A sliding elastic inertia power device of an engine

Abstract

A sliding elastic inertial power device of an engine comprises an oscillating rotating body; the oscillating rotating body comprises a sliding rod 1, a supporting pot and a sliding rod 2, wherein the sliding rod 1 and the sliding rod 2 are both connected to the side wall of the supporting pot, a counterweight iron ball is installed on the side wall of each sliding rod, and the counterweight iron ball is connected to the U-shaped bow tip at the top of the sliding rod through a tension spring or a steel wire rope, a counterweight mechanism is arranged inside the sliding rod 1, the supporting pot and the sliding rod 2, part of the top seat sliding block in the counterweight mechanism is not pushed open, and the bayonet on the corresponding sliding rod pops out under the action of the oppositely arranged spring to limit the sliding of the counterweight iron ball, and after the side wall of the supporting pot is inserted into the seat-type cam top column, as the supporting pot rotates, part of the top seat sliding block is pushed open, the bayonet is retracted, and the counterweight iron ball moves in the opposite direction under the action of the tension spring, thereby realizing reciprocating oscillation and driving the oscillating rotating body to rotate.

Description

Technical Field

[0001] The invention belongs to the technical field of new energy engines, and in particular relates to a sliding elastic inertia power device of an engine. Background Art

[0002] At present, various engines on the market have many problems such as low efficiency, energy waste, serious pollution, complex structure, high manufacturing and operation costs, etc., and the energy is single, mainly fossil energy. The application is unstable, discontinuous, and the utilization efficiency is low. For example, wind energy and solar energy are unstable, discontinuous, and have low utilization efficiency, and nuclear power is too complex and has high application conditions. Therefore, it is necessary to solve the above technical problems. Summary of the invention

[0003] The present invention provides a sliding elastic inertia power device for an engine, which aims to solve the technical problems of low efficiency, heavy pollution, complex structure, high manufacturing and operating costs of existing engines; at the same time, solve the technical problems of single energy, unstable application and discontinuity.

[0004] The technical solution of the present invention is achieved in this way:

[0005] A sliding elastic inertial power device of an engine, characterized in that it comprises an oscillating rotating body;

[0006] The oscillating rotating body includes a supporting pot O, a sliding rod H, a counterweight iron ball Q, a U-shaped bow U, a tension spring or a steel wire rope T; the supporting pot O is a spherical shell, and a hollow cylindrical sliding rod is symmetrically connected to the spherical surface on both sides thereof, and the two sliding rods are coaxial and the axis line passes through the center of the supporting pot; a counterweight iron ball Q is coaxially sleeved on the sliding rod H for sliding connection, and a U-shaped bow U is fixedly installed on the outer end of the sliding rod, which is bent toward the supporting pot and symmetrical to the sliding rod, and the U-shaped bow U is made of elastic material or non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs or steel wire ropes T to form two unilateral oscillating bodies on both sides of the supporting pot; and anti-collision and shock-absorbing pads Z are installed on the sliding boundary positions of the counterweight iron balls at both ends of the sliding rod;

[0007] A near latch pin KJ and a far latch pin KY are installed at the sliding boundary positions of the counterweight iron ball at both ends of the rod body of the slide rod. A double-channel sliding groove is provided inside the slide rod near the support pot side and is connected to the inside of the support pot, and a top seat slider D for controlling the far and near latch pins is installed in the double-channel sliding groove to slide and cooperate with the sliding groove. The two top seat sliders are connected to the near latch pin and the far latch pin for pulling control by steel wires respectively; and the near latch pin and the far latch pin are cross-arranged with the top seat sliders on both sides of the support pot; the near latch pin and the far latch pin are respectively located at the near and far positions of the sliding boundary of the counterweight iron ball, and can extend the rod body from the pin hole on the side wall of the rod body of the slide rod and be inserted into the insertion hole of the counterweight iron ball for limiting position;

[0008] A cam top column A is installed inside the support pot of the oscillating rotating body. The cam top column A is a double cam structure, which is a Z-shaped double cam structure with a cam protruding from the upper and lower sides and opposite sides of the cam hub in opposite directions. The cam top column pushes open the top seat slider and pulls the latch in the slide rod through a steel wire to be pulled out from the socket in the iron ball, thereby releasing the counterweight iron ball; driving the support pot to rotate;

[0009] The upper cam of the cam top column lifts up the top seat slider of the upper near-claw pin, and the lower cam lifts up the top seat slider of the lower far-claw pin on the same side, allowing the weighted iron balls of the two slide bars, slide bar 1 and slide bar 2, to slide; when the slide bar 1 rotates down and the slide bar 2 rotates up, the above action is repeated, and so on;

[0010] When the counterweight iron ball slides to the latch position at the outer end of the slide rod and the inner end of the slide rod, the latch is automatically locked into the socket through the action of the spring to lock the counterweight iron ball; the locking position of the counterweight iron ball on the two slide rods is set to two opposite positions, one far and one near.

[0011] The sliding elastic inertial power device of the engine, wherein the tension of the tension spring T is greater than the weight of the counterweight iron ball; the distance between the two bow tips of each U-shaped bow U is greater than the diameter of the counterweight iron ball Q.

[0012] In the sliding elastic inertia power device of the engine, the two oscillating rotating bodies share the same supporting pot and are symmetrically connected to the supporting pot.

[0013] A sliding elastic inertial power device of an engine, wherein the oscillating rotating body is installed in an outer shell C and rotates coaxially with the rotation center of the outer shell, the top of each U-shaped bow of the oscillating rotating body is fixedly connected to the inner wall of the outer shell, and a bracket shaft M coaxial with the rotation center of the outer shell C passes through the support pot and extends from openings on both sides thereof, and both ends of the bracket shaft M pass through the outer shell and are connected and fixed to a frame outside the outer shell; the cam top column A matches the top seat slider and is fixedly connected to the bracket shaft M.

[0014] The sliding elastic inertia power device of the engine, wherein the outer end of the bayonet is provided with a guide inclined surface contacting with the counterweight iron ball, the inner end of the bayonet is provided with a return spring, and the bayonet is arranged in the slide groove.

[0015] The sliding elastic inertial power device of the engine, wherein the U-shaped bow U is made of non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs T.

[0016] The sliding elastic inertia power device of the engine, wherein a plurality of U-shaped bows U are arranged at the outer end of the sliding rod H.

[0017] A sliding elastic inertial power device of an engine, wherein curved slide bars SH are symmetrically arranged on both sides of the slide bar H to form a slideway, the curved slide bar SH is a cylindrical rod body bent in an arc shape and located on both sides outside the counterweight iron ball, and the two ends of the curved slide bar SH are respectively connected to the two ends of the slide bar H; the counterweight iron ball Q is symmetrically connected to a connecting rod LG on both sides, the connecting rod LG is a cylindrical rod body and is perpendicular to the slide bar H, a curved slider SK is installed on the connecting rod LG, the curved slider SK is connected to the corresponding tension spring or wire rope T of the bow tip L, a through circular hole is opened in the middle of the curved slider SK, the connecting rod LG passes through the circular hole on the curved slider SK and is slidably connected to it, a universal wheel B is installed on the curved slider SK, the wheel on the universal wheel B is a groove pulley, the groove pulley of the universal wheel B is engaged with the curved slide bar SH on the same side, and slides along the curved slide bar SH.

[0018] The sliding elastic inertial power device of an engine, wherein the tension of the U-shaped bow U or the tension spring T matches the product of the ratio of the actual length of the curved slide rod SH to the length of the slide rod H and the weight of the counterweight iron ball Q, and the tension of the U-shaped bow U or the tension spring T is greater than the product.

[0019] The sliding elastic inertial power device of the engine, wherein the distance between the two bow tips of the U-shaped bow U is greater than the distance between the farthest ends of the two connecting rods LG symmetrically arranged on the counterweight iron ball Q.

[0020] Beneficial effects of the present invention:

[0021] The oscillating rotating body in the present invention is equipped with a counterweight mechanism on the slide bars 1 and 2 on both sides of the supporting pot. Each of the slide bars 1 and 2 is equipped with a counterweight iron ball that can slide back and forth along the side wall of the slide bar. The top seat slider is pushed open by the cam top column to release the counterweight iron ball. The counterweight iron ball moves under the action of the tension spring. As the supporting pot rotates, the part of the top seat slider that has been pushed open is released, and the bayonet resets and locks the counterweight iron ball, thereby realizing reciprocating motion and driving the oscillating rotating body to rotate, so as to solve the problems of low engine efficiency, heavy pollution, complex structure, and high manufacturing and operating costs. Curved slide bars are arranged on both sides of the slide bar to form a slideway, so as to achieve the purpose of reciprocating motion of the counterweight iron on the slide bar, and the moving trajectory is more stable. BRIEF DESCRIPTION OF THE DRAWINGS

[0022] Figure 1 It is a schematic diagram of the action state of a weighted iron ball when a group of oscillating rotating bodies of the present invention rotate to do work to a 0 degree position.

[0023] Figure 2 This is a schematic diagram of the action state of the weighted iron ball when the oscillating rotating body rotates clockwise to 90 degrees.

[0024] Figure 3 , Figure 4 This is a schematic diagram of the action state of the weighted iron ball when the oscillating rotating body rotates clockwise to 180 degrees.

[0025] Figure 5 This is a schematic diagram of the action state of the weighted iron ball when the oscillating rotating body rotates clockwise to 270 degrees.

[0026] Figure 6 This is a schematic diagram of the group of oscillating rotating bodies rotating clockwise to 360 degrees (i.e. the original 0 degree position).

[0027] Figure 7 It is a schematic diagram of the structure of a group of internal counterweight control mechanisms of an oscillating rotating body of the present invention.

[0028] Figure 8 It is a schematic diagram of the axial partial cross-section structure of a set of oscillating rotating bodies and the connection between the cam top column, the bracket shaft and the frame of the present invention.

[0029] Fig. 9 It is a schematic diagram of the positional relationship of two groups of oscillating rotating bodies connected in the housing in the second embodiment of the present invention and their connection with the housing,

[0030] Fig.10 This is a schematic diagram of the action state of a weighted iron ball when a group of oscillating rotating bodies rotate to do work to a 0 degree position according to the third embodiment of the present invention.

[0031] Fig.11 1 is a schematic diagram of the action state of the weighted iron ball when the group of oscillating rotating bodies rotates clockwise to 90 degrees in the third embodiment of the present invention.

[0032] Fig.12 , Fig.13 A schematic diagram of the action state of the weighted iron ball when the oscillating rotating body group rotates clockwise to 180 degrees in the third embodiment of the present invention,

[0033] Fig.14 1 is a schematic diagram of the action state of the weighted iron ball when the group of oscillating rotating bodies rotates clockwise to 270 degrees in the third embodiment of the present invention.

[0034] Fig.15 is a schematic diagram of the group of oscillating rotating bodies in the third embodiment of the present invention when rotating clockwise to 360 degrees (i.e., the original 0 degree position),

[0035] Fig.16 This is a schematic diagram of a group of oscillating rotating bodies in the third embodiment of the present invention.

[0036] Fig.17 is a rear view schematic diagram of an oscillating rotating body in the third embodiment of the present invention,

[0037] Fig.18 yes Fig.17 AA surface cross-section diagram,

[0038] Fig.19 is a schematic top view of an oscillating rotating body in the third embodiment of the present invention,

[0039] Fig. 20 yes Fig.19 BB surface cross-section diagram,

[0040] Fig.21 It is a schematic side view of an oscillating rotating body in the third embodiment of the present invention.

[0041] Explanation of the accompanying figures: support pot O, slide bar H, slide bar one H1, slide bar two H2, curved slide bar SH, counterweight iron ball Q, counterweight iron ball one Q1, counterweight iron ball two Q2, curved slider SK, connecting rod LG, anti-collision shock-absorbing pad Z, U-shaped bow U, U-shaped upper bow U1, U-shaped lower bow U2, bow tip L, tension spring or wire rope T, cam top column A, top seat slider D, inner top seat slider one D-L1, outer top seat slider one D-W1, inner top seat slider two D-L2, outer top seat slider two D-W2, near latch pin KJ, near latch pin one KJ1, near latch pin two KJ2, far latch pin KY, far latch pin one KY1, far latch pin two KY2, shell C, bracket shaft M, universal wheel B. DETAILED DESCRIPTION

[0042] The specific structure and implementation methods of the present invention are described in detail below with reference to the accompanying drawings.

[0043] See also Figure 1As shown, a sliding elastic inertia power device of an engine of the present invention comprises an oscillating rotating body;

[0044] The oscillating rotating body includes a supporting pot O, a sliding rod H, a counterweight iron ball Q, a U-shaped bow U, a tension spring or a steel wire rope T; the supporting pot O is a spherical shell, and a hollow cylindrical sliding rod is symmetrically connected to the spherical surface on both sides thereof, and the two sliding rods are coaxial and the axis line passes through the center of the supporting pot; a counterweight iron ball Q is coaxially sleeved on the sliding rod H for sliding connection, and a U-shaped bow U is fixedly installed on the outer end of the sliding rod, which is bent toward the supporting pot and symmetrical to the sliding rod, and the U-shaped bow U is made of elastic material or non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs or steel wire ropes T to form two unilateral oscillating bodies on both sides of the supporting pot; and anti-collision and shock-absorbing pads Z are installed on the sliding boundary positions of the counterweight iron balls at both ends of the sliding rod;

[0045] See also Figure 7 As shown, a near latch pin KJ and a far latch pin KY are installed at the sliding boundary positions of the counterweight iron ball at both ends of the rod body of the slide rod, a double-channel sliding groove is provided inside the slide rod near the support pot side and is communicated with the inside of the support pot, and a top seat slider D for controlling the far and near latch pins is respectively installed in the double-channel sliding groove to slide with the sliding groove, and the two top seat sliders are respectively connected to the near latch pin and the far latch pin for pulling control by steel wires; and the near latch pin and the far latch pin are cross-arranged with the top seat sliders on both sides of the support pot; the near latch pin and the far latch pin are respectively located at the near and far positions of the sliding boundary of the counterweight iron ball, and can extend the rod body from the pin hole on the side wall of the rod body of the slide rod and be inserted into the insertion hole of the counterweight iron ball for limiting position;

[0046] A cam top column A is installed inside the support pot of the oscillating rotating body. The cam top column A is a double cam structure, which is a Z-shaped double cam structure with a cam protruding from the upper and lower sides and opposite sides of the cam hub in opposite directions. The cam top column pushes open the top seat slider and pulls the latch in the slide rod through a steel wire to be pulled out from the socket in the iron ball, thereby releasing the counterweight iron ball; driving the support pot to rotate;

[0047] The upper cam of the cam top column lifts up the top seat slider of the upper near-claw pin, and the lower cam lifts up the top seat slider of the lower far-claw pin on the same side, allowing the weighted iron balls of the two slide bars, slide bar 1 and slide bar 2, to slide; when slide bar 1 rotates down and slide bar 2 rotates up, the above action is repeated, and so on; Figure 6 or Figure 3 ;

[0048] When the weighted iron ball slides to the position of the latch at the first outer end of the slide rod and the second inner end of the slide rod, the latch automatically snaps into the jack through the action of the spring to lock the weighted iron ball; Figure 1The locking positions of the counterweight iron ball on the two slide bars are set to two opposite positions, one far and one near. Figure 4 ;

[0049] In the sliding elastic inertia power device of the engine, the tension of the tension spring T is greater than the weight of the counterweight iron ball.

[0050] The sliding elastic inertia power device of the engine, wherein the distance between the two bow tips of each U-shaped bow U is greater than the diameter of the counterweight iron ball Q.

[0051] See also Fig. 9 As shown, the two oscillating rotating bodies share the same supporting pot and are symmetrically connected to the supporting pot.

[0052] The oscillating rotating body is installed in the shell C and rotates coaxially with the rotation center of the shell. The top of each U-shaped arch of the oscillating rotating body is fixedly connected to the inner wall of the shell. The bracket shaft M coaxial with the rotation center of the shell C passes through the support pot and extends from the openings on both sides thereof. The two ends of the bracket shaft M pass through the shell and are connected and fixed to the frame outside the shell; the cam top column A matches the top seat slider and is fixedly connected to the bracket shaft M, see Figure 8 shown.

[0053] See also Figure 7 As shown, a sliding elastic inertia power device of an engine is described, wherein the outer end of the bayonet is provided with a guide inclined surface that contacts the counterweight iron ball, the inner end of the bayonet is provided with a return spring, and the bayonet is arranged in a slide groove.

[0054] The sliding elastic inertial power device of the engine, wherein the U-shaped bow U is made of non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs T.

[0055] The sliding elastic inertia power device of the engine, wherein a plurality of U-shaped bows U are arranged at the outer end of the sliding rod H.

[0056] A sliding elastic inertial power device of an engine, wherein curved slide bars SH are symmetrically arranged on both sides of the slide bar H to form a slideway, the curved slide bar SH is a cylindrical rod body bent in an arc shape and located on both sides outside the counterweight iron ball, and the two ends of the curved slide bar SH are respectively connected to the two ends of the slide bar H; the counterweight iron ball Q is symmetrically connected to a connecting rod LG on both sides, the connecting rod LG is a cylindrical rod body and is perpendicular to the slide bar H, a curved slider SK is installed on the connecting rod LG, the curved slider SK is connected to the corresponding tension spring or wire rope T of the bow tip L, a through circular hole is opened in the middle of the curved slider SK, the connecting rod LG passes through the circular hole on the curved slider SK and is slidably connected to it, a universal wheel B is installed on the curved slider SK, the wheel on the universal wheel B is a groove pulley, the groove pulley of the universal wheel B is engaged with the curved slide bar SH on the same side, and slides along the curved slide bar SH.

[0057] The sliding elastic inertial power device of the engine, wherein the tension of the U-shaped bow U or the tension spring T matches the product of the ratio of the actual length of the curved slide bar SH to the length of the slide bar H and the weight of the counterweight iron ball Q, and the tension of the U-shaped bow U or the tension spring T is greater than the product. The sliding elastic inertial power device of the engine, wherein the distance between the two bow tips of the U-shaped bow U is greater than the distance between the farthest ends of the two connecting rods LG symmetrically arranged on the counterweight iron ball Q.

[0058] The specific embodiments of the present invention are described in further detail below:

[0059] Please refer to the engine weight iron ball working process. Figures 1 to 8 ,in, Figure 1-Figure 6 It indicates the working state of a group of oscillating rotating bodies rotating to do work, in which the first and second weighted iron balls take turns to do work 360 degrees;

[0060] When a group of oscillating rotating bodies rotate to do work to the 0 degree position, such as Figure 1 As shown. The upper and lower sides of the support pot O are the slide bar 1 H1 and the slide bar 2 H2. At this time, the counterweight iron ball 1 Q1 slides to the bottom of the U-shaped upper bow U1, and the tension spring T on the U-shaped upper bow U1 is pulled to the bottom of the U-shaped upper bow U1 and locked by the far-pin 1 KY1. The tension potential energy direction of its tension spring T points to the intersection of the slide bar 1 H1 and the virtual line X between the two bow tips. At the same time, the counterweight iron ball 2 Q2 slides upward along the side wall of the slide bar 2 H2 to a position close to the support pot and is locked by the near-pin 2 KJ2. At this time, the counterweight iron ball 2 Q2 is close to the support pot O, and the tension spring T on the bow tip L of the U-shaped lower bow U2 is also pulled toward the support pot O. The tension potential energy direction of its tension spring T points to the intersection of the slide bar 2 H2 and the virtual line X between the two bow tips. At this time, the gravity potential energy reserve of the counterweight iron ball 1 Q1 on the slide bar 1 H1 is completed, and it begins to rotate in the clockwise direction to do work.

[0061] When the oscillating rotating body rotates clockwise to 90 degrees, the action state of the weighted iron ball is as follows: Figure 2 As shown, the huge eccentric force generated by the movement of two counterweight iron balls generates gravitational potential energy. Considering the two counterweight iron balls as a whole, their gravitational potential energy is the mass of 2 counterweight iron balls × 9.8 × half of the moving distance of one counterweight iron ball, that is, 2 × 1000 kg × 9.8 × 0.5 m = 9800 joules. If only one counterweight iron ball is referred to, its gravitational potential energy is the mass of 1 counterweight iron ball × 9.8 × the moving distance of one counterweight iron ball, 1000 kg × 9.8 × 1 m = 9800 joules. Here, the cam top column A vertically fixed in the support pot O does not contact any top seat slider, and the oscillating rotating body continues to rotate in the clockwise direction.

[0062] When the oscillating rotating body rotates clockwise to 180 degrees, the action state of the weighted iron ball is as follows: Figure 3 As shown in the figure, the weighted iron ball Q1 as a particle moves vertically downward by 1 meter, so as mentioned above, the work done is 1000 kg × 9.8 × 1 meter = 9800 joules. The engine oscillation rotating body rotates to this point, and Figure 1 In contrast, the slide bar H1 rotates to the bottom of the support pot O. At this point, the counterweight iron ball Q1 completes a cycle of work. At the same time, the cam top column A fixed in the support pot O simultaneously pushes open the near latch pin KJ2 and the far latch pin KY1. As the latch opens, the counterweight iron ball Q2 accelerates to slide toward the middle position of the slide bar H2, and the counterweight iron ball Q1 accelerates to slide toward the middle position of the slide bar H1. In addition, due to the inertia of the counterweight iron ball during movement, the counterweight iron ball Q2 will slide to the top of the slide bar H2 in a short time and be buffered by the anti-collision cushion pad Z and locked by the far latch pin KY2. The counterweight iron ball Q1 will slide to the end of the slide bar H1 close to the support pot in a short time and be buffered by the anti-collision cushion pad Z and locked by the near latch pin KJ1. Figure 4 At this point, the counterweight iron ball Q1 and the counterweight iron ball Q2 have completed work and exchanged motion states.

[0063] like Figure 4As shown, the U-shaped lower bow U2 is above the support pot, the counterweight iron ball Q2 is at the bottom of the U-shaped lower bow U2, and the tension spring T on the bow tip L of the U-shaped lower bow U2 is also pulled toward the bottom of the U-shaped lower bow U2, and the tension potential energy direction of the tension spring T points to the intersection of the slide bar H2 and the virtual line X between the two bow tips. At this time, the counterweight iron ball Q1 is close to the support pot O, and the tension spring T on the bow tip L of the U-shaped upper bow U1 is also pulled toward the support pot O. The tension potential energy direction of the tension spring T points to the intersection of the slide bar H1 and the virtual line X between the two bow tips. The reserve of elastic potential energy in this link is ready for the next lifting of the two counterweight iron balls. The two counterweight iron balls are lifted again, and the counterweight iron ball Q1 and the counterweight iron ball Q2 complete the position handover. With the reserve of gravity potential energy, the counterweight iron ball Q2 begins to rotate clockwise to do work.

[0064] When the oscillating rotating body rotates clockwise to 270 degrees, the action state of the weighted iron ball is as follows: Figure 5 As shown, the slide bar H1 and slide bar H2 connected on both sides of the support pot O are parallel to the ground. During the rotation process, the weighted iron ball Q2 on the slide bar H2 rotates in the clockwise direction, and its gravitational potential energy does work to the outside. The weighted iron ball Q2 as a particle moves vertically downward by 1 meter, so the work done is 1000 kg × 9.8 × 1 meter = 9800 joules. The cam top column A fixed vertically in the support pot O does not contact any top seat slider, and the engine continues to rotate in the clockwise direction.

[0065] When the oscillating rotating body rotates clockwise to 360 degrees (i.e. the original 0 degree position), the action state of the weighted iron ball is as follows: Figure 6 As shown, the upper and lower sides of the support pot O are slide bar 1 H1 and slide bar 2 H2 respectively, and the counterweight iron ball 2 Q2 as a mass point moves vertically downward by 1 meter, so it does work of 1000 kg × 9.8 × 1 meter = 9800 joules. When the engine oscillation rotating body rotates to this point, the counterweight iron ball 2 Q2 completes a cycle of work. At this time, the cam top column A fixed in the support pot O simultaneously pushes open the near latch pin 1 KJ1 and the far latch pin 2 KY2. As the latch is opened, the counterweight iron ball Q2 slides rapidly toward the middle of the slide bar H2, and the counterweight iron ball Q1 slides rapidly toward the middle of the slide bar H1. In addition, due to the inertia of the counterweight iron ball in motion, the counterweight iron ball Q2 slides to the end of the slide bar H2 close to the support pot in a short time and is buffered by the anti-collision cushion Z and locked by the near latch KJ2. The counterweight iron ball Q1 slides to the top of the slide bar H1 in a short time and is buffered by the anti-collision cushion Z and locked by the far latch KY1. Figure 1 As shown in the figure, the counterweight iron ball Q1 and the counterweight iron ball Q2 complete the work and exchange the motion state, and then return to the initial state. At this time, the two counterweight iron balls have rotated a circle, completing a work cycle, and the cycle continues on this basis.

[0066] The work done by the oscillating rotating body during one rotation is completed by the cooperation of two weighted iron balls. Each weighted iron ball rotates 180 degrees. When it moves 2 meters straight on the slide bar, the work done by the two weighted iron balls is 1000×9.8×2×2=39200 joules. It can be seen that when each weighted iron ball is in operation, the gravitational potential energy generated by its mass does work externally, and the energy displaced is twice the gravitational potential energy of the weighted iron ball. If the mass of the weighted iron ball is doubled or the sliding distance on the slide bar is doubled, the gravitational potential energy of the weighted iron ball will increase by 2 times. This shows that the engine can produce huge energy.

[0067] like Figure 7 As shown, the counterweight mechanism of the present invention. An inner top seat slider D-L1 and an outer top seat slider D-W1 are installed in the sliding groove of the top seat slider where the inner wall of the support pot O is connected to the slide bar H1 (that is, their positions are one inside and one outside, and are not on the same rotation plane). The inner top seat slider D-L1 is connected to the near latch pin KJ1 with a steel wire, and the outer top seat slider D-W1 is connected to the far latch pin KY1 with a steel wire; an inner top seat slider D-L2 and an outer top seat slider D-W2 are installed in the sliding groove of the top seat slider where the inner wall of the support pot O is connected to the slide bar H2 (that is, their positions are one inside and one outside, and are not on the same rotation plane). The inner top seat slider D-L2 is connected to the near latch pin KJ2 with a steel wire, and the outer top seat slider D-W2 is connected to the far latch pin KY2 with a steel wire; the counterweight iron ball can only do work when it is at the top of the sliding rod. Therefore, whenever the counterweight iron ball slides on the sliding rod to a position close to the support pot, the corresponding near latch pin must be opened in time to allow it to slide to the top.

[0068] As shown in this figure, the upper part of the cam post A is bent inward. Figure 8 , bypassing the outer top seat slider D-W1, and pressing against the inner top seat slider D-L1 which is staggered inwards, the inner top seat slider D-L1 pulls the near latch pin KJ1 through the steel wire to retract into the inner part of the slide bar 1, so that the counterweight iron ball Q1 is quickly pulled to the top of the slide bar H1 by the tension spring T on the U-shaped upper bow U1 and locked by the far latch pin KY1. At the same time, the lower part of the cam top column A is bent outwards, bypassing the inner top seat slider D-L2, and pressing against the outer top seat slider D-W2 which is staggered outwards, the outer top seat slider D-W2 pulls the far latch pin KY2 through the steel wire to retract into the inner part of the slide bar 2, so that the counterweight iron ball Q2 is quickly pulled to the top of the slide bar H2 by the tension spring T on the U-shaped lower bow U2 and locked by the near latch pin KY2. At this time, the counterweight mechanism completes the task of simultaneously controlling the two counterweight iron balls to obtain gravitational potential energy.

[0069] like Fig. 9As shown, two or more pairs of oscillating rotating bodies in a cross pattern can be installed on the support pot of the present invention. Each oscillating rotating body is connected and fixed to the outer shell C by a U-shaped bow sleeved on the top of the two slide rods, which plays the role of safety and inertia wheel. This engine can be designed and arranged in parallel in countless combinations as needed. The work done by a counterweight iron ball in one rotation of the engine of this structure is 1000×9.8×2=19600 joules, and a total of 4 counterweight iron balls do a total work of 19600×4=78400 joules. According to the acceleration of gravity, the speed of the engine of this structure rotates about 3 times per second, and its power is about 78400÷0.33=235200 watts, a total of 235.2 kilowatts.

[0070] The U-shaped bow in the present invention is made of elastic material or non-elastic material, wherein the non-elastic material is a metal material that is not easily deformed, such as high carbon steel. When the U-shaped bow is made of elastic material, the two ends of the bow tip are connected by tension springs or steel wire ropes, and when the U-shaped bow is made of non-elastic material, the two ends of the bow tip are only connected by tension springs. Multiple U-shaped bows can be fixedly installed on the outer end of each sliding rod to form a cage top to provide additional elastic force.

[0071] like Fig.17 As shown in the figure, the actual length of the curved slide bar SH is different from that of the slide bar H. The reciprocating sliding lines of the curved slide block SK and the counterweight iron ball Q are separated, and the two are organically connected by the connecting rod LG to form a dual-type slide bar motion association system. The curved slide block SK is respectively connected to the bow tips L at both ends of the corresponding U-shaped bow through symmetrically arranged tension springs or wire ropes T. The U-shaped bow U uses the elastic energy generated by deformation to drive the counterweight iron ball Q on the slide bar H to slide upward reciprocatingly through the connecting rod LG, and each time it reaches the end point of the slide bar H.

[0072] like Fig.16As shown, the counterweight iron ball Q is lifted back and forth by a dual-type sliding bar motion association system. The system structure and principle are that there are two sliding objects, curved sliders SK and counterweight iron ball Q, on the curved sliding bar SH and sliding bar H with the same straight length at both ends, which reciprocate on the curved sliding bar and sliding bar respectively. The objects on the two sliding bars are parallel and organically connected by a connecting rod LG. The objects on the two sliding bars have the same running time and the same required energy, but the running distance, running speed and other parameters are different. The running parameters of the curved sliding bar SH are larger than those of the objects on the sliding bar H; the ratio of the running parameters of the two objects is proportional to the actual length ratio of the two sliding bars, which can be called the curved and straight dual-type sliding bar association effect. This technical solution is a curved and straight sliding bar. In fact, the spatial shape of the two sliding bars can be any shape under the condition that the objects installed on them can operate normally, and the properties reflected by the running of the objects on them correspond to the actual length ratio of the two sliding bars. In addition, the mass of the objects on the two sliding bars and the energy used can be converted to each other, which is completely reflected by energy. In this scheme, the straight lengths of the two ends of the curved slide bar SH and the slide bar H are the same. For the convenience of calculation, the actual length ratio of the two slide bars is set to 2:1; the weighted iron ball Q is 1000 kg. The curved slide bar SH is equipped with a curved slider SK, which is connected to the bow tips L at both ends of the corresponding U-shaped bow through symmetrically arranged tension springs or wire ropes T. The elastic energy acts on the curved slider SK through the curved slide bar SH, and the curved slider SK is transmitted to the weighted iron ball Q through the connecting rod LG and slides back and forth on the slide bar H. The connecting rod LG can slide randomly in the connecting hole of the curved slider SK, thus forming a dual-type slide bar association effect. The effect is that the running time and running energy of the related sliding parts on the two slide bars are the same, but the running distance and running speed are different. The running parameters of the curved slide bar SH are larger than those of the sliding parts on the slide bar H; the running parameter ratio of the two parts is proportional to the actual length ratio of the two slide bars. Therefore, when the running parameters of one part change, the related parameters of the other part will inevitably produce a corresponding effect. Some parameters of this scheme have been fixed in advance, and this effect will be transferred to other parameters. If the actual running distance of the two objects is different, but the performance effect is the same when referring to the straight slide bar H; the running energy of the two objects is also the same due to the conduction effect of the connecting rod LG. Therefore, the corresponding elastic energy of the U-shaped bow U should be 1000×9.8×2=19600 joules, and the energy obtained or reflected by the counterweight iron ball Q is also 1000×9.8×2=19600 joules, but the actual weight of the counterweight iron ball Q is only 1000×9.8×1=9800 joules. In this way, its elastic energy drives the counterweight iron ball Q to run back and forth on the slide bar H through the connecting rod LG, and reaches the top of the slide bar H every time.

[0073] Embodiment 1

[0074] The oscillating rotating body in the first embodiment of the present invention includes a support pot O, a slide bar 1 H1, and a slide bar 2 H2. The support pot is symmetrically provided with slide bars 1 and 2 along the radial direction. Anti-collision and shock-absorbing pads Z are installed on the sliding boundary of the weighted iron balls at both ends of each slide bar. A slidingly connected weighted iron ball 1 Q1 is provided on a coaxial sleeve of the slide bar. A U-shaped upper bow U1 bent toward the support pot is installed on the outer end of slide bar 1. The two ends of the weighted iron ball 1 are connected to the corresponding bow tips at both ends of the U-shaped upper bow through symmetrically arranged tension springs T; a slidingly connected weighted iron ball 2 Q2 is provided on the coaxial sleeve of slide bar 2. A U-shaped lower bow U2 bent toward the support pot is installed on the outer end of slide bar 2. The two ends of the weighted iron ball 2 are connected to the corresponding bow tips at both ends of the U-shaped lower bow through symmetrically arranged tension springs T. The U-shaped bow is made of non-elastic material. Figure 7 As shown;

[0075] The support pot O, the slide bar H1 and the slide bar H2 are hollow inside and are provided with a counterweight mechanism. A near latch pin KJ1 is installed at a position near the support pot inside the slide bar H1, a far latch pin KY1 is installed at a position near the shock-absorbing pad inside the slide bar 1, a near latch pin KJ2 is installed at a position near the support pot inside the slide bar H2, and a far latch pin KY2 is installed at a position near the shock-absorbing pad inside the slide bar 2; a double-channel sliding groove is provided inside the end of the support pot connected to the slide bar 1, an inner top seat D-L1 is installed in one channel, and the inner top seat 1 is connected to the near latch pin 1 through a steel wire, and an outer top seat D-W1 is installed in the other channel, and the outer top seat 1 is connected to the far latch pin 1 through a steel wire; a There is a sliding groove with double channels, and an inner top seat D-L2 is installed in one channel, and the inner top seat is connected to the near pin 2 by a steel wire, and an outer top seat D-W2 is installed in the other channel, and the outer top seat is connected to the far pin 2 by a steel wire. A cam top column A is installed inside the support pot and is fixed to the external frame by a camshaft. The cam top column A is a double cam structure, which is a Z-shaped double cam structure with a cam protruding from the upper and lower sides and opposite sides of the cam hub in opposite directions. Whenever the sliding rod on the support pot rotates to be perpendicular to the ground, the cam top column pushes open the top seat slider in the left sliding groove on the two vertical sliding rods, and pulls the pin in the sliding rod through the steel wire to pull it out of the socket in the counterweight iron ball, thereby releasing the counterweight iron ball.

[0076] A single set of oscillating rotating bodies is provided, which is installed in the shell C and rotates coaxially with the rotation center of the shell. The top of each U-shaped arch of the oscillating rotating body is fixedly connected to the inner wall of the shell. The bracket shaft M coaxial with the rotation center of the shell C passes through the support pot and extends from the openings on both sides thereof. The two ends of the bracket shaft M pass through the shell and are connected and fixed to the frame outside the shell; the cam top column A matches the top seat slider and is fixedly connected to the bracket shaft M. Figure 8 , 9 shown.

[0077] Embodiment 2

[0078] In the second embodiment of the present invention, the single group of oscillating rotating bodies in the original embodiment one is changed into two groups of oscillating rotating bodies arranged crosswise, and the rest of the structure is unchanged from the embodiment one and will not be described in detail. The two oscillating rotating bodies share the same support pot and are symmetrically connected to the support pot. The cam top column A is a double cam structure. Whenever a group of oscillating rotating bodies rotates to a vertical position, the cam top column will push open the corresponding top seat slider, and pull the latch in the slide rod through the steel wire to pull it out of the socket in the iron ball, thereby releasing the counterweight iron ball; driving the support pot to rotate; see Figure 8 , 9 shown.

[0079] Embodiment 3

[0080] The oscillating rotating body in the third embodiment of the present invention is symmetrically provided with a slide bar 1 H1 and a slide bar 2 H2 on the outer ring of its supporting pot O; curved slide bars SH are arranged in parallel on both sides of the slide bars 1 and 2, and a curved slider SK is arranged on the curved slide bar SH, and a universal wheel B is arranged on the side of the curved slider SK. Under the guidance of the universal wheel B, the curved slider SK can reciprocate along the curved slide bar SH, and the curved slider SK is slidably connected to the connecting rod LG connected to the counterweight iron ball Q. At the same time, the curved slider is respectively connected to the tension spring or wire rope T provided at the corresponding U-shaped bow tip L. A counterweight mechanism is installed inside the slide bars 1 and 2, and each of the two slide bars is provided with a counterweight iron ball Q that can slide back and forth thereon, and the top seat slider D is pushed open by the cam top column A to release the counterweight iron ball. The counterweight iron ball allows the counterweight mechanism to cooperate with the corresponding elastic energy of the U-shaped bow, and the curved slide bar SH with different spatial shapes is organically connected to the slide bar H and the two objects are operated, producing energy conduction, allocation, distance control and other functions, solving the problem that the rebound of gravity elastic devices such as bungee jumping cannot reach the top. As the support pot rotates, the part of the top seat slider D that has been pushed open is released, and the bayonet resets and locks the counterweight iron ball, thereby realizing the up and down oscillation of the counterweight iron ball to drive the oscillating rotating body to rotate. The remaining structures have not been changed compared with the first embodiment and will not be repeated.

[0081] The engine weight iron ball working process in the third embodiment of the present invention, please refer to Figures 10 to 16 ,in, Figure 10-15 It indicates the working state of a group of oscillating rotating bodies rotating to do work, in which the first and second weighted iron balls take turns to do work 360 degrees;

[0082] When a group of oscillating rotating bodies rotate to do work to the 0 degree position, such as Fig.10As shown. The upper and lower sides of the support pot O are sliding rods 1 H1 and 2 H2. The two sides of the counterweight iron ball Q1 and the counterweight iron ball Q2 are both provided with connecting rods LG for installing the curved slider SK. The curved slider SK can slide on the corresponding connecting rod LG. The curved slider SK is connected to the bow tip L through a tension spring or a wire rope T. The curved sliders SK on both sides of the counterweight iron ball Q1 move toward the bottom of the U-shaped upper bow U1 along the curved sliding rod SH and finally drive the counterweight iron ball Q1 to slide along the sliding rod H1 to the bottom of the U-shaped upper bow U1. The tension spring T on the U-shaped upper bow U1 is pulled toward the bottom of the U-shaped upper bow U1 and locked by the far-locking pin KY1. The tension potential energy direction of the tension spring T points to the intersection of the sliding rod H1 and the virtual line X between the two bow tips. At the same time, the curved sliders SK on both sides of the counterweight iron ball Q2 move toward the support pot along the curved slide bar SH and eventually drive the counterweight iron ball Q2 to slide along the slide bar H2 to a position close to the support pot, and is locked by the near latch KJ2. At this time, the counterweight iron ball Q2 is close to the support pot O, and the tension spring T on the bow tip L of the U-shaped lower bow U2 is also pulled toward the support pot O. The tension potential energy direction of the tension spring T points to the intersection of the slide bar H2 and the virtual line X between the two bow tips. At this time, the gravity potential energy reserve of the counterweight iron ball Q1 on the slide bar H1 is completed, and it begins to rotate in the clockwise direction to do work.

[0083] When the oscillating rotating body rotates clockwise to 90 degrees, the action state of the weighted iron ball is as follows: Fig.11 As shown, the two weighted iron balls are accelerated by the curved slider to generate huge eccentric force to obtain gravitational potential energy. Considering the two weighted iron balls as a whole, their gravitational potential energy is the mass of 2 weighted iron balls × 9.8 × half of the moving distance of one weighted iron ball, that is, 2 × 1000 kg × 9.8 × 0.5 m = 9800 joules. If only one weighted iron ball is referred to, its gravitational potential energy is the mass of 1 weighted iron ball × 9.8 × the moving distance of one weighted iron ball, 1000 kg × 9.8 × 1 m = 9800 joules. Here, the cam top column A vertically fixed in the support pot O does not contact any top seat slider, and the oscillating rotating body continues to rotate in the clockwise direction.

[0084] When the oscillating rotating body rotates clockwise to 180 degrees, the action state of the weighted iron ball is as follows: Fig.12 As shown in the figure, the weighted iron ball Q1 as a particle moves vertically downward by 1 meter, so as mentioned above, the work done is 1000 kg × 9.8 × 1 meter = 9800 joules. The engine oscillation rotating body rotates to this point, and Figure 1In contrast, the slide bar H1 rotates to the bottom of the support pot O. At this point, the counterweight iron ball Q1 completes a cycle of work. At the same time, the cam top column A fixed in the support pot O simultaneously pushes open the near latch pin KJ2 and the far latch pin KY1. As the latch pins open, the counterweight iron ball Q2 accelerates to slide toward the middle position of the slide bar H2 under the action of the curved slider, and the counterweight iron ball Q1 accelerates to slide toward the middle position of the slide bar H1 under the action of the curved slider. In addition, due to the inertia of the counterweight iron ball during movement, the counterweight iron ball Q2 will slide to the top of the slide bar H2 in a short time and be buffered by the anti-collision and shock-absorbing pad Z and locked by the far latch pin KY2. The counterweight iron ball Q1 will slide to the end of the slide bar H1 close to the support pot in a short time and be buffered by the anti-collision and shock-absorbing pad Z and locked by the near latch pin KJ1. Fig.13 At this point, the counterweight iron ball Q1 and the counterweight iron ball Q2 have completed work and exchanged motion states.

[0085] like Fig.13 As shown, the U-shaped lower bow U2 is above the support pot, and the curved sliders SK on both sides of the counterweight iron ball Q2 move toward the bottom of the U-shaped lower bow U2 along the curved slide bar SH and finally drive the counterweight iron ball Q2 to slide along the slide bar H2 to the bottom of the U-shaped lower bow U2. The tension spring T on the bow tip L of the U-shaped lower bow U2 is also pulled toward the bottom of the U-shaped lower bow U2, and the tension potential energy direction of the tension spring T points to the intersection of the slide bar H2 and the virtual line X between the two bow tips. At this time, the counterweight iron ball Q1 is close to the support pot O, and the tension spring T on the bow tip L of the U-shaped upper bow U1 is also pulled toward the support pot O along the curved sliders SK on both sides of the counterweight iron ball Q1. The tension potential energy direction of the tension spring T points to the intersection of the slide bar H1 and the virtual line X between the two bow tips. The reserve of elastic potential energy in this link is ready for the next lifting of the two counterweight iron balls. The two counterweight iron balls are lifted again, and the counterweight iron ball Q1 and the counterweight iron ball Q2 complete the position handover. The counterweight iron ball Q2 with the gravitational potential energy reserve begins to rotate in the clockwise direction and do work.

[0086] When the oscillating rotating body rotates clockwise to 270 degrees, the action state of the weighted iron ball is as follows: Fig.14 As shown, the slide bar H1 and slide bar H2 connected on both sides of the support pot O are parallel to the ground. During the rotation process, the weighted iron ball Q2 on the slide bar H2 rotates in the clockwise direction, and its gravitational potential energy does work to the outside. The weighted iron ball Q2 as a particle moves vertically downward by 1 meter, so the work done is 1000 kg × 9.8 × 1 meter = 9800 joules. The cam top column A fixed vertically in the support pot O does not contact any top seat slider, and the engine continues to rotate in the clockwise direction.

[0087] When the oscillating rotating body rotates clockwise to 360 degrees (i.e. the original 0 degree position), the action state of the weighted iron ball is as follows: Fig.15As shown, the upper and lower sides of the support pot O are slide bar 1 H1 and slide bar 2 H2 respectively, and the counterweight iron ball 2 Q2 as a mass point moves vertically downward by 1 meter, so it does work of 1000 kg × 9.8 × 1 meter = 9800 joules. When the engine oscillation rotating body rotates to this point, the counterweight iron ball 2 Q2 completes a cycle of work. At this time, the cam top column A fixed in the support pot O simultaneously pushes open the near latch pin 1 KJ1 and the far latch pin 2 KY2. As the latch is opened, the counterweight iron ball Q2 slides rapidly toward the middle of the slide bar H2, and the counterweight iron ball Q1 slides rapidly toward the middle of the slide bar H1. In addition, due to the inertia of the counterweight iron ball in motion, the counterweight iron ball Q2 slides to the end of the slide bar H2 close to the support pot in a short time and is buffered by the anti-collision cushion Z and locked by the near latch KJ2. The counterweight iron ball Q1 slides to the top of the slide bar H1 in a short time and is buffered by the anti-collision cushion Z and locked by the far latch KY1. Fig.10 As shown in the figure, the counterweight iron ball Q1 and the counterweight iron ball Q2 complete the work and exchange the motion state, and then return to the initial state. At this time, the two counterweight iron balls have rotated a circle, completing a work cycle, and the cycle continues on this basis.

[0088] The work done by the oscillating rotating body during one rotation is completed by the cooperation of two weighted iron balls. Each weighted iron ball rotates 180 degrees. When it moves 2 meters straight on the slide bar, the work done by the two weighted iron balls is 1000×9.8×2×2=39200 joules. It can be seen that when each weighted iron ball is in operation, the gravitational potential energy generated by its mass does work externally, and the energy displaced is twice the gravitational potential energy of the weighted iron ball. If the mass of the weighted iron ball is doubled or the sliding distance on the slide bar is doubled, the gravitational potential energy of the weighted iron ball will increase by 2 times. This shows that the engine can produce huge energy.

Claims

1. A sliding elastic inertia power device of an engine, characterized in that: The invention comprises an oscillating rotating body; the oscillating rotating body comprises a supporting pot (O), a sliding rod (H), a counterweight iron ball (Q), a U-shaped bow (U), a tension spring or a steel wire rope (T); the supporting pot (O) is a spherical shell, and a hollow cylindrical sliding rod is symmetrically connected to the spherical surface on both sides of the supporting pot, and the two sliding rods are coaxial and the axis line passes through the center of the supporting pot; a counterweight iron ball (Q) is coaxially sleeved on the sliding rod (H) and a U-shaped bow (U) bent toward the supporting pot and symmetrical to the sliding rod is fixedly installed on the outer end of the sliding rod, and the U-shaped bow (U) is made of elastic material or non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs or steel wire ropes (T) to form two unilateral oscillating bodies on both sides of the supporting pot; and anti-collision and shock-absorbing pads (Z) are installed at the sliding boundary positions of the counterweight iron balls at both ends of the sliding rod; A near latch pin (KJ) and a far latch pin (KY) are installed at the sliding boundary positions of the counterweight iron ball at both ends of the rod body of the slide rod. A double-channel sliding groove is provided inside the slide rod near the support pot side and is connected to the inside of the support pot. A top seat slider (D) for controlling the far and near latch pins is installed in the double-channel sliding groove to slide and cooperate with the sliding groove. The two top seat sliders are connected to the near latch pin and the far latch pin for pulling control by steel wires respectively; and the near latch pin and the far latch pin are cross-arranged with the top seat sliders on both sides of the support pot; the near latch pin and the far latch pin are respectively located at the near and far positions of the sliding boundary of the counterweight iron ball, and can extend the rod body from the pin hole on the side wall of the rod body of the slide rod and be inserted into the insertion hole of the counterweight iron ball for limiting position; A cam top column (A) is installed inside the support pot of the oscillating rotating body. The cam top column (A) is a double cam structure, which is a Z-shaped double cam structure with a cam protruding from the upper and lower sides and opposite sides of the cam hub in opposite directions. The cam top column pushes open the top seat slider and pulls the latch in the slide rod through a steel wire to be pulled out from the socket in the iron ball, thereby releasing the counterweight iron ball; driving the support pot to rotate; The upper cam of the cam top column lifts up the top seat slider of the upper near-claw pin, and the lower cam lifts up the top seat slider of the lower far-claw pin on the same side, allowing the weighted iron balls of the two slide bars, slide bar 1 and slide bar 2, to slide; when the slide bar 1 rotates down and the slide bar 2 rotates up, the above action is repeated, and so on; When the counterweight iron ball slides to the latch position at the outer end of the slide rod and the inner end of the slide rod, the latch is automatically locked into the socket through the action of the spring to lock the counterweight iron ball; the locking position of the counterweight iron ball on the two slide rods is set to two opposite positions, one far and one near.

2. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: The tension of the tension spring (T) is greater than the weight of the counterweight iron ball; the distance between the two bow tips of each U-shaped bow (U) is greater than the diameter of the counterweight iron ball (Q).

3. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: The two oscillating rotating bodies share the same supporting pot and are symmetrically connected to the supporting pot.

4. A sliding elastic inertia power device of an engine as claimed in claim 1 or 3, characterized in that: The oscillating rotating body is installed in the outer shell (C) and rotates coaxially with the rotation center of the outer shell. The top of each U-shaped bow of the oscillating rotating body is fixedly connected to the inner wall of the outer shell. The bracket shaft (M) coaxial with the rotation center of the outer shell (C) passes through the support pot and extends from the openings on both sides thereof. Both ends of the bracket shaft (M) pass through the outer shell and are connected and fixed to the frame outside the outer shell; the cam top column (A) matches the top seat slider and is fixedly connected to the bracket shaft (M).

5. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: The outer end of the bayonet is provided with a guide inclined surface contacting the counterweight iron ball, the inner end of the bayonet is provided with a return spring, and the bayonet is arranged in the slide groove.

6. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: The U-shaped bow (U) is made of non-elastic material, and the two ends of the counterweight iron ball are connected to the corresponding bow tips at the two ends of the U-shaped bow through symmetrically arranged tension springs (T).

7. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: A plurality of U-shaped bows (U) are arranged at the outer end of the slide rod (H).

8. The sliding elastic inertia power device of an engine as claimed in claim 1, characterized in that: The two sides of the slide bar (H) are symmetrically provided with curved slide bars (SH) to form a slideway. The curved slide bars (SH) are cylindrical rod bodies bent into an arc shape and are located on both sides outside the counterweight iron ball. The two ends of the curved slide bars (SH) are respectively connected to the two ends of the slide bar (H). The two sides of the counterweight iron ball (Q) are symmetrically connected with connecting rods (LG). The connecting rods (LG) are cylindrical rod bodies and are perpendicular to the slide bar (H). A curved slide block (SK) is installed on the connecting rod (LG). The block (SK) is connected to the tension spring or wire rope (T) of the corresponding bow tip (L), a through circular hole is opened in the middle of the curved slider (SK), the connecting rod (LG) passes through the circular hole on the curved slider (SK) and is slidably connected thereto, a universal wheel (B) is installed on the curved slider (SK), the wheel on the universal wheel (B) is a groove pulley, the groove pulley of the universal wheel (B) is engaged with the curved slide bar (SH) on the same side, and slides along the curved slide bar (SH).

9. The sliding elastic inertia power device of an engine as claimed in claim 8, characterized in that: The tension of the U-shaped bow (U) or the tension spring (T) matches the product of the ratio of the actual length of the curved slide bar (SH) to the length of the slide bar (H) and the weight of the counterweight iron ball (Q), and the tension of the U-shaped bow (U) or the tension spring (T) is greater than the product.

10. The sliding elastic inertia power device of an engine as claimed in claim 8, characterized in that: The distance between the two bow tips of the U-shaped bow (U) is greater than the distance between the farthest ends of the two connecting rods (LG) symmetrically arranged on the counterweight iron ball (Q).

Images