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R E S E A R C H

Open Access

On positive periodic solutions of second

order singular equations

Yunhai Wang

1

and Yuanfang Ru

2*

*Correspondence: [email protected] 2College of Science, China pharmaceutical University, Nanjing, P.R. China

Full list of author information is available at the end of the article

Abstract

Using the fixed point theorem, we study the existence and multiplicity of positive periodic solutions for the second order differential equations

¨

x+a(t)x=f(x),

x(0) =x(T), x(0) =˙ x(T).˙

For given nonnegative constants 0 <

β

1<

β

2<· · ·<

β

N, the functionfmay be

singular atx=

β

i.

Keywords: Periodic solutions; Second order differential equations; Singular; Fixed point theorem

1 Introduction

We say that the differential equation

¨

x+a(t)x=λf(t,x) +e(t) (1.1)

is singular if the nonlinear termf is singular, which means that a vector-valued function f is only defined onR×RN\withRN being nonempty and for anyx

0∈,

lim

xx0

f(t,x) = +∞, uniformly int∈R.

During the last two decades, the existence of nontrivial periodic solutions of (1.1) has been studied by many researchers in nonsingular case as well as singular case. Usually, the proof is based on either the method of upper and lower solutions [2,10,15], fixed point theorems [6,7,17–19], alternative principle of Leray–Schauder [4,11], or topological degree theory [23,24]. To our attention, Wang in [22] studied the existence, multiplicity, and nonexis-tence results for positive solutions of the singular periodic boundary value problem (1.1) in terms of different values ofλ∈R. But most of these papers are concerned with singu-larity atx=x0. Later, a similar idea is used to study the singular periodic systems with two

parameters,

⎧ ⎨ ⎩ ¨

u+a1(t)u=λb1(t)f1(u,v),

¨

v+a2(t)v=μb2(t)f2(u,v),

(1.2)

(2)

where (λ,μ)∈R2

+\ {0, 0}. One nice result proved in [20] is that there exist three nonempty

subsets ofR2

+\ {0, 0}:,1,2such thatR+2\ {0, 0}=1∪2and (1.2) has at least

two positive periodic solutions for (λ,μ)∈1, one positive periodic solution for (λ,μ)∈

, and no positive periodic solutions for (λ,μ)∈2. Note that in this paper the word

“singularity” is understood in a more general way because we only need thatf1is singular

at the whole linex-axis andf2is singular at the whole liney-axis. The proof is based on

the following vector version of Krasnosel’skii’s fixed point theorem [14]. In addition, there are many papers concerned with the existence and multiplicity of radial solutions of the elliptic equations with the regular or singular nonlinearities. We refer the readers to [1,3,

5,8,12,13,16,21].

Motivated by these recent developments, in this paper, we investigate the existence and multiplicity ofT-periodic solutions of the following problem:

⎧ ⎨ ⎩ ¨

x+a(t)x=f(x),

x(0) =x(T), x˙(0) =x˙(T), (1.3)

where the functionf may be singular atx=βi(i= 1, . . . ,N). For convenience, we give the

following notations:

a∗= min

t∈[0,T]a(t), a

= max

t∈[0,T]a(t),

f∗(r) =maxf(x) :θrxr, wherer> 0,θ∈(0, 1).

Forν= 0 orν= +∞, there exist nonnegative constantsdefined as

=lim xν

f(x) x .

The main results can be expressed as follows.

Theorem 1.1 Assume that the function f satisfies the following conditions:

(A) f may be singular atx=βi(i= 1, . . . ,N)and continuous on

(0,β1, ), (β1,β2), . . . , (βN–1,βN), (βN, +∞);

(B) For any interval(βi,βi+1),i= 1, . . . ,N– 1,

(i) f(x) –aβi≥0, forx∈(βi,βi+1),

(ii) there existsR¯i∈(βi,βi+1)such that

max

x∈[θR¯i+(1–θ)βi,R¯i]

f(x) <R¯iβi MT +a∗βi.

Then(1.3)has at least(2N– 2)positive periodic solutions.

(3)

(C) There existsR¯>βN such that

(i) f(x) –aβN≥0, forx∈(βN,R¯),

(ii) max

x∈[θR¯+(1–θ)βN,R¯]

f(x) <R¯–βN MT +aβn.

Then(1.3)has at least(2N– 1)positive periodic solutions.

Theorem 1.3 Assume that(A)and(B)hold.In addition,the function f satisfies the fol-lowing condition:

(D) There existsr¯∈(0,β1)such thatf∗(r¯) <MTr¯ .

Then(1.3)has at least(2N– 1)positive periodic solutions.

Corollary 1.4 Assume that(A)and(B)hold.If f0= 0, then(1.3)has at least(2N– 1)

positive periodic solutions.

Theorem 1.5 Assume that(A), (B),and(D)hold.If f0= +,then(1.3)has at least(2N)

positive periodic solutions.

Theorem 1.6 Assume that(A), (B), (C),and(D)hold.Then(1.3)has at least(2N)positive periodic solutions.

Theorem 1.7 Assume that(A)and(B)hold.In addition,the function f satisfies the fol-lowing condition:

(E) There existsRˆ>βN

θ such that

(i) f(x) –aβN≥0, forx∈(βN,Rˆ),

(ii) max

x∈[θRˆ,Rˆ]

f(x) < R¯

MT +min

a∗– 1

MT, 0 βN.

If f∞= +∞,then(1.3)has at least(2N)positive periodic solutions.

Theorem 1.8 Assume that(A), (B), (C),and(D)hold.If f0= +,then(1.3)has at least

(2N+ 1)positive periodic solutions.

Theorem 1.9 Assume that(A), (B), (D),and(E)hold.If f∞= +∞,then(1.3)has at least (2N+ 1)positive periodic solutions.

Theorem 1.10 Assume that (A), (B), (D),and(E)hold.If f0= +∞and f∞= +∞,then (1.3)has at least(2N+ 2)positive periodic solutions.

2 Preliminary

The functionasatisfies the following assumption:

(H) The functionais continuous, positive,T-periodic and the linear equation

¨

x+a(t)x= 0has a positive Green’s functionG(t,s), i.e.,

G(t,s) > 0 for all(t,s)∈[0,T]×[0,T],

m= min

(4)

From (H), it is clear that a functionx(t) is aT-periodic solution of (1.3) if and only if

x(t) =

T

0

G(t,s)fx(s)ds.

Define the operatorA:KEby

Ax(t) =

T

0

G(t,s)fx(s)ds, 0≤tT.

LetEdenote the Banach spaceC[0,T] with the usual max-norm and define a subconeK by

K=x(t)∈C[0,T] :x(t)≥θx.

Forr> 0, let

Kr:=

x(t)∈K:x(t)<r,

∂Kr:=

x(t)∈K:x(t)=r.

Therefore, the solution of (1.3) is equivalent to the fixed point of the operatorA. The discussion is based on the following well-known fixed point theorem.

Lemma 2.1([9, Theorem 2.3.4]) Let E be a Banach space and KE be a cone in E.

Assume that1,2are open subsets of E with0∈1,1⊂2,and let T:K∩(2\1)→

K be a completely continuous operator such that either

(i) Tuu,uK1andTuu,uK2;or

(ii) Tuu,uK1andTuu,uK2.

Then T has a fixed point in K∩(2\1).

3 Proof of the main results

First, we consider the existence of solutions of (1.3) on (0,β1) .

Lemma 3.1 Assume that(H), (A),and(D)hold.Then(1.3)has at least one positive

peri-odic solution.

Proof Sincef(·) is singular atx=β1–, there exists sufficiently smallδ< (1 –θ)β1such that

f(x)≥ρx, for 0 <|xβ1|<δ1, whereρ satisfies ρm|2|θ ≥1,2 is given as follows.

ChooseR∈(β1–δ,β1). Then, forx∂KR, one hasx(t)≥θxθR. IfθRβ1–δ, then

β1δ

θRβ1. Further, we haveδ> (1 –θ)β1, which yields a contradiction. Now we only

consider the caseθR<β1–δ. Let [0,T] =1∪2, where

1=

t∈[0,T] :θRx(t) <β1–δ

,

2=

t∈[0,T] :β1–δx(t)≤R

(5)

Sincex=Randxis continuous,2is nonempty and|2|> 0. Therefore, we have

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)ds

m

1

fx(s)ds+

2

fx(s)ds

m

2

fx(s)dsρm|2|θxx.

For anyx∂Kr¯, we have

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)ds

T

0

G(t,s) r¯

MT ds<x.

From [22], it is clear thatA:KR\K¯rK, andAis completely continuous onKR\K¯r.

Therefore, by Lemma2.1, (1.3) has at least a positive solutionx(t)∈KR\K¯r.

Lemma 3.2 Assume that(H)and(A)hold.If f0= 0,then(1.3)has at least one positive

periodic solution.

Proof Sincef0= 0, there exists sufficiently small¯r> 0 such thatf(x)xforx[0,¯r],

whereMT< 1. Then, for anyx∂K¯r, we have

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)dsMTx<x.

The remainder is similar to the proof of Lemma3.1, so we omit it.

Lemma 3.3 Assume that(H), (A),and(D)hold.If f0= +,then(1.3)has at least two

positive periodic solutions.

Remark f0= +implies thatf may be singular atx= 0.

Proof Sincef(·) is singular atx=β1–, from the proof of Lemma3.1, there existsR∈(β1–

δ,β1) >¯rsuch thatAx>xforx∂KR

Sincef0= +, there exists sufficiently smallr<r¯such thatf(x)xforx[0,r], where

mθT> 1. Then, for anyx∂Kr, we have

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)dsmθTx<x.

For anyx∂Kr¯, we have

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)dsMTx<x.

(6)

Therefore, by Lemma2.1, (1.3) has at least two positive solutions x1(t)∈KR\K¯r and

x2(t)∈K¯r\Kr.

Second, we give some existence results of solutions of (1.3) on (βN, +∞).

Lemma 3.4 Assume that(H), (A),and(C)hold.Then(1.3)has at least one positive peri-odic solution.

Remark Sincef(·) is singular atx=βN+, there exists sufficiently smallδ< 1–θ

θ such that

f(x)≥ρxfor 0 <xβN <δ. Chooser∈(βN,βN +δ). Then, forx∂Kr, one hasx(t)≥

θxθr. Ifθrβn, thenβθNrβN+δ, which yields a contradiction. Thereforeθr<

βN, which implies thatAis not continuous onKR\Kr, whereR>βθN.

Proof Letω=uβN. Then (1.3) is equivalent to the problem ⎧

⎨ ⎩ ¨

ω+a(t)ω=f(ω+βN) –a(t)βN=F(ω),

ω(0) =ω(T), ω˙(0) =ω˙(T). (3.1)

From (A) and (C), it follows that (a1) limω→0+F(ω) = +∞;

(a2) letr=R¯–βN,F(ω)≥0, forω∈(0,r);

(a3) there exists sufficiently smallr<rsuch that

F(ω) >, forω∈(0,r),

whereLmT> 1.

Define the operatorA:KEby

Tx(t) =

T

0

G(t,s)(s) +βN

a(t)βN

ds, 0≤tT.

Then, for anyω∂Kr, from (ii) of (C), we have

max

ω∈[θr,r]

(s) +βN

a(t)βN

≤ max

ω∈[θr,r]

(s) +βN

aβN

= max

x∈[θR¯+(1–θ)βN,R¯]

f(x) –aβN<

r MT.

Further, we have

= max

t∈[0,T](t) =tmax∈[0,T]

T

0

G(t,s)(s) +βN

a(t)βN

ds

MT max

ω∈[θr,r]

(s) +βN

a(t)βN

<r=ω.

Forω∂K¯r, we have

=max

t∈[0,T](t) =tmax∈[0,T]

T

0

G(t,s)(s) +βN

a(t)βN

ds

(7)

From (f5) and the Arzela–Ascoli theorem it follows thatT is completely continuous on

Kr\K¯r. Therefore, by Lemma2.1, (3.1) has at least a positive solutionω(t)∈Kr\Kr¯. Namely,

(1.3) has at least a positive solutionx(t) =ω(t) +βN satisfyingx(t)<βN+r=R¯.

Corollary 3.5 Assume that(H)and(A)hold.In addition,

(f1) f(·)is continuous on(βN, +∞)andf(x)≥aβN on(βN, +∞).

If f∞= 0,then(1.3)has at least one positive periodic solution.

Proof If (f1) holds, thenF(ω)≥and (i) of (C) hold. From (f1) andf∞= 0 it follows that

limω→+∞F(ωω)= 0. Then there exists sufficiently largeR> 0 such thatF(ω)≤ωforωR,

whereMT< 1. Choose˜r>max{Rθr}, where¯ris given in (a3). Then, for anyω∂K˜r, one

hasω(t)≥θω>R, and further we have

= max

t∈[0,T]

T

0

G(t,s)(s)dsMTω<ω.

Combining Lemma3.4and Lemma2.1, we have that (1.3) has at least one positive

pe-riodic solution.

Lemma 3.6 Assume that(H), (A),and(E)hold.If f∞= +∞,then(1.3)has at least two

positive periodic solutions.

Proof It is easy to see that (E) implies (C). Then, from Lemma3.3, we can obtain a solution x1(t) satisfyingx1(t)<R¯.

For anyx(t)∈∂KRˆ, we get

Ax= max

t∈[0,T]Ax(t) =tmax∈[0,T]

T

0

G(t,s)fx(s)ds

MT max

x∈[θRˆ,Rˆ]

fx(s)<Rˆ=x.

By the definition off∞=∞, there existsR>Rˆ such thatf(x)≥μxforxR, whereμ satisfiesμmTθ> 1.

ChooseR=Rθ. Then, forx∂KR, one hasx(t)≥θxR, and

Ax= max

t∈[0,T]

T

0

G(t,s)fx(s)ds

μmTθx>x.

From (A) and the Arzela–Ascoli theorem it follows thatAis completely continuous on KR\KRˆ. Therefore, by Lemma2.1, (1.3) has another positive solutionx2(t)∈KR\KRˆ.

Finally, we are studying the existence of solutions of (1.3) on (βi,βi+1),i= 1, 2 . . . ,N– 1.

Lemma 3.7 Assume that(H), (A),and(B)hold.Then(1.3)has at least two positive

(8)

Proof Letω=uβi. Then (1.3) is equivalent to the problem ⎧

⎨ ⎩ ¨

ω+a(t)ω=f(ω+βi) –a(t)βi=Fi(ω),

ω(0) =ω(T), ω˙(0) =ω˙(T). (3.2)

From (A) and (B), it follows that

(F1) Fi(·)is nonnegative and continuous on(0,βi+1–βi);

(F2) Fi(·)is singular atx= 0+,(βi+1–βi)–;

(F3) Letr¯i=R˜iβi∈(0,βi+1–βi)such thatFi∗(r¯i) <MTr¯i .

Then from Lemma3.3it follows that (1.3) has at least two positive periodic solutions.

Now we give the proof of the main results.

Proof of Theorem1.1 The number of the interval (βi,βi+1) isN– 1, then we can obtain the

result from Lemma3.7.

Proof of Theorem1.2 From Lemmas3.4and3.7the result follows.

Proof of Theorem1.3 From Lemmas3.1and3.7the result follows.

Proof of Corollary1.4 From Lemmas3.2and3.7the result follows.

Proof of Theorem1.5 From Lemmas3.3and3.7the result follows.

Proof of Theorem1.6 From Lemmas3.1,3.4, and3.7the result follows.

Proof of Theorem1.7 . From Lemmas3.6and3.7the result follows.

Proof of Theorem1.8 From Lemmas3.3,3.4, and3.7the result follows.

Proof of Theorem1.9 From Lemmas3.1,3.6, and3.7the result follows.

Proof of Theorem1.10 From Lemmas3.3,3.6, and3.7the result follows.

Now we just give an example to illustrate Theorem1.10.

Example For convenience, we consider the following periodic boundary value problem:

⎧ ⎨ ⎩ ¨

x+μx=f(x),

x(0) =x(T), x˙(0) =x˙(T),

(3.3)

wherea(t) =μis a constant such that (H) holds, andf(x) is expressed by

f(x) =

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

C0101+(x021)ν02, x∈(0,β1); C11

(xβ1)ν11 + C12

(xβ2)ν12 +β1μ, x∈(β1,β2);

C21

(xβ2)ν21 + C22

(xβ3)ν22 +β2μ, x∈(β2,β3); C31

(9)

where

(I) Cijare positive constants; (i= 0, 1, 2, 3,j= 1, 2);

(II) a∗=a∗=μ;

(III) ν01< 1,ν11,ν21,ν31> 0,ν32> 1,ν02,ν12,ν22are even.

It is obvious that (A) holds. First we show that assumption (B) holds.

(i) f(x) –aβi≥0 obviously holds forx∈(βi,βi+1),

(ii) max

x∈[θR¯i+(1–θ)βi,R¯i]

f(x) <R¯iβi MT +aβi

max

x∈[θR¯i+(1–θ)βi,R¯i]

Ci1

(xβi)νi1

+ Ci2 (xβi+1)νi2

<R¯iβi

MT .

IfCij(i= 1, 2,j= 1, 2) is sufficiently small, there existsR˜i∈(βi,βi+1) such that the above

inequality holds.

Second, ifC0j(j= 1, 2) is sufficiently small, there exists¯r∈(0,β1) such thatf∗(r¯) <MTr¯ ,

namely (D) holds.

Third, it is clear thatf(x) –aβN ≥0 forx∈(βN,Rˆ). In addition, ifC3j(j= 1, 2) is

suffi-ciently small, there existsRˆ>βN

θ such that

max

x∈[θRˆ,Rˆ]

f(x) < R¯

MT +min

a∗– 1

MT, 0 βN,

namely (E) holds.

Finally, we can verify that

f0=lim

x→0

f(x) x =xlim→0

C0101+(xCβ102)ν02

x = +∞,

f∞= lim

x→∞ f(x)

x =xlim→∞

C31

(xβ3)ν31+C3232+β3μ

x = +∞.

Therefore, by Theorem1.10, (3.3) has at least (2N+ 2) positive periodic solutions.

4 Conclusion

Some sufficient conditions are given to illustrate the existence and multiplicity of positive periodic solutions for the second order differential equations

⎧ ⎨ ⎩ ¨

x+a(t)x=f(x),

x(0) =x(T), x˙(0) =x˙(T).

For given nonnegative constants 0 <β1<β2<· · ·<βN, the functionf may be singular at

x=βi.

Acknowledgements

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Funding

The authors were supported by NNSF of China (No.11501165), the projects of Guizhou Provincial Science and Technology Fund (QKH-JICHU [2017], Grant no. 1408, QKH-LH [2014], Grant no. 7366).

Availability of data and materials

Not applicable.

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

All the authors contributed equally and significantly in writing this article. All the authors read and approved the final manuscript.

Author details

1School of Mechanical Engineering, Guizhou Institute of Technology, Guiyang, P.R. China.2College of Science, China pharmaceutical University, Nanjing, P.R. China.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 3 April 2018 Accepted: 11 July 2018

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