Skip to content


  • Research
  • Open Access

Hölder continuity of weak solution to a nonlinear problem with non-standard growth conditions

Boundary Value Problems20182018:131

  • Received: 14 June 2018
  • Accepted: 16 August 2018
  • Published:


We study the Hölder continuity of weak solution u to an equation arising in the stationary motion of electrorheological fluids. To this end, we first obtain higher integrability of Du in our case by establishing a reverse Hölder inequality. Next, based on the result of locally higher integrability of Du and difference quotient argument, we derive a Nikolskii type inequality; then in view of the fractional Sobolev embedding theorem and a bootstrap argument we obtain the main result. Here, the analysis and the existence theory of a weak solution to our equation are similar to the weak solution which has been established in the literature with \(\frac{3d}{d+2}\leq p_{\infty}\leq p(x)\leq p_{0}<\infty\), and in this paper we confine ourselves to considering \(p(x)\in(\frac{3d}{d+2},2)\) and space dimension \(d=2,3\).


  • Higher integrability
  • Hölder continuity
  • Nonlinear problem
  • Fractional Sobolev space
  • Electrorheological fluids

1 Introduction

Let \(\Omega\subset\mathbb{R}^{d}\ (d=2,3)\) be a bounded Lipschitz domain. This paper deals with a nonlinear problem (1.6) which arises in the steady motions of a special incompressible non-Newtonian fluid: electrorheological fluids, one example of smart fluids that change their viscosity rapidly when an electric field is applied. In the field of mechatronics, this fluid is actively being researched and numerous research activities on this fluid have been performed in various engineering applications. Also in the mathematical community such materials are intensively investigated being non-Newtonian fluids [9, 10, 1214, 34]. Note that one of the first mathematical investigations of non-Newtonian models was carried out by Ladyzhenskaya in 1966 [2628]; the author considered the modified Navier–Stokes equations
$$\begin{aligned} \textstyle\begin{cases} u_{t}-\operatorname{ div} a(Du)+D\phi=-\operatorname{ div}(u\otimes u)+f & \text{in } \Omega , \\ \operatorname{ div} u=0&\text{in } \Omega, \end{cases}\displaystyle \end{aligned}$$
where \(u:\Omega\longrightarrow\mathbb{R}^{d}, \phi:\Omega \longrightarrow\mathbb{R}\), are the unknown velocity, pressure, respectively. \(f:\Omega\longrightarrow\mathbb{R}^{d}\) is a given density of the bulk force. Du denotes the symmetric part of the velocity gradient u, namely \(Du=\frac{1}{2}(\nabla u+(\nabla u)^{T})\), \(a:\mathbb{R}^{d\times d}\longrightarrow\mathbb{R}^{d\times d}\) depends in a nonlinear way by Du. We note that there is abundant literature on the power-law model
$$ a(Du)=\nu_{0}\bigl(\nu_{1}+ \vert Du \vert ^{2}\bigr)^{\frac{q-2}{2}}Du+\nu_{2}Du, $$
with \(\nu_{0}>0, \nu_{1}, \nu_{2}\geq0\), here \(q>1\) is a positive constant. For example, the existence of measure-valued solutions was shown to (1.1)–(1.2) for \(q>\frac{2d}{d+2}\) in [29, 36], for \(q>\frac{2d}{d+2}\), the existence of a weak solution has been studied in [6, 15, 3032]. In [46], Wolf constructed a weak solution \(u\in L^{q}(0,T;V_{q}(\Omega))\cap C_{w}(0,T;L^{2}(\Omega))\) to (1.1)–(1.2) for the power with \(q>2\frac{d+1}{d+2}\). In 2014, Bae and Jin [5] studied the local in time existence of a weak solution to (1.1)–(1.2) for \(\frac{3d}{d+2}< q<2\) when \(d=2,3\) and the global in time existence of a weak solution for \(q\geq\frac{11}{5}\), when \(d=3\).
When q as a positive constant is replaced by a variable exponent \(p(x)\), then the model of (1.2) can be seen as the variable exponent power-law model. According to the model proposed by Rajagopal and Růžička [38, 41], the system of electrorheological fluids reads
$$ \textstyle\begin{cases} \operatorname{ div }E=0, \qquad \operatorname{ curl }E=0 & \text{in } \Omega, \\ E\cdot n=E_{0}\cdot n& \text{on } \partial\Omega,\\ u_{t}-\operatorname{ div} S(Du,E)+u\cdot\nabla u+\nabla\phi=f+\chi^{E}E\cdot \nabla E & \text{in } Q_{T}, \\ \operatorname{ div} u=0,\qquad u|_{t=0}=u_{0}& \text{in } Q_{T},\\ u=0& \text{on } \partial\Omega, \end{cases} $$
with \(f,E_{0},u_{0}\) are given. \(Q_{T}=[0,T]\times\Omega\), \(E:Q_{T}\longrightarrow\mathbb{R}^{d}\) is the electric field, \(u:Q_{T}\longrightarrow\mathbb{R}^{d}\) is the velocity, \(\phi :Q_{T}\longrightarrow\mathbb{R}\) is the pressure, \(f:Q_{T}\longrightarrow \mathbb{R}^{d}\) is the mechanical force and \(\chi^{E}\) is the positive constant dielectric susceptibility. \(S(D,E):\mathbb{R}^{d\times d}_{\mathrm{sym}}\times\mathbb{R}^{d}\longrightarrow\mathbb{R}^{d\times d}_{\mathrm{sym}}\) denotes the stress tensor, which is under non-standard growth conditions
$$\begin{aligned} S(Du,E)= {}& \alpha_{21}\bigl(\bigl(1+ \vert Du \vert ^{2}\bigr)^{\frac{p( \vert E \vert ^{2})-1}{2}}-1\bigr)E\otimes E \\ &{}+\bigl(\alpha_{31}+\alpha_{33} \vert E \vert ^{2}\bigr) \bigl(1+ \vert Du \vert ^{2} \bigr)^{\frac{p( \vert E \vert ^{2})-2}{2}}Du \\ &{} +\alpha_{51}\bigl(1+ \vert Du \vert ^{2} \bigr)^{\frac{p( \vert E \vert ^{2})-2}{2}}\bigl((Du)E\otimes E+E\otimes(Du)E\bigr). \end{aligned}$$
Here \(\alpha_{ij}\) are material constants such that
$$ \alpha_{31}>0, \qquad \alpha_{33}>0,\qquad \alpha_{33}+ \frac{4}{3}\alpha_{51}>0, $$
and \(p=p(|E|^{2})>1\) is continuous. We shall note that the system (1.4) is separated into the quasi-static Maxwell’s equation (1.4)1–(1.4)2 (cf. [25]) and the equation of motion and the conservation of mass (1.4)3-(1.4)5, where E can be viewed as a parameter.

Note that the higher differentiability of weak solutions to (1.3)–(1.4) had been obtained in [40, 41], the first regularity result for the model of electrorheological fluids proposed in [41], and in any case the first in a point-wise sense. A further step, the Hausdorff dimension of the singular set \(\Omega \backslash\Omega_{0}\) has been studied in [3]. Related regularity results in the stationary case can also be found in [1, 2, 10, 45] and the references therein. For the non-stationary case, one can refer [4, 41].

In this paper, we are interested in the (interior) regularity properties of weak solutions to the stationary case of (1.3)–(1.4):
$$ \operatorname{ div} u=0, \qquad {-}\operatorname{ div} S(Du,E)+u\cdot\nabla u+\nabla\phi =f+\chi^{E}E\cdot\nabla E. $$
The issue of regularity of solutions to (1.5) has been performed in [41] where the author proves the existence of a \(W^{2,2}\) solution to (1.5). Here we analyze the system arising from (1.5) as
$$ \textstyle\begin{cases} -\operatorname{ div} S(Du)+u\cdot\nabla u+\nabla\phi=f& \text{in } \Omega, \\ \operatorname{ div} u=0& \text{in } \Omega,\\ u=0& \text{on } \partial\Omega, \end{cases} $$
where \(f:\Omega\longrightarrow\mathbb{R}^{d}\), and
$$ S(Du)=\bigl(\mu_{0}+ \vert Du \vert ^{2} \bigr)^{\frac{p(x)-2}{2}}Du, $$
with \(\mu_{0}> 0\). \(p(\cdot):\Omega\longrightarrow[1,\infty) \) is a given Hölder (log-Hölder) continuous function that satisfies
$$ \frac{ 3d}{d+2}< p_{\infty}\leq p(x)\leq p_{0}< 2, \qquad \bigl\vert p(x)-p(y) \bigr\vert \leq \omega\bigl( \vert x-y \vert \bigr)\leq c_{0} \vert x-y \vert ^{2\theta_{1}}, $$
for all \(x,y\in\bar{\Omega}\), where \(c_{0}\geq1\) is a constant, \(\theta _{1}=\frac{A_{d}(d+2)-3d}{2A_{d}}\in(0,1)\) and \(A_{d}\) be a constant defined in (3.29), \(p_{\infty}:=\min_{x\in\bar{\Omega}}p(x)\) and \(p_{0}:=\max_{x\in\bar{\Omega}}p(x)\), \(\omega:\mathbb {R}^{+}\longrightarrow\mathbb{R}^{+}\) is the modulus of \(p(\cdot)\), which satisfies
$$ \omega(6R)< 1, \qquad\omega(R)\log\frac{1}{R}\leq L, $$
for all \(0< R\leq1\) and \(L>0\) is a constant. In this paper, we assume \(\mu_{0}=1\), then from the definition of \(S(Du)\),
$$ \bigl\vert S(Du) \bigr\vert \leq\bigl(1+ \vert Du \vert ^{2}\bigr)^{\frac{p(x)-1}{2}}. $$
The purpose of this paper is to study the Hölder continuity of a weak solution u to (1.6), to this end, various higher integrability results are important to overcome the lack of standard growth conditions of the system. Thus, we first improve the power of integrability of \(D u\in L^{p(x)}_{\mathrm{loc}}\), \(p(x)\in(1,2)\) by establishing a reverse Hölder inequality, and at this point, using the Gerhing lemma 2.4, we can deduce that \(Du\in L^{p(x)(1+\delta_{1})}\) for some positive constant \(\delta_{1}>0\). Next, by a difference quotient argument, we proceed to show the fractional differentiability of Du. For this purpose, we construct a Nikolskii type inequality (3.38), from which, by the fractional order Sobolev embedding theorem and a standard bootstrap argument, we have \(Du\in L^{\eta}\) with \(\eta\geq d\). Note that the self-improving property to a class of elliptic system was first observed by Elcrat and Meyers in [33] (see also [20] and [43]), but their argument is based on the reverse Hölder inequality and a modification of the Gehring lemma. Finally, by the Sobolev embedding theorem, we derive the Hölder continuity of u. In the whole paper, the key point is to suppose that \(p(\cdot)\) satisfies the log-Hölder conditions (1.8)–(1.9), which implies that
$$ \frac{1}{r}\sim\frac{1}{r^{p_{2}/p_{1}}}\quad \text{and}\quad \frac {1}{r}\sim \frac{1}{r^{p_{2}^{2}/p_{1}^{2}}}, $$
for all \(r\in(0,1]\) when \(p_{1}:=\inf_{x\in B_{3r}}p(x)\), \(p_{2}:=\sup_{x\in B_{3r}}p(x)\). Moreover, when \(p(x)\) satisfies the log-Hölder continuous conditions, one can use the Korn inequality with variable exponent case (Lemma 2.3), which is the main tool to prove the local higher integrability of u in terms of Du. We also observe that, for the sake of brevity and in order to highlight the main ideas, we confine ourselves to the considered homogeneous case of (1.6). For the non-homogeneous case (\(f\in W^{-1,p'(x)}(\Omega )\)), there are some technique difficulties in the proof of higher integrability of Du (Lemma 3.1), and we will investigate it in our future work. The result of this paper reads as follows.

Theorem 1.1

Suppose \(f=0\). Let \(\Omega\subset\mathbb{R}^{d}\) \((d=2,3)\) be a bounded domain with Lipschitz boundary Ω and let \(p(\cdot ):\Omega\longrightarrow(\frac{3d}{d+2},2)\) be log-Hölder continuous where \(\frac{3d}{d+2}< p_{\infty }\leq p\leq p_{0}<2\) satisfies (1.8)(1.9), and \(S(Du)\) satisfies (1.10). \((u,\phi)\in(V_{p(x)},L_{0}^{p'(x)}(\Omega))\) are the solutions of (1.6)(1.7). Then
$$ u\in C^{\alpha}(\Omega) \quad\textit{for some } \alpha\in(0,1). $$

The rest of paper is organized as follows. In Sect. 2, we present some notions of variable exponents spaces, the definition of a weak solution to (1.6), the property of a difference quotient with variable exponents, and formulate some lemma which will be used in later. In Sect. 3, we first prove the locally higher integrability of Du (Lemma 3.1). Next, by the known result of the difference quotient argument, the log-Hölder continuity of \(p(\cdot)\), we derive the fractional differentiability of Du, then, by the fractional Sobolev space embedding theorem and a standard bootstrap argument, we obtain the higher integrability of Du (the power of integrability is bigger than that in Lemma 3.1). At last, we prove the main result of Theorem 1.1.

2 Preliminaries

2.1 Basic notions

In the present paper we shall often write p or \(p(\cdot)\) instead of \(p(x)\) if there is no danger of confusion and the exponent q denotes a constant. c denotes a general constant which may vary in different estimates. If the dependence needs to be explicitly stressed, some notations like \(c', c_{0}, c_{1}, c(k_{0})\) will be used. \(A\sim B\) means there exist constants \(c_{1}\) and \(c_{2}\) such that \(c_{1}B\leq A\leq c_{2}B\). \(B_{r}(x_{0}):=\{x:\operatorname{dist}(x,x_{0})< r\}\), we denote the average integral of u on \(B_{r}\) as \((u)_{r}:=(u)_{B_{r}}=\frac{1}{|B_{r}|}\int_{B_{r}}u\,dx\). We recall in what follows some definitions and basic properties of the generalized Lebesgue–Sobolev spaces \(L^{p(x)}(\Omega)\) and \(W^{1,p(x)}(\Omega)\) (for more details one can refer to [8, 11, 1618, 2224, 37, 39, 44] and the references therein). Let \(P(\Omega)\) be the set consisting of a Lebesgue measurable function \(p(\cdot):\Omega\longrightarrow[1,\infty]\), where \(\Omega\subset\mathbb{R}^{d}\) \((d\geq2)\) is nonempty. Now, for any \(p(x)\in P(\Omega)\), let us introduce the spaces which are used in this paper,
$$\begin{aligned} &V_{p(x)}:= \bigl\{ u: u\in W^{1,p(x)}(\Omega), \operatorname{ div} u=0 \bigr\} , \\ &L_{0}^{p(x)}(\Omega):= \biggl\{ u: u\in L^{p(x)}( \Omega), \int _{\Omega }u\,dx=0 \biggr\} . \end{aligned}$$
Next, let us introduce the embedding properties of the generalized Lebesgue space. Firstly, we know that
$$ L^{p(x)}(\Omega) \hookrightarrow L^{q(x)}(\Omega), $$
if and only if
$$ q(x) < p(x) \quad\text{a.e. in $\Omega$} . $$
Moreover, if \(q\in P(\Omega)\) and \(q(x)< p^{*}(x)\) and for all \(x\in \bar {\Omega}\), then the embedding \(W^{1,p(x)}\hookrightarrow L^{q(x)}(\Omega )\) is compact and continuous, where \(p^{*}(x)=np(x)/(n-p(x))\) if \(p(x) < n\) or \(p^{*}(x)=+\infty\) if \(p(x)=n\). In what follows we denote \(L^{p'(x)}(\Omega)\) as the conjugate of \(L^{p(x)}(\Omega)\), where \(1/p(x)+1/p'(x)=1\), then for all \(p(x)\in P(\Omega),u\in L^{p(x)}(\Omega),v\in L^{p'(x)}(\Omega)\) we have
$$ \int_{\Omega} \bigl\vert u(x)v(x) \bigr\vert \,dx\leq2 \bigl\vert u(x)\bigr\vert _{L^{p(x)}} \bigl\vert v(x)\bigr\vert _{L^{p'(x)}}. $$
From the definition of variable exponent Lebesgue space above, now we introduce a basic property of \(L^{p(x)}(\Omega)\).

Lemma 2.1

Let \(p(x)\in P(\Omega)\) satisfy \(1\leq t_{1}\leq p(x)\leq t_{2}<\infty\), then for every \(u\in L^{p(x)}(\Omega)\)
$$ \min \bigl\{ \Vert u \Vert _{L^{p(x)}(\Omega)}^{t_{1}}, \Vert u \Vert _{L^{p(x)}(\Omega )}^{t_{2}} \bigr\} \leq \int_{\Omega} \vert u \vert ^{p(x)}\,dx\leq\max \bigl\{ \Vert u \Vert _{L^{p(x)}(\Omega)}^{t_{1}}, \Vert u \Vert _{L^{p(x)}(\Omega)}^{t_{2}} \bigr\} . $$
A proof can be retrieved e.g. from Lemma 3.2.5 in [11]. For convenience, we may denote inequality (2.2) as
$$ \Vert u \Vert _{L^{p(x)}(\Omega)}^{s_{1}}\leq \int_{\Omega} \vert u \vert ^{p(x)}\,dx\leq \Vert u \Vert _{L^{p(x)}(\Omega)}^{s_{2}}, $$
where \(s_{1},s_{2}\) equal to \(t_{1}\) or \(t_{2}\).

The following conclusion from fluid dynamics ensures local bounds of u in terms of Du on the scale of \(L^{q}\) space.

Lemma 2.2

(Korn inequality)

Let \(1<\gamma_{1}\leq q\leq\gamma_{2}\) and assume that \(u\in L^{q}(B_{r}(x_{0}),\mathbb{R}^{d})\) satisfies \(Du\in L^{q}(B_{r}(x_{0}),\mathbb {R}^{d\times d}_{\mathrm{sym}})\). Then \(\nabla u\in L^{q}(B_{r}(x_{0}),\mathbb {R}^{d\times d})\) and for a constant \(c=c(d,\gamma_{1},\gamma_{2})\) we have
Additionally, if \(u=0\) on \(\partial B_{r}(x_{0})\), then

Its proof may be found, e.g., in [35]. In addition, we shall use the Korn inequality with variable exponent case, and we formulate it in the form we need (cf. Theorem 14.3.23 in [11]).

Lemma 2.3

Let \(B_{r}\subset\mathbb{R}^{d}\) be a bounded ball, let \(p(x)\) satisfies \(log\)-Hölder conditions and \(1< p_{\infty}\leq p(x)\leq p_{0}<\infty \). Then
$$\begin{aligned} \begin{aligned} & \bigl\Vert \nabla u-(\nabla u)_{r} \bigr\Vert _{L^{p(x)}(B_{r})} \leq c \bigl\Vert D u-(D u)_{r} \bigr\Vert _{L^{p(x)}(B_{r})}, \\ & \Vert \nabla u \Vert _{L^{p(x)}(B_{r})}\leq c \bigl\Vert D u-(D u)_{r} \bigr\Vert _{L^{p(x)}(B_{r})}+\frac{c}{r} \bigl\Vert u-(u)_{r} \bigr\Vert _{L^{p(x)}(B_{r})}, \end{aligned} \end{aligned}$$
for all \(u\in W^{1,p(x)}(B_{r})\).

Next, we introduce the Gehring lemma in a version formulated by Giaqunta and Giusti (see, e.g., Chapter V, Proposition 1.1 in [20] or Theorem 6.6 in [21]).

Lemma 2.4

Let \(\Omega\subset R^{d}\), \(0< m<1\), and \(f\in L^{1}_{\mathrm{loc}}(\Omega)\), \(g\in L^{\sigma}_{\mathrm{loc}}(\Omega)\) for some \(\sigma>1\) be two nonnegative functions such that for any ball \(B_{\rho}\) with \(B_{3\rho}\subset \subset\Omega\)
where \(b_{1},b_{2}>1\) and \(0< k\leq k_{0}=k_{0}(m,d)\). Then there exists a constant \(\gamma_{0}=\gamma_{0}(d,m,b_{1})>1\) such that
$$ f\in L^{\gamma}_{\mathrm{loc}}\quad \textit{for all } 1< \gamma< \min\{ \gamma _{0},\sigma\}. $$

In order to show the interior higher integrability of Du, we shall use the following lemma, which is a well-known result (Bogovskii theorem), and we restate in the form we need (cf. [7, 19]).

Lemma 2.5

Let \(B_{R}\subset\mathbb{R}^{d}\) and let \(f\in L^{q}(B_{R})\) with \(1< q_{1}< q< q_{2}\) be such that \((f)_{R}=0\). Then there exists \(v\in W_{0}^{1,q}(B_{R}; \mathbb{R}^{d})\) satisfying
$$ \operatorname{ div} v=f $$
and such that
$$ \int_{B_{R}} \vert \nabla v \vert ^{q_{3}}\,dx\leq c \int_{B_{R}} \vert f \vert ^{q_{3}}\,dx, $$
for every \(q_{3}\in[q_{1},q]\), where \(c=c(d,q_{1},q_{2})\) is independent of \(R>0\). Moreover, if the support of f is contained in \(B_{r}\subset B_{R}\), the same result holds for v.
Recalling the structure of \(S=S(Du)\) in (1.7) with \(\mu_{0}=1\), then we have
$$\begin{aligned} S_{ij}(\xi)= \textstyle\begin{cases} (1+ \vert \xi \vert ^{2})^{\frac{p(x)-2}{2}}\xi_{ij},& \xi\in R^{d\times d}_{\mathrm{sym}}, \xi\neq0, \\ 0, & \xi=0, \end{cases}\displaystyle \end{aligned}$$
with \(\frac{3d}{d+2}< p_{\infty}\leq p(x)\leq p_{0}\leq2\). Define
$$ S(\xi):=A(x,\xi)=\bigl(1+ \vert \xi \vert ^{2} \bigr)^{\frac{p(x)-2}{2}}\xi, \quad \xi \in R^{d\times d}_{\mathrm{sym}}. $$
Then \(A:\Omega\times R^{d\times d}_{\mathrm{sym}}\longrightarrow R^{d\times d}_{\mathrm{sym}}\) satisfy
$$\begin{aligned} & \bigl\vert A(x,\xi)-A(x_{0},\xi) \bigr\vert \\ &\quad \leq\omega\bigl( \vert x-x_{0} \vert \bigr) \bigl[ \bigl(1+ \vert \xi \vert ^{2}\bigr)^{\frac{p(x)-1}{2}} + \bigl(1+ \vert \xi \vert ^{2}\bigr)^{\frac{p(x_{0})-1}{2}} \bigr]\bigl(1+\log\bigl(1+ \vert \xi \vert \bigr)\bigr), \end{aligned}$$
$$\begin{aligned} & A(x,\xi)\cdot\xi\geq \vert \xi \vert ^{p(x)}-1. \end{aligned}$$
From the definition of \(S_{ij}(\xi)\), we can also obtain
$$ \frac{\partial S_{ij}(\xi)}{\partial\xi_{kl}}=\bigl(p(x)-2\bigr) \bigl(1+ \vert \xi \vert ^{2}\bigr)^{\frac{p(x)-4}{2}}\xi_{kl}\xi_{ij}+ \bigl(1+ \vert \xi \vert ^{2}\bigr)^{\frac {p(x)-2}{2}} \delta_{ki}\delta_{lj}, $$
where \(\delta_{ij}\) is Kronecker’s delta, for all \(\xi,\eta\in R^{d\times d}_{\mathrm{sym}}, |\xi|+|\eta|>0\),
$$\begin{aligned} & \bigl(S_{ij}(\xi)-S_{ij}(\eta) \bigr) ( \xi_{ij}-\eta _{ij}) \\ &\quad = \int_{0}^{1}\frac{d}{dt}S_{ij} \bigl(\eta+t(\xi-\eta)\bigr)\,dt(\xi _{ij}-\eta _{ij}) \\ &\quad \geq \int_{0}^{1}\bigl(p(\cdot)-1\bigr) \bigl(1+\bigl( \eta+t(\xi-\eta)\bigr)^{2}\bigr)^{\frac {p(\cdot )-2}{2}} \vert \xi-\eta \vert ^{2}\,dt \\ &\quad \geq \int_{0}^{1}\bigl(p(\cdot)-1\bigr) \bigl(1+ \bigl\vert \eta+t(\xi-\eta) \bigr\vert \bigr)^{p(\cdot )-2} \vert \xi -\eta \vert ^{2}\,dt \\ &\quad \geq\bigl(p(\cdot)-1\bigr) \bigl(1+ \vert \xi \vert + \vert \eta \vert \bigr)^{p(\cdot)-2} \vert \xi-\eta \vert ^{2} \\ &\quad \geq k_{0}\bigl(1+ \vert \xi \vert + \vert \eta \vert \bigr)^{p(\cdot)-2} \vert \xi-\eta \vert ^{2}, \end{aligned}$$
where \(k_{0}=p_{\infty}-1\), and in the third inequality we have taken into account the inequality
$$ \bigl(1+ \vert \xi \vert + \vert \eta \vert \bigr)^{-(2-p(\cdot))}\leq \int_{0}^{1}\bigl(1+ \vert \xi+t\eta \vert \bigr)^{-(2-p(\cdot))}\,dt, \quad\text{a.e. in } \Omega. $$

2.2 The property of difference quotient

In the whole paper, we will employ the difference
$$ \triangle_{\lambda,k}u(x):=u(x+\lambda e_{k})-u(x), $$
where \(e_{k}=(0,\ldots,1,\ldots,0)\) and 1 at the kth place \((k=1,\ldots,d)\). Moreover, for simplicity, we may repeat, using the parameter \(p_{1}, p_{2}\):
$$ p_{1}:=\inf_{x\in B_{3r}}p(x),\qquad p_{2}:=\sup _{x\in B_{3r}}p(x). $$
Let \(B_{r}=B_{r}(x_{0})\subset\Omega\) be a ball such that \(\bar {B}_{6r}\subset \Omega\), in what follows, we will repeatedly use the following fact.

Lemma 2.6

Let \(1\leq p(\cdot)\leq q_{0}<\infty\) (\(q_{0}\) is a constant) and \(f\in W^{1,p(\cdot)}(\Omega)\), then, for all \(V\subset\subset\Omega \subset \mathbb{R}^{d}\), there exists a constant \(c>0\) such that
$$ \int_{B_{mr}} \vert \triangle_{\lambda,k}u \vert ^{p(x)}\,dx \leq c \vert \lambda \vert ^{p_{1}} \int_{B_{(m+1)r}} \biggl\vert \frac{\partial u}{\partial x_{k}} \biggr\vert ^{p(x)}\,dx, $$
for all \(|\lambda|< r<1, k=1,\ldots,d\), \(m=1,2\).


We first assume \(u(x)\) is smooth, then for all \(x\in V, i=1,2,\ldots ,d\) and \(0<|h|<\frac{1}{2}\operatorname{dist} (V,\partial\Omega)\)
$$ u(x+he_{i})-u(x)=h \int_{0}^{1}\frac{\partial u(x+the_{i})}{\partial x_{i}}\,dt, $$
from above, then we have
$$ \begin{aligned} \int_{V} \bigl\vert D^{h} u(x) \bigr\vert ^{p(\cdot)}\,dx={}& \int_{V} \Biggl\{ \sum_{i=1}^{d} \biggl\vert \frac{u(x+he_{i})-u(x)}{h} \biggr\vert ^{2} \Biggr\} ^{\frac {p(\cdot)}{2}}\,dx \\ \leq{}& \int_{V} \Biggl\{ \sum_{i=1}^{d} \biggl[ \int_{0}^{1} \bigl\vert \nabla u(x+the_{i}) \bigr\vert \,dt \biggr]^{2} \Biggr\} ^{\frac{p(\cdot)}{2}}\,dx \\ \leq{}& c\sum_{i=1}^{d} \int_{V} \int_{0}^{1} \bigl\vert \nabla u(x+the_{i}) \bigr\vert ^{p(\cdot )}\,dt\,dx \\ \leq{}&c \int_{\Omega} \bigl\vert \nabla u(x) \bigr\vert ^{p(\cdot)}\,dx, \end{aligned} $$
where c is independent of \(p(\cdot)\), and in the second inequality we have taken into account the fact
$$ \bigl( \bigl\vert u(x) \bigr\vert + \bigl\vert v(x) \bigr\vert \bigr)^{p(x)}\leq2^{\sup_{x\in V} p(x)-1}\bigl( \bigl\vert u(x) \bigr\vert ^{p(x)}+ \bigl\vert v(x) \bigr\vert ^{p(x)}\bigr),\quad p(x)\geq1. $$
Indeed, when \(|u|\) or \(|v|\) equal to zero, the above inequality is obvious, and without loss of generality, we may assume \(|u|,|v|\neq0\), and
$$ V=V_{1}\cup V_{2},\qquad V_{1}:= \bigl\{ x: \vert u \vert \geq \vert v \vert \bigr\} ,\qquad V_{2}:= \bigl\{ x: \vert v \vert \geq \vert u \vert \bigr\} . $$
It is only enough to consider \(|u|\geq|v|\) in \(V_{1}\), set \(t:=\frac {|u|}{|v|}\geq1\), observe the function
$$ f(t)=\frac{(1+t)^{p(x)}}{1+t^{p(x)}},\quad t\geq1, p(x)\geq1, $$
then we obtain, for any fixed x, \(\sup_{t\geq1}f(t)=2^{p(x)-1}\). Hence,
$$ \frac{(1+t)^{p(x)}}{1+t^{p(x)}}\leq2^{p(x)-1}, \quad\mbox{a.e. }x\in V_{1}, $$
whence (2.10) in \(V_{1}\), by set \(t:=\frac{|v|}{|u|}\), we have same conclusion in \(V_{2}\), thus we obtain (2.10). From the definition of a generalized Lebesgue space, we obtain (2.9) if u is smooth, then, for all \(u\in W^{1,p(\cdot)}(\Omega)\), (2.9) holds. □

2.3 Definition of the weak solutions to (1.6)

Suppose \(\frac{3d}{d+2}\leq p_{\infty}\leq p(x)\leq p_{0}<\infty\), and \(f\in W^{-1,p'(\cdot)}(\Omega)\) is given, then \((u,\phi)\in (V_{p(\cdot)}, L_{0}^{p(\cdot)'}(\Omega) )\) is said to be a weak solution to (1.6)–(1.10), if and only if
$$ \int_{\Omega}S(Du)\cdot D\varphi \,dx- \int_{\Omega}u\otimes u\cdot \nabla \varphi\, dx- \int_{\Omega}\phi\operatorname{ div} \varphi\,dx+(f, \varphi)=0, $$
for all \(\varphi\in W_{0}^{1,p(x)}(\Omega)\), or
$$ \int_{\Omega}S(Du)\cdot D\varphi\, dx- \int_{\Omega}u\otimes u\cdot \nabla \varphi\, dx+(f, \varphi)=0, $$
for all \(\varphi\in V_{p(x)}\). For more details, one can refer for instance to [11] (Chap. 14, Sect. 4, p. 472) or [41].

3 Hölder continuity of weak solutions

We note that the starting point for any comparison and freezing argument in the setting of variable \(p(x)\)-growth problems is a quantitative higher integrability result. Hence, in order to obtain the interior differentiability of weak solution to (1.6), we shall first show the locally higher integrability of Du. At this point, we define a global positive constant \(\alpha\in(1, [(d+2)p_{\infty }-d]/2d)\), from which we then have the following result.

Lemma 3.1

Suppose \(f=0\). Let \(\Omega\subset\mathbb{R}^{d}\) \((d=2,3)\) be a bounded domain with Lipschitz boundary Ω and let \(p(\cdot ):\Omega\longrightarrow(\frac{3d}{d+2},2)\) be log-Hölder continuous with \(\frac{3d}{d+2}< p_{\infty}\leq p\leq p_{0}<2\) satisfying (1.8) and (1.9), and S satisfying (1.10). \((u,\phi)\in(V_{p(x)},L_{0}^{p'(x)}(\Omega))\) is the solution of (1.6)(1.7). Then there exist constants \(c,\delta_{1}>0\) both depending on \(d,p_{0},p_{\infty}\) and \(r_{0}\in(0,1)\) suitable small, such that if \(B_{2r}\subset\subset\Omega\) for any \(r\in(0,r_{0})\), then


Without loss of generality, we first set \(r_{0}=\frac{1}{2}\), and we will specify it in later. Let \(\eta\in C_{0}^{\infty}(B_{2r})\) with \(r\in (0,r_{0})\) be a cut-off function such that
$$ \textstyle\begin{cases} \eta=1& \text{in } B_{r},\\ 0\leq\eta\leq1& \text{in } B_{2r},\\ \vert \nabla\eta \vert \leq\frac{c}{r}& \text{in } B_{2r}, \end{cases} $$
where c is a positive constant independent of r. Let
$$ \varphi=\eta^{2}\bigl(u-(u)_{2r}\bigr)+w, $$
where the function w is defined according to Lemma 2.5 as a solution to
$$ \operatorname{ div} w=-\operatorname{ div}\bigl(\eta^{2} \bigl(u-(u)_{2r}\bigr)\bigr)=-\bigl(u-(u)_{2r}\bigr)\cdot \nabla \bigl(\eta^{2}\bigr). $$
It is obvious that such a function w exists, since
$$ \operatorname{ div} u=0,\qquad \int_{B_{2r}}\bigl(u-(u)_{2r}\bigr)\cdot\nabla\bigl( \eta ^{2}\bigr) \,dx=0. $$
We claim that \(w\in W_{0}^{1,p_{2}}(B_{2r})\). In fact, from Lemma 2.5, we have
for some exponent \(q>p_{2}\) such that the right hand side is finite.
Taking into account (2.12), we let φ in (3.2) be a test function, thus
$$\begin{aligned} 0= {}& \int_{B_{2r}} \eta^{2} S(Du)\cdot Du\,dx+2 \int_{B_{2r}}\eta S(Du)\cdot \bigl(\bigl(u-(u)_{2r} \bigr)\cdot\nabla\eta\bigr)\,dx \\ & {}+ \int_{B_{2r}} S(Du)\cdot Dw\,dx+ \int_{B_{2r}}(u\cdot\nabla u)\cdot \bigl(\bigl(u-(u)_{2r} \bigr)\eta^{2}\bigr)\,dx \\ &{}+ \int_{B_{2r}}(u\cdot\nabla u)\cdot w\,dx \\ :={}&I_{1}+I_{2}+I_{3}+I_{4}+I_{5}. \end{aligned}$$
Now, we estimate the terms \(I_{1}\)\(I_{5}\). Using (2.7), we first infer that
$$ I_{1}\geq \int_{B_{2r}}\eta^{2} \vert Du \vert ^{p(x)}\,dx-cr^{d} . $$
Note that \(2p'(x)\geq2\) and \(\eta\in[0,1]\), thus, by (1.10) and the Young inequality
$$ \vert I_{2} \vert \leq\varepsilon \int_{B_{2r}}\eta^{2} \vert Du \vert ^{p(x)}\,dx +c(\varepsilon ) \int_{B_{2r}} \biggl\vert \frac{u-(u)_{2r}}{r} \biggr\vert ^{p(x)}\,dx+cr^{d}, $$
where ε is a positive constant that will be specified later.
Likewise, taking into account (3.4), we arrive at
$$\begin{aligned} \vert I_{3} \vert \leq{}&\varepsilon \int_{B_{2r}} \vert Du \vert ^{p(x)}\,dx+c( \varepsilon) \int _{B_{2r}} \vert Dw \vert ^{p(x)} \,dx+cr^{d} \\ \leq{}& \varepsilon \int_{B_{2r}} \vert Du \vert ^{p(x)}\,dx+c( \varepsilon) \int _{B_{2r}} \biggl\vert \frac{u-(u)_{2r}}{r} \biggr\vert ^{p_{2}}\,dx+cr^{d}. \end{aligned}$$
Observe that
$$ \bigl\Vert u-(u)_{2r} \bigr\Vert _{L^{q}(B_{2r})}\leq c(q) \Vert u \Vert _{L^{q}(B_{2r})} $$
for any \(q\geq1\), with \(c(q)\geq1\). Thus, appealing to the Young and Hölder inequalities, we have
$$\begin{aligned} \vert I_{4} \vert \leq{}& \Vert \nabla u \Vert _{L^{ (\frac{1}{2} (\frac {p_{\infty }}{\alpha} )^{*} )'}(B_{2r})} \bigl\Vert u-(u)_{2r} \bigr\Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r})} \Vert u \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r}) } \\ \leq{}& c \Vert \nabla u \Vert _{L^{ (\frac{1}{2} (\frac{p_{\infty }}{\alpha } )^{*} )'}(B_{2r})} \Vert u \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r})}^{2} \\ \leq{}&c \int_{B_{2r}} \vert \nabla u \vert ^{\frac{dp_{\infty}}{(d+2)p_{\infty }-2d\alpha}}\,dx+c \int_{B_{2r}} \vert u \vert ^{ (\frac{p_{\infty}}{\alpha } )^{*}}\,dx. \end{aligned}$$
Similarly, using the Hölder and Young inequalities again, from the property of w in (3.4) and noting that \(w\in W_{0}^{1,p_{2}}(B_{2r})\), the term \(I_{5}\) can be estimated as
$$\begin{aligned} \vert I_{5} \vert \leq{}& \Vert \nabla u \Vert _{L^{\frac{dp_{\infty}}{(d+2)p_{\infty }-2d\alpha }}(B_{2r})} \Vert u \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r}) } \Vert w \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r})} \\ \leq{}& c \Vert \nabla u \Vert _{L^{\frac{dp_{\infty}}{(d+2)p_{\infty}-2d\alpha }}(B_{2r})} \Vert u \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r})} \Vert \nabla w \Vert _{L^{\frac{p_{\infty}}{\alpha}}(B_{2r})} \\ \leq{}& c \Vert \nabla u \Vert _{L^{\frac{dp_{\infty}}{(d+2)p_{\infty}-2d\alpha }}(B_{2r})} \Vert u \Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r}) } \bigl\Vert u-(u)_{2r} \bigr\Vert _{L^{ (\frac{p_{\infty}}{\alpha} )^{*}}(B_{2r})} \\ \leq{}&c \int_{B_{2r}} \vert \nabla u \vert ^{\frac{dp_{\infty}}{(d+2)p_{\infty }-2d\alpha}}\,dx+c \int_{B_{2r}} \vert u \vert ^{ (\frac{p_{\infty}}{\alpha } )^{*}}\,dx. \end{aligned}$$
Inserting the estimation (3.6)–(3.10) into (3.5) and choosing \(\varepsilon=\frac{1}{4}\), we conclude that
Next, we shall show a reverse Hölder inequality. In view of the Sobolev–Poincaré and Korn inequalities in Lemma 2.2, the last term on the right hand side of (3.11) can be estimated as
where \(c=c(d,p_{0},p_{\infty})\) and in the fourth inequality, we have taken into account that \(p_{2}\alpha/p_{\infty}>1\) and \(\int_{B_{2r}}|\nabla u|^{p_{\infty}/\alpha}\,dx\leq1\) for any \(r\in (0,r_{0}']\) with \(r_{0}'\leq1\) suitable small, since we have absolute continuity of the integral. At this stage, we have determined \(r_{0}=\min\{\frac{1}{2},r_{0}'\}\).
Now, inserting (3.12) into (3.11), we conclude that
Taking into account Lemma 2.4, we set
$$\begin{aligned} &g:= \vert \nabla u \vert ^{\frac{dp_{\infty}}{(d+2)p_{\infty}-2d\alpha }}+ \vert \nabla u \vert ^{\frac{p_{\infty}}{\alpha}} + \vert u \vert ^{ (\frac{p_{\infty}}{\alpha} )^{*}}+1, \\ &f:= \vert Du \vert ^{p(x)}. \end{aligned}$$
From the definition of α, we can see that
$$ \frac{d}{(d+2)p_{\infty}-2d\alpha}\in(0,1), \qquad \biggl(\frac{p_{\infty}}{\alpha} \biggr)^{*}< \frac{p_{\infty}^{*}}{\alpha}< p_{\infty}^{*}. $$
Thus, we infer that \(g\in L^{\sigma}(B_{2r})\) for some \(\sigma=\sigma (d,p_{\infty},\alpha)=\sigma(d,p_{\infty})>1\). At this point, there exists a constant \(\delta_{1}>0\) such that \(\gamma=1+\delta_{1}\) in Lemma 2.4, then the result (3.1) holds. □

Based on the interior higher integrability of Du, we now turn to a proof of the Hölder continuity of u. For the main difficult result from the difference quotient of \(S(Du)\) in (3.15), for dealing with it, we need the monotonicity (2.8) and the growth condition (2.6) of \(S(\cdot)\). Furthermore, we may repeatedly use the log-Hölder property of \(p(x)\) and the local higher integrability of Du.

Proof of Theorem 1.1

For \(i,j=1,2,\ldots,d\). Let \(\xi\in C_{0}^{\infty}\) be a cut-off function for \(B_{2r}\), i.e.,
$$ \textstyle\begin{cases} \xi=1 &\text{in } B_{r},\\ 0\leq\xi\leq1&\text{in } B_{2r},\\ \vert \frac{\partial\xi}{\partial x_{i}} \vert \leq\frac{c}{r},\qquad \vert \frac{\partial^{2} \xi}{\partial x_{i}\,\partial x_{j}} \vert \leq\frac{c}{r^{2}} & \text{in } B_{2r}, \end{cases} $$
where \(c>0\) is a positive constant independent of r. Define
$$ \varphi=\triangle_{-\lambda,k}\bigl(\xi^{2} \triangle_{\lambda,k}u\bigr), $$
where \(|\lambda|< r<1\), \(k=1,\ldots,d\). One can see that φ is an admissible test function in (2.11). Now we divide the proof into several steps.
Step 1 (Fractional differentiability of Du). To begin with, we choose φ in (3.14) as a test function, inserting it into (2.11) with \(f=0\), which implies
$$\begin{aligned} & \int_{B_{2r}}S_{ij}(Du)D_{ij}\bigl( \triangle_{-\lambda,k}\bigl(\xi ^{2}\triangle _{\lambda,k}u\bigr) \bigr)\,dx+ \int_{B_{2r}}u_{i}\partial_{i} u_{j} \triangle _{-\lambda ,k}\bigl(\xi^{2} \triangle_{\lambda,k}u_{j}\bigr)\,dx \\ &\quad = \int_{B_{2r}}\phi\partial_{i}\bigl( \triangle_{-\lambda,k}\bigl(\xi ^{2}\triangle _{\lambda,k}u_{i} \bigr)\bigr) \,dx. \end{aligned}$$
Observe that
$$\begin{aligned} & \int_{B_{2r}}S_{ij}(Du)D_{ij}\bigl( \triangle_{-\lambda,k}\bigl(\xi ^{2}\triangle _{\lambda,k}u\bigr) \bigr)\,dx \\ &\quad= \int_{B_{2r}} \bigl[\triangle_{\lambda ,k}S_{ij}(Du) \bigr]\xi^{2}\triangle_{\lambda,k}D_{ij} u\,dx \\ &\qquad{} + \int_{B_{2r}}S_{ij}(Du)\triangle_{-\lambda,k} \biggl(\xi \biggl(\frac {\partial\xi}{\partial x_{i}}\triangle_{\lambda,k}u_{j}+ \frac{\partial \xi }{\partial x_{j}}\triangle_{\lambda,k}u_{i} \biggr) \biggr)\,dx \end{aligned}$$
$$\begin{aligned} &\triangle_{\lambda,k}S(Du) \\ &\quad = \bigl(1+ \bigl\vert Du(x+ \lambda e_{k}) \bigr\vert ^{2}\bigr)^{\frac{p(x+\lambda e_{k})-2}{2}}Du(x+ \lambda e_{k}) \\ &\qquad{}-\bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2}\bigr)^{\frac{p(x+\lambda e_{k})-2}{2}}Du(x) \\ &\qquad{}+ \bigl[ \bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2} \bigr)^{\frac{p(x+\lambda e_{k})-2}{2}}Du(x)-\bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2} \bigr)^{\frac{p(x)-2}{2}}Du(x) \bigr]. \end{aligned}$$
Then from (2.8) we arrive at
$$\begin{aligned} &k_{0} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(x+\lambda e_{k})-2} \cdot \vert \triangle_{\lambda,k}Du \vert ^{2}\xi ^{2}\,dx \\ &\quad \leq - \int_{B_{2r}}S_{ij}(Du)\triangle_{-\lambda,k} \biggl(\xi \biggl(\frac{\partial\xi}{\partial x_{i}}\triangle_{\lambda,k}u_{j}+ \frac {\partial \xi}{\partial x_{j}}\triangle_{\lambda,k}u_{i} \biggr) \biggr)\,dx \\ &\qquad{}- \int_{B_{2r}}u_{i}\partial_{i}u_{j} \bigl(\triangle_{-\lambda,k} \bigl(\xi ^{2}\triangle_{\lambda,k}u_{j} \bigr) \bigr)\,dx + \int_{B_{2r}}\phi\partial_{i} \bigl( \triangle_{-\lambda,k} \bigl(\xi ^{2}\triangle_{\lambda,k}u_{i} \bigr) \bigr)\,dx \\ &\qquad{}- \int_{B_{2r}} \bigl[ \bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2}\bigr)^{\frac{p(x+\lambda e_{k})-2}{2}}D_{ij}u(x)-\bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2}\bigr)^{\frac{p(x)-2}{2}}D_{ij}u(x) \bigr] \\ &\qquad{}\times\triangle_{\lambda,k}D_{ij}u\,dx \\ &\quad =:H_{1}+H_{2}+H_{3}+H_{4}. \end{aligned}$$
Since \(p(x)\) is Hölder continuous, we can choose \(0< r<1\) suitable small such that
$$ p_{2}\leq p_{1}(1+\delta_{1})\leq p(x) (1+ \delta_{1}). $$
By Lemma 3.1, we can see that
$$\begin{aligned} &k_{0} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(x+\lambda e_{k})-2} \cdot \vert \triangle_{\lambda,k}Du \vert ^{2}\xi ^{2}\,dx \\ &\quad\leq k_{0} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p_{2}-2} \cdot \vert \triangle_{\lambda,k}Du \vert ^{2}\xi^{2}\,dx \\ &\quad\leq ck_{0} \int_{B_{3r}} \bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)^{p_{2}} \,dx\leq c. \end{aligned}$$
From the previous inequality, one can see that, for suitable small \(r\in (0,1]\) and \(|\lambda|< r\),
$$ \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(x+\lambda e_{k})-2} \cdot \vert \triangle_{\lambda,k}Du \vert ^{2}\xi^{2}\,dx< 1, $$
this conclusion will be heavily used in the following estimate. Furthermore, taking into account the Korn inequality (2.4) and (3.1), we are in a position to obtain
$$ \int_{B_{2r}} \vert \nabla u \vert ^{p(x+\lambda e_{k})}\,dx< \int_{B_{3r}}\bigl( \vert \nabla u \vert ^{p_{2}}+1 \bigr)\,dx\leq c $$
for all \(|\lambda|< r\), where c is a determined positive constant independent of λ, and from now on \(r\in(0,1]\) is a fixed constant. For simplicity of notation, in the following paper, we may denote \(p(x+\lambda e_{k})\) as \(p(\bar{x})\). Now, we turn to an estimate of \(H_{1}\), \(H_{3}\)\(H_{4}\).
Estimation of \(H_{1}\). By Hölder inequality with variable exponent, from (1.10), (2.3) and (2.9), we find that
$$\begin{aligned} H_{1}\leq{}& 2\sum_{i,j=1} ^{d} \bigl\Vert S_{ij}(Du) \bigr\Vert _{L^{p'(\bar {x})}(B_{2r})} \\ &{}\times \biggl\Vert \triangle_{-\lambda,k} \biggl(\xi \biggl( \frac {\partial\xi }{\partial x_{i}}\triangle_{\lambda,k}u_{j}+\frac{\partial\xi }{\partial x_{j}} \triangle_{\lambda,k}u_{i} \biggr) \biggr) \biggr\Vert _{L^{p(\bar {x})}(B_{2r})} \\ \leq{}& c \vert \lambda \vert ^{p_{1}/p_{2}} \biggl( \int_{B_{2r}} \bigl(1+ \vert D u \vert ^{p(\bar{x})} \bigr) \,dx \biggr)^{\frac{1}{q_{1}}} \\ &{}\times\sum_{i,j=1} ^{d} \biggl\Vert \frac{\partial}{\partial x_{k}} \biggl(\xi \biggl(\frac{\partial\xi}{\partial x_{i}}\triangle _{\lambda ,k}u_{j}+\frac{\partial\xi}{\partial x_{j}}\triangle_{\lambda ,k}u_{i} \biggr) \biggr) \biggr\Vert _{L^{p(\bar{x})}(B_{2r})} \\ \leq{}& c \frac{ \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{q_{1}}} \\ &{} \times\biggl[ \frac{ \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{s_{1}}} + \bigl\Vert \xi\nabla(\triangle_{\lambda,k}u) \bigr\Vert _{L^{p(\bar {x})}(B_{2r})} \biggr], \end{aligned}$$
for all \(0<|\lambda|<r<1\), and \(s_{1}\) equal to \(p_{1}\) or \(p_{2}\), \(q_{1}\) equal to \(p_{1}'\) or \(p_{2}'\), and in the last inequality we have used the fact \(|Du|\leq|\nabla u|\). Note that
$$ \xi\nabla(\triangle_{\lambda,k}u)=\nabla(\xi\triangle_{\lambda,k}u )- \nabla\xi\triangle_{\lambda,k}u \quad\text{and}\quad \bigl(\nabla(\xi \triangle _{\lambda,k}u)\bigr)_{2r}=0= \bigl(D(\xi\triangle_{\lambda,k}u) \bigr)_{2r}. $$
Thus, by the Korn inequality (2.5), we infer that
$$\begin{aligned} & \bigl\Vert \xi\nabla(\triangle_{\lambda,k}u) \bigr\Vert _{L^{p(\bar {x})}(B_{2r})} \\ &\quad\leq \bigl\Vert \nabla(\xi\triangle_{\lambda,k}u) \bigr\Vert _{L^{p(\bar{x})}(B_{2r})} + \Vert \nabla\xi\triangle_{\lambda,k}u \Vert _{L^{p(\bar {x})}(B_{2r})} \\ &\quad\leq \bigl\Vert D(\xi\triangle_{\lambda,k}u) \bigr\Vert _{L^{p(\bar{x})}(B_{2r})} + \Vert \nabla\xi\triangle_{\lambda,k}u \Vert _{L^{p(\bar {x})}(B_{2r})} \\ &\quad\leq c \biggl( \int_{B_{2r}} \bigl\vert \xi D(\triangle_{\lambda,k}u) \bigr\vert ^{p(\bar {x})}\,dx \biggr)^{\frac{1}{s_{1}}} +c\frac{ \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int_{B_{2r}} \vert \nabla u \vert ^{p(\bar{x})}\,dx \biggr)^{\frac{1}{s_{1}}}, \end{aligned}$$
where in the last inequality, for simplicity, we just denote the exponent as \(1/s_{1}\), and it cannot add any confusion when the exponent is replaced by one of another character.
Now, inserting (3.20) into (3.19), we obtain
$$\begin{aligned} H_{1} \leq{}&\frac{c \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{q_{1}}+\frac{1}{s_{1}}} \\ &{}+ \frac{c \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac{1}{q_{1}}}\cdot \biggl( \int_{B_{2r}} \bigl\vert \xi D (\triangle_{\lambda,k}u) \bigr\vert ^{p(\bar{x})} \,dx \biggr)^{\frac{1}{s_{1}}} \\ :={}& A+B. \end{aligned}$$
Taking into account (3.18), we can see that the term A in the previous inequality is bounded from above for fixed r suitable small. On the other hand, observe that, for any suitable function \(f,g\) and \(q\leq s<2\), by the Hölder inequality,
$$\begin{aligned} \int \vert f \vert ^{s}\,dx&= \int\bigl( \vert g \vert ^{\frac{s(q-2)}{2}} \vert f \vert ^{s}\bigr) \vert g \vert ^{\frac {s(2-q)}{2}}\,dx \\ &\leq \bigl\Vert \vert g \vert ^{\frac{s(q-2)}{2}} \vert f \vert ^{s} \bigr\Vert _{L^{\frac{2}{s}}}\bigl\Vert |g|^{\frac{s(2-q)}{2}}\bigr\Vert _{L^{\frac{2}{2-s}}}. \end{aligned}$$
Thus, in order to estimate the term B in (3.21), take
$$ g=\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr),\qquad f=\xi D (\triangle _{\lambda,k}u), $$
\(s=q=p(\bar{x})\) in previous inequality. If \(\frac{t_{1}}{s_{1}}\geq1\), by the Hölder inequality, the Young inequality with \(k_{0}/4\) and (2.3), we obtain
$$\begin{aligned} B\leq{}& \frac{c \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda,k}u) \bigr\vert ^{2} \xi ^{2}\,dx \biggr)^{\frac{t_{1}}{2s_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac{2-t_{2}}{2s_{1}}} \\ \leq{}&\frac{k_{0}}{4} \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx \biggr)^{\frac{t_{1}}{s_{1}}} \\ &{}+c(k_{0})\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {2}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})} \,dx \biggr)^{\frac{2-t_{2}}{s_{1}}} \\ \leq{}&\frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx \\ &{}+c(k_{0})\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {2}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})} \,dx \biggr)^{\frac{2-t_{2}}{s_{1}}}, \end{aligned}$$
where \(t_{1}, t_{2}\) are equal to \(p_{1}\) or \(p_{2}\), and in the last inequality we have used the fact \(\frac{t_{1}}{s_{1}}\geq1\) and (3.17).
Likewise, if \(0<\frac{t_{1}}{s_{1}}<1\), that is, \(t_{1}=p_{1}, s_{1}=p_{2}\), by the Hölder inequality, the Young inequality with \(k_{0}/4\) and (2.3), we arrive at
$$\begin{aligned} B\leq{}& \frac{c \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda,k}u) \bigr\vert ^{2} \xi ^{2}\,dx \biggr)^{\frac{p_{1}}{2p_{2}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac{2-t_{2}}{2p_{2}}} \\ \leq{}&\frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx \\ &{}+c(k_{0}) \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac{2p_{2}}{q_{1}(2p_{2}-p_{1})}} \\ &{}\times\frac{ \vert \lambda \vert ^{2p_{1}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}(2p_{2}-p_{1})}} \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})} \,dx \biggr)^{\frac{2-t_{2}}{2p_{2}-p_{1}}} \\ \leq{}&\frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx \\ &{}+c(k_{0}) \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac{2p_{2}}{q_{1}(2p_{2}-p_{1})}} \\ &{}\times\frac{ \vert \lambda \vert ^{2p_{1}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})} \,dx \biggr)^{\frac{2-t_{2}}{2p_{2}-p_{1}}}. \end{aligned}$$
Combining (3.22) with (3.23), we obtain
$$\begin{aligned} B \leq{}& \frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx \\ &{}+c(k_{0})\frac{ \vert \lambda \vert ^{2p_{1}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {2p_{2}}{q_{1}(2p_{2}-p_{1})}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})} \,dx \biggr)^{\frac{2-t_{2}}{2p_{2}-p_{1}}} \\ &{} +c(k_{0})\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {2}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})} \,dx \biggr)^{\frac{2-t_{2}}{s_{1}}}. \end{aligned}$$
Inserting (3.24) into (3.21), we finally obtain
$$\begin{aligned} H_{1}\leq{}& \frac{c \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}}\biggl[ \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac {1}{q_{1}}+\frac {1}{s_{1}}} \\ &{}+ \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p\bar{x})} \bigr)\,dx \biggr)^{\frac{2}{q_{1}}} \\ &{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac {2-t_{2}}{s_{1}}} \biggr] \\ &{}+c\frac{ \vert \lambda \vert ^{2p_{1}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \biggl( \int_{B_{2r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar{x})} \bigr)\,dx \biggr)^{\frac{2p_{2}}{q_{1}(2p_{2}-p_{1})}} \\ & {}\times\biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})} \,dx \biggr)^{\frac{2-t_{2}}{2p_{2}-p_{1}}} \\ &{} +\frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda ,k}u) \bigr\vert ^{2} \xi^{2} \,dx, \end{aligned}$$
for all \(0<|\lambda|<r<1\).
Estimation of \(H_{3}\). To begin with, we note that
$$ \frac{\partial}{\partial x_{i}} \bigl( \triangle_{-\lambda,k} \bigl(\xi^{2} \triangle_{\lambda,k}u_{i} \bigr) \bigr)=2 \biggl( \triangle _{-\lambda ,k} \biggl(\xi\frac{\partial\xi}{\partial x_{i}} \triangle_{\lambda ,k}u_{i} \biggr) \biggr), $$
then from (2.9), (2.3), similar to (3.24), we can see that
$$\begin{aligned} H_{3}= {}& 2 \int_{B_{2r}}\phi \biggl(\triangle_{-\lambda,k} \biggl(\xi \frac {\partial\xi}{\partial x_{i}} \triangle_{\lambda,k}u_{i} \biggr) \biggr)\,dx \\ \leq{}& c \vert \lambda \vert ^{p_{1}/p_{2}} \Vert \phi \Vert _{L^{p'(\bar{x})}(B_{2r})} \biggl( \int_{B_{2r}} \biggl\vert \nabla \biggl(\xi\frac{\partial\xi}{\partial x_{i}} \triangle_{\lambda,k}u_{i} \biggr) \biggr\vert ^{p(\bar{x})} \,dx \biggr)^{\frac {1}{t_{3}}} \\ \leq{}&c \vert \lambda \vert ^{p_{1}/p_{2}} \Vert \phi \Vert _{L^{p'(x)}(B_{3r})} \\ &{}\times \biggl[\frac{ \vert \lambda \vert ^{p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl( \int _{B_{2r}} \vert \nabla u \vert ^{p(\bar{x})}\,dx \biggr)^{\frac{1}{t_{3}}} + \frac{1}{r^{p_{2}/p_{1}}} \biggl( \int_{B_{2r}} \bigl\vert \xi D(\triangle _{\lambda ,k }u) \bigr\vert ^{p(\bar{x})}\,dx \biggr)^{\frac{1}{s_{1}}} \biggr] \\ \leq{}&c\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \Vert \phi \Vert _{L^{p'(x)}(B_{3r})} \biggl( \int_{B_{3r}} \bigl(1+ \vert \nabla u \vert ^{p(\bar {x})} \bigr)\,dx \biggr)^{\frac{1}{t_{3}}} \\ &{}+c\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \Vert \phi \Vert ^{2}_{L^{p'(x)}(B_{3r})} \biggl( \int _{B_{2r}}\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac{2-t_{2}}{s_{1}}} \\ &{}+c(k_{0})\frac{ \vert \lambda \vert ^{2p_{2}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \Vert \phi \Vert _{L^{p'(x)}(B_{3r})}^{2p_{2}/(2p_{2}-p_{1})} \\ &{}\times \biggl( \int_{B_{2r}}\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})}\,dx \biggr)^{\frac{2-t_{2}}{2p_{2}-p_{1}}} \\ &{}+\frac{k_{0}}{4} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda,k}u) \bigr\vert ^{2} \xi^{2} \,dx, \end{aligned}$$
where \(t_{3}\) is equal to \(p_{1}\) or \(p_{2}\), and we replace \(t_{3}\) by \(s_{1}\) in the second inequality if there is no danger of any possible confusion, since from (3.19) and (3.21), we infer that \((\int_{B_{2r}}|\xi D(\triangle_{\lambda,k }u)|^{p}\,dx )^{\frac {1}{s_{1}}} \) is biggest for all cases of the value of \(t_{3}\).
Estimation of \(H_{4}\). Now, since \(0< r<1\) is suitably small, we have
$$ p_{2}\biggl(1+\frac{\delta_{1}}{4}\biggr)\leq p_{1}(1+ \delta_{1})\leq p(x) (1+\delta_{1}). $$
From (2.6) and Lemma 3.1, we can find that
$$\begin{aligned} H_{4} \leq{}& c\omega\bigl( \vert \lambda \vert \bigr) \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x) \bigr\vert ^{2}\bigr)^{\frac {p_{2}-1}{2}} \\ &{}\times\bigl(\log\bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)+1\bigr) \bigl( \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr) \,dx \\ \leq{}&c\omega\bigl( \vert \lambda \vert \bigr) \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)^{p_{2}} \bigl(\log ^{\frac{p_{2}}{p_{2}-1}}\bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)+1 \bigr) \\ &{}+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert ^{p_{2}} \,dx \\ \leq{}& c \vert \lambda \vert ^{2\theta_{1}} \int_{B_{3r}} \bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)^{p_{2}(1+\frac {\delta_{1}}{4})} \,dx \\ \leq{}& c \vert \lambda \vert ^{2\theta_{1}} \int_{B_{3r}} \bigl(1+ \bigl\vert Du(x) \bigr\vert \bigr)^{p(x)(1+\delta _{1})} \,dx\leq c\frac{\lambda^{2\theta_{1}}}{r^{\delta_{1}\,d}}, \end{aligned}$$
for all \(0<|\lambda|\leq r\).
Inserting (3.25)–(3.27) into (3.16), we finally obtain
$$\begin{aligned} &\frac{k_{0}}{2} \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2}\cdot \bigl\vert D(\triangle_{\lambda,k}u) \bigr\vert ^{2} \xi^{2} \,dx \\ &\quad \leq H_{2}+ c\frac{ \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2p_{2}/p_{1}}} \biggl[ \biggl( \int_{B_{3r}} \bigl(1+ \vert \nabla u \vert ^{p(x)} \bigr) \,dx \biggr)^{\frac {1}{q_{1}}+\frac{1}{s_{1}}} \\ &\qquad{}+ \Vert \phi \Vert _{L^{p'(x)}(B_{3r})} \biggl( \int_{B_{3r}} \bigl(1+ \vert \nabla u \vert ^{p(x)} \bigr)\,dx \biggr)^{\frac{1}{t_{3}}} \\ &\qquad{} + \biggl( \Vert \phi \Vert ^{2}_{L^{p'(x)}(B_{3r})} + \biggl( \int _{B_{3r}} \bigl( 1+ \vert \nabla u \vert ^{p(x)} \bigr)\,dx \biggr)^{\frac {2}{q_{1}}} \biggr) \\ &\qquad{}\times \biggl( \int_{B_{2r}}\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})}\,dx \biggr)^{\frac{2-t_{2}}{s_{1}}} \biggr] \\ &\qquad{} +\frac{ \vert \lambda \vert ^{2p_{2}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \biggl( \int _{B_{2r}}\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac {2-t_{2}}{2p_{2}-p_{1}}} \\ &\qquad{}\times \biggl( \int_{B_{3r}} \bigl(1+ \vert \nabla u \vert ^{p(x)} \bigr)\,dx \biggr)^{\frac{2p_{2}}{q_{1}(2p_{2}-p_{1})}} \\ &\qquad{} +\frac{ \vert \lambda \vert ^{2p_{2}/(2p_{2}-p_{1})}}{r^{2p_{2}^{2}/p_{1}^{2}}} \biggl( \int _{B_{2r}}\bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})}\,dx \biggr)^{\frac {2-t_{2}}{2p_{2}-p_{1}}} \\ &\qquad{}\times \Vert \phi \Vert _{L^{p'(x)}(B_{3r})}^{2p_{2}/(2p_{2}-p_{1})}+c \frac{\lambda ^{2\theta_{1}}}{r^{\delta_{1}d}}. \end{aligned}$$
Estimation of \(H_{2}\). To estimate \(H_{2}\), we first note that
$$\begin{aligned} H_{2}= {}& \int_{B_{2r}} (\triangle_{\lambda,k }u_{i} ) \frac {\partial u_{j}(x+\lambda e_{k})}{\partial x_{i}}\xi^{2}\triangle_{\lambda,k} u_{j} \,dx \\ &{}+ \int_{B_{2r}}u_{i} \biggl(\triangle_{\lambda,k} \frac{\partial u_{j}}{\partial x_{i}} \biggr)\xi^{2}\triangle_{\lambda,k} u_{j}\,dx \\ := {}& C+D, \end{aligned}$$
where \(i,j=1,\ldots,d\). From now on, we assume for the moment that we have proved
$$ u\in W^{1,s}_{\mathrm{loc}}(\Omega), $$
with \(s\in[p_{\infty},A_{d}]\), \(A_{d}\leq d\), and
$$\begin{aligned} A_{d}:= \textstyle\begin{cases} d, & d=2, \\ \frac{3p_{0}d}{(d+2)p_{0}-2\bar{p}_{\infty}}, & d=3, \end{cases}\displaystyle \end{aligned}$$
here we denote \(3d/(d+2)\) by \(\bar{p}_{\infty}\), we will see that the assumption of (3.29) is valid later. From the Hölder inequality, we have
$$ C\leq \int_{B_{2r}} \vert \triangle_{\lambda,k}u \vert ^{2} \bigl\vert \nabla u(x+\lambda e_{k}) \bigr\vert \,dx\leq c \Vert \triangle_{\lambda,k}u \Vert _{L^{2s'}(B_{2r})}^{2} \Vert u \Vert _{W^{1,s}(B_{3r})}. $$
We let \(s^{*}=\frac{ds}{d-s}\), since \(s<2s'<s^{*}\), by interpolation, it follows that
$$ \Vert \triangle_{\lambda,k}u \Vert _{L^{2s'}(B_{2r})}^{2} \leq \Vert \triangle _{\lambda ,k}u \Vert _{L^{s^{*}}(B_{2r})}^{2(1-\theta)} \cdot \Vert \triangle_{\lambda ,k}u \Vert _{L^{s}(B_{2r})}^{2\theta} \leq c \vert \lambda \vert ^{2\theta} \Vert u \Vert ^{2}_{W^{1,s}(B_{3r})}, $$
with \(\theta=\frac{s(d+2)-3d}{2s}\).
Combining (3.30) with (3.31), we arrive at
$$ C\leq c \vert \lambda \vert ^{2\theta} \Vert u \Vert ^{3}_{W^{1,s}(B_{3r})}. $$
For the term D, by integration by parts, we get
$$ D=- \int_{B_{2r}}u_{i}(\triangle_{\lambda,k}u_{j})^{2} \xi\frac{\partial \xi }{\partial x_{i}}\,dx. $$
Similar to the estimation of the term C, we obtain
$$\begin{aligned} D \leq& \frac{c}{r} \Vert \triangle_{\lambda,k}u \Vert _{L^{2s'}(B_{2r})}^{2} \Vert u \Vert _{W^{1,s}(B_{3r})} \leq \frac{c}{r} \vert \lambda \vert ^{2\theta} \Vert u \Vert ^{3}_{W^{1,s}(B_{3r})}. \end{aligned}$$
Together (3.32) with (3.33), we finally obtain
$$ H_{2}\leq c \biggl(1+\frac{1}{r} \biggr) \lambda^{2\theta} \Vert u \Vert ^{3}_{W^{1,s}(B_{3r})}\leq \frac{c\lambda^{2\theta}}{r^{2}} \Vert u \Vert ^{3}_{W^{1,s}(B_{3r})}. $$
Since \(s\in[p_{\infty},A_{d}]\), we can see that
$$ \textstyle\begin{cases} \frac{p_{1}}{p_{2}}\geq\frac{p_{\infty}}{p_{0}}\geq\theta,\\ \frac{2p_{1}}{2p_{2}-p_{1}}\geq\frac{2p_{\infty}}{2p_{0}-p_{\infty}}\geq \theta, \end{cases} $$
and from (1.8), (1.9), we have
$$ r^{-(p_{2}-p_{1})}=2^{p_{2}-p_{1}}e^{(p_{2}-p_{1})\log\frac{1}{2r}}\leq 2^{p_{2}-p_{1}}e^{\omega(2r)\log\frac{1}{2r}}\leq c(L), $$
for all \(0< r<1\). Moreover, since \(\delta_{1}\) is independent of r, we can choose \(\delta\in(0,\delta_{1}]\) to be a constant, replacing \(\delta _{1}\) by δ in (3.27), such that \(\delta d\leq2\). Now, taking into account (3.35), (3.36), inserting (3.34) into (3.28), we finally obtain
$$\begin{aligned} & \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar {x})-2}\cdot \bigl\vert \triangle_{\lambda,k}D(u) \bigr\vert ^{2} \xi ^{2}\,dx \\ &\quad\leq\frac{c \vert \lambda \vert ^{2p_{1}/p_{2}}}{r^{2(1+(p_{2}-p_{1})/p_{1})}}+\frac {c \vert \lambda \vert ^{2p_{1}/(2p_{2}-p_{1})}}{r^{2(1+(p_{2}-p_{1})(p_{2}+p_{1})/p_{1}^{2})}} +\frac{c}{r^{2}} \vert \lambda \vert ^{2\theta}+c\frac{\lambda^{2\theta _{1}}}{r^{\delta d}} \\ &\quad \leq\frac{c}{r^{2}} \vert \lambda \vert ^{2\theta}, \end{aligned}$$
for all \(0<|\lambda|<r<1\) with c depends on \(\Vert u \Vert _{W_{\mathrm{loc}}^{p(x)}(\Omega)}\), \(\Vert u \Vert _{W^{1,s}_{\mathrm{loc}}(\Omega)}\), L and \(\Vert \phi \Vert _{L^{p'(x)}_{\mathrm{loc}}(\Omega)}\), and in the last inequality we have used the fact \(\theta_{1}\geq\theta\).
In what follows, we set
$$ \gamma:=\frac{2s}{s+2-\bar{p}_{\infty}}\in \biggl[\frac{2p_{\infty }}{2p_{\infty}+2-\bar{p}_{\infty}},\frac{2A_{d}}{2A_{d}+2-\bar {p}_{\infty }} \biggr]. $$
Observe that
$$ \frac{2s(\gamma-2)}{2\gamma}=\bar{p}_{\infty}-2 \quad\text{for all } s \in[p_{\infty},A_{d}]. $$
Taking into account (3.19), with the aid of the Hölder inequality, we infer that
$$\begin{aligned} & \int_{B_{r}} \bigl\vert \triangle_{\lambda,k} D(u) \bigr\vert ^{\gamma}\,dx \\ &\quad\leq \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{\bar{p}_{\infty}-2} \bigl\vert \triangle_{\lambda,k}D(u) \bigr\vert ^{2} \xi ^{2}\,dx \biggr)^{\frac{\gamma}{2}} \\ &\qquad{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{s}\,dx \biggr)^{\frac{2-\gamma}{2}} \\ &\quad\leq \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{p(\bar{x})-2} \bigl\vert \triangle_{\lambda,k}D(u) \bigr\vert ^{2} \xi^{2}\,dx \biggr)^{\frac{\gamma}{2}} \\ &\qquad{}\times \biggl( \int_{B_{2r}} \bigl(1+ \bigl\vert Du(x+\lambda e_{k}) \bigr\vert + \bigl\vert Du(x) \bigr\vert \bigr)^{s}\,dx \biggr)^{\frac{2-\gamma}{2}} \leq\frac{c \vert \lambda \vert ^{\gamma\theta}}{r^{2}}, \end{aligned}$$
where in the first inequality, we have taken into account \(\frac {\gamma }{2-\gamma}(2-\bar{p}_{\infty})=s\).
Appealing to (3.38), the equivalence of the Nikolskii fractional space and the Sobolev space [42], we have
$$ Du\in W^{t,\gamma}_{\mathrm{loc}}(\Omega), \quad\text{for all } t\in [0,\theta], $$
then the fractional order Sobolev embedding theorem implies that
$$ Du \in L^{\frac{d\gamma}{d-t\gamma}}\quad \text{for all } t\in [0,\theta]. $$
Step 2 (Higher integrability of Du). We set
$$ T(s):=\frac{d\gamma}{d-\theta\gamma}=\frac{4sd}{10d-2\bar {p}_{\infty}d-4s}. $$
Then, from the definition of \(\bar{p}_{\infty}\), by a direct calculation, we find that
$$ T(s)-s\geq\sigma:=\frac{6d+2\bar{p}_{\infty}d+4p_{\infty }}{10d-2\bar {p}_{\infty}d-4p_{\infty}}>0. $$
Taking into account (3.39), (3.40), we obtain
$$ Du\in L^{\eta}(B_{\frac{r}{2}}), \quad\text{for all } \eta\in \bigl[1,T(s)\bigr]. $$
We use that \(u\in V_{p(x)}\) is any weak solution to (1.6) and \(p(x)\geq p_{\infty}\). Thus, we claim that \(s=p_{\infty}\) such that (3.29) holds. We set
$$ s_{0}:=p_{\infty},\qquad s_{1}:=s_{0}+ \frac{\sigma}{2}. $$
In virtue of (3.40), we see that
$$ T(s_{0})>s_{1}>s_{0}=p_{\infty}. $$
Taking into account (3.41),
$$ Du\in L^{s_{1}}(B_{\frac{r}{2}}). $$
By the Korn inequality, we have
$$ u\in W^{1,s_{1}}_{\mathrm{loc}}(\Omega), $$
from the above, it follows that (3.29) holds with \(s=s_{1}\). Now, if \(s_{1}> A_{d}\), we have proved the higher integrability of Du, and we can derive the Hölder continuity of u by the Sobolev imbedding theorem, since \(Du\in L^{\eta}(B_{\frac{ r}{2}})\) for all \(\eta\in [1,T(A_{d})]\), and \(T(A_{d})> d\). If \(s_{1}\leq A_{d}\), we continue the process above, such that there is a \(s_{i}> A_{d}\) \((i>1)\). Without loss of generality, we assume that \(s_{1}\leq A_{d}\), then from (3.29), (3.39)–(3.42),
$$ Du\in L^{\eta_{1}}(B_{\frac{r}{2}}),\quad \eta_{1}\in \bigl[1,T(s_{1})\bigr]. $$
Note that \(T(s_{1})>T(s_{0})\), then we can increase the power of integrability of Du by a standard bootstrap argument. We set
$$ \tilde{s}:=\sup \bigl\{ s\in[p_{\infty},A_{d}]: u \in W^{1,s}_{\mathrm{loc}}(\Omega ) \bigr\} . $$
We may assume that \(s=A_{d}\), otherwise, \(s< A_{d}\). Define
$$ \bar{s}:=\tilde{s}-\frac{\sigma}{4}, $$
by the definition of , we can obtain \(u\in W^{1,\bar {s}}_{\mathrm{loc}}(\Omega)\), since \(\tilde{s}>p_{\infty}+\sigma\). From (3.41), it follows that
$$ Du\in L^{\eta}(B_{\frac{r}{2}}), \quad\text{for all } \eta\in \bigl[1,T( \bar{s})\bigr]. $$
Then, choose \(\eta:=T(\bar{s})-\frac{\sigma}{4}\), and taking into account (3.40), we find that
$$ \eta\geq\bar{s}+\sigma-\frac{\sigma}{4}\geq\tilde{s}+\frac {\sigma}{2}, $$
it contradicts (3.43).
By the conclusion above, from now on we have
$$ u\in W^{1,s}_{\mathrm{loc}}(\Omega), \quad\text{for all } s \in[p_{\infty},A_{d}], $$
then, from (3.41), we have
$$ u\in W^{1,T(s)}_{\mathrm{loc}}(\Omega),\quad \text{for all } s\in [p_{\infty},A_{d}]. $$
Note that \(T(A_{d})>T(s)\), thus
$$ u\in W^{1,\eta}_{\mathrm{loc}}(\Omega), \quad\text{for all } \eta\in \bigl[p_{\infty},T(A_{d})\bigr], $$
with \(T(A_{d})> d\). Now, making use of the Sobolev embedding theorem, from (3.44), \(u\in C^{\alpha}(\Omega)\), for some \(\alpha\in(0,1)\). □



The authors wish to thank the referees and the editor for their valuable comments and suggestions.

Availability of data and materials

Not applicable.


This work was supported by the National Natural Science Foundation of China (No. 11271305, 11531010). The second author was partially supported by the China Scholarship Council (No. 20170631 0012) as an exchange Ph.D. student at Purdue University.

Authors’ contributions

Each of the authors contributed to each part of this study equally, all authors read and approved the final manuscript.

Competing interests

The authors declare that they have no competing interests.

Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

School of Mathematical Sciences, Xiamen University, Xiamen, P.R. China
School of Mechanical and Electronic Engineering, Tarm University, Alar, P.R. China


  1. Acerbi, E., Mingione, G.: Regularity results for a class of functionals with nonstandard growth. Arch. Ration. Mech. Anal. 156, 121–140 (2001) MathSciNetView ArticleMATHGoogle Scholar
  2. Acerbi, E., Mingione, G.: Regularity results for electrorheological fluids: the stationary case. C. R. Acad. Sci. Paris, Ser. I 334, 817–822 (2002) MathSciNetView ArticleMATHGoogle Scholar
  3. Acerbi, E., Mingione, G.: Regularity results for stationary electro-rheological fluids. Arch. Ration. Mech. Anal. 164, 213–259 (2002) MathSciNetView ArticleMATHGoogle Scholar
  4. Acerbi, E., Mingione, G., Seregin, G.: Regularity results for parabolic systems related to a class of non-Newtonian fluids. Ann. Inst. Henri Poincaré, Anal. Non Linéaire 21(1), 25–60 (2004) MathSciNetMATHGoogle Scholar
  5. Bae, H.O., Jin, B.J.: Regularity of non-Newtonian fluids. J. Math. Fluid Mech. 16, 225–241 (2014) MathSciNetView ArticleMATHGoogle Scholar
  6. Bellout, H., Bloom, F., Nečas, J.: Young measure-valued solutions for non-Newtonian incompressible fluids. Commun. Partial Differ. Equ. 19, 1763–1803 (1994) MathSciNetView ArticleMATHGoogle Scholar
  7. Bogovskii, M.E.: Solutions of some problems of vector analysis, associated with the operators div and grad. In: Theory of Cubature Formulas and the Application of Functional Analysis to Problems of Mathematical Physics. Trudy Sem. S. L. Soboleva, vol. 1, pp. 5–40. Akad. Nauk SSSR Sibirsk. Otdel., Inst. Mat., Novosibirsk (1980) Google Scholar
  8. Bonanno, G., Molica Bisci, G., Rădulescu, V.: Infinitely many solutions for a class of nonlinear eigenvalue problem in Orlicz–Sobolev spaces. C. R. Math. Acad. Sci. Paris 349(5–6), 263–268 (2011) MathSciNetView ArticleMATHGoogle Scholar
  9. Diening, L.: Theoretical and numerical results for electrorheological fluids. PhD thesis, University of Freiburg, Germany (2002) Google Scholar
  10. Diening, L., Ettwein, F., Růžička, M.: \(C^{1,\alpha}\)-Regularity for electrorheological fluids in two dimensions. Nonlinear Differ. Equ. Appl. 14(1–2), 207–217 (2007) View ArticleMATHGoogle Scholar
  11. Diening, L., Harjulehto, P., Hästö, P., Růžička, M.: Lebesgue and Sobolev Spaces with Variable Exponents. Springer, Berlin (2011) View ArticleMATHGoogle Scholar
  12. Diening, L., Málek, J., Steinhauer, M.: On Lipschitz truncations of Sobolev functions (with variable exponent) and their selected applications. ESAIM Control Optim. Calc. Var. 14(2), 211–232 (2008) MathSciNetView ArticleMATHGoogle Scholar
  13. Diening, L., Růžička, M.: Strong solutions for generalized Newtonian fluids. J. Math. Fluid Mech. 7, 413–450 (2005) MathSciNetView ArticleMATHGoogle Scholar
  14. Diening, L., Růžička, M.: An existence result for non-Newtonian fluids in nonregular domains. Discrete Contin. Dyn. Syst., Ser. S 3, 255–268 (2010) MathSciNetView ArticleMATHGoogle Scholar
  15. Diening, L., Růžička, M., Wolf, J.: Existence of weak solutions for unsteady motions of generalized Newtonian fluids. Ann. Sc. Norm. Super. Pisa, Cl. Sci. 9(1), 1–46 (2010) MathSciNetMATHGoogle Scholar
  16. Edmunds, D., Rákosník, J.: Sobolev embeddings with variable exponent. Stud. Math. 143(3), 267–293 (2000) MathSciNetView ArticleMATHGoogle Scholar
  17. Edmunds, D., Rákosník, J.: Sobolev embeddings with variable exponent II. Math. Nachr. 246/247, 53–67 (2002) MathSciNetView ArticleMATHGoogle Scholar
  18. Fu, Y., Shan, Y.: On the removability of isolated singular points for elliptic equations involving variable exponent. Adv. Nonlinear Anal. 5(2), 121–132 (2016) MathSciNetMATHGoogle Scholar
  19. Galdi, G.P.: An Introduction to the Mathematical Theory of the Navier–Stokes Equations. Vol. 1. Linearized Steady Problems. Springer Tracts in Natural Philosophy, vol. 38. Springer, Berlin (1994) MATHGoogle Scholar
  20. Giaquinta, M.: Multiple Integrals in the Calculus of Variations and Nonlinear Elliptic Systems. Princeton Univ. Press, Princeton (1983) MATHGoogle Scholar
  21. Giusti, E.: Direct Methods in the Calculus of Variations. World Scientific, Singapore (2003) View ArticleMATHGoogle Scholar
  22. Ho, K., Sim, I.: A-priori bounds and existence for solutions of weighted elliptic equations with a convection term. Adv. Nonlinear Anal. 6(4), 427–445 (2017) MathSciNetMATHGoogle Scholar
  23. Hudzik, H.: The problems of separability, duality, reflexivity and of comparison for generalized Orlicz–Sobolev spaces \(W^{k}_{M }(\Omega)\). Comment. Math. Prace Mat. 21, 315–324 (1979) MATHGoogle Scholar
  24. Kovácik, O., Rákosník, J.: On spaces \(L^{p(x)}\) and \(W^{k,p(x)}\). Czechoslov. Math. J. 116(41), 592–618 (1991) MATHGoogle Scholar
  25. Kristály, A., Repovš, D.: On the Schrödinger–Maxwell system involving sublinear terms. Nonlinear Anal., Real World Appl. 13(1), 213–223 (2012) MathSciNetView ArticleMATHGoogle Scholar
  26. Ladyzhenskaya, O.A.: New equations for description of motion of viscous incompressible fluids and global solvability of boundary value problems for them. Proc. Steklov Inst. Math. 102 95–118 (1967) Google Scholar
  27. Ladyzhenskaya, O.A.: On nonlinear problems of continuum mechanics. In: Proc. Internat. Congr. Math. Proc. Internat. Congr. Math. (Moscow 1966), pp. 560–573. Nauka, Moscow (1968) English translation in: Amer. Math. Soc. Translation (2) 70 (1968) Google Scholar
  28. Ladyzhenskaya, O.A.: On some modifications of the Navier–Stokes equations for large gradient of velocity. Zap. Nauchn. Sem. LOMI 7, 126–154 (1968) English translation in: Sem. Math. V.A. Steklov Math. Inst. Leningrad 7 (1968) Google Scholar
  29. Málek, J., Nečas, J., Novotný, A.: Measure-valued solutions and asymptotic behavior of a multipolar model of a boundary layer. Czechoslov. Math. J. 42(117), 549–576 (1992) MathSciNetMATHGoogle Scholar
  30. Málek, J., Nečas, J., Rokyta, M., Růžička, M.: Weak and Measure-Valued Solutions to Evolutionary Partial Differential Equations. Applied Mathematics and Mathematical Computation, vol. 13. Chapman & Hall, London (1996) MATHGoogle Scholar
  31. Málek, J., Nečas, J., Růžička, M.: On the non-Newtonian incompressible fluids. Math. Models Methods Appl. Sci. 3(1), 35–63 (1993) MathSciNetView ArticleMATHGoogle Scholar
  32. Málek, J., Nečas, J., Růžička, M.: On weak solutions to a class of non-Newtonian incompressible fluids in bounded three-dimensional domains: the case \(p \geq 2\). Adv. Differ. Equ. 6(3), 257–302 (2001) MathSciNetMATHGoogle Scholar
  33. Meyers, N.G., Elcart, A.: Some results on regularity of weak solutions of nonlinear elliptic system. J. Reine Angew. Math. 311/312, 145–169 (1979) Google Scholar
  34. Mihăilescu, M., Rădulescu, V.: A multiplicity result for a nonlinear degenerate problem arising in the theory of electrorheological fluids. Proc. R. Soc. Lond., Ser. A, Math. Phys. Eng. Sci. 462(2073), 625–2641 (2006) MathSciNetMATHGoogle Scholar
  35. Mosolov, P., Mjasnikov, V.: On the correctness of boundary value problems in the mechanics of continuous media. Mat. Sb. 88(130), 256–267 (1972) MathSciNetGoogle Scholar
  36. Nečas, J.: Theory of multipolar viscous fluids. In: The Mathematics of Finite Elements and Applications, VII (Uxbridge, 1990), pp. 233–244. Academic Press, London (1991) Google Scholar
  37. Rădulescu, V.D., Repovš, D.D.: Partial Differential Equations with Variable Exponents. Variational Methods and Qualitative Analysis. Monographs and Research Notes in Mathematics. CRC Press, Boca Raton (2015) View ArticleMATHGoogle Scholar
  38. Rajagopal, K., Růžička, M.: On the modeling of electrorheological materials. Mech. Res. Commun. 23, 401–407 (1996) View ArticleMATHGoogle Scholar
  39. Repovš, D.: Stationary waves of Schrödinger-type equations with variable exponent. Anal. Appl. (Singap.) 13(6), 645–661 (2015) MathSciNetView ArticleMATHGoogle Scholar
  40. Růžička, M.: Flow of shear dependent electrorheological fluids: unsteady space periodic case. In: Sequeira, A. (ed.) Appl. Nonlinear Anal, pp. 485–504. Plenum, New York (1999) Google Scholar
  41. Růžička, M.: Electrorheological Fluids: Modeling and Mathematical Theory. Lecture Notes in Mathematics, vol. 1748. Springer, Berlin (2000) MATHGoogle Scholar
  42. Simon, J.: Sobolev, Besov and Nikolskii fractional spaces: imbedding and comparions for vector valued spaces on an interval. Ann. Mat. Pura Appl. (4) LCVII, 117–148 (1990) View ArticleMATHGoogle Scholar
  43. Stredulinsky, E.W.: Higher integrability from reverse Hölder inequalities. Indiana Univ. Math. J. 29, 407–413 (1980) MathSciNetView ArticleMATHGoogle Scholar
  44. Tan, Z., Zhou, J.: Higher integrability of weak solution of a nonlinear problem arising in the electrorheological fluids. Commun. Pure Appl. Anal. 15(4), 1335–1350 (2016) MathSciNetView ArticleMATHGoogle Scholar
  45. Tan, Z., Zhou, J.: Partial regularity of a certain class of non-Newtonian fluids. J. Math. Anal. Appl. 455(2), 1529–1558 (2017) MathSciNetView ArticleMATHGoogle Scholar
  46. Wolf, J.: Existence of weak solutions to the equations of non-stationary motion of non-Newtonian fluids with shear rate dependent viscosity. J. Math. Fluid Mech. 9(1), 104–138 (2007) MathSciNetView ArticleMATHGoogle Scholar


© The Author(s) 2018