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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 …This is important for long run times since 10n bombardment of the grids, hence grid wire…
  • p. 9 …This time can be restated in terms of the number of ion recirculations in the IEC…
  • p. 15 …This work and others on the small gridded systems at that time showed several important problems…
  • p. 17 …interesting concept is the idea of ion focusing, either in space or time, or some other…
  • p. 18 …confinement time for aneutronic fusion. This assumes, however, very precise control is maintained over the energy…
  • p. 23 …By selecting the pulse width to match or exceed the ion confinement time, typically order of…
  • p. 27 …This is the approach used at the UIUC. However, introduction of the source into the configuration…
  • p. 30 …The second jet would serve the integration purpose of the platform without having to expend time…
  • p. 35 …The issue then is how to achieve adequate confinement times. The approach being pursued at UIUC…
  • p. 36 …step in a timely fashion, however. The Dipole Assisted IEC (DaIEC) The dipole assisted IEC DaIEC…
  • p. 38 …in the current experiment. It is found that electron density increases about 17 times more than…
  • p. 41 …Namely, the time scale for collisional degradation of the beam-like ion distribution function is crucial…
  • p. 42 …would homogenize the speed within the ion beam a~er some time, making the speed difference…
  • p. 43 …1) The electrostatic well is deep enough (Eo > 100 kV); 2) Ion confinement time is long…
  • p. 44 …The source to sink issue noted several times here can be explained as follows. Two opposite…
  • p. 49 …The time convergence test suggests that employing the largest time step compatible with accuracy in a…
  • p. 50 …When an ion beam is hot, the waves excited by the instability are ion acoustic type…
  • p. 51 …used an analytical model of charge- exchange collisions in the IEC plasma to include ion time…
  • p. 53 …Nevins, Can inertial electrostatic confinement work beyond the ion-ion collisional time scale?" Phys. Plasmas, Vol…
  • p. 54 …This method uses a pulsed high-energy neutron source and the time-of-flight (TOF) diagnostics…
  • p. 57 …The longer the charge time, the higher the charge in the energy storage capacitor bank and…
  • p. 58 …The challenge in these systems is that the unloading time is short and the container is…
  • p. 59 …by the number of detectors, the detector configuration, the collimated beam size, the acquisition time, and…
  • p. 62 …The Tokamak has a shorter trip time by employing a power level that is six times…
  • p. 63 …In this fashion, an array of multiple IECs increase the overall confinement time roughly in proportion…
  • p. 64 …This recirculation significantly increases the confinement time verses that of a simple cusp devise, leading to…
  • p. 65 …This re-trapping greatly increases the confinement time of a MCSA fusion device. 58 UNCLASSIFIED/;CEiOAt…
  • p. 66 …in the IEC high power-to-weight of the MCSA enables fast trip times. The concept…
  • p. 67 …across the outer surface, so increased confinement times have been achieved by going to the massively…
  • p. 68 …Here n is the ion density and Tis the ion confinement time. Assuming the converged core…
  • p. 69 …A specially designed radio frequency (RF) ion gun is installed on the side of the chamber…
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Table 5.2. Comparison of IEC Design and Magnetic Fusion Design
Fu~ion Ship I Fu~ion Ship [I Spherical Tokamak
Overall Mass r,Metric T_) \Oil \IKJ ln911
Overall 1.en_grh (ml 174 .11KJ 2411
\umher ot crew 111 111 6- 12
Thrust Power rMWJ Xn 7511 48311
Reactor gain 4 9 7.1
Reactor p<iwer (MW J 2% 217X 7X95
'l'hru~t ~y~tem Krypton ion Argon ion 11 1 - magnetic nozzle
Specific impulse (sec.) ln,IKil l\lKil 15,435
Jupiter one way trip time (day.\J 41!1 2111 I IX
The design of Space Ship II uses "coupled" IEC reactors that use magnetic guide
channels. This concept, termed the Magnetically-Channeled Spherical IEC Array (MCSA)
concept is briefly discussed next (Reference 5.3).
MAGNETICALLY-CHANNELED SPHERICAL IEC ARRAY {MCSA}
CONCEPT
The Magnetically-Channeled Spherical IEC Array (MCSA) concept for a hybrid magnetic
assisted spherical IEC configuration maintains the basic ion-injected IEC reactor
configuration but adds magnetic channels for coupling exhaust plasma and reaction
products. The MCSA is illustrated conceptually in Figure 5.7. The SIEC is confined in a
hexapole field configuration is quite different from the hexapole field used in R.W.
Bussard's Polywell. It is in turn located in a field channel (Bz field) created by a column
of Helmholtz coils. The field strengths of these coil sets is adjusted such that the fields
cancel in the center of the IEC, giving a larger field null region compared to that in a
cusp confined field. The MCSA configuration retains the advantage of stability due to
good field curvature obtained in a cusp. In addition, it also effectively closes the "belt"
loss cone. As shown later, leakage in that direction is led around the hexapole coils and
back into the confinement region, termed here as "recirculation." Losses include
scattering into the spindal loss cone along the z-axis and stochastic scattering due to
the violation of adiabatic invariance in the field null region. However, with the present
channel configuration, the axial losses from one IEC configuration enter a neighboring
unit. Thus, as they pass through the field null region in that unit, stochastic scattering
leads to "retrapping" of much of this flow. Experimental verification of this "retrapping"
is then a second physics Proof-of-Principle (POP) objective. In this fashion, an array of
multiple IECs increase the overall confinement time roughly in proportion to the number
of units. In operation, electrons would be magnetically confined as described, providing
electrostatic confinement of ions injected into the Spherical IEC region. An additional
benefit of this configuration is that in a reactor embodiment, both leaking fuel plasma
and energetic charged fusion products (e.g. the 14-MeV proton from D- 3He), can be
collimated and aimed into a direct energy converter such as a TWDEC (Reference 5.4).
This results in a high overall energy conversion efficiency. Alternately, for space
propulsion, the proton beam, augmented by injection of heavy atoms to increase the
flow mass, can be directly exhausted for thrust.
56
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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.