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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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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.
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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.