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 see that both summands in the formula for k(z, τ) lie in the sector Σ π/2+θa ∩ {z ∈<br />
C : Im(z) ≥ 0}. This means in particular k(z, τ) �= 0.<br />
Case 2: arg(1/ � da(z)) ≤ arg(1/ � db(z)). This time we have arg(κ) ∈ [0, θb], arg(1−κ) ≤<br />
0 and again |κ| < 1. We write k(z, τ) as<br />
k(z, τ) = ˆb(z) + 1<br />
3â(z) �<br />
â(z)<br />
1<br />
( ˆb(z) + 1<br />
+<br />
3â(z))τ 2<br />
4κ √ �<br />
ν + 1<br />
√ √ .<br />
ν + 1 + κν + 1<br />
Clearly, 1/[( ˆb(z) + 1/3â(z))τ 2 ] ∈ Σπ/2+θb ∩ {z ∈ C : Im(z) ≥ 0}. Now we look at the<br />
second summand. The inequality arg(1 − κ) ≤ 0 yields<br />
By employing (5.47), we get<br />
�<br />
κ<br />
arg<br />
√ �<br />
ν + 1<br />
√ √<br />
ν + 1 + κν + 1<br />
arg(1 + κν) = arg((1 − κ) + κ(1 + ν)) ≤ arg(κ(1 + ν))<br />
= arg(κ) + arg(1 + ν). (5.47)<br />
≥ arg(κ) + 1<br />
1<br />
2arg(1 + ν)− 2 max {arg(1 + ν), arg(1 + κν)}<br />
≥ 1<br />
2arg(κ) ≥ 0.<br />
On the other hand it is easy to see that<br />
�<br />
κ<br />
arg<br />
√ �<br />
ν + 1<br />
√ √<br />
ν + 1 + κν + 1<br />
≤ π 3<br />
4 + 2 θb.<br />
Therefore both summands in parentheses lie in the sector Σπ/2+θb ∩ {z ∈ C : Im(z) ≥ 0}.<br />
If arg(z) ∈ (−π/2, 0] then all signs of the arguments in the above lines change which<br />
means that the summands under consideration lie in the corresponding sectors in the<br />
lower half plane.<br />
By continuity of the argument function, there exists η > 0 such that, in each case, the<br />
summands under consideration lie in a sector of angle θ < π, for all (z, τ) ∈ Σ π<br />
2 +η × Ση.<br />
Consequently, there is c > 0 such that<br />
�<br />
|k(z, τ)| ≥ c |ν| +<br />
�<br />
�<br />
�<br />
4(1 − κ)<br />
�<br />
√ ��<br />
ν + 1 �<br />
√ √ �<br />
ν + 1 + κν + 1<br />
� ,<br />
for all (z, τ) ∈ Σ π<br />
2 +η × Ση. From the boundedness of the function ψ defined by<br />
ψ(ρ) =<br />
4 1 + 3 ρ<br />
1 + 1<br />
3 ρ , ρ ∈ Σ π<br />
2 +η,<br />
it follows that |1 − κ(z)| is bounded away from zero. We also see that the term<br />
� (κν + 1)/(ν + 1) is bounded, for all (z, τ) ∈ Σ π<br />
2 +η × Ση. Thus we obtain the desired<br />
estimate (5.46). �<br />
By (5.46), it follows that the function l0 defined by<br />
l0(z, τ) =<br />
ν + 2<br />
k(z, τ) , (z, τ) ∈ Σ π<br />
2 +η × Ση<br />
90<br />
(5.48)