2012
DOI: 10.1137/100795954
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Asymptotic-preserving Projective Integration Schemes for Kinetic Equations in the Diffusion Limit

Abstract: We investigate a projective integration scheme for a kinetic equation in the limit of vanishing mean free path, in which the kinetic description approaches a diffusion phenomenon. The scheme first takes a few small steps with a simple, explicit method, such as a spatial centered flux/forward Euler time integration, and subsequently projects the results forward in time over a large time step on the diffusion time scale. We show that, with an appropriate choice of the inner step size, the time-step restriction o… Show more

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Cited by 41 publications
(80 citation statements)
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“…However, as ε goes to 0, we obtain the limiting system (1.5) for which a standard finite volume/forward Euler method only needs to satisfy a stability restriction of the form ∆t ≤ C∆ x, with C a constant that depends on the specific choice of the scheme. In [8], it was proposed to use a projective integration method to accelerate such a brute-force integration; the idea, originating from [5], is the following. Starting from a computed numerical solution f n at time t n = n∆t, one first takes K + 1 inner steps of size δt using (1.7), denoted as f n,k+1 , in which the superscripts (n, k) denote the numerical solution at time t n,k = n∆t + kδt.…”
Section: Projective Integrationmentioning
confidence: 99%
“…However, as ε goes to 0, we obtain the limiting system (1.5) for which a standard finite volume/forward Euler method only needs to satisfy a stability restriction of the form ∆t ≤ C∆ x, with C a constant that depends on the specific choice of the scheme. In [8], it was proposed to use a projective integration method to accelerate such a brute-force integration; the idea, originating from [5], is the following. Starting from a computed numerical solution f n at time t n = n∆t, one first takes K + 1 inner steps of size δt using (1.7), denoted as f n,k+1 , in which the superscripts (n, k) denote the numerical solution at time t n,k = n∆t + kδt.…”
Section: Projective Integrationmentioning
confidence: 99%
“…see the bottom of page 22 in [1], and compare with the consistency derivation in [2]. However, equation (5) is valid only if one has…”
mentioning
confidence: 79%
“…From (24), is is clear that Integrating the equations in (26) over S 2 , adding them together, and applying the results of (27) and (28) gives…”
Section: Diffusive Scattering Limitmentioning
confidence: 99%