JPS595889A - Power enlarging machine utilizing speciality of planetary gear mechanism - Google Patents

Abstract

PURPOSE:To increase the output of a motor by a method wherein a power, enlarged than the input thereof, is produced in the rotary body effecting planetary revolution utilizing the meshing effect of an internal gear, a gear, a sun gear and the like. CONSTITUTION:When a pulley 2, integral with a boss 1, the sun gear 11 and the like made four revolution, the gears 7, 8 make one revolution by three turns thereof along the internal gear 6, however, the whole of the machine makes one revolution at the same time. An external reaction with respect to the revolution of the machine is not existing at all, therefore, a canceling loss of the output due to the reaction is also not existing, and the machine converts the power, increased than the input therefor, into an electric power most efficiently in the machine under being revolved. The electric power is outputted to the outside of the machine as an electric current which has no resistance with respect to the revolution of the machine and, therefore, the output, stronger than the input, may be obtained by rotating the electric motor.

Description

DETAILED DESCRIPTION OF THE INVENTION OBJECTS OF THE INVENTION The present invention relates to a power multiplier that utilizes the special characteristics of a planetary mechanism. Whether power increase is possible or not should be considered as a mechanical issue. Therefore, there must be mechanisms that are possible and mechanisms that are impossible, but first I will explain the basis for why they are conventionally impossible. The increase in power is shown in Figure 44, Figure 4.
It is agreed that mechanisms such as those shown in Figure 5, Figure 46, Figure 47, etc. are theoretically and practically impossible no matter how they are combined, and this is common knowledge.
The explanation will be as follows in order to facilitate comparison with the planetary mechanism shown in FIG. 43, which is capable of increasing power. Figure 44 is axis (D)
is fixed at a certain position, and the center of integral wheels (F) and (H) with two steps of large and small circumferences is attached rotatably as shown in the figure, ((H) is twice as large as (F)). wheel CI-I
When the string is pulled in the direction of the arrow (B1) with a point (E) on the circumference of the wheel CF) as a point of emphasis, and in the direction of the arrow (A1) with a point (C) on the circumference of the wheel CF) as a point of emphasis. , arrow (
If the pulling force in the direction of arrow (A1) is 2 kg, then
) is balanced by 4 kg, which is the axis CD)
The radius (A) of wheel (F) from the center of is i of radius CB) of wheel (H), and the circumference of wheel CF) is g of (H). Therefore, force and circumferential distance are inversely proportional. This means that no matter what kind of mechanism you combine with the wheels (F) and (H) as gears, as long as the shaft (D) is fixed at a fixed position, force and distance are always inversely proportional, so it is impossible to increase the power. This proves that. Also, Figure 45 and Figure 46 are wheels (7)
This is the measurement of force and distance when moving on a plane. Place the wheel (7) in position (El) as shown in Figure 45,
Press the tip of the push rod (1) at the position of the apex (Dl),
When pushed in the direction of the arrow (Fl) and rotated once as shown in Fig. 46, the wheel (7) stops at the position (B2).This state is measured as follows. Starting point (E) of wheel (7)
The distance (C1) section from l) to the stopped position (B2) is the same as the circumference of the μ-ring (7), but the tip of the push rod (1) is the distance from the starting line (G1) to (G2). is in progress. This distance is twice the circumferential distance of the wheel (7) (B2)
The section is the distance traveled by the push rod (1) when it hits the wheel (7), and the section (A2) is the distance traveled without contacting the wheel (7). When measuring the force and distance in this state, the push rod (1) is placed at the apex (Dl) of the wheel (7) as the point of effort (A
2) (B2) While the wheels are traveling in section (B2),
) is (c) from the starting point (El) to (B2).
l) section, therefore, it is the cause of the (A2) (B2) section in which the push rod (1) has advanced. On the other hand, wheels (7
) is applied with twice the force of the push rod (1) that presses the top of the wheel (7). The force of pulling in the direction of the arrow (sl), focusing on the position (1) of the main wheel (7), is also the 2nd position of the push rod (1).
Acts twice. Of course, this is the case when the forces indicated by arrows (Sl) and (B2) are applied separately. Like this, the wheels (
7) When rolled on a straight line, force and distance are always inversely proportional. This is also considered to be one of the reasons why it is impossible to increase the power in the past. Therefore, this invention constructs a mechanism that makes it possible to increase the power after grasping the grounds that it was previously impossible.

Theory and experiments necessary to construct an invention.

This uses a planetary mechanism, and is different from the cases shown in FIGS. 44, 45, and 46, in which power cannot be increased by the action of force, but the extended distance of rotation is completely different. In other words, as shown in Fig. 43, the gear (7) is meshed with the internal gear (6) to expand the movement distance of the fulcrum CD (in this case, the inner periphery of the internal gear (6) is the fulcrum CD). On the other hand, as shown in Fig. 42, if the force gear (11) is made as small as possible, the moving distance of the force point (E) will be the distance between the force point (E) and the fulcrum CD). The difference becomes smaller and the rate of increase in power becomes larger. Analyzing this point is as follows.

Since the purpose of Figure 43 is to theoretically explain the possibility of increasing power, it is a disk to which the leg (5) fixing the central shaft (4) provided in the experimental mechanism and the gear (7) are attached. Frame (67)
is excluded. The central shaft (4) that is fixed in Figure 43
A gear (7) is meshed between a power point gear (11) and an internal gear (6) which are reversibly attached to the power point gear (11) and a gear (7).
) is the force point (E), and if you try to rotate the force gear (11) in the direction of the arrow (S), the gear (7) will be pushed by the force gear (11) in the direction of the arrow (B1). . On the other hand, when the point (C) of the gear (7) is pulled in the direction of the arrow (A1) with a string, the meshing point of the internal gear (6) and the gear (7) acts as a fulcrum (D). Comparing the forces of arrows (A1) and (BI) in this state, the force acting in the direction of arrow (B1) is 2kII, just as in the case of Fig. 44.
If so, the force acting in the direction of arrow (A1) is balanced by 4 points. However, when the power point gear (11) is rotated and the gear (7) is made to go around the internal gear (6), unlike the case shown in FIG. 44, the extended distance of force and rotation will not be inversely proportional. In other words, when considering the gear (7) as - lever gears, the relationship between the points of force (E), the point of emphasis (C), the fulcrum CD), etc. in Fig. 44 is as follows. Although the relationship is exactly the same as the above, by planetary rotation, the 43rd
The results shown in Fig. 44 are completely different from those shown in Fig. 44. This is the 44th
It can be seen that this is due to the difference between a mechanism in which the fulcrum (CD) is fixed at a fixed point for transmission as shown in the figure, and a mechanism in which the planets rotate simultaneously while moving the fulcrum (D) as in Fig. 43. If this planetary rotation is analyzed in Fig. 41, it will be as follows.In this figure, internal gear (6), gear (7), and power point gear (11)
The tooth parts such as these are omitted.

When the power point gear (11) is rotated in the direction of the arrow (8) and the gear (7) is moved one rotation from the position of the starting line (K1) in the direction of the arrow (S), the gear (7) moves to (K2). ) stop at the line. At this time, the power point gear (11) has the same number of teeth as the gear (7), so if it rotates once and rotates twice in the direction of mark (S),
Gear (7) stops at line (K3). On the other hand, the power point gear (11) rotates twice and further rotates between (Hl) and (H2), resulting in an immediate rotation. Also, connect the gear (7) to the starting line (K
When the gear (7) is rotated three times in the direction of the arrow (S) from the position 1), the gear (7) goes around the internal gear (6) and returns to the position of the starting line (K1). On the other hand, the power point gear (11) rotates three times and further meshes (Hl) (H2) numbers as the gear (7) moves. When meshing, if an input is applied to the power point gear (11) with 1 force and it rotates 4 times, the gear (7) rotates 3 times,
Since twice the force acts on the emphasis point (C) as on the emphasis point CB),
The input and output are as follows. ((Rotational speed of force gear (11) 4 x Force 1 - Human power 4° Rotational speed of gear (7) 3 x Force 2
= Output 6° Output 6 ÷ Input 4 = 1.5° °C Output is 1.5 times the input).

In the case of Fig. 42, the power point gear (11) is an apricot of the internal gear (6), so if the gear (7) rotates and goes around the internal gear (6), the power point gear (11) becomes 7 Rotates, so the input and output are as follows.

(Rotational speed of power point gear (11) 7 x Force 1 - Human power 7° Inner circumferential distance of internal gear (6) 6 x Force 2 = Output 12° Output 12 ÷ Input cuff = 1.7° Therefore, the output is 1 of the input. (more than 7 times)
.

Note that twice the force as the force point (B) acts on the circular line (R) at the center of the gear (7) shown in Fig. 43, as well as the point of force (C), but In a mechanism where the disc frame (67) and the Boo IJ- (76) are integrated, the Boo I
Even if you try to get an output from J-(76), the force and distance are always inversely proportional, so the output will not be greater than the input. Therefore, in the planetary mechanism, there is a bifurcation point between a mechanism that makes it possible to increase the power and a mechanism that does not. In order to prove the above theory, experiments such as those shown in FIGS. 37, 38, 40, 50, 51, and 52 were conducted, and the explanation will be given first from FIGS. 37, 38, and 40. 37 is a front view, FIG. 38 is a left side view of FIG. 37, and FIG. 40 is a right side view of FIG. 37. Tighten the two disc frames (67) together with the bolts (66) and nuts (15) shown in Figure 39 as shown in the figure, and then
As shown in Figure 9, the gear (7) and the gear (10) integrated with the boss (10)
8) Attach the boss (22) and the gear (21) integrated with it to the disc frame (67) with the shaft (9) as shown in Fig. 37, so that it protrudes from the left side of the disc frame (67). A snap ring (25) is used to prevent the protrusion of the shaft (9) from coming off.

The gear (19) integrated with the boss (2o) as shown in Fig. 22 meshes with the gear (21) as shown in Fig. 37, and the gear (27) integrated with the boss (28) and the boss (71) mesh with each other as shown in Fig. 37. The integral Boo'J- (73) is attached to the left side of the disc frame (67) with the shaft (24), and the end of the shaft (24) protrudes from the right side of the disc frame (67). Snap ring (25)
Attach it to prevent it from coming off. Gears (8), (21
) is integrated with the shaft (9) using the parallel key (65) as shown in FIG. 32, and the elastic body (
56) fitted as shown in FIGS. 33 and 34, the gear (7) is placed so as not to be fixed to the shaft (9). Gear (19) (
27), pulley (73), etc. are integrated with the shaft (24) using a parallel key (65), as shown in FIG. The gear (4') is passed through the center of the disc frame (67).
s) (7) is engaged with the internal gear (6) which is fixed to the base plate ('50) with the leg (53) as shown in Fig. 37 and Fig. 40, and as shown in Fig. 26 and Fig. 27 Boss (1) as shown in Figure 28
Power point gear (11) integrated with pulley (2) etc.
is attached to the right end of the center shaft (4), meshed with the gears (7) and (7) as shown in Fig. 37 and Fig. 40, and the power point gear (1
A pipe (12) is inserted between 1) and the disc frame (67) to prevent the aircraft from moving, and a pipe (60) is also fitted to the left end of the center shaft (4) to prevent the aircraft from moving. . Center axis (4)
Both ends are legs (
Attach it to the top of 5) as shown in the figure and secure it with the setscrew (3). The above is the experimental mechanism shown in FIGS. 37, 38, and 40. As explained in Fig. 41, if the force point gear (11) integrated with Boo IJ-(2) rotates four times, the rotation status is as follows: Gear (7) (8)F! 3 rotations and internal gear (6)
The disc frame (67) rotates once, but the gear (27) (19) and Boo! J-(73) is smaller than the other gears and is designed to rotate 4 times, the same as the power gear (11). Also, the rotation distance is the same as the power gear (11) (inner periphery distance of the internal gear (6)). The circumferential distance of the ten force point gear (11) is 4 rotations, while all the other gears are the internal gear (6 rotations).
) This mechanism was tested using the following method. Goo like figure 40! One end of the string (70) is hung on the shaft (72) fixed to I-(2'), the other end is connected to the meter (74), and the disc frame (67) is attached as shown in Fig. 37 and Fig. 38. The instrument (69) connected to the string (70) is hung on the shaft (68) fixed to the shaft, and the other end of the string (70) is hung on the shaft (72) fixed to the pulley (73). (
74) in the direction of the arrow (Sl), the disc frame (67) rotates in the direction of the arrow (N) due to gear transmission.At this time, if the scale of the meter (74) reaches 2 kg, the meter (69
) is 4 kg. This is because there is no external reaction to the rotating machine, and therefore there is no offset loss of output due to reaction, so the gear (7) explained in Fig. 43
This is thought to be the result of the leverage acting directly within the five aircraft. Next, the experiments shown in FIGS. 50, 51, and 52 will be explained. This mechanism is shown in Fig. 37, Fig. 38, and Fig. 40.
4) and the gears (19), (27) and pulleys (
73), etc., and the shaft (9) on the left side of the disc frame (67).
) has a long end, and a Boo IJ- (62) is fixed to it as shown in the figure, and everything else is the same mechanism as in Figures 37, 38, and 40. As shown in Fig. 50 and Fig. 51, the string (7o) is attached to the shaft (68) which is fixed to the disc frame (67).
The other end of the string (7o) is hung on the shaft (72) fixed to the boo IJ- (62), and the other end of the string (7o) connected to the meter (74) is attached. The end is the 52nd
Shaft (72) fixed to Boo IJ-(2) as shown in the diagram
When the instrument (74) is pulled in the direction of the arrow (Sl), the disc frame (67) rotates in the direction of the arrow (N).
At this time, if the scale of the meter (74) reaches 2 kg, the meter (69)
) will be 4 kg.

This is exactly the same result as the experiments shown in FIGS. 37, 38, and 40. In other words, since there is no external reaction to the rotating body, there is no offset loss of output due to reaction, and the fourth
It is thought that this is because the lever action of the gear (7) explained in Fig. 3 acts directly on the inside of the 5 aircraft, but Fig. 37 Fig. 38
The experiment shown in Fig. 40 and the experiment shown in Fig. 50, Fig. 51, and Fig. 52 show that although there are differences in gear transmission, the disc frame (67) and the gear (7) have the same results. ) (8) and the interlocking pulley (62), this is because the force acts on average as internal resistance of a single rotating body rotating around the central axis (4). I can think about it.

As proof of this, no matter where the instrument (69) is mounted on the disc frame (67), if you wrap the string (70) around the pulley (62) as shown in Figure 51 and make an inquiry, the instrument ( 74
) indicates 2 kg, the scale of the meter (69) indicates 4k.
g. That is, twice as much force acts on the meter (69) as on the meter (74). This experiment is the same even if performed using FIG. It is well known and common sense that the greatest loss of power is the offset loss of output due to the reaction of the operating machine.
In order to achieve the purpose of increasing power, we believe that it is necessary to directly connect the generator to the planetary mechanism, and to create a mechanical condition that eliminates the offset loss of output due to external reactions to the rotating aircraft. This invention is non-polluting and can generate even more power by connecting them one after another, so the main purpose of this invention is to create power sources everywhere.

Structure of the Invention This invention is constructed based on the above-mentioned theory and experiment. As shown in FIG. 10, FIG. 11, and FIG. (57)
Insert the cylinder (16) as shown in Figure 1, and press the edge (18)
And the disc frame (13) has four places around the rim with poles 1- (17)
and nuts (15), tighten the screws to unite them, and then
As shown in Fig. 9, Fig. 30, and Fig. 31, the gear (21) is integrated with the boss (22), the gear (8) is integrated with the boss (10), and the elastic body (56) shown in Fig. 35 and Fig. 36. As shown in Figure 34, the fitted gear (7) etc. are attached to the disc frame (13) and the support plate (
59) to the shaft (9) passing through it as shown in Fig. 1, and as shown in Fig. 32, use the parallel key (65) to connect the shaft (9) and the gears (21), (8). etc. are integrated, but the gear (7) is placed separately, and a snap ring (25) is attached to the shaft (9) protruding from the left side of the support plate (59) to prevent it from coming off. As shown in Fig. 22, the gear (27) integrated with the boss (28), the gear (19) integrated with the boss (20), etc. are connected to the disc frame (13) and the support plate (59) as shown in Fig. 1. ), the gears (21) and (19) are meshed, the gear (27) is attached to the left side of the support plate (59), and the parallel key is attached as shown in Figure 25. With (65), shaft (24) and gear (27) (19)
etc. are integrated, and the shaft (24) protruding from the right side of the disc frame (13) is prevented from coming off using a snap ring (25). As shown in Fig. 16, Fig. 17, and Fig. 18, the internal gear (26) with the bearing (54) fitted into the boss (55) is attached to the support plate (59) in the cylinder (16) as shown in Fig. 1. Figure 1, Figure 16, into the left side of the gear (27).
Mesh as shown in Figure 18.

The protrusion (58) of the disc frame (34) shown in FIGS. 7, 8, and 9 is fitted into the left end of the cylinder (16).
) and the disc frame (34).

The projection (33) on the left side of the disc frame (34) has a 19th
Ventilation holes (52) and (37) as shown in Figure 20 and Figure 21.
The gear (29) is connected to a generator (51) fixed to the shaft (51).
32) as shown in FIG. 1, and the gear (29) meshes with the internal gear (26). The left end of the generator (32) is fitted into the protrusion (36) of the disc frame (35) shown in Figure 4, Figure 5, and Figure 6 to connect the disc frame (35), (34) and cylinder (16). The edge (18) etc. are screwed together using the bold (31) and nut (15). In the end, the disc frame (35), (3
4), (13) and the cylinder (16) etc. are integrated, and the bearing (54) at the center of the disc frame (35), (34), (13) internal gear (26) etc. has a central shaft ( 4) through
Gears (7) and (8) are attached to the base plate (50) by means of legs (53).
) is meshed with the internal gear (6) fixed to the disc frame (1
The pipe (12) and the 26th center shaft (4) on the right side of 3)
As shown in Figures 27 and 28, the Boo! is integrated with the boss (1)! J-(2) and the power point gear (11) are installed, and the power point gear (11) is kept spaced by the length of the pipe (12) so that the power point gear (11) meshes only between the gears (7) and (7). . Insulator (3) fixed to the left side of the disc frame (35)
8) In order to prevent the movement of the aircraft, a pipe (60) is attached to the center shaft (4) as shown in Fig. 1 and Fig. 4, and a base plate (50) is attached to both ends of the center shaft (4). Attach it to the legs (5) that are fixed upright at both ends of the body and secure it with set screws (3). A conductive wire (39) drawn out from the generator (32) is connected to the current collecting ring (41) which is integrated with the insulator (38) fixed to the disc frame (35), and the current collecting ring (42) is a conductor (4o
) are connected as shown in Figure 4. At the bottom of the insulator (38), the insulator (45) is fixed to the position of the leg (5) as shown in the figure with a screw (49) as shown in Fig. 1 and Fig. 2. The brush (43) connected to the conducting wire (47) is connected to the current collecting ring (4
In 1), the brushes (44) connected to the conductor (48) are brought into contact with the current collection ring (42) and fixed with setscrews (46), and the conductors (47) and (48) are made long. and connect it to the electric motor. The above is the structure of a power multiplier that takes advantage of the special characteristics of the planetary mechanism.

Effects of the Invention To use this invention, the Boo IJ-(2) and the electric motor are connected with a belt to rotate the aircraft, and the rotation and force conditions at this time are shown in Figures 41 and 43. As explained above, the Boo U-(
2) If the power point gear (11) etc. rotates 4 times, the gears (7) (8)
) makes three revolutions inside the internal gear (6), and at the same time, the entire machine rotates once. At this time, the action of the elastic body (56) loaded in the gear (7) flexibly receives the reaction force of the aircraft at the time of startup, thereby alleviating the friction of the gear and shaft. ) always pushes in the direction of weaker force in an attempt to return to its original shape, so the loss of input is the least.
In addition, the effect of the force explained in Fig. 43 and the effects of the external force on the rotation of the aircraft as proven by experiments such as Fig. 37, Fig. 38, Fig. 40, Fig. 50, Fig. 51, Fig. 52, etc. Since there is no reaction from It is possible to generate a current that is equal to no resistance and send it to the outside of the aircraft to rotate the motor and produce an output that is stronger than the input. This invention can be connected one after another to obtain even more powerful power, and since it is non-polluting and can be easily installed anywhere, it will not be difficult to create a power source that can replace nuclear power generation. Think about it.

[Brief explanation of drawings]

Figure 1 is a front view of this machine, but it is used to show the inside.
A part of it was cut out. FIG. 2 is a left side view of FIG. 1, with part of the leg (5) cut away. Figure 3 is a right side view of Figure 1. FIG. 4 is a partially cutaway view of the disc frame (35) and the parts attached thereto. FIG. 5 is a left side view of FIG. 4, but is not cut away as in FIG. 4. FIG. 6 is a right side view of FIG. 4, but is not cut away as in FIG. 4. FIG. 7 is a front view of the disc frame (34). FIG. 8 is a left side view of FIG. 7. FIG. 9 is a right side view of FIG. 7. FIG. 10 is a front view of the cylinder (16), with a portion cut away to show the internal support plate (59). 11th
The figure is a left side view of Figure 1θ, but there is no cut section. FIG. 12 is a right side view of FIG. 10, but without the cut section. FIG. 13 is a front view of the disc frame (13). FIG. 14 is a left side view of FIG. 13. FIG. 15 is a right side view of FIG. 13. FIG. 16 shows the internal gear (26), which is partially cut away to show the inside. FIG. 17 is a left side view of FIG. 16, but the internal gear (26) is not cut away. Figure 18 is the first
Although this is a right side view of FIG. 6, the internal gear (26) is not cut away. FIG. 19 is a front view of the generator (32). Figure 20 is 19th
Left side view of the figure. FIG. 21 is a right side view of FIG. 19. 22nd
The figure is a front view of gears (27), (19), etc. attached to the shaft (24). FIG. 23 is a left side view of FIG. 22. Figure 24 is the second
Right side view of Figure 2. Figure 25 shows the shaft (24) and parallel key (6).
5) Front view. Figure 26 shows the boo IJ that is integrated with the boss (1).
(2) and a front view of the power point gear (11). Figure 27 is the 26th
Left side view of the figure. FIG. 28 is a right side view of FIG. 26. 29th
The figure is a front view of gears (2L), (8), (7), etc. attached to the shaft (9). FIG. 30 is a left side view of FIG. 29. FIG. 31 is a right side view of FIG. 29. Figure 32 shows the shaft (9) and parallel key (6).
5) Front view. Figure 33 is a left side view of gear (7) with the shaft (9) between gears (8) and (7) shown in Figure 29 cut away, with one corner of the gear (7) elastic body (56) etc. also cut away. It is. FIG. 34 is a right side view of FIG. 33. Figure 35 shows an elastic body (5
6) side view. FIG. 36 is a right side view of FIG. 35. 37th
The figure is a front view of the mechanism used in the experiment. FIG. 38 is a left side view of FIG. 37. FIG. 39 is a front view of ball 1-(66) used to integrate two disc frames (67). FIG. 40 is a right side view of FIG. 37. Figure 41 shows internal gear (6) and gear (7).
) A diagram for explaining the rotational status of each gear, although teeth such as the power point gear (11) are omitted. In Fig. 42, the teeth of the internal gear (6), gear (7), power point gear (11), etc. are omitted as in Fig. 41, but the gear (7) is made larger and the power point gear (11) is omitted.
) is made smaller and the rotation rate is compared with the case of Fig. 41. FIG. 43 is a diagram for theoretically explaining the lever action of the gear (7) in a state that is easy to compare with FIG. 44. 44th
The figure is a so-called inversely proportional mechanism in which force and distance are inversely proportional, which rotates around an axis (I) fixed at a fixed position, and is used to explain the limitations on which it is impossible to increase power. Figures 45 and 46 show that the wheel (7) is rolled on a flat surface to show that distance and force are inversely proportional. Fig. 43 is a mechanism diagram proving that force and distance are inversely proportional even if the force acting only on the (R) line shown in Fig. 49 is used. FIG. 48 is a left side view of FIG. 47. Figure 49 is the right side of the box in Figure 47. Figure 50 is a front view of the experimental mechanism. FIG. 51 is a left side view of FIG. 50. FIG. 52 is a right side view of FIG. 50. 475) 61st Prisoner-i485-

Claims (1)

[Claims] As explained through theory and experiment, due to the meshing action of internal gear (6), gears (7), (8), power point gear (11), etc.
Inside the planetary rotating body, the power that is increased from the input power is directly converted into electric power by a generator directly connected to the planetary mechanism, which is then output as a current to the outside of the aircraft, which rotates the electric motor connected by a conductor and produces an output. A power increasing machine that utilizes the special characteristics of the planetary mechanism.