Physics:Magnetized liner inertial fusion

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Short description: Method of producing controlled nuclear fusion
The MagLIF concept
MagLIF basic idea

Magnetized liner inertial fusion (MagLIF) is an emerging method of producing controlled nuclear fusion. It is part of the broad category of inertial fusion energy (IFE) systems, which drives the inward movement of fusion fuel, thereby compressing it to reach densities and temperatures where fusion reactions occur. Previous IFE experiments used laser drivers to reach these conditions, whereas MagLIF uses a combination of lasers for heating and Z-pinch for compression. A variety of theoretical considerations suggest such a system will reach the required conditions for fusion with a machine of significantly less complexity than the pure-laser approach. There are currently at least two facilities testing feasibility of the MagLIF concept, the Z-machine at Sandia Labs in the US and Primary Test Stand (PTS) located in Mianyang, China.[1]

Description

MagLIF is a method of generating energy by using a 100 nanosecond pulse of electricity to create an intense Z-pinch magnetic field that inwardly crushes a fuel filled cylindrical metal liner (a hohlraum) through which the electric pulse runs. Just before the cylinder implodes, a laser is used to preheat fusion fuel (such as deuterium–tritium) that is held within the cylinder and contained by a magnetic field. Sandia National Labs is currently exploring the potential for this method to generate energy by utilizing the Z machine.

MagLIF has characteristics of both inertial confinement fusion (due to the usage of a laser and pulsed compression) and magnetic confinement (due to the utilization of a powerful magnetic field to inhibit thermal conduction and contain the plasma). In results published in 2012, a LASNEX based computer simulation of a 70 megaampere facility showed the prospect of a spectacular energy return of 1000 times the expended energy. A 60 MA facility would produce a 100× yield. The currently available facility at Sandia, Z machine, is capable of 27 MA and may be capable of producing slightly more than breakeven energy while helping to validate the computer simulations.[2] The Z-machine conducted MagLIF experiments in November 2013 with a view towards breakeven experiments using D–T fuel in 2018.[3]

Sandia Labs planned to proceed to ignition experiments after establishing the following:[4]

  1. That the liner will not break apart too quickly under the intense energy. This has been apparently confirmed by recent experiments. This hurdle was the biggest concern regarding MagLIF following its initial proposal.
  2. That laser preheating is able to correctly heat the fuel—to be confirmed by experiments starting in December 2012.
  3. That magnetic fields generated by a pair of coils above and below the hohlraum can serve to trap the preheated fusion fuel and importantly inhibit thermal conduction without causing the target to buckle prematurely—to be confirmed by experiments starting in December 2012.

Following these experiments, an integrated test started in November 2013. The test yielded about 1010 high-energy neutrons.

As of November 2013, the facility at Sandia labs had the following capabilities:[3][5]

  1. 10 tesla magnetic field
  2. 2 kJ laser
  3. 16 MA
  4. D–D fuel

In 2014, the test yielded up to 2×1012 D–D neutrons under the following conditions:[6]

  1. 10 tesla magnetic field
  2. 2.5 kJ laser
  3. 19 MA
  4. D–D fuel

Experiments aiming for energy breakeven with D-T fuel were expected to occur in 2018.[7]
To achieve scientific breakeven, the facility is going through a 5-year upgrade to:

  1. 30 teslas
  2. 8 kJ laser
  3. 27 MA
  4. D–T fuel handling[3]

In 2019, after encountering significant problems related to mixing of imploding foil with fuel and helical instability of plasma,[8] the tests yielded up to 3.2×1012 neutrons under the following conditions:[9]

  1. 1.2 kJ laser
  2. 18 MA

In 2020, "the burn-averaged ion temperature doubled to 3.1 keV and the primary deuterium–deuterium neutron yield increased by more than an order of magnitude to 1.1×1013 (2 kJ deuterium–tritium equivalent) through a simultaneous increase in the applied magnetic field (from 10.4 to 15.9 T), laser preheat energy (from 0.46 to 1.2 kJ), and current coupling (from 16 to 20 MA)."[10]

See also

References

  1. ↑ Hailong, Zhao (12 May 2020). "Preliminary exploration of MagLIF concept and feasibility analysis on PTS facility". High Power Laser and Particle Beams 32 (6): 62002–62010. doi:10.11884/HPLPB202032.190352. https://www.hplpb.com.cn/en/article/doi/10.11884/HPLPB202032.190352. 
  2. ↑ Slutz, Stephen; Roger A. Vesey (12 January 2012). "High-Gain Magnetized Inertial Fusion". Physical Review Letters 108 (2): 025003. doi:10.1103/PhysRevLett.108.025003. PMID 22324693. Bibcode: 2012PhRvL.108b5003S. 
  3. ↑ 3.0 3.1 3.2 Gibbs WW (2014). "Triple-threat method sparks hope for fusion". Nature 505 (7481): 9–10. doi:10.1038/505009a. PMID 24380935. Bibcode: 2014Natur.505....9G. 
  4. ↑ "Dry-Run Experiments Verify Key Aspect of Nuclear Fusion Concept: Scientific 'Break-Even' or Better Is Near-Term Goal". http://www.sciencedaily.com/releases/2012/09/120917124210.htm. 
  5. ↑ Ryan, McBride. "Magnetized LIF and Cylindrical Dynamic Materials Properties Experiments on Z". Krell Institute. https://www.youtube.com/watch?v=gBtu8S9vAtY. 
  6. ↑ Gomez, M. R.. "Experimental Verification of the Magnetized Liner Inertial Fusion (MagLIF) Concept". Krell Institute. http://www.krellinst.org/ssgf/conf/2014/video/mgomez. 
  7. ↑ Cuneo, M.E. (2012). "Magnetically Driven Implosions for Inertial Confinement Fusion at Sandia National Laboratories". IEEE Transactions on Plasma Science 40 (12): 3222–3245. doi:10.1109/TPS.2012.2223488. Bibcode: 2012ITPS...40.3222C. 
  8. ↑ Seyler, C.E.; Martin, M.R.; Hamlin, N.D. (2018). "Helical instability in MagLIF due to axial flux compression by low-density plasma". Physics of Plasmas (Physics of Plasmas 25, 062711 (2018)) 25 (6): 062711. doi:10.1063/1.5028365. Bibcode: 2018PhPl...25f2711S. https://www.osti.gov/biblio/1456307. 
  9. ↑ Gomez, M. R. (2019). "Assessing Stagnation Conditions and Identifying Trends in Magnetized Liner Inertial Fusion". IEEE Transactions on Plasma Science (IEEE Transactions on Plasma Science vol. 47/5) 47 (5): 2081–2101. doi:10.1109/TPS.2019.2893517. Bibcode: 2019ITPS...47.2081G. 
  10. ↑ Gomez, M. R. (2020). "Performance Scaling in Magnetized Liner Inertial Fusion Experiments". Phys. Rev. Lett. (American Physical Society) 125 (15): 155002. doi:10.1103/PhysRevLett.125.155002. PMID 33095639. Bibcode: 2020PhRvL.125o5002G. 



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