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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 …at 25mtorr, 20mA 31 Figure 4.1. Cross Section of the Experimental Layout of the PFX…
  • p. 6 …p- 11B Fusion Cross Section Energy Requirements ............................... 62 Figure 6.2. IEC System With Radio Frequency…
  • p. 8 …In practice however, the scattering cross section is larger than the fusion cross section. Thus many…
  • p. 9 …on the fuel via the selection of cross sections in the derivation. Magnetic confinement is generally…
  • p. 26 …near the peak energy of the fusion cross section. Thus this issue deserves more study to…
  • p. 27 …can provide valuable data regarding 3He fusion cross sections at "low" energies with better counting statistics…
  • p. 33 …the plasma to expand giving a broad cross section beam. Experimental Jet Design and Performance Figure…
  • p. 41 …it suffers from several Figure 4.1. Cross Section of the Experimental Layout of the PFX…
  • p. 52 …D2+ ions have a smaller CX cross section and it takes about 20 passes for most…
  • p. 65 …point, the vector direction they assume in crossing the null is random. The result then can…
  • p. 68 …the peak of the p- 11 B cross section. In contrast, in Maxwellian-type plasmas typical…
  • p. 69 …p- 11 B Fusion Cross Section Energy Requirements. The p-"B reaction rate approaches that of…
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Section II. Select Experiments
In this section some select experiments are briefly reviewed with the main focus on ion-
injected IECs. Beginning with the early Hirsch gun injected IEC experiments that are
important both historically and from a physics perspective. Other experiments aimed at
"spin-off" applications are then covered, followed by a discussion of several recent gun
injection type studies. Readers interested in more detail should consult references.
In Reference 2.1, Robert Hirsh disclosed experimental results with very high D-T
neutron rates from an ion-injected IEC shown if Figure 2.1.
Note that six ion "guns" were used to create a low energy ion beam that entered the
chamber and was trapped via electrostatic structures to form the potential well
structure desired for IEC operation. However, differential pumping was not used so
beam-background and charge-exchange collision must have still played a significant
role in this experiment. Still Hirsch obtained "record" neutron rates for DT fusion shown
in Figure 2.2.
ROBERT L. Hl~SCl!
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Figure 2.1. The "Historic" Early IEC Ion Injection
Experiment of R. Hirsch Working With Philo
Farnsworth
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w
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t DJ7.8 IJ.1CRONS
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Figure 2.2. Neutron Rates Measured With the IEC of
Figure 2.1 Exceeded 109 DT n/s at 150 kV. For
perspective, note that, as discussed later, UIUC IEC gridded
devices routinely produce 108 DD n/s at ~ 80 kV. This is
slightly above Hirsch's result but uses higher ion currents.
The key point about this remarkable result is that the neutron production rates are well
about that predicted by simple beam-background fusion reactions, implying that benefit
14
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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.