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Title:
ELECTRODYNAMIC SPACE THRUSTER METHOD AND APPARATUS
Document Type and Number:
WIPO Patent Application WO/2012/001459
Kind Code:
A1
Abstract:
A method and apparatus for producing a linear thrust force, comprising an array of phase-shifted electric oscillations having frequency greater than or equal to ratio of the speed of electromagnetic waves in free space to length of the array (f ≥ c/L). Operated at adequate frequencies and powers, such device can produce highly efficient levels of thrust force for propelling spacecrafts and satellites with low consumption of energy. Further comprises a custom amplifier for producing and radiating powerful electric oscillations by accelerating, decelerating, and retaking electrons, producing several megawatts of thrust power.

Inventors:
L. FERREIRA, Moacir, Jr. (R: Edvald Ribas Borba, tv119 casa10 cjtoPrataIV Sítio Cercado, -650 Curitiba-PR, 81910, BR)
Application Number:
IB2010/052975
Publication Date:
January 05, 2012
Filing Date:
June 30, 2010
Export Citation:
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Assignee:
L. FERREIRA, Moacir, Jr. (R: Edvald Ribas Borba, tv119 casa10 cjtoPrataIV Sítio Cercado, -650 Curitiba-PR, 81910, BR)
International Classes:
B64G1/40
Download PDF:
Claims:
The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:

1. A method of generating thrust force, comprising the steps of:

(a) providing an array of at least three spaced-apart means for radiating phased electric oscillations,

(b) establishing the frequency of said phased electric oscillations to be greater than or equal to ratio of the speed of electromagnetic waves in free space to length of the said array (f > c/L),

wherein each of said means for radiating phased electric oscillations are preferably disposed in-line with its respective frequency phase shifted from each other,

whereby a linear thrust force will be created.

2. The method of claim 1, wherein step (a) said means for radiating phased electric oscillations, further including the step of:

producing said radiating phased electric oscillations, comprising the steps of:

(a) providing a means for emitting electrons,

(b) providing a first electric field for accelerating said electrons,

(c) providing a second electric field for decelerating said electrons,

(d) providing a means for retaking said electrons,

wherein said first electric field should preferably be generated by an electric voltage higher than 256kV, wherein said means for retaking said electrons should preferably be composed by a plurality of electron bean collectors,

whereby accelerating and decelerating said electrons will create said electric oscillations.

3. The method of claim 1, wherein step (a) said means for radiating phased electric oscillations is a dipole antenna.

4. The method of claim 1, wherein step (a) said means for radiating phased electric oscillations is a loop antenna.

5. The method of claim 1, wherein step (a) said means for radiating phased electric oscillations is a conventional antenna selected from a group consisting of helical antenna, rhombic antenna, beverage antenna and microwave antenna.

6. An apparatus for generating thrust force comprising:

an arrangement of three or more side-by-side, preferably inline and evenly-spaced, means for emitting electromagnetic waves,

wherein said means for emitting electromagnetic waves are phase-shifted from each other having a frequency preferably greater than or equal to ratio of the speed of electromagnetic waves in free space to length of said arrangement (f > c/L),

whereby said arrangement of phased waves will produce an effective thrust force.

7. The apparatus of claim 6, wherein said means for emitting electromagnetic waves further comprises: an electron source device for emanating electrons,

a positive electric voltage applied for speeding up said electrons,

a negative electric voltage applied for braking said electrons,

a plurality of electron beam collectors for recovering said electrons,

wherein said positive voltage should preferably be higher than 256kV,

whereby speeding up and braking said electrons will produce said electromagnetic waves.

8. The apparatus of claim 6, wherein said means for emitting electromagnetic waves is a dipole antenna.

9. The apparatus of claim 6, wherein said means for emitting electromagnetic waves is a loop antenna.

10. The apparatus of claim 6, wherein said means for emitting electromagnetic waves is a typical antenna selected from a group consisting of helical antenna, rhombic antenna, beverage antenna and microwave antenna.

Description:
ELECTRODYNAMIC SPACE THRUSTER METHOD AND APPARATUS

Technical Field

This invention relates to a method and apparatus which use phase-shifted electric oscillations for generating a linear thrust force in free space.

Background Art

Propulsion in space occurs generally by expelling reaction mass, in accordance with Newton's third law of motion, commonly paraphrased as: "For every action force there is an equal, but opposite, reaction force" or in other words "action and reaction are always equal and opposite".

Hence, expelling the reaction mass, the system power increases with the square of exhaust velocity, which indicate that most of the energy goes away with the exhausting mass, which can be attested using well-known formulas: nriiVi + m 2 v 2 = 0 with ½miVi 2 + ½m 2 v 2 2 = E, and also by Tsiolkovsky rocket equation:

Apparently, it is virtually impossible to violate Newton's third law for reducing the energy going away with the propellants, although there are some researches being carried out by universities and space agencies around the world. There are hypothetical space drives such as the bias drive, diametric drive, negative mass propulsion, photon rocket, disjunction drive, quantum vacuum energy, and reactionless drive. Also, there are practical devices in development such as Mach Effect Propulsion, GRASP - Gravity Research for Advanced Space Propulsion, Asymmetrical Capacitors, Lifters (Biefeld-Brown effect), Emdrive, and others already patented (US patent: 3130945, 2949550, 6492784, 6317310, 6098924, 6193194, 5546743, and 6745980).

Most of the concepts such as Inertial Propulsion Engine, also known as the reactionless drive or inertia drive, which uses motion of internal masses to create a net thrust, are considered incorrect due to infringement of classical physics laws, and by not demonstrating results. Other concepts have exhibited only few milli Newtons of thrust force presenting almost no practical application.

Theory

Propagation of electromagnetic waves in the outer space has a lot of theories without a definitive or conclusive explanation. This disclosure use one more practical that is based on waveguide interspace, a wave needs a means to propagate, in a waveguide, such means is the resulting electric field inside the waveguide interspace, which is in a particular electrostatic equilibrium, thus oscillations on electron orbit in the waveguide walls, transfer energy propagating the wave by perturbing such means, this can be applicable to optical fiber, metallic and dielectric waveguides. As it is widely supposed, electromagnetic wave propagates in the outer space in TEM mode (Transverse ElectroMagnetic), while inside waveguide, propagates in either TE mode (Transverse Electric), TM mode (Transverse Magnetic), or in hybrid modes. Accepting the waveguide is in a particular electrostatic equilibrium, electromagnetic waves change this equilibrium, hence, theoretically, space can be thought as it is in electrostatic equilibrium and electromagnetic waves propagates in it by disturbing it, and if a physical body can travel inside a waveguide in this way, thereby it could hypothetically do this in the outer space supported by all matter in the nearby sideling universe, asteroids, planets, gases, cosmic dust, stars, galaxies, and other celestial bodies, independently of the interspace distance. Finally, it will be possible the physical body to travel in the outer space without infringement of the laws of classical physics, traveling in the outer space, as it were, an interspace.

Electromagnetic (EM) interactions, well-known premises:

- EM fields interact with the matter:

- Electric component (E) interacts with electric charges, fixed and moving,

- Magnetic component (H) interacts only with moving electric charges.

- EM wave is associated with accelerating/decelerating charges:

- When an electric charge accelerates or decelerates, EM wave is produced,

- When EM wave acts on an electric charge, it accelerates or decelerates.

Classic electromagnetic theory does not impose any distance limits. All electromagnetic waves can cross a vacuum. All electromagnetic waves travel through space at the nearly same speed, c = 2299792458 m/s.

Transverse waves having a high frequency may exhibit wave-particle duality, exhibiting properties of both waves and particles, as particles they have no mass, but may have insignificant momentum proportional to their frequency. Here, hypothetically, as a particular premise, spectrums below THz can be considered only as waves. Also, as it is well-known, magnetic fields are generated by variation on electric fields and vice-versa; hence, for simplification, sometimes electromagnetic waves can simply be referred as electric waves, to analyze it only from the electric field point of view to facilitate a preliminary comprehension of transverse waves.

It is known that electrons attract both positive and neutral particles. In a simplified theory, an electron traveling inside a waveguide can change continuously the electrostatic equilibrium, causing a kind of electrodynamic drag, slowing down the electron velocity, and also, hypothetically, causing a sort of traveling electrodynamic wave at sideways, and when the electron collides, theoretically, its perceptible mass increase could as well be assigned to the traveling electrodynamic wave dragging the electron. Hypothetically, electrodynamic wave needs a nearby universe, waveguide walls, for propagating, then the perceptible electromagnetic wave can be the "effect" and the electrodynamic wave propagating sidelong could be the "cause". If EM fields interact with the matter, hence, hypothetically, sideway electrodynamic drag and sideway electrodynamic wave could be in control of the inertia of neutral bodies, with instantaneous transverse interactions, still neither proven nor unproven.

Minimum energy and voltage for an accelerated electron to attain to speed of light, within ideal conditions: charge= -1.60218x10 19 C, mass=0.00091xl0 ~27 kg, c=299792458 m/s, 1 eV = 1.60218x10 19 J

E= 1 / 2 mv 2 ^E 0.00091xl0 "27 x(299792458) 2 ^Ej=40.89336xl0 15 J

E eV =40.89336xl0 15 /1.60218xl0 19 =255.23574xl0 3 eV ~ 256 keV

acceleration voltage:

E = qxU -> 40.89336x10 15 =1.60218xl0 19 xU U=255.23574xl0 3 ~ 256 kV

Note: using only classical formulas, these values are ideal, not taking into account electrodynamic drag, apparent mass increase effect, and losses due to electromagnetic radiation.

Considering a hypothetical impulse drive, working by accelerating and decelerating electrons, electromagnetic waves are produced similarly to a dipole antenna. Cyclically and continuously accelerating an electron beam current (I) to more than 256keV, decelerating, and retaking them, a linear and continuous thrust force could be generated; the voltage of acceleration (Vi) should be much higher than 256kV to try to produce more thrust than electromagnetic radiation. Having the voltage of retaking (V 2 ), the electric power would be but no warranty of a net thrust force will be effectively generated in this way.

However, having an array of three or more impulse drives, acting as dipole antennas, spaced-apart along a length (L), each impulse drive fed with phase-shifted pulses, having the frequency (f) of said pulses greater than or equal to ratio of the speed of electromagnetic waves (c) in free space to length of the array (f > c/L), with the array acting as a linear motor, there will be a higher probability of an effective net thrust be produced. The net thrust force is expected to be produced because the speed of electrodynamic waves is limited staying below of the speed of the sequenced pattern produced by the phase-shifted oscillations. In either transverse electric mode or transverse magnetic mode, the phase-shifted oscillations sequentially produces a transverse force, generating a sequenced pattern, which can produce a longitudinal force in the nearby universe, thereby creating a strong electrodynamic drag for sustaining the motion, providing an enormous chance of creating a net thrust force in the outer space.

These brief theories and premises are provided here only for simplification of understanding regarding this disclosure and do not encompass all possible nuances regarding the electrodynamic behavior. Many theories and variations exist for explaining transverse wave propagation in the outer space, and a full discussion of this is subject well beyond the scope of this disclosure. Theory with a more practical sense, such as the waveguide-space theory, is the preferred in order to propose a workable device.

Summary of the Invention

The present invention was made in view of the prior art drawbacks described above, and the object of the present invention is to provide a workable method and apparatus to create thrust force in free space without transgressing the classical physics laws.

To solve the problem, the present invention provides an apparatus and method for creating net thrust force using an array of spaced-apart phase-shifted electric oscillations in order to produce an interpolation to modulate a sequenced virtual electric wave pattern a little faster than a normal electrodynamic wave in free space, which is mathematically true by following equation: (f > c/L), where f is frequency, c is the speed of electromagnetic wave in vacuum, and L is the array length. Considering the arrangement floating inside a waveguide interspace, it will produce an action similar to which is produced by a linear motor, acting as an "electrodynamic caterpillar", running much faster than an electrodynamic wave inside the waveguide, which produces a reaction force due to electrodynamic drag, hence, a linear net thrust force will be generated by mutual forces of action and reaction. For a low thrust, an array of conventional antenna can be used; to produce a higher thrust power, this disclosure also presents a "transverse impulse drive" using electron beam collectors, similar to a TWT/Klystron, for producing powerful electric oscillations by cyclically accelerating, decelerating and recovering electrons.

Objects and Advantages

Accordingly, it is an object of this invention to provide a method and apparatus for creating a linear thrust force from a sequenced pattern of phase-shifted electric oscillations.

It is a further object of this invention to provide a method and apparatus for producing and radiating powerful electric oscillations by speeding up, braking and recapturing electrons, constituting an impulse drive.

It is still another object of this invention to provide an alternative method or apparatus for radiating electromagnetic oscillations by using conventional dipole antennas.

It is another object of this invention to provide an alternative method or apparatus for radiating electromagnetic oscillations by using conventional loop antennas.

These and other objects and features of the invention will become apparent from the following description in connection with the appended drawings illustrating preferred embodiment of the invention. It is to be understood, however, that these are given by way of illustration and not of limitation and that changes may be made in the detailed construction, materials, form and size of the parts, without affecting the scope of the invention.

Drawings Figures

FIG. 1 is an illustration of an embodiment for producing and radiating electric oscillations comprised of an electron source, a power supply, and a set of electron beam collectors;

FIG. 2 is a cross-section taken of the embodiment of FIG. 1 to clarity the electron emission, acceleration, deceleration and recovering;

FIG. 3 is an illustration of a preferred embodiment for producing phased electric oscillations comprised of an array of the embodiment of FIG. 1;

FIG. 4 is an illustration of an alternative embodiment for radiating phased electric oscillations comprised of an array of dipole antenna;

FIG. 5 is an illustration of another alternative embodiment for radiating phased electric oscillations comprised of an array of folded dipole antenna;

FIG. 6 is still an illustration of another alternative embodiment for radiating phased electric oscillations comprised of an array of loop antenna;

FIG. 7 is an illustration of a fusion-powered spacecraft using the preferred embodiment of FIG. 3 as a means of propulsion;

FIG. 8 is a diagram block comprising an oscillator, an amplifier, and six phase shifters.

Reference Numerals in Drawings

9 magnet 35 support thruster 03 59 negative wire 87 insulator 03

10 core insulator 36 electrical transformer 70 support loop 88 collector 04

12 injector belt 38 fuel reservoir 71 first folded 89 insulator 04

20 armature 39 base 72 last folded 90 collector 05

21 coolant pipe 40 wire controller 73 first loop 91 insulator 05

23 left 02 41 first dipole 74 last loop 92 collector 06

25 support thruster 02 42 battery bank 75 high voltage power supply 93 insulator 06

26 right 02 43 steam turbine 76 reactor output collector 94 collector 07

27 left 03 44 last dipole 77 reactor output insulator 95 support thruster 01

28 right 03 46 acceleration power supply 78 reactor output byproducts 96 casing

29 left 04 51 condenser 79 electron source 97 support top/left 01

30 right 04 54 right 01 82 collector 01 98 support bottom

31 left 05 55 spacecraft hull 83 insulator 01 99 support impulse drive

32 right 05 56 support dipole 84 collector 02

33 left 06 57 support folded 85 insulator 02

34 right 06 58 support reactor 86 collector 03 Description of Invention

In the following will be described at least two different practical workable embodiments of this invention. Preferred Embodiment

An embodiment for producing and radiating electric oscillations, constituting an impulse drive, is shown in FIG. 1, comprised by an electron source 79, preferably having a control grid, a wire 40 for controlling electron beam current, an insulating casing 96, a high voltage power supply 75, a set of electron beam collectors 82, 84, 86, 88, 90, 92 and 94, and their respective insulators 83, 85, 87, 89, 91 and 93. The power supply 75 having a plurality of positive terminals, each terminal connected to each electron beam collector. The power supply negative terminal is connected via wire 59 to the electron source. A main support 99, a top support 97, and bottom support 98, is to sustain the assembly.

A cross-section taken of FIG. 1, is shown in FIG. 2, to clarify the assembly of the electron source 79, and the set of electron beam collectors 82, 84, 86, 88, 90, 92 and 94, and their respective insulators 83, 85, 87, 89, 91 and 93, coaxially disposed along the longitudinal axis of the assembly.

Electron beam collectors and multistage depressed collectors are well-known technologies (US patent: 3925701, 3993925, 6909235 and 3662212) used in the traveling-wave tube (TWT) which is an electronic device used to amplify radio frequency signals to high power. The purpose of the collectors is for recapturing the spent electron beam recovering most of the energy remaining in the beam.

Higher powered TWT usually contain beryllium oxide ceramic as an electron collector because of its special electrical, mechanical, and thermal properties. There are many variations, configurations, dimensioning, materials, thermal overload compensation, regarding electron beam collector technology. Hence, given a required electric power, the beam collector technology can be freely dimensioned and adjusted to being used within the (FIG. 1 and FIG. 2) embodiment. Optionally, the insulating casing 96 can be comprised of a toroid-shaped cavity resonator, similar to Klystron, a microwave technology, to maximize the power radiating efficiency, and the electron source 79 can optionally be comprised of Lanthanum

hexaboride, Cerium hexaboride, or Field Emitter Array Cathode (FEAC), instead of a conventional using tungsten wire.

A preferred embodiment for creating a linear thrust force is shown in FIG. 3, comprised by an array of twelve impulse drives (FIG. 1), six at left 97, 23, 27, 29, 31, 33, and six at right 54, 26, 28, 30, 32, 34, preferably disposed inline, symmetrically and equally spaced-apart, laying on support 95.

A fusion-powered spacecraft (weight: 500000kg, height: 30m, diameter: 15m) using the preferred embodiment of FIG. 3 as thruster is shown in FIG. 7, wherein three thruster represented by supports 95, 25 and 35, are equally spaced at an angle of 120° to sustain the base 39 which sustain a hull 55, preferably made of an aluminum alloy of at least 10 cm of thickness to protect against outer space radiation. The energy source can be supplied by a nuclear fusion reactor, already disclosed as "MAGNETIC AND ELECTROSTATIC NUCLEAR FUSION REACTOR" (PCT/IB2008/054254), comprised by six superconducting magnets 9 sustaining each other at arc-shaped injector belt 12, six core insulator 10 isolating the magnets to armature 20, three supports 58 equally spaced at an angle of 120° for withstanding the assembly, a battery bank 42, steam turbine 43, condenser 51, coolant pipe 21, acceleration power supply 46, and electrical transformer 36, further illustrating an array of ion bean collectors 76 and their respective insulators 77, a cover 78 for outputting fusion byproducts. The array of ions collectors are positioned at the six outputs for decelerating, recombining, and, with a multistage electric configuration, converting the kinetic energy from fusion charged byproducts into electric energy to power the thrusters. Unburned byproducts can be recycled for refueling the fusion reactor.

Phased array antennas are well-known technologies (US patent: 3680109, 5623270 and 6611230), this disclosure diverge a little from phased array technology regarding purpose and dipoles arrangement. This disclosure disposes dipoles, as transverse impulse drives, for creating thrust, while the phased array technology the dipoles are disposed in accordance with transmission of radio waves.

A diagram block for generating phased electric oscillations is shown in FIG. 8, comprised by, from left to right, an oscillator, an amplifier, and an array of six time-delay phase shifter. From top to bottom, each time- delay phase shifter translate phase angle respectively into 0°, 60°, 120°, 180°, 240°, and 300°. This diagram block is a basic schematic, there are other well-known technologies regarding multi-phase oscillator and phased array antennas that can be applied instead. Also, the amplifier can be a TWT, Klystron, or a

Magnetron for producing multi-megawatt of power. Alternative Embodiment

A basic or alternative embodiment, in transverse electric mode, is shown in FIG. 4, illustrating a sequence, first dipole 41 and last dipole antenna 44, forming an array of twelve dipole antenna, preferably inline and equally spaced-apart, laying on support 56. Another variation of the alternative embodiment is shown in FIG. 5, comprised by an array of twelve folded dipole antenna, first antenna 71, last antenna 72, laying on support 57.

Still another variation of the alternative embodiment, in transverse magnetic mode, is shown in FIG. 6, comprised by an array of six loop antenna, first antenna 73, last antenna 74, laying on support 70. The array of loop antenna is similar to a linear motor with single-coils, and as is widely known, the linear motor is similar to a three-phase rotary electric AC motor having its electromagnets (each electromagnet is a pair of magnetic poles) unwrapped and laid out side by side, to produce a linear thrust force.

Operation of Invention

A basic operation can be better understood from the FIG. 4 wherein each a pair of poles (dipole antenna) are fed with phase angles 120° apart, respectively each dipole antenna having angles of 0°, 120°, 240°, 0°, 120°, 240°, 0°, 120°, 240°, 0°, 120°, 240°, that is a three-phase system with four pairs of poles per phase. Putting it inside a dielectric or metallic waveguide without touching the walls, it is expected to act similarly to a linear motor. However, to proportionate a detectable thrust force inside the waveguide interspace, the frequency should be greater than or equal to ratio of the speed of electromagnetic waves in free space to length of the array times the number of pairs of poles per phase (f > (c/L) x p), where f is frequency, c is the speed of electric wave in vacuum, L is the array length, and p is the number of pairs of poles per phase (a pair of poles is a dipole).

For example, an array length of 5m: f > (c/L) x p -> f > (299792458/5) x 4 -> f > 240 MHz

Another example still using FIG. 4, is with each dipole antenna having phase angles 30° apart, respectively

0°, 30°, 60°, 90°, 120°, 150°, 180°, 210°, 240°, 270°, 300°, 330°, that is a twelve-phase system with one pair of poles per phase: f > (c/L) x p ^ f > (299792458/5) x 1 ^ f > 60 MHz

In the outer space, the net thrust force will be produced as a consequence of the speed of

electrodynamic waves is limited staying below of the speed of the sequenced pattern produced by the phased electric oscillations. The phased electric oscillations sequentially produce a transverse force, generating the sequenced pattern, consequently, producing a longitudinal force, creating a strong electrodynamic drag for sustaining the motion, producing the net thrust force in the outer space, independently of the interspace distance.

With more number of phases, energy flux (electric power) will be more constant, smoothly and continuously creating the thrust force, and with less number of pairs of poles per phase it requires less frequency. Hence, number of poles can be one, number of phases must be at least three, also the number of dipole antennas must be at least three, and with one pair of poles per phase the equation can be simplified to (f>(c/L)), constituting a preferred equation.

The array of folded dipole antenna illustrated in FIG. 5, works similarly as already explained in FIG. 4, both in transverse electric mode, differing regarding their impedances, as well it works for other types such as loop antenna, helical antenna, rhombic antenna, beverage antenna and microwave antenna. The array of loop antenna illustrated in FIG. 6 is an example in transverse magnetic mode; it is the closest correlation with a conventional linear AC motor.

When the electrons in a conductor, (antenna wire) are made to oscillate back and forth, electromagnetic waves are produced, these waves radiate outwards from the source at the speed of about 300 million meters per second.

For producing multi-megawatt electric oscillations, there are technologies such as Magnetron, Klystron and Traveling Wave Tube (TWT). Powerful electric oscillations can be created by accelerating, decelerating, and retaking electrons.

The proposed variation of a TWT as the preferred transverse impulse drive (FIG. 1 and FIG. 2), has the electron source 79 for emitting electrons that are accelerated toward the positive potential applied at collector 82, and successively being decelerated by the collectors 84, 86, 88, 90, 92 and 94, until the electrons land softly on collectors going to power supply 75, and again going via wire 59 to the electron source, creating powerful electric oscillations. The wire 40(FIG. 1) is for applying a signal of phase-shifted oscillations to control the electron source 97. This transverse impulse drive can be considered as a pair of poles, although asymmetric in comparison to a dipole antenna.

The operation of the preferred embodiment can be better understood from the FIG. 3 wherein each transverse impulse drive 97, 23, 27, 29, 31, and 33, at left side, can be considered as an array of pairs of asymmetrical poles, having phase angles 60° apart, respectively each one having angles of 0°, 60°, 120°, 180°, 240°, and 300°, that is a six-phase system with one pair of asymmetrical poles per phase. The transverse impulse drive at right side 54, 26, 28, 30, 32, and 34, are similar to the left side, they are for compensating possible transverse displacement of the assembly due to its dipole asymmetry, for example, each one can be either in-phase 0°, contra-phase 180°, or out of phase 90°, regarding its peer at left side, to compensate rotation, sideway shifting, and vibration.

Having a length of 10m, using the simplified equation: f > (c/L) -> f > (299792458/10) -> f > 30 M Hz

A frequency at least 30 M Hz will be enough for generating a linear net force.

Expecting maximum thrust performance, with 100% of efficiency, the minimum power consumption per kilogram with an acceleration of 10 m/s 2 (~1 g-force), not taking into account losses due to electromagnetic radiation:

a=Av/At

E=½mv 2 E=½xlx(10) 2 E = 50 J ^ E/t = 50J/s P = 50W

It will be 50W/kg (50kW/tonne) to reach an acceleration of 10 m/s 2 (~1 g-force).

Comparatively, propulsion method with higher exhaust velocities (specific impulse) is more propellant- efficient; however, power consumption increases with the square of the exhaust velocity; hence, using direct aneutronic fusion propulsion, having its exhausting byproducts (11.49254xl0 6 m/s) as the reaction mass from hydrogen-boron-11 (66 TJ/kg) fusion reaction :

1) hV! + m 2 v 2 = 0 ^ 1x10 + m 2 xll. = 0 m 2 = 8.7013xl0 "7 kg

or by Tsiolkovsky rocket equation: ->

10 = 11.49254xl0 6 xln(l/(l-m 2 )) m 2 = 8.7013xl0 "7 kg

2) /iiThV! 2 + ½m 2 v 2 2 = E ^ ½lxl0 2 + ½8.7013xl0 ~7 x(11.49254xl0 6 ) 2 = E ^ E = 57.46277x10 s J

The power consumption will be 57.46MWatts per kilogram to achieve an acceleration of 10 m/s 2 (~1 g-force).

Using the electrodynamic thruster, the minimum electric power, not considering electromagnetic losses, for thrusting a spacecraft of 500000kg (500 tonnes) is: 500000kg x 50W/kg = 25MWatts

Comparatively, using expelling mass: 500xl0 3 x 57.46x10 s = 28.73 Tera Watts; the power consumption ratio is 57.46xl0 6 /50 = 1149200

In this way, the electrodynamic thruster will consume a million times less power to thrust a spacecraft, assuming it with 100% of efficiency without electromagnetic losses. However, in practice, many losses will occur, but even with losses, it is expected to be more efficient than conventional propulsion by expelling reaction mass, that which was to be demonstrated.

Conclusion, Ramifications, and Scope of Invention

Accordingly, the reader will see that the electrodynamic thruster of this invention evolves an improved propulsion concept, that can be used to thrust, for example, solar-powered satellites and fusion-powered spacecrafts, at very high performance levels, exceeding conventional means by factors of a million; and also it is relatively inexpensive; system performance is competitive; having a scalability of size and power, easier engineering and maintainability.

While my above description contains a lot of specificities, these should not be construed as limitations on the scope of the invention, but rather as an exemplification of one preferred embodiment thereof. Many other variations are possible. For example, it can be comprised by three or more transducers, varying form and size of the parts. It will be appreciated by those of ordinary skill in the art that various changes can be made in the parts and steps of the apparatus and method without departing from the spirit and scope of the invention.

Accordingly, the scope of the invention should be determined not by the embodiments illustrated, but by the appended claims and their legal equivalents.