Startseite Periodic solutions for second order differential equations with indefinite singularities
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Periodic solutions for second order differential equations with indefinite singularities

  • Shiping Lu EMAIL logo und Xingchen Yu
Veröffentlicht/Copyright: 14. September 2019

Abstract

In this paper, the problem of periodic solutions is studied for second order differential equations with indefinite singularities

x(t)+f(x(t))x(t)+φ(t)xm(t)α(t)xμ(t)+β(t)xy(t)=0,

where fC((0, +∞), ℝ) may have a singularity at the origin, the signs of φ and α are allowed to change, m is a non-negative constant, μ and y are positive constants. The approach is based on a continuation theorem of Manásevich and Mawhin with techniques of a priori estimates.

MSC 2010: 34B16; 34B18; 34C25

1 Introduction

In the past years, the problem of existence of periodic solutions to second order differential equations with definite singularities, either attractive type or repulsive type, was extensively studied by many researchers [1], [2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14]. In [15], Hakl and Torres investigated the problem of periodic solutions to the equation

x(t)=g(t)xμ(t)h(t)xy(t)+r(t), (1.1)

where g, h, r are T–periodic functions with g, h, rL([0, T], ℝ). Chu and et. al in [16] studied the problem of twist periodic solutions to (1.1) for the case of r(t) ≡ 0. We notice that in [15] and [16], the functions of g(t) and h(t) are required to be g(t) ≥ 0 and h(t) ≥ 0 a.e. t ∈ [0, T]. Recently, the periodic problem for second order differential equations with indefinite singularities has attract much attention from researchers (see [12] and [17]-[20]). For example, in [18], the authors considered the existence of positive periodic solutions to the equation like

x(t)=α(t)xμ, (1.2)

where the sign of weight function α(t) can change on [0, T], and μ ≥ 1. The equations like (1.2) with indefinite singularities can be used to model some important problems appearing in many physical contexts (see [21] and the references therein).

In this paper, we consider the problem of periodic solutions to the equation

x(t)+f(x(t))x(t)+φ(t)xm(t)α(t)xμ(t)+β(t)xy(t)=0, (1.3)

where fC((0, +∞), ℝ), φ, α and β are T–periodic and in L([0, T], ℝ), m, μ and y are constants with m ≥ 0 and μy > 0. By using a continuation theorem of Manásevich and Mawhin, some new results on the existence of periodic solutions to (1.3) are obtained. In (1.3), the signs of α(t), β(t) and φ(t) are all allowed to change. This means that the singularity associated to restoring force α(t)xμ+β(t)xy at x = 0 is indefinite type(see [18, 19]). The periodic problem for equation (1.3) has been investigated in recent paper [20]. However, in [20], β(t) ≡ 0, and the functions of α(t) and φ(t) are required to be either α(t) ≥ 0 a.e. t ∈ [0, T], > 0 and φ̄ > 0, or φ(t) ≥ 0 a.e. t ∈ [0, T], > 0 and φ̄ > 0. The significance of present paper relies in the following aspects. Firstly, the coefficient function f(x) associated to friction term f(x)x′ may have a singularity at x = 0. Secondly, compared with the case where the signs of functions φ(t), α(t) and β(t) are in definite, the work of obtaining the estimates of periodic solutions to (1.3) is more difficult. In order to overcome this difficulty, we propose a function F(x) = 1x f(s)ds. By analyzing some properties of F(x) at x = 0 and x = +∞, we investigate the mechanism under which how the singularity associated to f(x) at x = 0 influences the priori estimates of periodic solutions. Moreover, the constant μ in (1.3) is allowed to be in (0, 1). For this case, even if α(t) and β(t) are constant functions, the singular restoring force α(t)xμ+β(t)xy has a weak singularity at x = 0. Finally, by using a theorem in present paper, a new result on the existence of periodic solutions is obtained for Rayleigh-Plesset equation

ρ(RR+32(R)2)=[PvP(t)]+Pg0(R0R)3k2SR4νRR (1.4)

in the case of k ∈ ( 13 , +∞). Equation (1.4) is used in physics of fluids to model the oscillations of the radius R(t) of a spherical bubble immersed in a fluid under the influence of a periodic acoustic field P(see [21]-[25]), and PL([0, T], ℝ). The physical meaning of the rest of the parameters in (1.4) can also be seen in Section 3 of [5]. By using the methods of upper and lower solutions, the authors in [5] obtained the following result:

Theorem 1.1

Suppose that Pv > P and

52ρ(PvP(t))(6k25)[(25)25(5S)6k5(6k5)6k5(5Pg0R03k2ρ)6k25]56k2,fort[0,T]. (1.5)

Then there exists at least one positive Tperiodic solution to the Rayleigh-Plesset equation (1.4) in the case of k ∈ ( 13 , +∞).

2 Preliminaries

Throughout this paper, let CT = {xC(ℝ, ℝ) : x(t + T) = x(t) for all t ∈ ℝ} with the norm defined by |x| = maxt∈[0,T] |x(t)|, and CT1 = {xC1(ℝ, ℝ): x(t + T) = x(t) for all t ∈ ℝ} with the norm defined by ||x||CT1=max{|x|,|x|}. For any T–periodic function y(t) with yL([0, T], ℝ), y+(t) and y(t) is denoted by max{y(t), 0} and –min{y(t), 0}, respectively, and y¯=1T0Ty(s)ds. Clearly, y(t) = y+(t) – y(t) for all t ∈ ℝ, and ȳ = y+y.

Lemma 2.1

([20, 26]). Assume that there exist positive constants M0, M1 and M2 with 0 < M0 < M1, such that the following conditions hold.

  1. For any λ ∈ (0, 1], each possible positive Tperiodic solution x to the equation

    u(t)+λf(u(t))u(t)+λφ(t)um(t)λα(t)xμ(t)+λβ(t)xy(t)=0

    satisfies the inequalities M0 < x(t) < M1 and |x′(t)| < M2, for all t ∈ [0, T].

  2. Each possible solution c to the equation

    α¯cμβ¯cyφ¯cm=0

    satisfies the inequality M0 < c < M1.

  3. The inequality

    (α¯M0μβ¯M0yφ¯M0m)(α¯M1μβ¯M1yφ¯M1m)<0

    holds.

Then, equation (1.3) has at least one Tperiodic solution u such that M0 < u(t) < M1 for all t ∈ [0, T].

Remark 2.1

If φ̄ > 0 and > 0, then we have from the condition of m ≥ 0 and μ > y > 0 that there are two constants D1 and D2 with 0 < D1 < D2 such that

α¯xμβ¯xyφ¯xm>0,forallx(0,D1)

and

α¯xμβ¯xyφ¯xm<0,forallx(D2,).

Lemma 2.2

([5]). Let u ∈ [0, ω] → ℝ be an arbitrary absolutely continuous function with u(0) = u(ω). Then the inequality

(maxt[0,ω]u(t)mint[0,ω]u(t))2ω44ω|u(s)|2ds

holds.

Now, we embed equation (1.3) into the following equations family with a parameter λ ∈ (0, 1]

x+λf(x)x+λφ(t)xmλα(t)xμ=0,λ(0,1]. (2.1)

Let

D={xCT1:x+λf(x)x+λφ(t)xmλα(t)xμ+λβ(t)uy(t)=0,λ(0,1];x(t)>0,t[0,T]}, (2.2)
F+F(x)=1xf(s)ds (2.3)

and

G(x)=1xsμf(s)ds. (2.4)

Lemma 2.3

Assume > 0 and φ̄ > 0, then for each uD, there are constants τ1, τ2 ∈ [0, T] such that

u(τ1)max{1,(α+¯+β¯φ¯)1m+y}:=A0 (2.5)

and

u(τ2)A1, (2.6)

where

A1=min{(α¯2φ+¯)1μ+m,(α¯2β+¯)1μy},β+¯>0(α¯φ+¯)1μ+m,β+¯=0, (2.7)

m, μ and y are determined in equation (1.3)

Proof

Let uD, then

u(t)+λf(u(t))u(t)+λφ(t)um(t)λα(t)uμ(t)+λβ(t)uy(t)=0, (2.8)

which together with the fact of u(t) > 0 for all t ∈ [0, T] gives

uum+λf(u)uum+λφ(t)λα(t)um+μ+λβ(t)uy+m(t)=0.

Integrating the above equality over the interval [0, T], we obtain

0Tuumdt+λ0Tφ(t)dt=λ0Tα(t)um+μdtλ0Tβ(t)uy+m(t)dt,

i.e.,

0Tuumdt+λTφ¯=λ0Tα(t)um+μdtλ0Tβ(t)uy+m(t)dt. (2.9)

Since

0Tuumdt0, (2.10)

it follows from (2.9) that

Tφ¯0Tα(t)um+μdt0Tβ(t)uy+m(t)dt0Tα+(t)um+μ(t)dt+0Tβ(t)uy+m(t)dt. (2.11)

From (2.11), we can conclude that there is a point ξ ∈ [0, T] such that

u(ξ)max{1,(α+¯+β¯φ¯)1m+y}. (2.12)

If (2.12) does not hold, then

u(t)>max{1,(α+¯+β¯φ¯)1m+y}forallt[0,T],

which implies that

u(t)>1forallt[0,T] (2.13)

and

u(t)>(α+¯+β¯φ¯)1m+yforallt[0,T]. (2.14)

From (2.11), (2.13) and μ > y, and by using mean value theorem of integrals, we have that there exists a point η ∈ [0, T] such that

Tφ¯Tα+¯+Tβ¯um+y(η),

i.e.,

u(η)(α+¯+β¯φ¯)1m+y, (2.15)

which contradicts to (2.14). This contradiction verifies (2.12), and so (2.5) holds. Meanwhile, we can assert that (2.6) is true. In fact, multiplying two sides of (2.8) with uμ(t) and integrating it over the interval [0, T], we obtain that

0Tuμ(t)u(t)dtλ0Tφ(s)uμ+mdsλ0Tβ(t)uμy(t)dt+λTα¯=0,

which together with

0Tuμ(t)u(t)dt=0Tuμ1(s)|u(s)|2dt0

yields

Tα¯0Tφ(s)uμ+mds+0Tβ(t)uμy(t)dt0Tφ+(s)uμ+m(s)ds+0Tβ+(t)uμy(t)dt.

Thus, there is a point η ∈ [0, T] such that

u(η)A1,

where A1 is defined by (2.7). This implies that (2.6) holds.□

Lemma 2.4

Assume > 0 and φ̄ > 0, and suppose that the following assumptions

C0:=supx[A1,+)[F(x)+Tφ¯xm]<+, (2.16)

and

lims0+(F(s)Tα¯sμTβ+¯sy)>C0 (2.17)

hold, where F(x) is defined by (2.3).

Then there exists a constant y0 > 0, such that

mint[0,T]u(t)y0,uniformlyforuD.

Proof

For each uD, we have

u(t)+λf(u(t))u(t)+λφ(t)um(t)λα(t)uμ(t)+λβ(t)uy(t)=0,λ(0,1]. (2.18)

Since u(t) is a T–periodic function, there are two points t1, t2 ∈ ℝ such that 0 < t2t1T with u(t1) = maxt∈[0,T] u(t) and u(t2) = mint∈[0,T] u(t). Assumptions of > 0 and φ̄ > 0 implies that (2.6) in Lemma 2.3 holds. This gives

A1u(t1)<+,

to which by applying assumption (2.16) yields

F(u(t1))+Tφ¯um(t1)supA1s<+[F(s)+Tφ¯sm]:=C0<+. (2.19)

By integrating (2.18) over the interval [t1, t2], we get

t1t2f(u(t))u(t)dt=t1t2α(t)uμ(t)dtt1t2β(t)uy(t)dtt1t2φ(t)um(t)dt. (2.20)

It follows from (2.19), (2.20) and the condition φ̄ > 0 that

F(u(t2))=F(u(t1))t1t2φ(t)um(t)dt+t1t2α(t)uμ(t)dtt1t2β(t)uy(t)dtF(u(t1))+0Tφ(t)um(t)dt+0Tα+(t)uμ(t)dt+0Tβ(t)uy(t)dt. (2.21)

On the other hand, by integrating (2.18) on [0, T], we get

0Tα(t)uμ(t)dt=0Tβ(t)uy(t)dt+0Tφ(t)um(t)dt,

i.e.,

0Tα+(t)uμ(t)dt+0Tβ(t)uy(t)dt+0Tφ(t)um(t)dt=0Tα(t)uμ(t)dt+0Tβ+(t)uy(t)dt+0Tφ+(t)um(t)dt.

Substituting it into (2.21), we have from (2.19) that

F(u(t2))F(u(t1))+0Tα(t)uμ(t)dt+0Tβ+(t)uy(t)dt+0Tφ+(t)um(t)dtF(u(t1))+Tφ+¯um(t1)+Tα¯uμ(t2)+Tβ+¯uy(t2)C0+Tα¯uμ(t2)+Tβ+¯uy(t2),

and so

F(u(t2))Tα¯uμ(t2)Tβ+¯uy(t2)C0. (2.22)

Assumption (2.17) ensures that there exists a constant y0 > 0 such that

F(s)Tα¯sμTβ+¯sy>C0,foralls(0,y0). (2.23)

Combining (2.23) with (2.22), we can get

mint[0,T]u(t)=u(t2)y0. (2.24)

Lemma 2.5

Assume > 0 and φ̄ > 0. Suppose further that the following assumptions

B0:=infx[A1,+)[F(x)Tφ+¯xm]> (2.25)

and

lims0+(F(s)+Tα¯sμ+Tβ+¯sy)<B0 (2.26)

hold. Then there exists a constant y1 > 0, such that

mint[0,T]u(t)y1,uniformlyforuD.

Proof

Suppose that uD, then u satisfies (2.18). Let t1 and t2 be defined as same as the ones in the proof of Lemma 2.4. From (2.6) in Lemma 2.3, we see that

A1u(t1)<+,

which together with assumption (2.25), yields that

F(u(t1))Tφ+¯um(t1)infA1s<+[F(s)Tφ+¯sm]:=B0. (2.27)

By integrating (2.18) over the interval [t1, t2], we get

F(u(t2))=F(u(t1))+t1t2α(t)uμ(t)dtt1t2β(t)uy(t)dtt1t2φ(t)um(t)dtF(u(t1))0Tα(t)uμ(t)dt0Tβ+(t)uy(t)dt0Tφ+(t)um(t)dtF(u(t1))Tα¯uμ(t2)Tβ+¯uy(t2)Tφ+¯um(t1),

i.e.,

F(u(t2))+Tα¯uμ(t2)Tβ+¯uy(t2)F(u(t1))Tφ+¯um(t1).

From (2.27), we obtain

F(u(t2))+Tα¯uμ(t2)+Tβ+¯uy(t2)B0. (2.28)

Assumption (2.26) implies that there exists a constant y1 > 0 such that

F(s)+Tα¯sμ+Tβ+¯sy<B0,foralls(0,y1),

which together with (2.28) gives

mint[0,T]u(t)=u(t2)y1.

3 Main Results

Theorem 3.1

Assume φ̄ > 0 and > 0. Suppose further

lims0+(F(s)Tα+¯sμTβ¯sy)=+ (3.1)

and

limx+(F(x)+Tφ+¯xm)=. (3.2)

Then equation(1.3) has at least one positive Tperiodic solution.

Proof

Firstly, we will prove that there exist two constants y2 > 0 and y3 > 0 with y3 > y2, such that

mint[0,T]u(t)y2,uniformlyforuD (3.3)

and

maxt[0,T]u(t)y3,uniformlyforuD. (3.4)

For each uD, u satisfies (2.18). Let t1 and t2 be defined as same as the ones in the proof of Lemma 2.4, that is 0 < t2t1T, u(t1) = maxt∈[0,T] u(t) and u(t2) = mint∈[0,T] u(t). Take t3 = t1 + T, then u(t3) = maxt∈[0,T] u(t) and 0 ≤ t3t2 < T. It is easy to see that (2.16) can be deduced from (3.2), and (3.1) verifies (2.17). By using Lemma 2.4, as well as (2.5) in Lemma 2.3, we know that

A0mint[0,T]u(t)=u(t2)y0. (3.5)

Integrating (2.18) over the interval [t2, t3], we have

F(u(t3))=F(u(t2))+t2t3α(t)uμ(t)dtt2t3β(t)uy(t)dtt2t3φ(t)um(t)dtF(u(t2))0Tα(t)uμ(t)dt0Tβ+(t)uy(t)dt0Tφ+(t)um(t)dtF(u(t2))Tα¯uμ(t2)Tβ+¯uy(t2)Tφ+¯um(t3),

i.e.,

F(u(t3))+Tφ+¯um(t3)F(u(t2))Tα¯uμ(t2)Tβ+¯uy(t2),

which together with (3.5) gives

F(u(t3))+Tφ+¯um(t3)infx[y0,A0][F(x)Tα¯xμTβ+¯xy]:=ρ0>.

It follows from (3.2) that there is a constant y3 > 0 such that

maxt[0,T]u(t)=u(t3)y3. (3.6)

From (3.5) and (3.6), we see that the conclusions of (3.3) and (3.4) hold. Next, we will show that there exists a positive constant ρ1 such that

maxt[0,T]|u(t)|ρ,uniformlyforuD. (3.7)

In fact, if uD, then

u(t)+λf(u(t))u(t)+λφ(t)um(t)λα(t)uμ(t)+λβ(t)uy(t)=0,λ(0,1]. (3.8)

Let u attain its maximum over [0, T] at t1 ∈ [0, T], then u′(t1) = 0 and we deduce from (3.8) that

u(t)=λt1t[f(u(s))u(s)φ(s)um(s)+α(s)uμ(s)β(s)uy(s)]ds

for all t ∈ [t1, t1 + T]. Thus,

|u(t)|λ|F(u(t))F(u(t1))|+λt1t1+T|α(s)uμ(s)|ds+λt1t1+T|β(s)uy(s)|ds+t1t1+T|φ(s)|um(s)ds2maxy2uy3|F(u)|+0T|α(t)uμ(t)|dt+0T|β(t)uy(t)|dt+0T|φ(s)|um(s)ds.

It follows from (3.4) and (3.3) that

|u(t)|2maxy0uy3|F(u)|+T|α|¯y1μ+T|β|¯y1y+Ty3m|φ|¯:=ρ,forallt[0,T],

and so

maxt[0,T]|u(t)|ρ,uniformlyforuD,

which implies that (3.7) holds. Let m0 = min{D1, y2} and m1 = max{y3, D2} be two constants, where D1 and D2 are constants determined in Remark 2.1, then from (3.4), (3.3) and (3.7), we see that each possible positive T–periodic solution u to equation(2.1) satisfies

m0<u(t)<m1,|u(t)|<ρ1forallt[0,T]

This implies that condition 1 of Lemma 2.1 is satisfied. Also, we can deduce from Remark 2.1 that

α¯xμβ¯xyφ¯xm>0,forx(0,m0]

and

α¯xμβ¯xyφ¯xm<0,forx[m1,+),

which gives that condition 2 of Lemma 2.1 holds. Furthermore, we have

α¯m0μβ¯m0yφ¯m0mα¯m1μβ¯m1yφ¯m1m<0.

So condition 3 of Lemma 2.1 holds, too. By using Lemma 2.1, we see that equation(1.3) has at least one positive T–periodic solution.□

Theorem 3.2

Assume φ̄ > 0 and > 0. Suppose further

lims0+(F(s)+Tα+¯sμ+Tβ¯sy)= (3.9)

and

limx+(F(x)Tφ+¯xm)=+. (3.10)

Then equation(1.3) has at leat one positive Tperiodic solution.

Proof

From the proof of Theorem 3.1, we see that it suffices for us to verify (3.4) and (3.3). In order to do it, let uD, u satisfies (2.18). Let t2 and t3 be defined as same as the ones in the proof of Theorem 3.1, that is 0 ≤ t3t2 < T, u(t3) = maxt∈[0,T] u(t) and u(t2) = mint∈[0,T] u(t). It is easy to see that (2.25) can be deduced from (3.10), and (3.9) verifies (2.26). By using Lemma 2.5 and (2.5) in Lemma 2.4, we know that

A0mint[0,T]u(t)=u(t2)y1. (3.11)

Integrating (2.18) over the interval [t2, t3], we have

F(u(t3))=F(u(t2))+t2t3α(t)uμ(t)dtt2t3β(t)uy(t)dtt2t3φ(t)um(t)dtF(u(t2))+0Tα+(t)uμ(t)dt+0Tβ(t)uy(t)dt+0Tφ(t)um(t)dtF(u(t2))+Tα+¯uμ(t2)+Tβ¯uy(t2)+Tφ¯um(t3),

i.e.,

F(u(t3))Tφ¯um(t3)F(u(t2))+Tα+¯uμ(t2)+Tβ¯uy(t2), (3.12)

which together with (3.11) and gives

F(u(t3))Tφ¯um(t3)supx[y0,A0][F(x)+Tα+¯xμ+Tβ¯xy]:=C0<+.

It follows from (3.10) and the condition φ̄ > 0 that there is a constant ρ2 > 0 such that

maxt[0,T]u(t)=u(t3)ρ2. (3.13)

From (3.11) and (3.13), we see that the conclusions of (3.3) and (3.4) hold.□

Theorem 3.3

Assume φ̄ > 0, > 0 and

limx+[G(x)Tβ+¯xμyTφ+¯xμ+m]=+. (3.14)

If

limx0+G(x)<C0Tα¯, (3.15)

then equation(1.3) has at least one positive Tperiodic solution, where G(x) is defined by (2.4) and

C0:=infx[A1,+)[G(x)Tβ+¯xμyTφ+¯xμ+m]. (3.16)

.

Remark 3.1

Assumption (3.14) implies that C0 ∈ (–∞, +∞) is a constant.

Proof

Similar to the proof of Theorem 3.2, we need only prove the estimates of (3.4) and (3.3). Let uD, then u satisfies (2.18). Let t1 and t2 be as same as the ones in the proof of Lemma 2.4. Multiplying (2.18) with uμ(t) and integrating it on [t4, t2], we get

t1t2u(t)uμ(t)dt+λt1t2uμ(t)f(u(t))u(t)dt=λt4t2α(t)dtλt4t2φ(t)um+μ(t)dtλt4t2β(t)uμy(t)dt. (3.17)

Since t1t2u(t)uμ(t)dt0, it follows from (3.17) and (3.16) that

G(u(t2))G(u(t1))+t1t2α(t)dtt1t2φ+(t)um+μ(t)dtt1t2β+(t)uμy(t)dtG(u(t1))Tα¯Tφ+¯um+μ(t1)Tβ+¯uμy(t1). (3.18)

By using (2.6) and (3.16), we get

G(u(t2))infx[A1,+)[G(x)Tφ+¯xm+μTβ+¯xμy]Tα¯=C0Tα¯,

which together with (3.15) verifies (3.4). Thus, according to (2.5), we arrive at

y2u(t2)A0. (3.19)

On the other hand, by (3.18) again, we obtain from (3.19) that

G(u(t1))Tφ+¯um+μ(t1)Tβ+¯uμy(t1)G(u(t2))+Tα¯maxy2xA0G(x)+Tα¯. (3.20)

By assumption (3.14), we see that there is a constant y3 > y2 such that

G(s)Tφ+¯sm+μTβ+¯sμy>maxy2xA0G(x)+Tα¯,foralls(y3,+). (3.21)

Therefore, (3.20) and (3.21) imply

maxt[0,T]u(t)=u(t4)y3. (3.22)

From (3.19) and (3.22), we see that the (3.4 and (3.3) hold.□

Theorem 3.4

Assume φ̄ > 0, > 0 and

limx+[G(x)+Tβ+¯xμy+Tφ+¯xμ+m]=. (3.23)

If

limx0+G(x)>C1+Tα¯, (3.24)

then equation(1.3) has at least one positive Tperiodic solution, where

C1:=supx[A1,+)[G(x)+Tβ+¯xμy+Tφ+¯xμ+m]. (3.25)

Remark 3.2

From assumption (3.23), one can find that C1 ∈ (–∞, +∞) is a constant.

Proof

Let uD. If set t4 = t2T, then 0 < t1t4T and u(t4) = mint∈[0,T] u(t). Multiplying (2.18) with uμ(t) and integrating it on [t4, t1], we get

t4t1u(t)uμ(t)dt+λt4t1uμ(t)f(u(t))u(t)dt=λt4t1α(t)dtλt4t1φ(t)um+μ(t)dtλt4t1β(t)uμy(t)dt. (3.26)

By using t4t1u(t)uμ(t)dt0, it follows from (3.26) that

G(u(t1))G(u(t4))+t4t1α(t)dtt4t1φ+(t)um+μ(t)dtt4t1β+(t)uμy(t)dtG(u(t4))Tα¯Tφ+¯um+μ(t1)Tβ+¯uμy(t1), (3.27)

which together with (3.25) gives

G(u(t4))G(u(t1))+Tφ+¯um+μ(t1)+Tβ+¯uμy(t1)+Tα¯supx[A1,+)[G(x)+Tβ+¯xμy+Tφ+¯xμ+m]+Tα¯C1+Tα¯.

In view of (3.24), we get that there is a constant y4 > 0 such that

mint[0,T]u(t)>y4.

This together with (2.5) yields

y4u(t4)A0.

It follows from (3.27) that

G(u(t1))+Tφ+¯um+μ(t1)+Tβ+¯uμy(t1)+Tα¯G(u(t4))Tα¯miny4xA0G(x)Tα¯,

to which by applying (3.23), we get that there is a constant y5 > y4 such that

maxt[0,T]u(t)=u(t1)<y5.

Example 3.1

Consider the following equation

x(t)(xm+1x2)x(t)+(1+2sint)xm(t)12costx23(t)+sintx12(t)=0, (3.28)

where m ∈ [0, +∞) is a constant.

Corresponding to (1.3), we have f(x)=xm1x2,μ=23,y=12, φ(t) = 1 + 2 sin t, α(t) = 1 – 2 cos t, β(t) = sin t and T = 2π. Clearly, = 1 > 0 and φ̄ = 1 > 0. Since A1=(α¯φ¯)1m+μ=1 and

F(x)=1xf(s)ds=xm+1m+1+1xmm+1,

we have

limx+(F(x)+Tφ+¯xm)=. (3.29)

Furthermore, from α+¯=5π32 and μ = 23 < 1, we have

lims0+(F(s)Tα+¯sμTβ¯sy)=+, (3.30)

Thus, by using Theorem 3.1, we have that equation(3.28) has at least one positive 2π-periodic solution.

Now, we study the existence of periodic solutions to equation (1.4). By using the change of variable R = x25 , from [5], we see that equation (1.4) changes to

x+4νx45x+5[P(t)Pv]2ρx15+5Sx15(5Pg0R03k2ρ)1x6k15=0, (3.31)

where the parameters of S, ρ, ν, Pg0 and R0 are positive constants, k ∈ ( 13 , +∞). Corresponding to (1.3), we have f(x)=4νx45,φ(t)=5[P(t)Pv]2ρ,α(t)5Pg0R03k2ρ,β(t)5S,μ=6k15andy=m=15. Thus,

G(x)=1xsμf(s)ds=4ν1xs6k1545ds=10ν3kx6k510ν3k,

and from (2.7), we see

A1=min{(α¯2φ+¯)1μ+m,(α¯2β+¯)1μy}=min{(Pg0R03k2[P(t)Pv]+¯)1μ+m,(Pg0R03k2S)1μy}. (3.32)

If 10ν3k>5T2ρ[P(t)Pv]+¯, then

G(x)Tβ+¯xμyTφ+¯xμ+m=(10ν3k5T2ρ[P(t)Pv]+¯)x6k55TSx6k2510ν3k,

and so assumption (3.14) holds. Let

H(x)=(10ν3k5T2ρ[P(t)Pv]+¯)x6k55TSx6k25.

Clearly, if A1>(5TSσ1)52, then

C0:=infx[A1,+)[G(x)2Tβ+¯xμy2Tφ+¯xμ+m]=infx[A1,+)H(x)10ν3k=H(A1)10ν3k>10ν3k, (3.33)

where

σ1=10ν3k5T2ρ[P(t)Pv]+¯. (3.34)

Furthermore,

limx0+G(x)=10ν3k,

which together with (3.33) yields

limx0+G(x)<C0Tα¯.

This implies that assumption (3.15) holds. Thus, By using Theorem 3.3, we obtain the following result.

Theorem 3.5

Assume k ∈ ( 13 , +∞), P > Pv. If 10ν3k>5T2ρ[P(t)Pv]+¯, and

A1>(5TSσ1)52,

then (3.31) has at least one positive Tperiodic solution, where σ1 and A1 is defined by (3.34) and (3.32), respectively.

Remark 3.2

Since the condition P > Pv in Theorem 3.5 is essentially different from the corresponding one of P < Pv in Theorem 1.1, Theorem 1.4 can be regarded as a new result on the existence of periodic solutions to Rayleigh-Plesset equation (1.4).

Acknowledgement

This work was sponsored by NSF of China (No. 11271197).

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Received: 2019-02-04
Accepted: 2019-05-16
Published Online: 2019-09-14

© 2020 Shiping Lu and Xingchen Yu, published by De Gruyter

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

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