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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. 8 …hence a good probability of fusing before being lost from the fusion reaction chamber. In the…
  • p. 11 …If it can, the device would be simpler and smaller than a Tokamak, making it an…
  • p. 14 …However, they showed that grid deformation could be very harmful. This deserves several comments. First, the…
  • p. 15 …Again, this issue will be addressed further later. While earlier workers sought small grid openings designed…
  • p. 17 …More insights will be provided throughout this report, but the reader is encouraged to study the…
  • p. 19 …Upscattering out of the well must be minimized while electron 12 UNCLASSIFIED//EOAt OFFIQI.«1k 11181…
  • p. 29 …It operates by convergence of ions created between the grid and wall onto a small volume…
  • p. 30 …Such thrusters, however, do not scale well to lower powers for small satellites, nor are exhaust…
  • p. 33 …first, the channel grid will be separately hinged with a small servo motor such that its…
  • p. 35 …Thus, the mass of the IEC jet thruster system can potentially be reduced compared to a…
  • p. 43 …More insight into this can be obtained from the distribution functions for trapped ions, sketched in…
  • p. 44 …The source to sink issue noted several times here can be explained as follows. Two opposite…
  • p. 47 …However, since the fusion core radius in these calculations is very small on the order of…
  • p. 49 …instability in finite spherical systems may be excited for small beam velocities compared to those of…
  • p. 50 …However, an experimental study should be performed to verify this result. RIDER - ENERGY BALANCE STUDY Todd…
  • p. 53 …In addition, since both D-D and D- 3He reactions can be used for proton production…
  • p. 54 …This can be viewed as a small scale soft source for individual laboratory studies such as…
  • p. 55 …The 14.1-MeV neutrons from the D-T reaction will be the primary source for…
  • p. 59 …Due to their small size, they can be used in a large array along with TOF…
  • p. 65 …If vis large compared to v11, the effective scattering angle will be large, resulting in retrapping…
  • p. 67 …Fortunately, the IEC can be scaled up in energy gain while keeping a small size since…
  • p. 68 …The small size of the IEC is a key characteristic. If rapid development is to be…
  • p. 71 …In other words, this could also be thought of as a Q=100 DT equivalent breakeven…
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These studies did not yet include differential pumping so that number of recirculation
passes by an ion, [3, was low, roughly 2, due to major charge exchange losses. The
injected ion current, I, with one gun was only ~ 50 mA. Still, based on measurements
of neutrons emitted using deuterium fuel, the Q (fusion energy gain/energy in) was
order of 10·6 which is remarkable for such a small device. These results, plus supporting
computer simulation studies, show that the scale-up of this device to 12 injector guns
plus adding strong differential pumping, could potentially achieve breakeven.
The proposed ion injected IEC device
with 12 guns is shown schematically in
Figure 6.3. The key to achieving
breakeven conditions in this device is to
inject ions with good focus and the
desired angular momentum. The RF ion
gun has a unique magnetic nozzle to
achieve that. Electrons are
simulateously introduced in a measured
fashion. This eliminates the need for a
grid by formation of a deep potential
well (ion trap). Also, differential
pumping between the guns and the
main chamber provides the high
vacuum needed to avoid charge
exchange. This configuration is highly
non-Maxwellian due to the beam
dominated nature of the trapped ions.
Figure 6,2. IEC System With Radio Frequency Ion
Gun
(Although, as pointed out in the disuccion of L. Chacon's work, thermalized ions build
up and additional quasi- Maxwellian distriution in the trap). Still, detailed analysis such
as done by Momota and Kim (discussed earlier) shows that the beam ion momentum
provided sufficient "stiffness" to the system to maintain stability. This assumes,
however, very precise control is maintained over the energy and angular momentum of
injected ions and a balanced supply of electrons is provided. An RF ion injector capable
of such operation has been demonstrated at UIUC as discussed earlier.
Figure 6.3. Multiple Ion Gun Concept
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Figure 6.4. Differentially Pumped RF-Driven Ion
Gun. Six guns shown for simplicity, but twelve are
proposed for the breakeven study.
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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.