Documents / Report

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…
UNCLASSIFIED/ ff81il 8ffl&I.t.k Wfili 8Hklf
experimental parameters were obtained. The parameters which were varied include the
background pressure, the ratio of electron to ion circulating currents, the applied
potential difference between the grids, and the inner grid variables such as measured
current, transparency, and construction error. When estimates of each of these
parameters which simulate the ion injection mode experiment were inserted into the
model, the resulting potential profile exhibited no more than a shallow potential well.
This result is consistent with that of beam defection measurements in the ion injection
mode experiments. In spite of these assumptions, the model is extremely valuable in
determining the relative (sensitivity of the potential well profile and depth to effects of
many of the system parameters.
It has been found that for the "medium" level of ion currents under discussion, the
most critical factors which inhibit deep well formation are inadequate spherical focusing
and charge neutralization. The focusing is determined to a great extent by the degree
to which the grids are spherical potential surfaces. The grid must approach a spherical
shape within a few percent before other factors such as grid transparency and
background pressure play an important role. However, as the current is increased, the
requirements for sphericity are somewhat relaxed. For a grid construction error of less
than 5 percent, increasing the grid transparency and decreasing the pressure will also
lead to significant improvement in well depth."
These results were somewhat encouraging. However, they showed that grid
deformation could be very harmful. This deserves several comments. First, the present
author (G. Miley) later showed that design of grids with larger openings provided the
STAR mode where ion beams passed through the center of the openings, avoiding grid
collisions and making sphericity of the grid itself less important. This is important for
small neutron/proton source type devices. However, the assumption of grids fails to
address the question of how a grid could survive in a power reactor or if they could be
eliminated to use a potential well with virtual electrode formation. The use of grids
cannot be completely ruled out for power reactors. Magnetic field protection techniques,
active cooling, etc. are conceivable.
Another question relates to the role of background gas in the IEC. The point is this:
When Miley moved to simplify the device for small neutron sources, he used the
discharge between the grid and vessel to form the ions needed for acceleration and
fusion. This inherently forces use of a modest background neutral gas pressure of the
fuel (typically deuterium) inside the reaction vessel. That in turn results in ion reactions
with the background gas becoming a dominant process in these IECs. Such interaction
includes fusion itself, scattering, charge exchange, etc. This greatly changes the plasma
physics of the IEC as opposed to the ideal of a potential well with "zero" background
pressure. Some key differences in the physics of such IECs were brought out by Tim
Thomson in his experimental study described in Reference 1.4. He noted that: "In
present gridded systems, convergence is not important since beam-target fusion
reaction dominate the reactivity of these devices, as evidenced by the linear scaling of
reactivity of these devices, as evidenced by the linear scaling of reactivity with the
cathode current. In fact, convergence may reduce the reactivity by forming a virtual
anode that limits the central ion density. However, this space charge effect can be
overcome by proper introduction of electrons. Good convergence is required to achieve
optimal beam-beam reactivity scaling for the application that require higher fusion
reaction rates, and the importance of symmetry in determining convergence places a
7
UNCLASSIFIED/;CEiOAt OFFIGIPk IP&'i OIIU{

Not linked to a story yet.

About this file

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.