Laser wake-field acceleration (LWFA)-based nuclear fission system and related techniques
A laser wake-field acceleration (LWFA)-based nuclear fission system and related techniques are disclosed. In accordance with some embodiments, the disclosed system may be configured to accelerate charged particles, such as protons, to velocities close to the speed of light utilizing LWFA. The system also may be configured, in accordance with some embodiments, to use these high-energy relativistic charged particles in causing nuclear fission of a given downstream fissionable target, thereby releasing large amounts of harvestable energy. Optionally, the system further may be configured, in accordance with some embodiments, to utilize charged particles resulting from the fission in producing electrical energy.
1. A system comprising:
a laser wake-field accelerator comprising:
at least one laser source configured to produce a laser beam; and
a plasma source configured to produce a plasma;
wherein the laser wake-field accelerator is configured to direct the laser beam to be incident with the plasma to produce a charged particle beam; and
an energy collector configured to collect energy released from nuclear fission of a fissionable target struck by the charged particle beam.
2. The system of claim 1 , wherein the charged particle beam is a proton beam.
3. The system of claim 1 , wherein the charged particle beam has an energy in a GeV range.
4. The system of claim 1 , wherein the energy collector is configured to utilize a magneto-hydrodynamic technique in collecting energy released from the nuclear fission.
5. The system of claim 1 , further comprising an electrical energy generator configured to generate electrical energy utilizing charged particles resulting from the nuclear fission.
6. The system of claim 5 , wherein the electrical energy generator comprises a magnetic structure through which the charged particles pass so as to generate electrical energy.
7. The system of claim 1 , wherein the fissionable target comprises a heavy metal.
8. The system of claim 7 , wherein the fissionable target comprises lead (Pb).
9. The system of claim 1 , wherein the fissionable target comprises either a fissile material or a fertile material and has a k-effective in the range of about 0.05-0.2.
10. The system of claim 1 , wherein the fissionable target comprises either a fissile material or a fertile material and has a k-effective of about 0.2 or less.
11. A method of harvesting energy from a nuclear fission reaction, the method comprising:
generating at least one laser beam;
delivering the at least one laser beam to a plasma so as to generate, via laser wake-field acceleration, a charged particle beam;
delivering the charged particle beam to a fissionable target so as to cause nuclear fission thereof; and
collecting energy released from the nuclear fission of the fissionable target.
12. The method of claim 11 , wherein the charged particle beam is a proton beam.
13. The method of claim 11 , wherein the charged particle beam has an energy in a GeV range.
14. The method of claim 11 , wherein the at least one laser beam is generated by at least one laser source of a laser wake-field accelerator.
15. The method of claim 11 , wherein collecting energy released from the nuclear fission of the fissionable target is performed, at least in part, utilizing at least one energy collector.
16. The method of claim 15 , wherein the energy collector is configured to utilize a magneto-hydrodynamic technique in collecting energy released from the nuclear fission.
17. The method of claim 11 , further comprising:
generating electrical energy utilizing charged particles resulting from the nuclear fission.
18. The method of claim 17 , wherein generating electrical energy is performed, at least in part, utilizing an electrical energy generator.
19. The method of claim 18 , wherein the electrical energy generator comprises a magnetic structure through which the charged particles pass so as to generate electrical energy.
20. The method of claim 11 , wherein the fissionable target comprises a heavy metal.
21. The method of claim 20 , wherein the fissionable target comprises lead (Pb).
22. The method of claim 11 , wherein the fissionable target comprises either a fissile material or a fertile material and has a k-effective in the range of about 0.05-0.2.
23. The method of claim 11 , wherein the fissionable target comprises either a fissile material or a fertile material and has a k-effective of about 0.2 or less.
24. The method of claim 11 , wherein the nuclear fission is caused by striking of the fissionable target via at least one of an electron, a proton, and an ion of the charged particle beam.
25. The method of claim 11 , wherein the charged particle beam is not a gamma radiation or photon beam.
26. The system of claim 1 , wherein the nuclear fission is caused by striking of the fissionable target via at least one of an electron, a proton, and an ion of the charged particle beam.
27. The system of claim 1 , wherein the charged particle beam is not a gamma radiation or photon beam.
28. A system comprising:
a laser wake-field accelerator comprising:
at least one laser source configured to produce a laser beam; and
a plasma source configured to produce a plasma;
wherein the laser wake-field accelerator is configured to direct the laser beam to be incident with the plasma to produce a charged particle beam that has an energy in a GeV range; and
an energy collector configured to collect energy released from nuclear fission of a fissionable target struck by at least one of an electron, a proton, and an ion of the charged particle beam.