Quasilinear parabolic problems with nonlinear boundary conditions
Quasilinear parabolic problems with nonlinear boundary conditions
Quasilinear parabolic problems with nonlinear boundary conditions
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(H2) a ∈ Cul(J × R n , Sym{n}), b1 ∈ L∞(J × R n , R n ), b0 ∈ L∞(J × R n );<br />
(H3) ∃a0 > 0 : a(t, x)ξ · ξ ≥ a0|ξ| 2 , t ∈ J, x ∈ R n , ξ ∈ R n .<br />
Then the Volterra equation (4.1) admits a unique solution in the space<br />
Z := H α p (J; Lp(R n )) ∩ Lp(J; H 2 p(R n ))<br />
if and only if the function f is subject to the subsequent <strong>conditions</strong>.<br />
(i) f ∈ H α p (J; Lp(R n ));<br />
(ii) f|t=0 ∈ γ0Z := B<br />
(iii) ∂tf|t=0 ∈ γ1Z := B<br />
2<br />
2− pα<br />
pp<br />
(R n ), if α > 1/p;<br />
1 1<br />
2(1− − α pα )<br />
pp<br />
(R n ), if α > 1 + 1/p.<br />
Proof. We start <strong>with</strong> the necessity part. Suppose that v ∈ Z solves (4.1). By assumption<br />
(H2), we immediately verify that A(t, x, Dx)v ∈ Lp(J; Lp(R n )). Thus, in view of (H1),<br />
f = v − k ∗ A(·, x, Dx)v ∈ H α p (J; Lp(R n )), i.e. condition (i) is satisfied. To see (ii)<br />
and (iii), apply Theorem 3.2.1 to the space Lp(R n ) and the operator A = −∆ <strong>with</strong><br />
domain H 2 p(R n ), and use (Lp(R n ), H 2 p(R n ))s, p = B 2s<br />
pp(R n ), s ∈ (0, 1), together <strong>with</strong><br />
∂ j<br />
t v|t=0 = ∂ j<br />
t f|t=0 in case α > j + 1/p, j = 0, 1.<br />
The sufficiency part is more involved. Suppose f satisfies (i)-(iii). In order to prove<br />
existence of a unique solution of (4.1) in Z, we use localization and perturbation to<br />
reduce (4.1) to related equations <strong>with</strong> constant coefficients.<br />
Given η > 0, assumption (H2) allows us to select a large ball Br0 (0) ⊂ Rn such that<br />
|a(t, x) − a(t, ∞)| B(R n×n ) ≤ η<br />
2 , for all t ∈ J, x ∈ Rn , |x| ≥ r0.<br />
Putting U0 = R n \ Br0 (0) we can further cover Br0 (0) by finitely many balls Uj =<br />
Brj (xj), j = 1, . . . , N, and choose a partition 0 =: T0 < T1 < . . . < TM−1 < TM := T<br />
such that for all i = 0, . . . , M − 1, j = 1, . . . , N,<br />
and<br />
|a(t, x) − a(Ti, xj)| B(R n×n ) ≤ η, t ∈ [Ti, Ti+1], x ∈ Brj (xj),<br />
|a(t, ∞) − a(Ti, ∞)| B(R n×n ) ≤ η<br />
2 , t ∈ [Ti, Ti+1].<br />
Define coefficients of spatially local operators A j<br />
# (t, x, Dx) = −a j (t, x) : ∇ 2 x e.g. by<br />
reflection, that is<br />
and<br />
a 0 �<br />
a(t, x) : t ∈ J, x /∈ Br0<br />
(t, x) :=<br />
(0)<br />
a(t, r2 0 x<br />
|x| 2 ) : t ∈ J, x ∈ Br0 (0)<br />
a j �<br />
a(t, x) : t ∈ J, x ∈ Brj<br />
(t, x) :=<br />
(xj)<br />
a(t, xj + r2 x−xj<br />
j |x−xj| 2 ) : t ∈ J, x /∈ Brj (xj)<br />
for each j = 1, . . . , N. With x0 = ∞, we then have<br />
|a j (t, x) − a(Ti, xj)| B(R n×n ) ≤ η, t ∈ [Ti, Ti+1], x ∈ R n ,<br />
for all i = 0, . . . , M − 1, j = 0, . . . , N.<br />
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