R E S E A R C H
Open Access
Bounded solutions for the nonlinear wave
equation
Tacksun Jung
1and Q-Heung Choi
2**Correspondence: [email protected] 2Department of Mathematics
Education, Inha University, Incheon, 402-751, Korea
Full list of author information is available at the end of the article
Abstract
We investigate the number of periodic weak solutions for the wave equation with nonlinearity decaying at the origin. We get a theorem which shows the existence of a bounded weak solution for this problem. We obtain this result by approaching the variational method and applying the critical point theory for the indefinite functional induced from the invariant subspaces and the invariant functional.
MSC: 35L05; 35L70
Keywords: wave equation; critical point theory; invariant function; invariant subspace; (P.S.)ccondition; eigenvalue problem
1 Introduction and statement of the main result
Letg(x,t,u) be aCfunction from [,π]×R×RtoRandT-periodic int. In this paper we are concerned with the number of weak periodic solutions of the following wave equation with boundary and periodic conditions:
utt–uxx=g(x,t,u),
u(,t) =u(π,t) = ,
u(x,t+T) =u(x,t),
ut(x, ) =ut(x,T) ∀x∈[,π],
(.)
whereT is a rational multiple ofπ. We assume thatgsatisfies the following conditions:
(g) g∈C([,π]×R×R,R)isT-periodic int,
(g) g(x,t, ) = ,g(x,t,ξ) =o(|ξ|)uniformly with respect tox∈[,π]andt∈R, (g) there existsC> such that|g(x,t,ξ)|<C∀x∈[,π],t∈R,ξ∈R.
Nonlinear problem of this type has been considered by many authors (cf.[–]).
The purpose of this paper is to show the existence ofT-periodic weak solutions of prob-lem (.).
Our main result is as follows.
Theorem . Assume that g satisfies(g)-(g).Then problem(.)has at least one bounded solution.
For the proof of our main result, we approach the variational method and apply the critical point theory induced from the invariant subspaces and the invariant functional.
The outline of the proof of Theorem . is as follows. In Section , we introduce two Banach spacesHandEof functions satisfying some symmetry properties, stable byA(Au=utt–
uxx),g such that the intersection ofHwith the kernel ofAis reduced to . The search
of a solution of problem (.) in the spaceH reduces the problem to a situation where A–is a compact operator. In Section , we introduce a functionalIdefined onEwhose critical points and weak solutions of (.) possess one-to-one correspondence. We prove thatI∈C(E,R) and satisfies the Palais-Smale condition. By a critical point theorem for
indefinite functionals (cf.[]), we prove that there exists at least one solution of (.) which is bounded, and we prove Theorem ..
2 Invariant Banach space
Let= (,π)×(,T);Tis a rational multiple ofπ
T=πb a ,
whereaandbare coprime integers. LetAbe the operator defined by
D(A) =u∈C()|u(,t) =u(π,t) = ∀t∈[,T],
u(x, ) =u(x,T) ∀x∈[,π],
ut(x, ) =ut(x,T) ∀x∈[,π]
,
Au=utt–uxx.
LetAbe the adjoint ofAinL(). We investigate the weak solutions of
Au=g(x,t,u).
We note that the eigenvalues ofAareλjk=j– (Tπk),j= , , . . . andk= , , , . . . , and the
corresponding eigenfunctions are
sinjxsinπkt
T and sinjxcos πkt
T .
We also note that the set of functionssinjxsinπTkt,sinjxcosπTkt is an orthogonal base forL(). Letube a function ofL(). Then there exists one and only one function of
L([,π]×R) which isT-periodic intand equalsuon. We shall denote this function
byu. Let us denote an elementu, inL(), by
u=
j>,k
ujksinjxexpik
a bt
with
uj,k=u¯j,–k.
We assume thatbis even andais odd. LetHbe the closed subspace ofL() defined by
H=
u∈L()u(x,t) = –u
x,t+T
ThenHis invariant under shift: Leth∈Handτ be a real number. Ifv(x,t) =u(x,t+τ), thenv∈H.His invariant underg: Letu∈Hsuch thatg(u)∈L(). Theng(u)∈H. Let
˜
u(x,t) =u(x,t+T). Then
u=
j>,k
ujk(–)ksinjxexpik
a bt.
Therefore
u∈H ⇐⇒ uj,k= for any evenk. (.)
LetAbe a linear operator ofHdefined by
D(A) =D(A)∩H,
Au=Au.
ThenAis self-adjoint inHandH∩N(A) ={}, whereN(A) is the kernel ofA. In fact, let
u∈H∩N(A). Then
u=uj,ksinjxexpik
a bt,
j–k
a
b = ⇒ uj,k= .
Letjandkbe such that
j–k
a
b = .
Sincebis even andais odd,kis even. Using (.), we haveuj,k= , and thereforeH∩N(A) =
{}. The eigenvalues ofAarej– (πTk), wherejis odd andkis even andH∩N(A) ={}.
Givenu∈H, we write
u=
j>
uj,ksinjxexpi
πkt
T , jis odd,kis even
with
uj,k=u¯j,–k.
Let
E=
u∈H
j,k
j–a
k
b
· |uj,k|< +∞ ,
(u,v) =
j,k
j–a
k
b
where ( , ) is a scalar product onE. With this scalar product,Eis a Hilbert space with a norm
u= (u,u), u∈E.
Let
ur=
|u|r
r
, r≥.
By the classical theorem of Riesz (cf.[, p.]), we have
ur≤
πT
r
j,k
|uj,k|r
r
, r≥, r+
r= .
Since for every>o
jodd,keven
|j–ak
b |+
<∞,
it follows that for everyr∈[, +∞), there iscr∈Rsuch that
ur≤cru. (.)
Let
E+=
uu∈E,uj,k= ifj–
ak b < ,
E–=
uu∈E,uj,k= ifj–
ak
b > .
Then E=E+⊕E–. Let P+ be the orthogonal projection fromE ontoE+ andP– be the
orthogonal projection fromEontoE–. We can writeu=P+u+P–uforu∈E.
3 Critical point theorem and the proof of Theorem 1.1 Now, we are going to seek a functionuinEsuch that
Au=g(x,t,u). (.)
We consider the associated functional of (.),
I(u) =
–|ut|+|ux|
dx dt–
G(x,t,u)dx dt
=
P+u–P–u
–
G(x,t,u)dx dt, (.)
where
G(x,t,u) = u
g(x,t,s)ds.
We recall the critical point theorem for the indefinite functional (cf.[]). Let
Br=
u∈H|u ≤r, ∂Br=
u∈H|u=r.
Theorem .(Critical point theorem for the indefinite functional) Let E be a real Hilbert space with E=E⊕Eand E=E⊥.Suppose that I∈C(E,R)satisfies(PS),and that
(I) I(u) =(Lu,u) +bu,whereLu=LPu+LPuandLi:Ei→Eiis bounded and
self-adjoint,i= , , (I) bis compact,and
(I) there exist a subspaceE˜⊂Eand setsS⊂E,Q⊂ ˜Eand constantsα>ωsuch that
(i) S⊂EandI|S≥α,
(ii) Qis bounded andI|∂Q≤ω,
(iii) Sand∂Qlink.
Then I possesses a critical value c≥α.
The eigenvalues ofAareλjk =j– (Tπk), wherejis odd andkis even,j= , , . . . and
k= , , , . . . . ThusA–
is a compact operator.
It is convenient for the following to rearrange the eigenvaluesλjk, wherejis odd andkis
even, by increasing magnitude: from now on we denote by (η–i)i≥=λjk< the sequence
of negative eigenvalues, by (η+i)i≥=λjk> the sequence of positive ones, so that
· · · ≤ηi–≤ · · · ≤η–≤η– <η+ ≤η+≤ · · · ≤η+i ≤ · · ·. (.)
We note that each eigenvalue has a finite multiplicity and thatη–
i →–∞,ηi+→+∞as
i→ ∞.
We shall show that the functionalIsatisfies the geometrical assumptions of the critical point theorem for the indefinite functional.
By the following lemma, I(u)∈C(E,R) and the solutions of (.) coincide with the
nonzero critical points ofI(u).
Lemma . Assume that g satisfies(g)-(g).Then I(u)is continuous and Fréchet differ-entiable in E with the Fréchet derivative
I(u)h=
–ut·ht+ux·hx–g(x,t,u)h
dx dt
= (P+u,P+h) – (P–u,P–h) –
g(x,t,u)h dx dt
for all h∈E.Moreover,if we set
F(u) =
G(x,t,u)dx dt,
then F(u)is continuous with respect to weak convergence,F(u)is compact,and
F(u)h=
g(x,t,u)h dx dt for all h∈E.
For the proof of Lemma ., refer to [].
Lemma . Assume that g satisfies(g)-(g).The problem
utt–uxx in E,
u(,t) =u(π,t) = ,
u(x,t+T) =u(x,t),
ut(x, ) =ut(x,T) ∀x∈[,π]
(.)
has only a trivial solution.
Proof LetAu=utt–uxx. SinceH∩N(A) ={},E∩N(A) ={}. Thus (.) has only a trivial
solution.
Lemma . Assume that g satisfies(g)-(g).Then I(u)satisfies the Palais-Smale condi-tion:If for a sequence(um),I(um)is bounded from above and I(um)→as m→ ∞,then
(um)has a convergent subsequence.
Proof Let (um) be a sequence withI(um)≤MandI(um)→ asm→ ∞. It suffices to
show that (um) is bounded. By contradiction, we suppose thatum → ∞asm→ ∞. Let
wm=uumm. Thenwm= andwmconverges weakly to an element, sayw. Then we have
M
um
≤ I(um)
um
=
–(wm)t+(wm)xx
–
G(x,t,um)
um
. (.)
SinceG(x,t,u) is bounded, lettingm∞in (.), we have
≤limP+wm–limP–wm=
–|wt|+|wxx|
. (.)
On the other hand, we have
←− I
(u
m)
um
=
–(wm)t
+(wm)xx
–
g(x,t,um)
um
. (.)
Lettingm→ ∞in (.), we have
= lim
m→∞P+wm
– lim
m→∞P–wm
=
–|wt|+|wxx|
=P+w–P–w. (.)
By (.) and (.), limm→∞P+wm =P+w and limm→∞P–wm =P–w. Thus limm→∞wm=w, sowm converges strongly to wand by (.),wis a weak solution
of the problem
wtt–wxx= inE.
Let
Q= (B¯R∩E–)⊕ {re|e∈∂B∩E+ <r<R}.
Lemma . Assume that g satisfies the conditions(g)-(g).There exist a subspaceE˜⊂E and sets∂Bρ⊂E,Q⊂ ˜E and constantsρ> andα> such that
(i) ∂Bρ⊂E+andI|∂Bρ≥α,
(ii) there aree∈∂B∩E+andR>ρsuch that ifQ= (B¯R∩E–)⊕ {re| <r<R},then
I|∂Q≤,
(iii) there existsu∈E\Qsuch thatu>RandI(u)≤, (iv) ∂Bρand∂Qlink.
Proof (i) Letu∈E+. SinceG(x,t,u) is bounded, there exists a constantC> such that
I(u) = P+u
–
P–u
–
G(x,t,u)
≥
P+u
–C
forC> . Then there exist a constantρ> and a constantα> such that ifu∈∂Bρ∩E+,
thenI(u)≥α.
(ii) Let us choose an elemente∈B∩E+. Letu∈(B¯r∩E–)⊕ {re| <r}. Thenu=v+w,
v∈Br∩E–,w=re. We note that
ifv∈Br∩E–, then
–|vt|+|vx|
dx dt≤ηi–vL()< .
Thus we have
I(u) = r
–
v
–
G(x,t,v+re)
≤
r
+
η
–
vL()+C
forC> . Then there existsR>ρ> such that ifu∈Q= (B¯R∩E–)⊕ {re| <r<R}, then
I(u)|∂Q≤.
(iii) Let us chooseu∈E\Q. By (ii),I(u)≤.
(iv)SandQlink at the set{e}.
Proof of Theorem. By Lemma .,I(u) is continuous andFréchetdifferentiable inE. By Lemma ., the functional I satisfies the (PS) condition. We note that I() = . By Lemma ., there are constantsρ> ,α> and a bounded neighborhoodBρof such that
I|∂Bρ∩E+≥α, and there aree∈∂B∩E+andR>ρsuch that ifQ= (B¯R∩E–)⊕{re| <r<R}.
Let us set
=γ ∈C(Q,¯ H)|γ = id on∂Q.
By Theorem .,Ipossesses a critical valuec≥α. Moreover,ccan be characterized as
c=inf γ∈maxu∈QI
Thus we prove thatIhas at least one nontrivial critical point, we denote byu˜ a critical point ofIsuch thatI(u) =˜ c. We claim thatcis bounded. In fact, we have
c≤ max ≤τ≤I(τu),
and by (g),
I(τu) =τ
P+u
–
P–u
–
G(x,t,τu)dx dt
≤τu–
G(x,t,τu)dx dt
≤Cτu+C
for some constantC> . Since ≤τ≤,cis bounded:
c<C.˜ (.)
We claim thatu˜is bounded. In fact, by contradiction,u˜tt+u˜xx=g(x,t,u) and, for any˜ K> ,
max|˜u(x,t)|>Kimply that
c=I(u) =˜
P+u˜–P–u˜
–
G(x,t,u)˜ dx dt
is not bounded, which is absurd to the fact thatc=I(u) is bounded. Thus˜ u˜is bounded, so (.) has at least one bounded weak solution, and hence we prove Theorem ..
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Author details
1Department of Mathematics, Kunsan National University, Kunsan, 573-701, Korea.2Department of Mathematics
Education, Inha University, Incheon, 402-751, Korea.
Acknowledgements
This work (Choi) was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (KRF-2013010343).
Received: 27 June 2013 Accepted: 25 October 2013 Published:25 Nov 2013
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Cite this article as:Jung and Choi:Bounded solutions for the nonlinear wave equation.Boundary Value Problems