Device for Converting Rotary Motion Into Unidirectional Motion

1. Field of the Invention

Along with rocket and jet engines, devices that convert rotary motion into unidirectional motion share the unique characteristic of not requiring engagement with a reactive medium in order to produce a propulsive force. One method of producing an unbalanced centrifugal force is to vary the radius of gyration of a plurality of gyrating masses continuously during their cycle of revolution and in such a manner that each gyrating mass in succession moves through both a maximum-radial-distance predetermined position and a minimum-radial-distance predetermined position during the cycle of revolution. The maximum-radial-distance and the minimum-radial-distance predetermined positions are 180.degree., or a half-cycle of revolution, apart.

Since the magnitude of the centrifugal force, which is produced by a gyrating mass, is proportional to the radius of gyration of the gyrating mass, the sum of the centrifugal force components which are produced by those gyrating masses which are, at a given moment, just approaching, just leaving, and positioned at the maximum-radial-distance predetermined position exceeds the sum of the centrifugal force components which are produced by those gyrating masses which are, at the same given moment, just approaching, just leaving, and positioned at the minimum-radial-distance predetermined position, there is thus a net imbalance of centrifugal force components which can be used to propel a vehicle.

2. Description of the Prior Art

The prior art has provided several systems which, for one reason or another, suffer many disadvantages making them not acceptable to general usage, such as being overly complex to manufacture, require complex driving systems and critically interrelated rotating components, and the like.

An example is the device of I. B. Laskowitz which is described in U.S. Pat. Nos. 1,953,964 and 2,009,780. Laskowitz refers to his device as a "Centrifugal Variable Thrust Mechanism" and discloses a relatively complicated method for varying the magnitude and direction of the resultant unbalanced force. Since the magnitude of the resultant unbalanced force can be varied by simply varying the rate of rotation of the input drive shaft, the only useful function of Laskowitz's variable mechanism is in varying the direction of the resultant unbalanced force. A major problem of Laskowitz's device is that the point of application of the resultant force, relative to the axis of rotation of the gyrating masses, is dependent on the direction chosen for the resultant unbalanced force. This problem is due to Laskowitz's use of two mutually perpendicular shafts to transmit the resultant unbalanced force to two different positions on his device.

The device disclosed in this patent application overcomes all the difficulties inherent in Laskowitz's device. The mechanism disclosed in this patent application also offers improvements and advantages over the "Transmitting Mechanism" which is disclosed in U.S. Pat. No. 1,445,474 (dated Feb. 13, 1923). The "Transmitting Mechanism", which is described in U.S. Pat. No. 1,445,474, employes a circular ring, rather than springs, to keep the roller-type cam followers in contact with an eccentrically-disposed circular cam. The circular ring encircles all of the roller followers and is in rolling contact with each roller follower. The circular ring is thus rotated in a direction which is opposite to that of the eccentrically-disposed circular cam by traction between the circular ring's inner surface and the roller followers. A major fault of this "Transmitting Mechanism" is that, at any given instant, the roller followers are rotating at different rates, thus the rate of rotation of the circular ring can't correspond directly to the rate of rotation of any particular roller follower.

The prior art has provided various methods of supporting and varying the radius of gyration of the gyrating masses and of changing the direction of the resultant unbalanced force, but each of those methods suffers from one or more difficulties or disadvantages. The invention disclosed in this patent application overcomes those difficulties and disadvantages by a simple mechanism which is comprised of a pair of normally non-rotating circular cams which engage a pair of cam followers which are attached to connecting rods which in turn are connected to the gyrating masses.

The direction of the resultant unbalanced force can be selectively changed by simply rotating in unison the pair of normally non-rotating circular cams.

Counterweights are attached to each cam in such a manner that the combined mass of the cam and the counterweight is equally distributed about the axis of rotation of the gyrating masses. This prevents changes in the distribution of mass, relative to the center of mass of a vehicle which is being propelled by the device, when the cams are rotated to change the direction of the resultant unbalanced force.

In the accompanying drawings forming a part of this specification, and in which like reference characters are employed to designate like parts throughout the same:

FIG. 1 illustrates a partial top plan view of the gyrating-mass support structure;

FIG. 2 illustrates a partial elevation of the pair of normally non-rotating, eccentrically disposed, circular cams and how they are mounted for independent rotation of the gyrating-mass support structure. Also illustrated is the method of connecting the gyrating masses to the cams and how the cams are rotated to change the direction of the resultant unbalanced force;

FIGS. 3a, 3b, and 3c illustrate, respectively, the side, the rear, and the top or bottom view of one of the gyrating masses and its associated connecting rod and cam followers;

FIGS. 4a and 4b illustrate, respectively, the side and bottom views of the top cam of FIG. 2;

FIGS. 5a and 5b illustrate, respectively, the side and top views of the lower cam of FIG. 2;

FIG. 6 illustrates a partial elevation of the invention in a cross-sectional view along the line 6 -- 6 of FIG. 1.

Referring now to the drawings in detail and in particular to FIG. 1, the gyrating-mass support structure, 1, contains eight, hollow, cylindrical chambers, 2a - 2h, each of which contains a bearing or bushing, 3. Mounted for sliding radial movement within each bearing or bushing, 3, is a cylindrical mass, 4. Each cylindrical mass, 4, is connected to one end of a connecting rod, 5, by means of a pin, 7. Mounted at the opposite end of and on opposite sides of each connecting rod, 5, are two roller-type cam followers, 8, each of which engages one of the eccentrically disposed, normally non-rotating, circular cams, 9a, 9b (cam 9b is not illustrated in FIG. 1). Cam 9a contains a square hole, 10, which receives an end of a square shaft, 11, (not illustrated in FIG. 1) which protrudes from cam 9b and which allows both cams, 9a, 9b, to be rotated in unison for purposes of changing the direction of the resultant unbalanced force which direction is indicated by arrow 12. The maximum-radial-distance predetermined position is illustrated by the position of chamber 2a and the minimum-radial-distance predetermined position is illustrated by the position of chamber 2e. Each cam, 9a, 9b, has a counterweight, 13a, 13b (13b is not illustrated in FIG. 1), attached to it. The combined mass of each cam, 9a, 9b, and its respective counterweight, 13a, 13b, is equally distributed about the axis of rotation of the gyrating masses and the gyrating-mass support structure 1, in order to prevent changes in the distribution of mass about the center of mass of a craft or vehicle which is being propelled by the device when the normally non-rotating cams 9a, 9b, are rotated to change the direction of the resultant unbalanced force.

Referring now to FIG. 2, the method of varying the radius of gyration of the gyrating masses, 4, and of changing the direction of the resultant unbalanced force are illustrated. A single gyrating mass, 4, is shown connected to the pair of cams, 9a, 9b, by means of connecting rod 5 and cam followers 8. The gyrating mass, 4, is connected to the connecting rod, 5, by means of pin 7. The cam followers, 8, are attached to the connecting rod, 5, by means of shaft 20. Cam 9a has a square hole, 10, which receives one end of a square shaft, 11, which protrudes from cam 9b and which allows both cams to be rotated in unison in order to change the direction of the resultant unbalanced force which is indicated by arrow 12. Shafts, 14a, 14b, are attached, respectively, to cams 9a, 9b, and which allows those cams to be rotated independently of the gyrating-mass support structure, 1. Bearings, 15, and collars, 16, allow the independent rotation of shafts, 14a, 14b, and their associated cams, 9a, 9 b. One end of shaft 14b is attached to a spur gear, 17, which engages a worm gear, 18. The rotation of worm gear 18 causes spur gear 17, shafts 14a and 14b, and cams 9a, 9b, to rotate about their common axis of rotation thus changing the direction of the resultant unbalanced force. Drive shaft, 19, rotates the gyrating-mass support structure, 1, and the gyrating masses, 4. Counterweights, 13a, 13b, are attached to their respective cams, 9a, 9b, in order to equalize the distribution of mass about the axis of rotation of the cams. 21 is part of the frame that supports the entire device.

Referring to FIGS. 3a, 3b, and 3c, a single gyrating mass, 4, is shown attached to a connecting rod, 5, by means of a pin, 7. Roller-type cam followers, 8, are mounted for rotation on shafts or rods, 20, on opposite sides of the connecting rod, 5.

Referring to FIGS. 4a and 4b, cam 9b is illustrated along with its associated shaft, 14b, square shaft 11, and counterweight 13b.

Referring to FIGS. 5a and 5b, cam 9a is illustrated along with its associated shaft 14a, square hole 10, and counterweight 13a.

Referring to FIG. 6, the gyrating-mass support structure, 1, is shown mounted for rotation within frame 21 by means of bearings, 15, and collars, 16. The drive shaft, 19, rotates the gyrating-mass support structure, 1, and the gyrating masses, 4, which are mounted for radial movement within the bearings or bushings, 3, which are located in the cylindrical chambers, 2a - 2e. The gyrating masses, 4, are attached to connecting rods, 5, by means of pins 7. Roller-type cam followers, 8, are mounted at the opposite end of and on opposite sides of the connecting rods, 5. The cam followers on each connecting rod engage the cams, 9a, 9b, and are rotatably mounted on the shafts or rods, 20. Square shaft 11 protrudes from cam 9b and is inserted in a square hole in cam 9a. Cams 9a and 9b are connected to shafts 14a and 14b, respectively, for independent rotation by means of bearings 15 and collars 16. One end of shaft 14b is connected to spur gear 17 which engages worm gear 18. Worm gear 18 is mounted on frame 21 by the partial support 22. The direction of the resultant unbalanced force is changed by rotating worm gear 18 which in turn causes the spur gear 17, shafts 14a and 14b, and cams 9a and 9b to rotate.