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Periodic solutions for a differential inclusion problem involving the p(t)-Laplacian

  • Peng Chen EMAIL logo and Xianhua Tang
Published/Copyright: December 19, 2020

Abstract

In the present paper, we consider the nonlinear periodic systems involving variable exponent driven by p(t)-Laplacian with a locally Lipschitz nonlinearity. Our arguments combine the variational principle for locally Lipschitz functions with the properties of the generalized Lebesgue-Sobolev space. Applying the non-smooth critical point theory, we establish some new existence results.

MSC 2010: 34C25; 58E30; 47H04

1 Introduction

In recent years, the study on p(t)-Laplacian problems has attracted more and more attention. The p(t)-Laplacian possesses more complicated nonlinearities than the p-Laplacian. For example, it is inhomogeneous, this causes many troubles, and some classical theories and methods, such as the theory of Sobolev spaces, are not applicable. The study of various mathematical problems with variable exponent growth condition has been received considerable attention in recent years. These problems are interesting in applications and raise many difficult mathematical problems. One of the most studied models leading to problems of this type is the model of motion of electro-rheological fluids, which are characterized by their ability to drastically change the mechanical properties under the influence of an exterior electromagnetic field [44]. Problems with variable exponent growth conditions also appear in the mathematical modeling of stationary thermo-rheological viscous flows of non-Newtonian fluids and in the mathematical description of the filtration processes of an ideal barotropic gas through a porous medium [1,2]. Another field of application of equations with variable exponent growth conditions is image processing [4]. We refer the reader to [35, 40, 41, 42, 43, 44] for an overview of and references on this subject, and to [6,7,8,9,13,14,20,21,33,34, 37,39, 40, 41, 42] for the study of the p(t)-Laplacian equations and the corresponding variational problems.

Recently, Wang and Yuan [37] obtained the existence of periodic solutionsfor p(t)-Laplacian system:

(1.1) u ( t ) p ( t ) 2 u ( t ) = j ( t , u ( t ) ) ,  a.e.t [ 0 , T ] , u ( 0 ) u ( T ) , u ( 0 ) = u ( T ) ,

where j(t, u) is measurable in t ∈ [0, T], continuously diferentiable in u ∈ ℝN. More precisely, they were able to prove that, under suitable conditions, the system might have at least one solution, or have infinite number of solutions. Since many free boundary problems and obstacle problems may be reduced to partial differentia1 equations with discontinuous nonlinearities, now a question arises: whether there exist solutions for system (1.1) in the case where the potential function j(t, x) is nonsmooth in x ∈ ℝN. We require that j(t, ·) is only locally Lipschitz. That is the main problem which we want to solve in the present paper.

The operator (|u'(t)|p(t)−2u'(t))' is said to be p(t)-Laplacian, which becomes p-Laplacian when p(t) ≡ p (a constant) and the problem (1.1) reduces to the following

(1.2) u ( t ) p 2 u ( t ) j ( t , u ) ,  a.e.t [ 0 , T ] , u ( 0 ) = u ( T ) , u ( 0 ) = u ( T ) ,

where j(t, u) is locally Lipschitz in u ∈ ℝN.

Periodic problems involving the scalar p-Laplacian were studied by many authors. We mention the works by Dang and Oppenheimer [10], Del Pino, Manasevich and Murua [11], Gasinski and Papageorgiou [16, 17, 18], Papageorgiou and Rǎdulescu [30], Yang [38] and the references [15,22,28,30, 31, 32,38].

The goal of this paper is to discuss the existence of solutions of the following differential equation with p(t)-Laplacian and a nonsmooth potential

(1.3) u ( t ) p ( t ) 2 u ( t ) j ( t , u ( t ) ) ,  a.e.t [ 0 , T ] , u ( 0 ) = u ( T ) , u ( 0 ) = u ( T ) ,

where p(t) > 1, u ∈ ℝN, j(t, s) is locally Lipschitz function in the s-variable integrand (in general it can be nonsmooth), and ∂j(t, s) is the subdifferential with respect to the s-variable in the sense of Clarke [3,5].

This paper is organized as follows. In Section 2, we present some necessary preliminary knowledge on generalized gradient of the locally Lipschitz function and variable exponent Sobolev spaces. In Section 3, we give the main results and their proofs.

2 Preliminaries

The nonsmooth critical point theory for locally Lipschitz functionals is based on the subdifferential theory of Clarke [5].

Let X be a Banach space and let X* be its topological dual. By <· > we denote the duality brackets for the pair (X, X*). A function ϕ : X → ℝ is said to be locally Lipschitz, if for every xX, we can find a neighbourhood U of x and a constant k > 0 (depending on U), such that |ϕ(y) − ϕ(z)| ≤ kyz║, ∀ y, zU.

For a locally Lipschitz function ϕ : X → ℝ we define

ϕ 0 ( x ; h ) = lim x x ; λ 0 sup ϕ x + λ h ϕ x λ .

It is obvious that the function hϕ0(x; h) is sublinear, continuous and so is the support function of a nonempty, convex and w*-compact set ∂ϕ(x) ⊆ X*, defined by

ϕ ( x ) = x X ; < x , h >≤ ϕ 0 ( x ; h ) , h X .

The multifunction x∂ϕ(x) is known as the generalized (or Clarke) subdifferential of ϕ. If ϕ, ψ : X → ℝ are locally Lipschitz functions, then (ϕ + ψ)(x) ⊆ ∂ϕ(x) + ∂ψ(x) and for every λ ∈ ℝ, (λϕ)(x) = λ∂ϕ(x).

Let ϕ : X → ℝ be a locally Lipschitz function. A point xX is said to be a critical point of ϕ if 0 ∈ ∂ϕ(x). If xX is a critical point of ϕ, then c = ϕ(x) is a critical value of ϕ. It is easy to see that, if xX is a local extremum of ϕ, then 0 ∈ ∂ϕ(x). Moreover, the multifunction x∂ϕ(x) is upper semicontinuous from X into X* equipped with the w* topology, i.e., for any UX* w*-open, the set {xX : ∂ϕ(x) ⊆ U} is open in X. For more details we refer to Clarke [5]. The critical point theory for smooth functions uses a compactness condition known as the Palais-Smale condition (PS). In the present nonsmooth setting this condition takes the following form:

The locally Lipschitz function ϕ : X → ℝ satisfies the nonsmooth PS condition if any sequence {xn}n≥1X such that {ϕ(xn)}n≥1 is bounded and m(xn) = min[║x*║ : x*∂ϕ(xn)] → 0 as n → ∞, has a strongly convergent subsequence.

If ϕC1(X, ℝ), then as we already mentioned ∂ϕ(x) = {ϕ'(x)} and so the above definition of the P.S. condition coincides with the classical (smooth) one. In the context of the smooth theory, Cerami introduced a weaker compactness condition which in our nonsmooth setting has the following form:

The locally Lipschitz function ϕ : X → ℝ satisfies the nonsmooth Cerami condition (nonsmooth C-condition for short), if any sequence {xn}n≥1X such that {ϕ(xn)}n≥1 is bounded and (1 + ║xn║)m(xn) → 0 as n → ∞, has a strongly convergent subsequence.

Lemma 2.1

[27] Assume that φ is a locally Lipschitz functional on a Banach space X and φ : X → ℝ satisfies:

  1. φ is weakly lower semicontinuous;

  2. φ is coercive.

Then there exists x*X such that φ(x*) = minx∈X φ(x).

Lemma 2.2

[22] Let X be a Banach space and φ : X → ℝ a locally Lipschitz functional satisfying the (C) condition. If X = YV with Y a finite-dimensional subspace of X. φ satisfies the nonsmooth C-condition,

c = inf y Γ max x E φ ( y ( x ) )

and there exists an r > 0 such that

max [ φ ( x ) : x Y , x = r ] inf [ φ ( x ) : x V ] ,

where Γ = {γC(E, X) : γ|∂E = id}, E = {xY : ║x║ ≤ r} and ∂E = {xY : ║x║ = r}, then

c inf V φ

and c is a critical value of φ. Moreover, if c = infV φ, then V ՈKc ≠ ∅, where Kc = {xX : φ(x) = c, λ(x) = 0}.

Lemma 2.3

[22] Let X be a reflexive Banach space, ϕ : X → ℝ a locally Lipschitz functional satisfying the PS-condition. Assume that there exist x0, x1X, c0 ∈ ℝ and ϱ > 0 such thatx1x0║ > ϱ and

max ϕ x 0 , ϕ x 1 < c 0 = inf ϕ ( y ) : y x 0 = ϱ .

Then, ϕ has a critical point xX with c = ϕ(x) ≥ c0 given by

c = inf y Γ 1 max t T ϕ ( y ( t ) ) ,

where Γ1 = {γC([0, 1], x) : γ(0) = x0, γ(1) = x1}.

In order to discuss (1.3), we recall some known results from critical point theory and the properties of space W1,p(t) for the convenience of the readers.

Let p(t) ∈ C(0, T;ℝ) and 1 < p := inft∈[0,T]p(t) ≤ supt∈[0,T]p(t) := p+ < ∞. Define

L p ( t ) 0 , T ; R N = u L 1 0 , T ; R N 0 T u ( t ) p ( t ) d t <

with the norm

| u | p ( t ) = inf λ > 0 0 T u λ p ( t ) d t 1 .

For u L l o c 1 0 , T ; R N , let u' denote the weak derivative of u, i.e., u L l o c 1 0 , T ; R N and satisfy

0 T u φ d t = 0 T u φ d t , φ C 0 0 , T ; R N .

Define

W 1 , p ( t ) 0 , T ; R N = u L p ( t ) 0 , T ; R N u L p ( t ) 0 , T ; R N

with the norm

u = inf λ > 0 0 T u λ p ( t ) + u λ p ( t ) d t 1 .

We call the space Lp(t) a generalized Lebesgue space, it is a special kind of generalized Orlicz spaces. The space W1,p(t) is called a generalized Sobolev space, it is a special kind of generalized Orlicz-Sobolev spaces. For the general theory of generalized Orlicz spaces and generalized Orlicz-Sobolev spaces, see [13,14].

Proposition 2.4

[14] Let

ρ ( u ) = 0 T u p ( t ) d t , u L p ( t ) ,

then

  1. | u | p ( t ) < 1 ( = 1 ; > 1 ) ρ ( u ) < 1 ( = 1 ; > 1 ) ;

  2. |u|p(t)>1|u|p(t)pρ(u)|u|p(t)p+,|u|p(t)<1|u|p(t)p+ρ(u)|u|p(t)p;

  3. | u | p ( t ) 0 ρ ( u ) 0 ; | u | p ( t ) ρ ( u ) .

  4. Let uLp(t) \ {0}, thenup(t) = λ if and only if ρ u λ = 1.

Proposition 2.5

[13] Lp(t) and W1,p(t) are Banach spaces with the norms defined above. When p > 1, they are reflexive.

Let C T = C T R , R N = u C R , R N : u is T-periodic}.

Definition 2.6

[13] Let u, vL1(0, T;ℝN). If

0 T v φ d t = 0 T u φ ˙ d t , φ C T R , R N ,

then v is called a T-weak derivative of u and is denoted by u ˙ .

Definition 2.7

[24] Define

W T 1 , p 0 , T ; R N = u L p 0 , T ; R N : u ˙ L p 0 , T ; R N

with the norm u W T 1 , p = | u | p p + | u ˙ | p p 1 / p .

Definition 2.8

[13, 14] Define

W T 1 , p ( t ) 0 , T ; R N = u L p ( t ) 0 , T ; R N : u ˙ L p ( t ) 0 , T ; R N

and H T 1 , p ( t ) 0 , T ; R N to be the closure of W T 1 , p ( t ) 0 , T ; R N .

From Definition 2.7 and 2.8 we see that, for uL1(0, T;ℝN), the weak derivative u' and the T-weak derivative are two different conceptions (see [13] for details). Although the two derivatives are distinct, we have

Proposition 2.9

[13, 14]

  1. C T 0 , T ; R N is dense in W T 1 , p ( t ) 0 , T ; R N ;

  2. W T 1 , p ( t ) 0 , T ; R N = H T 1 , p ( t ) 0 , T ; R N = u W T 1 , p ( t ) 0 , T ; R N : u ( 0 ) = u ( T ) ;

  3. If u H T 1 , 1 , the weak derivative is also the T-weak derivative u ˙ , i . e . , u = u ˙ .

Proposition 2.10

[13] Let u W T 1 , 1 , then

  1. 0 T u ˙ d t = 0 ;

  2. u has its continuous representation, which is still denoted by u,

    u ( t ) = 0 t u ˙ ( s ) d s + u ( 0 ) , u ( 0 ) = u ( T ) .
  3. u ˙ is the classical derivative of u if u ˙ C 0 , T ; R N .

Proposition 2.11

[13]

  1. H T 1 0 , T ; R N is a reflexive Banach space if p > 1;

  2. There is a continuous embedding W T 1 , p ( t ) H T 1 , p ( t ) C 0 , T ; R N . When p > 1, the embedding is compact.

Proposition 2.12

[14] If

1 p ( t ) + 1 q ( t ) = 1 ,

then

  1. (Lp(t))* = Lq(t), where (Lp(t))* is the dual space of Lp(t);

  2. uLp(t), vLq(t), we have

Ω u ( t ) v ( t ) d t 2 | u | p ( t ) | v | q ( t ) .

Let

W p e r 1 , p ( t ) 0 , T ; R N = u L p ( t ) 0 , T ; R N : u ( 0 ) = u ( T ) , u L p ( t ) 0 , T ; R N .

Obviously, W p e r 1 , p ( t ) 0 , T ; R N is a reflexive Banach space with the norm

u = inf λ > 0 0 T u λ p ( t ) + u λ p ( t ) d t 1 .

Consider the following functional:

J ( u ) = 0 T 1 p ( t ) u p ( t ) d t , u W p e r 1 , p ( t ) 0 , T ; R N .

We know that (see [2]) J C 1 W p e r 1 , p ( t ) , R and p(t)-Laplacian operator (|u'|p(t)−2u')' is the derivative operator of J in the weak sense. Denote A = J : W p e r 1 , p ( t ) 0 , T ; R N W p e r 1 , p ( t ) 0 , T ; R N , then

< A ( u ) , v >= 0 T u ( t ) p ( t ) 2 u ( t ) , v ( t ) R N d t , u , v W p e r 1 , p ( t ) 0 , T ; R N .

Proposition 2.13

[14] J' is a mapping of (S)+, i.e., if

u n u  and  lim n J u n J ( u ) , u n u 0 ,

then un has a convergent subsequence in W p e r 1 , p ( t ) 0 , T ; R N .

For every u W p e r 1 , p ( t ) 0 , T ; R N , set

u ¯ = 1 T 0 T u ( t ) d t , u ~ ( t ) = u ( t ) u ¯ .

By virtue of [35], there exists a > 0 such that

(2.1) u ~ a u p ( t ) , u W p e r 1 , p ( t ) 0 , T ; R N .

The corresponding functional φ : W p e r 1 , p ( t ) 0 , T ; R N R for (1.3) is defined by:

(2.2) φ ( u ) = 0 T 1 p ( t ) u p ( t ) d t 0 T j ( t , u ) d t , u W p e r 1 , p ( t ) 0 , T ; R N .

3 Main results and their Proofs

Our hypotheses on the function p(t) and j(t, u) are the following:

(P) p(t) ∈ C(0, T;ℝ), p(t + T) = p(t) and 1 < p := inft∈[0,T] p(t) ≤ supt∈[0,T] p(t) := p+ < ∞, ∀ t ∈ ℝ;

H(j)1 j : [0, T] × ℝN is a function such that:

  1. for all u ∈ ℝN , tj(t, u) is measurable;

  2. for almost all t ∈ [0, T], uj(t, u) is locally Lipschitz;

  3. for every w∂j(t, u), there exists αL1[0, T] such that for almost all t ∈ [0, T], we have |w| ≤ α(t);

  4. j(t, u) → −∞ as |u| → ∞uniformly for almost all t ∈ [0, T];

  5. there exists u0 ∈ ℝN \ {0} such that 0 T j t , u 0 d t > 0  and  0 T j ( t , 0 ) d t 0.

Theorem 3.1

If hypotheses (P), H(j)1 hold, then problem (1.3) has at least one nontrivial periodic solution.

We can weaken hypothesis H(j)1 (iv) at the expense of introducing an extra unilateral growth condition.

More precisely, the new hypotheses on j(t, u) are the following:

H(j)2 j : [0, T] × ℝN is a function such that:

  1. for all u ∈ ℝN , tj(t, u) is measurable;

  2. for almost all t ∈ [0, T], uj(t, u) is locally Lipschitz;

  3. for every w∂j(t, u), there exists αL1[0, T] such that for almost all t ∈ [0, T], we have |w| ≤ α(t);

  4. j(t, u) → −∞ as |u| → ∞for almost all tE ⊂ [0, T] with measE > 0;

  5. there exists βL1[0, T] such that for almost all t ∈ [0, T], u ∈ ℝN, we have

    j ( t , u ) β ( t ) ;
  6. there exists u0 ∈ ℝN \ {0} such that 0 T j t , u 0 d t > 0 a n d 0 T j ( t , 0 ) d t 0.

Theorem 3.2

If hypotheses (P), H(j)2 hold, then problem (1.3) has at least one nontrivial periodic solution.

In the previous existence theorems the energy functional φ defined in (2.2) was coercive and so the solution was obtained by an application of the least action principle. In the next existence theorem the energy functional φ is bounded below but not necessarily coercive. In this case the hypotheses on the nonsmooth potential j(t, u) are the following:

H(j)3 j : [0, T] × ℝN is a function such that j(·, 0) ∈ L1[0, T] and:

  1. for all u R N , t j ( t , u ) is measurable;

  2. for almost all t ∈ [0, T], uj(t, u) is locally Lipschitz;

  3. for every r > 0, there exists αrL1[0, T] such that for almost all t ∈ [0, T], |u| ≤ r and all w∂j(t, u), we have |w| ≤ αr(t);

  4. there exist 0 < μ < p and M > 0 such that for almost all t ∈ [0, T] and all |u| ≥ M, we have

    j 0 ( t , u ; u ) < μ j ( t , u ) ;
  5. j(t, u) → +∞ uniformly for almost all t ∈ [0, T] as |u| → ∞.

Theorem 3.3

If hypotheses (P), H(j)3 hold, then problem (1.3) has at least one nontrivial periodic solution.

Next, we will establish some existence results by using nonsmooth Mountain Pass theorem. Our hypotheses on the nonsmooth potential function j(t, u) are the following:

H(j)4 j : [0, T] × ℝN ↦ ℝ is a function such that j(t, 0) = 0 for every t ∈ [0, T];

  1. for all u ∈ ℝN , tj(t, u) is measurable;

  2. for almost all t ∈ [0, T], uj(t, u) is locally Lipschitz;

  3. for every w∂j(t, u), there exists αC([0, T], ℝ) such that for almost all t ∈ [0, T], we have

    | w | b ( t ) | u | α ( t ) 1 ,

    where b L α ( t ) [ 0 , T ] L + [ 0 , T ] a n d p + < α α ( t ) α + ;

  4. there exists constants M > 0, α, β > 0 and ν < p such that for almost all t ∈ [0, T] and all u ∈ ℝN \ {0}, we have

    0 p + + 1 α + β | u | v j ( t , u ) j 0 ( t , u ; u ) ;
  5. for every u ∈ ℝN , w∂j(t, u) we have

    lim | u | 0 w | u | p ( t ) 1 = 0 ;
  6. there exists a function q(t) > 0(p+ < qq(t) ≤ q+) such that for almost all t ∈ [0, T] and all u ∈ ℝN, we have

lim | u | + inf j ( t , u ) | u | q ( t ) > 0.

Theorem 3.4

If hypotheses (P), H(j)4 hold, then problem (1.3) has at least one nontrivial periodic solution.

Theorem 3.5

If hypotheses (P), H(j)4 (j), (i)-(iii), (v) and the following conditions hold:

(vi’) there exist μ > p+ and M > 0 such that

μ j ( t , u ) j 0 ( t , u ; u ) , t [ 0 , T ] , | u | M ,

and 0 T j t , u 0 d t > 0  as  u 0 R N , u 0 M .

Then problem (1.3) has at least one nontrivial periodic solution.

Proof of Theorem 3.1

We consider the locally Lipschitz energy functional φ : W p e r 1 , p ( t ) 0 , T ; R N R defined by

φ ( u ) = 0 T 1 p ( t ) u p ( t ) d t 0 T j ( t , u ) d t .

It is easy to verify that φ is locally Lipschitz by H(j)1 (iii) and (2.1).

Because of hypothesis H(j)1(iv) and Lemma 3 [35], for almost all t ∈ [0, T], u ∈ ℝN, we have

(3.1) j ( t , u ) G ( u ) + y ( t ) ,

where γL1[0, T], GC(ℝN , ℝ) is subadditive, i.e., G(x + y) ≤ G(x) + G(y) for all x, y ∈ ℝN and is coercive, i.e., G(u) → +∞ as |u| → ∞.

Consider the direct sum decomposition

W p e r 1 , p ( t ) 0 , T ; R N = R N V ,

where

V = v W p e r 1 , p ( t ) 0 , T ; R N : 0 T v ( t ) d t = 0 .

For every u W p e r 1 , p ( t ) 0 , T ; R N we have u = u ¯ + u ~ ,  where u ¯ R N , u ~ V . By (3.1), we have

(3.2) φ ( u ) = 0 T 1 p ( t ) u p ( t ) d t 0 T j ( t , u ) d t 1 p + 0 T u p ( t ) d t + 0 T G ( u ( t ) ) d t y 1 .

From the properties of the continuous function G mentioned above, we have

(3.3) G ( u ¯ ) = G ( u ¯ + u ~ ( t ) u ~ ( t ) ) G ( u ¯ + u ~ ( t ) ) + G ( u ~ ( t ) ) G ( u ¯ ) G ( u ~ ( t ) ) G ( u ( t ) ) G ( u ¯ ) u ~ ( t ) 4 G ( u ( t ) ) , t [ 0 , T ] .

Using (3.3) in (3.2), we obtain

(3.4) φ ( u ) 1 p + 0 T u ~ p ( t ) d t + G ( u ¯ ) T c 1 u ~ p ( t ) c 2 ,

where c1, c2 > 0.

Noting that u u ¯ + u ~ , by virtue of (2.1), (3.4) and the coercivity on G, we infer that φ is coercive.

Owing to the fact the compact embedding of W per  1 , p ( t ) 0 , T ; R N C 0 , T ; R N and the weak lower semi-continuity of the norm functional in a Banach space, we infer that φ is weakly lower semicontinuous. So by hypothesis H(j)1(v) and the Weierstrass theorem (Lemma 2.1) we can find u0 such that

< m = inf φ = φ ( u ) φ u 0 < 0 φ ( 0 ) u 0 , 0 φ ( u ) .

Next, we will show that u the solution of (1.3).

In fact, let u W p e r 1 , p ( t ) 0 , T ; R N be such that 0 ∈ ∂φ(u). Define the nonlinear operator A : W p e r 1 , p ( t ) 0 , T ; R N W p e r 1 , p ( t ) 0 , T ; R N as follows

< A ( u ) , v >= 0 T u p ( t ) 2 u ( t ) , v ( t ) R N d t , u , v W p e r 1 , p ( t ) 0 , T ; R N .

Thus,

A ( u ) = w ,

where wLq(t)(0, T;ℝN) and w ∈ ∂j(t, u(t)). Here 1 p ( t ) + 1 q ( t ) = 1.

For every x, y ∈ ℝN, the following inequalities hold [23]:

(3.5) | x | p 2 x | y | p 2 y , x y ( p 1 ) | x y | 2 1 + | x | 2 + | y | 2 p 2 2 , p [ 1 , 2 ] .

and

(3.6) | x | p 2 x | y | p 2 y , x y ( p 1 ) | x | p 2 2 + | y | p 2 2 x p 2 2 x | y | p 2 2 y , p [ 2 , + ) .

An argument similar to the one used in [37] shows that for every v W p e r 1 , p ( t ) 0 , T ; R N , thus

< A ( u ) , v >= 0 T u ( t ) p ( t ) 2 u ( t ) , v ( t ) d t = 0 T ( w ( t ) , v ( t ) ) d t ,

which implies that (|u'(t)|p(t)−2u'(t))' has T-weak derivative and satisfy

u ( t ) p ( t ) 2 u ( t ) = w .

It follows from C [ 0 , T ] , R N W p e r 1 , p ( t ) [ 0 , T ] , R N  and  W p e r 1 , p ( t ) [ 0 , T ] , R N C [ 0 , T ] , R N that u(t) is continuous for every t ∈ [0, T]. It is obviously that (|u'(t)|p(t)−2u'(t))'Lq(t)([0, T], ℝN). Since L q ( t ) L 1 , then we have (|u'(t)|p(t)−2u'(t))'L1([0, T], ℝN), which implies that u ( t ) p ( t ) 2 u ( t ) W p e r 1 , 1 [ 0 , T ] , R N . By Proposition 2.4 (2), we have

u ( 0 ) p ( 0 ) 2 u ( 0 ) = u ( T ) p ( T ) 2 u ( T ) .

Noting that p(0) = p(T), we can obtain u'(0) = u'(T). Since u W p e r 1 , p ( t ) 0 , T ; R N , then u(0) = u(T). So u is the solution of (1.3).

Proof of Theorem 3.2

Given δ > 0, by Lemma 2 [35] and H(j)2 (iv), we can find EδE such that meas(E\Eδ)< δ as |u| → ∞, j(t, u) → −∞ uniformly for all tEδ , u ∈ ℝN, so for almost all tEδ , u ∈ ℝN we have

(3.7) j ( t , u ) G ( u ) + y ( t ) ,

with GC(ℝN , ℝ), γL1(Eδ) as in the proof of Theorem 3.1. Then for every u W p e r 1 , p ( t ) 0 , T ; R N , by (3.4), (3.7) and H(j)2 (v) we have

φ ( u ) = 0 T 1 p ( t ) u p ( t ) d t 0 T j ( t , u ) d t 1 p + 0 T u p ( t ) d t E δ j ( t , u ) d t [ 0 , T ] E δ j ( t , u ) d t 1 p + 0 T u p ( t ) d t + E δ G ( u ( t ) ) d t y 1 β 1 1 p + 0 T u ~ p ( t ) d t + G ( u ¯ ) meas E δ c 3 u ~ p ( t ) c 4 .

where c3, c4 > 0. Therefore φ is coercive. The rest of the proof goes as that of Theorem 3.1.

Proof of Theorem 3.3

Consider the locally Lipschitz energy functional φ : W p e r 1 , p ( t ) 0 , T ; R N R defined by

φ ( u ) = 0 T 1 p ( t ) u ( t ) p ( t ) d t 0 T j ( t , u ( t ) ) d t .

Step 1: φ satisfies the nonsmooth C-condition.

Let {un}n≥1 be a (C)-sequence of φ, i.e., there exists M1 > 0 such that

φ u n M 1 , 1 + u n m u n 0.

Since φ u n W p e r 1 , p ( t ) 0 , T ; R N is weakly compact and the norm functional in a Banach space is weakly compact, from the Weierstrass theorem (Lemma 2.1), we can find u n φ u n such that m u n = u n .

Define the nonlinear operator A : W p e r 1 , p ( t ) 0 , T ; R N W p e r 1 , p ( t ) 0 , T ; R N

< A ( u ) , v >= 0 T u ( t ) p ( t ) 2 u ( t ) , v ( t ) R N d t , u , v W p e r 1 , p ( t ) 0 , T ; R N .

Then

u n = A u n w n ,

where wn ∈ ∂j(t, un).

From the choice of the sequence u n n 1 W p e r 1 , p ( t ) 0 , T ; R N we have

< u n , u n >= 0 T u n ( t ) p ( t ) d t 0 T w n ( t ) , u n ( t ) d t ϵ n , ϵ n 0.

Thus,

(3.8) 0 T u n ( t ) p ( t ) d t 0 T j 0 t , u n ( t ) ; u n ( t ) d t ϵ n ,

and also

(3.9) μ p + 0 T u n p ( t ) + 0 T μ j t , u n ( t ) d t μ M 1 .

It follows from (3.8) and (3.9) that

(3.10) 1 μ p + 0 T u n p ( t ) + 0 T μ j t , u n ( t ) j 0 t , u n ( t ) ; u n ( t ) d t ϵ n + μ M 1 .

By H(j)3 (iv), we have

0 T μ j t , u n ( t ) j 0 t , u n ( t ) ; u n ( t ) d t = u n M μ j t , u n ( t ) j 0 t , u n ( t ) ; u n ( t ) d t + u n > M μ j t , u n ( t ) j 0 t , u n ( t ) ; u n ( t ) d t c 5 ,

where c5 > 0 is independent of n.

Therefore, from (3.10) we have

1 μ p + 0 T u n p ( t ) ϵ n + μ M 1 + c 6 , n 1.

By the Poincare-Wirtinger inequality (2.1), u ~ n is bounded in W p e r 1 , p ( t ) 0 , T ; R N .

It follows from H(j)3 and Lemma 3 [35] that for almost all t ∈ [0, T] and all u ∈ ℝN, we have

(3.11) j ( t , u ) G ( u ) + y ( t ) ,

with γL1[0, T], GC(ℝN , ℝ) is subadditive, coercive and satisfies G(u) ≤ |u| + 4 for all u ∈ ℝN.

From the choice of the sequence u n n 1 W p e r 1 , p ( t ) 0 , T ; R N we have

1 p + 0 T u ~ n p ( t ) 0 T j t , u n ( t ) d t M 1 , n 1.

Since u ~ n is bounded, there exists M2 > 0, n ≥ 1 such that

0 T j t , u n ( t ) d t M 2 .

By (3.11), we get

0 T G u n ( t ) d t + y 1 M 2 ,

thus, there exists M3 > 0 such that G u ¯ n b M 3 , n 1.

Due to the coercivity of G, we infer that u ¯ n n 1 R N is bounded. Therefore u n n 1 W p e r 1 , p ( t ) 0 , T ; R N is bounded and so by passing to a subsequence if necessary, we may assume that

u n u  in  W per  1 , p ( t ) 0 , T ; R N , u n u  in  C per  0 , T ; R N .

Next, we will prove that u n u  in  W per  1 , p ( t ) 0 , T ; R N . By Proposition 2.13, it suffices to prove that the following inequality hold:

lim ¯ n < A u n A ( u ) , u n u >≤ 0 , ε n 0.

In fact, from the choice of the sequence {un}n≥1 we have

< u n , u n > ε n 0.

Recall that u n = A u n w n , then we have

< A u n , u n u > 0 T w n ( t ) , u n ( t ) u ( t ) R N d t ε n , n 1.

By H(j)3(iii), {wn}⊆ L1[0, T] is bounded and

0 T w n ( t ) , u n ( t ) u ( t ) R N d t 0 ( n ) .

Then

lim ¯ n < A u n , u n u >≤ 0.

So lim ¯ n < A u n A ( u ) , u n u >≤ 0 , ε n 0.

Step 2: Similar to the proof in [30, 31], we have j(t, sx) ≤ sμj(t, x) for every s ≥ 1, we omit its proof course.

Step 3: φ|V is coercive, i.e., for every vV, φ(v) → +∞ asv║ → ∞.

Let vV be such that |{tT : ║v(t) > M║}|1 > 0, we have

φ ( v ) = 0 T 1 p ( t ) v p ( t ) d t 0 T j ( t , v ( t ) ) d t = 0 T 1 p ( t ) v p ( t ) d t | v | M j ( t , v ( t ) ) d t | v | < M j ( t , v ( t ) ) d t .

Because of hypothesis H(j)3(iii) and the mean value theorem for locally Lipschitz functions, we see that there exists c7 > 0 such that

(3.12) | v | < M j ( t , v ( t ) ) d t c 7 .

Also using Step 2, we have

(3.13) | v | M j ( t , v ( t ) ) d t = | v | M j | v ( t ) | M M v ( t ) | v ( t ) | d t | v | M | v ( t ) | μ M μ j t , M v ( t ) | v ( t ) | d t v ( t ) μ M μ | v | M j t , M v ( t ) | v ( t ) | d t .

Noting that for ║u║ = M, from the subdifferential chain rule, for almost all tT we have

(3.14) j ( t , x ) = j ( t , 0 ) + 0 1 x j ( t , r x ) , x d r j ( t , x ) β M ( t ) , β M L 1 [ 0 , T ] .

By (3.13) and (3.14), we have

(3.15) | v | M j ( t , v ( t ) ) d t v μ M μ c 8 , c 8 > 0.

Using (3.15) and Poincare-Wirtinger inequality (2.1) we have

φ ( v ) 1 p v p ( t ) p c 8 M μ v μ c 9 1 p v p ( t ) p c 10 v p ( t ) μ c 11 ,

which yields that φ|V is coercive since μ < p.

Step 4: φ|RN is anticoercive, i.e., φ(y) → −∞ asy║ → ∞, y ∈ ℝN, this claim is a direct consequence of hypothesis H(j)3 (v).

Step 1, 3 and 4 permit the application of the nonsmooth saddle point theorem, so we can find u W p e r 1 , p ( t ) 0 , T ; R N such that

0 φ ( u ) .

As before, we can show that u W per  1 , p ( t ) 0 , T ; R N solves (1.3).

Proof of Theorem 3.4

Consider the locally Lipschitz energy functional φ : W p e r 1 , p ( t ) 0 , T ; R N R defined by

φ ( u ) = 0 T 1 p ( t ) u p ( t ) d t 0 T j ( t , u ( t ) ) d t .

We divide our proof into two steps.

Step 1: φ satisfies nonsmooth (C)-condition.

Let u n n 1 W p e r 1 , p ( t ) 0 , T ; R N be a (C)-sequence of φ, i.e., there exists M1 > 0 such that

φ u n M 1 , 1 + u n m u n 0 ( n ) .

It is apparent that m u n = u n , n 1 for some u n φ u n . Taking into account the fact that the set φ u n W p e r 1 , p ( t ) 0 , T ; R N is weakly compact, we define the nonlinear operator A : W p e r 1 , p ( t ) 0 , T ; R N W p e r 1 , p ( t ) 0 , T ; R N as follows

< A ( u ) , v >= 0 T u ( t ) p ( t ) 2 u ( t ) v ( t ) d t , u , v W p e r 1 , p ( t ) 0 , T ; R N .

From the definition of and Proposition 2.13 we know that A is maximal monotone (see [16]), hence we have

u n = A u n w n ,

where wnLq(t)(0, T;ℝN), wn(t) ∈ ∂j(t, un(t)), ∀ n ≥ 1, with 1 p ( t ) + 1 q ( t ) = 1. Then, we have

(3.16) C 1 p + φ u n u n , u n 0 T p + p ( t ) u n p ( t ) d t p + R j t , u n d t 0 T u n p ( t ) d t + R w n u n 0 T p + j t , u n d t j 0 t , u n ; u n d t

for every ( t , u ) [ 0 , T ] × R N { 0 } . By H ( j ) 4 (iv) we have

p + j t , u n j 0 t , u n ; u n 0

and

(3.17) j ( t , u ) α + β | u | v p + j ( t , u ) j 0 ( t , u ; u ) .

It follows from (2.1), (3.16) and (3.17) that

1 p + u n p ( t ) p 0 T 1 p ( t ) u n p + d t = I u n + 0 T j t , u n ( t ) d t I u n + 0 T α + β u n ( t ) v p + j t , u n j 0 t , u n ; u n d t
(3.18) C 2 + 0 α + β u n ( t ) v p + j t , u n j 0 t , u n ; u n d t C 2 + α + β u n v 0 T p + j t , u n j 0 t , u n ; u n d t C 2 + C 1 α + β u n v C 2 + C 1 α + β u n v C 2 + C 1 α + C ν β u n p ( t ) v ,

which yields that u n p ( t ) is bounded since ν < p.

We claim that ║un║ is bounded. If not, suppose that the sequence ║un║ is not bounded. Note that ║un║ = unp(t)+unp(t)andunp(t)is bounded, we have |un|p(t) → ∞. From Proposition 3.1 of [35], we have |un(t)| → ∞ as n → ∞ uniformly for t ∈ [0, T]. By virtue of H(j)4 (vi), there exists constants c1, M2 > 0 such that

j ( t , u ( t ) ) | u | q ( t ) c 1 > 0

as |u| ≥ M2. Namely,

(3.19) j ( t , u ( t ) ) c 1 | u | q ( t ) .

Then

(3.20) lim n 0 T j t , u n ( t ) d t = + .

However

0 T j t , u n ( t ) d t = 0 T 1 p ( t ) u n ( t ) p ( t ) d t φ u n ( t ) 1 p ρ u n + φ u n ( t )

is bounded, which is contrary to (3.20). Thus {un} is a bounded sequence in W p e r 1 , p ( t ) 0 , T ; R N and so we may assume that u n u  in  W per  1 , p ( t ) 0 , T ; R N .

Next, we prove that u n u  in  W per  1 , p ( t ) 0 , T ; R N . From Proposition 2.13, if suffices to prove that

lim ¯ n < A u n A ( u ) , u n u >≤ 0 , ε n 0.

Indeed, from the choice of the sequence {un}n≥1, we have

< u n , u n > ε n 0.

Using u n = A u n w n , we have

< A u n , u n u > 0 T w n ( t ) , u n ( t ) u ( t ) R N d t ε n , n 1.

Since {wn}n≥1L1[0, T] is bounded and

0 T w n ( t ) , u n ( t ) u ( t ) d t 0 ( n ) .

Then

lim ¯ n < A u n A ( u ) , u n u >≤ 0.

Step 2: φ satisfies nonsmooth Mountain Pass Theorem.

Let ε > 0 be small enough, by virtue of hypotheses H(j)4(iii), (v) we have

j ( t , u ) ε | u | p ( t ) + c ( ε ) | u | α ( t ) , ( t , u ) [ 0 , T ] × R N .

Let |u|p(t) = ρ be small enough, then

φ ( u ) 1 p + 0 T u ( t ) p ( t ) d t ε 0 T | u ( t ) | p ( t ) d t c ( ε ) 0 T | u ( t ) | α ( t ) d t 1 p + | u | p ( t ) p + ε 0 T u p ( t ) d t c ( ε ) 0 T | u | α ( t ) d t 1 p + | u | p ( t ) p + ε | u | p ( t ) p + c ( ε ) | u | p ( t ) α

For the arbitrariness of ε, we may choose ε small enough such that ε a 0 < 1 2 p + , then

φ ( u ) 1 2 p + | u | p ( t ) p + c ( ε ) | u | p ( t ) α .

Since p+ < α, there exist a constant r > 0 such that φ(u) ≥ r as ║u║ = ρ small enough.

By virtue of H(j)4 (vi), there exists constants c1, M2 > 0 such that

j ( t , u ( t ) ) | u | q ( t ) c 1 > 0

as |u| ≥ M2. Namely,

(3.21) j ( t , u ( t ) ) c 1 | u | q ( t ) .

By H(j)4 (iii), we have

(3.22) | j ( t , u ( t ) ) | c 2 b ( t ) , t [ 0 , T ] , | u | M 2 .

Then, for every u W p e r 1 , p ( t ) 0 , T ; R N { 0 }  and  σ > 1 we have

φ ( σ u ) = 0 T 1 p ( t ) σ u p ( t ) d t 0 T j ( t , σ u ) d t σ p + p 0 T u p ( t ) d t c 1 σ q 0 T | u | q ( t ) d t + c 2 0 T b ( t ) d t ,

which implies that φ(σu) → −∞ (σ → +∞) since q > p+.

As before, we can show that u W p e r 1 , p ( t ) 0 , T ; R N solves (1.3), we omit its proof process.

Acknowledgement

This work is partially supported by the NSFC (No:11871305) and supported by Foundation of Hubei Educational Committee (D20161206). The authors would like to express their gratitude to the referees for valuable comments and suggestions.

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Received: 2020-06-27
Accepted: 2020-09-30
Published Online: 2020-12-19

© 2021 Peng Chen and Xianhua Tang, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  63. Global well-posedness of the full compressible Hall-MHD equations
  64. Σ-Shaped Bifurcation Curves
  65. On the critical behavior for inhomogeneous wave inequalities with Hardy potential in an exterior domain
  66. On singular quasilinear elliptic equations with data measures
  67. On the sub–diffusion fractional initial value problem with time variable order
  68. Partial regularity of stable solutions to the fractional Geľfand-Liouville equation
  69. Ground state solutions for a class of fractional Schrodinger-Poisson system with critical growth and vanishing potentials
  70. Initial boundary value problems for the three-dimensional compressible elastic Navier-Stokes-Poisson equations
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