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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.
“Works”29 pages
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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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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.