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AAWSAP DIRD, Inertial Electrostatic Confinement Fusion, March 2010

U.S. Department of War · 2010-03-10 · 72 pages · text from the file's own layer

This Defense Intelligence Reference Document, dated 10 March 2010, was prepared by the Defense Intelligence Agency's Defense Warning Office under the Advanced Aerospace Weapon System Applications Program. It surveys the basics, experimental status, theory and possible uses of inertial electrostatic confinement (IEC) fusion, with emphasis on work at the University of Illinois Urbana-Champaign. It covers neutron sources, explosives detection and space propulsion. It ends by proposing a 12-gun hydrogen plasma experiment meant to show breakeven conditions for p-11B fuel.

From the source:Release of 2026-09-18 Incident: 3/10/10, Las Vegas, Nevada. Released with redactions. This document is a Defense Intelligence Reference Document (DIRD), a technical reference format used by the Defense Intelligence Agency (DIA) to capture baseline knowledge on a specific topic for later analytic use. DIRDs are best understood as reference and synthesis products rather than as original research. It is one of 38 DIRDs produced under the Advanced Aerospace Weapon System Applications Program (AAWSAP) between 2009 and 2011. Because AAWSAP’s scope permitted a broad range of supporting topics, not every DIRD in the series directly concerns aerospace systems or future threat assessment. The following summary reflects the DIRD’s scope and framing at the time of writing and should not be read as implying current validation of the concepts discussed. This DIRD surveys inertial electrostatic confinement (IEC) fusion, a relatively unconventional fusion concept that uses electric fields rather than the more established magnetic or laser-based approaches to confine ions, and it reviews both the underlying physics and the experimental work associated with the concept. The report emphasizes that IEC may have nearer-term value as a compact neutron, proton, or x-ray source and as a platform for studying experimental fusion approaches, while also presenting more ambitious possibilities such as aneutronic power generation and propulsion applications. At the same time, it makes clear that the concept remained far from practical fusion power, with experimental devices operating several orders of magnitude below breakeven and with major unresolved issues involving confinement, losses, grid damage, and scale-up. Overall, the document treats IEC as a technically interesting but still highly speculative path toward fusion energy, while suggesting that its more limited spin-off applications were more plausible in the near term than its long-range power generation or propulsion applications.

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let Extraction
To obtain thrust from an IEC device, a valley or trough must be created in the
electrostatic potential, and a hole must be physically cut into the ground sphere. This
allows high-speed ions to escape in the form of a plasma jet as described in the
preceding section. Ions are generated near the ground potential with the aid of electron
emitters and additional grids. A central spherical electrical grid accelerates ions to the
core region. A cylindrical "channel" grid with the same electrostatic potential as the
central spherical grid creates a passage through which ions can escape to the outside.
Thus this trough in the electrostatic potential profile across the centerline (thrust axis)
of the IEC thruster is a unique feature compared to the linear profile for a planar
device.
The ion beams finally exit through an opening in the ground sphere of the IEC device .
The channel grid must be well insulated from the ground potential to prevent short
circuiting or arc-over; thus a separate insulated feed-through cable maintains the
negative potential on the inner spherical and channel grids. Makeup propellant gas is
fed into the ionization regiion throug h needle-valve-controlled tubing located around the
chamber wall. Ionization of the propellant uses the electron emitter-guide grid design
described earlier. The inner grid serves to both extract and accelerate ions, forming the
microchannels. To control neutralization of the plasma jet, additional electron emitters
are attached close to the jet discharge hole . A combination of electron emission rates
and jet grid bias can be used to control the beam space charge, hence the growth of
focusing of the beam during propagation. In present experiments, however, the
electron rate is fixed at a suitable value while the jet grid bias is varied.
Control of the jet diameter and focus is obtained in two ways: first, the channel grid will
be separately hinged with a small servo motor such that its axis can be moved over a
volume defined by a 10 percent cone angle; second, the grid bias can be varied over a
range up to the chamber potential to provide focus control over the jet flow. A large
negative grid bias will cause a narrow focus while small potential values will allow the
plasma to expand giving a broad cross section beam.
Experimental let Design and Performance
Figure 3.3 shows the thruster experiment components. It is also of interest to •consider
the typical dimensions involved to illustrate the compactness of the unit. The
experimental studies use an existing spherical IEC chamber of ~30-cm with a 1-cm
diameter port on one side of it for beam extraction. (This is somewhat larger than
envisioned for application to micro-satellites). An 8-cm diameter spherical electrical
tungsten or tantalum wire grid, having a geometric transparency of ~90 percent, will
mount inside the chamber. A ~1-cm diameter hole will be cut into the side of the wire
grid, and this hole will be aligned with the hole in the chamber wall and connected to it
by a 2-cm diameter cylindrical guide grid. The insulator covering the grounded wall
must be of sufficient size to prevent arc-over from the ground to the cylindrical grid.
The inner electrical grids are connected to a 500-kV de power supply through the
insulated feed -through cable. A positively-charged outer grid with a variable voltage of
~10-100 Vis mounted on a swivel connector at the outside of the beam extraction
port of the chamber, in combination with four electron emitters, generates ions. The
choice for the voltages on the outer grids is flexible, so long as a sufficient ion
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Official release, from the pursue collection. The PDF is mirrored here; the original link is above. 72 pages are in the text index: search them above, or from the library's search.