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84882092086
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See Section 3.4. The principle was established for the ground state of the electron gas by, extended to finite temperatures by, It was first applied to classical systems by
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84882200541
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See Chapter 5, Section 5.5.
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See Chapter 5, Section 5.5.
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45
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0037145613
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For a listing of many of the proposed equations and an assessment of their relative merits, see
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36849106010
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0345045853
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The HNC approximation was developed independently by several workers. For some historical background, see
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84882104683
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The implementation of certain theories also requires a knowledge of the hard-sphere y(r) inside the hard core, a parametrisation of which is given by
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Verlet L., Weis J.J., Grundke E.W., Henderson D. Phys. Rev. A. Mol. Phys. 1972, 24:269. The implementation of certain theories also requires a knowledge of the hard-sphere y(r) inside the hard core, a parametrisation of which is given by.
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Verlet, L.1
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77
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84882059739
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This transformation is achieved by a topological reduction based on Lemma 5 of Section 3.7.
-
This transformation is achieved by a topological reduction based on Lemma 5 of Section 3.7.
-
-
-
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78
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84882051327
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-
We use electrostatic units (esu).
-
We use electrostatic units (esu).
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79
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0036608173
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See, e.g.
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0030239698
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For examples of this approach, see
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0001638742
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Note that the "bridge function" in these and related papers is sometimes defined, in the present notation, as ?d(r).
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84926805355
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See note 14. The hard-sphere bridge function has also been parametrised as a function of packing fraction by
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Malijevskỳ A., Labík S. Mol. Phys. 1987, 60:663. See note 14. The hard-sphere bridge function has also been parametrised as a function of packing fraction by.
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97
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84882068488
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This result follows straightforwardly from the thermodynamic relations (2.3.8) and (2.3.9)
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This result follows straightforwardly from the thermodynamic relations (2.3.8) and (2.3.9).
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98
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7644232888
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For later developments see, e.g.
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84882123222
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For the extension to three dimensions, see
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0001608409
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84882224128
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84882143105
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See Chapter 5, Section 5.6.
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When g(d) = 1, (7.2.2) reduces to the result obtained by solution of the Boltzmann equation in a first-order approximation; higher-order corrections are of order 2%. See, e.g.,, Cambridge University Press, New York
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Bien, T.1
Possiel, M.2
Döge, G.3
Yarwood, J.4
Arnold, K.E.5
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