2016
DOI: 10.1007/978-3-319-32144-8_1
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On Linear Hypocoercive BGK Models

Abstract: We study hypocoercivity for a class of linear and linearized BGK models for discrete and continuous phase spaces. We develop methods for constructing entropy functionals that prove exponential rates of relaxation to equilibrium. Our strategies are based on the entropy and spectral methods, adapting Lyapunov's direct method (even for "infinite matrices" appearing for continuous phase spaces) to construct appropriate entropy functionals. Finally, we also prove local asymptotic stability of a nonlinear BGK model.

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Cited by 31 publications
(115 citation statements)
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“…for x ∈ T 1 , velocities v ∈ R, and the Maxwell distribution M T (v) = (2πT ) − 1 2 e − |v| 2 2T , with given temperature T . Exponential decay towards the equilibrium for this vcontinuous model was proved in §4.3 of [1]. We reduce the model drastically and allow only for two discrete velocities v ± = ±1, denoting f ± (x, t) := f (x, ±1, t).…”
Section: Two Velocity Bgk Model With Uncertain Coefficientsmentioning
confidence: 97%
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“…for x ∈ T 1 , velocities v ∈ R, and the Maxwell distribution M T (v) = (2πT ) − 1 2 e − |v| 2 2T , with given temperature T . Exponential decay towards the equilibrium for this vcontinuous model was proved in §4.3 of [1]. We reduce the model drastically and allow only for two discrete velocities v ± = ±1, denoting f ± (x, t) := f (x, ±1, t).…”
Section: Two Velocity Bgk Model With Uncertain Coefficientsmentioning
confidence: 97%
“…In this section we first review (from [1]) the Lyapunov functional method for non-defective ODEs and then extend it to the defective case. This is based on constructing a norm adapted to the problem that allows to recover the sharp decay behavior.…”
Section: Lyapunov Functionals For Defective Odesmentioning
confidence: 99%
“…In fact in this limit case the microscopic coercivity nevertheless holds once accounting for the larger null space of L 1 . We are not concerned in this case for which the NESS is already known, and we refer to [1] for a study of the microscopic coercivity and hypocoercivity for the equation of this limit case; This could also be deduced from the abstract results in [12].…”
Section: Microscopic Coercivitymentioning
confidence: 99%
“…Second proof of Theorem 2. We consider α ∈ [0, 1) (for α = 1 the result is already known from [1]). We apply the previous Theorem 13 with H being the subspace of H α = L 2 (f −1 ∞,α dxdv) consisting of functions that satisfy the zero global mass condition´T ×R h(x, v) dx dv = 0.…”
Section: Hypocoercivitymentioning
confidence: 99%
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