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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We remark that the constant C2 stems from finding an upper bound for the integral<br />
� T2<br />
T1 |t − τ|−β dt, τ ∈ [0, T2], where β < 1 is a fixed number. Thus if T1 and T2 vary<br />
<strong>with</strong>in the set [0, T ], C2 can be chosen to be independent of those numbers.<br />
Set<br />
and<br />
|m| M T 1 = |m| L∞([0,T1]×R n ) + [m] C r 1 ([0,T1]; C(R n )) + [m] C([0,T1]; C r 2 (R n ))<br />
[m] M T 1 , T 2 = [m] C r 1 ([T1,T2]; C(R n )) + [m] C([T1,T2]; C r 2 (R n )) .<br />
Then our observations can be summarized as follows.<br />
Lemma 4.2.2 Suppose that 1 < p < ∞, 0 < T , 0 ≤ T1 ≤ T2 ≤ T , and 0 <<br />
si < ri < 1 for i = 1, 2. Let Y T2 s1 = Bpp([0; T2]; Lp(Rn )) ∩ Lp([0, T2]; Bs2 pp(Rn )), and<br />
M T2 r1 = C ([0, T2]; C(Rn )) ∩ C([0, T2]; Cr2 (Rn )). Then there exists a constant C > 0 not<br />
depending on T1 and T2, such that<br />
�<br />
|mf| Y T2 ≤ C<br />
(4.27)<br />
for all m ∈ M T2 and f ∈ Y T2 .<br />
4.2.3 Variable coefficients<br />
�<br />
|m| M T 1 |f| Y T 1 + |m| L∞([T1,T2]×R n )(1 + [m] M T 1 , T 2 )|f| Y T 2<br />
The goal of this subparagraph is to extend the results proven in Subsection 4.2.1 to variable<br />
coefficients. Besides we no longer stick to differential operators consisting only of the<br />
principal part but consider general operators of second (Volterra equation) respectively<br />
first order (<strong>boundary</strong> condition).<br />
To start <strong>with</strong>, recall the notation R n+1<br />
+ = {(x′ , y) ∈ Rn+1 : x ′ ∈ Rn , y > 0}. Define<br />
the operators A(t, x, Dx) and B(t, x ′ , Dx) by<br />
and<br />
A(t, x, Dx) = −a(t, x) : ∇ 2 x + a1(t, x) · ∇x + a0(t, x), t ∈ J, x ∈ R n+1<br />
+ ,<br />
B(t, x ′ , Dx) = −∂y + b(t, x ′ ) · ∇x ′ + b0(t, x ′ ), t ∈ J, x ′ ∈ R n , (4.28)<br />
respectively. We are concerned <strong>with</strong> the two separate <strong>problems</strong><br />
� v + k ∗ A(·, x, Dx)v = f, t ∈ J, x ∈ R n+1<br />
+ ,<br />
v = g, t ∈ J, x ′ ∈ R n , y = 0<br />
� v + k ∗ A(·, x, Dx)v = f, t ∈ J, x ∈ R n+1<br />
+ ,<br />
B(t, x ′ , Dx)v = h, t ∈ J, x ′ ∈ R n , y = 0<br />
and seek, as in Subsection 4.2.1, unique solutions in the regularity class<br />
Z = H α p (J; Lp(R n+1<br />
+ )) ∩ Lp(J; H 2 p(R n+1<br />
+ )).<br />
Concerning (4.29), we have the following result.<br />
, (4.29)<br />
, (4.30)<br />
Theorem 4.2.3 Let 1 < p < ∞, J = [0, T ], n ∈ N, and k ∈ K 1 (α, θ), where θ < π, and<br />
α ∈ (0, 2) \<br />
� 1<br />
p , 2<br />
2p−1<br />
1 3<br />
, 1 + p , 1 + 2p−1<br />
�<br />
. Suppose a ∈ Cul(J × R n+1<br />
+ , Sym{n + 1}), a1 ∈<br />
L∞(J × R n+1<br />
+ , Rn+1 ), a0 ∈ L∞(J × R n+1<br />
+ ), and assume further that there exists c0 > 0<br />
such that a(t, x)ξ · ξ ≥ c0|ξ| 2 , t ∈ J, x ∈ Rn+1 , ξ ∈ Rn+1 .<br />
Then (4.29) has a unique solution in the space Z if and only if the data f and g are<br />
subject to the <strong>conditions</strong> (i)-(vi) stated in Theorem 4.2.1.<br />
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