Source: https://patents.google.com/patent/US9875816B2/en
Timestamp: 2019-04-23 23:29:58+00:00

Document:
2017-12-07 Assigned to GENERAL FUSION INC. reassignment GENERAL FUSION INC. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: LABERGE, MICHEL GEORGES, RICHARDSON, DOUGLAS H.
Embodiments of systems and methods for compressing plasma are described in which plasma pressures above the breaking point of solid material can be achieved by injecting a plasma into a funnel of liquid metal in which the plasma is compressed and/or heated.
This application is a division of U.S. patent application Ser. No. 13/935,281, filed Jul. 3, 2013, entitled “SYSTEMS AND METHODS FOR COMPRESSING PLASMA,” now U.S. Pat. No. 9,424,955, which is a continuation of U.S. patent application Ser. No. 12/699,725, filed Feb. 3, 2010, entitled “SYSTEMS AND METHODS FOR COMPRESSING PLASMA,” now U.S. Pat. No. 8,537,958, which claims the benefit under 35 U.S.C. §119(e) of U.S. Provisional Patent Application No. 61/149,886, filed Feb. 4, 2009, entitled “SYSTEMS AND METHODS FOR ACCELERATING AND COMPRESSING A PLASMA;” each of the foregoing is hereby incorporated by reference herein in its entirety.
The present disclosure relates to embodiments of systems and methods for compressing plasma. In certain such embodiments, a plasma toroid is compressed using a liquid metal funnel.
Various systems for heating and compressing plasmas to high temperatures and densities have been described. One approach for accomplishing plasma heating and compression by spherical focusing of a large amplitude acoustic pressure wave in a liquid medium is described in U.S. Patent Publication No. 2006/0198486, published Sep. 7, 2006, entitled “Pressure Wave Generator and Controller for Generating a Pressure Wave in a Fusion Reactor”, which is hereby incorporated by reference herein in its entirety. In certain embodiments of this approach, a plurality of pistons is arranged around a substantially spherical vessel containing a liquid medium. A vortex or cavity is created in the liquid medium. The pistons are accelerated and strike the outer wall of the vessel generating an acoustic wave. The acoustic wave generated in the liquid medium converges and envelopes a plasma that is introduced into the vortex, thereby heating and compressing the plasma.
A pressure wave generator of the type described in U.S. Patent Publication No. 2006/0198486 can be employed in a Magnetized Target Fusion (MTF) reactor as described, for example, in U.S. Patent Publication No. 2006/0198483, published Sep. 7, 2006, entitled “Magnetized Plasma Fusion Reactor,” which is hereby incorporated by reference herein in its entirety. In certain such implementations, a magnetized plasma is introduced into a vortex that is created in the liquid medium, such as molten lead-lithium (PbLi). The acoustic wave produced by the impact of pistons surrounding the spherical reactor vessel can compress the magnetized plasma to high density and temperature.
In some embodiments of the above-described devices, compressed gas such as steam or air can be used to accelerate the pistons. Typically the desired piston impact velocity for plasma compression is of the order of 100 m/s, and so generally a compressed gas pressure of about 1,300 psi is used to accelerate the pistons. To achieve the symmetry of implosion that may be useful or desirable in some implementations, the timing of the piston firing, trajectory, and impact is precisely controlled for each piston. For example, for some plasma compression implementations, all the pistons preferably strike the vessel wall within about 1μs of each other. In some such implementations, a servo control system can be used to measure precisely the position of each piston and control its trajectory to attain the requisite impact time.
Whilst certain embodiments of such mechanical compression systems are attractive from, for example, a cost perspective, certain such implementations may need frequent maintenance, especially in applications where the repetition frequency of piston firing is high.
Embodiments of systems and methods for compressing plasma are disclosed. Some embodiments comprise electrically accelerating a plasma, for example, by using a plasma accelerator such as, e.g., a rail gun. The plasma can be accelerated into a funnel of liquid metal where the plasma is further compressed. The use of the liquid metal allows high plasma densities to be achieved, because, in some embodiments, the pressure attained can be higher than the breakpoint or yield strength of solid materials typically used in the apparatus itself.
In certain embodiments, a low density and temperature spheromak or toroidal plasma is formed using a plasma gun, for example, a magnetized coaxial gun. The toroidal plasma is electrically accelerated, compressed and heated to a high density and temperature using a plasma accelerator (e.g., a tapered rail gun) that extends towards a liquid metal funnel. The liquid metal funnel in some implementations can be formed of molten metal such as, for example, molten lead-lithium (PbLi). In various embodiments, the toroidal plasma can be formed as a field-reversed configuration (FRC) or other compact toroid.
In some implementations, the plasma can include a fusionable material such as, for example, isotopes of light elements (e.g., deuterium, tritium, helium-3, lithium-6, and/or lithium-7). The higher plasma densities and/or temperatures that are achievable in some such implementations can be sufficient for the initiation of fusion reactions. Some fusion reactions produce neutrons. Therefore, some embodiments of the system can be configured as neutron sources. Some embodiments of the systems and methods may provide sufficient fusion reactions for net energy production to occur (e.g., above breakeven).
An embodiment of an apparatus for compressing plasma is disclosed. The apparatus comprises a plasma gun configured to generate a compact toroid of plasma, a plasma accelerator, and a liquid funnel system. The plasma accelerator has a first end, a second end, and a longitudinal axis between the first end and the second end. The plasma accelerator is configured to receive the compact toroid at the first end and to accelerate the compact toroid along the longitudinal axis toward the second end. The liquid funnel system comprises a liquid funnel having a substantially cylindrical passage substantially aligned with the longitudinal axis of the plasma accelerator. The passage has a first inner diameter at a top end of the passage and a second inner diameter at a bottom end of the passage. The second inner diameter can be less than the first inner diameter in some embodiments. The liquid funnel system is configured to receive the compact toroid from the second end of the plasma accelerator and to compress the compact toroid as the compact toroid moves along the passage from the top end toward the bottom end. The system can be configured such that a pressure of the compact toroid when below the top end is greater than a pressure of the compact toroid when above the top end.
An embodiment of a liquid metal funnel system configured for compressing plasma is disclosed. The liquid metal funnel system comprises a liquid metal funnel having a substantially cylindrical passage having a first inner diameter at a first end of the passage and a second inner diameter at a second end of the passage. The second inner diameter can be less than the first inner diameter. The liquid metal funnel can be oriented such that the first end of the passage is higher than the second end of the passage. The liquid metal funnel can be configured to receive a plasma from a plasma injector and to compress the plasma as the plasma moves along the passage from the first end toward the second end.
An embodiment of a method of compressing a plasma is disclosed. The method comprises generating a toroidal plasma, accelerating the toroidal plasma along a longitudinal direction, and introducing the accelerated toroidal plasma into a passage in a liquid funnel. The passage can have a first size at a first end of the passage and a second size at a second end of the passage. The second size can be smaller than the first size. The method can also include compressing the toroidal plasma as the toroidal plasma moves from the first end of the passage toward the second end of the passage.
FIG. 1A is a schematic cross-sectional diagram showing an embodiment of a system compressing a plasma in a tapered liquid metal funnel. In this embodiment, a plasma gun forms a compact toroid that is accelerated by a plasma accelerator toward the liquid metal funnel.
FIG. 1B is a schematic cross-sectional diagram showing another embodiment of a system for compressing a plasma in a liquid metal funnel system. In this embodiment, the funnel system comprises a liquid metal funnel and an axial liquid metal guide disposed substantially along a central axis of the funnel. In this embodiment, the plasma accelerator comprises a plasma restrictor that comprises a constriction in a propagation channel of the accelerator.
FIG. 1C is a schematic cross-sectional diagram showing another embodiment of a system for compressing a plasma in a liquid metal funnel system. In this embodiment, the plasma accelerator comprises a plasma restrictor that comprises one or more magnetic coils.
FIG. 1D is a perspective cutaway view of an embodiment of a system for compressing a plasma. The embodiment shown in FIG. 1C is generally similar to the embodiment schematically shown in FIG. 1B.
FIG. 2 is a graph indicating an example calculation of the energy of the plasma to achieve the Lawson criteria for various plasma densities and an example calculation of the magnetic pressure of a plasma at various plasma densities. These example calculations are based on Bohm diffusion and certain other assumptions described below. Note that a pressure of 1 atmosphere (atm) is about 105 Pa.
FIG. 3 is a schematic cross-sectional diagram showing an example of a toroidal plasma within a tapered liquid metal funnel.
FIG. 4 is a graph showing an example calculation of the plasma energy to achieve the Lawson criteria for various plasma densities, taking into account various power losses that can occur in an example embodiment of a plasma compression system.
Tapered coaxial plasma spheromak accelerators have been built and studied in the past for, e.g., x-ray production, tokomak fuelling, and plasma physics research. However, the maximum achievable magnetic pressure has been limited by the strength of the solid materials used in the apparatus (e.g., a fracture limit, yield strength, or breakpoint of the solid materials). In certain embodiments of the present approach, the magnetic pressure that can be achieved has been increased significantly beyond this limit by using a tapered or funnel-shaped liquid metal tube as described in more detail below.
With reference to the drawings, FIGS. 1A-1D schematically illustrate several embodiments of a system 1000 that can be used to accelerate and compress a plasma. The embodiments shown in FIGS. 1A-1D comprise a plasma gun 100 configured to generate a toroidal plasma (for example, a compact toroid such as, e.g., a spheromak), a plasma accelerator 110 configured to accelerate the plasma along a longitudinal axis 115 of the accelerator 110, and a liquid metal funnel system 120 into which the plasma accelerated by the accelerator 110 is introduced for further compression. In various embodiments, the plasma gun 100 may comprise a magnetized plasma gun that has a gun axis that is substantially aligned or coaxial with the longitudinal axis 115 of the accelerator 110. In some embodiments, the plasma gun 100 comprises a Marshall-type plasma gun. In various embodiments, the plasma accelerator 110 may comprise a rail gun configured to accelerate the plasma using magnetic and/or electromagnetic forces. In some embodiments, the plasma accelerator 110 can provide some degree of plasma compression as the plasma is accelerated along the longitudinal axis 115. For example, the rail gun can comprise one or more tapered electrodes to compress the plasma during acceleration along the longitudinal axis 115. The liquid metal funnel system 120 may comprise a liquid metal funnel, cylinder, or tube 8 having a passage substantially aligned with the longitudinal axis 115 of the accelerator 110. In some embodiments, a cross-section and/or inner diameter of the passage can change from an upper end of the funnel to a lower end of the funnel, e.g., the cross-section (and/or inner diameter) can decrease to allow the plasma to be compressed as the plasma moves below the upper end and toward the lower end. In certain embodiments, the plasma gun 100 and/or the plasma accelerator 110 are positioned substantially above the liquid funnel system 120. In certain embodiments, the upper end of the funnel 8 is substantially above the lower end of the funnel 8.
The toroidal plasma generated by the plasma gun 100 can be a compact toroid such as, e.g., a spheromak, which is a toroidal plasma confined by its own magnetic field produced by current flowing in the conductive plasma. In other embodiments, the compact toroid can be a field-reversed configuration (FRC) of plasma, which may have substantially closed magnetic field lines with little or no central penetration of the field lines.
As schematically illustrated in the embodiments shown in FIGS. 1A-1D, gas from one or more tanks 4 is introduced into the gun by fast puff valves 3. In some implementations, the initial gas pressure is about 15 pounds per square inch (psi) (e.g., about 1.03×105 Pa). The gas may comprise a fusionable material. For example, the fusionable material may comprise one or more isotopes of light elements such as, e.g., isotopes of hydrogen (e.g., deuterium and/or tritium), isotopes of helium (e.g., helium-3), and/or isotopes of lithium (e.g., lithium-6 and/or lithium-7). Other fusionable materials can be used. Combinations of elements and isotopes can be used. For example, in some implementations, a 50% deuterium-50% tritium gas mixture is introduced from the tank 4 using about 100 puff valves 3. Each pulse from the valves introduces about 2 mg of gas, in one implementation. In other embodiments, a different number of valves can be used and/or a different mass of gas can be introduced. In other implementations, the percentages of deuterium and tritium, respectively, can be different from 50%-50%.
Coils 5 induce a magnetic field in the space between an outer electrode 7 and a formation electrode 14. The coils 5 can be configured to provide a mostly radial stuffing magnetic field of about 0.8 Tesla in some implementations. In the embodiment schematically illustrated in FIGS. 1A-1C, the formation electrode 14 is substantially cylindrical, and the outer electrode 7 is tapered inward toward the liquid metal funnel system 120. In the embodiments schematically illustrated in FIGS. 1B-1D, the magnetic field is produced by 3 magnetic coils 5 a, 5 b, and 5 c, although fewer or greater numbers of coils may be used in other embodiments. In some embodiments, the coil 5 a comprises about 140 turns of hollow square 6 mm×6 mm copper wire. During operation of the system, the wire can carry a current of about 1000 Amps at a voltage of about 630 V dissipating about 630 kW. Coil 5 b comprises about 224 turns of hollow square 6 mm×6 mm copper wire carrying a current of about 1000 Amps at a voltage of about 832 V dissipating about 830 kW. Coil 5 c comprises about 552 turns of hollow square 6 mm×6 mm copper wire carrying a current of about 1000 Amps at a voltage of about 844 V dissipating about 840 kW. In some embodiments, the coils 5 a, 5 b, and 5 c will run substantially continuously during operation of the system. In some embodiments, a cooling system (not shown) provides water (or another coolant), which flows in the hollow wires to cool them.
In certain implementations of the system, it is desirable to introduce gas only between the outer electrode 7 and the formation electrode 14. In certain such implementations, the valves 3 open and close sufficiently rapidly to introduce the gas so that it is substantially confined between the electrodes 7 and 14. For example, at room temperature (e.g., about 20 C), the thermal velocity of the gas is about 900 m/s. If, for example, the distance between the electrodes 7 and 14 is about one meter, the gas could be injected for a duration of less than about 1 ms to provide gas for the generation of each compact toroid. In some implementations, Parker Series 99 valves can be used (available from Parker Hannifin, Cleveland, Ohio).
In some embodiments, the formation electrode 14 is electrically connected to a capacitor bank 1. In some such embodiments, the capacitor bank 1 can comprise a capacitance of about 4.1 mF and the bank can be charged at a voltage of about 22 kV. In some cases, the capacitor bank 1 comprises about eighty 52 μF individual capacitors (e.g., General Atomics Energy Products (San Diego, Calif.), model 33677 capacitors). The individual capacitors can be connected in parallel. The capacitor bank 1 can be connected to the formation electrode 14 using a transmission line. In some embodiments, the total inductance of the transmission line and capacitors is about 20 nF, which advantageously provides a sufficiently fast electric discharge.
During operation of the system 1000, when the gas introduced by the puff valves 3 achieves a suitable pressure between the electrodes 7 and 14, the capacitor bank 1 discharges in the gas, turning the gas into a plasma. The discharge can occur when the capacitor bank voltage exceeds the breakdown voltage of the gas (which can depend on the gas pressure). In some implementations, the bank 1 discharges when the gas pressure is about 10 mTorr (e.g., about 1.3 Pa). The discharge can occur at other gas pressures in other embodiments. In the embodiment shown in FIG. 1A, a switch 2 is activated to discharge the capacitor bank 1 through the gas, generating a plasma. A possible advantage of embodiments using the switch 2 is that the switch can be activated so that the discharge occurs when the gas is at a desired pressure, which may allow increased flexibility during operation.
The current rises (e.g., to about 3 MAmp in about 20 μs in some cases), and the magnetic field from this current forces the plasma in the downward direction in FIGS. 1A-1C, toward the plasma accelerator 110. The stuffing magnetic flux from the coils 5 wraps itself around the plasma. The magnetic field reconnects to form closed magnetic surfaces, and the plasma forms a compact toroid. For example, the toroid may be a spheromak 16 having a relatively low density (e.g., about 1015 cm −3, in some cases) and temperature (e.g., about 20 eV, in some cases).
In some implementations of the system 1000, after a relatively small delay (e.g., about 30 μs, in some cases) to allow the magnetic fields to reconnect and/or to allow turbulence, if present, to settle, the spheromak 16 is accelerated and compressed by the plasma accelerator 110 toward the liquid metal funnel system 120.
For example, in the embodiments schematically illustrated in FIGS. 1A-1D, acceleration electrodes 6 are connected to a second capacitor bank 11, which is used to provide energy to the plasma. In some embodiments, the capacitor bank 11 has a capacitance of about 2.6 mF and is charged at a voltage of about 88 kV. In some such embodiments, the capacitor bank 11 comprises about 100 pairs of 52 μF, 44 kV individual capacitors with each pair electrically connected in series, and the 100 pairs electrically connected in parallel. In some embodiments, the capacitors comprise General Atomics Energy Products (San Diego, Calif.), model 32283 capacitors. In some implementations, the capacitor bank 11 is electrically connected to the acceleration electrode 6 using a substantially disk-shaped transmission line 15 substantially surrounding the coaxial gun 100 to reduce or minimize inductance. The current rise-time of some embodiments is about 40 μs because of the relatively large capacitance of the bank 11. In some embodiments, a substantially disk-shaped transmission line can be used to electrically connect the capacitor bank 1 to the formation electrode 14. In some embodiments, two substantially disk-shaped transmission lines are used: a first substantially disk-shaped transmission line electrically connecting the capacitor bank 1 to the formation electrode, and a second substantially disk-shaped transmission line electrically connecting the capacitor bank 11 to the acceleration electrode 6.
The plasma accelerator 110 comprises a plasma propagation channel 114 through or along which the toroidal plasma 16 is accelerated. For example, as schematically illustrated in FIGS. 1A-1D, the acceleration electrode 6 can be disposed within the outer electrode 7, and the plasma propagation channel 114 comprises space between the electrodes 6 and 7. The plasma propagation channel 114 can have a cross-section (perpendicular to the longitudinal axis 115) that changes (in shape, size, width, spacing, and/or any other way) from a first end 112 a to a second end 112 b of the accelerator. For example, in the embodiments illustrated in FIGS. 1A-1D, at least one of the electrodes 6 and 7 can be tapered from the first end 112 a of the accelerator 100 (e.g., near the plasma gun 100) to the second end 112 b of the accelerator 100 (e.g., near the funnel system 120). For example, in some embodiments, the radius of the accelerator 110 (e.g., a radius from the longitudinal axis 115 to the center of the channel 114) decreases by a factor of about 30 from the first end 112 a to the second end 112 b. In other embodiments, the radius of the accelerator 110 decreases from the first end to the second end by a factor of about 2, about 5, about 10, about 20, about 50, about 100, or some other factor. In various embodiments, the radius decrease of the accelerator from the first end to the second end can be in a range from about 10 to about 50, in a range from about 20 to about 40, or some other range.
With further reference to the embodiments schematically illustrated in FIGS. 1A-1D, the magnetic force of the plasma accelerator 110 accelerates the toroidal plasma 16 between the tapered coaxial electrodes 6 and 7 and heats and compresses the plasma to higher temperature and density, forming a compressed toroidal plasma 12.
The configuration of the electrodes 6, 7 can be selected to provide a desired amount of compression as the plasma moves from the first end 112 a to the second end 112 b of the accelerator 110. For example, one or more factors including the tapering, shape, and/or spacing of the electrodes 6, 7 can be selected to provide a desired compression. In the case of some toroidal configurations of plasma (e.g., compact toroids), the compression of the plasma in some implementations of the system 1000 can be measured in terms of a radial compression of the toroid (e.g., a ratio of the radius of the toroid when in a first position in the system to the radius of the toroid when in a second position in the system). For example, in some embodiments, the radial compression of the plasma as the plasma moves from the first end 112 a to the second end 112 b of the accelerator 110 is about 30:1. The radial compression of the plasma in the accelerator 110 can be different in other embodiments such as, for example, about 2:1, about 5:1, about 10:1, about 15:1, about 20:1, about 30:1, about 50:1, about 100:1, etc. In various embodiments, the compression of the plasma in the accelerator 110 can be in a range from about 10:1 to about 50:1, in a range from about 20:1 to about 40:1, or in some other appropriate range. In some embodiments, tapering of the electrodes 6, 7 is not used in the accelerator 110, and there is substantially no compression of the plasma in the accelerator 110.
In other embodiments, the plasma accelerator 110 may be configured so that the outer electrode 7 acts as the acceleration electrode. In other embodiments, both electrodes 6 and 7 can be used to electromagnetically accelerate the plasma from the first end to the second end. In other embodiments, additional electrodes can be used (e.g., to assist stabilizing the plasma and/or to inhibit tilting of the toroid in the channel 114).
The electrodes 6, 7, and/or 14 can be formed from electrically conductive metal. The electrodes 6, 7, and/or 14 can be formed in one or more sections. For example, in some embodiments, the electrodes 6, 7, and/or 14 comprise one or more stainless steel 304 plates or sheets having a thickness of about 5 mm. The sections of the electrodes can be joined together by welding, fasteners (e.g., bolts), etc. In other embodiments, the electrodes can be formed from additional and/or different materials and/or thicknesses of material. In some implementations, the plasma can become sufficiently hot to at least partially vaporize some of the electrodes. Vaporization of the electrode may in some cases contaminate the plasma with metallic impurities that can cool down the plasma. Therefore, in certain implementations that utilize electrodes that can (at least partially) vaporize, one or more of the electrodes 6, 7, and 14 can be coated with a high melting point material such as, e.g., tungsten. The coating material can be selected so that the melting point of the coating material (e.g., tungsten) is greater than the melting point of the electrode material (e.g., stainless steel). For example, in some implementations, tungsten is plasma sprayed on the electrode material (e.g., stainless steel 304). For example, Flamespray Northwest in Seattle, Wash., provides plasma spraying services. In other embodiments, the high melting point material can be layered or deposited on the electrode. In other embodiments, the electrodes are formed from the high melting point material.
During the current rise time, the plasma will accelerate as it moves in the plasma propagation channel 114 (e.g., the space between the acceleration electrode 6 and the outer electrode 7) toward the liquid metal funnel system 120. In some implementations, the plasma accelerates for a distance of about 20 m and then for another distance of about 20 m or so to finish discharging the capacitor bank 11. In such embodiments, the total length of the plasma accelerator 110 is about 40 m. Different lengths of the plasma accelerator are possible. For example, the voltage on the capacitors in the bank 11 can be increased while the capacitance of the bank 11 is reduced, thereby maintaining the energy stored in the capacitor bank 11. This can reduce the current rise time and length of the accelerator 110. Use of higher voltage in some implementations may have possible disadvantages such as being technologically challenging and expensive.
In some embodiments, the plasma accelerator 110 comprises a plasma restrictor 23. The length of an embodiment of the accelerator 110 comprising a plasma restrictor can be less than the length of an accelerator embodiment that does not comprise a plasma restrictor. In the embodiment shown in FIG. 1B, the plasma restrictor 23 is disposed near the first end 112 a of the accelerator 110, for example, below the first end 112 a. As the current to the electrodes 6 and/or 7 increases, the magnetic field of the plasma accelerator 110 is initially insufficient to force the plasma past the restrictor 23. Movement of the plasma along the propagation channel 114 is inhibited. The system can be configured such that as the magnetic field of the accelerator 110 increases (e.g., as the current and/or voltage supplied to the electrodes 6 and/or 7 increases), the magnetic field increases and reaches a threshold value at which the magnetic force is sufficient to force the plasma past the restrictor 23. The plasma then accelerates along the propagation channel 114. For example, the system may be configured such that at (or near) peak current the magnetic force is sufficient to push the plasma through the restrictor 23 and to start the plasma accelerating down the plasma accelerator 110.
In some embodiments, the plasma restrictor 23 comprises a constriction in the plasma propagation channel 114. For example, the constriction may comprise a narrowing of the space between the acceleration electrode 6 and the outer electrode 7. In some embodiments, the constriction is provided by disposing one or more structures 23 a in the plasma acceleration channel 114 (see, e.g., FIG. 1B). In other embodiments, the constriction in the plasma channel 114 is provided by shaping the outer electrode 7 and/or the acceleration electrode 6 so that the channel 114 narrows at the location of the constriction. The location, shape, size, spacing, and/or number of constrictions (e.g., structures disposed in or along the channel 114 or narrowings of the channel 114) disposed along the propagation channel 114 can be selected to provide a desired amount of restriction against movement of the plasma along the channel 114. In some such implementations, an accelerator length of about 10 m can be used to transfer the energy from the capacitor bank 11 to the plasma using an 88 kV capacitor voltage.
After the plasma is formed, the plasma electrically contacts the outer electrode 7 and the acceleration electrode 6. This contact can short circuit the acceleration capacitor bank 11 and start current flowing through the plasma. As discussed above, it may be desirable in some implementations to delay the acceleration (e.g., for about 30 μs, in some cases) to allow the closed magnetic surfaces to form and/or for turbulence, if present, to settle. In some such implementations, a saturable inductor 17 (see, e.g., FIG. 1B) is used to delay the voltages provided to the electrodes. The saturable inductor 17 can be disposed in transmission line 15. The saturable inductor 17 may comprise a saturable magnetic material. For example, an amorphous metal such as, e.g., METGLAS 2605Co (available from Metglas Inc., Conway, S.C.) can be used. To provide a delay of about 30 μs at a voltage of about 88 kV the inductor 17 can store about 88 kV multiplied by 30 μs=2.6 V·s. In some embodiments, the inductor 17 is substantially toroidal with a cross-section of about 0.6 m2 and a major radius of about 1 m. In some embodiments, the inductor 17 comprises Metglas wound tape with a saturation field of about 1.8 Tesla to provide an appropriate delay.
In the embodiments schematically illustrated in FIGS. 1A-1D, the system is configured so that at or before the point where the pressure of the plasma builds so that it could exceed the break point or strength of the material or the assembly comprising the electrodes 6 and/or 7 (or other components of the accelerator near the second end 112 b), the plasma exits the accelerator 110 and enters the liquid metal funnel system 120. An advantage of some of these embodiments is that the pressure of the plasma in the accelerator is increased to a relatively large value without damaging the accelerator (e.g., due to yield failure and/or deformation of second end 112 b of the accelerator 110).
In the illustrated embodiments, the liquid metal funnel system 120 comprises a tank 10 and one or more pumps 9 configured to circulate the liquid metal to form a liquid metal funnel 8. The liquid metal flows from a top end of the funnel system 120 to a bottom end of the funnel system 120 under the influence of gravity. In some embodiments, the top end of the funnel system 120 is substantially above the bottom end of the funnel system 120. In some embodiments, the pumps 9 may provide a pressure to the liquid metal, which may also influence the flow of the liquid metal in the tank 10. In some implementations, the funnel 8 has a substantially cylindrical shape having a passage 125 that is substantially aligned with a longitudinal axis of the plasma accelerator 110. The cross-section of the passage 125 (perpendicular to a longitudinal axis of the passage 125) may be substantially circular, substantially oval, substantially polygonal, or any other shape. The cross-sectional shape (and/or size) of the passage can change from the top end to the bottom end. For example, the cross-sectional area at the bottom end may be less than the cross-sectional area at the top end. The passage 125 may have an inner surface having an inner diameter. The cross-section of the inner surface can be substantially circular, substantially oval, substantially polygonal (e.g., rectangular), or any suitable shape. The inner diameter at the bottom end can be less than the inner diameter at the top end. The cross-sectional shape, size, and/or the inner diameter of the passage can be configured to provide a desired amount of compression for the plasma as it moves below the top end. For example, in some embodiments, the inner diameter of the passage 125 at the bottom end is about a factor of 3 smaller than the inner diameter of the passage 125 at the top end. The ratio of the inner diameter of the passage at the top end to the inner diameter of the passage at the bottom end can be about 1.5, about 2, about 4, about 5, about 10, about 15, or greater. This ratio can be in a range from about 1.5 to about 5, from about 2 to about 4, or some other range.
In some embodiments, the plasma may move from the top end to the bottom end of the passage. In other embodiments, the plasma pressure may become sufficiently large during movement of the plasma along the channel that the plasma may disrupt the funnel 8 before the plasma reaches the bottom end of the passage.
In certain embodiments, the liquid material comprising the liquid funnel 8 does not substantially rotate around an axis of the passage. In other embodiments, the liquid material can be introduced into the tank 10 so that the liquid material rotates around the axis of the passage as the liquid material moves from the top end to the bottom end. Funnels in which the liquid material possesses some amount of rotation (or swirling) may provide advantages in some implementations such as, e.g., increasing stability of the inner surface of the passage.
Because the plasma can move at a speed (e.g., about several tens of km/s, or higher, in some cases) that is higher than the speed of sound in the liquid metal (e.g., about 3 km/s, in some cases), the liquid metal does not have time to move out of the way as the plasma moves through the liquid funnel system 120 (e.g., the inertia of the liquid metal funnel at least partially confines the plasma). The liquid metal therefore tends to act as if it were a solid to the plasma and can act to confine the plasma in the passage 125 of the funnel 8. The plasma can experience compression (and heating) in the funnel 8 as the plasma moves from the top end of the funnel 8 to the bottom end of the funnel 8. For example, a pressure of the plasma when the plasma is below the top end of the funnel 8 can be greater than a pressure of the plasma when the plasma is above the top end of the funnel 8. FIGS. 1A-1C schematically illustrate the compressed plasma toroid 13 in the funnel 8.
The radial compression of the plasma in the passage 125 of the funnel 8 can be about 3:1 (or greater) in some implementations. In other implementations, the radial compression of the plasma can be about 1.5:1, about 2:1, about 4:1, about 5:1, about 7:1, about 10:1, about 15:1, or greater. The radial compression of the plasma in the passage 125 of the funnel 8 may be in a range from about 1.5:1 to about 5:1, from about 2:1 to about 4:1, or some other range. In certain implementations, a desired total radial compression of the plasma measured between the first end of the accelerator 110 and the final position of the plasma in the funnel 8 (e.g., when the plasma pressure becomes sufficiently large to disrupt the funnel) can be about 200:1, about 150;1, about 100:1, about 90:1, about 75:1, about 50:1, about 30:1, about 20:1, about 10:1, or some other value. The total radial compression can be in a range from about 50:1 to about 150:1, from about 75:1 to about 125:1, about 80:1 to about 100:1, or some other range.
In some implementations, the desired total radial compression of the plasma toroid (e.g., from the first end 112 a of the accelerator 110 to the final position of the plasma in the funnel 8) can be achieved by configuring the system 1000 to have a first compression ratio in the accelerator 110 and to have a second compression ratio in the funnel 8 such that the first compression ratio multiplied by the second compression ratio equals the desired total compression ratio. For example, to achieve a total compression of about 90:1, the accelerator 110 can be configured to provide a first compression ratio of about 30:1 and the funnel 8 can be configured to provide a second compression ratio of about 3:1. These ratios are not limitations on the disclosed systems and methods, and continuing with this example, a total compression ratio of 90:1 can be achieved differently in different implementations of the system 1000, e.g., about 45:1 in the accelerator and about 2:1 in the funnel, about 18:1 in the accelerator and about 5:1 in the funnel, and so forth. In some embodiments, the first compression ratio in the accelerator 110 is selected so that a pressure of the plasma at the second end 112 b of the accelerator is at or below the material strength or breakpoint of the materials or assemblies of materials at the second end 112 b of the accelerator 110. In some implementations, the accelerator 110 can be configured to provide a desired first compression ratio more readily than the liquid funnel can be configured to provide a desired second compression ratio. In some such implementations, it may be advantageous for the accelerator 110 to provide more compression than the funnel 8 (e.g., the first compression ratio is larger than the second compression ratio).
The liquid funnel 8 can comprise a suitable liquid metal such as, for example, molten lead-lithium (PbLi) with about 17% lithium (Li). Other lithium percentages can be used in other embodiments (e.g., 0%, 5%, 10%, 15%, 20%, 25%, etc.). Also, other liquid materials (e.g., other liquid metals, liquid metal alloys, etc.) can be used in other embodiments. For example, in other embodiments, substantially pure liquid lithium and/or enriched liquid lithium can be used. In some embodiments, the liquid metal comprises one or more lithium isotopes, which can absorb neutrons and produce tritium.
In some implementations of a system in which the plasma comprises a fusionable material, the plasma can be compressed to a density and/or temperature sufficient to initiate at least some thermonuclear reactions in the fusionable material. The thermonuclear reactions may produce neutrons. Some of the neutrons may be used for neutron analysis if the system is configured, e.g., as a neutron source. Some of the neutrons may be absorbed by, e.g., the liquid metal funnel 8 and their energy converted to heat in the molten funnel. Some of this heat may be extracted to produce electrical power (e.g., via steam turbines) if the system is configured, e.g., as an energy source. During or after passage of the plasma through the funnel 8, the liquid metal funnel 8 generally is at least partially disturbed and/or destroyed (e.g., the liquid metal splashes outwards but is contained by a tank 10). The pumps 9 circulate liquid metal into the tank 10 to re-form the liquid metal funnel 8 for subsequent injections (or shots) of the plasma. Accordingly, embodiments of the system schematically illustrated in FIGS. 1A-1D may be configured to act as a pulsed source of neutrons and/or energy as plasma toroids are repeatedly introduced into the liquid metal funnel 8.
In some embodiments (see, e.g., FIGS. 1B-1D), in addition to the liquid metal funnel 8, the liquid funnel system 120 comprises a substantially central or axial liquid guide 22. For example, the liquid guide 22 can be substantially aligned with the longitudinal axis 115 of the accelerator 110 and/or the axis of the passage 125. The liquid guide 22 can be configured to stabilize and/or reduce a tendency for tilting of the plasma torus in the funnel system 120. In some embodiments, the liquid guide 22 is supplied by liquid metal from a liquid metal storage tank or reservoir 18. The storage tank 18 is disposed between the acceleration electrodes 6 in some embodiments. In the embodiment shown in FIG. 1B, the liquid guide 22 flows at least partially under gravity toward the bottom of the tank 10, and a pump 21 can be used to recirculate the liquid metal back into the storage tank 18 for reuse. In some such embodiments, it is advantageous if the liquid metal used for the funnel 8 and the liquid metal used for the liquid guide 22 comprise the same material, because of the likely mixing of the liquid metal of the guide 22 and the liquid metal of the funnel 8 in the tank 10. For example, the liquid metal for the liquid guide 22 can comprise molten PbLi.
In some such embodiments, the plasma is compressed between the inner surface of the funnel 8 and the outer surface of the liquid guide 22, which advantageously may provide a larger amount of compression than embodiments not using a liquid guide 22. The size and/or shape of the funnel 8 and/or the liquid guide 22 can be configured to provide a desired amount of compression and/or heating for the plasma as the plasma moves below the top of the liquid metal funnel system 120. The liquid guide 22 may be physically and/or electrically isolated from the liquid funnel 8 (and/or the tank 10) in various embodiments.
An advantage of some embodiments of the system that use a liquid guide 22 is that the liquid metal is electrically conductive and acts like a substantially central or axial electrode. In some such embodiments, the electrical current from the plasma accelerator 110 can continue to provide a magnetic (and/or electromagnetic) force that pushes on the plasma to provide further compression. Accordingly, some such embodiments can provide additional compression compared to certain embodiments not comprising the liquid guide, in which compression in the funnel 8 is provided primarily by the momentum of the plasma.
In certain embodiments, the liquid guide 22 is electrically isolated from the outer electrode 7, to reduce the likelihood of or avoid shorting the electrical circuit. In certain such embodiments, the liquid guide 22 is not provided continuously into the tank 10. For example, the liquid funnel system 120 may comprise a liquid guide injection system that injects the liquid guide 22 into the passage of the funnel 8 at desired times. For example, the liquid guide injection system can comprise a pulse valve 20 that can be opened shortly before a plasma shot. The plasma shot can be fired before the lower end of the liquid metal in the liquid guide 22 contacts the bottom of the tank 10 (or contacts liquid metal at the bottom of the tank 10), because such contact is likely to complete the electrical circuit. After each shot, the pump 21 (e.g., an intermittent pump) recirculates some of the liquid metal in the tank 10 to the storage tank 18. In some embodiments, the pump 21 operates to refill the storage tank 18 when the acceleration electrode 6 is not at a high voltage (e.g., between shots of plasma). In some embodiments, a portion of the recirculation plumbing (e.g., a return pipe 31) used for recirculating the liquid metal into the tank 18 comprises an electrically insulated section 19 (see, e.g., FIGS. 1B and 1C). The insulator section 19 can be oriented substantially vertically to permit drainage of residual liquid metal after refilling of the storage tank 18 to reduce the likelihood of short circuiting the acceleration electrode 6. In some embodiments, the space above the fluid in the storage tank 18 is pressurized (e.g., at a pressure of about 30 psi, in some cases) (e.g., about 2.07×105 Pa) with an inert gas such as, e.g., argon. The pressurized inert gas provides a downward force on the liquid in the storage tank 18 that (in combination with gravity) allows the liquid metal to be ejected at a desired speed.
The following discussion is intended to give illustrative, non-limiting examples of certain parameters of an embodiment of a system that could be used to achieve certain plasma compression values. Various assumptions are discussed in the context of these examples, and various equations and example calculations are provided herein to highlight some of the factors and considerations involved in an example embodiment of a system for compressing a plasma. The following discussion is not intended to limit the scope of the systems and methods described herein, nor end-uses or applications of the disclosed systems. In other implementations of the systems and methods described herein, other equations, parameters, factors, and considerations may be applicable.
Magnetized Target Fusion (MTF) systems typically use significant energy (e.g., about 100 MJ in some cases) to compress the plasma. For generating fusion energy in many systems, the well-known Lawson criteria indicates that a plasma of density n, maintained at a temperature of 10 keV, for a time τ, should be selected so that nτ>1020 m−3 s for fusion heating to exceed plasma heat losses. However, the plasma cools down with a time τ=r2/χ where r is the smallest distance between the hot plasma core and the cold edge of the reactor, and χ is the diffusivity. Therefore, a larger plasma (e.g., larger r) may be beneficial but uses more energy for its formation, and generally therefore a larger and more expensive apparatus.
The energy in the plasma is 3/2 NkTi for the ions and 3/2N kTe for the electrons, where Ti is ion temperature, Te is electron temperature and N is the number of ions or electrons. The number of ions and electrons is equal in the case of overall charge neutrality. Assuming Ti and Te are the same temperature, then the thermal energy (Eth) in the plasma is 3 NkT.
with N=nV, where V is plasma volume, and Emag=Eth/β where β is the ratio of plasma pressure/magnetic pressure. The total energy is the thermal energy Eth plus the magnetic energy Emag. For a torus, the volume is 2π2r2R where R is the major radius (around the torus) and r is the minor radius. For a compact torus R is approximately equal to r so the volume can be approximated as 2π2r3.
E=7×1016 (1+1/β) χ3/2 n −1/2 Joules with n in m−3 and χ in m2/s.
where ρi is the ion gyroradius and vi is the ion thermal velocity.
Assuming Bohm diffusion (as a worst case example scenario), the minimal plasma energy to achieve the Lawson criterion for various plasma densities (e.g., at 10 keV and β=0.1 typical of certain spheromaks) can be predicted from the above equations for the above example system and is shown in the graph illustrated in FIG. 2 (solid line with diamonds). The magnetic pressure of a plasma at a temperature of 10 keV, β=0.1 at various densities is also plotted on the graph shown in FIG. 2 (solid line with squares). The maximum pressure that solid material can take before breaking is typically about 1×104 atm (e.g., about 1000 MPa). At that pressure, the example calculations shown in FIG. 2 indicate the example system should provide about 100 MJ in the plasma to achieve break-even, and possibly a few times more than that energy for a practical gain. Assuming a transfer efficiency from the power source to the plasma of about 50%, the system should provide at least about 200 MJ of energy to heat the plasma to a fusion temperature.
Embodiments of the disclosed system configured as an energy source may provide advantages. For example, using a liquid metal funnel can allow pressures in the plasma to be achieved that are above the breaking point of solid materials. Therefore, embodiments of the disclosed systems may provide increased plasma density, which advantageously reduces the energy used by the system. This may also reduce the cost and/or size of the system.
In some embodiments of the present systems and methods, the plasma pressure increases as the plasma is accelerated and then compressed as the plasma moves down the accelerator 110 (e.g., along the propagation channel 114 between the coaxial tapered electrodes 6, 7). At or before the point along the plasma path where the plasma pressure meets and/or exceeds the strength of the confining electrode material, the plasma is directed into the liquid metal funnel system 120 in which further compression occurs. For example, the plasma compression can be about a factor of 30 in the accelerator and about a factor of 3 in the funnel system. In some embodiments, the plasma can be accelerated to a speed greater than about 100 km/s down the accelerator 110. The speed of sound in the liquid metal is generally of the order 3 km/s, so the liquid metal does not have time to move out of the way, and a high plasma pressure is maintained in the funnel 8. In some implementations, a shock wave wake may be generated in the liquid metal. The energy in the shock wave wake is drawn from the plasma kinetic energy; which can be a new energy loss mechanism in some such embodiments.
where R is the radius of the liquid metal funnel 25.
where K is the volume compression modulus and V0 is the initial volume at zero compression.
In some implementation, electrical currents may be induced in the liquid metal by the magnetic field of the spheromak. Resistive losses in the liquid metal may reduce the energy in the magnetic field that contains the plasma, representing another possible energy loss mechanism in some cases. The following illustrative example is used to provide an estimate for this energy loss mechanism.
where L is the length of the plasma, B is the magnetic field in the spheromak (or other suitable compact torus) and μ0 is the vacuum permeability.
where T is in eV and n is in m−3 and Zeff=ΣZ2nz/n where Z is the atomic number of the impurity and nz is its density. The Bremsstralung radiation power losses are a function of the square of the impurity atomic number Z, so having a low impurity content can be advantageous in some cases, especially for impurities with high atomic numbers.
Continuing with this illustrative, non-limiting example calculation, dividing the energy in the plasma configuration by these various power losses gives a total plasma confinement time τ. Using that confinement time it is possible to calculate the minimum plasma energy to achieve a Lawson break-even condition at various densities for this example embodiment of the system. The energy for this embodiment is shown in the graph of FIG. 4.
Note that the energy used may be more than indicated by the example graph in FIG. 2 in some implementations, because energy loss mechanisms particular to the above example embodiment have been taken into account. The graph in FIG. 4 shows that an example estimate for the minimum plasma energy used is about 3 MJ at an example density of 1019 cm−3. Compare this to the example results shown in FIG. 2 that indicate less than about 1 MJ at this example density. The plasma outer radius R is 2.4 cm in this example calculation. The confinement time is 10 μs in this example calculation. The magnetic field is 200 Tesla, and the pressure is 0.16 Mbar, in this example calculation. A possible value for the speed of the plasma during maximum compression is just above the speed of sound, for example, about 5 km/s. Based on these example values, the plasma moves only about 50 mm during the time where the plasma temperature and pressure conditions could allow fusion to occur.
As discussed above, during and/or after the passage of the plasma, the liquid metal funnel may tend to be outwardly disrupted in some implementations of the system. In some such implementations, the system can be configured so that the liquid metal funnel will reform after a time Lfe/vf where Lfe is the length of the funnel and vf is the speed at which the liquid is expelled from the nozzles (that input liquid metal into the tank 10 of the funnel system 120). These parameters can be used to determine an example estimate for the maximum pulse repetition rate in such an embodiment. In this illustrative, non-limiting example, about 1 m of the liquid metal is used to absorb most of the neutrons so, for example, a 2 m long liquid metal funnel, where the plasma temperature and pressure conditions are suitable for fusion to occur in the center, would be appropriate for some embodiments. Assuming vf is approximately 10 m/s, the repetition rate could be about 5 Hz in this example. Finally if the net energy out is of the order of the energy in, the plasma will produce approximately 3 MJ at 5 Hz yielding a power output of approximately 15 MW, which is suitable for a small power plant. Note that these estimates provide one possible estimate for the size of a power plant producing break-even in this example, and a larger plant may provide more power but may cost more to develop and build.
Continuing with this illustrative, non-limiting example, working from the conditions at maximum compression and assuming that some plasma guns 100 typically produce plasma densities not much in excess of about 1014 cm−3, the initial plasma formation at the first end 112 a of the plasma accelerator 110 would be about 2.2 m in diameter in order to provide the final 2.4 cm radius compressed plasma with a density of about 1019 cm −3. The length of the plasma formation initially will be about 1 m, so this is about the length estimated for the formation region in this example implementation. Therefore, the ratio of the radial size of the compact toroid at the first end 112 a of the accelerator 110 to the radial size of the compact toroid when the toroid is in the liquid metal funnel 8 is about 100 to 1 in this example. In other embodiments, this ratio can be different such as, for example, about 5:1, about 10:1, about 25:1, about 50:1, about 90:1, about 125:1, about 150:1, about 200:1, or some other value.
Accordingly, in this example, a final speed of the plasma is about 1700 km/s. In order for the transit time of the plasma to equal half the ringing time, an accelerator length of about 40 m can be used in some cases. The length of the accelerator can be advantageously reduced by using a plasma restrictor at or near the first end 112 a of the accelerator 110 (see, e.g., the constriction shown in FIG. 1B or the magnetic coils 23 b shown in FIG. 1C). As the current increases, limited by the inductance, the plasma is unable to pass through the constriction. In some embodiments, the system is configured such that only at or near peak current is the magnetic force strong enough to force the plasma through the constriction and rapidly accelerate the plasma. In some such embodiments, because the plasma starts accelerating only at (or near) peak current, an accelerator that is only about ¼ the length (e.g., about 10 m, in some cases) can be used. This would provide a reasonable, practical, realistic implementation of a system for compressing plasma and, in some cases, initiating fusion reactions. Implementations of such a system may have other uses as well.
As discussed above, certain embodiments of the above-described systems and methods can be used to compress a plasma that comprises a fusionable material sufficiently that fusion reactions and useful neutron production can occur. For example, the fusionable material may comprise one or more isotopes of light elements such as, e.g., deuterium, tritium, helium-3, lithium-6, lithium-7, etc. Accordingly, certain embodiments of the system may be configured and operated to act as neutron generators or neutron sources. Neutrons so produced have a wide range of practical uses in research and industrial fields. For example, a neutron source can be used for neutron activation analysis (NAA) which can provide multi-element analysis of major, minor, trace, and rare elements in a variety of substances (e.g., explosives, drugs, fissile materials, poisons, etc.) and can be used in a variety of applications (e.g., explosive detection and identification, ecological monitoring of the environment and nuclear waste, etc.). Embodiments of the system configured as a neutron source can also be used for materials research (e.g., analyzing the structure, dynamics, composition, and chemical uniformity of materials), for non-destructive testing of industrial objects (e.g., via neutron radiography and/or neutron tomography), and for many other industrial and technological applications. For example, embodiments of the system may be used for nuclear waste remediation and generation of medical nucleotides.
Embodiments of the above-described systems and methods for plasma heating and compression are also suited for applications in the study of high energy density plasma including, for example, applications in astrophysics and nuclear physics.
Recent advances in energy storage (for example, supercapacitors) and high-power semiconductor switching have driven down the cost of high-power electrical components. Further developments in electrical pulse power systems and increasing demand for such components for a variety of applications is expected to make an electrically-driven MTF system (and/or neutron source) cost competitive with other approaches. In applications where cost is less of a factor (e.g., fusion space propulsion where a lower mass payload may be at a premium), embodiments of such an electrically-driven system may be already appealing compared to other possible technologies.
In certain implementations of the systems and methods disclosed herein, achieving plasma compression based on an electrical rather than a mechanical approach (e.g., certain piston-based systems) can, in some cases, be expected to reduce system maintenance and offer other advantages. For example, in some such implementations, the acceleration system can be configured with fewer or no moving parts and can be of lower weight. In some embodiments, synchronization issues are simplified relative to certain embodiments of a piston-based system.
While particular elements, embodiments, examples, and applications of the present disclosure have been shown and described, it will be understood, that the scope of the disclosure is not limited thereto, since modifications can be made by those skilled in the art without departing from the scope of the present disclosure, particularly in light of the foregoing teachings. Thus, for example, in any method or process disclosed herein, the acts or operations making up the method/process may be performed in any suitable sequence and are not necessarily limited to any particular disclosed sequence. Elements and components can be configured or arranged differently, combined, and/or eliminated in various embodiments. Reference throughout this disclosure to “some embodiments,” “an embodiment,” or the like, means that a particular feature, structure, step, process, or characteristic described in connection with the embodiment is included in at least one embodiment. Thus, appearances of the phrases “in some embodiments,” “in an embodiment,” or the like, throughout this disclosure are not necessarily all referring to the same embodiment and may refer to one or more of the same or different embodiments. Indeed, the novel methods and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, additions, substitutions, equivalents, rearrangements, and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions described herein.
Various aspects and advantages of the embodiments have been described where appropriate. It is to be understood that not necessarily all such aspects or advantages may be achieved in accordance with any particular embodiment. Thus, for example, it should be recognized that the various embodiments may be carried out in a manner that achieves or optimizes one advantage or group of advantages as taught herein without necessarily achieving other aspects or advantages as may be taught or suggested herein.
Conditional language used herein, such as, among others, “can,” “could,” “might,” “may,” “e.g.,” and the like, unless specifically stated otherwise, or otherwise understood within the context as used, is generally intended to convey that certain embodiments include, while other embodiments do not include, certain features, elements and/or steps. Thus, such conditional language is not generally intended to imply that features, elements and/or steps are in any way required for one or more embodiments or that one or more embodiments necessarily include logic for deciding, with or without operator input or prompting, whether these features, elements and/or steps are included or are to be performed in any particular embodiment. No single feature or group of features is required for or indispensable to any particular embodiment. The terms “comprising,” “including,” “having,” and the like are synonymous and are used inclusively, in an open-ended fashion, and do not exclude additional elements, features, acts, operations, and so forth. Also, the term “or” is used in its inclusive sense (and not in its exclusive sense) so that when used, for example, to connect a list of elements, the term “or” means one, some, or all of the elements in the list.
The example calculations, results, graphs, values, and parameters of the embodiments described herein are intended to illustrate and not to limit the disclosed embodiments. Other embodiments can be configured and/or operated differently than the illustrative examples described herein.
wherein compressing the toroidal plasma comprises compressing the toroidal plasma between an inner surface of the passage in the liquid funnel and an outer surface of the liquid guide.
2. The method of claim 1, wherein generating the toroidal plasma comprises generating a spheromak.
3. The method of claim 1, wherein accelerating the toroidal plasma comprises accelerating the toroidal plasma with an electromagnetic rail gun.
4. The method of claim 3, wherein accelerating the toroidal plasma with the electromagnetic rail gun comprises compressing the toroidal plasma by the rail gun.
5. The method of claim 1, further comprising recirculating liquid to form the liquid funnel.
6. The method of claim 1, wherein the liquid funnel comprises a liquid metal.
7. The method of claim 1, further comprising electrically isolating the liquid guide from the liquid funnel when the toroidal plasma is between the first end and the second end of the passage in the liquid funnel.
8. The method of claim 1, further comprising discharging a capacitor bank to provide electrical energy for accelerating the toroidal plasma.
9. The method of claim 8, wherein discharging the capacitor bank comprises using a saturable inductor to delay discharging the capacitor bank.
compressing the toroidal plasma as the toroidal plasma moves from the first end of the passage toward the second end of the passage.
11. The method of claim 10, wherein generating the toroidal plasma comprises generating a spheromak.
12. The method of claim 10, wherein accelerating the toroidal plasma comprises accelerating the toroidal plasma with an electromagnetic rail gun.
13. The method of claim 12, wherein accelerating the toroidal plasma with the electromagnetic rail gun comprises compressing the toroidal plasma by the rail gun.
14. The method of claim 10, further comprising recirculating liquid to form the liquid funnel.
15. The method of claim 10, wherein the liquid funnel comprises a liquid metal.
16. The method of claim 10, further comprising discharging a capacitor bank to provide electrical energy for accelerating the toroidal plasma.
17. The method of claim 16, wherein discharging the capacitor bank comprises using a saturable inductor to delay discharging the capacitor bank.
A. Prosperetti, "No Nuclear Fusion' from glowing bubbles", Chemistry & Industry News, http://ci.mond.org/9708/970810.html, Apr. 21, 2007.
A. Takahashi, "Comments on work on sonofusion of D in acetone", http://www.cf.ale.iwateu.ac.jp/jcf/mlist00042.html, Mar. 3, 2002.
B. Bauer et al., "Magnetized High Energy Density Laboratory Plasmas," http://fusionenergy.lanl.gov/mhedlp-wp.pdf, Apr. 20, 2007, in 24 pages.
B. E. McDonald, "Modeling nonlinear compressional waves in marine sediments", Nonlin. Processes Geophys., vol. 16, Feb. 26, 2009, pp. 151-157.
Bellan, P.M., "Spheromaks: A practical applicationo f magnetohydrodynamic dynamos and plasma self-organization," Imperial College Press, 2000, pp. 1-9, 268-275.
Bohm, "Quantum Theory", Dover Publish, Inc., 1979, pp. 177-181, New York, USA.
Brenner et al, "Single-bubble Sonoluminescence", Reviews on Modern Physics, Apr. 2002, vol. 74, pp. 425-484.
Browne, M.W., "New Shot at Cold Fusion by Pumping Sound Waves into Tiny Bubbles," New York Times, Dec. 20, 1994.
Browning, P.K. et al., "Power Flow in a Gun-Injected Spheromak Plasma", The American Physical Society, Physical Review Letters, vol. 68, No. 11, Mar. 16, 1992, pp. 1718-1721.
C. W. Hartman et al, "A Compact Torus Fusion Reactor Utilizing a Continuously Generated String of CT's. The CT String Reactor, CTSR", Journal of Fusion Energy (2008), Nov. 2, 2007 published online, Issue 27, pp. 44-48.
C. W. Hartman et al, "Acceleration of Spheromak Toruses, Experimental results and fusion applications", OSTI ID: 5240480; DE90005312, Proceedings of 11th US/Japan workshop on field-reversed configurations and compact toroids; Dec. 1, 1989, Los Alamos, NM, USA, Nov. 7-9, 1989.
C. W. Hartman et al., "Acceleration of Compact Toroid Plasma Rings for Fusion Applications," Lawrence Livermore National Laboratory, UCRL-98504, Prepared for Submittal to IAEA 12th International Conference on Plasma Physics and Controlled Nuclear Fusion Research in Nice, France, Oct. 12-19, 1988, in 16 pages.
C.E.Kessel "Control of plasma profiles in a Tokamak", NSF Workshop on Mathematical Modeling and Control of Plasma in Magnetic Fusion, General Atomics, May 11-12, 2006, in 20 pages.
C.E.Kessel et al., "Simulations and Experiments on Modifying the q-Profile for Advanced Tokamak Discharges on Alcator C-Mod", APS Division of Plasma Physics, Nov. 2007, in 40 pages.
C.W. Hartman et al., "Acceleration of Compact Torus Plasma Rings in a Coaxial Rail-Gun", 7th Symposium on Compact Toroid Research, Santa Fe, New Mexico, May 21-23, 1985, in 6 pages.
C.W. Hartman et al., "Acceleration of Compact Toruses and Fusion Applications" , Workshop on Physics of Alternative Magnetic Confinement Schemes, UCRL-JC-106121 Preprint, Oct. 11, 1990, Issue UCRL-JC-106121 Prepr, Varenna, Italy, Oct. 15-24, 1990.
Ch. Mangeant et al., "Syrinx Project: Compact Pulse-Current Generators Devoted to Material Study Under Isentropic Compression Loading", in Pulsed Power Plasma Science, IEEE, Jun. 2001, in 4 pages.
Ch. Seife, "Sun in a Bottle", Chapter 10, pp. 220-227, Penguin Books Ltd., London, UK (2008).
Compact Toroid, Wikipedia, Http://en.wikipedia.org/wiki/Compact-toroid, downloaded Mar. 14, 2014.
Compact Toroid, Wikipedia, Http://en.wikipedia.org/wiki/Compact—toroid, downloaded Mar. 14, 2014.
D. Braaten, "'Ridiculously easy' test yields claim of energy triumph", Washington Times, Mar. 24, 1989, p. A5.
D. Braaten, "‘Ridiculously easy’ test yields claim of energy triumph", Washington Times, Mar. 24, 1989, p. A5.
D. Foley, "Star in a Jar", Popular Science, Dec. 1998.
D. Orlikowski et al., "New experimental capabilities and theoretical insights of high pressure compression waves", Lawrence Livermore National Laboratory, UCRL-PROC-233023, Jul. 24, 2007, 10 pages.
D.J. Meeker et al., "A High Efficiency I.C.F. Driver Employing Magnetically Confined Plasma Rings", UCRL-91693 Preprint, Lawrence Livermore National Laboratory, Mar. 4, 1985, in 8 pages.
D.M.Willett et al., "The internal magnetic structure and current drive in the SPHEX spheromak", Plasma Phys. Control. Fusion, vol. 41, Mar. 1999, pp. 595-612.
D.N. Hill et al., "Field and Current Amplification in the SSPX Spheromak," 19th IAEA Fusion Energy Conference, Oct. 8, 2002, in 8 pages.
Extended European Search Report, dated May 31, 2013 in corresponding European Application No. 10738264.0, 8 pages.
F. D. Witherspoon et al., "A contoured gap coaxial plasma gun with injected plasma armature," American Institute of Physics, Review of Scientific Instruments 80, 083506, Aug. 2009, in 15 pages.
F. D. Witherspoon et al., "Pulsed Injector Development for Dense Plasma Jets," Research Funded by the DOE Office of Fusion Energy Science through Grants DE-FG02-04ER83978, DE-FG02-05ER54810, DE-FG02-05ER84189, Feb. 2007, in 32 pages.
F.Crisanti et al., "Active control of the plasma current profile on JET Experiments", 30th Conference on Contr. Fusion and Plasma Phys., St. Petersburg, Jul. 7-11, 2003, ECA vol. 27A, P-2.88, in 4 pages.
Fortov, V., "Nonideal plasma under extreme conditions generated by shock waves", Plasma Phys. Control, Fusion, 45, pp. Al-A6 (2003).
Fowler, T.K., "Pulsed Spheromak Fusion Reactors", Comments on Plasma Physics & Controlled Fusion, Comments on Modern Physics, vol. 1(3), Part C, 1999, pp. 83-98.
Fowler, T.K., "Pulsed Spheromak Reactor With Adiabatic Compression", Lawarence Livermore National Laboratory, in 13 pages, Mar. 29, 1999.
Fowler, T.K., "Stability of Spheromaks Compressed by Liquid Walls", Lawrence Livermore National Laboratory, in 9 pages, Aug. 17, 1999.
G. Pusch, "Why is acetone used in sonofusion experiments?", website http://www.physics-talk.com, Apr. 26, 2004.
Gregory H. Miller et al., "The Equation of State of a Molten Komatiite 1. Shock Wave Compression to 36 GPa", Journal of Geophysical Research, vol. 96, No. B7, Jul. 10, 1991, pp. 11,831-11,848.
H. P. Furth, "The Tokamak," Fusion, vol. 1, Magnetic Confinement, Part A, ed. Edward Teller, Academic Press, pp. 123-242, 1981.
H. S. McLean et al, "Design and operation of a passively switched repetitive compact toroid plasma accelerator", Fusion Technology, May 1998, vol. 33, pp. 252-272.
Hitoshi Takeuchi et al., "Equations of State of Matter from Shock Wave Experiments", Journal of Geophysical Research, vol. 71, No. 16, Aug. 15, 1966, pp. 3985-3994.
Howard, S. et al., "Development of merged compact toroids for use as a magnetized target fusion plasma," Journal of Fusion Energy, Nov. 11, 2008, vol. 28, No. 2, pp. 156-161, available Jun. 2008.
Hsu, S.C. et al., "On the Jets, Kinks, and Spheromaks Formed by a Planar Magnetized Coaxial Gun", California Institute of Technology, Pasadena, CA 91125, Feb. 2, 2008, pp. 1-16.
I. Sample, "Science runs into trouble with bubbles", The Guardian, Mar. 11, 2004.
International Preliminary Report on Patentability dated Jan. 31, 2012 for Int3 l Application No. PCT/US2010/043587, in 8 pages.
International Search Report and Written Opinion dated Jun. 23, 2009 for Int'l Application No. PCT/IB2010/000368.
International Search Report and Written Opinion dated Nov. 30, 2010 for Int'l Application No. PCT/US2010/043587.
Intrator, T. et al., "A high density field reversed configuration (Frc) target for magnetized target fusion: First internal profile measurements of a high density FRC," Phys. Plasmas, vol. 11, No. 5, pp. 2580-2585, May 2004.
J. D. Graham et. al., "Shiva Star-MARAUDER Compact Torus System," Digest of Technical Papers, 8th IEEE International, Pulsed Power Conference, Jun. 1991 pp. 990-993.
J. D. Graham et. al., "Shiva Star—MARAUDER Compact Torus System," Digest of Technical Papers, 8th IEEE International, Pulsed Power Conference, Jun. 1991 pp. 990-993.
J. Eddleman et al., "Final Report on the LLNL Compact Torus Acceleration Project," Lawrence Livermore National Laboratory, UCRL-ID-120238, Mar. 19, 1995, in 62 pages.
J. H. Degnan,et al, "Compression of compact toroids in conical-coaxial geometry", Fusion Technology, Mar. 1995, vol. 27, Issue 2, pp. 107-114.
J. H. Degnan,et al., "Compact toroid formation, compression, and acceleration", Phys. Fluids B, Aug. 1993, vol. 5 , Issue 8, pp. 2938-2958.
J. H. Hammer, et al, "Experimental demonstration of acceleration and focusing of magnetically confined plasma rings", Physical Review Letters, Dec. 19, 1988, vol. 61, Issue 25, pp. 2843-2846.
J. Nguyen et al., "Specifically Prescribed Dynamic Thermodynamic Paths and Resolidification Experiments", Lawrence Livermore National Laboratory, UCRL-JRNL-201169, Nov. 25, 2003, in 8 pages.
J. Wilson, "Hot Sounds", http://www. popularmechan ic.com/science/research/12816666.html, Feb. 1, 1998.
J.D. Lawson, "Some Criteria for a Power Producing Thermonuclear Reactor", Proc. Phys. Soc, 1957, Issue B70, pp. 6-10.
J.E.Barton et al., "Closed-loop control of the safety factor profile in the TCV Tokamak", 53rd IEEE Conference on Decision and Control, Dec. 15-17, 2014, Los Angeles, California, pp. 5660-5665.
J.T.Slough et al., "Multimegawatt solid state rf driver for generating rotating magnetic fields", Review of Scientific Instruments, vol. 71, No. 8, Aug. 2000, pp. 3210-3213.
K. Suslick, "Chemistry cast doubt on bubble fusion", Nuclear News, Sep. 2002.
Kirkpatrick, R.C., "Assessment of the Acoustically Driven MTF Experiments being conducted by Dr. Michel Laberge of General Fusion, Inc.," in 3 pages, May 2007.
Kiuttu, G.F., et al., "Acceleration and compression of compact toroid plasmas," 1994 10th International Conference on High-Power Particle Beams, IET, vol. 1, pp. 150-158, Jun. 1994.
Knief, R. A., Nuclear Engineering, Theory and Technology of Commercial Nuclear Power, Hemisphere Publishing Corp., pp. 640-643, 1992.
L. A. Artsimovich, "Controlled Thermonuclear Reactions", Gordon & Breach Science Publishers, 1964, pp. 1-9, New York , USA.
L. Bertolini, et al, "SHARP, a first step towards a full sized Jules Verne Launcher", Lawrence Livermore National Lab; OSTI ID: 10125664; Legacy ID: DE94007029 Report No. UCRL-JC-114041; CONF-9305233-2, May 1, 1993, Issue CONF-9305233-2.
L. Bertolini, et al, "SHARP, a first step towards a full sized Jules Verne Launcher", Lawrence Livermore National Lab; OSTI ID: 10125664; Legacy ID: DE94007029 Report No. UCRL-JC—114041; CONF-9305233-2, May 1, 1993, Issue CONF-9305233—2.
L. Crum, "Sonoluminescence and Acoustic Inertial Confinement", Fifth International Symposium on Cavitation, Nov. 1-4, 2003, Osaka , Japan.
Laberge, M., "Acoustic Wave Driven MTF Fusion Reactor," in 20 pages, Mar. 2007.
Laberge, M., "An Acoustically Driven Magnetized Target Fusion Reactor," Journal of Fusion Energy, vol. 27, Nos. 1-2, pp. 65-68, Jul. 11, 2007.
Laberge, M., "Evidence of Fusion Products in Acoustically Driven MTF," in 41 pages, Mar. 2007.
Laberge, M., "Experimental Results for an Acoustic Driver for MTF," Journal of Fusion Energy, Jun. 2009, vol. 28, Nos. 2, pp. 179-182, available Jun. 2008.
Liu, D. et al., "Bench Test and Preliminary Results of Vertical Compact Torus Injection Experiments on the STOR-M Tokamak", Nuclear Fusion 46 (006) pp. 104-109, Dec. 16, 2005.
Logan, B.G., et al., "Compact Torus Accelerator Driven Inertial Confinement Fusion Power Plant HYLIFE-CT," Lawrence Livermore National Laboratory, UCRL-TR-211025, Apr. 1, 2005, in 85 pages.
M. Delage et al., "Progress Towards Acoustic Magnetized Target Fusion: An Overview of the R&D Program at General Fusion", 33rd Ann. Conf. Can. Nuc. Soc., Jun. 2012, in 13 pages.
Miyazawa, J. et al., "Design of Spheromak Injector Using Conical Accelerator for Large Helical Device", Fusion Engineering and Design 54 (2001), pp. 1-12.
Moss et al, "Hydrodynamic simulations of bubble collapse and picosecond sonoluminescence", The Physics of Fluids, 1994, vol. 6 , Issue 9, pp. 2979-2985.
N. M. Schnurr et. al., "An Analytical Investigation of the Impingement of Jets on Curved Deflectors", AIAA Journal, vol. 10, No. 11, Nov. 1972, in 41 pages.
Olynyk, G. et al., "Development of a Compact Toroid Fuelling System for ITER", Nuclear Fusion, vol. 48, No. 9, Sep. 2008.
Olynyk, G. M., "Design and evaluation of a repetitive-fire compact toroid fuelling system for ITER," thesis submitted to the Department of Physics, Queen's University, Ontario, Canada, Mar. 2007, in 48 pages.
Partial Translation of Office Action received in corresponding Japanese Application No. 2011-548807, dated Apr. 10, 2012, 5 pages.
R. E. Peterkin, Jr., , "Direct electromagnetic acceleration of a compact toroid to high density and high speed", Physical Review Letters, Apr. 17, 1995, vol. 74, Issue 16, pp. 3165-3168.
R. L. Miller and R. A. Krakowski, "Assessment of the slowly-imploding liner (LINUS) fusion reactor concept", Los Alamos Scientific Laboratory, Oct. 1980, Issue Rept. No. LA-UR-80-3, Los Alamos, NM, USA.
R. S. Hawke, "Design and Analysis of Isentropic Compression Experiments", Lawrence Livermore Laboratory, Preprint UCRL-81797, May 7, 1979, in 23 pages.
R. Siemon, et al., "The Relevance of Magnetized Target Fusion (MTF) to practical energy production", A white paper for consideration by the fusion community and the Fusion Energy Scientific Advisory Committee, Jun. 3, 1999, Draft 2.
R. W. Moir et al., "HYLIFE-II: An approach to a long-lived, first-wall component for inertial fusion power plants", Lawrence Livermore National Lab, Aug. 1, 1994, vol. Report No. UCRL-J, Issue CONF-940933-46.
R.C. Duck et al., "Structure of the n = 1 responsible for relaxation and current drive during sustainment of the SPHEX spheromak", Plasma Physics and Controlled Fusion, vol. 39, No. 5, May 1997, 715-736.
R.G. Kraus et al., "Equation of state of ductile granular materials", DYMAT International Conference on Mechanical and Physical Behaviour of Materials, Sep. 2009, pp. 1317-1323.
Raman, R. et al., "Compact Toroid Fuelling for ITER", Fusion Engineering and Design 39-40 (1998), pp. 977-985.
Raman, R. et al., "Experimental Demonstration of Nondisruptive, Central Fueling of a Tokamak by Compact Toroid Injection," Phys. Rev. Lett., 1994, pp. 3101-3105.
Raman, R. et al., "Experimental Demonstration of Tokamak Fueling by Compact Toroid Injection," Nuclear Fusion, vol. 37, 1997, pp. 967-972.
Raman, R. et al., "ITER Task D315 (1997): Conceptual Design Definition of a Compact Toroid Injection System", CFFTP G-9729, in 24 pages, Sep. 1997.
Raman, Roger et al., "Design of the Compact Toroid Fueler for Center Fueling Tokamak de Varennes", Fusion Technology, A Journal of the American Nuclear Society, vol. 24, No. 3, Nov. 1993, pp. 239-250.
Richardson et al., "Status of Progress Towards Acoustic Magnetized Target Fusion at General Fusion", 34th Annual Conference on the Canadian Nuclear Society, Jun. 12, 2013, in 15 pages.
Robert S. Hixson et al., "Shock Compression Techniques for Developing Multiphase Equations of State", Los Alamos Science, No. 28, Jan. 2003, pp. 114-119.
S. Putterman, "Sonoluminescence: Sound into Light", Scientific American, Feb. 1995, pp. 46-51.
Schaffer, M.J., "Slow Liner Fusion," General Atomics Report GA-A22689, Aug. 1997, in 6 pages.
Siemon, R.E. et al., "Why Magnetized Target Fusion Offers a Low-Cost Development Path for Fusion Energy," in 49 pages, Dec. 1997.
T. E. Markusic et al., "Visualization of Current Sheet Canting in a Pulsed Plasma Accelerator", IEPC-99-206, 26th International Electric Propulsion Conference in Kitakyushu, Japan, Oct. 17-21, 1999, in 8 pages.
T. W. Kornack, "Magnetic Reconnection Studies on SSX", Swarthmore College Department of Physics and Astronomy, Jun. 10, 1998, Swarthmore, PA, USA.
Taleyarkhan et al, "Evidence for Nuclear Emissions During Acoustic Cavitation", Science, Mar. 8, 2002, vol. 295.
Thio, Y.C.F., et al., "Magnetized Target Fusion Driven by Plasma Liners", 2002, in 3 pages.
Thomas S. Duffy et al., "Compressional sound velocity, equation of state, and constitutive response of shock-compressed magnesium oxide", Journal of Geophysical Research, vol. 100, No. B1, pp. 529-542, Jan. 10, 1995.
Tobin, M. T., et al., "The Compact Torus Accelerator, A Driver for ICF," UCRL-93901-R1, Lawrence Livermore National Laboratory, Jul. 31, 1986, in 9 pages.
V. Suponitsky et al., "An Overview of Computational Results at General Fusion Inc. with Focus on Hydrodynamics", Proceedings of CFD Society of Canada Conference, May 2012, in 9 pages.
V. Suponitsky et al., "On the Collapse of a Gas Cavity by an Imploding Molten Lead Shell and Richtmyer-Meshkov Instability", Proceedings of the 20th Annual Conference of the CFD Society of Canada, Canmore, Alberta, Canada, May 9-12, 2012, in 8 pages.
V. Suponitsky et al., "Richtmyer-Meshkov instability of a liquid-gas interface driven by a cylindrical imploding wave", Computers & Fluids, vol. 89, Jan. 20, 2014, in 19 pages.
V.V. Prut et al., "Metallic Z-pinch method: the isentropic compression of hydrogen", JETP Lett. vol. 29, No. 1, Jan. 5, 1979, pp. 30-33.
W. J. Nellis et al., "Equation of state of shock-compressed liquids: Carbon dioxide and air", American Institute of Physics, J. Chem. Phys., vol. 95 (7), Oct. 1, 1991, pp. 5268-5272.
Wurden, G.A. et al., "FRC Plasma Studies on the FRX-L Plasma Injector for MTF", Paper IC/P6-53, 20th IAEA Fusion Energy Conference, Nov. 2004, in 7 pages.
Wurden, G.A. et al., "High Pressure Field Reversed Configuration Plasmas in FRX-L for Magnetized Target Fusion", in 2 pages, Jan. 26, 2006.
Wurden, G.A. et al., "Magnetized Target Fusion: A Burning FRC Plasma in an Imploded Metal Can," J. Plasma Fusion Res. Series, vol. 2, pp. 238-241, Aug. 1999.
Wurden, G.A. et al., "Progress on the FRX-L FRC Plasma Injector at LANL for Magnetized Target Fusion", pp. 1-6, Mar. 1, 2002.
Wurden, G.A., Letter to Dr. Laberge, in 1 page, May 2007.
Xiao, C. et al., "Improved Confinement Induced by Tangential Injection of Compact Torus Into the Saskatchewan Torus-Modified (STOR-M) Tokamak," Phys. Plasmas, vol. 11, No. 8, Aug. 2004, pp. 4041-4049.
Y. C. F. Thio et al., "Magnetized Target Fusion in a Spheroidal Geometry With Standoff Drivers," Fusion Technology 20, 1991, in 22 pages.
Y. C. F. Thio et al., "Pulsed Electromagnetic Acceleration of Plasmas," 38th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit, Jul. 7-10, 2002, in 9 pages.
Y. Mizuno et al., "A Rectangular Pulse Vertical Field Circuit for a Small Tokamak", Electrical Engineering in Japa, vol. 133, No. 4, 2000, Translated from Denki Gakkai Ronbunshi, vol. 119-A, No. 12, Dec. 1999, pp. 1390-1396.
ES2259088T3 (en) 2006-09-16 Controlled fusion in a field reversed configuration and direct energy conversion.

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 Application No. 10738264
 Application No. 2011

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