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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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There are several advantages of the dipole-assisted IEC. By applying the desired
voltage to the cathode grid, high-energy ions are easily obtained, hence plasma heating
is straightforward. Indeed in this case fusion is dominated by beam-beam (non-
Maxwellian reactions). Also, the dipole magnet at the center of the device produces
field lines that trap ions and compresses them within the inner radius of the dipole.
Thus, a very high ion density can be achieved leading to high reaction rates via beam-
beam fusion. Biasing the dipole magnet to the same potential as the cathode grid
solves the problem of space charge build-up due to the high ion density at the center of
Da!EC.
DAIEC EXPERIMENTS
The purpose of current experiments is to investigate the focusing effect of a dipole
magnetic field in a spherical IEC. In particular, the primary goal is to measure the
increase in plasma densities achieved by a dipole-assisted IEC. In theory, the
introduction of a current ring or dipole coil into the base configuration would focus
particles into the center of the dipole, increasing the plasma density at the core of the
device. A schematic of the current experimental setup is shown in Figure 3.5.
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Figure 3.5. (a} Dipole Magnetic Field and (b} Layout of Devices
This experiment employs two split spherical grids as shown in Figure 3.5. Ions are
created in the discharge between these grids and the vessel wall. They are extracted
and accelerated by the grid potential so they pass through the dipole field of Figure
3.Sa. Experiments have confirmed that an order of magnitude density increase (vs. no
dipole present) can be achieved in the center region. A double Langmuir probe is
inserted at various positions throughout the center region.
The use of a bias on the dipole magnet structure to control space charge build-up was
also studied. In an ion-injected IEC partial space-charge neutralization at the core
30
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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.