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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. 8 …hence a good probability of fusing before being lost from the fusion reaction chamber. In the…
  • p. 11 …If it can, the device would be simpler and smaller than a Tokamak, making it an…
  • p. 14 …However, they showed that grid deformation could be very harmful. This deserves several comments. First, the…
  • p. 15 …Again, this issue will be addressed further later. While earlier workers sought small grid openings designed…
  • p. 17 …More insights will be provided throughout this report, but the reader is encouraged to study the…
  • p. 19 …Upscattering out of the well must be minimized while electron 12 UNCLASSIFIED//EOAt OFFIQI.«1k 11181…
  • p. 29 …It operates by convergence of ions created between the grid and wall onto a small volume…
  • p. 30 …Such thrusters, however, do not scale well to lower powers for small satellites, nor are exhaust…
  • p. 33 …first, the channel grid will be separately hinged with a small servo motor such that its…
  • p. 35 …Thus, the mass of the IEC jet thruster system can potentially be reduced compared to a…
  • p. 43 …More insight into this can be obtained from the distribution functions for trapped ions, sketched in…
  • p. 44 …The source to sink issue noted several times here can be explained as follows. Two opposite…
  • p. 47 …However, since the fusion core radius in these calculations is very small on the order of…
  • p. 49 …instability in finite spherical systems may be excited for small beam velocities compared to those of…
  • p. 50 …However, an experimental study should be performed to verify this result. RIDER - ENERGY BALANCE STUDY Todd…
  • p. 53 …In addition, since both D-D and D- 3He reactions can be used for proton production…
  • p. 54 …This can be viewed as a small scale soft source for individual laboratory studies such as…
  • p. 55 …The 14.1-MeV neutrons from the D-T reaction will be the primary source for…
  • p. 59 …Due to their small size, they can be used in a large array along with TOF…
  • p. 65 …If vis large compared to v11, the effective scattering angle will be large, resulting in retrapping…
  • p. 67 …Fortunately, the IEC can be scaled up in energy gain while keeping a small size since…
  • p. 68 …The small size of the IEC is a key characteristic. If rapid development is to be…
  • p. 71 …In other words, this could also be thought of as a Q=100 DT equivalent breakeven…
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Figure 3.1. Two Types of Cylindrical IECs. The hollow cathode on the left (often termed the C-Device) and the
2-D gridded version on the right, often Just called "the" cylindrical IEC.
The hollow cathode "C-Device" of Figure 3.1 has an insulated vacuum chamber with an
alternating series of hollow cylindrical cathodes and anodes spaced along a common
longitudinal axis. Biased end plates serve as charged particles "reflectors". The anodes,
cathodes and end plates are biased to steady state and/or pulsed voltages, depending
on the operational mode. This configuration is used to initiate a plasma discharge,
resulting in electrostatic confinement of fusion fuel ions in both the axial and radial
directions (Reference 3.4). Present operation produces about 107 n/s (D-D) steady
state while for pulsed output 10 9 n/s (D-D) is obtained.
In "the" cylindrical version 2-D IEC (Figure 3.1), a cylindrical cathode grid is placed with
its axis concentric with the axis of the surrounding vacuum vessel. This is then, in
effect, a 2-D version of the spherical IEC. It operates by convergence of ions created
between the grid and wall onto a small volume along the axis, hence has sometimes
been called the "Radial Converging IEC (RC-IEC)". As already noted, the basic physics
of this version was originally studied in pioneering work by T. Dolan in 1970. However,
the concept lay dormant until revised and upgraded several decades later with
improved grid designs for neutron production by UIUC workers.
ELECTRICALLY-DRIVEN IEC JET THRUSTER
The use of an IEC design for space propulsion was originally proposed by R.W. Bussard
(Reference 3.6). (His concept was for a high thrust scram jet device. While very
attractive, this concept (and Miley et al.'s "Spaceship I & II concepts discussed later)
are for far-term use. Here we discuss near-term electronically driven IEC designed for
space applications. In this case, electrical power would come from a solar panel.
The IEC jet thruster is intended as an ultra-maneuverable space thruster for satellite
and small probe thrust operations. The IEC Jet design potential offers a unique
capability to cover a wide range of powers (few Watts to Kilowatts) with good efficiency
while providing a plasma jet that can start with a large diameter but be narrowed
directionally to focus on targets. The IEC thruster uses a spherical configuration,
wherein ions are generated and accelerated towards the center of a spherical vacuum
chamber. A virtual cathode forms in the high-density central core region, and combined
with a locally distorted cathode grid potential field, extracts accelerated ions into an
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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.