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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Turning to (c), let g ∈ Ξi+1 and v ∈ Zi+1(V −1<br />
i g). Evidently hij (g, v) ∈ Zi+1. If i > 0,<br />
we further have<br />
h ij (g, v)| [0,Ti] = (L ij<br />
i+1 (ϕjg + k ∗ Cj(·, x, Dx)v))| [0,Ti]<br />
= L ij<br />
i (ϕjg| [0,Ti] + k ∗ Cj(·, x, Dx)V −1<br />
i<br />
= ϕjV −1<br />
i<br />
g − Lij<br />
i<br />
g) (here ∗ is meant on [0, Ti])<br />
k ∗ (Aj<br />
# (·, x, Dx) − A j<br />
# (Ti, xj, Dx))ϕjV −1<br />
i g.<br />
Thus, w ∈ Zi+1(ϕjV −1<br />
i g) implies F (w) := Sijw + hij (g, v) ∈ Zi+1(ϕjV −1<br />
i g). In fact,<br />
(F (w))| [0,Ti] = L ij<br />
i k ∗ (Aj # (·, x, Dx) − A j<br />
# (Ti, xj, Dx))ϕjV −1<br />
i g + hij (g, v)| [0,Ti]<br />
= ϕjV −1<br />
i g.<br />
So F is a self-mapping of Zi+1(ϕjV −1<br />
i g). This is true for i = 0, too. Compare the<br />
initial values of all terms occurring above to see this. In view of (4.17), F is also a strict<br />
contraction. Hence the assertion follows by the contraction principle. �<br />
4.2 Half space <strong>problems</strong><br />
This section is devoted to <strong>parabolic</strong> <strong>problems</strong> of second order in a half space subject<br />
to general <strong>boundary</strong> <strong>conditions</strong>. In the first subsection we study the case in which the<br />
coefficients are constant and the differential operators consist only of their principal<br />
parts. Then we shall prove pointwise multiplication properties for the function spaces<br />
arising as the natural regularity classes on the <strong>boundary</strong>. These results allow us to treat<br />
also the case of variable coefficients by means of perturbation arguments. This will be<br />
done in the last part of this paragraph.<br />
4.2.1 Constant coefficients<br />
Let J = [0, T ] and R n+1<br />
+ = {x := (x′ , y) ∈ R n+1 : x ′ ∈ R n , y > 0}. We separately<br />
consider the <strong>problems</strong><br />
� u − k ∗ a : ∇ 2 xu = f, t ∈ J, x ∈ R n+1<br />
+ ,<br />
u = g, t ∈ J, x ′ ∈ R n , y = 0,<br />
� u − k ∗ a : ∇ 2 xu = f, t ∈ J, x ∈ R n+1<br />
+ ,<br />
−∂yu + b · ∇x ′u = h, t ∈ J, x′ ∈ R n , y = 0,<br />
(4.18)<br />
(4.19)<br />
where k is as in Section 4.1, a is an (n + 1)-dimensional real matrix, and b ∈ R n . We<br />
look for unique solutions u in the maximal regularity space<br />
As to (4.18), we have the following result.<br />
Z := H α p (J; Lp(R n+1<br />
+ )) ∩ Lp(J; H 2 p(R n+1<br />
+ )).<br />
Theorem 4.2.1 Let 1 < p < ∞, n ∈ N, and a ∈ Sym{n + 1}. Let further k ∈ K 1 (α, θ),<br />
where θ < π and α ∈ (0, 2) \<br />
definite.<br />
� 1<br />
p , 2<br />
2p−1<br />
1 3<br />
, 1 + p , 1 + 2p−1<br />
63<br />
�<br />
. Assume that a is positive