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Methods of Vanishing Viscosity for Nonlinear ... - ACMAC

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Navier-Stokes Equations: Key Estimates III<br />

Then<br />

That is,<br />

∫<br />

ε 2 |ρx (t, x)| 2<br />

∫<br />

(γ − t ∫<br />

1)2<br />

dx + ε ρ γ−3 |ρ<br />

ρ(t, x) 3 x | 2 dxdτ<br />

2 0<br />

∫ [ ]<br />

ρx u t ∫ t ∫<br />

= −2ε<br />

dx + 2ε |u x | 2 dxdτ<br />

ρ<br />

τ=0<br />

0<br />

∫<br />

≤ ε2 |ρx (t, x)| 2 ∫<br />

2 ρ(t, x) 3 dx + |ρ0,x (x)| 2<br />

ε2 dx + C.<br />

ρ 0 (x) 3<br />

∫<br />

ε 2 |ρx (t, x)| 2 ∫ t ∫<br />

ρ(t, x) 3 dx + ε ρ γ−3 |ρ x | 2 dxdτ<br />

0<br />

∫<br />

≤ C<br />

(ε 2 |ρ0,x (x)| 2 )<br />

ρ 0 (x) 3 dx + 1 .<br />

Case II: u + ≠ u − : More technically involved.<br />

Gui-Qiang Chen (Ox<strong>for</strong>d) <strong>Vanishing</strong> <strong>Viscosity</strong>/Conservation Laws June 20–24, 2011 23 / 40

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