DE19800308C1 - Mass displacement engine - Google Patents

Abstract

The engine has at least two pistons moving with the masses (4,4a) which are in equilibrium with opposing pistons (5,6) with accelerating pistons (5,6) which convert the potential energy of the masses into kinetic energy of the pistons. The weights operate on a cam with two different radii (R2,3) which is controlled by a hydraulic control valve circuit (11) for hydraulic force input from an auxiliary water source.

Description

The invention relates to a mass displacement engine Auxiliary energy according to the preamble of claim 1.

Currently, a. Motors known with the help of Combustion power, hydropower, electrical energy, steam and wind energy etc. are driven. A disadvantage of these Motors is that these motors consume a relatively high amount of energy, to achieve acceptable performance, d. H. a bad one Have efficiency. Furthermore, complex systems for Providing the drive energy required, e.g. B. water dams. Motors powered by wind power also mean one considerable effort in preparatory measures and are not exactly predictable, as it depends on the wind. Especially at Combustion engines are also polluting the environment. Furthermore a flywheel drive is known from DE 30 24 960 A1, in which a Flywheel, which has an imbalance, around its horizontal axis rotates and its dead center by one temporarily switched electric motor is overcome.  

A flywheel is described in DE 33 21 844 A1 Moment of inertia with the help of hydraulically displaceable pistons can change. Another solution is in DE 196 13 369 A1 described. It is a device for use the centrifugal force for energy production by means of a Rotation unit with at least one, in the direction of action of the Centrifugally movable mass, whose Translational movement exploited under the influence of gravity becomes. All of these solutions require a significant technical Effort and are therefore not profitable enough.

The invention is based on the task of a motor create, which eliminates the disadvantages of the known devices or deals. So z. B. based on the present functional model can be assumed that a drive with hydropower at least 100 times less water is required, than in previously known small hydropower plants.

The inventive solution to this problem is in Claim 1 specified. Special embodiments of the invention can be found in the subclaims.

It is therefore within the scope of the invention that a Mass displacement engine with auxiliary energy, with a mass on a mass carrier, a circular path on which it  is arranged in the direction of another mass z. B. through the earth the gravitational force is attracted ("falls down"), so designed is that at least two pistons, each with a mass, be moved. These acceleration pistons are in the Balance to each other and are subject to the principle of counteraction. You are going through the free falling first mass on a circular path co-accelerated. Since these accelerating pistons in the Equilibrium, this process is comparable to a accelerated mass-afflicted disc due to an attached mass with a corresponding moment of inertia J at which the potential energy the attached mass in the gravity field z. B. Earth in kinetic Energy of the entire system is converted and vice versa. The The arrangement of the entire system is thus comparable to that of a physical pendulum, in which, however, the back swing through Accelerating piston is prevented. The system is approaching its dead center (i.e. reversal point of the direction of movement) and falls below a certain angular velocity, the Accelerating piston via a control pulse by means of the Auxiliary energy is shifted to a smaller circular path, causing the system accelerated beyond the dead center and thus a rotation of the Systems is achieved. After the dead center is exceeded, the Control impulse, whereby  the acceleration pistons their centrifugal force again take original position and the whole Acceleration process can start again. The fed required auxiliary energy can be generated by water pressure, water vapor pressure, Air pressure or other energy sources are provided.

The invention allows several embodiments. For One of these is illustrated in the Drawings shown and described below. The Drawings show in

Fig. 1 is a schematic representation of the inventive mass displacement motor with power,

Fig. 2 is a schematic representation of a possible control for a mass transfer engine.

Since all mass-bearing bodies in the earth's gravitational field experience differently strong gravitational forces depending on their mass, they are of different weights. Nevertheless, they all fall to earth at a uniform rate, since the gravitational acceleration acting on each body is g = 9.81 m / s ² from the mass of the falling body. The mode of operation of the mass transfer motor is derived from this. A mass displacement engine 1 , according to FIG. 1, is at one location, an inflow, e.g. B. a stream, a river or another falling body of water. However, other media can also be provided as auxiliary energy sources. The auxiliary energy required for this system is z. B. provided that a flowing body of water, 2 or a falling amount of water is closed and introduced 10 m deeper into the system according to the invention. This creates a water pressure of 1 bar at the point of introduction P of the system according to the invention. These differences in height can be changed as desired, which is proportional to a change in the water pressure. The higher the auxiliary energy selected, the more favorable the efficiency of the system according to the invention, since the friction factor will be relatively lower. By coordinating the movements, it is possible to use the gravitational force directly. It is thus possible to perform work by converting potential energy in gravitational potential into kinetic and mechanical energy by means of a small supply of auxiliary energy and to convert the auxiliary energy into the desired form of energy or work with a high degree of efficiency.

The operation of the mass transfer engine 1 is as follows. A mass 3 (m1) attached to a mass carrier is on a circular path 7 (R1) in the direction of a second mass, for. B. dropped the earth. In this free fall, the mass 3 (m1), in this case, moves two further masses 4 , 4 a (m2), which are represented by acceleration pistons 5 , 6 which are in equilibrium with one another and work according to the counteraction principle. Since gravity acceleration is independent of mass, mass 3 (m1) can also accelerate acceleration pistons 5 , 6 in free fall on a circular path 7 (R1). So that the acceleration pistons 5 , 6 each get the momentum to change their position at the right time, two cam disks 9 , 10 and a control unit, here a 3 / 2-way valve 11 , are arranged on a camshaft 8 ( FIG. 2). A closing angle 12 (x1) and an opening angle 13 (x2) are set with these cam disks 9 , 10 . When the mass 3 (m1) reaches the closing angle 12 (x1), the cam radius 9 pushes the tappet shaft 14 of the 3/2 way valve 11 upwards. The pressure P of this 3/2-way valve 11 can now reach A by way of A at a displacement-changing cylinder 15 . The cylinder 15 makes a stroke with a rope pulley 17 with its stroke movement 16 (Z1). A control cable 18 placed around the pulley 17 is anchored on one side at a fixed point 19 . This second end of the control cable 18 is connected by a camshaft bushing 20 to the masses 4 , 4 a (m2) of the rotating system. Since there is a rectilinear and a rotating movement on the control cable 18 , a clutch 21 was provided. Through this fixed point connection 19 of the cable 18 , the cylinder stroke 16 is doubled on the side 22 (Z3). 1 cm of travel on cylinder 15 corresponds to 2 cm of travel in radius 23 (m2) after 24 . Through this process, the masses 4 , 4 a (m2) are shifted from radius 23 (R2) to radius 24 (R3). This shift causes a resulting accelerating angular momentum. After reaching the upper O-point 13 (x2), the control pulse can be omitted and the tappet roller 14 goes back from point 9 to point 10 . As a result of the withdrawal of the control pulse, the masses 4 , 4 a (m2), following the centrifugal force acting on them, can now return from 24 (R3) to the starting position 23 (R2). The piston 15 of the cylinder 15 is brought back into the starting position in connection with the pulley 17 by the corresponding power transmission. 25 with the return stroke is designated Z2. Now the masses 4 , 4 a (m2) are again on the web 23 (R2). The piston of the cylinder 15 is also in the starting position and the acceleration process starts again. There is a control lever 27 on the system for the stroke determination of the cylinder 15 . With position A the system can run without load and with position B with load. The speed can be read on the tachometer 26 . At 28 is a radius (R4), the tap for work delivery. In Fig. 1 a radius displacement segment 29 is shown which is fixedly connected to the control unit of FIG. 2. The mass 3 , (m1) is displaced by the radius displacement element 29 at the beginning of the radius displacement 31 (x3) by a radius displacement roller 33 with connection to 3 (m1) from the circular path 7 (R1) to a smaller circular path determined by the radius displacement element 29 . Due to the reduction in the circular path at the beginning of the radius displacement 31 (x3), the mass 3 (m1) also receives an additional temporary acceleration pulse due to the increase in angular velocity before the top dead center is reached. At the end of the radius displacement 32 (x4), the mass 3 (m1) returns to the initial radius 7 (R1) due to the centrifugal force. The course of the radius shift 33 is designated by 30 (R5). The following parameters influence the process of mass transfer on the circular path. these are

• - mass (m1) x R1,
• - dimensions (m2) x R2,  
• - dimensions (m2) x R3,
• - closing angle x1,
• - opening angle x2,
• - rpm, without load,
• - rpm, with load,
• - Required force for changing the radius,
• - time for the radius change,
• - centrifugal force on the mass (m2),
• - difference between the radii R2 and R3,
• - Mass shift (m2) from R2 to R3 in relation to the Angular velocity increase,
• - friction.

All these parameters influence the efficiency and are in a functioning system in a coordinated assignment each other, and are one for different dimensions Mass-transfer engine to concretize.  

The possible uses of the system according to the invention are diverse. Some of these are listed below. That's the way it is possible to do various work with the system, such as B. Lifting, pushing, etc. Furthermore, it is possible to use electrical current to create. It can be used to generate compressed air and water be pumped. Waste water from multi-storey or high-rise buildings can be designed and used for pressure generation for these systems become. Another area of application is z. B. miniature systems for Play (see steam engine). With the establishment of this facility in certain leisure areas as well as spa and healing facilities new points of attraction can be created. It is also conceivable to have athletes generate energy in strength studios save and use by supplying this energy to the facility becomes.

Reference list

1

Mass transfer engine

2nd

Inflow

3rd

Mass (m1)

4th

1. mass (m2)

4th

a2. Mass (m2)

5

Accelerating piston

6

Accelerating piston

7

R1

8th

camshaft

9

Cam disc (NR2) cam disc radius 2

10th

Cam disc (NR1) Cam disc radius 1

11

Control unit / 3/2 way valve

12th

Closing angle x1

13

Opening angle x2

14

Tappet shaft

15

cylinder

16

Stroke (Z1)

17th

Rope pulley

18th

Control rope

19th

Benchmark

20th

Camshaft bushing for control cable

18th

21

clutch

22

Stroke doubling (Z3)

23

R2

24th

R3

25th

Return stroke Z2

26

Tachometer

27

Control lever

28

R4

29

Radius shift segment

30th

Radius displacement curve R5

31

Radius shift start x3

32

Radius shift end x4

33

Radius displacement roller with connection to (

3rd

, m1)

Claims (11)

1. Mass displacement engine with auxiliary energy, in which a mass falls down on a mass carrier, a circular path on which it is arranged in the direction of another mass (e.g. earth), characterized in that at least two pistons with the mass ( in each case m2) are moved, the masses ( 4 , 4 a, m2) being acceleration pistons ( 5 , 6 ) which are in equilibrium with one another and are subject to the principle of counteraction, in this case the potential energy of the attached mass is converted into kinetic energy, the acceleration pistons ( 5 , 6 , m2), which are connected to a control unit ( 11 ) with an applied pressure, from the radius ( 23 , R2) to the radius ( 24 , R3) and backwards from the radius ( 24 , R3) to the radius ( 23 , R2) are relocatable and thus allow the system to rotate. 2. mass displacement engine with auxiliary energy according to claim 1, characterized in that it emits with a control pulse Control unit for the radius change is provided. 3. mass displacement engine with auxiliary energy according to claim 1 and 2, characterized in that the mass ( 3 , m1) by an offset of the acceleration piston ( 5 , m2) to the other acceleration piston ( 6 , m2) standing in imbalance, is replaced. 4. mass displacement engine with auxiliary energy, according to claims 1 to 3 characterized in that the auxiliary energy required by water pressure, water vapor pressure, air pressure or other Energy sources can be provided. 5. Mass transfer engine with auxiliary energy after previous Claims, characterized in that one or more Revolutions per control pulse can be selected. 6. Mass displacement motor with auxiliary energy according to the preceding claims, characterized in that the centrifugal force acting on the acceleration piston ( 5 , 6 ) (in the rotating system), the return displacement of the acceleration piston ( 5 , 6 ) from ( 24 , R3) to ( 23 , R2 ) causes. 7. mass displacement motor with auxiliary energy according to the preceding claims, characterized in that the centrifugal force through the use of mechanical aids, such as. B. tension or compression springs can be supported, or that the acceleration pistons ( 5 , 6 ) can be brought into the new starting position by the use of mechanical aids. 8. mass displacement motor with auxiliary energy according to the preceding claims, characterized in that the control pressure for the closing angle ( 12 , x1) and the opening angle ( 13 , x2), acting directly on the acceleration piston ( 5 , 6 ), can be switched. 9. Mass displacement engine with auxiliary energy after previous Claims, characterized in that the location of the Control unit is freely selectable.   10. mass displacement engine with auxiliary energy according to the preceding claims, characterized in that the piston movements with the masses (each m2) also by non-linear movements, for. B. can be shifted from the radius ( 23 , R2) to the radius ( 24 , R3) and rearward and the shift is carried out by discs, levers or other connections. 11. mass displacement motor with auxiliary energy according to the preceding claims, characterized in that the mass ( 3 , m1) by a Radiusverlagerungsegment ( 29 ), which is firmly connected to the control unit of FIG. 2, at the Radiusverlagerbeginning ( 31 , x3) by the Radiusverlagerungsrolle ( 33 ) with connection to ( 3 , m1) is moved from the circular path ( 7 , R1) to a smaller circular path determined by the radius displacement segment ( 29 ) and at ( 32 , x4) the mass ( 3 , m1) comes from the centrifugal force back to the initial radius ( 7 , R1).