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Equation of state and optimum compression in inertial fusion energy

Published online by Cambridge University Press:  15 October 2007

S. Eliezer ,
M. Murakami  and
J.M. Martinez Val
S. Eliezer*
Affiliation:
Soreq, NRC, Yavne, Israel ETSII, Polytechnic University Madrid, Spain
M. Murakami
Affiliation:
ILE, Osaka University, Osaka, Japan
J.M. Martinez Val
Affiliation:
ETSII, Polytechnic University Madrid, Spain
*
Address correspondence and reprint request to: S. Eliezer, Soreq, NRC, Yavne, Israel. E-mail: [email protected]
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Abstract

The inertial confinement fusion (ICF) philosophy is based on high compression. The reasoning is that (a) it is cheaper (energetically) to compress than to heat and (b) nuclear reactions are proportional to density square, therefore the more you compress the better you are in ICF. Of course the only limitations of compression are the hydrodynamic instabilities (like Rayleigh-Taylor, etc). Many of the references in the literature require extremely high compression and in particular the pB11 needs extremely huge compressions. In this paper it is shown that there is an optimum of compression, namely gain G is maximum for a definite compression. The value of this density (for a given fuel mass and particular ICF scheme) depends on the equation of state (EOS). We calculate this value for fast ignition (FI) schemes and compare it with the central spark ignition (CSI) model. The gain calculations are based on the ideal gas for the ions and the Fermi-Dirac EOS for the electrons with an effective alpha, as usually suggested from simulations. The “optimum compression” idea is easily understood from the following argument: From EOS data one needs an infinite energy to compress to an infinite density. Since the energy output is finite it is clear that G is zero for infinite compression. On the other hand for normal density with small fuel mass (~ few mg) the gain is also zero. Therefore a maximum should exist somewhere. For the deuterium-tritium fuel with a mass of few mg one gets an optimum at few hundred g/cc. If you compress more then the gain is going down. So there is a desired maximum compression fixed by EOS. Last but not least, bremsstrahlung losses in degenerate plasma are discussed and the clean fusion (i.e., without neutrons) of proton + B11 → 4α is analyzed.

Keywords

CompressionEquation of StateFast ignitionGainInertial confinement fusionNuclear fusionProton-boron11 nuclear fusion
Type
Research Article
Information
Laser and Particle Beams , Volume 25 , Issue 4 , December 2007 , pp. 585 - 592
Copyright
Copyright © Cambridge University Press 2007

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