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The electrical and thermal conductivity model used is a recent model by M. P. Desjarlais. The model is similar to the Lee-More-Desjarlais (LMD) model, however, ab-initio calculations indicated that the LMD model underestimated the conductivity of aluminum by ∼70% in the dense liquid regime and appropriate corrections to the LMD model were made. This model has resulted in improved agreement in MHD simulations of wire expansion and flyer plate experiments.
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The initial flyer thickness was nominally 800 μm. The ∼300 μm. thickness refers to portion of the flyer at impact that remained unaffected by magnetic diffusion.
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In actuality, the flyer plate experiences further quasi-isentropic compression and release, but that process can be treated as being reversible, and thus we only need consider the release from the shocked state.
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note
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Predictions for SESAME 3700, 3711, 3715, and 3719 are shown. SESAME 3716 exhibits a very similar response to 3715.
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70
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84865042928
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edited by J. Davis, C. Deeney, and N. R. Pereira (AIP, New York)
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R. W. Lemke, M. D. Knudson, A. C. Robinson, T. A. Haill, K. W. Struve, T. A. Mehlhorn, and J. R. Asay, in Dense Z-Pinches, edited by J. Davis, C. Deeney, and N. R. Pereira (AIP, New York, 2002), pp. 299-304.
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(2002)
Dense Z-Pinches
, pp. 299-304
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Lemke, R.W.1
Knudson, M.D.2
Robinson, A.C.3
Haill, T.A.4
Struve, K.W.5
Mehlhorn, T.A.6
Asay, J.R.7
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71
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0142022621
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unpublished
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D. E. Bliss, R. T. Collins, D. G. Dalton, E. J. Dawson, Jr., R. L. Doty, T. L. Downey, H. C. Harjes, E. A. Illescas, B. A. Lewis, J. A. Mills, S. D. Floor, J. W. Podsednik, S. T. Rogowski, M. S. Shams, and K. W. Struve (unpublished).
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Bliss, D.E.1
Collins, R.T.2
Dalton, D.G.3
Dawson E.J., Jr.4
Doty, R.L.5
Downey, T.L.6
Harjes, H.C.7
Illescas, E.A.8
Lewis, B.A.9
Mills, J.A.10
Floor, S.D.11
Podsednik, J.W.12
Rogowski, S.T.13
Shams, M.S.14
Struve, K.W.15
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72
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0142054644
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note
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p Hugoniots were virtually identical. When the preheated flyer was in the liquid state, the same was true for the stress regime where it was applied (∼4 Mbar). These calculations validate the principal assumption used to analyze the present experiments.
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