812
Views
9
CrossRef citations to date
0
Altmetric
Research Articles

On the oscillation of second-order half-linear functional differential equations with mixed neutral term

ORCID Icon & ORCID Icon
Pages 481-489 | Received 18 Dec 2018, Accepted 07 Mar 2019, Published online: 27 Mar 2019

Abstract

In this article, the authors establish new sufficient conditions for the oscillation of solutions to a class of second-order half-linear functional differential equations with mixed neutral term. The results obtained improve and complement some known results in the relevant literature. Examples illustrating the results are included.

1991 Mathematics Subject Classifications:

1. Introduction

This paper deals with the oscillatory behaviour of solutions to a class of second order half-linear functional differential equations with mixed neutral term of the form (1) (r(t)(z(t))α)+q(t)xα(h(t))=0,tt0>0,(1) where z(t)=x(t)+p1(t)x(g1(t))+p2(t)x(g2(t)), α is a quotient of odd positive integers, and the following conditions are always assumed to hold:

(C1)

r,q:[t0,)(0,) are real valued continuous functions with t0r1/α(s)ds=;

(C2)

g1,g2,h:[t0,)R are real valued continuous functions such that g1(t)<t, g2(t)>t, g1 and g2 are strictly increasing, and limtg1(t)=limtg2(t)=limth(t)=;

(C3ξ)

p1,p2:[t0,)R are real valued continuous functions with p1(t)0, p2(t)1, and p2(t)1 eventually;

or

(C3ϕ)

p1,p2:[t0,)R are real valued continuous functions with p2(t)0, p1(t)1, and p1(t)1 eventually.

By a solution of equation (Equation1) we mean a function x:[tx,)R, txt0, such that zC1([tx,),R), r(z)αC1([tx,),R), and which satisfies (Equation1) on [tx,). We consider only those solutions x(t) of (Equation1) that satisfy sup{|x(t)|:tT}>0 for all Ttx; moreover, we tacitly assume that (Equation1) possesses such solutions. Such a solution x(t) of (Equation1) is said to be oscillatory if it has arbitrarily large zeros on [tx,); otherwise, it is called nonoscillatory. Equation (Equation1) is said to be oscillatory if all its solutions are oscillatory.

Oscillation and asymptotic behaviour of solutions to various classes of delay and advanced neutral differential and dynamic equations have been widely discussed in the literature; see, for example, [Citation1–19], and the references contained therein.

However, oscillation results for mixed neutral differential and dynamic equations are relatively scarce in the literature; some results can be found, for example, in [Citation20–32], and the references cited therein. We would like to point out that the results obtained in [Citation20–32] require both of p1 and p2 to be constants or bounded functions, and hence, the results established in these papers cannot be applied to the cases where limtp1(t)= and /or limtp2(t)=. In view of the observations above, we wish to develop new sufficient conditions which can be applied to the cases where limtp1(t)= and /or limtp2(t)=. In this connection, the results obtained in the present paper are new, improve and complement some existing results in the relevant literature. Furthermore, the results in this paper can easily be extended to more general second-order mixed neutral differential and dynamic equations to obtain more general oscillation results. It is therefore hoped that the present paper will contribute significantly to the study of oscillation of solutions of second-order mixed neutral differential equations.

2. Some preliminary lemmas

In this section, we present some lemmas that will play an important role in establishing our main results. For notational purposes, we let, for any continuous function d, d+t:=max0,dt,Rt,t1:=t1tr1/α(s)ds, and throughout this paper, we define ξ(t):=1p2(g21(t))11p2(g21(g21(t)))p1(g21(t))p2(g21(g1(g21(t)))),ϕt:=1p1(g11(t))11p1(g11(g11(t)))m(g11(g11(t)))m(g11(t))p2(g11(t))p1(g11(g2(g11(t))))m(g11(g2(g11(t))))m(g11(t)) for all sufficiently large t, where g11 and g21 denote the inverse functions of g1 and g2, respectively, and m is a function to be specified later.

Lemma 2.1

[Citation33]

If D and E are nonnegative and λ>1, then λDEλ1Dλλ1Eλ, where equality holds if and only if D=E.

Lemma 2.2

Assume that conditions (C1)–(C3ξ) (or (C1), (C2), and (C3ϕ)) hold, and let x(t) be an eventually positive solution of (Equation1). Then there exists t1t0 such that, for tt1, (2) rtztα<0,zt>0,and zt>0.(2)

Proof.

The proof is standard and so we omit the details of its proof.

Lemma 2.3

In addition to conditions (C1)(C3ξ) (or (C1), (C2), and (C3ϕ)), assume that x(t) is an eventually positive solution of (Equation1) such that (Equation2) holds. If there exist a positive function mC1([t0,),R) and a t2[t1,) such that (3) mtr1/αtRt,t1mt0fortt2,(3) then (4) zt/mt0fortt2.(4)

Proof.

Since r(t)(z(t))α is decreasing on [t1,), we obtain (5) zt=zt1+t1trszsα1/αr1/αsdsr1/αtRt,t1zt.(5) Thus, in view of (Equation3) and (Equation5), we see that (6) ztm(t)=ztm(t)ztm(t)m2(t)ztm2tmtr1/αtRt,t1mt0,(6) for tt2 and for some t2[t1,). This completes the proof of the lemma.

Lemma 2.4

Let conditions (C1)(C3ξ) hold and ξ(t)>0. If x(t) is an eventually positive solution of (Equation1) such that (Equation2) holds, then z(t) satisfies the inequality (7) rtztα+qtξαhtzαg21ht0(7) for sufficiently large t.

Proof.

Let x(t) be an eventually positive solution of (Equation1) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ξ(t)>0 and z(t) satisfies (Equation2) for tt1 and for some t1[t0,). From the definition of z(t), (see also (8.6) in [Citation1]), we obtain (8) x(t)=1p2(g21(t))z(g21(t))x(g21(t))p1(g21(t))x(g1(g21(t)))=z(g21(t))p2(g21(t))z(g21(g21(t)))x(g21(g21(t)))p1(g21(g21(t)))x(g1(g21(g21(t))))p2(g21(t))p2(g21(g21(t)))p1(g21(t))p2(g21(t))z(g21(g1(g21(t))))x(g21(g1(g21(t))))p2(g21(g1(g21(t))))p1(g21(g1(g21(t))))x(g1(g21(g1(g21(t)))))p2(g21(g1(g21(t))))z(g21(t))p2(g21(t))z(g21(g21(t)))p2(g21(t))p2(g21(g21(t)))p1(g21(t))z(g21(g1(g21(t))))p2(g21(t))p2(g21(g1(g21(t)))).(8) Using the fact that the functions z, g1 and g2 are strictly increasing, and noting that g1(t)<t<g2(t), we get (9) z(g21(g21(t)))<z(g21(t))(9) and (10) z(g21(g1(g21(t))))<z(g21(t)).(10) Using (Equation9) and (Equation10) in (Equation8) gives (11) x(t)1p2(g21(t))11p2(g21(g21(t)))p1(g21(t))p2(g21(g1(g21(t))))z(g21(t))(11) for tt1. Since limth(t)=, we can choose t2t1 such that h(t)t1 for all tt2. Thus, from (Equation11) we have (12) xh(t)ξh(t)zg21h(t)fortt2.(12) Substituting (Equation12) into (Equation1) gives (Equation7) and completes the proof.

Lemma 2.5

Let conditions (C1), (C2), and (C3ϕ) hold. Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If x(t) is an eventually positive solution of (Equation1) such that (Equation2) holds, then z(t) satisfies the inequality (13) rtztα+qtϕαhtzαg11ht0(13) for sufficiently large t.

Proof.

Let x(t) be an eventually positive solution of (Equation1) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ϕ(t)>0 and z(t) satisfies (Equation2) for tt1 and for some t1[t0,). Following a similar argument as in the proof of Lemma 2.4, we obtain (14) x(t)z(g11(t))p1(g11(t))z(g11(g11(t)))p1(g11(t))p1(g11(g11(t)))p2(g11(t))z(g11(g2(g11(t))))p1(g11(t))p1(g11(g2(g11(t)))).(14) Using the fact that g1 and g2 are strictly increasing, and noting that g1(t)<t<g2(t), we get (15) g11(g11(t))>g11(t)(15) and (16) g11(g2(g11(t)))>g11(t).(16) Since (Equation3) holds, we again have (Equation4) holds, i.e. z/m is nonincreasing on [t2,)[t1,). Thus, we deduce from (Equation15) and (Equation16) that (17) m(g11(g11(t)))z(g11(t))m(g11(t))z(g11(g11(t)))fortt2,(17) and (18) m(g11(g2(g11(t))))z(g11(t))m(g11(t))z(g11(g2(g11(t))))fortt2,(18) respectively.

Using (Equation17) and (Equation18) in (Equation14) yields (19) x(t)1p1(g11(t))11p1(g11(g11(t)))m(g11(g11(t)))m(g11(t))p2(g11(t))p1(g11(g2(g11(t))))m(g11(g2(g11(t))))m(g11(t))z(g11(t))(19) for tt2. Since limth(t)=, we can choose t3t2 such that h(t)t2 for all tt3. Thus, from (Equation19) we have (20) xh(t)ϕh(t)zg11h(t)fortt3.(20) Substituting (Equation20) into (Equation1) gives (Equation13) and completes the proof.

3. Main results

In this section, we present some sufficient conditions for the oscillation of all solutions of equation (Equation1). We begin with the following result.

Theorem 3.1

Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that (Equation3) holds. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (21) limsuptTtχ1sη+srsmsαmαsds=,(21) where χ1t=ηtqtξαhtmαg21htmαt, then every solution of equation (Equation1) is oscillatory.

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ξ(t)>0 and z(t) satisfies (Equation2) for tt1. (The proof if x(t) is eventually negative is similar, so we omit the details of that case here as well as in the remaining proofs in this paper). Proceeding as in the proofs of Lemmas 2.3 and 2.4, we see that (Equation4), (Equation5) and (Equation7) hold on [t2,)[t1,). Define the Riccati substitution (22) ωt=ηtrtztαzαtfortt1.(22) Clearly ω(t)>0 for tt1, and from (Equation7) we obtain (23) ωtη+trtztαzαtηtqtξαhtzαg21htzαtαηtrtztztα+1fortt2.(23) From g2(t)h(t) and the fact that g2 is strictly increasing, we see that tg21(h(t)). Hence, by (Equation4) we get (24) zg21htztmg21htmtfortt2.(24) Substituting (Equation24) into (Equation23) gives (25) ωtη+trtztαzαtηtqtξαhtmαg21htmαtαηtrtztztα+1fortt2.(25) In view of (Equation3) and (Equation5), it is easy to see that (26) mtmt1r1/αtRt,t1ztzt.(26) From (Equation26), z(t)>0, and z(t)>0, (Equation25) yields (27) ωtη+trtmtαmαtηtqtξαhtmαg21htmαt(27) for tt2. An integration of (Equation27) from t2 to t gives t2tχ1sη+srsmsαmαsdsωt2, which contradicts condition (Equation21). This completes the proof.

Theorem 3.2

Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that (Equation3) holds. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (28) limsuptTtχ1s1α+1α+1rsη+sα+1ηαsds=,(28) where χ1(t) is as in Theorem 3.1, then every solution of (Equation1) oscillates.

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ξ(t)>0 and z(t) satisfies (Equation2) for tt1. Proceeding as in the proof of Theorem 3.1, we again arrive at (Equation25) for tt2. From (Equation22) and the definition of χ1(t), inequality (Equation25) can be written as (29) ωtη+tηtωtχ1tαηtrt1/αωα+1/αtfortt2.(29) Applying Lemma 2.1 with λ:=(α+1)/α, D=α1/ληtrt1/α1/λωt,andE=αα+1ηtrt1/α1/λα1/λη+tηtα, we obtain (30) η+tηtωtαηtrt1/αωλt1α+1α+1rtη+tα+1ηαt.(30) Substituting (Equation30) into (Equation29) gives ωt1α+1α+1rtη+tα+1ηαtχ1t. Integrating the last inequality from t2 to t yields t2tχ1s1α+1α+1rsη+sα+1ηαsdsωt2, which is a contradiction to our assumption (Equation28). This proves the theorem.

Theorem 3.3

Let α1. Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that (Equation3) holds. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (31) limsuptTtχ1sr1/αsη+s24αηsRs,t1α1ds=,(31) where χ1(t) is as in Theorem 3.1, then every solution of equation (Equation1) oscillates.

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ξ(t)>0 and z(t) satisfies (Equation2) for tt1. Proceeding as in the proof of Theorem 3.2, we again arrive at (Equation29) which can be written as (32) ωtη+tηtωtχ1tαω1/α1tηtrt1/αω2tfortt2.(32) From (Equation22) and (Equation5), we obtain (33) ωt1/α1=ηtrt1/α1zt1αzt1α=ηtrt1/α1ztα1ztα1ηtrt1/α1r1/αtRt,t1α1=ηt1/α1Rt,t1α1.(33) Using (Equation33) in (Equation32), we conclude that (34) ωtη+tηtωtχ1tαRt,t1α1ηtr1/αtω2tfortt2.(34) Completing the square with respect to ω, it follows from (Equation34) that (35) ωtχ1t+r1/αt4αRt,t1α1η+t2ηt.(35) Integrating (Equation35) from t2 to t gives t2tχ1sr1/αsη+s24αηsRs,t1α1dsωt2, which contradicts condition (Equation31). This completes the proof of the theorem.

Theorem 3.4

Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (36) limsuptTtχ2sη+sRαs,t1ds=,(36) where χ2t=ηtqtξαht, then every solution of equation (Equation1) is oscillatory.

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ξ(t)>0 and z(t) satisfies (Equation2) for tt1. Proceeding exactly as in the proof of Theorem 3.1, we again arrive at (Equation23) for tt2. From g2(t)h(t) and the fact that g2 is strictly increasing, we see that (37) tg21ht,(37) and so (38) zg21htzt1.(38) Using (Equation38) in (Equation23) yields (39) ωtη+trtztαzαtχ2tαηtrtztztα+1  fortt2.(39) Taking into account that (Equation5) holds, and using the fact that z(t)>0, inequality (Equation39) takes the form ωtη+tRαt,t1χ2tfortt2. The remainder of the proof is similar to that of Theorem 3.1, and so the details are omitted.

Theorem 3.5

Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (40) limsuptTtχ2s1α+1α+1rsη+sα+1ηαsds=,(40) where χ2(t) is as in Theorem 3.4, then equation (Equation1) is oscillatory.

Proof.

The proof follows from (Equation22), (Equation30), (Equation39), and Theorem 3.2.

Theorem 3.6

Let α1. Assume that (C1)(C3ξ) hold, ξ(t)>0 and g2(t)h(t). If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T(t1,), (41) limsuptTtχ2sr1/αsη+s24αηsRs,t1α1ds=,(41) where χ2(t) is as in Theorem 3.4, then equation (Equation1) is oscillatory.

Proof.

The proof follows from (Equation22), (Equation33), (Equation39), and Theorem 3.3.

Theorem 3.7

Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (42) limsuptTtχ3sη+srsmsαmαsds=,(42) where χ3t=ηtqtϕαhtmαg11htmαt, then every solution of equation (Equation1) is oscillatory.

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ϕ(t)>0 and z(t) satisfies (Equation2) for tt1. Proceeding as in the proofs of Lemmas 2.3 and 2.5, we see that (Equation4), (Equation5) and (Equation13) hold for tt3 and for some t3[t2,)[t1,). Define again Riccati substitution w by (Equation22). Then, it follows from (Equation22) and (Equation13) that (43) ωtη+trtztαzαtηtqtϕαhtzαg11htzαtαηtrtztztα+1fortt3.(43) Since g1(t)h(t) and g1 is strictly increasing, we see that tg11(h(t)). Hence, from (Equation4) we get (44) zg11htztmg11htmt.(44) Substituting (Equation44) into (Equation43) gives (45) ωtη+trtztαzαtηtqtϕαhtmαg11htmαtαηtrtztztα+1fortt3.(45) The remainder of the proof is similar to that of Theorem 3.1, and so the details are omitted.

Theorem 3.8

Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (46) limsuptTtχ3s1α+1α+1rsη+sα+1ηαsds=,(46) where χ3(t) is as in Theorem 3.7, then every solution of equation (Equation1) oscillates.

Proof.

The proof follows from (Equation22), (Equation30), (Equation45), and Theorem 3.2.

Theorem 3.9

Let α1. Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (47) limsuptTtχ3sr1/αsη+s24αηsRs,t1α1ds=,(47) where χ3(t) is as in Theorem 3.7, then every solution of equation (Equation1) oscillates.

Proof.

The proof follows from (Equation22), (Equation33), (Equation45), and Theorem 3.3.

Theorem 3.10

Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (48) limsuptTtχ4sη+sRαs,t1ds=,(48) where χ4t=ηtqtϕαht, then every solution of equation (Equation1) is oscillatory

Proof.

Let x(t) be a nonoscillatory solution of (Equation1). Without loss of generality, we may assume that there exists t1[t0,) such that x(t)>0, x(g1(t))>0, x(g2(t))>0, x(h(t))>0, ϕ(t)>0 and z(t) satisfies (Equation2) for tt1. Proceeding as in the proof of Theorem 3.7, we again arrive at (Equation43). From g1(t)h(t) and the fact that g1 is strictly increasing, we see that (49) tg11ht,(49) and so, from the fact that z(t)>0, we have (50) zg11htzt1.(50) Using (Equation50) in (Equation43) gives (51) ωtη+trtztαzαtηtqtϕαhtαηtrtztztα+1.(51) Taking into account that (Equation5) holds, and from the fact that z(t)>0, inequality (Equation51) takes the form ωtη+tRαt,t1ηtqtϕαht. The remainder of the proof is similar to that of Theorem 3.1, and so the details are omitted.

Theorem 3.11

Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (52) limsuptTtχ4s1α+1α+1rsη+sα+1ηαsds=,(52) where χ4(t) is as in Theorem 3.10, then equation (Equation1) is oscillatory.

Proof.

The proof follows from (Equation22), (Equation30), (Equation51), and Theorem 3.2.

Theorem 3.12

Let α1. Assume that conditions (C1), (C2), and (C3ϕ) hold and g1(t)h(t). Assume further that there exists a positive function mC1([t0,),R) such that ϕ(t)>0 and (Equation3) hold. If there exists a positive function ηC1([t0,),R) such that, for all sufficiently large t1[t0,) and for some T[t2,)(t1,), (53) limsuptTtχ4sr1/αsη+s24αηsRs,t1α1ds=,(53) where χ4(t) is as in Theorem 3.10, then equation (Equation1) is oscillatory.

Proof.

The proof follows from (Equation22), (Equation33), (Equation51), and Theorem 3.3.

We conclude this paper with the following examples to illustrate the above results. First example is concerned with the case where p2(t) as t, second example is concerned with the case where p1 and p2 are constants or bounded functions, third example is concerned with the case where p1(t) and p2(t) as t, and fourth example is concerned with the case where p1(t) as t.

Example 3.13

Consider the neutral differential equation (54) x(t)+xt2+tx(2t)3+t4+1x32t1=0,t13.(54) Here we have α=3, r(t)=p1(t)=1, p2(t)=t, q(t)=t4+1, g1(t)=t/2, g2(t)=2t and h(t)=2t1. It is clear that conditions (C1)(C3ξ) hold, g2(t)h(t), and (55) ξ(t)=1t/211t/41t/8=2t24t2>0.(55) On the other hand, if we choose m(t)=R(t,t1), we see that m(t)=t1t1r1/α(s)ds=13tds=t13, and so (Equation3) holds. With η(t)=t, condition (Equation21) with T>13 becomes limsuptTtχ1sη+srsmsαmαsds=limsuptTts(s4+1)4s26(2s1)23s27/2s1331(s13)3ds=, due to limsuptTts(s4+1)4s26(2s1)23s27/2s133ds= and limsuptTt1(s13)3ds<. Hence, by Theorem 3.1, every solution of (Equation54) is oscillatory.

Example 3.14

Consider the neutral differential equation (56) 1t1/3x(t)+2xt3+8x(4t)1/3+t2+tx1/35t=0,t2.(56) Here we have α=1/3, r(t)=1/t1/3, p1(t)=2, p2(t)=8, q(t)=t2+t, g1(t)=t/3, g2(t)=4t and h(t)=5t. It is clear that conditions (C1)(C3ξ) hold, g2(t)h(t), and (57) ξ(t)=1811828=564>0.(57) On the other hand, if we choose m(t)=R(t,t1), we see that m(t)=t1t1r1/α(s)ds=2tsds=t242, and (Equation3) holds. With η(t)=c>0 is a constant, condition (Equation36) with T>2 becomes limsuptTtχ2sη+sRαs,t1ds=limsuptTtcs2+s5641/3ds=, i.e. condition (Equation36) holds. Hence, by Theorem 3.4, every solution of (Equation56) is oscillatory.

Example 3.15

Consider the neutral differential equation (58) x(t)+3txt3+tx(2t)3+t5+tx3t4=0,t2.(58) Here we have α=3, r(t)=1, p1(t)=3t, p2(t)=t, q(t)=t5+t, g1(t)=t/3, g2(t)=2t and h(t)=t/4. It is clear that conditions (C1)(C3ϕ) hold and g1(t)h(t). If we choose m(t)=R(t,t1), we see that m(t)=t2, (Equation3) holds, and (59) ϕ(t)=19t1127t9t23t23t54t18t23t2=108t2120t+41458t3972t2>0.(59) With η(t)=t2, we see that condition (Equation42) holds for T>2. Hence, by Theorem 3.7, every solution of (Equation58) is oscillatory.

Example 3.16

Consider the neutral differential equation (60) x(t)+etx(t2π)+x(t+π)+2etxtπ2=0,t5.(60) Here we have α=1, r(t)=p2(t)=1, p1(t)=et, q(t)=2et, g1(t)=t2π, g2(t)=t+π and h(t)=tπ/2. It is clear that conditions (C1), (C2), and (C3ϕ) hold, and g1(t)h(t). On the other hand, if we choose m(t)=R(t,t1), we see that m(t)=t5, and so, ϕ(t)>0 and (Equation3) hold. With η(t)=c, it is easy to see that condition (Equation48) holds. Hence, by Theorem 3.10, every solution of (Equation60) is oscillatory. In fact, x(t)=sint is such a solution.

Disclosure statement

No potential conflict of interest was reported by the authors.

References

  • Agarwal RP, Grace SR, O'Regan D. The oscillation of certain higher-order functional dfferential equations. Math Comput Model. 2003;37:705–728.
  • Agarwal RP, Bohner M, Li T, et al. Oscillation of second-order Emden–Fowler neutral delay differential equations. Ann Math Pura Appl. 2014;193:1861–1875.
  • Baculíková B, Dzurina J. Oscillation theorems for second order neutral differential equations. Comput Math Appl. 2011;61:94–99.
  • Bohner M, Grace SR, Jadlovská I. Oscillation criteria for second-order neutral delay differential equations. Electron J Qual Theory Differ Equ. 2017;2017(60):1–12.
  • Chen D-X. Oscillation of second-order Emden-Fowler neutral delay dynamic equations on time scales. Math Comput Model. 2010;51:1221–1229.
  • Han Z, Li T, Sun S, et al. Remarks on the paper [Appl Math Comput. 2009;207:388–396]. Appl Math Comput. 2010;215:3998–4007.
  • Graef JR, Tunç E, Grace SR. Oscillatory and asymptotic behavior of a third-order nonlinear neutral differential equation. Opuscula Math. 2017;37(6):839–852.
  • Kubiaczyk I, Saker SH, Sikorska-Nowak A. Oscillation criteria for nonlinear neutral functional dynamic equations on time scales. Math Slovaca. 2013;63:263–290.
  • Li T, Agarwal RP, Bohner M. Some oscillation results for second-order neutral dynamic equations. Hacet J Math Stat. 2012;41:715–721.
  • Li T, Rogovchenko YV. Oscillatory behavior of second-order nonlinear neutral differential equations. Abstr Appl Anal. 2014;2014: Article ID:143614:8 pages.
  • Li T, Rogovchenko YV. Oscillation of second-order neutral differential equations. Math Nachr. 2015;268:1150–1162.
  • Li T, Rogovchenko YV. Oscillation criteria for second-order superlinear Emden–Fowler neutral differential equations. Monatsh Math. 2017;184:489–500.
  • Li T, Thandapani E, Graef JR, et al. Oscillation of second-order Emden–Fowler neutral differential equations. Nonlinear Stud. 2013;20(1):1–8.
  • Liu H, Meng F, Liu P. Oscillation and asymptotic analysis on a new generalized Emden-Fowler equation. Appl Math Comput. 2012;219:2739–2748.
  • Saker SH, Graef JR. Oscillation of third-order nonlinear neutral functional dynamic equations on time scales. Dyn Syst Appl. 2012;21:583–606.
  • Shi Y, Han Z, Sun Y. Oscillation criteria for a generalized Emden–Fowler dynamic equation on time scales. Adv Differ Equ. 2016;2016: Article ID:3:1–12.
  • Tunç E. Oscillatory and asymptotic behavior of third-order neutral differential equations with distributed deviating arguments. Electron J Differ Equ. 2017;2017(16):1–12.
  • Tunç E, Özdemir O. On the asymptotic and oscillatory behavior of solutions of third-order neutral dynamic equations on time scales. Adv Difference Equ. 2017;2017: Article ID:127:1–13.
  • Wang R, Li Q. Oscillation and asymptotic properties of a class of second-order Emden–Fowler neutral differential equations. Springer Plus. 2016;5:1956, 15 pages.
  • Agwa HA, Khodier AMM, Arafa HM. Oscillation of second-order nonlinear neutral dynamic equations with mixed arguments on time scales. J Basic Appl Res Int. 2016;17:49–66.
  • Arul R, Shobha VS. Oscillation of second order nonlinear neutral differential equations with mixed neutral term. J Appl Math Phys. 2015;3:1080–1089.
  • Han Z, Li T, Zhang C, et al. Oscillation criteria for certain second-order nonlinear neutral differential equations of mixed type. Abstr Appl Anal. 2011;2011: Article ID:387483:1–9.
  • Grace SR. Oscillations of mixed neutral functional differential equations. Appl Math Comput. 1995;68:1–13.
  • Ji T, Tang S, Thandapani E. Oscillation of second-order neutral dynamic equations with mixed arguments. Appl Math Inf Sci. 2014;8:2225–2228.
  • Li T. Comparison theorems for second-order neutral differential equations of mixed type. Electron J Differ Equ. 2010;2010(167):1–7.
  • Li T, Baculíková B, Dzurina J. Oscillation results for second-order neutral differential equations of mixed type. Tatra Mt Math Publ. 2011;48:101–116.
  • Li T, Senel MT, Zhang C. Oscillation of solutions to second-order half-linear differential equations with neutral terms. Electron J Differ Equ. 2013;2013(229):1–7.
  • Qi Y, Yu J. Oscillation of second order nonlinear mixed neutral differential equations with distributed deviating arguments. Bull Malays Math Sci Soc. 2015;38:543–560.
  • Thandapani E, Padmavathi S, Pinelas P. Oscillation criteria for even-order nonlinear neutral differential equations of mixed type. Bull Math Anal Appl. 2014;6(1):9–22.
  • Thandapani E, Selvarangam S, Vijaya M, et al. Oscillation results for second order nonlinear differential equation with delay and advanced arguments. Kyungpook Math J. 2016;56:137–146.
  • Yan J. Oscillations of higher order neutral differential equations of mixed type. Israel J Math. 2000;115:125–136.
  • Zhang C, Baculíková B, Dzurina J, et al. Oscillation results for second-order mixed neutral differential equations with distributed deviating arguments. Math Slovaca. 2016;66(3):615–626.
  • Hardy GH, Littlewood JE, Polya G. Inequalities. Reprint of the 1952 ed. Cambridge: Cambridge University Press; 1988.