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Modélisation, analyse mathématique et simulations numériques de ...

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

4.2 Numerical schemes and main results 97<br />

where β0, g and h are some constants <strong>de</strong>pending only on U0.<br />

Hence the subcharacteristic condition reads, in our case:<br />

<br />

<br />

<br />

∂uR(u,v) <br />

<br />

∂vR(u,v)<br />

< √ a.<br />

For the sequel, we <strong>de</strong>fine for any N > 0 and α > 0,<br />

⎧<br />

⎪⎨<br />

⎪⎩<br />

U(N,α) :=<br />

<br />

1+ 1<br />

<br />

√ N , α<br />

F(N,α) := sup |A(ξ)|,<br />

|ξ|≤U(N,α)<br />

V(N,α) := U(N,α) + 1<br />

√ α F (N,α) .<br />

We also <strong>de</strong>note by I(N,α) the compact s<strong>et</strong><br />

(4.2.3)<br />

I(N,α) := − √ aV(N,α), √ aV(N,α) 2 . (4.2.4)<br />

Moreover, we assume that the initial conditions u ε 0 ,vε 0<br />

L ∞ (R), such that:<br />

are boun<strong>de</strong>d in<strong>de</strong>pen<strong>de</strong>ntly of ε in<br />

<br />

N0 := max supu<br />

ε>0<br />

ε 0L∞,supv ε>0<br />

ε 0L∞ <br />

< ∞. (4.2.5)<br />

Consi<strong>de</strong>r any a0 > 0 and assume that the function R ∈ 1 (R×R,R) satisfies (4.1.3) and<br />

(4.2.2). We choose the characteristic speed √ a > 0 and the param<strong>et</strong>er β > 0 such that<br />

⎧<br />

⎪⎨<br />

⎪⎩<br />

where V is given by (4.2.3).<br />

<br />

√ √a0,<br />

a > max<br />

g(V(N0,a0))<br />

<br />

,<br />

β0(V(N0,a0))<br />

β = h(V(N0,a0)),<br />

Remark 2.1. Note that if we differentiate with respect to u the equilibrium equation<br />

we obtain<br />

R(u,A(u)) = 0,<br />

A ′ (u) = − ∂uR(u,A(u))<br />

∂vR(u,A(u))<br />

(4.2.6)<br />

(4.2.7)<br />

and thus recover the well known subcharacteristic condition in the case of semi-linear<br />

relaxation, namely:<br />

|A ′ (u)| < √ a.

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