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Defense Intelligence Reference Document Inertial Electrostatic Confinement Fusion

Defense Intelligence Agency · 72 pages · text from the file's own layer

This Defense Intelligence Agency reference document, dated 10 March 2010, covers inertial electrostatic confinement (IEC) fusion. It was produced in FY 2009 under the DIA's Advanced Aerospace Weapon System Applications (AAWSA) program. The report focuses on work at the University of Illinois Urbana-Champaign and reviews IEC basics, experiments, theory and applications such as neutron sources, explosives detection and space propulsion. It concludes by proposing a breakeven experiment for p-11B fusion that uses a hydrogen plasma simulation.

  • p. 5 …Sketch of Two Opposite Limits of the Beam·Maxwellian Equilibrium .. 38 Figure 4.5. The Definition…
  • p. 6 …Comparison of Analytical and Numerical Estimates of Q-Values in a Beam-Dominated Solution -- for a…
  • p. 8 …shows the "Star Mode" discharge where ion beams are created that pass through the grid openings…
  • p. 9 …discussed later where the recirculating ions possess beam-like trajectories passing through the center of the…
  • p. 10 UNCLASSIFIED/ ;raA 8FFIIItliL ~81!! SHL'f beam-like ions. Since electron energy loss processes such as…
  • p. 11 …In addition, its beam-like reactions (highly non-Maxwellian) make the IEC very well suited for…
  • p. 13 …a beam created at the anode and accelerated by the applied cathode voltage; a low-energy…
  • p. 14 …Good convergence is required to achieve optimal beam-beam reactivity scaling for the application that require…
  • p. 15 …The observed loss of convergence with decreasing pressure and increasing current makes achieving significant beam-beam…
  • p. 16 …For a power reactor the objective is to obtain ion beam-beam collisions in this central…
  • p. 17 …the "conventional" beam-like one. A key issue for this concept is how much plasma compression…
  • p. 19 …The main beam observed is a direct path along the injector angle. Other faint light channels…
  • p. 21 …Note that six ion "guns" were used to create a low energy ion beam that entered…
  • p. 22 UNCLASSIFIED/;SflHl 8FFIIItliL ~81!! 8HL'I' was obtained from recirculation beam-beam reactions in a potential…
  • p. 23 …The key physics point is that the beam-beam fusion rate scales as the ion current…
  • p. 26 …Scoping calculations of beam-background fusion rates predict that a 3 He- 3 He reaction product…
  • p. 27 …of the ion density squared scaling for beam-beam reactions. REFERENCES 2.1 R. L. Hirsch…
  • p. 28 …As such, the beam convergence (compression) is limited to lower values, hence lower core densities (an…
  • p. 30 …by the intersection of the multiple ion beams, serves to deflect ions into the escaping jet…
  • p. 31 …The result is the formation of the intense space charge neutralized ion beam (or "plasma jet…
  • p. 32 …in the symmetric microchannels into a directed beam or jet. Comparison to a Conventional "Plasma" Thruster…
  • p. 33 …The ion beams finally exit through an opening in the ground sphere of the IEC device…
  • p. 35 …These devices operate with ~ 80- keV D-ion beams using the non-Maxwellian character of the…
  • p. 36 …Two ion sources inject 40-keV deuterium and helium-3 ion beams toward the center of…
  • p. 37 …Indeed in this case fusion is dominated by beam-beam (non- Maxwellian reactions). Also, the dipole…
  • p. 38 …the center potential and consequently allow incoming beam ions to penetrate into the core region. In…
  • p. 39 …Comparison of Analytical and Numerical Estimates of Q-values in a beam-Dominated Solution -- for a…
  • p. 40 …Hora, "Converging Beam Neutron Source for Driving a Sub-critical Fission Reactor", Proceedings, ICONE 8, CD…
  • p. 41 …Namely, the time scale for collisional degradation of the beam-like ion distribution function is crucial…
  • p. 42 …For example, a tightly focused monoenergetic ion beam is in fact a pessimistic scenario, because different…
  • p. 44 …Thus, weak sinks and strong sources will result in a large beam population, increasing the beam…
  • p. 45 …Sketch of Two Opposite Limits of the Beam-Maxwellian Equilibrium. The solid line corresponds to a…
  • p. 46 …injected beam current, average injection energy, energy spread associated with the velocity component in both parallel…
  • p. 47 …As stated in Section I, the current scaling for beam-beam reactions is strictly 12. However…
  • p. 48 …is very encouraging for formation of deep wells in IEC devices designed for reactors using beam…
  • p. 49 …To do this, it is assumed that the electrostatic confinement equilibrium ion beams are proportional to…
  • p. 50 …When an ion beam is hot, the waves excited by the instability are ion acoustic type…
  • p. 51 …Rider was particularly interested in the claim that due to its beam-like non- Maxwellian plasma…
  • p. 52 …Diagram Showing Equipotential Surfaces of the IEC Cathode Grid and Their Focusing Effect on a Beam…
  • p. 59 …of detectors, the detector configuration, the collimated beam size, the acquisition time, and other scan-related…
  • p. 63 …Alternately, for space propulsion, the proton beam, augmented by injection of heavy atoms to increase the…
  • p. 68 …Due to its inherent non-Maxwellian (beam-like) plasma, the IEC is especially well suited for…
  • p. 70 …This configuration is highly non-Maxwellian due to the beam dominated nature of the trapped ions…
UNCLASSIFIED/;SflHl 8FFIIItliL ~81!! 8HL'I'
was obtained from recirculation beam-beam reactions in a potential well such as in
Figure 2.1 (but without multiple structures). Indeed, to further confirm the existence of
a potential well, Hirsch did both collimated neutron and gamma measures. As shown in
the paper, he found structure for both consistent with well formation. One possible
explanation is that the ion-electron densities obtained were high enough to "burn out"
(completely ionize) the background neutrals in the potential well. There is no direct
evidence to support this view however.
These important results have never been fully explained. Attempts to reproduce his
experiments were done by Gardner and co-workers at Brigham Young University
(Reference 2.1) who borrowed the original device used by Hirsch. However, despite
many months of effort, the neutron production they obtained was significantly lower
than that reported by Hirsch. They attributed this problem to a failure to regain the gun
alignment necessary to have a highly converged plasma "core" in the center of the
device. A major hurdle to this appears to have been that no provision was made to
allow precision alignment of the gun ions entering the device (although the
investigators did not mention this explicitly). Later when Miley reinitiated gun
experiments, his first gun design followed many of the design elements used by Hirsch,
but incorporated electrostatic beam steering. This worked well, but the design was
eventually discarded to move to RF guns with much higher beam currents. In addition,
the gun design of Figure 1.5 uses a magnetic nozzle for reducing the exiting beam
diameter and to allow strong differential pumping (not used in the prior Hirsch
experiments).
It should be stressed again here that the terms "injector" and "gun" are misleading.
The objective is to simply "flow" low energy ions into the device such that they are then
accelerated to fusion energies by either the grid or the virtual electrode structure. Thus,
a loss of "excess" energy after injection is needed trap the ion, i.e. prevent it from
simply passing through the potential well and hitting the opposite wall. A biased
reflector on the opposite wall can be introduced to help prevent this, but this only works
well if the entering ions have little excess energy. To further understand this problem,
the reader is advised to study the design of the Hirsch chamber of Reference 2.2 which
uses an auxiliary biased grid ("reflector") near the wall. Indeed the issue of how to best
introduce ions into the potential well so that their energy falls below that required to
escape the well is a key for proper design of the IEC. In addition to designs to cause an
initial ion energy loss to "drop" them into the potential well, designs with ion sourced
"imbedded" in the well such that ions are born trapped are discussed later.
Gridded devices for near-term applications such as neutron activation analysis (NAA) do
not rely on virtual well potential traps. Rather, the negative bias of the grid forms a
potential trap, and ions are born within the potential trap by ionization collisions in the
internal plasma discharge.
Note that the electron injected case faces the same problem of getting ions into the
potential trap. The approach used with the Polywell employs an embedded ion source
plus relies on "burn out" densities to eliminate neutrals. Success with this technique,
after many problems, was the key that lead to the "breakthrough" reported by R. W.
Bussard (as noted earlier) just before he passed away.
15
UNCLASSIFIED/ ,<EiOA. OFFIIIAL ~!JI! 8HL I

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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 72 pages are in the text index: search them above, or from the library's search.