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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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are observed. For example, with the device of Figure 3.2b, the input power is about 2
kW with over 1.5 kW being carried out by the jet flow. Consequently, this configuration
provides a way to efficiently convert the energy stored by accelerated ions in the
symmetric microchannels into a directed beam or jet.
Comparison to a Conventional "Plasma" Thruster
The IEC thruster can be viewed as transforming a conventional ion thruster into a
spherical form. In the IEC thruster of Figure 3.2b, ions are produced in the gas
discharge region through the injection and oscillation of electrons about a guide grid
that is held to a slightly positive potential. A second grid extracts ions from the
discharge region and accelerates them towards the center of the device. This type of
ion formation in the IEC has been studied extensively by workers at Nambe Tech, a
"spin-off" company by LANL workers (Reference 3.8). In the case of a planar thruster,
ions are also formed in a discharge region. However, instead of a guide grid, a
magnetic field is used to contain electrons, providing a long path to maximize ionization
collisions. The ion source regions are basically the same, then, for both IEC and planar
ion thrusters, and the extraction/acceleration provided by the grids and the magnetic
fields play equivalent roles in the respective devices. However, the IEC jet thruster
concept must extract a net thrust from the spherical configuration. That is where the
two concepts (planar vs. IEC) diverge, and the star-jet operational mode becomes
essential. The micro-channel formation in the STAR mode acts to maintain and store
the accelerated ions until they are diverted directionally and escape out through the
plasma jet opening. The opening is biased, enabling the control of the potential gradient
between the grid and the opening, hence allowing for increased control of the intensity
of the plasma jet.
The maintenance of STAR mode is then fundamental to the success of IEC jet
operation. Both experimental data and particle-in-cell (PIC) code simulations show that
the energetic ions can be maintained in microchannels for hundreds of passes. The jet
opening allows escape into it in less than ten passes. Consequently, a majority of the
ions, >95 percent, escape at full energy. Thus, the star-jet provides an amazingly good
method to both store and direct the energetic ions.
Overall, the IEC configuration offers distinct advantages. First, the grid structures used
in the IEC thruster are much more open than those used in the conventional planar
thruster designs. When combined with microchannel ion focusing, this prevents ion-grid
collisions, greatly reducing grid erosion and significantly increasing the thruster lifetime.
Second, transforming the device into a sphere makes the overall unit more compact per
unit-ion-source volume, implying a weight reduction advantage. Third, unwanted
neutral propellant gas leakage would be reduced, due to the smaller net opening
required by the high-density jet, vs. a conventional planar thruster having multiple grid
openings. This advantage becomes especially important for thruster applications.
Assuming that the IEC thruster efficiency would be comparable to that of the planar Ion
thruster design, based on these operational improvements, the IEC thruster then offers
significant advantages. [Note that an alternate IEC thruster concept is described later in
the section on J. Khachan's work. It too looks very promising.]
25
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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.