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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.
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)
(1) where
, α is a quotient of odd positive integers, and the following conditions are always assumed to hold:
(C1) |
| ||||
(C2) |
| ||||
(C3ξ) |
or | ||||
(C3ϕ) |
|
By a solution of equation (Equation1(1)
(1) ) we mean a function
,
, such that
,
, and which satisfies (Equation1
(1)
(1) ) on
. We consider only those solutions
of (Equation1
(1)
(1) ) that satisfy
for all
; moreover, we tacitly assume that (Equation1
(1)
(1) ) possesses such solutions. Such a solution
of (Equation1
(1)
(1) ) is said to be oscillatory if it has arbitrarily large zeros on
; otherwise, it is called nonoscillatory. Equation (Equation1
(1)
(1) ) 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 and
to be constants or bounded functions, and hence, the results established in these papers cannot be applied to the cases where
and /or
. In view of the observations above, we wish to develop new sufficient conditions which can be applied to the cases where
and /or
. 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,
and throughout this paper, we define
for all sufficiently large t, where
and
denote the inverse functions of
and
, respectively, and m is a function to be specified later.
Lemma 2.1
[Citation33]
If D and E are nonnegative and then
where equality holds if and only if D=E.
Lemma 2.2
Assume that conditions (C1)– (or (C1), (C2), and
) hold, and let
be an eventually positive solution of (Equation1
(1)
(1) ). Then there exists
such that, for
(2)
(2)
Proof.
The proof is standard and so we omit the details of its proof.
Lemma 2.3
In addition to conditions –
(or
and
), assume that
is an eventually positive solution of (Equation1
(1)
(1) ) such that (Equation2
(2)
(2) ) holds. If there exist a positive function
and a
such that
(3)
(3) then
(4)
(4)
Proof.
Since is decreasing on
, we obtain
(5)
(5)
Thus, in view of (Equation3
(3)
(3) ) and (Equation5
(5)
(5) ), we see that
(6)
(6)
for
and for some
. This completes the proof of the lemma.
Lemma 2.4
Let conditions –
hold and
. If
is an eventually positive solution of (Equation1
(1)
(1) ) such that (Equation2
(2)
(2) ) holds, then
satisfies the inequality
(7)
(7) for sufficiently large t.
Proof.
Let be an eventually positive solution of (Equation1
(1)
(1) ) such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
and for some
. From the definition of
, (see also (8.6) in [Citation1]), we obtain
(8)
(8)
Using the fact that the functions z,
and
are strictly increasing, and noting that
, we get
(9)
(9) and
(10)
(10) Using (Equation9
(9)
(9) ) and (Equation10
(10)
(10) ) in (Equation8
(8)
(8) ) gives
(11)
(11) for
. Since
, we can choose
such that
for all
. Thus, from (Equation11
(11)
(11) ) we have
(12)
(12) Substituting (Equation12
(12)
(12) ) into (Equation1
(1)
(1) ) gives (Equation7
(7)
(7) ) and completes the proof.
Lemma 2.5
Let conditions
and
hold. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If
is an eventually positive solution of (Equation1
(1)
(1) ) such that (Equation2
(2)
(2) ) holds, then
satisfies the inequality
(13)
(13) for sufficiently large t.
Proof.
Let be an eventually positive solution of (Equation1
(1)
(1) ) such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
and for some
. Following a similar argument as in the proof of Lemma 2.4, we obtain
(14)
(14) Using the fact that
and
are strictly increasing, and noting that
, we get
(15)
(15) and
(16)
(16) Since (Equation3
(3)
(3) ) holds, we again have (Equation4
(4)
(4) ) holds, i.e. z/m is nonincreasing on
. Thus, we deduce from (Equation15
(15)
(15) ) and (Equation16
(16)
(16) ) that
(17)
(17) and
(18)
(18) respectively.
Using (Equation17(17)
(17) ) and (Equation18
(18)
(18) ) in (Equation14
(14)
(14) ) yields
(19)
(19)
for
. Since
, we can choose
such that
for all
. Thus, from (Equation19
(19)
(19) ) we have
(20)
(20) Substituting (Equation20
(20)
(20) ) into (Equation1
(1)
(1) ) gives (Equation13
(13)
(13) ) and completes the proof.
3. Main results
In this section, we present some sufficient conditions for the oscillation of all solutions of equation (Equation1(1)
(1) ). We begin with the following result.
Theorem 3.1
Assume that –
hold,
and
. Assume further that there exists a positive function
such that (Equation3
(3)
(3) ) holds. If there exists a positive function
such that, for all sufficiently large
and for some
,
(21)
(21) where
then every solution of equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. (The proof if
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
(4)
(4) ), (Equation5
(5)
(5) ) and (Equation7
(7)
(7) ) hold on
. Define the Riccati substitution
(22)
(22) Clearly
for
, and from (Equation7
(7)
(7) ) we obtain
(23)
(23)
From
and the fact that
is strictly increasing, we see that
. Hence, by (Equation4
(4)
(4) ) we get
(24)
(24) Substituting (Equation24
(24)
(24) ) into (Equation23
(23)
(23) ) gives
(25)
(25)
In view of (Equation3
(3)
(3) ) and (Equation5
(5)
(5) ), it is easy to see that
(26)
(26) From (Equation26
(26)
(26) ),
, and
, (Equation25
(25)
(25) ) yields
(27)
(27) for
. An integration of (Equation27
(27)
(27) ) from
to t gives
which contradicts condition (Equation21
(21)
(21) ). This completes the proof.
Theorem 3.2
Assume that –
hold,
and
. Assume further that there exists a positive function
such that (Equation3
(3)
(3) ) holds. If there exists a positive function
such that, for all sufficiently large
and for some
(28)
(28) where
is as in Theorem 3.1, then every solution of (Equation1
(1)
(1) ) oscillates.
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. Proceeding as in the proof of Theorem 3.1, we again arrive at (Equation25
(25)
(25) ) for
. From (Equation22
(22)
(22) ) and the definition of
, inequality (Equation25
(25)
(25) ) can be written as
(29)
(29) Applying Lemma 2.1 with
,
we obtain
(30)
(30) Substituting (Equation30
(30)
(30) ) into (Equation29
(29)
(29) ) gives
Integrating the last inequality from
to t yields
which is a contradiction to our assumption (Equation28
(28)
(28) ). This proves the theorem.
Theorem 3.3
Let . Assume that
–
hold,
and
. Assume further that there exists a positive function
such that (Equation3
(3)
(3) ) holds. If there exists a positive function
such that, for all sufficiently large
and for some
(31)
(31) where
is as in Theorem 3.1, then every solution of equation (Equation1
(1)
(1) ) oscillates.
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. Proceeding as in the proof of Theorem 3.2, we again arrive at (Equation29
(29)
(29) ) which can be written as
(32)
(32) From (Equation22
(22)
(22) ) and (Equation5
(5)
(5) ), we obtain
(33)
(33)
Using (Equation33
(33)
(33) ) in (Equation32
(32)
(32) ), we conclude that
(34)
(34) Completing the square with respect to ω, it follows from (Equation34
(34)
(34) ) that
(35)
(35) Integrating (Equation35
(35)
(35) ) from
to t gives
which contradicts condition (Equation31
(31)
(31) ). This completes the proof of the theorem.
Theorem 3.4
Assume that –
hold,
and
. If there exists a positive function
such that, for all sufficiently large
and for some
(36)
(36) where
then every solution of equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. Proceeding exactly as in the proof of Theorem 3.1, we again arrive at (Equation23
(23)
(23) ) for
. From
and the fact that
is strictly increasing, we see that
(37)
(37) and so
(38)
(38) Using (Equation38
(38)
(38) ) in (Equation23
(23)
(23) ) yields
(39)
(39) Taking into account that (Equation5
(5)
(5) ) holds, and using the fact that
, inequality (Equation39
(39)
(39) ) takes the form
The remainder of the proof is similar to that of Theorem 3.1, and so the details are omitted.
Theorem 3.5
Assume that –
hold,
and
. If there exists a positive function
such that, for all sufficiently large
and for some
(40)
(40) where
is as in Theorem 3.4, then equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation30
(30)
(30) ), (Equation39
(39)
(39) ), and Theorem 3.2.
Theorem 3.6
Let . Assume that
–
hold,
and
. If there exists a positive function
such that, for all sufficiently large
and for some
(41)
(41) where
is as in Theorem 3.4, then equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation33
(33)
(33) ), (Equation39
(39)
(39) ), and Theorem 3.3.
Theorem 3.7
Assume that conditions
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(42)
(42) where
then every solution of equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. Proceeding as in the proofs of Lemmas 2.3 and 2.5, we see that (Equation4
(4)
(4) ), (Equation5
(5)
(5) ) and (Equation13
(13)
(13) ) hold for
and for some
. Define again Riccati substitution w by (Equation22
(22)
(22) ). Then, it follows from (Equation22
(22)
(22) ) and (Equation13
(13)
(13) ) that
(43)
(43)
Since
and
is strictly increasing, we see that
. Hence, from (Equation4
(4)
(4) ) we get
(44)
(44) Substituting (Equation44
(44)
(44) ) into (Equation43
(43)
(43) ) gives
(45)
(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
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(46)
(46) where
is as in Theorem 3.7, then every solution of equation (Equation1
(1)
(1) ) oscillates.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation30
(30)
(30) ), (Equation45
(45)
(45) ), and Theorem 3.2.
Theorem 3.9
Let . Assume that conditions
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(47)
(47) where
is as in Theorem 3.7, then every solution of equation (Equation1
(1)
(1) ) oscillates.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation33
(33)
(33) ), (Equation45
(45)
(45) ), and Theorem 3.3.
Theorem 3.10
Assume that conditions
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(48)
(48) where
then every solution of equation (Equation1
(1)
(1) ) is oscillatory
Proof.
Let be a nonoscillatory solution of (Equation1
(1)
(1) ). Without loss of generality, we may assume that there exists
such that
,
,
,
,
and
satisfies (Equation2
(2)
(2) ) for
. Proceeding as in the proof of Theorem 3.7, we again arrive at (Equation43
(43)
(43) ). From
and the fact that
is strictly increasing, we see that
(49)
(49) and so, from the fact that
, we have
(50)
(50) Using (Equation50
(50)
(50) ) in (Equation43
(43)
(43) ) gives
(51)
(51) Taking into account that (Equation5
(5)
(5) ) holds, and from the fact that
, inequality (Equation51
(51)
(51) ) takes the form
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
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(52)
(52) where
is as in Theorem 3.10, then equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation30
(30)
(30) ), (Equation51
(51)
(51) ), and Theorem 3.2.
Theorem 3.12
Let . Assume that conditions
and
hold and
. Assume further that there exists a positive function
such that
and (Equation3
(3)
(3) ) hold. If there exists a positive function
such that, for all sufficiently large
and for some
(53)
(53) where
is as in Theorem 3.10, then equation (Equation1
(1)
(1) ) is oscillatory.
Proof.
The proof follows from (Equation22(22)
(22) ), (Equation33
(33)
(33) ), (Equation51
(51)
(51) ), 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 as
, second example is concerned with the case where
and
are constants or bounded functions, third example is concerned with the case where
and
as
, and fourth example is concerned with the case where
as
.
Example 3.13
Consider the neutral differential equation
(54)
(54) Here we have
,
,
,
,
,
and
. It is clear that conditions
hold,
, and
(55)
(55) On the other hand, if we choose
, we see that
and so (Equation3
(3)
(3) ) holds. With
, condition (Equation21
(21)
(21) ) with T>13 becomes
due to
and
Hence, by Theorem 3.1, every solution of (Equation54
(54)
(54) ) is oscillatory.
Example 3.14
Consider the neutral differential equation
(56)
(56) Here we have
,
,
,
,
,
,
and
. It is clear that conditions
–
hold,
, and
(57)
(57) On the other hand, if we choose
, we see that
and (Equation3
(3)
(3) ) holds. With
is a constant, condition (Equation36
(36)
(36) ) with T>2 becomes
i.e. condition (Equation36
(36)
(36) ) holds. Hence, by Theorem 3.4, every solution of (Equation56
(56)
(56) ) is oscillatory.
Example 3.15
Consider the neutral differential equation
(58)
(58) Here we have
,
,
,
,
,
,
and
. It is clear that conditions
hold and
. If we choose
, we see that
, (Equation3
(3)
(3) ) holds, and
(59)
(59) With
, we see that condition (Equation42
(42)
(42) ) holds for T>2. Hence, by Theorem 3.7, every solution of (Equation58
(58)
(58) ) is oscillatory.
Example 3.16
Consider the neutral differential equation
(60)
(60) Here we have
,
,
,
,
,
and
. It is clear that conditions
,
, and
hold, and
. On the other hand, if we choose
, we see that
, and so,
and (Equation3
(3)
(3) ) hold. With
, it is easy to see that condition (Equation48
(48)
(48) ) holds. Hence, by Theorem 3.10, every solution of (Equation60
(60)
(60) ) is oscillatory. In fact,
is such a solution.
Disclosure statement
No potential conflict of interest was reported by the authors.
ORCID
Ercan Tunç http://orcid.org/0000-0001-8860-608X
Orhan Özdemir http://orcid.org/0000-0003-1294-5346
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