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ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu

INFINITELY MANY SOLUTIONS FOR KIRCHHOFF TYPE PROBLEMS WITH NONLINEAR NEUMANN BOUNDARY

CONDITIONS

WEI-BING WANG, WEI TANG

Abstract. In this article, we study a Kirchhoff type problem with nonlinear Neumann boundary conditions on a bounded domain. By using variational methods, we prove the existence of infinitely many solutions.

1. Introduction

In this work, we study the multiplicity of solutions for the elliptic problem

−h MZ

|∇u|pdxip−1

pu=f(x, u), in Ω,

|∇u|p−2∂u

∂ν =λk(u) +µg(u), on∂Ω,

(1.1)

where M(t) =a+bt, p > N,a >0, b≥0, Ω is a nonempty bounded open subset ofRN with a boundary of classC1, ∂u∂ν is the outer unit normal derivative, ∆pu:=

div(|∇u|p−2∇u) is thep-Laplacian operator,λ, µ are positive real parameters, the functionsf, k, g satisfy hypotheses stated as follows:

(H1) k, g∈C(R,R) and there exist two positive constantsρ, ρ such that

|K(u)|+|G(u)| ≤ρ(|u|ρ+ 1) for allu∈R, where K(u) =Ru

0 k(s)ds,G(u) =Ru 0 g(s)ds.

(H2) f ∈C(Ω×R,R) and there exist two positive constantsa1, a2 such that a1|u|p≤ −F(x, u)≤a2|u|p

for all (x, u)∈Ω×R, whereF(x, u) =Ru

0 f(x, s)ds.

(H3) f ∈C(Ω×R,R) and there exist two positive constants%, % such that

|F(x, u)| ≤%(|u|%+ 1) for all (x, u)∈Ω×R.

(H4) there exist two positive constantsb1, b2 such that b1|u|p≤ −G(u)≤b2|u|p for allu∈R.

2010Mathematics Subject Classification. 35J60, 35J20.

Key words and phrases. Kirchhoff type equation; weak solution; critical point.

c

2016 Texas State University.

Submitted December 18, 2015. Published July 13, 2016.

1

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Problem (1.1) is the nonlocal problem, which is related to the model introduced by Kirchhoff [15],

ρ∂2u

∂t2 −ρ0

h + E 2L

Z L 0

|∂u

∂x|2dx∂2u

∂x2 = 0, (1.2)

which extends the classical D’Alembert’s wave equation by considering the effects of the changes in the length of the strings during the vibrations. Interest of the mathematicians on the nonlocal problems has increased because they represent a variety of relevant physical and engineering situations[4, 12]. Many interesting results for Kirchhoff type problems were obtained and we refer to[1, 2, 3, 8, 9, 11, 13, 14, 17, 18, 19] and references therein for an overview on these subjects.

Relatively speaking, Kirchhoff type problems with nonlinear boundary conditions have rarely been considered. In addition, when involving the existence of infinitely many solutions, most results assume that nonlinear term is odd in order to apply some variant of the classical Lusternik-Schnirelmann theory and only a few papers deal with nonlinearities having no symmetry properties[5, 6, 16].

The main purpose of this article is to establish the existence of infinitely many solutions for (1.1) without the assumption of symmetry property, by adopting the framework of Bonanno and Molica Bisci [6].

2. Preliminaries

LetX be a reflexive real Banach space andIλ :X →Ra functional satisfying the structure hypothesis:

(H5) Iλ(u) = Ψ(u)−λΦ(u) for allu∈X, where Ψ,Φ :X→Rare two functions of class C1 onX with Ψ coercive, i.e. limkuk→+∞Ψ(u) = +∞, andλis a real parameter.

Provided that infXΨ< r, put φIλ(r) := inf

u∈Ψ−1(]−∞,r[)

supu∈(Ψ−1]−∞,r[)Φ(u)

−Φ(u)

r−Ψ(u) ,

γ:= lim inf

r→+∞φIλ(r), δ:= lim inf

r→(infXΨ)+φIλ(r).

When γ = 0( or δ = 0) we agree to read γ1 (or 1δ) as +∞. Our main tool is a smooth version of critical point theorem which are recalled below, see [6].

Theorem 2.1. Assume that (H5)holds. Then:

(a) For each r > infXΨ and every λ ∈]0,1/φIλ(r)[, the restriction of the functional Iλ to Ψ−1(]− ∞, r[) has a global minimum, which a s critical point (local minimum) of Iλ inX.

(b) Ifγ <+∞, then, for eachλ∈]0,1/γ[, the following alternative holds:either (1) Iλ possess a global minimum, or

(2) there is a sequence{un}of critical points of Iλ such that limn→∞Ψ(un) = +∞.

(c) Ifδ <+∞, then, for eachλ∈]0,1/δ[, the following alternative holds: either (1) there is a global minimum ofΦwhich is a local minimum of Iλ, or (2) there is a sequence{un}of pairwise distinct critical points of Iλ such

thatlimn→∞Ψ(un) = infXΨ, which weakly converges to a global min- imum ofΦ.

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LetW1,p(Ω) be the usual Sobolev space endowed with the norm kuk:=Z

(|∇u|p+|u|p)dx1/p

or

kuk:=Z

|∇u|pdx+ Z

∂Ω

|u|p1/p ,

wheredσ is the measure on the boundary. Clearly,k · kis equivalent tok · k. Let k := sup

u∈W1,p(Ω)\{0}

maxx∈Ω|u(x)|

kuk , k:= sup

u∈W1,p(Ω)\{0}

maxx∈Ω|u(x)|

kuk

(2.1) Sincep > N, the embeddingW1,p(Ω),→C(Ω) is compact, and thus 0<k,k<∞,

|u(x)| ≤kkuk, |u(x)| ≤kkuk foru∈W1,p(Ω). (2.2) A weak solution of problem (1.1), we mean that a functionu∈W1,p(Ω) satisfies

h MZ

|∇u|pdxip−1Z

|∇u|p−2∇u∇vdx

− Z

f(x, u)vdx− Z

∂Ω

(λk(u) +µg(u))vdσ= 0 for everyv∈W1,p(Ω).

Define the functionals onW1,p(Ω) by Γ(u) =1

p

Z R|∇u|pdx 0

Mp−1(s)ds= ( 1

bp2

a+bR

|∇u|pdxp

−ap

, b >0,

ap−1 p

R

|∇u|pdx, b= 0,

ψ(u) = Γ(u)− Z

F(x, u)dx, ϕ(u) = Z

∂Ω

K(u) +µ λG(u)

dσ, ψ(u) = Γ(u)−µ

Z

∂Ω

G(u)dσ, ϕ(u) = Z

∂Ω

K(u)dσ+1 λ

Z

F(x, u)dx, Jλ(u) =ψ(u)−λϕ(u), Iλ(u) =ψ(u)−λϕ(u).

Conditions (H1) and (H2) (or (H1) and (H3)) and p > N guarantee thatψ, ϕ (orψ, ϕ) are well defined and of classC1. Moreover,

hJλ0(u), vi=hIλ0(u), vi

=h MZ

|∇u|pdxip−1Z

|∇u|p−2∇u∇vdx

− Z

f(x, u)vdx− Z

∂Ω

(λk(u) +µg(u))vdσ.

Hence, the critical points ofJλ or Iλ are the weak solutions of (1.1).

3. Main results Put

a3=ap−1

p , a1 , b3=ap−1

p , b1 , |Ω|= Z

dx, |∂Ω|= Z

∂Ω

dσ.

Moreover, let

A:= lim inf

ξ→+∞

max|t|≤ξK(t)

ξp , A0:= lim inf

ξ→0+

max|t|≤ξK(t)

ξp ,

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B:= lim sup

ξ→+∞

K(ξ)

ξp , B0:= lim sup

ξ→0+

K(ξ) ξp , G:= lim sup

ξ→+∞

max|t|≤ξG(t)

ξp , G0:= lim sup

ξ→0+

max|t|≤ξG(t)

ξp .

F:= lim sup

ξ→+∞

R

max|t|≤ξF(x, t)dx

ξp , F0:= lim sup

ξ→0+

R

max|t|≤ξF(x, t)dx ξp

We present our main results as follows.

Theorem 3.1. Assume that (H1), (H2) hold and there exist two real sequences {αn},{βn} with limn→∞βn = +∞and a positive constant ρ >0 such that

n|< 1 k

a3

a2|Ω|

1/p

βn, G(t)≥0, ∀t≥ρ, A:= lim

n→∞

max|t|≤βnK(t)−K(αn) βnp−kpa2a−13 |Ω|αnp

< a3B kp|Ω|a2

, G:= lim

n→∞

max|t|≤βnG(t)−G(αn) βnp−kpa2a−13 |Ω|αpn

<+∞.

Then for eachλ∈Λ :=]λ1, λ2[, where λ1= |Ω|a2

|∂Ω|B, λ2= a3

kp|∂Ω|A, there existsµλ>0, where

µλ= 1 G

a3

kp|∂Ω| −λA

,

such that for all µ∈[0, µλ[,(1.1)has an unbounded sequence of weak solutions.

Proof. First, we observe that owing to the condition A < a3B/(kp|Ω|a2), the interval Λ is non-empty. Moreover, for each fixed ¯λ∈ Λ and taking into account that A¯λ < a3/kp|∂Ω|, one has 0< µλ¯ <∞. Our aim is to apply Theorem 2.1.

For this end, we showγ <+∞, where γis defined in Theorem 2.1.

By Assumption (H2), we have

a3kukp≤ψ(u)≤max(2a)p−1

p , a2 kukp+(2b)p−1

p kukp2. (3.1) Putrnpna3/kp for alln∈N, by (2.2) and (3.1), one has

ψ−1(]− ∞, rn])⊆ {u∈W1,p(Ω) :kuk≤βn}, ψ(αn) =−

Z

F(x, αn)dx≤a2|Ω|αpn< rn. Hence,

φJλ(rn) = inf

u∈ψ−1(]−∞,rn[)

supu∈(ψ−1]−∞,rn[)ϕ(u)

−ϕ(u) rn−ψ(u)

≤ inf

ψ(u)<rn

|∂Ω|max|t|≤βn[K(t) +µ¯λG(t)]−ϕ(u) rn−ψ(u)

≤|∂Ω|max|t|≤βn[K(t) +µλ¯G(t)]−ϕ(αn) rn−ψ(αn)

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≤|∂Ω|max|t|≤βn[K(t)−K(αn)]

rn−a2|Ω|αpn

¯λ

|∂Ω|max|t|≤βn[G(t)−G(αn)]

rn−a2|Ω|αpn

≤kp|∂Ω|

a3

A+µ λ¯G

<+∞.

Sinceµ∈[0, µ¯λ[, γ≤lim inf

n→+∞φJλ(rn)< kp|∂Ω|

a3

Aλ¯

λ¯ G

= 1

¯λ<+∞;

that is, 0< λ1 <λ <¯ 1/γ. The condition (b) of Theorem 2.1 can be applied and either Jλ¯ has a global minimum or there exists a sequence {un} of weak solutions of the problem (1.1) such thatkunk → ∞asn→ ∞.

Now, we verify thatJ¯λis unbounded from below. First, assume thatB= +∞.

Accordingly, fixed C with C > a2|Ω|/¯λ|∂Ω| and {cn} be a sequence of positive numbers withcn→+∞asn→ ∞such that

K(cn)> Ccpn, nsufficiently large.

Taking the sequence {vn} ⊆W1,p(Ω) such that vn(x) = cn, x ∈ Ω, for the suffi-¯ ciently largen, one has

Jλ¯(vn) =− Z

F(x, vn)dx−¯λ Z

∂Ω

K(vn)dσ−µ Z

∂Ω

G(vn)dσ

≤a2|Ω|cpn−¯λ Z

∂Ω

K(vn)dσ≤(a2|Ω| −Cλ|∂Ω|)c¯ pn; that is,J¯λ→ −∞as n→ ∞.

Next, assume that B <+∞. Since ¯λ > λ1 =a2|Ω|/|∂Ω|B, we fix 0< ε <

Bλ|∂Ω|a¯2|Ω|. Let{cn}be a sequence of positive numbers withcn →+∞asn→ ∞ such that

(B−ε)cpn< K(cn)<(B+ε)cpn, nsufficiently large

Arguing as before and by choosingvn≡cn, for the sufficiently largen, one has Jλ¯(vn) =−

Z

F(x, vn)dx−¯λ Z

∂Ω

K(vn)dσ−µ Z

∂Ω

G(vn)dσ

≤a2|Ω|cpn−(B−ε)¯λ|∂Ω|cpn → −∞ as n→ ∞.

Hence,J¯λ is unbounded from blew and the proof is complete.

Corollary 3.2. Assume that (H1), (H2) hold. Further suppose that G <+∞, A < a3B/(kp|Ω|a2) and there exists ρ > 0 such that G(t) ≥0 for all t ≥ ρ.

Then for eachλ∈]λ3, λ4[, where λ3= |Ω|a2

|∂Ω|B

, λ4= a3 kpA|∂Ω|, there existsµ˜λ>0, where

˜ µλ= 1

G a3

kp|∂Ω|−λA ,

such that for all µ∈[0,µ˜λ[,(1.1)has an unbounded sequence of weak solutions.

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Proof. Let{βn}be a sequence of positive numbers which approaches infinity such that

A= lim

ξ→+∞

max|t|≤βnK(t) βpn

. Takingαn = 0 for everyn∈Nand noting that

G= lim

n→+∞

max|t|≤βnG(t) βnp

≤G,

from Theorem 3.1, we obtain the conclusion.

Applying part (c) of Theorem 2.1, we get the following theorem.

Theorem 3.3. Assume that (H1), (H2) hold and there exist two real sequences {αn},{βn} with limn→∞βn = 0and positive constant ρ >0 such that

n|<1 k

a3

a2|Ω|

1/p

βn, G(t)≥0, ∀0≤t≤ρ, A0:= lim

n→∞

max|t|≤βnK(t)−K(αn) βnp−kpa2a−13 |Ω|αnp

< a3B0

kp|Ω|a2, G0:= lim

n→∞

max|t|≤βnG(t)−G(αn) βnp−kpa2a−13 |Ω|αpn

<+∞.

Then for eachλ∈]λ4, λ5[, where λ4= |Ω|a2

|∂Ω|B0

, λ5= a3 kp|∂Ω|A0

, there existsµ¯λ>0, where

¯ µλ= 1

G0

a3

kp|∂Ω| −λA0

,

such that for allµ∈[0,µ¯λ[,(1.1)has a sequence of weak solutions, which converges strongly to zero.

Corollary 3.4. Assume that (H1), (H2) hold. Further suppose that G0 < +∞, A0 < a3B0/(kp|Ω|a2)and there existsρ >0 such thatG(t)≥0 for all 0 < t≤ρ.

Then for eachλ∈]λ7, λ8[, where λ7= |Ω|a2

|∂Ω|B0

, λ8= a3 kpA0|∂Ω|, there existsµˆλ>0, where

ˆ µλ= 1

G0 a3

kp|∂Ω|−λA0 ,

such that for allµ∈[0,µˆλ[,(1.1)has a sequence of weak solutions, which converges strongly to zero.

Now, we consider the case when (H1), (H3), (H4) hold.

Theorem 3.5. Assume that(H1), (H3), (H4)hold andF(x, u)≥0 forx∈Ω, u≥ r >0. If there exists the positive constantλ¯ such that

λB¯ > b2, F< b3

kp −λ|∂Ω|A¯ ,

then (1.1)has an unbounded sequence of weak solutions for λ= ¯λ,µ= 1.

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Proof. Letλ= ¯λ, µ= 1 and{βn}be a sequence of positive numbers withβn→+∞

asn→ ∞such that

A= lim

n→+∞

max|t|≤βnK(t) βnp

. By Assumption (H4), we have

b3kukp≤ψ(u)≤max(2a)p−1 p , b2

okukp+(2b)p−1

p kukp2. (3.2) Putrnpnb3/kp for alln∈N, by (2.2) and (3.2), one has

ψ−1(]− ∞, rn])⊆ {u∈W1,p(Ω) :kuk≤βn}.

Hence,

φIλ(rn) = inf

u∈ψ−1 (]−∞,rn[)

supu∈(ψ−1

]−∞,rn[)ϕ(u)

−ϕ(u) rn−ψ(u)

≤ supu∈(ψ−1

]−∞,rn[)ϕ(u) rn

≤ max{u∈X:kuk≤βn}ϕ(u) rn

≤ kp b3

|∂Ω|max|t|≤βnK(t) βnp

+ 1 λ¯ R

max|t|≤βnF(x, t)dx βnp

≤ kp b3

|∂Ω|A+ 1 λ¯F

< 1

¯λ.

The rest proof is similar to that of Theorem 3.1 and we omit it.

Theorem 3.6. Assume that(H1), (H3), (H4)hold andF(x, u)≥0 forx∈Ω,¯ 0≤ u≤r(r >0). If there exists the positive constantλ¯ such that

λB¯ 0> b2, F0< b3 kp

−λ|∂Ω|A¯ 0,

then (1.1) has a sequence of weak solutions for λ = ¯λ, µ = 1, which converges strongly to zero.

4. Examples

In this section, we present the two examples which provide the problems that admit infinitely many solutions.

Example 4.1. Consider the differential equation

−h 1 +b

Z 1 0

|u0|2dxi

u00(x) +u(ucosu+ 2 sinu+ 4) = 0, x∈(0,1),

−u0(0) =λk(u(0)) +µg(u(0)), u0(1) =λk(u(1)) +µg(u(1)),

(4.1)

whereb≥0,

k(u) =

(u2sin(lnu), u >0,

0, u≤0, g(u) =u−sinu.

Then

f(u) =−u(ucosu+ 2 sinu+ 4), −F(u) =u2(2 + sinu),

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K(u) = (u3

8[3 sin(lnu)−cos(lnu)], u >0,

0, u≤0,

G(u) = 1

2u2+ cosu−1, |Ω|=|∂Ω|= 1, a1= 1, a2= 3, a3=1 2. According to [7, Remark 1], one has the estimate k≤√

2. Taking αn=e(2n+1)π, βn =e2(n+1)π, we easily obtain that

A= 0, B= +∞, G= e−1 2(e−6k2).

By Theorem 3.1, (4.1) has an unbounded sequence of weak solutions for λ >0, 0≤µ < e−6k2

k2(e−1). Example 4.2. Consider the differential equation

−h MZ

|∇u|pdxip−1

pu=c(x)|u|ρ−1u, in Ω,

|∇u|p−2∂u

∂ν =λk(u)− |u|p−2u, on∂Ω,

(4.2)

whereM(t) =a+bt,p > N,a >0, b≥0, 1< ρ < p,c∈C(Ω) andc(x)≥0, Ω is a nonempty bounded open subset ofRN with a boundary of classC1,

k1= 2, kn+1=k12n , ln=k10n , n∈N, k(t) =





(lp−0.5n −kp+0.5n )(1− |ln−t|), ln−1≤t≤ln+ 1, n≥1, (kn+1p+0.5−lp−0.5n )(1− |kn+1−t|), kn+1−1≤t≤kn+1+ 1, n≥1,

0, otherwise.

Noting that

K(kn+ 1) =knp+0.5−k1p+0.5, K(ln+ 1) =lp−0.5n −k1p+0.5, n≥2, we have

n→∞lim

K(kn+ 1)

(kn+ 1)p = +∞, lim

n→∞

K(ln+ 1) (ln+ 1)p = 0.

Hence, A = 0, B = +∞. It is easy to check that F = 0. By Theorem 3.5, (4.2) has an unbounded sequence of weak solutions for allλ >0.

Acknowledgments. The authors express their gratitude to the reviewers for care- ful reading and helpful suggestions which led to an improvement of the original manuscript. The work is supported by Hunan Provincial Natural Science Founda- tion of China (2015JJ2068) and NNSF of China (11501190).

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Wei-Bing Wang (corresponding author)

Department of Mathematics, Hunan University of Science and Technology, Xiangtan, Hunan 411201, China

E-mail address:[email protected]

Wei Tang

Department of Mathematics, Hunan University of Science and Technology, Xiangtan, Hunan 411201, China

E-mail address:[email protected]

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