Electronic Journal of Differential Equations, Vol. 2007(2007), No. 177, pp. 1–9. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) EXISTENCE OF POSITIVE SOLUTIONS FOR p(x)-LAPLACIAN PROBLEMS GHASEM A. AFROUZI, HORIEH GHORBANI Abstract. We consider the system of differential equations −∆p(x) u = λ[g(x)a(u) + f (v)] in Ω −∆q(x) v = λ[g(x)b(v) + h(u)] in Ω u=v=0 on ∂Ω where p(x) ∈ C 1 (RN ) is a radial symmetric function such that sup |∇p(x)| < ∞, 1 < inf p(x) ≤ sup p(x) < ∞, and where −∆p(x) u = − div |∇u|p(x)−2 ∇u which is called the p(x)-Laplacian. We discuss the existence of positive solution via sub-super-solutions without assuming sign conditions on f (0), h(0). 1. Introduction The study of differential equations and variational problems with nonstandard p(x)-growth conditions has been a new and interesting topic. Many results have been obtained on this kind of problems; see for example [3, 4, 5, 6, 7, 8, 13]. In [5, 6] Fan and Zhao give the regularity of weak solutions for differential equations with nonstandard p(x)-growth conditions. Zhang [11] investigated the existence of positive solutions of the system −∆p(x) u = f (v) in Ω −∆p(x) v = g(u) in Ω (1.1) u = v = 0 on ∂Ω where p(x) ∈ C 1 (RN ) is a function, Ω ⊂ RN is a bounded domain. The operator −∆p(x) u = − div |∇u|p(x)−2 ∇u) is called p(x)-Laplacian. Especially, if p(x) is a constant p, System (1.1) is the well-known p-Laplacian system. There are many papers on the existence of solutions for p-Laplacian elliptic systems, for example [1, 3, 4, 5, 6, 7, 8, 9]. 2000 Mathematics Subject Classification. 35J60, 35B30, 35B40. Key words and phrases. Positive radial solutions; p(x)-Laplacian problems; boundary value problems. c 2007 Texas State University - San Marcos. Submitted July 18, 2007. Published December 17, 2007. 1 2 G. A. AFROUZI AND H. GHORBANI EJDE-2007/177 In [9] the authors consider the existence of positive weak solutions for the pLaplacian problem −∆p u = f (v) in Ω −∆p v = g(u) in Ω (1.2) u = v = 0 on ∂Ω . There the first eigenfunctions is used for constructing the subsolution of p-Laplacian problems. Under the condition limu→+∞ f (M (g(u))1/(p−1) /up−1 = 0, for all M > 0, the authors show the existence of positive solutions for problem (1.2). In this paper, at first, we consider the existence of positive solutions of the system −∆p(x) u = F (x, u, v) in Ω −∆p(x) v = G(x, u, v) in Ω (1.3) u = v = 0 on ∂Ω 1 N where p(x) ∈ C (R ) is a function, F (x, u, v) = [g(x)a(u) + f (v)], G(x, u, v) = [g(x)b(v) + h(u)], and Ω ⊂ RN is a bounded domain. Then we consider the system −∆p(x) u = λF (x, u, v) in Ω −∆p(x) v = λG(x, u, v) in Ω (1.4) u = v = 0 on ∂Ω where p(x) ∈ C 1 (RN ) is a function, F (x, u, v) = [g(x)a(u) + f (v)], G(x, u, v) = [g(x)b(v) + h(u)], λ is a positive parameter and Ω ⊂ RN is a bounded domain. To study p(x)-Laplacian problems, we need some theory on the spaces Lp(x) (Ω), 1,p(x) W (Ω) and properties of p(x)-Laplacian which we will use later (see [4]). If Ω ⊂ RN is an open domain, write C+ (Ω) = {h : h ∈ C(Ω), h(x) > 1 for x ∈ Ω} h+ = supx∈Ω h(x), h− = inf x∈ΩRh(x), for any h ∈ C(Ω), Lp(x) (Ω) = {u|u is a measurable real-valued function, Ω |u|p(x) dx < ∞}. Throughout the paper, we will assume that p ∈ C+ (Ω) and 1 < inf x∈RN p(x) ≤ supx∈RN p(x) < N . We introduce the norm on Lp(x) (Ω)by Z u(x) p(x) | dx ≤ 1}, |u|p(x) = inf{λ > 0 : | λ Ω and (Lp(x) (Ω), | · |p(x) ) becomes a Banach space, we call it generalized Lebesgue space. The space (Lp(x) (Ω), | · |p(x) ) is a separable, reflexive and uniform convex Banach space (see [4, Theorem 1.10, 1.14]). The space W 1,p(x) (Ω) is defined by W 1,p(x) (Ω) = {u ∈ Lp(x) (Ω) : |∇u| ∈ p(x) L (Ω)}, and it is equipped with the norm kuk = |u|p(x) + |∇u|p(x) , 1,p(x) ∀u ∈ W 1,p(x) (Ω). We denote by W0 (Ω) the closure of C0∞ (Ω) in W 1,p(x) (Ω). W 1,p(x) (Ω) and 1,p(x) (Ω) are separable, reflexive and uniform convex Banach space (see [4, TheW0 orem 2.1]). We define Z (L(u), v) = |∇u|p(x)−2 ∇u∇vdx, ∀u, v ∈ W 1,p(x) (Ω), RN EJDE-2007/177 EXISTENCE OF POSITIVE SOLUTIONS 3 then L : W 1,p(x) (Ω) → (W 1,p(x) (Ω))∗ is a continuous, bounded and is a strictly monotone operator, and it is a homeomorphism [7, Theorem 3.11]. 1,p(x) Functions u, v in W0 (Ω), is called a weak solution of (1.4); it satisfies Z Z 1,p(x) p(x)−2 |∇u| ∇u∇ξdx = λF (x, u, v)ξdx, ∀ξ ∈ W0 (Ω), ZΩ ZΩ 1,p(x) |∇v|q(x)−2 ∇v∇ξdx = λG(x, u, v)ξdx, ∀ξ ∈ W0 (Ω). Ω Ω We make the following assumptions (H1) p(x) ∈ C 1 (RN ) is a radial symmetric and sup |∇p(x)| < ∞ (H2) Ω = B(0, R) = {x||x| < R} is a ball, where R > 0 is a sufficiently large constant. (H3) a, b ∈ C 1 ([0, ∞)) are nonnegative, nondecreasing functions such that lim u→+∞ a(u) = 0, uP − −1 lim u→+∞ b(u) = 0. uP − −1 (H4) f, h ∈ C 1 ([0, ∞)) are nondecreasing functions, limu→+∞ f (u) = +∞, limu→+∞ h(u) = +∞, and 1 f (M (h(u)) p− −1 ) lim = 0, u→+∞ up− −1 ∀M > 0 . (H5) g : [0, +∞) → (0, ∞) is a continuous function such that L1 = minx∈Ω̄ g(x), and L2 = maxx∈Ω̄ g(x). We shall establish the following result. Theorem 1.1. If (H1)–(H5) hold, then (1.3) has a positive solution. Proof. We establish this theorem by constructing a positive subsolution (φ1 , φ2 ) and supersolution (z1 , z2 ) of (1.3), such that φ1 ≤ z1 and φ2 ≤ z2 . That is (φ1 , φ2 ) and (z1 , z2 ) satisfy Z Z Z |∇φ1 |p(x)−2 ∇φ1 · ∇ξdx ≤ g(x)a(φ1 )ξdx + f (φ2 )ξdx, ZΩ ZΩ ZΩ |∇φ2 |p(x)−2 ∇φ1 · ∇ξdx ≤ g(x)b(φ2 )ξdx + h(φ1 )ξdx, Ω Z ZΩ ZΩ |∇z1 |p(x)−2 ∇z1 · ∇ξdx ≥ g(x)a(z1 )ξdx + f (z2 )ξdx, Ω Z ZΩ ZΩ |∇z2 |p(x)−2 ∇z2 · ∇ξdx ≥ g(x)b(z2 )ξdx + h(z1 )ξdx, Ω 1,p(x) for all ξ ∈ W0 Ω Ω (Ω) with ξ ≥ 0. Then (1.3) has a positive solution. Step 1. We construct a subsolution of (1.3). Denote inf p(x) − 1 R−α , R0 = , 4(sup |∇p(x)| + 1) 2 b = min{a(0)L1 + f (0), b(0)L1 + h(0), −1}, α= 4 G. A. AFROUZI AND H. GHORBANI EJDE-2007/177 and let e−k(r−R) − 1, 2R0 < r ≤ R, p(2R0 )−1 R 2R 0 (keαk ) p(r)−1 eαk − 1 + (2R )N −1 r 1 π π 0 φ(r) = ×[ rN −1 sin(ε(r − 2R0 ) + 2 )(L1 + 1)] p(r)−1 dr, 2R0 − 2ε < r ≤ 2R0 , p(2R0 )−1 R eαk − 1 + 2R0 π (keαk ) p(r)−1 2R − 0 2ε 1 (2R0 )N −1 π ×[ rN −1 sin(ε0 (r − 2R0 ) + π2 )(L1 + 1)] p(r)−1 dr, r ≤ 2R0 − 2ε , where R0 is sufficiently large, ε is a small positive constant which satisfies R0 ≤ π 2R0 − 2ε , In the following, we will prove that (φ, φ) is a subsolution of (1.3). Since e−k(r−R) − 1, 2R0 < r ≤ R, p(2R0 )−1 αk p(r)−1 −(ke ) φ0 (r) = N −1 1 π 0) sin(ε(r − 2R0 ) + π2 )(L1 + 1)] p(r)−1 dr, 2R0 − 2ε ×[ (2R < r ≤ 2R0 , r N −1 π 0, 0 ≤ r ≤ 2R0 − 2ε , it is easy to see that φ ≥ 0 is decreasing and φ ∈ C 1 ([0, R]), φ(x) = φ(|x|) ∈ C 1 (Ω̄). Let r = |x|. By computation, −∆p(x) φ = − div |∇φ(x)|p(x)−2 ∇φ(x)) = −(rN −1 |φ0 (r)|p(r)−2 φ0 (r))0 /rN −1 . Then −k(r−R) p(r)−1 (ke ) − k(p(r) − 1) + p0 (r) ln k N −1 0 −kp (r)(r − R) + r , −∆p(x) φ = ε( 2R0 )N −1 (keαk )( p(2R0 ) − 1) r × cos(ε(r − 2R0 ) + π2 )(L1 + 1), 0, 2R0 < r ≤ R, π 2R0 − 2ε < r ≤ 2R0 , π 0 ≤ r ≤ 2R0 − 2ε , If k is sufficiently large, when 2R0 < r ≤ R, then ln k N −1 + R − r) + ] ≤ −kα. k kr Since α is a constant dependent only on p(x), if k is a big enough, such that −ka < b, and since φ(x) ≥ 0 and a, f are monotone, this implies −∆p(x) φ ≤ −k[inf p(x) − 1 − sup |∇p(x)|( −∆p(x) φ ≤ a(0)L1 + f (0) ≤ g(x)a(φ) + f (φ), 2R0 < |x| ≤ R . (1.5) If k is sufficiently large, then a(eαk − 1) ≥ 1, f (eαk − 1) ≥ 1, b(eαk − 1) ≥ 1, h(eαk − 1) ≥ 1 where k is dependent on a, f, b, h, p, and independent on R. Since 2R0 N −1 αk ( π ) (ke ) p(2R0 ) − 1) cos(ε(r − 2R0 ) + )(L1 + 1) r 2 π N p+ αkp+ ≤ ε(L1 + 1)2 k e , 2R0 − < |x| < 2R0 . 2ε −∆p(x) φ = ε( + + Let ε = 2−N k −p e−αkp . Then −∆p(x) φ ≤ L1 + 1 ≤ g(x)a(φ) + f (φ), 2R0 − π < |x| < 2R0 . 2ε (1.6) EJDE-2007/177 EXISTENCE OF POSITIVE SOLUTIONS 5 Obviously, −∆p(x) φ = 0 ≤ L1 + 1 ≤ g(x)a(φ) + f (φ), |x| < 2R0 − π . 2ε (1.7) Since φ(x) ∈ C 1 (Ω), combining (1.5), (1.6), (1.7), we have −∆p(x) φ ≤ g(x)a(φ) + f (φ) for a.e. x ∈ Ω. Similarly we have −∆p(x) φ ≤ g(x)b(φ) + h(φ), for a.e. x ∈ Ω. Let (φ1 , φ2 ) = (φ, φ), since φ(x) ∈ C 1 (Ω̄), it is easy to see that (φ1 , φ2 ) is a subsolution of (1.3). Step 2. We construct a supersolution of (1.3) Let z1 be a radial solution of −∆p(x) z1 (x) = (L2 + 1)µ, z1 = 0 in Ω, on ∂Ω . We denote z1 = z1 (r) = z1 (|x|), then z1 satisfies −(rN −1 |z10 |p(r)−2 z10 )0 = rN −1 (L2 + 1)µ, z1 (R) = 0, z10 (0) = 0 . Then z10 = −| and Z 1 r(L2 + 1)µ p(r)−1 | , N (1.8) R 1 r(L2 + 1)µ p(r)−1 dr. | N r We denote β = β((L2 + 1)µ) = max0≤r≤R z1 (r), then Z R Z R 1 1 1 r(L2 + 1)µ p(r)−1 r p(q)−1 β((L2 + 1)µ) = | | dr = ((L2 + 1)µ) | | p(r)−1 dr, N N 0 0 RR r 1 where q ∈ [0, 1]. Since 0 | N | p(r)−1 dr is a constant, then there exists a positive constant C ≥ 1 such that 1 1 1 ((L2 + 1)µ) p+ −1 ≤ β((L2 + 1)µ) = max z1 (r) ≤ C((L2 + 1)µ) p− −1 . (1.9) 0≤r≤R C We consider z1 = | −∆p(x) z1 = (L2 + 1)µ in Ω −∆p(x) z2 = (L2 + 1)h(β((L2 + 1)µ)) z1 = z2 = 0 in Ω on ∂Ω . Then we shall prove that (z1 , z2 ) is a supersolution for (1.3). For ξ ∈ W 1,p(x) (Ω) with ξ ≥ 0, it is easy to see that Z Z |∇z2 |p(x)−2 ∇z2 · ∇ξdx = (L2 + 1)h(β((L2 + 1)µ))ξdx Ω ZΩ Z ≥ L2 h(β((L2 + 1)µ))ξdx + h(z1 )ξdx. Ω Ω Similar to (1.9), we have 1 max z2 (r) ≤ C[(L2 + 1)h(β((L2 + 1)µ))] (p− −1) . 0≤r≤R 6 G. A. AFROUZI AND H. GHORBANI EJDE-2007/177 By (H3), for µ large enough we have 1 h(β((L2 + 1)µ)) ≥ b(C[(L2 + 1)h(β((L2 + 1)µ))] p− −1 ) ≥ b(z2 ). Hence Z p(x)−2 |∇z2 | Z ∇z2 · ∇ξdx ≥ Z g(x)b(z2 )ξdx + Ω h(z1 )ξdx, Ω (1.10) Ω Also Z |∇z1 |p(x)−2 ∇z1 · ∇ξdx = Ω Z (L2 + 1)µξdx. Ω By (H3), (H4), when µ is sufficiently large, according to (1.9), we have (L2 + 1)µ ≥ [ − 1 β((L2 + 1)µ)]p −1 C 1 1 ≥ L2 a(β((L2 + 1)µ)) + f [C[(L2 + 1) (p− −1) (h(β((L2 + 1)µ))) (p− −1) ] ≥ g(x)a(z1 ) + f (z2 ), then Z |∇z1 |p(x)−2 ∇z1 · ∇ξdx ≥ Z Ω Z g(x)a(z1 )ξdx + f (z2 )ξdx. Ω (1.11) Ω According to (1.10) and (1.11), we can conclude that (z1 , z2 ) is a supersolution of (1.3). Let µ be sufficiently large, then from (1.8) and the definition of (φ1 , φ2 ), it is easy to see that φ1 ≤ z1 and φ2 ≤ z2 . This completes the proof. Now we consider the problem −∆p(x) u = λF (x, u, v) in Ω −∆p(x) v = λG(x, u, v) in Ω (1.12) u = v = 0 on ∂Ω. If p(x) ≡ p (a constant), because of the homogenity of p-Laplacian, (1.3) and (1.4) can be transformed into each other; but, if p(x) is a general function, since p(x)-Laplacian is nonhomogeneous, they cannot be transformed into each other. So we can see that p(x)-Laplacian problem is more complicated than than that of p-Laplacian, and it is necessary to discuss the problem (1.4) separately. Theorem 1.2. If p(x) ∈ C 1 (Ω̄), Ω = B(0, R), and (H3)–(H5) hold, then there exists a λ∗ which is sufficiently large, such that (1.4) possesses a positive solution for any λ ≥ λ∗ . Proof. We construct a subsolution of (1.4). Let β ≤ |p(r1 ) − p(r2 )| ≤ R 4 satisfy 1 , ∀r1 , r2 ∈ [R − 2β, R]. 2 (1.13) In the following we denote δ = min{ inf p(x) − 1 }, 4(sup |∇p(x)| + 1) p+ ∗ = sup p(x), p− ∗ = R−2β≤|x|≤R inf p(x), R−2β≤|x|≤R b = min{a(0)L1 + f (0), b(0)L1 + h(0), −1}. (1.14) EJDE-2007/177 EXISTENCE OF POSITIVE SOLUTIONS Let α ∈ (0, β], and set −k(r−R) e − 1, R R−α αk p(R−α)−1 (R−α)N −1 αk e −1+ r (ke ) p(r)−1 [ rN −1 1 π φ(r) = × sin(ε(r − (R − α)) + 2 )(L1 + 1)] p(r)−1 dr, p(R−α)−1 R R−α N −1 eαk − 1 + R−α− π (keαk ) p(r)−1 [ (R−α) N −1 r 2ε 1 × sin(ε(r − (R − α)) + π2 )(L1 + 1)] p(r)−1 dr, 7 R − α < r ≤ R, R − 2β < r ≤ R − α, r ≤ R − 2β, π where ε = 2(2β−α) which satisfies ε(R − 2β − (R − α)) + π2 = 0. In the following, we will prove that (φ, φ) is a subsolution of (1.4). Since −k(r−R) e − 1, R − α < r ≤ R, p(R−α)−1 αk p(r)−1 −(ke ) N −1 φ0 (r) = [ (R−α) r N −1 1 × sin(ε(r − (R − α)) + π2 )(L1 + 1)] p(r)−1 dr, R − 2β < r ≤ R − α, 0, r ≤ R − 2β. It is easy to see that φ ≥ 0 is decreasing and φ ∈ C 1 ([0, R]), φ(x) = φ(|x|) ∈ C 1 (Ω). Let r = |x|. By computation, −k(r−R) p(r)−1 (ke ) [−k(p(r) − 1) +p0 (r) ln k − kp0 (r)(r − R) + N −1 ], R − α < r ≤ R, r −∆p(x) φ(x) = ε( R−α )N −1 (keαk )(p(R−α)−1) r × cos(ε(r − (R − α)) + π2 )(L1 + 1), R − 2β < r ≤ R − α, 0, r ≤ R − 2β. If k is sufficiently large, when R − α < r ≤ R, then we have ln k N −1 −∆p(x) φ ≤ −k p(r) [inf p(x) − 1 − sup |∇p(x)|( + R − r) + ] ≤ −k p(r) δ. k kr If k satisfies − k p∗ δ = −λb, (1.15) and since φ(x) ≥ 0 and a, f is monotone, it means that −∆p(x) φ ≤ λ(a(0)L1 + f (0)) ≤ λ(g(x)a(φ) + f (φ)), R − α < |x| ≤ R. (1.16) From (H3), (H4) there exists a positive constant M such that a(M − 1) ≥ 1, f (M − 1) ≥ 1, b(M − 1) ≥ 1, h(M − 1) ≥ 1. Let αk = ln M. (1.17) Since R − α N −1 αk ( π ) (ke ) p(R − α) − 1) cos(ε(r − (R − α)) + )(L1 + 1) r 2 N αk p+ −1 ∗ ≤ ε(L1 + 1)2 (ke ) , R − 2β < |x| < R − α, −∆p(x) φ(x) = ε( if + ε2N (keαk )p∗ −1 ≤ λ, (1.18) then −∆p(x) φ(x) ≤ λ(L1 + 1) ≤ λ(g(x)a(φ) + f (φ)), R − 2β < |x| < R − α. (1.19) 8 G. A. AFROUZI AND H. GHORBANI EJDE-2007/177 Obviously −∆p(x) φ(x) = 0 ≤ λL1 + 1 ≤ λ(g(x)a(φ) + f (φ)), |x| < R − 2β . (1.20) Combining (1.15), (1.17) and (1.18), we only need + −b p∗p−−1 p+ λ| ∗ M ∗ −1 ≤ λ, δ and according to (1.13), (1.14), we only need ε2N | + + π −b p∗ −−1 ( 2N M p∗ −1 | | p∗ )2p− ∗ ≤ λ. β δ Let + + −b p∗ −−1 − π λ∗ = ( 2N M p∗ −1 | | p∗ )2p∗ . β δ If λ ≥ λ∗ is sufficiently large, then (1.18) is satisfied. Since φ(x) = φ(|x|) ∈ C 1 (Ω), according to (1.16), (1.19) and (1.20), it is easy to see that if λ is sufficiently large, then (φ1 , φ2 ) is a subsolution of (1.4). Step 2. We construct a supersolution of (1.4). Similar to the proof of Theorem 1.1, we consider −∆p(x) z1 = λ(L2 + 1)µ in Ω −∆p(x) z2 = λ(L2 + 1)h(β(λ(L2 + 1)µ)) z1 = z2 = 0 in Ω on ∂Ω , where β = β(λ(L2 + 1)µ) = max0≤r≤R z1 (r). It is easy to see that Z Z |∇z2 |p(x)−2 ∇z2 · ∇ξdx = λ(L2 + 1)h(β(λ(L2 + 1)µ))ξdx Ω Ω Z Z ≥ λL2 h(β(λ(L2 + 1)µ))ξdx + λh(z1 )ξdx. Ω Ω Similar to (1.9), we have 1 max z2 (r) ≤ C[λ(L2 + 1)h(β(λ(L2 + 1)µ))] (p− −1) . 0≤r≤R By (H3) for µ large enough we have 1 h(β(λ(L2 + 1)µ)) ≥ b(C[λ(L2 + 1)h(β(λ(L2 + 1)µ))] p− −1 ) ≥ b(z2 ). Hence Z |∇z2 |p(x)−2 ∇z2 · ∇ξdx ≥ Ω Z Z λg(x)b(z2 )ξdx + Ω Also Z p(x)−2 |∇z1 | λh(z1 )ξdx. (1.21) Ω Z ∇z1 · ∇ξdx = Ω λ(L2 + 1)µξdx. Ω By (H3), (H4), when µ is sufficiently large, according to (1.9), we have (L2 + 1)µ ≥ − 1 1 [ β(λ(L2 + 1)µ)]p −1 λ C 1 ≥ L2 a(β(λ(L2 + 1)µ)) + f (C[λ(L2 + 1)h(β(λ(L2 + 1)µ))] (p− −1) ) . EJDE-2007/177 EXISTENCE OF POSITIVE SOLUTIONS 9 Then Z p(x)−2 |∇z1 | Ω Z ∇z1 · ∇ξdx ≥ Z λg(x)a(z1 )ξdx + Ω λf (z2 )ξdx. (1.22) Ω According to (1.21) and (1.22), we can conclude that (z1 , z2 ) is a supersolution of (1.4). Similar to the proof of Theorem 1.1, if µ is sufficiently large, we have φ1 ≤ z1 and φ2 ≤ z2 . This completes the proof. References [1] J. Ali, R. Shivaji, Positive solutions for a class of p-Laplacian systems with multiple parametes, J. Math. Anal. Appl. 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Shivaji, An existence result on positive solutions for a class of p-Laplacian systems, Nonlinear Anal. 56 (2024) 1007-1010. [10] M. Rûzicka, Electrorheological Fluids: Modeling and Mathematical Theory, Lecture Notes in Math, vol. 1784, Springer-Verlag, Berlin, 2000. [11] Q. H. Zhang, Existence of positive solutions for elliptic systems with nonstandard p(x)-growth conditions via sub-supersolution method, Nonlinear Anal. 67 (2007) 1055-1067. [12] Q. H. Zhang, Existence of positive solutions for a class of p(x)-Laplacian systems, J. Math. Anal. Appl. 302 (2005) 306-317. [13] V. V. Zhikov, Averaging of functionals of the calculus of variations and elasticity theory, Math. USSR Izv. 29 (1987) 33-36. Ghasem A. Afrouzi Department of Mathematics, Faculty of Basic Sciences, Mazandaran University, Babolsar, Iran E-mail address: afrouzi@umz.ac.ir Horieh Ghorbani Department of Mathematics, Faculty of Basic Sciences, Mazandaran University, Babolsar, Iran E-mail address: seyed86@yahoo.com