Weak Convergence Methods for Nonlinear Partial Differential ...
Weak Convergence Methods for Nonlinear Partial Differential ...
Weak Convergence Methods for Nonlinear Partial Differential ...
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We now prove an important necessary condition <strong>for</strong> weak lower semicontinuity.<br />
Theorem 2.40 1. If l ≥ f(u) <strong>for</strong> any sequence satisfying (H 0 ), then f is<br />
convex in the directions of Λ, i.e., t ↦→ f(a + tb) is convex ∀a ∈ R m , b ∈ Λ.<br />
2. If l = f(u) <strong>for</strong> any sequence satisfying (H 0 ), then f is affine in the directions<br />
of Λ.<br />
In the variational case this is called the “Legendre-Hadamard-” or “ellipticity<br />
condition”.<br />
Proof. Only the first statement is to be shown; the second is an immediate<br />
consequence of the first one.<br />
Let t 1 , t 2 ∈ R, y 1 = a + t 1 b, y 2 = a + t 2 b and µ ∈ (0, 1). b ∈ Λ implies ∃ξ ≠ 0<br />
such that ∑<br />
a ijk b j ξ k = 0 ∀i ∈ {1, ..., q}.<br />
j,k<br />
Let ψ : R → R be 1-periodic with<br />
{<br />
(1 − µ)(t 1 − t 2 ) <strong>for</strong> 0 ≤ t < µ<br />
ψ(t) =<br />
µ(t 2 − t 1 ) <strong>for</strong> µ ≤ t < 1.<br />
Define u (ν) ∈ L ∞ (Ω) (Q-periodic with Q = R(0, 1) n , R ∈ SO(n) such that<br />
Re 1 = ξ ) by |ξ|<br />
(<br />
u (ν) (x) = z + bψ ν ξ )<br />
|ξ| · x , z = µy 1 + (1 − µ)y 2 .<br />
Then u (ν) is highly oscillating and converges to<br />
Q<br />
Q<br />
w*- lim u (ν) = z<br />
because<br />
∫ ∫<br />
− u (ν) = z + b− ψ( ξ ∫ 1<br />
|ξ| · x) = z + ψ(t)dt<br />
Similarly,<br />
∫<br />
w*- lim f(u (ν) ) = − f<br />
Q<br />
0<br />
= z + µ(1 − µ)(t 1 − t 2 ) + (1 − µ)µ(t 2 − t 1 ) = z.<br />
( ( )) ξ<br />
z + bψ<br />
|ξ| · x =<br />
∫ 1<br />
0<br />
f(z + bψ(t))dt,<br />
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