As soon as the first empty carriage 14 reaches the upper point A of the circulation path 12, the mass body mounting system is activated and typically automatically reaches the mass body M to the upper point A of the circulation path 12. Attach to each empty trolley. Also, the mass body mounting system, after traveling along the mass body track 30, has a lower point F or Ge ′ (according to the system for utilizing the centrifugal force shown (FIG. 10 or FIG. 11 or others)). The kinetic energy WMA of each mass body M reaching the storage unit 40 is recovered. In the case shown in FIG. 10, the mass body mounting system gives the mass body M the same speed reached by the circuit Vcir using the input of the external energy Wmag as long as needed.

  Step d:

  It is preferable to stop or change all external energy inputs as soon as possible.

  Step e:

  When the target work value is reached, there is a selective coupling of the machine 10 to the loading machine.

  註:

  -Multiple machines 10 can be coupled to the same loading machine.

  -Referring to Figs. 5a to 5d, depending on the values of h and L, i.e. whether they are 0, the circuit 12 may have different configurations as shown. Furthermore, when h = 0, the masses M can be completely detached from their respective carriages 14 before ascending towards the upper point A, as shown in FIGS. 5c and 5d. The body track 30 is preferably arranged slightly laterally apart by a distance I from the upper and lower parts 22, 24 of the circulation path 12.

  Alternative form

  Although the closed circuit 12 disclosed above and shown in the drawings is in a generally vertical plane, those skilled in the art will recognize that any other closed circuit having only a portion thereof located in a non-horizontal plane of the present invention. It will be readily appreciated that it is considered not to depart from the scope.

  It is also clear that many technical solutions can significantly reduce the coefficient of friction, which in turn will reduce the resistance work (Wres). For example, instead of using the roller bearing 16, the carriage 14 can be moved over oil or compressed air, or can be levitated away from the inner rail using permanent magnets or the like.

  In a different way, as in the case of FIG. 10, the masses M are partially detached from their respective carriages 14 when they reach the starting point E of the lower circulation path 24, and the lower part 32 of the mass truck 30. Can begin to roll (see FIGS. 4, 6, and 7). A mass bearing M (not shown) is attached to the carriage so as to rollably push the mass M along the track lower part 32 so that it can be completely detached from the carriage at the lower point F. They will remain partially attached to their carriages 14.

  The mass body mounting system for mounting the mass M on each carriage 14 near the upper point A can be achieved in different ways as described in the following examples, without intending to limit it in any way.

である。 a—as shown schematically in FIG. 6, typically driven horizontally by the circuit 12 itself or attached to the circuit 12 itself to operate at a speed substantially equal to the circuit speed Vcir. By using the storage 40 of the mass body M to operate. This is because the mass body M desorbed from the lower point F is stored in the storage unit 40 (where its kinetic energy is recovered) in the mass body M having input external work (as in the case of FIG. 10). The mass M is easily applied to each empty carriage 14 that reaches the upper point A by supplying a large amount of energy that will allow it to reach the speed of the circulation path 12 when placed in Can be attached (inserted). The only condition for such a configuration is the number of mass bodies M in the storage 40 shown in dotted lines in FIG. 6 (in addition to the mass bodies M mounted on the circulation path 12 along its length completely). Would have to be at least equal to the distance d separating the positions of the empty carriages 14. From there, each mass body M is desorbed from each mass body M at the lower point F when each mass body M reaches the upper point A divided by the periodic distance P of period (i). . In other words,

It is.

  This solution can prove particularly suitable when h = L = 0 or L = 0 (see FIGS. 5b and 5d).

である。 The b-mounting system typically has a speed ratio Rv = (d + P) / to the circuit speed Vcir so that the mass M is moved from the upper point A to the empty carriage 14 at the system speed Vsys = Rv * Vcir. It includes a mass transport mechanism 42 with two equidistant arms 44 separated by a distance d + P, as driven by P by an external work Wmag (as in FIG. 10). In this case, as schematically shown in FIG. 7, the frictional force resulting from the weight of the mechanism on its own rotating shaft 46 is the friction of resistance work (Wres) when summed up. The conditions necessary for this mechanism to be realized are:

It is.

  In a different embodiment, as applicable in FIG. 11, the carriages 14 to which their masses M are attached by means of a mechanical system (not shown) do not roll on the inner rail Ri when applicable. By being releasably attached to it, it is possible to turn around four wheels R1, R2, R3, R4, which are directed against the wheel and in the axial direction, generating considerable friction and centrifugal force. Let In this way, the effect of the friction caused by the centrifugal force on any external rail Re is eliminated, so that everything is simplified to the problem of dealing with the problem of friction forces acting on the rotating shaft of the wheel. This simplified problem can easily be solved by a pressurized oil film. With such a solution, the closed circuit can generate a high speed and its high level of force.

  Although not shown herein, a plurality of similar closed circuits 12 are preferably arranged parallel to each other to drive a common output shaft coupled to one or more loading machines. Which is the force available on the output shaft multiplied by multiple circuits.

  As stated at the beginning of the description, the closed circuit 12 has at least one curve of the circuit (without considering the conversion of the mass body potential energy to kinetic energy) without departing from the scope of the present invention. It will be apparent to those skilled in the art that while having a system for utilizing centrifugal force on the part, it can be located generally in a horizontal plane.

  Although the present invention has been described with somewhat detailed embodiments, the disclosure has been made by way of example only and the invention is limited to the features of the embodiments described and illustrated herein. Not all variants and modifications are based on the principle of centrifugal force utilization, and optionally on the principle of gain of potential energy, as the subject of the invention claimed below. It should be understood that it is included within the scope and spirit of the present invention.

Claims (28)

A machine (10) for generating mechanical energy,
By the input of external energy (W0), at least temporarily around the at least one free wheel (R1, R2, R3, R4) is rotationally driven, and a plurality of mass bodies (M) move along themselves. A closed circuit (12) that is selectively mounted as follows:
A system for guiding the mass body (M) along the circulation path (12) so that the mass body can move along the circulation path (12);
Positioned on at least one curved portion of the closed circuit (12) for applying energy different from the input of the external energy (W0) to the circuit (12) from the centrifugal force of the mass (M). And a system for utilizing centrifugal force of the mass body.   The system for utilizing the centrifugal force of the mass body allows the mass body (M) to move substantially radially when in the at least one curved section. The machine (10) of claim 1. The mass body (M) is selectively attached to the closed circuit (12) between its relative upper point (A) and its relative lower point (F), and the upper side in the gravity field of the earth. During the fall from the point (A) to the lower point (F), kinetic energy resulting from the conversion of the potential energy of the mass body is supplied to the closed circuit (12), and the guidance system From 12), the mass (M) can move from the lower point (F) to the upper point (A) while being desorbed using at least its own kinetic energy at the lower point (F). A mass track (30) adapted to, the machine (10) comprising:
In order to selectively maintain the closed circuit (12) to a permanent dynamic imbalance, the mass (M) is removed from the closed circuit (12) at a position adjacent to the lower point (F). A system for desorption,
In order to selectively maintain the closed circuit (12) to a permanent dynamic imbalance, the mass (M) is placed in the closed circuit (12) at a position adjacent to the upper point (A). Including a system for wearing,
Machine (10) according to claim 1, characterized in that the at least one curved part of the closed circuit (12) is at least partly located between the upper point (A) and the lower point (F). ).   The machine (10) of claim 3, wherein the mass track (30) includes a substantially arcuate portion extending between the upper point (A) and the lower point (F).   The machine (10) of claim 4, wherein the mass track (30) includes a generally semi-circular portion extending between the upper point (A) and the lower point (F).   The closed circuit (12) includes a lower portion (24) ending at the lower point (F), and the mass track (30) along the mass body before reaching the lower point (F). The machine (10) of claim 4, comprising a lower track portion (32) that selectively and movably supports (M).   The mass track (30) is immediately after the system for utilizing the centrifugal force of the mass (M) and is on the trajectory of the mass (M) exiting the system for utilizing the centrifugal force. 5. A machine (10) according to claim 4, characterized in that it is oriented substantially tangential to the machine.   The guidance system includes a subsystem for selectively holding the mass (M) along the closed circuit (12) at least between the upper point (A) and the lower point (F). A machine (10) according to claim 4, characterized in that   The guidance system selectively accepts the mass (M) internally along the closed circuit (12) between the upper point (A) and the lower point (F); Including a plurality of mass carriages (14) that can be moved around one wheel (R1, R2, R3, R4), wherein the holding subsystem comprises the upper point (A) and the lower point (F) The machine (10) of claim 8, characterized in that the mass (M) is maintained in each of the carriages (14) between.   Each carriage (14) is along the at least one wheel (R1, R2, R3, R4) along the closed circuit (12) between the upper point (A) and the lower point (F). The movable part (14m) is closed with the fixed part (14f) and the movable part (14m) being close to each other. The movable part (14m) is movable in a radial direction with respect to the fixed part (14f) between the unfolded forms separated from the fixed part (14f). Machine (10).   When the carriage (14) is on the at least one curved section, the movable section (14m) of the carriage (14) is selectively and freely radially from the closed configuration to the deployed configuration. The machine (10) of claim 10, characterized in that it is movable.   12. A machine according to claim 11, wherein the desorption system includes a release mechanism for selectively desorbing the mass (M) from each of the carriages (14) in the vicinity of the lower point (F). 10).   The closed circuit (12) includes an upper part (22) starting from the upper point (A) and ending at an upper end point (b), and the mounting system includes the upper point (A) and the upper end point (b). Machine (10) according to claim 12, characterized in that the mass (M) is mounted on the closed circuit (12) at a position in between.   The mounting system includes a mass body storage unit (40) for receiving the mass body (M) detached from the lower point (F) in the vicinity of the upper point (A), and the mass body storage unit ( 40) temporarily includes at least one of the desorbed mass bodies (M) between the upper point (A) and the upper end point (b) and the at least one desorbed mass The body (M) is turned into an empty carriage among the plurality of carriages (14) such that each mass body (M) of the desorbed mass body (M) reaches the upper point (A). 14. Machine (10) according to claim 13, characterized in that it is mounted.   The system for mounting a mass body recovers at least a portion of the kinetic energy of the mass body (M) desorbed from the lower point (F) when it reaches the storage (40). The machine (10) of claim 14, characterized in that:   The system for mounting a mass body uses an input of a work (Wmag) outside the circulation path (12), and each mass body (M) at least sets the speed (Vcir) of the circulation path when mounted. 15. A machine (10) according to claim 14, characterized in that it can be provided.   The mounting system receives the desorbed mass (M) from the lower point (F) in the vicinity of the upper point (A) between the upper point (A) and the upper end point (b); Of the desorbed mass bodies (M), the received mass bodies (M) are moved so that each mass body (M) of the desorbed mass bodies (M) reaches the upper point (A). The machine (10) of claim 13, further comprising a mass transport mechanism (42) for mounting on an empty carriage of the plurality of carriages (14).   The release mechanism is selectively activated when the velocity of the mass (M) at the lower point (F) is equal to or greater than a predetermined value (Vcir (min)), thereby Machine (10) according to claim 12, characterized in that it ensures that the mass (M) has sufficient kinetic energy to reach the upper point (A).   The machine (10) of claim 1, wherein the masses (M) are spaced equidistant from each other along the closed circuit (12).   The kinetic energy supplied to the closed circuit (12) is consumed by frictional forces of the plurality of mass bodies (M) at respective relative displacements along it, and near the upper point (A) The machine (10) of claim 3, wherein the machine (10) is greater than resistance work (Wres) including work consumed by the mass mounting system for mounting each of the mass bodies (M).   When the system for desorbing a mass body reaches the upper point (A) when the mass body (M) reaches the upper point (A), the velocity of the circuit (12) using an input of external energy (Wmag) The machine (10) of claim 3, wherein the machine (10) is accelerated to a speed approximately equal to (Vcir).   The system for desorbing the mass body, the system for mounting the mass body, and the system for utilizing the centrifugal force of the mass body, the circulation path (12) has reached a predetermined speed (Vpre) Machine (10) according to claim 3, characterized in that it is only activated at a time. A machine (10) for generating mechanical energy,
A closed circuit (12) located around one or more rotating freewheels (R1, R2, R3, R4), having a plurality of mass bodies (M) moved along it, external Driven movably until a predetermined speed (Vpre) equal to or greater than the minimum speed (Vcir (min)) is reached using at least a temporarily maintained input of initial energy (W0) The closed circuit (12),
A system for allowing mass bodies (M) to be guided along their displacement along said closed circuit (12);
At least one curve of the closed circuit (12) to apply to the circuit (12) an energy different from the input of the external initial energy (W0) from the centrifugal force of the mass (M). A machine (10) comprising a system that enables the use of centrifugal force of the mass body (M) located in a section. While the mass body (M) is falling in the gravitational field of the earth, kinetic energy resulting from the potential energy conversion of the mass body (M) is supplied to the closed circuit (12), and the machine ( 10)
A system for detaching the mass (M) from the closed circuit (12) at its lower point (F) in order to maintain the closed circuit (12) to a permanent dynamic imbalance;
A system for attaching the mass body (M) to the closed circuit (12) at its upper point (A);
Using the kinetic energy from the speed of the mass body when desorbing from the closed circuit (12) at the time of desorption from the closed circuit (12) at the lower point (F), 24. The machine (10) of claim 23, comprising a system for adding the mass (M) to the closed circuit (12) at an upper point (A).   The system for attaching the mass body to the closed circuit (12) uses an input of external energy (W0, Wmag) to set the mass body (M) to the speed (Vcir) of the circuit when the mass body (M) is attached. 25. Machine (10) according to claim 24, characterized in that it can be reached.   A system that enables recovery by circulation of kinetic energy of the mass body (M) when the system for attaching the mass body (M) to the closed circuit (12) reaches the upper point (A). The machine (10) of claim 25, characterized in that it comprises.   24. The machine (10) of claim 23, wherein the shape of the circuit (12) causes a tangential reaction due to centrifugal force to add positive work to the moving component.   The shape of the circuit (12) is desorbed from the circuit (12) at the lower point (F) in addition to the kinetic energy generated by the speed (Vcir) of the circuit (12). 25. Machine (10) according to claim 24, characterized in that the mass (M) is allowed to have a large amount of energy, sometimes due to centrifugal forces.

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