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Defense Intelligence Reference Document Inertial Electrostatic Confinement Fusion

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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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Section I. IEC Background and Basics
Before considering detail, it is helpful to obtain a rough idea of how inertial electrostatic
confinement (IEC) fusion works.
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Figure 1.1. An UIUC Spherical IEC. The plasma discharge between the grid and vacuum wall creates an ion
source that is extracted and directed towards the center by the highly charged negative grid. A photograph of a
typical !EC chamber is shown in the center. A photograph of the discharge through the view port shows the "Star
Mode" discharge where ion beams are created that pass through the grid openings. This is important for long run
times since 10n bombardment of the grids, hence grid wire sputtering, is m1nim1zed.
For this purpose the experimental IEC device of Figure 1.1 is considered. As shown, this
"gridded" type IEC has a spherical mesh grid suspended on a high voltage feed-through
in the center of a metal vacuum vessel. The fusion "fuel", e.g. deuterium gas, is first
fed into the chamber originally prepared at high vacuum, e.g. 10- 7 Torr. The fuel gas
brings the pressure up into the 10's of Torr region. Then the voltage on the grid is
raised into the many (-) kV range, creating a plasma discharge between the high
voltage grid and chamber wall (electrically grounded). The high negative voltage on the
grid serves to extract the ion from the plasma, accelerating them towards the center of
the grid where in principle they interact and fuse. In practice however, the scattering
cross section is larger than the fusion cross section. Thus many ions scatter without
reacting (fusing). Many "near misses" essentially pass straight through the center of the
plasma core and exit. This dominance of scattering over fusion reactions is the central
issue of all fusion confinement approaches, forcing use of strong confinement so the
ions have many passes and hence a good probability of fusing before being lost from
the fusion reaction chamber. In the IEC multiple passes occur because the ions are
trapped in a potential "well" created by the buildup of positive charge due to the large
flow of the accelerated ions into a small "core" region in the center of the negative grid.
Viewed in another way, the ions extracted from the region between the grid and the
wall can scatter and pass back through the grid, but can only return to the same
potential surface they were born on. Thus they cannot reach the vessel wall, but
instead lose their kinetic energy, stop, and are accelerated by the grid potential back
into the center of the grid. This then provides many "recirculations" through the center
of the grid volume where they have a finite probability of fusing. If not for the existence
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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.