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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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exponents greater than 2. The first suggestion of th ils was By R. W. Bussard based on
theoretical arguments (see Section 1). Later, PIC studies by M. Ohnishi at Kyoto
University (now at Kansai University) also showed such strong scaling (not covered
here- but see M. Ohnishi in Proceedings of 16th IEEE/NPSS, vol. 2, pp. 1468-1471). The
unanswered question is at what current level this occurs. Future simulations shou ld
address that issue and also examine low angular momentum spread and higher ion
injection energies.
In summary, this study by Tzonev et al. is very encouraging for formation of deep wells
in IEC devices designed for reactors using beam-beam dominated fusion. However,
much more work needs to be done along these lines to fu lly identify the optima l ion
injection strategy for deep wells with minimum power input. As stressed earlier, the
potential well parameters must also be combined with a consistent calculation of the
energy gain (Q) following the methods of L. Chacon et al. to establish a complete
picture of energy gain possible in a power type IEC.
MOMOTA ET AL. - STUDY OF VIRTUAL ELECTRODE STRUCTURE
In another related study, Momota and Miley (Reference 4.5) used an analytic solution
to examine the angular momentum effects. "Double-we ll " potential structure (virtual
cathode formation) was studied in a stationary spherical IEC using the nonlinear
Poison's equations and particle densities derived from kinetic theory. A novel method to
obtain a spherica lly symmetric stationary distribution function is introduced and an
integral-differential equation is simplified by applying a re levant approximated formu la
for an integral. Electron and ion beams are co llision-free, and their velocities are
roughly aligned toward th e spherical center, but with a slight divergence. Analyses
show that the angular momentum of ions and the smaller one of the electrons create a
virtual cathode, i.e., a double-well structure, of the electrostatic potential on a potentia l
hill near the center. The density limit of an !EC well was found and the conditions
relevant to form a deep potential well was presented.
These results show trends roughly similar to the numerical studies of Tzonev, et al.,
and may be useful to persons wanting to study the effects analytically.
KIM - STABILITY ANALYSIS
In addition to achieving adequate potential well trapping for net energy production, the
question of stability of the non-Maxwellian plasma in the well must be considered.
(Note that "stabi lity" is a separate question from the therma li zation of the beam-like
distribution in the IEC discussed earlier. However, they are coupled nonlinear problems
due to the fact that the distribution function used for both calculations should be
consistent). N. Krall did some earlier studies to show that the distribution in the R.W.
Bussard type Polywell IEC are stable against key instabi lities such as two-stream. These
studies however, were internal company reports and not openly published . Some
information is given, however, in Reference 1.7. More recently, H.J. Kim, in his thesis
done with G. Miley, did an in-depth study of two stream -li ke instabilities in the ion
injected type IEC (see Reference 4.6). His work is very encouraging in that he identifies
a possible "window of stability" which depends on the injected energy distribution and
angular velocity spread . This result is summarized in Figure 4.10. The analysis is briefly
described as follows.
UNCLASSIFIED/ /&OA: O&&ICIAL !!ii ODt11 X
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