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Quasilinear parabolic problems with nonlinear boundary conditions

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3.2 A general trace theorem<br />

Let X be a Banach space of class HT , p ∈ (1, ∞), J = [0, T ] or R+, and A be an<br />

R-sectorial operator in X <strong>with</strong> arbitrary R-angle φR A < π. Further suppose γ ∈ [0, 1/p),<br />

s > 1/p − γ, and<br />

u ∈ Z := H s+γ<br />

p (J; X) ∩ H γ p (J; DA). (3.17)<br />

Our first aim is to prove that u(0) ∈ DA(1 + γ/s − 1/ps, p). To do so, note that, by the<br />

mixed derivative theorem, we have the embedding<br />

H s+γ<br />

p (J; X) ∩ H γ p (J; DA) ↩→ H (1−θ)s+γ<br />

p (J; DAθ), θ ∈ (0, 1). (3.18)<br />

We now distinguish two cases.<br />

Case 1: 1/p − γ < s < 2(1/p − γ). By hypothesis and (3.18), we see that<br />

u ∈ H s+γ<br />

p (J; X) ∩ H (1−θ)s+γ<br />

p (J; DAθ), θ ∈ (0, 1).<br />

If we put κ = (1 − θ)s + γ, B = Aθ , and a(t) = e−ttθs−1 , t > 0, then we are in the<br />

situation of Theorem 3.1.4, provided that κ < 1/p and θsπ/2 + φR B < π. But these<br />

two <strong>conditions</strong> are fulfilled <strong>with</strong> θ = 1/2. In fact, in case of θ = 1/2, we estimate<br />

κ = s/2 + γ < (1/p − γ) + γ = 1/p, as well as<br />

θs π<br />

2 + φR sπ 1<br />

B ≤ 4 + 2 φR π π<br />

A < 2 + 2<br />

= π,<br />

where the inequality φR B ≤ φR A /2 follows from Proposition 2.2.1. Further,<br />

1 + κ 1 2γ 2<br />

θs − θsp = 2 + s − ps ,<br />

and so, by Theorem 3.1.4 and Theorem 2.2.2, we obtain<br />

u(0) ∈ DB(2 + 2γ<br />

s<br />

2 − ps , p) = D A 1 2γ 2<br />

(2 +<br />

2 s − ps , p) = DA(1 + γ 1<br />

s − ps , p).<br />

Case 2: s ≥ 2(1/p − γ). Here, we look at the regularity <strong>with</strong> respect to the operator<br />

A. By hypothesis and (3.18),<br />

u ∈ H (1−θ)s+γ<br />

p (J; D A θ) ∩ H γ p (J; DA), θ ∈ (0, 1).<br />

Therefore, if we choose the base space Xθ = D(A θ ), then we get<br />

u ∈ H (1−θ)s+γ<br />

p (J; Xθ) ∩ H γ p (J; D A 1−θ), θ ∈ (0, 1).<br />

Again, we want to apply Theorem 3.1.4. So we have to ensure that 1/p < (1 − θ)s + γ<br />

and (1 − θ)sπ/2 + (1 − θ)φR A < π. But these <strong>conditions</strong> are satisfied for<br />

θ = 1 − η<br />

� �<br />

1<br />

s p − γ<br />

<strong>with</strong> an arbitrary η ∈ (1, 2/(1 + 1/p − γ)]. We namely have in this case<br />

� �<br />

1<br />

(1 − θ)s + γ = η p − γ + γ > 1<br />

p<br />

as well as<br />

(1 − θ)s π<br />

2 + (1 − θ)φR A < η<br />

� �<br />

1<br />

p − γ · π<br />

� � � �<br />

η 1<br />

1<br />

2 + s p − γ π ≤ η p − γ · π η<br />

2 + 2 π ≤ π,<br />

44

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