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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 …Sketch of Two Opposite Limits of the Beam·Maxwellian Equilibrium .. 38 Figure 4.5. The Definition…
  • p. 6 …Comparison of Analytical and Numerical Estimates of Q-Values in a Beam-Dominated Solution -- for a…
  • p. 8 …shows the "Star Mode" discharge where ion beams are created that pass through the grid openings…
  • p. 9 …discussed later where the recirculating ions possess beam-like trajectories passing through the center of the…
  • p. 10 UNCLASSIFIED/ ;raA 8FFIIItliL ~81!! SHL'f beam-like ions. Since electron energy loss processes such as…
  • p. 11 …In addition, its beam-like reactions (highly non-Maxwellian) make the IEC very well suited for…
  • p. 13 …a beam created at the anode and accelerated by the applied cathode voltage; a low-energy…
  • p. 14 …Good convergence is required to achieve optimal beam-beam reactivity scaling for the application that require…
  • p. 15 …The observed loss of convergence with decreasing pressure and increasing current makes achieving significant beam-beam…
  • p. 16 …For a power reactor the objective is to obtain ion beam-beam collisions in this central…
  • p. 17 …the "conventional" beam-like one. A key issue for this concept is how much plasma compression…
  • p. 19 …The main beam observed is a direct path along the injector angle. Other faint light channels…
  • p. 21 …Note that six ion "guns" were used to create a low energy ion beam that entered…
  • p. 22 UNCLASSIFIED/;SflHl 8FFIIItliL ~81!! 8HL'I' was obtained from recirculation beam-beam reactions in a potential…
  • p. 23 …The key physics point is that the beam-beam fusion rate scales as the ion current…
  • p. 26 …Scoping calculations of beam-background fusion rates predict that a 3 He- 3 He reaction product…
  • p. 27 …of the ion density squared scaling for beam-beam reactions. REFERENCES 2.1 R. L. Hirsch…
  • p. 28 …As such, the beam convergence (compression) is limited to lower values, hence lower core densities (an…
  • p. 30 …by the intersection of the multiple ion beams, serves to deflect ions into the escaping jet…
  • p. 31 …The result is the formation of the intense space charge neutralized ion beam (or "plasma jet…
  • p. 32 …in the symmetric microchannels into a directed beam or jet. Comparison to a Conventional "Plasma" Thruster…
  • p. 33 …The ion beams finally exit through an opening in the ground sphere of the IEC device…
  • p. 35 …These devices operate with ~ 80- keV D-ion beams using the non-Maxwellian character of the…
  • p. 36 …Two ion sources inject 40-keV deuterium and helium-3 ion beams toward the center of…
  • p. 37 …Indeed in this case fusion is dominated by beam-beam (non- Maxwellian reactions). Also, the dipole…
  • p. 38 …the center potential and consequently allow incoming beam ions to penetrate into the core region. In…
  • p. 39 …Comparison of Analytical and Numerical Estimates of Q-values in a beam-Dominated Solution -- for a…
  • p. 40 …Hora, "Converging Beam Neutron Source for Driving a Sub-critical Fission Reactor", Proceedings, ICONE 8, CD…
  • p. 41 …Namely, the time scale for collisional degradation of the beam-like ion distribution function is crucial…
  • p. 42 …For example, a tightly focused monoenergetic ion beam is in fact a pessimistic scenario, because different…
  • p. 44 …Thus, weak sinks and strong sources will result in a large beam population, increasing the beam…
  • p. 45 …Sketch of Two Opposite Limits of the Beam-Maxwellian Equilibrium. The solid line corresponds to a…
  • p. 46 …injected beam current, average injection energy, energy spread associated with the velocity component in both parallel…
  • p. 47 …As stated in Section I, the current scaling for beam-beam reactions is strictly 12. However…
  • p. 48 …is very encouraging for formation of deep wells in IEC devices designed for reactors using beam…
  • p. 49 …To do this, it is assumed that the electrostatic confinement equilibrium ion beams are proportional to…
  • p. 50 …When an ion beam is hot, the waves excited by the instability are ion acoustic type…
  • p. 51 …Rider was particularly interested in the claim that due to its beam-like non- Maxwellian plasma…
  • p. 52 …Diagram Showing Equipotential Surfaces of the IEC Cathode Grid and Their Focusing Effect on a Beam…
  • p. 59 …of detectors, the detector configuration, the collimated beam size, the acquisition time, and other scan-related…
  • p. 63 …Alternately, for space propulsion, the proton beam, augmented by injection of heavy atoms to increase the…
  • p. 68 …Due to its inherent non-Maxwellian (beam-like) plasma, the IEC is especially well suited for…
  • p. 70 …This configuration is highly non-Maxwellian due to the beam dominated nature of the trapped ions…
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intense quasi-neutral ion jet. The configuration, low gas leakage, and good heat
removal make it possible to scale the design to either low powers or high powers,
covering a range of interest for present small satellites on to future medium and large
satellites. In addition to maneuverable thrusting, the jet channel extraction technique
enables directing and focusing the plasma stream down on an asteroid or other object
for interrogation of it. Analysis of the plasma emission spectra would provide an
identification of the materials and surface features of the object. With further
development the IEC system potentially offers an attractive fusion power source.
Another advantage of the IEC jet thruster is that it provides a step towards a future p-
11 B IEC power source and/or thruster for satellite operations. This possibility is also
briefly discussed here.
Relation to Other Prior Thrusters
NASA and other laboratories have worked toward developing advanced Hall Thrusters
for future satellite applications. Such thrusters, however, do not scale well to lower
powers for small satellites, nor are exhaust plasma modifications possible to provide
fast maneuverability. The IEC-jet thruster appears uniquely able to address both issues.
Conventional plasma thrusters such as the Hall thruster have undergone much more
experimental study than the IEC-jet thruster. However, the simplicity of the IEC-Jet
thruster design and its thermal scalability makes it feasible to quickly develop and test,
making the lack of data base less of a liability.
In the jet thruster concept the plasma target at the center of the chamber, created by
the intersection of the multiple ion beams, serves to deflect ions into the escaping jet
plasma. The resulting virtual anode, in combination with curved potential lines created
by the cathode grid diverts ions, forming a strong plasma jet. This is channeled out
through an enlarged hole and guide structure in the grid (Figure 3.2). This design
promises a good efficiency and thrust while providing a low weight, and due to the very
open accelerator grid structure, a very long lifetime. Thus it provides a good thruster
for basic satellite operations and with the added jet control/focusing also provides
maneuverability.
In addition the IEC jet offers two added features that increase its potential effectiveness
for probing various space objects. The fact that the IEC jet can be controlled to form
over multiple areas around the sphere would allow the platform to maneuver itself close
to a target and then simply open a second jet offset 180 degrees from the propulsive
one. The second jet would serve the integration purpose of the platform without having
to expend time or additional resources such as fuel to reorient itself to direct the plume
at the target. Other current systems, such as Hall thrusters, would first have to position
itself close to the target, and then reorient such that the exhaust plume is properly
oriented. Thus, the IEC jet thruster would not be subject to expending the resources of
time and fuel that other platforms require. Another option for the IEC jet thruster is to
operate as a pulsed device. This becomes especially important when considering how
long it may take to disable a defensive target (the platform's impulse time to disable).
The use of an intense pulsed jet could disable the target before it has time to maneuver
or apply defensive layers. As discussed later, the basic IEC has been operated
experimentally in a pulsed mode using a capacitive power unit. However, to date,
formation of the jet has only been studied under steady-state operation.
23
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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.