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Positive solutions to a semipositone superlinear elastic beam equation

  • A semipositone fourth-order two-point boundary value problem is considered. In mechanics, the problem describes the deflection of an elastic beam rigidly fastened on the left and simply supported on the right. Under some conditions concerning the first eigenvalue corresponding to the relevant linear operator, the existence of nontrivial solutions and positive solutions to this boundary value problem is obtained. The main results are obtained by using the topological method and the fixed point theory of superlinear operators.

    Citation: Haixia Lu, Li Sun. Positive solutions to a semipositone superlinear elastic beam equation[J]. AIMS Mathematics, 2021, 6(5): 4227-4237. doi: 10.3934/math.2021250

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  • A semipositone fourth-order two-point boundary value problem is considered. In mechanics, the problem describes the deflection of an elastic beam rigidly fastened on the left and simply supported on the right. Under some conditions concerning the first eigenvalue corresponding to the relevant linear operator, the existence of nontrivial solutions and positive solutions to this boundary value problem is obtained. The main results are obtained by using the topological method and the fixed point theory of superlinear operators.



    The purpose of this paper is to investigate the existence of nontrivial solutions and positive solutions to the following nonlinear fourth-order two-point boundary value problem

    {u(4)(t)=λf(t,u(t)), 0t1,u(0)=u(0)=u(1)=u(1)=0,        (P)

    where λ is a positive parameter, f:[0,1]×RR is continuous. One function uC[0,1] is called a positive solution of problem (P) if u is a solution of (P) and u(t)>0,0<t<1.

    Fourth-order two-point boundary value problems appear in beam analysis (See [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15]). The deflection of an elastic beam rigidly fastened on the left and simply supported on the right leads to problem (P). The existence and multiplicity of positive solutions for the elastic beam equations have been studied extensively when the nonlinear term satisfies

    f(t,u)0, u0, (1)

    see for example [1,2,3,6,7,8,9,11] and references therein. Agarwal and Chow [1] investigated the problem (P) by using contraction mapping and iterative methods. Bai [3] applied upper and lower solution method and Yao [11] used Guo-Krasnosel'skii fixed point theorem of cone expansion-compression type. However there are only a few papers concerned with the non-positone or semipositone elastic beam equations. Yao [12] considered the existence of positive solutions of semipositone elastic beam equations by using a special cone and the fixed point theorem of cone expansion-compression type. In this paper, we assume that there exists a constant b>0 such that f(t,u)b for all t[0,1] and u(t)R, which implies that problem (P) is semipositone. We obtain the existence of nontrivial solutions and positive solutions to the semipositone boundary value problem (P) under some conditions concerning the first eigenvalue corresponding to the relevant linear operator by the topological method and the fixed point theory of superlinear operators.

    In this section, we give some preliminaries required in our subsequent discussions.

    Let E be an ordered Banach space in which the partial ordering is induced by a cone PE, θ the zero element of E. For the concepts and properties about the cone we refer to [16,17,18].

    Lemma 1. (see [19]). Let ΩE be a bounded open set, θΩ, and A:¯ΩE a completely continuous operator. If

    Axμx, xΩ,μ1,

    then deg (IA,Ω,θ)=1.

    Lemma 2. (see [19]). Let ΩE be a bounded open set and A:¯ΩE a completely continuous operator. If there exists u0E{θ} such that

    uAuμu0, uΩ,μ0,

    then deg(IA,Ω,θ)=0.

    The following is the famous Leray-Schauder theorem.

    Lemma 3. (see [18]). Let ΩE be a bounded open set, θΩ and A:¯ΩE a completely continuous operator with Aθ=θ. Suppose that the Frechet derivative Aθ of A at θ exists and 1 is not an eigenvalue of Aθ. Then there exists r0>0 such that for any 0<r<r0,

    deg(IA,Tr,θ)=deg(IAθ,Tr,θ)=(1)κ,

    where κ is the sum of algebraic multiplicities for all eigenvalues of Aθ lying in the interval (0, 1) and Tr={xEx<r}.

    Let G(t,s) be the Green's function of homogeneous linear problem u(4)(t)=0,u(0)=u(0)=u(1)=u(1)=0, which can be explicitly given by

    G(t,s)={112(1t)s2[3(1s)(1t)2(3s)],  0st1,112(1s)t2[3(1t)(1s)2(3t)],  0ts1. (2)

    By (2) and Yao [13] we have

    (G1) G(t,s)=G(s,t), 0t,s1;

    (G2) 16s2(1s)t2(1t)G(t,s)14t2(1t), 0t,s1;

    By (G1)(G2),

    G(t,s)16s2(1s)t2(1t)14s2(1s)23t2(1t)14s2(1s)34t3(1t)234t3(1t)2G(s,τ)=34t3(1t)2G(τ,s),

    and we have

    (G3) G(t,s)34t3(1t)2G(τ,s), 0t,s,τ1.

    It is well known that the problem (P) is equivalent to the integral equation

    u(t)=λ10G(t,s)f(s,u(s))ds.

    Let

    (Au)(t)=10G(t,s)f(s,u(s))ds, (3)
    (Bu)(t)=10G(t,s)u(s)ds. (4)

    By the famous Krein-Rutmann theorem (See [16]) and similar to Lemma 3 in [20], we have

    Lemma 4. Suppose that the linear operator B is defined by (4). Then the spectral radius r(B)0 and B has a positive eigenfunction corresponding to its first eigenvalue λ1=r1(B).

    In the sequel we always take E=C[0,1] with the norm u=max0t1|u(t)| and the cone P={uC[0,1]u(t)0,0t1}.

    Now let us list the following conditions which will be used in this paper:

    (H1) There exists a constant α>0 satisfying

    lim infu+f(t,u)uα, t[0,1]. (5)

    (H2) There exists a constant β with 0<β<α satisfying

    lim supu0|f(t,u)u|β, t[0,1]. (6)

    (H3) There exists a constant b>0 such that

    f(t,u)b, t[0,1],u(t)R. (7)

    (H4) limu+f(t,u)u=+.

    Theorem 5. Suppose that (H1)-(H3) hold. Then for any λ(λ1α,λ1β), problem (P) has at least one nontrivial solution, where λ1=r1(B) and B is given by (4).

    Proof. Let (Fu)(t)=f(t,u(t)) for all uE, then by (4), A=BF. Applying the Arzela-Ascoli theorem and a standard argument, we can prove that (λA):EE is a completely continuous operator. It is known to all that the nonzero fixed points of the operator λA are the nontrivial solutions of the boundary value problem (P).

    Now we show that there exists R0>0, such that for any R>R0,

    uλAuμu,μ0,uTR, (8)

    where u is the positive eigenfunction of B corresponding to its first eigenvalue λ1=r1(B), TR={uC[0,1]u<R} is a bounded open subset of E.

    If (8) is not true, then there exist μ0>0 (if μ0=0, then Theorem 5 holds) and u0TR such that

    u0λAu0=μ0u. (9)

    By (5) and (6), there exist l>0,r0>0 and 0<ε<min{αλλ1λ,λ1βλλ} such that

    f(t,u)(αε)ul, t[0,1],u0, (10)
    |f(t,u)|(β+ε)|u|, t[0,1],|u|r0. (11)

    It follows from (7) that

    f(t,u)b(αε)ub,t[0,1],u0. (12)

    Take ω=max{b,l}, then by (10) and (12) we have f(t,u)(αε)uω,t[0,1],uR. Let α1=αε, then

    λAu=λBFuλα1Buu1, uE, (13)

    where u1=10G(t,s)λωds. Take

    δ=23λ110s2(1s)u(s)ds>0.

    By (4) and (G2) we have

    u(t)=λ1Bu(t)=λ110G(t,s)u(s)dsλ11016s2(1s)t2(1t)u(s)ds16λ1t2(1t)10s2(1s)u(s)ds23λ1G(t,s)10s2(1s)u(s)ds=δG(t,s).

    Let

    P1={uP10u(t)u(t)dtλ11δu}.

    For any uP, we have

    10u(t)(λBu)(t)dt=10u(t)[10G(t,s)λu(s)ds]dt=10λu(s)[10G(s,t)u(t)dt]ds=10λu(s)Bu(s)dsλ11δ10G(t,s)λu(s)ds=λ11δ(λBu)(t).

    And so  10u(t)(λBu)(t)dtλ11δλBu, i.e.,  (λB)(P)P1. Since Fu0+ωP, then (λB)(Fu0+ω)P1 and μ0u=μ0λ1BuP1. By (9) we have u0+λBω=λAu0+μ0u+λBω=λB(Fu0+ω)+μ0uP1. Thus

    10u(t)(u0+λBω)(t)dtλ11δu0+λBωλ11δu0λ11δλBω. (14)

    Take ε0=α1λr(B)1>0. By (13) we have

    10u(t)(λAu0)(t)dt10u(t)α1(λBu0)(t)dt10u(t)u1(t)dt=α1λr(B)10u(t)u0(t)dt10u(t)u1(t)dt=10u(t)u0(t)dt+ε010u(t)(u0+λBω)(t)dtε010u(t)(λBω)(t)dt10u(t)u1(t)dt.

    Take R0=λ1ε0δ[ε0δλ11λBω+ε010u(t)(λBω)(t)dt+10u(t)u1(t)dt]. For any u0=R>R0, by (14) we have

    10u(t)(λAu0u0)(t)dtε0[λ11δu0λ11δλBω]ε010u(t)(λBω)(t)dt10u(t)u1(t)dt>ε0δλ11R0ε0δλ11λBωε010u(t)(λBω)(t)dt10u(t)u1(t)dt=0.

    But we see from (9) that

    10u(t)(u0λAu0)(t)dt=10u(t)μ0u(t)dt0,

    which is a contradiction. So (8) is true. By Lemma 2 we have

    deg(IλA,TR,θ)=0. (15)

    Next we show that

    (λA)uμu, uTr,μ1, (16)

    where 0<r<min{r0,R0}. Assume on the contrary that there exist u0Tr and μ01 such that (λA)u0=μ0u0. Since λA has no fixed point on Tr, we have μ0>1. Let B1=λ(β+ε)B, then r(B1)<1. By (11) we have |λAu0|(β+ε)λB|u0|=B1|u0|, then μ0|u0|B1|u0|, and therefore

    μn0|u0|Bn1|u0|. (17)

    Let D={vv|u0|}. It follows from (17) that {μn0Bn1|u0|n=1,2,}D. And u0Tr and θTr imply that d=d(θ,D)>0. Then one can have that

    Bn11u0Bn1u0du0μn0,n=1,2,,

    which shows

    r(B1)=limn(Bn1)1/nlimn(du0μn0)1/n=μ0>1.

    This contradicts r(B1)<1. So (16) holds. By Lemma 1, we have

    deg(IλA,Tr,θ)=1. (18)

    By (15) and (18), we have

    deg(IλA,TR¯Tr,θ)=deg(IλA,TR,θ)deg(IλA,Tr,θ)=1.

    Then λA has at least one fixed point in TR¯Tr. This means that problem (P) has at least one nontrivial solution.

    Remark 6. For any α>0 and β=0, the proof of Theorem 5 is valid. Then for any λ>0, problem (P) has at least one nontrivial solution.

    Corollary 7. Suppose that (H1) and (H2) hold. Assume there exists a constant b>0 such that

    f(t,u)bK, t[0,1],uλ1bβ,

    where K=maxt[0,1]10G(t,s)ds. Then for any λ(λ1α,λ1β) problem (P) has at least one nontrivial solution.

    Proof. Let

    f1(t,u)={f(t,u),uλ1bβ,t[0,1],    f(t,λ1bβ),u<λ1bβ,t[0,1],
    (A1u)(t)=10G(t,s)f1(s,u(s))ds.

    Then all conditions of Theorem 5 hold for f1. By Theorem 5, λA1 has at least one nonzero fixed point v(t), and

    v(t)=λ10G(t,s)f1(s,v(s))dsλbK10G(t,s)dsλ1bβ.

    Thus

    v(t)=λ10G(t,s)f1(s,v(s))ds=λ10G(t,s)f(s,v(s))ds=λAv(t).

    This indicates v(t) is a nontrivial solution of problem (P).

    Theorem 8. Suppose that (H1) and (H3) hold. Let f(t,0)0,t[0,1] and

    limu0f(t,u)u=ρ. (19)

    Then for any λ(λ1α,+) and λλ1ρ, problem (P) has at least one nontrivial solution.

    Proof. From the proof of Theorem 5, if (H1) and (H3) hold, then there exists R0>0 such that for any R>R0 and λ>λ1α (15) holds.

    Since f(t,0)0,t[0,1], then Aθ=θ. By (19) we have that the Frechet derivative Aθ of A at θ exists and (Aθu)(t)=10G(t,s)ρu(s)ds. Notice that λλ1ρ, then 1 is not an eigenvalue of λAθ. By Lemma 3 there exists r0>0, for any 0<r<min{r0,R0},

    deg(IλA,Tr,θ)=deg(IλAθ,Tr,θ)=(1)κ0, (20)

    where κ is the sum of algebraic multiplicities for all eigenvalues of λAθ lying in the interval (0, 1).

    By (15) and (20) λA has at least one nonzero fixed point. Thus problem (P) has at least one nontrivial solution.

    In many realistic problems, the positive solution is more significant. In this section we will study this question.

    Theorem 9. Suppose that (H4) holds. Then there exists λ>0 such that for any 0<λ<λ problem (P) has at least one positive solution.

    Proof. Let D=[0,1],D0=[t1,t2](0,1)D,η=mint1tt234t3(1t)2>0. By (H4) there exist b1>0 and R1>0 such that

    f(t,u)b1,t[0,1],u0,
    f(t,u)η1Nb1,t[t1,t2],uR1, (21)

    where N>1(t2t1)t2t1 is a natural number. Let

    f2(t,u)={f(t,u),u0,f(t,u),u<0.

    Then

    f2(t,u)b1,t[0,1],uR. (22)

    Let

    (A2u)(t)=10G(t,s)f2(s,u(s))ds.

    Obviously, A2:EE is a completely continuous operator.

    From Remark 6 and the proof of Theorem 5 there exists R0>0, for any R>R0,

    deg(IλA2,TR,θ)=0,λ>0. (23)

    Take 0<r<R0. Let m=max0t1,|u|r|f2(t,u)|, M=max0s,t1G(t,s), ¯λ=r(mM)1. For any 0<λ<¯λ,uTr, we have

    λA2u=max0t1|10λG(t,s)f2(s,u(s))ds|<¯λMm=r=u.

    Thus

    deg(IλA2,Tr,θ)=1,  0<λ<¯λ. (24)

    From (23) and (24) we have that for any 0<λ<¯λ, there exists uλC[0,1] with uλ>r such that uλ=λA2uλ. Now we show

    limλ0+, uλ=λA2uλ, uλ>ruλ=+. (25)

    In fact, if (25) doesn't hold, then there exist λn>0,uλnC[0,1] such that λn0,r<uλn<c (c>0 is a constant), and

    uλn=λnA2uλn. (26)

    Since A2 is completely continuous, then {uλn} has a subsequence (assume without loss of generality that it is {uλn}) converging to uC[0,1]. Let n+ in (26), we have u=θ, which is a contradiction of uλn>r>0. Then (25) holds.

    Next we show that there exists R=R(¯λ)>0 such that if 0<λ0¯λ,u0R and u0=λ0Au0, then u0(t)0. Take

    R=R(¯λ)=max{2η1R1, 2η1¯λb1M, 2¯λb1M}. (27)

    Assume that 0<λ0¯λ,u0R and u0=λ0Au0. Take any ¯t[t1,t2], by (G3) we have that for any τ[0,1],

    u0(¯t)=λ010G(¯t,s)[f2(s,u0(s))+b1]dsλ010b1G(¯t,s)dsλ0η10G(τ,s)f2(s,u0(s))ds¯λb1M=ηu0(τ)¯λb1M. (28)

    On account of the continuity of u0, there exists t[0,1] such that u0(t)=u0. Take τ=t in (28), by (27) we have

    u0(¯t)ηu0¯λb1MηR¯λb1M=η2R+η2R¯λb1Mη2RR1.

    Thus u0(¯t)R1, for any ¯t[t1,t2]. By (21) we have

    f2(s,u0(s))η1Nb1,sD0=[t1,t2]. (29)

    It follows from (G1) and (G3) that for any s[t1,t2] and t,τ[0,1]

    G(t,s)=G(s,t)ηG(τ,t)=ηG(t,τ). (30)

    Take DiD (i=1,2,,N) such that mesDi=mesD0, Ni=1DiDD0. By (29) and (30) we have that for any tD,sD0,τDi (i=1,2,,N),

    1NG(t,s)f2(s,u0(s))b1G(t,τ). (31)

    Notice that mesDi=mesD0(i=1,2,,N), then

    1ND0G(t,s)f2(s,u0(s))dsDib1G(t,τ)dτ, i=1,2,,N.

    Thus

    D0G(t,s)f2(s,u0(s))dsNi=1Dib1G(t,τ)dτDD0b1G(t,τ)dτ=DD0b1G(t,s)ds. (32)

    By (32) and (21) we have that for any t[0,1],

    u0(t)=λ0D0G(t,s)f2(s,u0(s))ds+λ0DD0G(t,s)f2(s,u0(s))ds0.

    For R in (27), by (25), there exists λ<¯λ such that if 0<λλ,uλr and uλ=λA2uλ, then uλR, thus uλ(t)0. By the definition of A2 and f2 we have

    uλ(t)=λ10G(t,s)f2(s,uλ(s))ds=λ10G(t,s)f(s,uλ(s))ds=λAuλ(t).

    So uλ(t) is a positive solution of problem (P).

    Remark 10. In Theorem 9 we obtain the existence of positive solutions for the semipositone boundary value problem (P) without that assuming (1) holds.

    Remark 11. Since we only study the existence of positive solutions for the boundary value problem (P), which is irrelevant to the value of f(t,u) when u0, we only suppose that f(t,u) is bounded below when u0. The nonlinear term f(t,u) may be unbounded from below when u0.

    Example 12. Consider the fourth-order boundary value problem

    {u(4)(t)=λ[(t+1)u33u], 0t1,u(0)=u(0)=u(1)=u(1)=0.                   (P1)

    In this example, f(t,u)=(t+1)u33u, then

    limu+f(t,u)u=limu+((t+1)u213u2)=+,

    which means that (H4) holds. By Theorem 9 there exists λ>0 such that for any 0<λ<λ BVP (P1) has at least one positive solution.

    Remark 13. In Example 12, the nonlinear term f doesn't satisfy (1) and (H3), but the existence of positive solutions of BVP (P1) is obtained by using our result.

    This work is supported by the Foundation items: National Natural Science Foundation of China (11501260), Natural Science Foundation of Jiangsu Higher Education Institutions(18KJB180027), and Postgraduate Research Innovation Program of Jiangsu Province(KYCX20_82).

    The authors declare that there is no conflict of interests regarding the publication of this article.



    [1] R. P. Agarwal, Y. M. Chow, Iterative method for fourth order boundary value problem, J. Comput. Appl. Math., 10 (1984), 203–217. doi: 10.1016/0377-0427(84)90058-X
    [2] Z. B. Bai, H. Y. Wang, On positive solutions of some nonlinear four-order beam equations, J. Math. Anal. Appl., 270 (2002), 357–368. doi: 10.1016/S0022-247X(02)00071-9
    [3] Z. B. Bai, The upper and lower solution method for some fourth-order boundary value problems, Nonlinear Anal.-Theor.,, 67 (2007), 1704–1709.
    [4] G. Bonanno, B. D. Bella, A boundary value problem for fourth-order elastic beam equations, J. Math. Anal. Appl., 343 (2008), 1166–1176. doi: 10.1016/j.jmaa.2008.01.049
    [5] G. Bonanno, B. D. Bella, D. O'Regan, Non-trivial solutions for nonlinear fourth-order elastic beam equations, Comput. Math. Appl., 62 (2011), 1862–1869. doi: 10.1016/j.camwa.2011.06.029
    [6] R. Graef, B. Yang, Positive solutions of a nonlinear fourth order boundary value problem, Communications on Applied Nonlinear Analysis, 14 (2007), 61–73.
    [7] C. P. Gupta, Existence and uniqueness results for the bending of an elastic beam equation, Appl. Anal., 26 (1988), 289–304. doi: 10.1080/00036818808839715
    [8] P. Korman, Uniqueness and exact multiplicity of solutions for a class of fourth-order semilinear problems, P. Roy. Soc. Edinb. A, 134 (2004), 179–190. doi: 10.1017/S0308210500003140
    [9] B. D. Lou, Positive solutions for nonlinear elastic beam models, International Journal of Mathematics and Mathematical Sciences, 27 (2001), 365–375. doi: 10.1155/S0161171201004203
    [10] R. Y. Ma, L. Xu, Existence of positive solutions of a nonlinear fourth-order boundary value problem, Appl. Math. Lett., 23 (2010), 537–543. doi: 10.1016/j.aml.2010.01.007
    [11] Q. L. Yao, Positive solutions for eigenvalue problems of four-order elastic beam equations, Appl. Math. Lett., 17 (2004), 237–243. doi: 10.1016/S0893-9659(04)90037-7
    [12] Q. L. Yao, Existence of n solutions and/or positive solutions to a semipositone elastic beam equation, Nonlinear Anal.-Theor., 66 (2007), 138–150. doi: 10.1016/j.na.2005.11.016
    [13] Q. L. Yao, positive solutions of nonlinear elastic beam equation rigidly fastened on the left and simply supported on the right, Nonlinear Anal.-Theor., 69 (2008), 1570–1580. doi: 10.1016/j.na.2007.07.002
    [14] C. B. Zhai, R. P. Song, Q. Q. Han, The existence and the uniqueness of symmetric positive solutions for a fourth-order boundary value problem, Comput. Math. Appl., 62 (2011), 2639–2647. doi: 10.1016/j.camwa.2011.08.003
    [15] X. P. Zhang, Existence and iteration of monotone positive solutions for an elastic beam equation with a corner, Nonlinear Anal.-Real, 10 (2009), 2097–2103. doi: 10.1016/j.nonrwa.2008.03.017
    [16] K. Deimling, Nonlinear Functional Analysis, Springer-Verlag, Berlin-Heidelberg-Newyork, 1985.
    [17] D. J. Guo, V. Lakshmikanthan, Nonlinear Problems in Abstract Cones, Academic press, San Diego, 1988.
    [18] D. J. Guo, Nonlinear Functional Analysis, second edn., Shandong Science and Technology Press, Jinan, 2001 (in Chinese).
    [19] H. Amann, Fixed point equations and nonlinear eigenvalue problems in ordered Banach spaces, SIAM Rev., 18 (1976), 620–709. doi: 10.1137/1018114
    [20] G. W. Zhang, J. X. Sun, Positive solutions of m-point boundary value problems, J. Math. Anal. Appl., 291 (2004), 406–418. doi: 10.1016/j.jmaa.2003.11.034
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