Combined propellant-less propulsion and reaction wheel device

Abstract

A method of de-spinning a rotor of a propulsion system includes providing one or more spinning rotors rotatably mounted on a frame with a bearing having a bearing outer race, bearing balls, and bearing inner race; providing a force mechanism coupled with the one or more spinning rotors for applying a load to the one or more spinning rotors; and loading an outer portion of the outer bearing race, bearing ball, and inner bearing race of the bearing, a load on the outer portion of the bearing race, bearing ball, and inner bearing race of the bearing corresponding to a force applied to the one or more spinning rotors by the drive mechanism. The one or more spinning rotors de-spin at a rate corresponding to the load on the bearing balls.

Claims

1. A method of de-spinning a rotor of a propulsion system, the method comprising: providing one or more spinning rotors rotatably mounted on a frame with a bearing having a bearing outer race, bearing balls, and bearing inner race; providing a force mechanism coupled with the one or more spinning rotors for applying a load to the one or more spinning rotors; loading an outer portion of the bearing outer race, bearing balls, and bearing inner race of the bearing, a load on the outer portion of the bearing outer race, bearing balls, and bearing inner race of the bearing corresponding to a force applied to the one or more spinning rotors by the force mechanism; wherein the one or more spinning rotors de-spin at a rate corresponding to the load on the bearing balls.

2. The method of claim 1, wherein the one or more spinning rotors comprises a pair of synchronized rotors.

3. The method of claim 2, further comprising a plurality of permanent magnets and arranged such that at least one permanent magnet of a first of the pair of synchronized rotors is attracted to at least one permanent magnet of a second of the pair of synchronized rotors when the permanent magnets are proximate one another at an inboard orientation.

4. The method of claim 3, further comprising providing one or more electromagnets located proximate to the pair of synchronized rotors, wherein the one or more electromagnets are aligned with the plurality of permanent magnets such that a rotational force is imparted on the pair of synchronized rotors when the one or more electromagnets are activated.

5. The method of claim 1, further comprising providing a vehicle on which the frame is mounted.

6. A reaction wheel thrust mechanism comprising: a first rotor rotatably coupled on a frame at a first bearing, the first bearing having a first outer bearing race, a plurality of first bearing balls, and a first inner bearing race; a second rotor rotatably coupled on the frame at a second bearing, the second bearing having a second outer bearing race, a plurality of second bearing balls, and a second inner bearing race; a plurality of permanent magnets located on the first rotor and the second rotor, the plurality of permanent magnets oriented such that at a first permanent magnet on the first rotor is attracted towards at a second permanent magnet on the second rotor when the first permanent magnet is at its most proximate location relative to the second permanent magnet to impart a force on the first bearing balls of the first rotor and the second bearing balls of the second rotor; a controller for controlling rotation speeds of the first rotor and the second rotor; wherein when electro-magnetic coils of the first rotor are activated by the controller, the electro-magnetic coils impart a torque onto the first rotor and the first rotor will impart reactionary torque onto the electro-magnetic coils and the frame and a vehicle attached thereto; and wherein when electro-magnetic coils of the first rotor are de-activated by the controller, the force imparted on the first bearing balls of the first rotor and the second bearing balls of the second rotor de-spin the first rotor and the second rotor.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) Further features, aspects, and advantages of the present disclosure will become better understood by reference to the following detailed description, appended claims, and accompanying figures, wherein elements are not to scale so as to more clearly show the details, wherein like reference numbers indicate like elements throughout the several views, and wherein:

(2) FIG. 1A shows an isometric view of one embodiment of a known self-propelling apparatus with integral electro-magnetic coils and permanent magnets mounted at the mid-plane of rotors with integrated spur gear profile for synchronization shown with a cut away in its enclosing shell and top plate for clarity;

(3) FIG. 1B shows an isometric view of one embodiment of a known self-propelling apparatus with integral electro-magnetic coils and permanent magnets mounted at the mid-plane of rotors with integrated spur gear profile for synchronization shown with a cut away in its enclosing shell and top plate for clarity;

(4) FIG. 2 shows an isometric view of one embodiment of a self-propelling apparatus with integral electro-magnetic coils and permanent magnets mounted at the mid-plane of rotors with integrated spur gear profile for synchronization shown without a top or enclosing element;

(5) FIG. 3A shows a top schematic view showing magnet pole orientation along with a first operating mode rotation direction and thrust direction relationship according to one embodiment of the present disclosure;

(6) FIG. 3B is a top schematic view showing magnet pole orientation along with a second operating mode rotation direction and thrust direction relationship according to one embodiment of the present disclosure;

(7) FIG. 4 is a close-up view of rotor bearings showing an outboard loading case along with outer-race and ball bearing rotation of both a first rotor and a second rotor according to one embodiment of the present disclosure;

(8) FIG. 5 is an exploded close-up view of a single bearing ball element and inner race element of both a first rotor and a second rotor illustrating the loading, normal and frictional forces according to one embodiment of the present disclosure;

(9) FIG. 6 is a graph showing the variation of loading in the +X direction on a first rotor due to the net magnetic attraction forces between its magnets and the magnets on a second rotor according to one embodiment of the present disclosure;

(10) FIG. 7 is a graph showing the relationship of rotor speed to generated thrust for rotors subjected to loading shown in FIG. 6 according to one embodiment of the present disclosure;

(11) FIG. 8 is a circuit schematic view illustrating an H-bridge unipolar electronic speed controller for a single set of coils around a single rotor;

(12) FIG. 9 is a circuit schematic view of a portion of the electronic control that allows current direction through the coils to be reversed thereby enabling thrust and reaction wheel direction control according to one embodiment of the present disclosure;

(13) FIG. 10 is a schematic view illustrating a series connection of a single set of rotor coils according to one embodiment of the present disclosure;

(14) FIG. 11 is a circuit schematic view of a portion of the electronic control circuit that allows a single set of rotor coils to be shorted to itself for enhanced reaction wheel function according to one embodiment of the present disclosure;

(15) FIG. 12 is a simplified control block diagram showing how the spacecraft controller/CPU, propulsion/reaction wheel device and spacecraft sensors could be used together according to one embodiment of the present disclosure; and

(16) FIG. 13 is a schematic illustrating the first stage of first rotor and second rotor independent control circuits according to one embodiment of the present disclosure.

DETAILED DESCRIPTION

(17) Various terms used herein are intended to have particular meanings. Some of these terms are defined below for the purpose of clarity. The definitions given below are meant to cover all forms of the words being defined (e.g., singular, plural, present tense, past tense). If the definition of any term below diverges from the commonly understood and/or dictionary definition of such term, the definitions below control.

(18) The terms, “for example,” “e.g.,” “in one/another aspect,” “in one/another scenario,” “in one/another version,” “in some configurations,” “in some implementations,” “preferably,” “usually,” “typically,” “may,” and “optionally,” as used herein, are intended to be used to introduce non-limiting embodiments. Unless expressly stated otherwise, while certain references are made to certain example system components or services, other components and services may be used as well and/or the example components may be combined into fewer components and/or divided into further components.

(19) Embodiments herein provide a self-propelling propulsion system powered with electricity and utilizing at least two synchronized rotors each with a multiplicity of electro-magnets or permanent magnets mounted along each rotor's perimeter which interact with the other rotor's magnetics through attracting or repelling forces. In some embodiments the rotors may be spun through use of an integral set of integral electromagnetic coils or through separate electric motors connected with a gear box. With either embodiment the device may be used to changed vehicle orientation through reactionary torques produced on the integral coil or separate electric motor stator elements. In the following description, numerous specific details are set forth. However, it is understood that embodiments may be practiced without these specific details. In other instances, well-known materials, structures, and techniques have not been shown in detail in order not to obscure the understanding of this description.

(20) Turning now to the drawings, which are included by way of example and not limitation, embodiments of the present disclosure are directed towards a single pair of interacting synchronized rotors having an equivalent number of permanent magnets mounted on each respectively.

(21) Furthermore, in some embodiments of the self-propelling apparatus the magnets mounted on the rotor will utilize different magnetic orientation, size, shape and number. Other embodiments may make use of magnetic sensors instead of optical sensors for tracking rotor position.

(22) One possible configuration of a self-propelling apparatus with integral electro-magnetic coils 100 is shown in FIG. 1A. Top 101 and bottom 102 plates of the apparatus are shown in FIG. 1A along with optical source and sensor 103 and enclosure panel 104. FIG. 1B shows a second optical source and sensor 105 along with coil support plates 106 and mounting L-brackets 107. In some embodiments the plates can be made from sheet metal or carbon fiber honeycomb panels.

(23) FIG. 2 shows a pair of rotors with integrated spur gear profile for synchronization 200 and 201. For clarity, the rotor on the left 200 of FIG. 2 is referred to as rotor 1 (or first rotor) and the rotor on the right 201 is referred to as rotor 2 (or second rotor). FIG. 2 also shows integral electro-magnetic C-coils 202 and coil clips 203. Also seen in FIG. 2 are transversely mounted permanent magnets 204 and magnet mounting L-brackets 205. Each rotor is shown mounted to independent shafts 206, 208 with bearings 207, 209.

(24) Referring to FIG. 3A a matched pair of integrated rotors with spur gear profile are shown 200 and 201. Orientations of permanent magnets are denoted by North N and South S labels 306. Also seen in FIG. 3A are arc shaped optical slots 307 which are aligned with an optical source and sensors. A relationship between rotor rotation direction and thrust direction is denoted by clockwise arrow 300 for rotor 1 200, counterclockwise arrow 301 for rotor 2 201 and thrust arrow in −Y direction 302. To help understand the loads acting on the rotor's zones 303, 304 and 305 are shown in FIG. 3A. The zones are described as outboard zone 303 of rotor 200, inboard zone 304 of rotors 200 and 201 and outboard zone 305 of rotor 201.

(25) Referring to FIG. 3B, a relationship between a counterclockwise rotating 308 rotor 200 with a clockwise 309 rotating rotor 201 will generate a thrust in the +Y direction 310 is shown.

(26) For magnet orientations shown in FIG. 3, it is shown that there will be attraction between neighboring magnets on rotor 200 and 201 as neighboring magnets travel through inboard zone 304. FIGS. 4 and 5 show how forces are carried from the rotor to the bearing outer race, bearing balls and inner race. FIG. 4 shows a close up of rotor bearings 207 and 209 along with arrows denoting loading direction 400 and 401 experienced by outer races of each bearing assembly during loading. It is also shown in FIG. 4 that if rotor 200 is spinning in a clockwise direction, an outer race 408 and bearing balls 406 will also be spinning in clockwise direction denoted by arrows 402 and 404. It is also shown that the neighboring rotor 201 will be spinning in the counterclockwise direction 403 along with its outer race 409 and its bearing balls 407.

(27) Thrust Generation—Traction Mechanism

(28) As an example to illustrate how attracting forces as shown in the figures will generate thrust, twelve Neodymium Boron magnets grade N42 strength are provided with dimension one inch tall by one inch wide by 3/16 inches thick each mounted with orientations shown in FIG. 3A. FIG. 6 shows a plot of a net force in the +X direction experienced by rotor 200 due to rotor 201 during one rotation. As stated above, because of magnet orientation, a net force between the rotors is known and will always be attractive, and will be carried by the ball bearings traveling on outboard side of the bearing i.e. zones 303 and 305 of FIG. 3A. Letting the instantaneous load on rotor 200 be L200(t) the following is defined:
L200(t)=(G200(t).sub.1+G200(t).sub.2+ . . . +G200(t).sub.N); summation of all bearing ball loads
where referring to FIG. 5, G200(t).sub.i, 502 is a load carried by an ith outboard ball bearing. As further shown in FIG. 5, a normal load 506 carried by inner race 500 due to the ith ball bearing and its instantaneous value is expressed as N200(t).sub.i. For non-slipping conditions, a frictional force 504 results and is experienced by the ith ball bearing due to the inner race along with 508 the frictional force experienced by the inner race due to the ith ball bearing rotation as shown in FIG. 5. Using the above expression for normal load, the instantaneous frictional force can be determined as
F.sub.f200(t).sub.i=mu.sub.s*N200(t).sub.i; where mu.sub.s is the static coefficient of friction
For the case of rotor 200 and its associated ball bearings rotating in clockwise direction 406, FIG. 5 shows that a force experienced by its inner race 500 will be in the −Y direction 508. Further, FIG. 5 shows how forces acting in rotor 201 ball bearing will act during its associated counterclockwise rotation. A loading on rotor 201 due to the magnets on rotor 200 will be in the −X direction and vary in a similar fashion to FIG. 6 which is provided as follows:
L201(t)=−L200(t); where L201(t) is the net load carried by rotor 2
where
L201(t)=(G201(t).sub.1+G201(t).sub.2+ . . . +G201(t).sub.N); summation of all bearing ball loads
Referring to FIG. 5, G201(t).sub.i 503 is the load carried by the ith outboard ball bearing. N201(t).sub.i 507 in FIG. 5 is a normal load carried by the inner race 501 due to rotor 201's ith ball bearing. For non-slipping conditions this results in a frictional force 505 experienced by the ith ball bearing due to the inner race along with 509 the frictional force experienced by the inner race due to the ith ball bearing rotation as shown in FIG. 5. This can be written as:
F.sub.f201(t).sub.i=mu.sub.s*N201(t).sub.i; where mu.sub.s is the static coefficient of friction
Frictional forces experienced by inner races 500 and 501 are both in the −Y direction and will therefore add constructively together. This constructive action will continue through their associated shafts resulting in a net translational force acting from the shafts onto the top and bottom plates of the device. This net translational force experienced by the device assembly will also be transferred onto any attached free-floating body i.e. propulsion will occur. It should be noted that there is an associated frictional force component in the +/−X direction as the ball bearings rotate. However, due to symmetry of the rotor motion and loading direction these X direction forces will cancel out.

(29) FIG. 7 shows a graph relating the rotor angular speed in radians per second to the measured thrust in Newtons for a device with loading per FIG. 6. The relationship between thrust and angular speed is dependent on ball bearing and inner race material as this variable determines the static friction coefficient. The total number of ball bearings to also effects the thrust to angular speed relationship in other embodiments.

(30) Table 1 below summarizes a relationship between the rotor loading, spin direction and the direction of the net thrust created.

(31) TABLE-US-00001 TABLE 1 Traction Traction between between Rotor Rotor 1 Rotor Rotor 2 Rotor 1 Radial ball bearing Rotor 2 Radial ball bearing Direction Spin Loading and fixed Spin Loading and fixed of Thrust Case Direction Direction race/shaft Direction Direction race/shaft on Frame 1 CW +x −y CCW +x −y +y 2 CW −x +y CCW −x +y −y 3 CCW +x +y CW +x +y −y 4 CCW −x −y CW −x −y +y
Uni-Polar Motor Circuit Configuration and Operation

(32) FIG. 8 shows a uni-polar control circuit configuration 800 for a single phase of coils mounted around the perimeter of a single rotor. This circuit embodiment has four sections: an optical sensor circuit 801, a pair of comparator circuits 802, a set of AND gates 803 and an H bridge transistor circuit 804. As shown in FIG. 8, an optical sensor circuit 801 includes a resistor (R_led) that adjusts the current delivered to the light source (e.g., LED) along with a resistor (R_trans) that limits current through the optical transistor. Light emitted from the light source will either reflect off the rotor or travel through the optical slots cut 307 into each rotor. When the light is reflected the optical transistor will turn ON and pull the voltage at point A1 low. When the light is not reflected the voltage at point A1 will remain high. The low voltage signal A1 is buffered through an operational amplifier and sent from point A2 into the positive input terminal of comparator circuit 1 op amp and the negative input terminal of comparator circuit 2 op amp.

(33) Each comparator circuit includes two resistors (e.g., R1 and R2) and an Op Amp. In comparator circuit 1 resistors R1 and R2 are configured in a voltage divider arrangement such that the voltage at point B1 is lower than point A2 when light is not reflected and greater than A2 when light is reflected. In comparator circuit 2 resistors R3 and R4 are configured in a voltage divider arrangement such that the voltage at point B2 is higher than point A2 when light is not reflected and lower than A2 when light is reflected. The outputs from the comparator circuits C1 and C2 are fed into a set of AND gates and then into an H-bridge circuit. Each AND gate also provides for an ENA command that can be controlled with a pulse width signal that will allow control for the rotor speed. When the voltage at C1 is high and C2 is low Q1 and Q4 will allow current to flow through the NPN transistor in the upper left corner and lower right corner of the H-bridge circuit, i.e., current will flow from point E1 to E2. When voltage at C1 is low and C2 is high Q2 and Q3 will allow current to flow through the NPN transistor in the lower left corner and upper right corner of the H-bridge circuit, i.e., current will flow from point E2 to E1. The optical slots and sensors are arranged to coincide with the rotor magnets reaching the middle of each C-coil element of a single-phase set of coils. Each set of phase coils can be connected in series or parallel. A series connection is shown in FIG. 10.

(34) Thrust direction control is provided by sending a HI signal at G1 to the NPN transistor 902 that will allow current to flow through the coil of a double pole double throw relay 901 as shown in circuit schematic 900 as seen in FIG. 9. Table 2 shows how DPDT state setting could control both reaction wheel and thrust direction.

(35) TABLE-US-00002 TABLE 2 Rotor Direction Rotor Coil DPDT Switch Spin Thrust Reaction Description State Direction State State Rotor 1 ON CW −y CCW Rotor 1 OFF CCW +y CW Rotor 2 ON CCW −y CW Rotor 2 OFF CW +y CCW
Reaction Wheel Operation

(36) By using independent electronic controllers to drive rotor 1 and rotor 2 integral electromagnetic coils this device can also be operated as a reaction wheel. Referring to Table 2, it is shown how DPDT state setting could control both reaction wheel and thrust direction. These torques are characterized by rotor momentum of inertia, angular speed and maximum current flow.

(37) Self-De-Spinning Operation/Feature

(38) As shown in FIG. 4, the rotor experiences a load in the +x direction during operation. The load is carried transiently by ball bearings as the ball bearings travel around the shaft. This loading will compress the ball bearing. Energy of each ball bearing compression is known and can be expressed as
u=½*sigma*epsilon; where u is the energy density, sigma is the stress and epsilon is the strain
and
U=Integral of u*dV; U total energy is equal to u integrated over its volume.

(39) The energy U for each ball bearing will be lost during each revolution it makes. The rate of energy loss will depend on rotor speed, the number of ball bearings and their respective radii and the ball bearing's material type. Rotor/reaction wheel will de-spin at a much quicker rate than if it were unloaded. The power loss of the rotor(s) can be characterized in terms of an average torque (Tao.sub.avg) needed to overcome the strain energy. Power lost will be of the form
Power Loss=Tao.sub.avg*omega; omega rotor angular speed
An amount of time delta_t it will take for a pair of rotors spinning with speed omega1 to come to a stop after powered has been turned off may be estimated.
Tao.sub.avg*delta_t=I.sub.rotor*(omega1−0); where I.sub.rotor is the rotor moment of inertia or
delta_t=I.sub.rotor*omega1/Tao.sub.avg
For the loading case shown in FIG. 6 Tao.sub.avg=0.063 Nm.

(40) In this way the device may be able to de-spin itself.

(41) Enhanced Torque/No Saturation Feature

(42) Another unique feature of this system is the ability to short a set rotor coils to enhance an ability to exert a desired torque. One embodiment of this circuit 1100 is shown in FIG. 11 which illustrates how a double throw double pole relay 1101 along with a transistor 1102 may be put in line with each set of rotor coils that will allow the coils to be shorted to itself through resistor 1103. Referring to Table 3, circuit configuration and system action table is shown for one such embodiment. FIG. 13 shows a schematic 1300 of how device rotor 1 coils 1301 and rotor 2 coils 1302 could be wired to a first enhanced mode reaction wheel relay stages 1303 and 1304.

(43) TABLE-US-00003 TABLE 3 Rotor Action Action Direction on on DPDT Rotor Enhance Rotor Rotor Switch Spin Torque 2 1 Description State Direction Mode Coils Coils Rotor 1 ON CW Rotor 2 ON CW — Rotor 1 OFF CCW Rotor 2 ON CCW — Rotor 2 ON CCW Rotor 1 ON — CCW Rotor 2 OFF CW Rotor 1 ON — CW

(44) FIG. 12 show how an overall control block diagram might look for integrating control of this device into an overall spacecraft system. A central processing unit can send out signals to control relays along with a pulse width modulated enable signal thereby controlling both speed and direction of each rotor. The block diagram assumes that the spacecraft will be equipped with accelerometers, gyroscopes sensors and also be capable of determining the difference to the current state and the desired state and then make necessary adjustments to pulse width values and/or relay settings in order to achieve the desired orientation and/or propulsion effect.

(45) The foregoing description of preferred embodiments of the present disclosure has been presented for purposes of illustration and description. The described preferred embodiments are not intended to be exhaustive or to limit the scope of the disclosure to the precise form(s) disclosed. Obvious modifications or variations are possible in light of the above teachings. The embodiments are chosen and described in an effort to provide the best illustrations of the principles of the disclosure and its practical application, and to thereby enable one of ordinary skill in the art to utilize the concepts revealed in the disclosure in various embodiments and with various modifications as are suited to the particular use contemplated. All such modifications and variations are within the scope of the disclosure as determined by the appended claims when interpreted in accordance with the breadth to which they are fairly, legally, and equitably entitled.