2018
DOI: 10.3934/krm.2018059
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Fractional diffusion limits of non-classical transport equations

Abstract: We establish asymptotic diffusion limits of the non-classical transport equation derived in [10]. By introducing appropriate scaling parameters, the limits will be either regular or fractional diffusion equations depending on the tail behaviour of the path-length distribution. Our analysis uses the Fourier transform combined with a moment method. We conclude with remarks on the diffusion limit of the periodic Lorentz gas equation.

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Cited by 17 publications
(19 citation statements)
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“…The theory has been extended over the last few years [3][4][5][6][7] and has found applications in other areas, including neutron transport in certain types of nuclear reactors [8][9][10], computer graphics [11][12][13], and problems involving anomalous diffusion (cf. [14]). Moreover, a similar kinetic equation has been independently derived for the periodic Lorentz gas in a series of papers by Golse (cf.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The theory has been extended over the last few years [3][4][5][6][7] and has found applications in other areas, including neutron transport in certain types of nuclear reactors [8][9][10], computer graphics [11][12][13], and problems involving anomalous diffusion (cf. [14]). Moreover, a similar kinetic equation has been independently derived for the periodic Lorentz gas in a series of papers by Golse (cf.…”
Section: Introductionmentioning
confidence: 99%
“…The assumption that Σ t is independent of both Ω and s is generally valid when the spatial locations of the scattering centers in the system are uncorrelated (Poisson distributed). This leads to the Beer-Lambert law, with particle flux decreasing as an exponential function of s. However, a nonexponential attenuation law for the particle flux occurs in certain heterogeneous media in which the scattering centers in the system are spatially correlated [2,[8][9][10][11][13][14][15][16][17][18][19]. The theory of nonclassical particle transport [1,[3][4][5][6][7] was developed to address this class of problems.…”
Section: Introductionmentioning
confidence: 99%
“…We note that working with a weighted density seems to be a general setting when deriving (fractional) diffusion limits of kinetic equations with extended variables. See for example in [14], where the macroscopic equations for a non-classical kinetic equation are derived for the weighted density function against the path length distribution. Compared with [14], the choice of the weight function χ 0 in this paper is much less obvious.…”
Section: Introductionmentioning
confidence: 99%
“…See for example in [14], where the macroscopic equations for a non-classical kinetic equation are derived for the weighted density function against the path length distribution. Compared with [14], the choice of the weight function χ 0 in this paper is much less obvious. Second, the derivation of the fractional diffusion equations in [1,9,19] relies on the method of auxiliary functions or a related Hilbert expansion.…”
Section: Introductionmentioning
confidence: 99%
“…Here we assume that φ is bounded from above and below. The equilibrium (1.12) arises in numerous areas of applications such as granular plasmas with dissipative collision [5,8,7,13,23], astrophysical plasmas [22], economy [12] and transport in atmospheric clouds [14]. See also [23] for a review of granular materials in which power law like distribution appears as a typical equilibrium in inelastic kinetic theory.…”
mentioning
confidence: 99%