WO2018087772A1

WO2018087772A1 - Unidirectional momentum generating machine

Info

Publication number: WO2018087772A1
Application number: PCT/IN2016/050393
Authority: WO
Inventors: Achal MOHANDAS
Original assignee: Mohandas Achal
Priority date: 2016-11-09
Filing date: 2016-11-09
Publication date: 2018-05-17

Abstract

This is a unidirectional linear momentum generating machine which can generate a force in one particular direction without a reaction force. This machine basically converts an elliptical motion into a linear motion by inducing a momentum inversion on a rotating matter and thereby using the reaction force generated by that to push the whole machine forward.

Description

Title

UNIDIRECTIONAL MOMENTUM GENERATING MACHINE

Technical Field

[0001] Related to Mechanical Engineering.

Disclosure of Invention

[0002] This is a unidirectional momentum generating machine. This machine is capable of generating a force in one particular direction and won't exert any force in the opposite direction. This machine's working maybe against some known laws in science, but this machine can work flawlessly in practice and theory. This machine primarily converts the rotational motion into a linear motion. The rotation however is an elliptical one and not circular. The main theory behind the working of this machine is, a controlled one directional push resulting in an opposite directional centrifugal force generated on a rotating matter due to the momentum inversing of the rotating matter. This will be elaborated in the following paragraphs.

[0003] The main parts of this machine are, a motor or an engine to drive, a

rotating axis which can slide on both directions on a shaft connected to the motor, two magnets attached on the both ends of the axis, a static magnet and a main body on which the motor and the static magnet are placed. The static magnet which is placed on the main body and the rotary magnets which are placed on the both ends of the axis are kept in a repulsive position. The like poles of the static and rotary magnets are kept face to face in order for it to repel each other. There is an imaginary elliptical rotary path that is showed in the diagrams. The rotating axis and the magnets on it should exactly follow this elliptical path while rotating. This elliptical path of the axis is created by the repulsion of the rotary magnets A and B to the static magnet. The static magnet which is attached to the main body is usually made of permanent magnets. The repulsive strength of this magnet to the rotary magnets can be adjusted by moving it back and forth or coupling the permanent magnet with an electromagnet or replacing it with an electromagnet. The driving motor or engine speed can also be adjusted in order to adjust the RPM (rotation per minute) of the axis. The shaft of the motor is connected to the rotating axis using a ball bearing to reduce friction. The rotary axis can also slide on the shaft on both directions from the centre according to the forces action up on it.

Now we will look how the machine generates a unidirectional force from the rotation of the axis. Consider the axis is rotating in high speed in counter clockwise direction. When the magnet A reaches 0°, it will be nearest to the centre point of the circle compared to the magnet B which will be at the farthest position from the centre of the circle as shown in diagram 1. In this point if the axis moves, the outward centrifugal force will act up on the magnet B because it is farthest from the centre compared to magnet A. Then when the magnet A leaves 0° and rotates further, it will come face to face with the static magnet and both are kept in repulsive position to each other. The static magnet and the driving motor are attached to the main body so that the repulsion between the static magnet and the magnet A will result in a forward movement of the main body and the backward movement of the magnet A or the magnet around 0° along with the axis and magnet B. The RPM of the motor should be finely tuned for both the magnet A and B to be in a equidistant position from the centre when the magnet A reaches 90° and the magnet B reaches 270° as shown in diagram 3. The magnet A and magnet B should follow the imaginary rotary path accurately so that the RPM of the motor should be adjusted accordingly. When the magnet A rotates from 0° and come face to face with the static magnet, it will start to move backwards and the static magnet along with the main body will start to move forward. The repulsion between magnet A and the static magnet will be maximum at 0° because both will be nearest at 0° and the repulsion will continue until the magnet A reaches 90°. The repulsion however will get reduced when the magnet A rotates further away from 0° towards 90°. This is due to the increasing of distance between the static magnet and the magnet A. However if we want to keep the repulsion at the maximum level until 90°, the angle of the static magnet should be adjusted accordingly. But this is not needed as the centrifugal force will get reduced as the magnets approach 90°. The magnet A will move backward and the main body with the static magnet will move forward when the axis rotates from 0° to 90° because of the repulsion and this movement will continue even after the magnet A goes over 90°. The magnet A will continue to move away from the main body even after the repulsion is gone at 90° because of the outward force it already acquired before. In simple words the inertia of the magnet A along with the axis will make it move away from the main body until it reaches 180°and that is the maximum distance the magnet A can go from the centre point. The magnetic repulsion however will end at 90°, but the force due to inertia will continue to act on the magnets and axis further away from 90° until the magnet A reaches 180°. In short, the magnets should follow the imaginary rotary path accurately and this means the magnets should start at minimum distance from the centre point at 0° and should be equidistant between each other when it reaches 90° and should be at the farthest point when it reaches 180°. The RPM of the motor and the power of the magnets should be adjusted accordingly and accurately for the magnets to follow the imaginary rotary path. When the magnet A reaches 180° the magnet B will be at 0° and whole process will repeat, means what happened to magnet A will happen to magnet B. This kind of rotation will make a centrifugal force on the magnet around 180° to 270° which will be the maximum at 180° because that magnet will be at the farthest from the centre and will be minimum or null at 270° because both the magnets will be equidistant from the centre. This centrifugal force generated at 180° to 270° will act on the opposite side and will act as a counter force against the repulsion of the static magnet and the magnet that goes from 0° to 90°. This is where the unidirectional force is created. In simple words the push of the static magnet to the rotary magnets from 0° to 90° will result in a centrifugal force at 180° to 270° because of the inability or inertia of the axis with the magnets to move quickly away as it gets pushed or repelled and also due to the centrifugal force experienced by the magnets rotating from 180° to 270°. The imaginary rotary path should be strictly followed by both the rotary magnets on the axis in order for the device to work and get the maximum performance.

Here the RPM of the motor should be changed according to the velocity of the main body in order to keep the axis following the imaginary rotary path. This is because when in still position the main body doesn't move and only the rotating axis and the magnets attached to it moves due to the repulsion so that the magnets will be equidistant from each other when it reaches 90° and 270° at lesser RPM than when the main body is moving and the RPM should be reduced in order for the magnets on the axis to follow the imaginary rotary path. Then when the main body starts to move forward in any angle greater than 180°, then the rotating magnets from 0° to 90° and 180° to 270° should go faster in order for it to keep up with the imaginary rotary path or to be equidistant from each other at 90° and 270°

respectively. The main body in fact doesn't move in straight direction at 180°, but after the effect of all forces and its vectors, it will go anywhere around 180°. Practically the main body will move away from the imaginary rotary path on an angle almost opposite to 0° to 90° or greater than 180° while it gains velocity because of the angle of repulsion of the static magnet to the rotary magnet and due to this the magnets on the axis rotating from 0° to 90° and 180° to 270° should move faster for it to keep up with the imaginary rotary path. This means RPM should be increased accordingly. So the velocity of the main body and RPM of the axis is directly proportional in this case. In any case or in any velocity the imaginary rotary path should be followed by the rotary magnets exactly and the speed of the rotation should be adjusted accordingly. This machine can be also designed for a clockwise rotary action of the axis in contrast with the counter clockwise rotary action that is shown in all the designs here. The only difference is that the position of the static magnet will change and the direction of the forces will be according to that.

However both the designs will yield the same result and can be done in any way according to the need.

Here we will also look at the starting scenario when the axis just begins to rotate. When the rotation of the axis starts from 0° or when it reaches 0° at the beginning, there will be no centrifugal force acting on the axis and there will be enough time for the rotary magnet at 0° to reach the farthest point from the centre even before it reaches 90° due to the repulsion of it with the static magnet. This will continue until 180° and the opposite magnet will be at 0° at this time and will be closest to the centre point. But due to the low centrifugal force acting up on the magnet at 0° because of the low rotation speed, the rotary magnet will get repelled to the farthest point before it reaches 90°. This will continue until enough centrifugal force has been acquired by the magnets due to the increased speed of the rotation of axis and when the axis reaches the right RPM, the magnet at 0° will reach the farthest point at 180° and will starts to follow the imaginary rotary path accurately. We can also adjust the power of the static magnets or rotary magnets and can achieve the correct rotary path in different RPM. Usually it is easier to have a permanent magnet at the axis and variable strength magnet as static magnet. There are also other things that affect the working of this device, like the mass of the rotary magnets and the axis, the angle of both the static magnet and the rotary magnet and the orientation of the machine according to the gravity of the Earth. In any case the imaginary rotary path should be followed accurately. The static magnet can be made fully by an electromagnet or the magnetic forces of the static magnet can be shielded for it not to get extended beyond 0° to 90° in order for it to avoid unnecessary influences on the rotary magnets. The magnetic flux on the sides of the rotary magnets could also be shielded for it not to have any unwanted influence on the static magnet. Another way of arranging both the rotary and static magnet is to place both parallel to each other. This means that we should place both the magnets parallel like both the poles of the magnets will be on top and bottom and to place both magnets near to each other like the south and north of both of the magnets should be near to each other respectively. This arrangement will reduce the effect of unwanted magnetic influences between both the static and rotary magnets.

[0007] We can also make this machine by placing the static magnet around the position from 180° to 270° in an attractive way as shown in diagram 8. It will be like both the rotary magnets A and B in an attractive position to the static magnet kept between 180° and 270°. So the working will be the same like before but there will be attraction instead of repulsion and here the rotary magnets will start to attract the static magnet at 180° and will continue to get attracted until 270°. This design is practically little bit hard to make because the static magnet should be very near to the rotary magnet at 180° in order for it to generate maximum pull force. This is because the maximum centrifugal force will be at 180° and in order to take advantage of that, the magnets should be close enough to have a strong attraction. However when the machine just starts or the axis just starts to rotate, there will be very less centrifugal force and due to this the static magnet will pull the rotary magnet at 180°completely towards it and both will collide due to attraction. In order to avoid this, at the starting phase of the machine or when the axis just starts to rotate the static magnet should be positioned backward enough in order for it to avoid attracting the rotary magnets fully. However the static magnet can be brought back near to the rotary magnet once the rotary magnets along with the axis achieve enough RPM and generate considerable centrifugal force in order for it not to get attracted by the static magnet fully but to keep up with the imaginary rotary path accurately. The rest of the working of this design is same like that in the repulsive design. Only difference is that the rotary magnets will be attracted by the static magnet that is fixed to the main body from 180° to 270° instead of it getting repelled by the static magnet from 0° to 90°.

[0008] In another design we can omit both the magnets on the axis and the main body and instead create the backward push mechanically by putting a solid semi ring on the main body and two ball bearings on the rotary axis or vice versa and use two solid masses on the both ends of the axis in order to provide better centrifugal force while rotating as shown in diagram 7. But this design is less energy efficient than the design using magnets because of the friction caused between the solid semi ring and the ball bearings. This arrangement works as same like the designs using magnets, but the only difference is that the push force is directly fed to the main body form the axis through the ball bearing that slides on the semi ring while it rotates. This semi ring will only allow the axis to go on a specified path and push the axis backward through the ball bearing to keep the axis with the imaginary rotary path. We can also use a semi ring track instead of a plain semi ring and make the ball bearing slide through that track in order for it to keep up with the rotary path, but this is not required because the push on the axis caused while sliding it through the semi ring itself will keep up with the exact path as only a push from the semi ring is required on the axis and after reaching the right RPM the axis will follow the imaginary rotary path accurately and thereby creates the push force required for the main body to move forward. In this device the RPM of the rotary axis should be maintained accurately. Here there is a possibility that the RPM can change due to friction when the ball bearing slides the semi ring. This should be avoided by placing a fly wheel on the shaft of the motor that is connected to the rotary axis to increase the moment of inertia and thereby mitigating the problem of lowering the RPM due to friction.

Vector Forces

[0009] There are many forces that act on the working this machine. They are the inertia of the main body and the axis, the force created by the single sided centrifugal action and the reaction force created by the motor or engine while it rotates the axis. The total output momentum will be a vector sum of all these forces. This is shown in diagram 6. First we will look at the reaction force generated on the motor while it rotates the axis. Consider the magnet A on the axis at 0° and it will be closest to the centre point at this position and the opposite magnet B will be farthest from the centre. When the magnet A is at 0° and it starts or continue to rotate towards 45°, then the opposite magnet B will rotates towards 225° at the same time. Here the magnet B will be at the farthest position from the centre when it is at 180° and due to this when the motor try to rotate the axis, the magnet B will exert a counter force on the motor which is connected to the main body. The counter force will be perpendicular to the axis and will be at 90° when the magnet B is at 180°. The magnet A however won't create a counter force to the motor because it will be near to the centre point when it starts from 0°. In simple words magnet B being farther away from the centre, will behave like a one sided mass that rotates on the axis. The counter force that starts at 90° will carry on as the axis rotates and will be at 135° when the magnet B reaches 225°. However the counter force will be lesser at 135° than at 90°. This is because when the magnet B rotates and reaches 225° from 180°, it will be nearer to the centre point than before. The counter force will be highest when the magnet B is at 180° and will get reduced when it rotates towards 270° and will be lowest or zero when it reaches 270°. There won't be any counter force at 180° or when the magnet B reaches 270° and the magnet A at 90° because both will be equidistant from the centre point at these angles. So in summary the counter force will begin and will be maximum on the motor at 90°, when the magnet A is at 0° and magnet B at 180°. The counter force on the motor will reduce and will be zero at 180°, when the magnet A is at 90° and magnet B at 270°.

Now the magnet A is at 90° and when it continue to rotate with the axis it will go further from the centre point and the magnet B will come closer to the centre point. This means that there will be more mass on the side of the magnet A which is rotating and approaching 135°. A counter force perpendicular to 90° will start to generate at 0° on the motor which is connected to the main body. This force will increase when the axis rotates further and when the magnet A reaches 135° the counter force will be at 45°. This counter force will be highest at 90° when the magnet A reaches 180°. This is because the magnet A will be at farthest position from the centre when it is at 180°. The magnet B will be at 0° and nearest to the centre at this position. Again the whole process will repeat with magnet B as it happened to magnet A while it turned from 0° to 180°. Due to this an even outward force is created from 0° to 180° on the motor and the main body which is connected to it. This outward counter force will be highest at 90° and will be lowest at 0° and 180°. The total vector force will push the main body and motor towards 90° because the highest force is at 90° and an even force starts from 0° and 180° and gets highest at 90°.

Now we will look at the force created by the push between the static magnet attached to the main body and the two magnets A and B on the axis while it goes through the magnetic repulsion path between 0° and 90°. This force is one of the reason why the one sided centrifugal action occurs at 180° to 270°. When the magnet A is at 0° and starts rotating towards 90°, it will get repelled by the static magnet. The repulsion will be highest at 0° because the magnet A will be closest to the centre at 0° and the magnet B will be farthest from the centre at 180°. The magnet A will also be the closest to the static magnet at 0°, hence it will get the maximum repulsion. Due to this the main body along with the static magnet will be repelled by magnet A and the main body will move in an opposite direction to magnet A. This force however will get reduced and will be minimum or null when the magnet A is at 90°and B at 270°. This is because both the magnets will be equidistant from each other at this point and won't be having any centrifugal force. So there will be maximum push towards 180° and minimum or no push towards 270°. The forward push or momentum will get reduced from 180° to 270°. The repulsion between the static magnet and the rotary magnets will also ends at 90°. The magnet B also will go through the path of magnet A, from 0° to 90° and will get repelled by the static magnet in the same way as it happened to magnet A. All the things that are occurring will be same in the case of both the magnets A and B. Position and the angle of the static magnet can also be adjusted for it to repel the magnets coming face to it. The maximum centrifugal force will be at 180° and the minimum at 270°. So there should be a maximum repulsion at 0° and minimum at 90° in order for the rotary magnets to keep up with imaginary rotary path. However adjustments in angle and position of the static magnet and rotary magnets can be made for fine tuning. Here the maximum forward momentum on main body will be at 180° and the minimum will be at 270°.

[0012] So due to the two forces like the reaction force on the motor by the rotation of the axis and the forward force on the main body by the repulsion of magnets, the total vector force or momentum that will be on the main body will be in a direction between 270° and 90°. In reality the vector force will be at a direction almost close to 180° because this is the angle where the maximum forward momentum will be there and the rest of the force vectors will direct the motion towards 180°. There will also be another force on the machine produced due to the rotation of the motor or engine. The motor body which is connected to the main body will tend to rotate in an opposite direction to the direction of the rotation of the motor. This force however is only a rotary one and can be countered by attaching another motor to it which rotates on similar speed or by attaching two machines side by side so that the rotary force on the main body of the two machines will cancel out each other.

[0013] Another force acting upon the main body and the axis is the inertia. Inertia is one of the reasons why the magnets A and B don't move suddenly when it is pushed by the static magnet, other being the centrifugal force that the rotary magnets already have. Due to the inertia, it will take some time for the static magnet to push the rotary magnets backward while it rotates from 0° to 90° and it is the same inertia that is keeping the rotary magnets moving away to the farthest point from the centre while it rotates from 90° to 180° even when the repulsion is gone between the static and rotary magnets. So the inertia is one of the reasons why the rotary magnets are keeping the imaginary rotary path. So inertia is one of the reasons why the one sided push from the static magnet results on the opposite directional centrifugal force. The RPM of the motor should also be adjusted

accordingly in order for the rotary magnets to follow the imaginary rotary path. However the backward push of the static magnet to the rotating magnets which results on the forward motion of the main body along with the rotary magnets won't result in any one directional motion because, the total momentum acquired by the main body by the backward push of the rotary magnets along with the axis will be cancelled by the force required to pull the rotary axis and the magnets along with the main body. This means when the main body along with the motor moves forward, the motor shaft which is connected to the rotating axis will pull the rotating axis and the rotary magnets along with it and due to this the forward push generated on the main body by the repulsion of the static and rotary magnets due to the inertia of the axis and rotary magnets will be cancelled by the force required for the axis and the rotary magnets to be pulled forward by the main body. Hence the one directional momentum is only created by the centrifugal force of the magnet that is rotating at 180° to 270°. The inertia of the rotary magnets and axis will only help to achieve this one directional centrifugal force by delaying the effect of the push caused by the static magnet to the rotary magnet and thereby keeping the rotary magnets on the imaginary rotary path accurately. So the backward push of the static magnet to the rotary magnets results in an opposite side centrifugal force by momentum inversing due to the inertia and the existing centrifugal force of the rotary magnets and the axis.

Brief Description of Drawings

[0014] There are total of eight drawings here and the drawings 1 to 5 shows the path taken by the rotary magnets on the axis through the imaginary rotary path. The diagram 6 shows the forces involved in this machine during its working and the diagram 7 shows the design with magnets omitted and it's working using mechanical push. The diagram 8 shows the design in which there is an attraction between the static and rotary magnets in order to create the one directional momentum.

[0015] Diagram 1 to 5 shows different angles of the rotation of the axis along with the magnets. In these diagrams there are two magnets, namely magnet A and magnet B mounted on an axis that is attached to a shaft of the motor by using a ball bearing. The axis has a sliding hole in which it can move in either way in one dimension. There is a static magnet which is like a semi ring and extends from 0° to 90° and the position and power of the magnet can be adjusted. Usually a permanent magnet is used, but an

electromagnet or a hybrid combination of electromagnet and permanent magnet can be used in order to adjust the magnetic strength. The static magnet and the rotary magnets on the axis are kept in repulsive position. The like poles of both the magnets will be kept face to face. There is the main body in which the static magnet and the driving motor or the engine is fitted. The imaginary rotary path is the path that should be followed by both the rotary magnets on the axis while rotating. The diagram 1 shows the magnet A at 0°, the diagram 2 shows the magnet A at 45°, the diagram 3 shows the magnet A at 90°, the diagram 4 shows the magnet A at 135° and the diagram 5 shows the magnet A at 180°. The rest of the things in the diagram 1 to 5 are the same. The magnet B will also rotate the same way like magnet A starting from 0° to 180° and will follow the same imaginary rotary path.

[0016] The diagram 6 shows the different forces generated while the machine works. The reaction force generated on the motor while the axis rotates is shown in the semi-circular line from 0° to 180°. Here the maximum reaction force is generated at 90° and the minimum is at 0° and 180°. The force will increase towards 90° from 0° and 180°. The reaction force generated due to the repulsion of static magnets and the rotary magnets is shown in the semi-circular line between 180° and 270°. Here the maximum force will be at 180° and the minimum at 270°. This force is the result of the one sided centrifugal force generated on the magnet around 180° to 270°. The diagram also shows the counter clockwise rotation direction of the axis. In this diagram the axis and the rotary magnets are not shown, but only the direction is shown. The other parts like the main body, static magnet, the driving motor or the engine and the imaginary rotary path are same like that in diagrams from 1 to 5.

[0017] In diagram 7 there is a different design. This design doesn't uses magnets in order to create push force at 0° to 90°, but do it by sliding two ball bearings that are attached to the axis on a semi ring that is attached to the main body. The two ball bearings are attached to the axis by an elastic material for a suspension. The push force is created when the ball bearing touches and slides through the semi ring starting from 0° until 90°. In this design two solid masses A and B that is mounted on the axis is used to increase the centrifugal force. The rest of the parts and working of this design is same as like in the diagrams 1 to 5. Here also the imaginary rotary path should be followed accurately by the rotary magnets and the axis in order for the machine to work perfectly. The only difference is that the push force is created mechanically by the ball bearing sliding on the semi ring. In this diagram, only the magnet A at 45° and B at 225° is shown. However the working will be same as like in the diagrams from 1 to 5 in which both the magnets A and B goes through 0° to 180° following the imaginary rotary path accurately.

In diagram 8 the static magnet is placed between 180° and 270° in an attractive position to the rotary magnets instead of the repulsive

arrangement in other designs. This design works by attracting the rotary magnets by the static magnets and thereby creating the centrifugal force required while keeping the rotary magnets on the imaginary rotary path. The position of the static magnet here can also be adjusted in order to change the magnetic strength of it in required conditions. All other parts of this design are the same like in the repulsive arrangement shown in diagram 1 to 5. The repulsive arrangement is practically better than this arrangement because this arrangement requires different adjustments of the static magnet according to the RPM of the machine as described in above paragraphs about the working of this design.

Prior Art

[0019] There are many designs already patented that are said to convert rotary motion into linear one, but everything failed to work practically because of the strict working conditions required for the machine to work. However there is no design that works exactly the same as this one and all of them varies considerably in design and working. As of now no previous designs have achieved a practical unidirectional motion mechanically.

The Best Mode for Carrying Out the Invention

[0020] The best mode for carrying out the invention is the design showed in the diagram from 1 to 5. This is a design that uses magnetic repulsion to achieve the unidirectional force.

Mode(s) for Carrying Out the Invention

[0021] There are three modes that are defined here that are shown in diagrams.

1 The design shown in diagram 1 to 5 which uses magnetic repulsion for achieving the unidirectional motion.

2 The design shown in diagram 8 which uses magnetic attraction to achieve unidirectional motion.

3 The design shown in diagram 7 which uses a mechanical method to generate the push required for a unidirectional force.

Industrial Applicability

[0022] This machine can be used to propel any kind of aircrafts, land vehicles or ships and can also be used to make vertical take-off and landing vehicles. This can be also used to propel any spacecraft's in space.

Claims

Claim 1. A unidirectional momentum generating machine, comprising: a main body; a motor or an engine with shaft to drive; a static magnet; a rotating axis having a sliding path on the centre; and two magnets mounted on both sides of the rotating axis. The rotary axis which revolves around with two magnets on both sides repels the static magnet kept on the main body when it rotates. The rotary magnets follow an imaginary rotary path that is created by the repulsion of the magnets. The one sided repulsion of the magnets will create a force which results in an opposite direction centrifugal force which pushes the main body forward.

Claim 2. A unidirectional momentum generating machine, comprising: a main body; a motor or engine with shaft to drive; a static magnet; a rotating axis having a sliding path on the centre; and two magnets mounted on both sides of the rotating axis. The rotary axis with two magnets which revolves around will get repelled by the static magnet as shown in the diagram 1 to 5. The rotary magnets follow an imaginary rotary path as shown in the diagrams. The one sided repulsion between the rotary and static magnets will result in an opposite directional centrifugal force which helps the machine to move forward.

Claim 3. Making of a unidirectional momentum generating machine,

comprising the steps of: placing an axis with two magnets mounted on its sides on a motor or an engine; and allowing it to slide on both directions from the centre; and placing the motor or engine along with a magnet on a main body; and allowing the magnets on the axis and the magnet on main body to repel each other while rotating the axis. The rotary axis follows an imaginary rotary path which enables it to create a one directional centrifugal force due to the repulsion between the magnets on the opposite side of the created centrifugal force.

Claim 4. A unidirectional momentum generating machine, comprising: a main body; a motor or an engine with shaft to drive; a static magnet; a rotating axis having a sliding path on the centre; and two magnets mounted on both sides of the rotating axis. The rotary axis which revolves around with two magnets on both sides attracts the static magnet kept on the main body when it rotates. The rotary magnets follow an imaginary rotary path that is created by the attraction of the magnets. The one sided attraction of the magnets will create a force which results in an opposite direction centrifugal force which pulls the main body forward.

Claim 5. A unidirectional momentum generating machine, comprising: a main body; a motor or engine with shaft to drive; a static magnet; a rotating axis having a sliding path on the centre; and two magnets mounted on both sides of the rotating axis. The rotary axis with two magnets which revolves around will get attracted to the static magnet as shown in the diagram 8. The rotary magnets follow an imaginary rotary path as shown in the diagrams. The one sided attraction between the static and rotary magnets will result in an opposite directional centrifugal force which helps the machine to move forward.

Claim 6. Making of a unidirectional momentum generating machine,

comprising the steps of: placing an axis with two magnets mounted on its sides on a motor or an engine; and allowing it to slide on both directions from the centre; and placing the motor or engine along with a magnet on a main body; and allowing the magnets on the axis and main body to attract each other while rotating the axis. The rotary axis should follow an imaginary rotary path which enables it to create a one directional centrifugal force due to the attraction between the magnets on the opposite side of the created centrifugal force.

Claim 7. A unidirectional momentum generating machine, comprising: a main body; a motor or an engine with shaft to drive; a rotating axis having a sliding path on the centre; a sliding ring; a ball bearing; and two solid masses mounted on both sides of the rotating axis. The rotary axis which revolves around has two solid masses attached to both sides in order for it to get an increased centrifugal force and is pushed by the sliding ring connected to the main body on a circular path while it rotates on a definite angle. The rotary axis follows an imaginary rotary path created by the push of the rotary axis to the sliding ring through the ball bearing. The sliding ring can also be connected on the rotating axis and the ball bearing on the main body. Here the one sided push of the sliding ring on the axis will create an opposite side centrifugal force which moves the main body forward.

Claim 8. A unidirectional momentum generating machine, comprising: a main body; a motor or an engine with shaft to drive; a rotating axis having a sliding path on the centre; a sliding ring; a ball bearing; and two solid masses mounted on both sides of the rotating axis. The rotating axis that revolves around will get pushed through a ball bearing by the semi ring attached to the main body as shown in diagram 7. The rotary axis should follow the imaginary rotary path as shown in the diagram. The one sided push between the rotary axis and the sliding ring will result in an opposite directional centrifugal force which moves the machine forward.

Claim 9. Making of a unidirectional momentum generating machine,

comprising the steps of: placing an axis with two solid masses mounted on its sides on a motor or an engine; and allowing it to slide on both directions on the shaft of the motor; and placing the motor or engine along with a sliding ring on a main body allowing the axis to be pushed by the sliding ring while it rotates. The axis while rotating follows an imaginary rotary path which enables it to create a one directional centrifugal force due to the push by the sliding ring on the axis on the opposite side of the generated centrifugal force.

Claim 10. A unidirectional momentum generating machine, comprising: a

rotating axis; a main body; a pull or push device attached to the rotating axis; a pull or push device attached to the main body; and a motor or engine to drive. The rotary axis while rotating will be pulled or pushed at a definite angle by the other pull or push device attached to the main body. This creates a rotary path which the axis rotates accordingly. The push or pull in one direction will create a unidirectional centrifugal force on the rotating axis in the opposite direction.