Patent Publication Number: US-2023159188-A1

Title: System and method for producing electromagnetic thrust

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application claims the benefit of U.S. Provisional Pat. Application 63/282,282, filed Nov. 23, 2021, entitled “SYSTEM AND METHOD FOR PRODUCING ELECTROMAGNETIC THRUST”, the entire disclosure of which is hereby incorporated herein by reference. 
    
    
     FIELD OF THE INVENTION 
     The present invention relates to systems and methods for producing electromagnetic thrust. 
     BACKGROUND 
     Various different technologies are commonly employed to launch rockets into low earth orbit, lunar orbit and on interplanetary missions as well as, in the case of Voyager, interstellar travel. Most commonly, liquid hydrogen and liquid oxygen are combined and ignited to create a controlled explosion pushing mass away from a craft resulting in an equal and opposite force forcing the mass of the craft into space. The great amount of energy released in such an explosion results in the rapid, if relatively brief, acceleration of the craft through the earth’s atmosphere and into space. Additional thrusts may be applied to maneuver the craft, to perform subsequent burns of the engines and to slow the craft down when entering orbit around another body. 
     Because the fuel consumption required for a mission profile requiring achieving earth orbit is so great, there is not left over much fuel to hurl the craft towards a distant planet. Further, as the engines tend to remain dormant for months or even years before decelerating the craft, there exists the danger that the engines will not reignite. 
     Because the vacuum of space does not retard the motion of a craft traveling through space, it would be advantageous to provide even a small but steady thrust to a craft over an extended period of time. Even a small thrust operating over a long period of time may result in substantial velocity. Towards this end, there have been developed ion thrust engines. An ion thruster or ion drive is a form of electric propulsion used for spacecraft propulsion. It creates thrust by accelerating ions using electricity. While using up only small amounts of mass accelerated to great speeds, such thrusters necessarily use up matter and produce very small amounts of thrust. 
     There is therefore a need for a system of propulsion that does not require the jettisoning of mass and which provides a measurable amount of thrust for a prolonged period of time. 
    
    
     
       BRIEF DESCRIPTION OF THE FIGURES 
       In the figures, which are not necessarily drawn to scale, like numerals may describe substantially similar components throughout the several views. Like numerals having different letter suffixes may represent different instances of substantially similar components. The figures illustrate generally, by way of example, but not by way of limitation, certain embodiments discussed in the present document, where: 
         FIG.  1 A  is an illustration of the physics of current flowing through two wires according to an exemplary and non-limiting embodiment; 
         FIG.  1 B  is an illustration of the propagation of magnetic fields emanating from a wire according to an exemplary and non-limiting embodiment; 
         FIG.  1 C  is an illustration of the propagation of magnetic fields emanating from a wire according to an exemplary and non-limiting embodiment; 
         FIGS.  2 A- 2 B  are illustrations of the timing of electric current in two wires according to an exemplary and non-limiting embodiment; 
         FIGS.  3 A- 3 B  are illustrations of the propagation of magnetic fields generated by two wires according to an exemplary and non-limiting embodiment; and 
         FIG.  4    is an illustration of a spacecraft powered by an electromagnetic thrust propulsion system according to an exemplary and non-limiting embodiment. 
     
    
    
     DETAILED DESCRIPTION 
     With reference to  FIG.  1 A , there are illustrated two currents, l1 and l2, flowing through two parallel wires separated by a distance r. The value of the magnetic field, B, present at the second wire resulting from l1 in the first wire is given by the equation: 
     
       
         
           
             B 
             = 
             
               
                 
                   μ 
                   0 
                 
                 ​ 
                 
                   I 
                   1 
                 
               
               
                 2 
                 π 
                 ​ 
                 r 
               
             
             , 
           
         
       
     
      where 
     
       
         
           
             
               μ 
               0 
             
             = 
             4 
             Π 
             × 
             
               
                 10 
               
               
                 − 
                 7 
               
             
             
               
                 N 
                 m 
               
               
                 
                   A 
                   2 
                 
               
             
             . 
           
         
       
     
     The force experienced by the second wire directed towards the first wire resulting from l2 flowing through the magnetic field B is given by the following equation: 
     
       
         
           
             F 
             = 
             
               I 
               2 
             
             Δ 
             L 
             B 
             . 
           
         
       
     
     Combining equations (1) and (2), the force per unit length (1 meter) acting on the second wire is given by: 
     
       
         
           
             
               F 
               
                 Δ 
                 L 
               
             
             = 
             
               
                 
                   μ 
                   0 
                 
                 
                   I 
                   1 
                 
                 
                   I 
                   2 
                 
               
               
                 2 
                 Π 
                 r 
               
             
             . 
           
         
       
     
     Substituting for µ_0, gives the following: 
     
       
         
           
             
               F 
               
                 Δ 
                 L 
               
             
             = 
             
               
                 2 
                 × 
                 
                   
                     10 
                   
                   
                     − 
                     7 
                   
                 
                 
                   I 
                   1 
                 
                 
                   I 
                   2 
                 
               
               r 
             
             . 
           
         
       
     
     Performing the same calculations to arrive at the force exerted on the first wire produces a force equal to that of F2 with an opposite direction. As a result, when current is flowing through both wires in the same direction, the wires experience an attractive force. When current is flowing in the opposite direction, the wires experience a repulsive force. 
     With reference to  FIG.  1 B , there is illustrated an exemplary and non-limiting embodiment illustration of the propagation of a pulsed magnetic field. In accordance with convention, wires shown on end have a “-” designating current coming out of and perpendicular to the page, while an “x” designates current flowing into the page. There is illustrated a cross-section view of the magnetic field, B, propagating in accordance with a current, l, flowing through the wire in a pulsed fashion as illustrated in  FIG.  1 C . With reference to the magnetic field illustrated propagating to the right and left of the wire, green areas represent portions of a pulse created when current is flowing out of or into the page through the wire. 
     With reference to  FIG.  1 C , when current is I and flowing out of the page, a magnetic field, B, is formed propagating to the right of the wire with an upwards orientation perpendicular to the direction of propagation. No magnetic field is produced when there is no current flowing. When current is -l and flowing into the page, a magnetic field, B, is formed propagating to the right of the wire with a downwards orientation perpendicular to the direction of propagation. Magnetic field B propagates at the speed at light at a speed of approximately 3.0 X 108 m/s. If each pulse lasts for 1 nanosecond, or, 1.0 X 10-9 seconds, the width of each pulse is .3 meters. 
     With reference to  FIG.  2 A , there is illustrated an exemplary graph of current flow through first wire  100 . In the example illustrated, the width of each pulse of current is 1 nanosecond and first and second wires  100 ,  102  are separated by a distance of .3 meters. Similarly,  FIG.  2 B  illustrates an exemplary graph of current flow through second wire  102 . As each pulse is .3 meters in width, each pulse extends for a distance approximately equal to the separation distance of the two wires. When the pulse width and separation distance are approximately equal, each wire during each nanosecond period of time during which current is flowing experiences a force on the wire resulting from the magnetic field generated by the current in the other wire in the preceding period of time. Note that the magnetic field propagated from each wire does not generate any force on the wire that produced the magnetic field. Likewise, for example, the magnetic field B produced by first wire  100  has no effect when passing through second wire  102  if there is no current flowing through second wire  102 . 
     With reference to  FIGS.  3 A and  3 B , there is illustrated the propagation of magnetic fields from each wire towards the other wire at various snapshots in time. As illustrated, at each moment in time, the top rendering of the two shows the magnetic field propagated from the first wire towards the second wire while the lower rendering shows the magnetic field propagated from the second wire towards the first wire. While the two instances of propagation are shown separately, one for each wire in isolation, the magnetic fields propagated by both wires are superimposed and pass through one another like ripples on a pond producing no effect one to the other. At t = .25 ns, with reference to  FIGS.  2 A and  2 B , the current through the first wire into the page is l1 while there is no current flowing through the second wire. As a result, neither wire experiences any force. 
     At t = 1.25 ns, with reference to  FIGS.  2 A and  2 B , the current through the second wire into the page is l2 while there is no current flowing through the first wire. Meanwhile, one quarter of the magnetic field pulse generate by first wire  100  from t=0 ms to t=1 ns is passing through second wire  102 . When this magnetic field interacts with current l2 at second wire  102 , a force F2 is generated on second wire  102  pointing to the left side of the page. 
     At t = 2.0 + ns (the instant just after t=2.0 ns), with reference to  FIGS.  2 A and  2 B , there is no current flowing through the second wire while a current of -l1 is flowing through the first wire out of the page. Meanwhile, the leading edge of the magnetic field pulse generate by second wire  102  from t=1 ns to t=2 ns is passing through first wire  100 . When this magnetic field interacts with current -l1 at first wire  100 , a force F1 is generated on first wire  100  likewise pointing to the left side of the page. 
     At t = 2.0 + ns (the instant just after t=2.0 ns), with reference to  FIGS.  2 A and  2 B , there is no current flowing through the second wire while a current of -l1 is flowing through the first wire out of the page. Meanwhile, the leading edge of the magnetic field pulse generate by second wire  102  from t=1 ns to t=2 ns is passing through first wire  100 . When this magnetic field interacts with current -l1 at first wire  100 , a force F1 is generated on first wire  100  likewise pointing to the left side of the page. 
     At t = 2.25 ns, with reference to  FIGS.  2 A and  2 B , there is still no current flowing through the second wire while a current of -l1 continues flowing through the first wire out of the page. Meanwhile, one quarter of the magnetic field pulse generate by second wire  102  from t=1 ns to t=2 ns has passed through first wire  100 . As this magnetic field continues to interact with current -l1 at first wire  100 , a force F1 continues to be generated on first wire  100  likewise pointing to the left side of the page. 
     At t = 3.0+ ns, with reference to  FIGS.  2 A and  2 B , current -l2 has just started flowing out of the page through the second wire while no current is flowing through the first wire. Meanwhile, the leading edge of the magnetic field pulse generate by first wire  100  from t=2 ns to t=3 ns is beginning to pass through second wire  102 . As this magnetic field interacts with current -l2 at second wire  102 , a force F2 is generated on second wire  102  likewise pointing to the left side of the page. 
     At t = 3.25 ns, with reference to  FIGS.  2 A and  2 B , there is still no current flowing through the first wire while a current of -l2 continues flowing through the second wire out of the page. Meanwhile, one quarter of the magnetic field pulse generate by first wire  100  from t=2 ns to t=3 ns has passed through second wire  102 . As this magnetic field continues to interact with current -l2 at second wire  102 , a force F2 continues to be generated on second wire  102  likewise pointing to the left side of the page. 
     Note that when the direction of current in each wire reverses so too does the direction of the magnetic field propagating from each wire. For example, the magnetic field at time t=1.25 ns created by current flowing into the page by second wire  102  at a point between the first and second wires points up on the page as shown by the arrow. Conversely, the magnetic field at time t=3.25 ns created by current flowing out of the page by second wire  102  at a point between the first and second wires points down. 
     As illustrated and described, during each nanosecond period of time a force F is generated pointing in the same direction by one wire or the other. The force F alternates between the two wires each pulse period. Were both wires to be fixed with respect to one another, the result would be the production of a force providing thrust to any structure incorporating the wires. The equations above are derived assuming parallel wires of infinite length. In some embodiments, the two wires may gently curve in a circular manner that approximates, for a unit length of a meter, two straight parallel wires. 
     With reference to  FIG.  4   , there is illustrated an exemplary and non-limiting embodiment of a first wire  400  and a second wire  402  extending parallel to one another in a generally circular fashion and forming a part of craft  404 . In some embodiments, electrical currents may be produced in both parallel wires  400 ,  402  in a manner as discussed above to produce a force perpendicular to the circular plane of the wires. As illustrated, a small modular reactor (SMR)  406  may be used to power the device. SMRs are a type of nuclear fission reactor which are smaller than conventional reactors and can produce on the order of 60 MW of power. Relying on nuclear power, SMRs can operate steadily for prolonged periods of time. In some embodiments, the wires may be formed of superconductors exhibiting no resistance and increasing the current flow attainable through the wires. In some embodiments, the superconducting material may be formed, at least in part, of metallic hydrogen. 
     In the following example, there is computed the thrust potential of such a configuration wherein the craft  404  has a mass approximately equal to that of a locomotive engine, or approximately 1.9X105 kg. In this example, the wires form circles having a diameter of 30 meters and the wires are .3 meters apart. The current signal for each wire is as described above with a pulsed current of +/- 2X103 A. In addition to the singularly illustrated wire setup comprised of the first wire  400  and second wire  402 , the setup is replicated 10 times. 
     In accordance with equation (4), the force F per meter of wire generated by each wire of the system is: 
     
       
         
           
             
               
                 2 
                 × 
                 
                   
                     10 
                   
                   
                     − 
                     7 
                   
                 
                 
                   I 
                   1 
                 
                 
                   I 
                   2 
                 
               
               r 
             
             = 
             
               
                 2 
                 × 
                 
                   
                     10 
                   
                   
                     − 
                     7 
                   
                 
                 
                   
                     2 
                     × 
                     
                       
                         10 
                       
                       3 
                     
                   
                 
                 
                   
                     2 
                     × 
                     
                       
                         10 
                       
                       3 
                     
                   
                 
               
               
                 .3 
               
             
           
         
       
     
      which equates to: 2.67 N per meter of wire. The length of each wire is approximately 2⊓d where d is 30 meters, or, 188 meters. Multiplying the force per meter by 188 meters equals 502 N of force per wire. Multiplying this by 10 engines provides 5020 N of force on the craft. In accordance with a = F/m, the acceleration produced by this force on the craft is approximately 5.02 X 103/1.9 X 105 kg which equals 2.64 X 10-2 m/sec2. 
     The distance from earth to mars is approximately 5.46 X 1010 meters. Half of this distance is approximately 2.73 X 1010 meters. 
     The amount of time required to traverse a distance Δx is .5at2 + v0t. If starting from rest with v0 = 0, Δx = .5at2. As a result,  
     
       
         
           
             Δ 
             t 
             = 
             
               
                 
                   
                     2 
                     Δ 
                     x 
                   
                   a 
                 
               
             
             = 
             
               
                 
                   
                     2 
                     
                       
                         2.73 
                         × 
                         
                           
                             10 
                           
                           
                             10 
                           
                         
                       
                     
                   
                   
                     2.64 
                     × 
                     
                       
                         10 
                       
                       
                         − 
                         2 
                       
                     
                   
                 
               
             
             = 
             1.43 
             
               
                  X 10 
               
               6 
             
              seconds 
             . 
           
         
       
     
     Divide this duration by 8.64 X 104 sec/day and the result is 16 days. As a result, from a standstill, the craft could accelerate at a constant rate for 16 days, rotate 180 degrees and decelerate at the same rate for an additional 16 days before coming to rest in orbit around Mars. In addition to its use in interplanetary or interstellar travel, the method of electromagnetic propulsion described herein may be used, for example, to aid in satellites maintaining their orbits in the face of orbit degradation such as may be caused by friction with the atmosphere.