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Degenerate nonlinear parabolic-hyperbolic equations and ... - SMAI

Degenerate nonlinear parabolic-hyperbolic equations and ... - SMAI

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<strong>Degenerate</strong> Parabolic Problems & FV Discretization Theoretical foundations Meshes, operators <strong>and</strong> scheme Discrete calculus & Convergence analysis<br />

Finite volume scheme for the problem...<br />

In addition, we take a usual two-point monotone consistent flux<br />

approximation to produce a discrete operator (divc F) T (·) which<br />

approximates the convection operator div F(·).<br />

With the notation introduced above, our discretization writes:<br />

find a discrete function u T,∆t satisfying for n = 1,...,N = T/∆t the <strong>equations</strong><br />

<br />

<br />

u<br />

<br />

<br />

<br />

T,n − u T,(n−1)<br />

+(div c<br />

∆t<br />

F) T [u T,n ]−div T [a0(∇ T w T,n )] = 0,<br />

w T,n = A(u T,n ),<br />

together with the boundary <strong>and</strong> initial conditions<br />

<br />

u<br />

for all n = 1,...,N,<br />

n K = 0 for all K near ∂Ω<br />

u n K ∗ = 0 for all K∗ near ∂Ω;<br />

u 0 K = 1<br />

<br />

<br />

mK<br />

K<br />

u0<br />

for all K, u 0 1<br />

K<br />

∗ =<br />

mK ∗<br />

K∗ u0 for all K ∗ .<br />

Theorem (main result of : Andr. & Bendahmane & Karlsen JHDE’11)<br />

The discrete solutions u T,∆t exist <strong>and</strong> converge to the unique entropy<br />

solution u as the discretization step (space <strong>and</strong> time) goes to zero.

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