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tel-00656013, version 1 - 3 Jan 2012<br />

106 An Asymptotic Preserving scheme<br />

4.3.3 BV estimates<br />

In this section, we obtain a BV estimate on the numerical solution to the scheme<br />

(4.2.13)-(4.2.14), that is, equivalently the scheme (4.3.2)-(4.3.3), with the time-space step<br />

h = (∆t,∆x) such that (4.2.8) is satisfied.<br />

Proposition 3.4. Assume that u0,v0 are uniformly boun<strong>de</strong>d with respect to ε in BV(R).<br />

For any a0 > 0 and N0 = max supu0L<br />

ε>0<br />

∞,supv0L<br />

ε>0<br />

∞<br />

<br />

, we assume that the function<br />

R ∈ C1 (R × R,R) satisfies (4.1.3)-(4.2.2) and choose a > 0, β > 0 such that (4.2.6) is<br />

verified. Then, for all n ∈ N, we have:<br />

TV(w n+1 ) + TV(z n+1 ) ≤ TV(w n ) + TV(z n ).<br />

Proof. First we note that u 0 , v 0 ∈ BV(R), then by construction, w 0 , z 0 ∈ BV(R) also.<br />

To prove the BV estimate, we proceed in two steps. On the one hand, using the TVD<br />

property of the upwind scheme, we g<strong>et</strong> that<br />

TV(w n+1/2 ) ≤ TV(w n ) and TV(z n+1/2 ) ≤ TV(z n ).<br />

On the other hand, we apply the nonlinear relaxation step (4.3.3) and from Lemma 3.1<br />

(iii) with w n+1/2<br />

1 = wn+1/2 (.) , z n+1/2<br />

1 = zn+1/2 (.) and w n+1/2<br />

2 = wn+1/2 (.+∆x), z n+1/2<br />

2 =<br />

zn+1/2 (.+∆x), it yields for any j ∈ Z,<br />

|w n+1<br />

j+1 −wn+1<br />

j | + |z n+1<br />

j+1 −zn+1<br />

j | ≤ |w n+1/2<br />

j+1 −wn+1/2<br />

j |+|z n+1/2<br />

j+1 −zn+1/2<br />

j |.<br />

Summing over j ∈ Z, we g<strong>et</strong> that<br />

TV(w n+1 ) + TV(z n+1 ) ≤ TV(w n+1/2 ) + TV(z n+1/2 )<br />

4.4 Trend to equilibrium<br />

≤ TV(w n ) + TV(z n ).<br />

In this section we first focus on the asymptotic behavior of the numerical solution to<br />

(4.2.13)-(4.2.14) when ε goes to zero or when times goes to infinity. Then, we prove that<br />

the numerical solution to (4.2.13)-(4.2.14) converges to a consistent approximation of the<br />

conservation laws (4.1.4) when ε goes to zero. It corresponds to the limit Pε h → P0 h , when<br />

ε → 0.<br />

4.4.1 Asymptotic behavior<br />

In this subsection, we drop the subscripts ε for sake of clarity.

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