Volume 2012, Article ID 549285,6pages doi:10.1155/2012/549285
Research Article
Integrability for Solutions of
Anisotropic Obstacle Problems
Hongya Gao, Yanjie Zhang, and Shuangli Li
College of Mathematics and Computer Science, Hebei University, Baoding 071002, China
Correspondence should be addressed to Hongya Gao,ghy@hbu.edu.cn
Received 30 March 2012; Revised 26 April 2012; Accepted 23 May 2012
Academic Editor: Martino Bardi
Copyrightq2012 Hongya Gao et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
This paper deals with anisotropic obstacle problem for the A-harmonic equation
n
i1Diaix, Dux 0. An integrability result is given under suitable assumptions, which
show higher integrability of the boundary datum, and the obstacle force solutionsuhave higher integrability as well.
1. Introduction and Statement of Result
LetΩbe a bounded open subset of Rn. Forpi>1,i1,2, . . . , n, we denotepmmaxi1,2,...,npi
andpis the harmonic mean ofpi, that is,
1
p
1 n
n
i1 1
pi. 1.1
The anisotropic Sobolev spaceW1,piΩis defined by
W1,piΩ v∈W1,1Ω:Div∈LpiΩfor everyi1,2, . . . , n. 1.2
Let us consider solutionsu∈W1,piΩof the followingA-harmonic equation:
n
i1
whereD D1, D2, . . . , Dnis the gradient operator, and the Carath´eodory functionsaix, ξ:
Ω×Rn → R,i1,2, . . . , n, satisfy
|aix, z| ≤c2hx |zi|pi−1, 1.4
for almost everyx∈Ω, for everyz∈Rn, and for anyi1,2, . . . , n, and there existsν∈0,∞
such that
ν n
i1
|zi−zi| pi ≤n
i1
aix, z−aix,zzi −zi, 1.5
for almost everyx∈Ω, for anyz,z∈Rn. The integrability condition forhx≥0 in1.4will
be given later.
Let ψ be any function in Ω with values in R∪ {±∞} and θ ∈ W1,piΩ, and we
introduce
Kpiψ,θΩ v∈W1,piΩ:v≥ψ, a.e.andv−θ∈W01,piΩ. 1.6
Note that
W01,piΩ v∈W01,1Ω:Div∈LpiΩfor everyi1,2, . . . , n. 1.7
The functionψis an obstacle andθdetermines the boundary values.
Definition 1.1. A solution to theKpiψ,θ-obstacle problem is a functionu∈ Kpiψ,θΩsuch that
Ω n
i1
aix, DuxDivx−Diuxdx≥0, 1.8
wheneverv∈ Kpiψ,θΩ.
Higher integrability property is important among the regularity theories of nonlinear
elliptic PDEs and systems, see the monograph1by Bensoussan and Frehse. Meyers and
Elcrat2first considered the higher integrability for weak solutions of1.3in 1975. Iwaniec
and Sbordone 3 obtained a regularity result for very weak solutions of theA-harmonic
equation1.3by using the celebrated Gehring’s Lemma. Global integrability for anisotropic
equation is contained in4. As far as higher integrability of∇uis concerned, in problems
with nonstandard growth a delicate interplay between the regularity with respect toxand
the growth with respect toξappears: see5. For a global boundedness result of anisotropic
variational problems, see6. For other related works, see7. We refer the readers to the
classical books by Ladyˇzenskaya and Ural’ceva8, Morrey9, Gilbarg and Trudinger10
and Giaquinta11for some details of isotropic cases.
In the present paper, we consider integrability for solutions of anisotropic obstacle
datum, and the obstacle force solutionsu, have higher integrability as well. The idea of this
paper comes from4, and the result can be considered as a generalization of4, Theorem 2.1.
Theorem 1.2. Letu ∈ Kpiψ,θΩbe a solution to the Kpiψ,θ obstacle problem andθ ∈ W1,qiΩ,
qi ∈pi,∞,i1,2, . . . , n, 0 ≤h∈LqmΩwithqm maxi1,...,nqi,ψ ∈−∞,∞is such that
θ∗max{ψ, θ} ∈θW01,qiΩ. Moreover,p < n. Then
u∈θ∗LtweakΩ, 1.9
where
t p
∗
1−bp∗/p pm/pm−1 > p
∗, 1.10
andbis any number verifying
0< b≤ min
j1,...,n
1−pj
qj
1− 1
pj
,
b <pm−1
pm p
p∗.
1.11
Remark 1.3. Take the obstacle function ψ to be minus infinity in Theorem 1.2, and the
condition1.4replaced by
|aix, z| ≤c21|zi|pi−1 1.2
for almost every x ∈ Ω, for every z ∈ Rn, and for any i 1,2, . . . , n, then we arrive at
Theorem 2.1 in4.
2. Proof of the Main Theorem
Proof ofTheorem 1.2. Letu ∈ Kpiψ,θΩbe a solution to theKpiψ,θ-obstacle problem. Takeθ∗
max{ψ, θ} ∈θW01,qiΩ. Let us considerL∈0,∞and
v
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
θ∗−L, foru−θ∗<−L,
u, for −L≤u−θ∗≤L,
θ∗L, foru−θ∗> L.
2.1
Thenv ∈ Kpiψ,θΩ. Indeed, for the second and the third cases of the above definition forv,
impliesvθ∗−L≥ψ. Sinceuθ∗θon∂Ω, thenvuon∂Ω, this impliesvθon∂Ω. By
Definition 1.1, one has
0≤
{|u−θ∗|>L}
n
i1
aix, DuxDivx−Diuxdx
{|u−θ∗|>L}
n
i1
aix, DuxDiθ∗x−Diuxdx.
2.2
Monotonicity1.5allows us to write
ν n i1
{|u−θ∗|>L}
|Diux−Diθ∗x|pidx
≤
{|u−θ∗|>L}
n
i1
aix, Dux−aix, Dθ∗xDiux−Diθ∗xdx,
2.3
which together with2.2implies
ν n i1
{|u−θ∗|>L}|Diux−Diθ∗x|
pidx
≤ −
{|u−θ∗|>L}
n
i1
aix, Dθ∗Diux−Diθ∗xdx.
2.4
We now use anisotropic growth1.4and the H ¨older inequality in2.4, obtaining that
ν n i1
{|u−θ∗|>L}|Diu−Diθ∗|
pi dx
≤ −n
i1
{|u−θ∗|>L}aix, Dθ∗Diu−Diθ∗dx
≤c2
n
i1
{|u−θ∗|>L}
h|Diθ∗|pi−1|Diu−Diθ∗|dx
≤c2
n
i1
{|u−θ∗|>L}h|Diθ∗|
pidx
pi−1/pi
{|u−θ∗|>L}|Diu−Diθ∗|
pidx
1/pi .
2.5
Lettibe such that
for everyi1, . . . , n;tiwill be chosen later. We use the H ¨older inequality as follows:
{|u−θ∗|>L}h|Diθ∗|
pi dx
pi−1/pi
≤
{|u−θ∗|>L}
h|Diθ∗|tidx
pi−1/ti
|{|u−θ∗|> L}|ti−pipi−1/tipi.
2.7
The following proof is similar to that of4, Theorem 2.1; we only list the necessary changes:
instead of4,3.14by
{|u−θ∗|>L}
h|Diθ∗|pidx
pi−1/pi
≤
{|u−θ∗|>L}h|Diθ∗|
ti dx
pi−1/ti
|{|u−θ∗|> L}|b
≤M|{|u−θ∗|> L}|b,
2.8
where
M max
j1,...,n
Ω
h|Djθ∗| tjdx
pj−1/tj
<∞, 2.9
and instead of4,3.19we use anisotropic Sobolev Embedding Theorem forv−u,
Ω|v−u|
p∗dx
1/p∗
≤c∗
n
i1
Ω|Div−u|
pidx
1/pi1/n
≤c∗
⎡
⎣n
i1
{|u−θ∗|>L}|Diu−Diθ∗|
pidx
1/pi⎤
⎦ 1/n
.
2.10
By|v−u| |u−θ∗| −L1{|u−θ∗|>L}, we obtain
{|u−θ∗|>L}|u−θ∗| −L
p∗
dx
1/p∗
Ω|v−u|
p∗
dx
1/p∗
. 2.11
Acknowledgment
The authors would like to thank the referee for valuable suggestions. Supported by NSFC
10971224and NSF of Hebei ProvinceA2011201011.
References
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