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1
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84889780308
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Springer, Berlin
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D. Jou, J. Casas-Vázquez, and G. Lebon, Extended Irreversible Thermodynamics, 2nd ed. (Springer, Berlin, 1996);
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(1996)
Extended Irreversible Thermodynamics, 2nd ed.
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Jou, D.1
Casas-Vázquez, J.2
Lebon, G.3
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7
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85037179742
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S. Chapman and T. Cowling, Mathematical Theory of Non-uniform Gases (Cambridge University Press, Cambridge, 1970)
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S. Chapman and T. Cowling, Mathematical Theory of Non-uniform Gases (Cambridge University Press, Cambridge, 1970).
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8
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85037227193
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R. Balescu, Transport Processes in Plasmas (North-Holland, Amsterdam, 1988), Vol. 1
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R. Balescu, Transport Processes in Plasmas (North-Holland, Amsterdam, 1988), Vol. 1.
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13
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85037178408
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Dependence of projectors on the distribution functions was discussed extensively in the paper
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Dependence of projectors on the distribution functions was discussed extensively in the paper
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15
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85037221579
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Except for Maxwellian molecules (interaction potential [Formula Presented] for which [Formula Presented] but [Formula Presented]. Same goes for the relaxation time approximation of the collision integral [Formula Presented]
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Except for Maxwellian molecules (interaction potential U∼r-4) for which L̂φ0≠0 but P2[FL̂φG]=FL̂φ0. Same goes for the relaxation time approximation of the collision integral (L̂=-τ-1).
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20
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0010425103
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a recent paper, alternative Grad-like approximations were suggested, and which use the “moments” of collision integral instead of the moments of the distribution function. When this approximation is taken as the input for the corrections procedure instead of the Grad’s as above, the local corrections satisfy the following integral equations: [Formula Presented] [Formula Presented]. Thus, both the inputs have the same limiting eigenvalue problems but proceed to this limit via apparently different sequences of approximations. PLEEE8
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In a recent paper, A. N. Gorban and I. V. Karlin, Phys. Rev. E 54, R3109 (1996), alternative Grad-like approximations were suggested, and which use the “moments” of collision integral instead of the moments of the distribution function. When this approximation is taken as the input for the corrections procedure instead of the Grad’s as above, the local corrections satisfy the following integral equations: L̂Yn=bnYn+1, and L̂Zn=anZn+1. Thus, both the inputs have the same limiting eigenvalue problems but proceed to this limit via apparently different sequences of approximations. PLEEE8
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(1996)
Phys. Rev. E
, vol.54
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Gorban, A.N.1
Karlin, I.V.2
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