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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 …Photo of Center Spot Formation ......................................................... 12 Figure 2.1. The "Historic" Early IEC Ion Injection Experiment…
  • p. 9 …The ideal, however, is the elimination of the grid altogether which can be done via formation…
  • p. 12 …This result was quite negative for electron formation of potential wells, but left the route possibly…
  • p. 14 …most critical factors which inhibit deep well formation are inadequate spherical focusing and charge neutralization. The…
  • p. 18 …The ion formation is done in the high pressure gun discharge region outside of the chamber…
  • p. 19 …Photo of Center Spot Formation. The main beam observed is a direct path along the injector…
  • p. 20 …Klevans, "Theory of Potential-Well Formation in an Electrostatic Confinement Device", J. of Appl. Phys., Vol…
  • p. 22 …As shown in the paper, he found structure for both consistent with well formation. One possible…
  • p. 30 …However, to date, formation of the jet has only been studied under steady-state operation. 23…
  • p. 31 …The result is the formation of the intense space charge neutralized ion beam (or "plasma jet…
  • p. 32 …This type of ion formation in the IEC has been studied extensively by workers at Nambe…
  • p. 35 …The approach being pursued at UIUC is the formation of deep potential wells with angular ion…
  • p. 45 …considered well formation with emphasis on angular momentum effects (Reference 4.4). Earlier studies had assumed…
  • p. 48 …is very encouraging for formation of deep wells in IEC devices designed for reactors using beam…
  • p. 49 …Krylov algorithm that does not require actual formation and storage of the Jacobian matrix to minimize…
  • p. 69 …While very demanding, plasma simulations show that carefully controlled injection can provide the potential well formation…
  • p. 70 …This eliminates the need for a grid by formation of a deep potential well (ion trap…
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The corresponding ion density profile, shown in Figure 4.8, has a high value inside the
virtual cathode (center core plasma) and also a peak in front of the grid (real cathode).
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Radios [ml Radius [m]
Figure 4.7. The Double Well Potential Calculated With Figure 4.8. Ion Density Profile for Potential
IXL Code for di3perp, i=I4keV, l;=SSA, Ie=S9A Well Shown in Figure 4.7
An important new insight obtained in
the study revealed that these potential
profiles create ion density distribution
functions completely different from the
ones observed when a single well
electrostatic potential exists. Two ion
density peaks were commonly observed
- one in the central IEC core region, and
one near the cathode wire grid as seen
in Figure 4.8. In this manner, the single
ion peak created by the single well
potential is split into two peaks. The
central ion peak has a much smaller
radius than the original peak. This
causes higher ion densities to occur in
the central potential well, which is
essential for the achievement of high
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Figure 4.9. The D-D Fusion Reac:::tion Rate Versus
Cathode Current for dEperp,1 = 8 keV
fusion rates. However, since the fusion core radius in these calculations is very small
on the order of 0.4 cm - 0.9 cm, the total number of neutrons emitted per second is too
low to create useful fusion power (see Figure 4.9). Still, the physics principles
illustrated provide important insight into injection issues.
A reduced angular momentum spread and higher injection energies would be required
to correct the well volume problem. Still, the D-D fusion rate scaling of 15 is
encouraging, and it is indeed surprising that this large angular momentum spread
achieves such distinct double well structures. As stated in Section I, the current scaling
for beam-beam reactions is strictly 12. However, as shown by Tzonev et al., nonlinear
changes in the potential well shape and ion density profile combine to cause the higher
power current scaling law. It would be anticipated, however, that this effect would
saturate at some current, tending back to the fundamental 12 relation. Along these
lines, it should be noted that prior investigators also predicted scaling laws with
40
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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.