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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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generation rate is achieved. The net accelerating voltage must be kept within the order
of 1 kV to ensure that the resultant exhaust velocity is in the range of 30,000 m/s (Isp
< 3000 seconds). The mission for a communications satellite is optimized with a
specific impulse in this range. A higher specific impulse would reduce propellant
requirements, but the power requirements and the mass associated with power source
components would increase correspondingly. Xenon is bled into the chamber through
holes at appropriate locations around the wall of the vessel.
Figure 3.3. Illustration of the IEC Jet Thruster Experiment Showing Central Grid and
Two Jet Grids, Opposite to Each Other With On-Off Action
Table 3.1 lists the estimated performance parameters for an IEC electrostatic ion
thruster based on experimental data available to date plus extrapolation of other ion
thruster data. The IEC device will have higher densities and temperatures in the central
core plasma than a conventional thruster, but the increased losses due to
Bremsstrahlung radiation are still negligible when compared to the other power losses.
Thermal radiation losses should be comparable to that in conventional thrusters. The
energy expenditure per ion for conventional ion thrusters and is~ 300 eV per ion. The
energy expenditure per ion for the IEC device has not been established experimentally,
but was estimated in Table 3.1 from simulation studies.
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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.