1965
DOI: 10.1063/1.1761243
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Numerical Integration of Kinetic Equations

Abstract: The problem of the relaxation to a Maxwellian of the Balescu-Lenard equation is solved numerically as an initial value problem for isotropic distributions of electrons situated in a neutralizing, uniformly smeared out background of positive charge. Several different forms for the initial distribution function are chosen: a Gaussian peaked at about 0.28 of the electron thermal speed, a resonance function, and a Maxwellian coexisting with a sharply peaked Gaussian (the peak of the Gaussian being located at two t… Show more

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Cited by 19 publications
(7 citation statements)
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“…We find, however, that there is not much difference between calculating the distributions with the full Lenard-Balescu collision operator versus using Landau with a well-chosen Coulomb logarithm, even in cases where the temperature separation is large. This is consistent with previous numerical comparisons of the two equations [5,6].…”
Section: Introductionsupporting
confidence: 93%
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“…We find, however, that there is not much difference between calculating the distributions with the full Lenard-Balescu collision operator versus using Landau with a well-chosen Coulomb logarithm, even in cases where the temperature separation is large. This is consistent with previous numerical comparisons of the two equations [5,6].…”
Section: Introductionsupporting
confidence: 93%
“…For the dielectric function we use the classical approximation; that is, we neglect quantum diffraction [5]. The main benefit of this is that the dielectric function takes the comparatively simple form (6). That is, the variables X and Y separate, facilitating analytical evaluation of the X-integral without losing any important physical content.…”
Section: Equation Coefficientsmentioning
confidence: 99%
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“…These difficulties, coupled with the fact that the Landau equation, despite its deficiencies, yields distributions that are likely qualitatively correct at weak coupling, have kept the Lenard-Balescu equation from being studied numerically in any serious way. We know of only one previous attempt: Dolinsky's pioneering 1965 solution of the classical LB equation 14 using a discretization method in velocity. This work predates the advent of conservative velocity discretization schemes even for the Fokker-Planck equation, but it is not completely clear that such methods are generically well-suited to the Lenard-Balescu equation anway because of the need to accurately integrate over the features of the dielectric function.…”
Section: Quantum Lenard-balescu Equationmentioning
confidence: 99%
“…Eq. (42) may also be integrated using a non-conservative method [30,16], but when this was tried in our code the distribution function, even when initialized as a Maxwellian, was visibly modified by numerical effects within a few collision times. This can be mitigated by using ultra-fine resolution in momentum-space, but such a grid would require a very small time-step and an enormous amount of computer memory.…”
Section: Characteristic Collisional Quantitiesmentioning
confidence: 99%