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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…
UNCLASSIFIED/ ;'f81il 8ffllltlit '11815 8HLV
Figure 4 is a schematic sketch of the ion injectors shown in Figure 6.3. A key
component is the magnetic focusing lens at the gun extraction port. This allows very
efficient differential pumping between the high pressure gun chamber and the low
pressure IEC chamber and provides focus control. This experiment will involve very
high power inputs (about a MW). To avoid excessive power supply and thermal
controls, a Marx bank pulsed power input with peak powers of~ 1 MW over 1 msec at
0.01 Hz will be used. Pulsed experiments with equivalent power inputs on one gun have
already been performed successfully. The pulse length is set long enough to provide
quasi equilibrium physics conditions in the trapped plasma during the "flat top" region
of the pulse". Thus the data obtained is relevant to eventful steady-state reactors
where the internal fusion power production alleviates the input power supply
requirement.
The energy gain (Q) scaling for such a device goes as ~I/a 2 where a is the radius of the
dense core spot formed in the IEC sphere, ~ is the number of ion recirculations in the
trap before the ion is lost, and I is the ion injected current. The 12 gun breakeven
design will provide an increase in ~ to ~ 1000 due to differential pumping effects, I will
increase to 6000 mA (due to multiple pulsed guns), and a will be cut down by 10 due to
improvements in focusing both and reduced collisionality. This predicts an increase in Q
(compared to prior gun experiment) of ~108 , giving Q=l ("breakeven") as required for
a p- 11B plasma (as noted earlier, this breakeven Q assumes a Lawson breakeven
confinement parameter of nT that exceeds the DT requirement by a factor of 100. In
other words, this could also be thought of as a Q=100 DT equivalent breakeven!) Such
an experiment would provide a physics proof-of-principle for this ion injected IEC
concept and provide the base for extending this configuration on to a power-producing
plant.
To accomplish this result quickly on a modest budget, we need to simplify the work by
avoiding the need to develop new injection technology for hydrogen-boron fuel plus
avoid the need to handle the fusion energy produced. Thus we propose to confirm the
achievement of breakeven conditions using a hydrogen plasma and diagnostics to show
that the nT and T corresponding to Q = 1 (p- 11 B) are obtained. (An alternate approach
might be to use deuterium as is done in present IEC neutron source studies. However,
that would require a massive shielding and other access restrictions for the neuron flux
levels). Modern plasma diagnostics can make quite precise measurement of the plasma
conditions needed for the confirmation, so the hydrogen equivalent approach is
recommended.
CONCLUDING REMARKS
Once achieved in hydrogen, these conditions could be fairly quickly confirmed with p-
11 B fuel in later experiments once the needed fuel handling system is added. Thus the
proposed hydrogen simulation of p- 11B breakthrough conditions would be a landmark
achievement, leading the way to rapid deployment of the technology needed to build
small fusion power plants. The technology development needed to proceed largely
involves the design and engineering of subsystems for the balance-of-plant (BOP).
Many of these can employ conventional equipment, but several require new
developments. These include the hydrogen-boron fuel injection system, the direct
energy conversion system to convert the charged particle product energy to electricity,
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UNCLASSIFIED/ /f81il 8ffIIIAL l!lliEii SU.bit

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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.