Available online throug
ISSN 2229 – 5046
International Journal of Mathematical Archive- 9(2), Feb. – 2018 284
CLASSIFICATIONS OF SOLUTIONS OF SECOND ORDER
NONLINEAR NEUTRAL DELAY DYNAMIC EQUATIONS OF MIXED TYPE
N. SIKENDER*
1, P. RAMI REDDY
2, M. VENKATA KRISHNA
3AND M. CHENNA KRISHNA REDDY
41,3,4
Department of Mathematics,
Osmania University, Hyderabad, Telangana, India.
2
Department of Mathematics,
Khairathabad Govt. Degree College, Hyderabad, Telangana, India.
(Received On: 22-12-17; Revised & Accepted On: 06-02-18)
ABSTRACT
In this paper, the authors classified all solutions of the second-order nonlinear neutral delay dynamic equations of
mixed type into four classes and obtained conditions for the existence / non-existence of solutions in these classes. Examples are included to illustrate the validiation of the main results.Keywords: second-order, neutral dynamic equations, oscillatory solution, mixed type, weakly oscillatory solution,
asymptotic behavior, time scales.
INTRODUCTION
In this paper, we are concerned to obtain the conditions for the existence / non-existence solutions of a class
M
+,M
−,OS
,WOS
and asymptotic behavior of solutions of a classM
+ andM
− of second order nonlinear neutral delay dynamic equations of mixed type(a(t)(x(t) b(t)x( (t)) c(t)x( (t))) )
∆ ∆
+ α + β +p(t)f (x( (t))) q(t)g(x( (t))) = 0,γ + δ (1) for t∈[t , )0 ∞T, where T is a time scale with supT =∞. In what follows, it is always assume that
1. 1
rd 0 T
a∈C ([t , ) , (0, ))∞ ∞ , 2 rd 0 T
b, c∈C ([t , ) , R)∞ and p, q∈C ([t , ) , R)rd 0 ∞T ; 2. f , g∈C(R, R) such that
uf u
( ) > 0
anug u
( ) > 0
foru
≠
0
;3. α β γ δ ∈, , , C (R, R)rd are strictly increasin functions such that
α
( )
t
≤
t
,β
( )
t
≥
t
, γ(t)≤t,δ
( )
t
≥
t
and limt→∞α(t) =limt→∞β(t) =limt→∞γ(t) =limt→∞δ(t) =∞Let tx∈[t , )0 ∞T such that
α
(
t
)
≥
t
0 andγ
(
t
)
≥
t
0 for all t∈[t , )x ∞T. By a solution of equation (1), we shall mean a function x∈C ([t , ) , R)rd x ∞T which has the properties x(t) b(t)x( (t)) c(t)x( (t))+ α + β ∈C ([t , ) , R)1rd x ∞ Tand 1
rd x T
a(t)(x(t) b(t)x( (t)) c(t)x( (t)))+ α + β ∈C ([t , ) , R)∞ and satisfies equation (1) on [t , )x ∞ T. As is customary, a solution of equation (1) is oscillatory solution (OS) if it is neither eventually positive nor eventually negative, otherwise it is called non-oscillatory. A non-oscillatory solution
x
(
t
)
of equation (1) is said to be weaklyoscillatory solution (WOS) if
x
(
t
)
is non-oscillatory andx
∆(
t
)
is oscillatory for large value of t∈[t , )0 ∞T.In recent years, there has been much research activity concerning the oscillation, nonoscillation and asymptotic behavior of solutions of various differential equations, difference equations and dynamic equations. For
instance in [7, 8, 9] etc., authors have been studied by classifying all solutions into four classes such as
M
+,M
−,OS
,WOS
and obtained criteria for the existence/non-existence of solutions. In order to extend and generalize theCorresponding Author: N. Sikender*
1,
papers [7, 8, 9], Rami Reddy et al. [10] were concerned the solutions of existence/non-existence of a class
M
+,M
−,OS
,WOS
of second order nonlinear neutral delay dynamic equation of the form( ( )( ( )
r t x t
+
p t x
( ) ( ( ))) )
α
t
∆ ∆+
q t f x
( ) ( ( ( ))) = 0 ,
β
t
(2) for t∈[t , )0 ∞T, subject to the conditions:4. 1
rd 0 T
r∈C ([t , ) , (0, ))∞ ∞ , 2 rd 0 T p∈C ([t , ) , R∞ ;
5. q∈C ([t , ) , R)rd 0 ∞T and
q
does not vanish eventually;6. 1
f∈C (R, R) such that
f
satisfiesuf u
( ) > 0
foru
≠
0
andf u
'( )
≥
0
foru
∈
R
; 7. α β∈, C ([t , ) , R)rd 0 ∞T are strictly increasing functions such that
α
( )
t
≤
t
,β
( )
t
≤
t
andlim
t→∞α
( ) =
t
∞
=
lim
t→∞β
( )
t
.The study of the oscillation and other asymptotic properties of solutions of neutral delay difference / differential / dynamic equations with positive and negative coefficients attracted a good bit of attention in the last several years. For instance in [16, 17, 18, 20] etc., and the references cited therein, authors have been studied certain criteria of second order nonlinear dynamic equations with positive and negative coefficients. In order to extend and generalize the papers [16, 17, 18, 19], sikender et al. [11] were concerned the solutions of
existence/non-existence of a class
M
+,M
−,OS
,WOS
of second order nonlinear neutral delay dynamic equation of the form
(r(t)(x(t)+p(t)x( (t))) )α ∆ ∆ +q(t)f (x( (t))) h(t)g(x( (t))) = 0β − γ (3)
for t∈[t , )0 ∞T, subject to the conditions:
8. 1
rd 0 T
r∈C ([t , ) , (0, ))∞ ∞ , 2
rd 0 T
p∈C ([t , ) , R)∞ and q, h∈C ([t , ) , R)rd 0 ∞ T ;
9.
f g
,
∈
C R R
( , )
such thatuf u
( ) > 0
andug u
( ) > 0
foru
≠
0
; 10. α β γ ∈, , C ([t , ) , T)rd 0 ∞T are strictly increasing functions such that( )
t
t
α
≤
,β
( )
t
≤
t
,γ
( )
t
≤
t
andlim
t→∞α
( ) =
t
∞
=
lim
t→∞β
( )
t
.Interest in Functional differential and difference equations is growing due to the development in science and technology and the varied applications in many areas. For examples, equations involving delay and those involving advance and a combination of both arise in nerve conduction (Life Science), organizational behaviour (Social sciences), Signal processing pantograph equations (Mechanical Engineering), to mention a few (see for e.g [12, 13, 14, 15]). Study of such equations has been an active area of research for many researchers and recently an importance is given to the unification of continuous and discrete aspects of analysis on time scales. In [10], the authors considered equation (1) with
c t
( ) = 0
,q t
( ) = 0
for all t∈[t , )0 ∞T and classified all solutions of (1) into four classes and obtained criteria for the existence / non-existence of solutions in these classes. In [11], the authors considered equation (1) withc t
( ) = 0
,p t
( )
≥
0
,q t
( )
≤
0
andδ
( )
t
≤
t
for all t∈[t , )0 ∞T and classified all solutions of (1) into four classes and obtained criteria for the existence / non-existence of solutions in these classes. But, now the authors are so much interested on mixed delays. In [6], the authors considered the neutral differential equations of mixed type of the form' ' 1 2
(a(t)(x(t) bx(t+ − τ +) cx(t+ τ )) ) +p(t)x (tα − σ +1) q(t)x (tβ + σ2) = 0,
0
t≥t > 0
(4) subject to the following conditions:
11. 1
0
a∈C ([t , ), R)∞ and is positive for all
t
≥
t
0;
12.
b
andc
are constants,τ
1,τ
2,σ
1 andσ
2 are nonnegative constants; 13.α
andβ
are the ratio of odd positive integers;14. p, q∈C ([t , ) , R).rd 0 ∞T
Motivated and inspired by the papers mentioned above, in this paper the authors are interested to study the
solutions of existence / non-existence of a class
M
+,M
−,OS
,WOS
and asymptotic behavior ofM
+ andM
− of equation (1). Here we consider two cases, namelyp
≤
0
,q
≥
0
andp
≥
0
,q
≤
0
for large t∈[t , )0 ∞T, to give sufficient conditions in order that every solution of equation (1) oscillates and to study the asymptotic nature of non-oscillatory solutions of equation (1) with respect to their asymptotic behavior all the solutions of equation (1) may bepriori divided in to the following classes:
1.
M
+=
{
x
∈
S
:
there exists some x 0 T1
t ∈[t ,∞) such that
x
(
t
)
x
∆(
t
)
≥
0
for x T 1 t∈[t , ) }∞ ;2.
M
−=
{
x
∈
S
:
there exists some x T 1© 2018, IJMA. All Rights Reserved 286
3.
OS
=
{
x
∈
S
:
there exists a sequence tn∈[t , )0 ∞ T,t
n→
∞
such that x t x t( ) (n n+1)≤0};4.
WOS
= {
x
∈
S
:
x
(
t
)
is non-oscillatory for large t∈[t , )0 ∞T, butx
∆(
t
)
oscillates}.With a very simple argument we can prove that M+, M−, OS, WOS are mutually disjoint. By the above
definitions, it turns out that solutions in the class
M
+ are eventually either positive nondecreasing or negativenonincreasing, solutions in the class
M
− are eventually either positive nonincreasing or negative nondecreasing, solutions in the classOS
are oscillatory, and finally solutions in the classWOS
are weakly oscillatory.In next Section, we mentioned important lemma's which are existing in the literature. In Section 2, we obtain sufficient conditions for the existence/non-existence in the above said classes. In Section 3, we discuss the asymptotic
behavior of solutions in the class of
M
+ andM
−.1. IMPORTANT LEMMA’S
Theorem 1.1 (Chain rule) ([1, Theorem 1.90]): Let f : R→R is continuously differentiable and suppose g : T→R
is delta differentiable. Then f g : T →R is delta differentiable and the formula
)
(
}
))
(
)
(
)
(
(
{
=
)
(
)
(
10
f
g
t
h
t
g
t
dh
g
t
t
g
f
∆∫
'+
µ
∆ ∆Theorem 1.2 ([1, Theorem 1.117]): Let a∈Tk, b∈T and assume f : T×Tk →R is continuous at
(
t
,
t
)
, wherek
t∈T with
t
>
a
. Also assume thatf
∆(
t
,.)
is rd-continuous on[
a
,
σ
(
t
)].
Suppose that for eachε
>
0
there exists a neighbourhoodU
oft
, independent ofτ
∈
[
a
,
σ
(
t
)]
, such that| ( ( ), )
f
σ
t
τ
−
f s
( , )
τ
−
f
∆( , )( ( )
t
τ σ
t
−
s
) |
≤
ε σ
| ( )
t
−
s
|
for alls
∈
U
wheref
∆ denotes the derivative off
with respect to the first variable. Then1.
( ) :=
t( , )
a
g t
∫
f t
τ τ
∆
implies ( ) = t ( , ) ( ( ), )a
g∆ t
∫
f∆ t τ τ∆ + f σ t t2.
( ) :=
b( , )
t
h t
∫
f t
τ τ
∆
implies ( ) = b ( , ) ( ( ), )t
h t∆
∫
f∆ t τ τ∆ − f σ t t .For more basic concepts in the time scale theory the readers are referred to the books (see [1, 2]).
2. EXISTENCE AND NON-EXISTENCE OF SOLUTIONS IN
M
+,M
−,OS
ANDWOS
First, we examine the existence of solutions of equation (1) in the class
M
+.Theorem 2.1: Assume that
( )
H
1b
(
t
)
,c
(
t
)
are non negative and non-decreasing;( )
H2p
(
t
)
is non positive andq
(
t
)
is non negative for t∈[t , ) ;0 ∞T( )
H3 there existsM
1>
0
such that 1( )
( )
f u M g u
≤ for
u
≠
0;
( )
H4g
is non-decreasing and( )
H5 10
( ( ) ( )) = limsupt t
t M p s q s s
→∞
∫
+ ∆ ∞ hold. Then for equation (1), we haveM
= .
ϕ
+
Proof: Suppose that the equation (1) has a solution
x
∈
M
+. Without loss of generality, we may assume thatx t
( ) > 0
and
x
∆(
t
)
≥
0
for large t∈[t , )0 ∞ T (the proof is similar ifx
(
t
)
<
0
andx
∆(
t
)
≤
0
for large t∈[t , )0 ∞ T). Thenthere exists t1∈[t , )0 ∞T such that
x
(
t
)
,x
(
α
(
t
))
,x
(
γ
(
t
))
all are positive andx
∆(
t
)
,x
∆(
α
(
t
))
,x
∆(
γ
(
t
))
all are non-negative for all t∈[t , )1 ∞ T.Define,
))
(
(
)
(
))
(
(
)
(
)
(
=
)
(
t
x
t
b
t
x
t
c
t
x
t
z
+
α
+
β
(2.1)Using (2.1), equation (1) becomes
0
=
)))
(
(
(
)
(
)))
(
(
(
)
(
))
(
)
(
(
a
t
z
∆t
∆+
p
t
f
x
γ
t
+
q
t
g
x
δ
t
or
)
(
)))
(
(
(
)))
(
(
(
)
(
=
)))
(
(
(
))
(
)
(
(
t
q
t
x
g
t
x
f
t
p
t
x
g
t
z
t
a
∆ ∆−
−
δ
γ
δ
for t∈[t , )1 ∞T. (2.2)Now for t∈[t , )1 ∞ T,
a(t)z (t) (a(t)z (t)) =
g(x( (t))) g(x( (t)))
∆
∆ ∆ ∆
δ δ
1 (a( (t))z ( (t)))
g(x( (t))) ∆
∆
+ σ σ
δ
( ( )
( ))
( ( ( ( ))))
=
( ( ( ))
( ( )))
,
( ( ( )))
( ( ( ))) ( ( ( )))
a t z t
g x
t
a
t z
t
g x
t
g
σx
t
g x
t
δ
σ
σ
δ
δ
δ
∆ ∆ ∆
∆
−
implies that,
a(t)z (t) (a(t)z (t)) =
g(x( (t))) g(x( (t)))
∆
∆ ∆ ∆
−
δ δ
(a( (t))z ( (t)))
∆
σ σ
1 ' 0
{ g (x( (t)) h (t)(x( (t))) )dh}(x( (t)))
g (x( (t)))g(x( (t)))
∆ ∆
σ
δ + µ δ δ
δ δ
∫
or( )
( )
( ( )
( ))
=
( ( ( )))
( ( ( )))
a t z t
a t z t
g x
δ
t
g x
δ
t
∆
∆ ∆ ∆
−
(a( (t))z ( (t)))∆
σ σ
1 ' 0
{ g (x( (t)) h (t)(x( (t))) )dh}x ( (t)) (t)
g (x( (t)))g(x( (t)))
∆ ∆ ∆
σ
δ + µ δ δ δ
δ δ
∫
(2.3) Therefore,( )
( )
( ( )
( ))
( ( ( )))
( ( ( )))
a t z t
a t z t
g x
δ
t
g x
δ
t
∆ ∆ ∆ ∆
≤
(2.4)for all t∈[t , )1 ∞ T, due to
( )
H
4 ,z
∆(
t
)
≥
0
andx
∆(
δ
(
t
))
≥
0
for all t∈[t , )1 ∞ T. From (2.2) and (2.4), we have( )
( )
( ( ( )))
( )
( )
( ( ( )))
( ( ( )))
a t z t
f x
t
p t
q t
g x
t
g x
t
γ
δ
δ
∆ ∆
≤ −
−
)
(
)))
(
(
(
)))
(
(
(
)
(
q
t
t
x
g
t
x
f
t
p
−
−
≤
γ
γ
≤
−
(
M
1p
(
t
)
+
q
(
t
))
for t∈[t , )1 ∞T, due to
( )
H
2 -( )
H
4 . Integrating the last inequality fromt
1 tot
, we obtain.
))
(
)
(
(
)))
(
(
(
)
(
)
(
)))
(
(
(
)
(
)
(
1 1 1 11
M
p
s
q
s
s
t
x
g
t
z
t
a
t
x
g
t
z
t
a
tt
+
∆
−
≤
−
∆∫
∆δ
δ
From
( )
H
5 , we obtain,
=
)))
(
(
(
)
(
)
(
liminf
−∞
∆ ∞→
g
x
t
t
z
t
a
t
δ
which contradicts the assumption
z t
∆( )
≥
0
for larget
. Thus, the theorem is proved.Example 2.2: In Theorem 2.1, the assumption
( )
H
5 cannot be dropped. For this, suppose T = R, and consider thefollowing differential equation
' ' 2
1 1
(x(t) (3t 1)x(t 1)) 2(2t 5)x(t )) 2 t + + − + − + 3 3 3 ( 18)
x (t 2)
t (t 2)
− + − −
0,
=
3)
5)
(
5)(
(
28)
10
5)(
(
14
2 22
+
+
+
+
+
+
+
x
t
x
t
t
t
t
t
(2.5)3
≥
t
. For this differential equation, all assumptions of Theorem 2.1 hold, but( )
H
5 is violated. The equation (2.5) has© 2018, IJMA. All Rights Reserved 288
Theorem 2.3: Assume that condition
( )
H
1 and( )
H
6p
(
t
)
is non negative andq
(
t
)
is non positive for t∈[t , )0 ∞T;( )
H
7 there existsM
2>
0
such that 2( )
|
|
( )
g u
M
f u
≤
foru
≠
0;
( )
H
8f
is non-decreasing;( )
H
9 20
( ( )
( ))
=
limsup
t tt
p s
M q s
s
→∞
∫
+
∆
∞
, hold. Then for equation (1), we haveM
= .
ϕ
+
Proof: Suppose that the equation (1) has a solution
x
∈
M
+. Without loss of generality, we may assume that( ) > 0
x t
andx t
∆( )
≥
0
for large t∈[t , )0 ∞ T (the proof is similar ifx t
( ) < 0
andx
∆(
t
)
≤
0
for large t∈[t , )0 ∞T). Then there exists t1∈[t , )0 ∞T such thatx
(
t
)
,x
(
α
(
t
))
,x
(
γ
(
t
))
all are positive andx
∆(
t
)
,x
∆(
α
(
t
))
,x
∆(
γ
(
t
))
all are non-negative for all t∈[t , )1 ∞ T.Define
z
(
t
)
as in Theorem 2.1, and from( )
H
1 , we getz
(
t
)
>
0
andz
∆(
t
)
≥
0
for all t∈[t , ) .1 ∞T Using (2.1), equation (1) becomes0
=
)))
(
(
(
)
(
)))
(
(
(
)
(
))
(
)
(
(
a
t
z
∆t
∆+
p
t
f
x
γ
t
+
q
t
g
x
δ
t
or
)
(
)))
(
(
(
)))
(
(
(
)
(
=
)))
(
(
(
))
(
)
(
(
t
q
t
x
f
t
x
g
t
p
t
x
f
t
z
t
a
γ
δ
γ
−
−
∆ ∆
for t∈[t , )1 ∞ T (2.6)
Now for t∈[t , )1 ∞ T,
a(t)z (t) (a(t)z (t)) =
f (x( (t))) f (x( (t)))
∆
∆ ∆ ∆
γ γ
1
(a( (t))z ( (t)))( )
f (x( (t)))
∆ ∆
+ σ σ
γ
(a(t)z (t))
= (a( (t))z ( (t))) f (x( (t)))
∆ ∆
∆
− σ σ
γ
(f (x( (t)))) , f (x( (t)))f (x( (t)))
∆
σ
γ
γ γ
implies that,
a(t)z (t) (a(t)z (t)) =
f (x( (t))) f (x( (t)))
∆
∆ ∆ ∆
−
γ γ
(a( (t))z ( (t)))
∆
σ σ
1 ' 0
{ f (x( (t)) h (t)(x( (t))) )dh}(x( (t)))
f (x( (t)))f (x( (t)))
∆ ∆
σ
γ + µ γ γ
γ γ
∫
or
( )
( )
( ( )
( ))
=
( ( ( )))
( ( ( )))
a t z t
a t z t
f x
γ
t
f x
γ
t
∆
∆ ∆ ∆
−
(a( (t))z ( (t)))∆
σ σ
1 ' 0
{ f (x( (t)) h (t)(x( (t))) )dh}x ( (t)) (t)
f (x( (t)))f (x( (t)))
∆ ∆ ∆
σ
γ + µ γ γ γ
γ γ
∫
(2.7)
Therefore,
( )
( )
( ( )
( ))
( ( ( )))
( ( ( )))
a t z t
a t z t
f x
γ
t
f x
γ
t
∆
∆ ∆ ∆
≤
(2.8)
for all t∈[t , )1 ∞ T, due to (H8),
z
∆(
t
)
≥
0
andx
∆(
γ
(
t
))
≥
0
for all t∈[t , )1 ∞ T.From (2.6) and (2.8), we have
( )
( )
( ( ( )))
( )
( )
( ( ( )))
( ( ( )))
a t z t
g x
t
p t
q t
f x
t
f x
t
δ
β
γ
∆ ∆
≤ −
−
( ( ( )))
( )
( )
( ( ( )))
g x
t
p t
q t
f x
t
δ
δ
≤ −
−
≤
−
(
p
(
t
)
+
M
2q
(
t
))
1 1
2 1
1
( )
( )
( )
( )
( ( )
( ))
.
( ( ( )))
( ( ( )))
t
t
a t z t
a t z t
p s
M q s
s
f x
γ
t
f x
γ
t
∆ ∆
−
≤ −
∫
+
∆
From
( )
H
9 , we obtain( )
( )
=
,
liminf
( ( ( )))
t
a t z t
f x
γ
t
∆
→∞
−∞
which contradicts the assumption z t∆( )≥0 for large
t
. Thus, the theorem is proved.Example 2.4: Let T = R, and consider the following differential equation
2 2
1
( ( )
(
2 ) (
2)
(2
1) (
9))
3
8
' '
x t
t
t x t
t
x t
t
−
t
+
+
− +
−
+
3 2 2 3 2
12
x (t 1 / 2)(x (t 1 / 2) 1) t(3t 8) (t 1 / 2) (t t 5 / 4)
+ − − +
− − − + −
5 2 2 5
8
(5
6) = 0,
(3
t
−
8 ) (5
t
t
+
6)
x
t
+
(2.9)
1
≥
t
. For this differential equation, all assumptions of Theorem 2.3 hold, but( )
H
9 is violated. The equation (2.9) hasa solution
x
(
t
)
=
t
∈
M
+.
Theorem 2.5: Assume that conditions
( )
H
2 ,( )
H
3 ,( )
H
4 ,( )
H
5 and( )
H10−
1
<
b
(
t
)
+
c
(
t
)
≤
0
for t∈[t , )0 ∞T andc
(
t
)
is non negative;( )
H11M
1p
(
t
)
+
q
(
t
)
≥
0
for t∈[t , )0 ∞ T;( )
H120
1
=
( )
t
a t
t
∞
∆
∞
∫
hold. Then for equation (1), we haveM
+= .
ϕ
Proof: Suppose that the equation (1) has a solution x∈M+. Without loss of generality, we may assume that
x t
( ) > 0
and
x t
∆( )
≥
0
for large t∈[t , )0 ∞T (the proof is similar ifx
(
t
)
<
0
andx
∆(
t
)
≤
0
for large t∈[t , )0 ∞T). Then there exists t1∈[t , )0 ∞T such thatx
(
t
)
,x
(
α
(
t
))
,x
(
γ
(
t
))
all are positive andx t
∆( )
,x
∆( ( ))
α
t
,x
∆( ( ))
γ
t
all are non-negative for all t∈[t , )1 ∞T.Define
z
(
t
)
as in Theorem 2.1, we have))
(
(
)
(
))
(
(
)
(
)
(
=
)
(
t
x
t
b
t
x
t
c
t
x
t
z
+
α
+
β
≥
(1
+
b
(
t
)
+
c
(
t
))
x
(
α
(
t
))
>
0
for t∈[t , )1 ∞T. From (1), we have
)))
(
(
(
))
(
)))
(
(
(
)))
(
(
(
)
(
(
=
))
(
)
(
(
q
t
g
x
t
t
x
g
t
x
f
t
p
t
z
t
a
δ
δ
γ
+
−
∆ ∆
)))
(
(
(
))
(
)))
(
(
(
)))
(
(
(
)
(
(
q
t
g
x
t
t
x
g
t
x
f
t
p
δ
γ
γ
+
−
≤
≤
−
(
M
1p
(
t
)
+
q
(
t
))
g
(
x
(
δ
(
t
)))
≤
0,
for t∈[t , )1 ∞T.Hence,
a t z t
( )
∆( )
is non-increasing for t∈[t , )1 ∞T.We claim that,
a
(
t
)
z
∆(
t
)
≥
0
for t∈[t , )1 ∞ T.If
a
(
t
)
z
∆(
t
)
<
0
for t∈[t , )1 ∞T, thena
(
t
)
z
∆(
t
)
≤
a
(
t
1)
z
∆(
t
1)
or.
)
(
1
)
(
)
(
)
(
1 1t
a
t
z
t
a
t
© 2018, IJMA. All Rights Reserved 290
Integrating the above inequality from
t
1 tot
, we obtain.
)
(
1
)
(
)
(
)
(
)
(
1 1 1
1
s
s
a
t
z
t
a
t
z
t
z
tt
∆
≤
−
∆∫
This gives that
z
(
t
)
→
−∞
ast
→
∞
due to( )
H
12 , which is a contradiction toz t
( ) > 0
. Thusa t z t
( )
∆( )
≥
0
for1 T
t∈[t , )∞ . Now proceeding as in the proof of Theorem 2.1, and using
( )
H
11 , we get.
=
)))
(
(
(
)
(
)
(
lim
−∞
∆
∞
→
g
x
t
t
z
t
a
t
δ
This contradicts the fact that
z t
∆( )
≥
0
for large t. Hence, the theorem is proved.Example 2.6: Let T = hZ ,
h
is a ratio of odd positive integers, and consider the following h-difference equation2
1
2(
( ( )
(
2 )
(
2 )))
2
t h h
h
e
hx t
e x t
h
e
x t
h
−
∆
∆
−
−
+
+
3
2 12
2 2
1
1
(4
12 )
(
1)
(
) = 0,
2
2
h h
t h h t
e
e
e
x t
h
e
e x t
h
h
h
− +
+
+
−
−
+
+
+
(2.11)h
t
>
12
. For this difference equation, all assumptions of Theorem 2.5 hold, but( )
H
12 is violated. The equation(2.11) has a solution
x
(
t
)
=
e
t∈
M
+.
Theorem 2.7: Assume that conditions
( )
H
6 ,( )
H
7 ,( )
H
8 ,( )
H
9 ,( )
H
10 ,( )
H
12 and( )
H
13 .p
(
t
)
+
M
2q
(
t
)
≥
0
for t∈[t , )0 ∞ T hold. Then for equation (1), we have=
φ
.
+
M
Proof: The proof is similar to that of Theorem 2.5.
Next, we examine the problem of the existence of solutions of equation (1) in the class
M
−:
Theorem 2.8: Assume that
( )
H
6 ,( )
H
7 ,( )
H
8 and( )
H
14b
(
t
)
andc
(
t
)
are non-negative and non-increasing;( )
H
15f
(
uv
)
=
f
(
u
)
f
(
v
)
;( )
H
16γ
(
t
)
≤
α
(
t
)
;( )
H
17 the function)
(
1
u
f
is locally integrable on(0,
c
)
and(
−
c
,0)
for somec
>
0
,i.e.,
∫
<
∞
)
(
0
f
u
du
c
,
∫
−∞
−
(
)
>
0u
f
du
c
;
( )
H
18t t T
1 limsup
a(s)f (1 b(s) c(s))
→∞
∫
+ +(
)
s
2
T(p(v)+M q(v)) v∆ ∆s =∞
∫
fort
≥
T
.Then for equation (1), we have
M
−=
φ
.Proof: Suppose that equation (1) has a solution
x
∈
M
−. Without loss of generality, we may assume thatx
(
t
)
>
0
and
x
∆(
t
)
≤
0
for large t∈[t , )0 ∞ T (the proof is similar ifx
(
t
)
<
0
andx
∆(
t
)
≥
0
for large t∈[t , )0 ∞ T). Thenthere exists t1∈[t , )0 ∞T such that
x
(
t
)
,x
(
α
(
t
))
,x
(
γ
(
t
))
all are positive andx
∆(
t
)
,x
∆(
α
(
t
))
,x
∆(
γ
(
t
))
allare non-positive for all t∈[t , )1 ∞ T. Define
z
(
t
)
as in Theorem 2.1 and using( )
H
14 , we see thatz
(
t
)
>
0
and0
)
(
≤
∆
t
As in the proof of Theorem 2.3, we obtain
s
s
q
M
s
p
t
x
f
t
z
t
a
t
x
f
t
z
t
a
tt
+
∆
−
−
∆∫
∆))
(
)
(
(
=
)))
(
(
(
)
(
)
(
)))
(
(
(
)
(
)
(
2 1 1 1 1γ
γ
ors
s
q
M
s
p
t
x
f
t
z
t
a
tt
+
∆
−
≤
∫
∆))
(
)
(
(
)))
(
(
(
)
(
)
(
2 1γ
ors
s
q
M
s
p
t
a
t
x
f
t
z
tt
+
∆
−
≤
∫
∆))
(
)
(
(
)
(
1
)))
(
(
(
)
(
2 1γ
for t∈[t , )1 ∞T. (2.12)We see that
z
(
t
)
≤
(1
+
b
(
t
)
+
c
(
t
))
x
(
γ
(
t
))
. Sincex
is non-increasing and from( )
H
15 , we see that)))
(
(
(
))
(
)
(
(1
))
(
(
z
t
f
b
t
c
t
f
x
t
f
≤
+
+
γ
(2.13)Combining (2.12) and (2.13), we obtain
)))
(
(
(
))
(
)
(
(1
)
(
))
(
(
)
(
t
x
f
t
c
t
b
f
t
z
t
z
f
t
z
γ
+
+
≤
∆ ∆.
))
(
)
(
(
))
(
)
(
(1
)
(
1
2 1s
s
q
M
s
p
t
c
t
b
f
t
a
tt
+
∆
+
+
−
≤
∫
Integrating from
t
1 tot
, we obtainz( t ) z( t )1
s f (s)
∆
−
∫
t s2 t1 t1
1
( (p(v) M q(v)) v) s
a(s)f (1 b(s) c(s))
≤ − + ∆ ∆
+ +
∫
∫
or
z( t ) 1 z( t )
s f (s)
∆ ≥
∫
t s2 t1 t1
1
( (p(v) M q(v)) v) s
a(s)f (1 b(s) c(s))+ + + ∆ ∆
∫
∫
Using
( )
H
18 , we obtain,
=
)
(
limsup
(1))
(
∞
∆
∫
∞
→
f
s
s
t z t z twhich is a contradiction to
( )
H
17 . Hence, the theorem is proved.Theorem 2.9: Assume that
( )
H
2 ,( )
H
3 ,( )
H
4 ,( )
H
5 ,( )
H
11 ,( )
H
12 and( )
H
19b
,c
are non negative constants,( )
H
20f
is nonincreasing hold.Then every solution of equation (1) is either oscillatory or weakly oscillatory.
Proof: From Theorem 2.1, it follows that for equation (1), we have
M
+=
ϕ
. To complete the proof, it suffices toshow that for equation (1),
M
−=
φ
. Letx
∈
M
−, thenx
(
t
)
>
0
andx
∆(
t
)
≤
0
for t∈[t , )1 ∞T. Definez
(
t
)
asin Theorem 2.1, we have
z
(
t
)
>
0
andz
∆(
t
)
≤
0
for t∈[t , )1 ∞T due to (H19). Using (2.1), equation (1) becomes( ( )
a t z t
∆( )) =
∆−
p t f x
( ) ( ( ( )))
γ
t
−
q t g x
( ) ( ( ( )))
δ
t
( ( ( )))
=
( )
( )) ( ( ( ))
( ( ( )))
f x
t
p t
q t g x
t
g x
t
γ
δ
δ
−
−
( ( ( )))
(
( )
( )) ( ( ( )))
( ( ( )))
f x
t
p t
q t g x
t
g x
t
δ
δ
γ
≤ −
−
© 2018, IJMA. All Rights Reserved 292
Hence,
( ( )
a t z t
∆( ))
∆≤
0
for t∈[t , )1 ∞ T, due to (H11).This implies that,
a
(
t
)
z
∆(
t
)
is nonincreasing for t∈[t , )1 ∞ T. Then there exists k(< 0)∈R and t2∈[t , )1 ∞T such thatk
t
z
t
a
(
)
∆(
)
≤
or
)
(
1
)
(
t
a
k
t
z
∆≤
Integrating the above inequality from
t
2 tot
, we obtain.
)
(
1
)
(
)
(
2
2
s
s
a
k
t
z
t
z
tt
∆
≤
−
∫
This implies that
z
(
t
)
→
−∞
ast
→
∞
. Which gives a contradiction toz
(
t
)
>
0
.Hence, the theorem is proved.
Theorem 2.10: Assume that
( )
H
6 ,( )
H
7 ,( )
H
8 ,( )
H
12 ,( )
H
13 ,( )
H
19 and( )
H
21g
is nonincreasing hold.Then every solution of equation (1) is either oscillatory or weakly oscillatory.
Proof: The proof is similar to that of Theorem 2.9 and hence complete the proof.
Remark 2.11: In Theorem 2.9 and Theorem 2.10, we used
f
is nonincreasing andg
is nondecreasing respectively.In this cases
f
andg
are defined on R {0}− only.
3. BEHAVIOR OF SOLUTIONS IN
M
+ ANDM
−
Theorem 3.1: Assume that
( )
H
6 ,( )
H
7 ,( )
H
8 ,( )
H
14 ,( )
H
15 ,( )
H
16 and( )
H
18 hold. Then every solution −∈
M
t
x
(
)
, we havelim
t→∞x
(
t
)
=
0.
Proof: The argument used in the proof of Theorem 2.8, again leads that
.
=
)
(
1
limsup
(1))
(
∆
∞
∫
∞ →
s
s
f
t z
t z t
This implies that,
lim
t→∞z
(
t
)
=
0
. Butz
(
t
)
>
x
(
t
)
for all t∈[t , )1 ∞ T.This shows that
lim
t→∞x
(
t
)
=
0.
Hence complete the proof of the theorem.Theorem 3.2: Assume that
( )
H
1 ,( )
H
2 ,( )
H
3 ,( )
H
4 ,( )
H
11 and( )
H
221
+
b
(
t
)
+
c
(
t
)
is bounded,( )
H
23 →∞∫
+
∫
∆
)
∆
=
∞
)
(
1
(
))(
(
)
(
(
limsup
1v
s
v
a
s
q
s
p
M
sT t
T
t for all
T
≥
t
0 hold.Then every solution of (1) in the class
M
+ is unbounded.Proof: Let
x
be a solution of (1) such thatx
∈
M
+. Proceeding as in the proof of Theorem 2.1, by definingz
(
t
)
asin (2.1), we have
z
(
t
)
>
0
,z
∆(
t
)
≥
0
for allt
∈
[
t
1,
∞
)
due to( )
H
1 . Then from (1), we obtain (2.2). Consider thefunction
1
( )
( )
1
( ) =
,
( ( ( )))
( )
t
t
a t z t
w t
s
g x
δ
t
a s
∆
we have,
t t1
1 1
w (t) = (a(t)z (t)) s
g(x( (t))) a(s)
∆ − ∆ ∆ ∆ −
δ
∫
t t1
1 1
(a( (t))z ( (t))) s
g(x( (t))) a(s) ∆
∆
σ σ ∆
δ
∫
f (x( (t))) = (p(t)
g(x( (t)))
γ δ
t t
t1 t1
1 1 1
q(t)) s (a( (t))z ( (t)) s
a(s) g(x( (t))) a(s)
∆
∆
+ ∆ − σ σ ∆
δ
∫
∫
( t ) t1
1 1
(a( (t))z ( (t)) s ,
a(s) g(x( (t)))
∆ σ
∆
− σ σ ∆
δ
∫
implies that 1 t t1 1w (t) (M p(t) q(t)) s
a(s) ∆ ≥ + ∆ −
∫
1 (a(t)z (t)) a(t)g(x( (t))) ∆ − δ
( t ) t1
1 1
(a( (t))z ( (t)) s
a(s) g(x( (t)))
∆ σ
∆
σ σ ∆
δ
∫
+
−
∆
+
∫
∆)))
(
(
(
)
(
)
(
1
))
(
)
(
(
=
1 1t
x
g
t
z
s
s
a
t
q
t
p
M
t tδ
( t ) t1
1 1
a( (t))z ( (t))) s
a(s) g(x( (t)))
∆ σ
∆
σ σ ∆
δ
∫
1
1
1
( )
(
( )
( ))
.
( )
( ( ( )))
t
t
z t
M p t
q t
s
a s
g x
δ
t
∆
≥
+
∫
∆ −
Integrating the above inequality from
t
1 tot
, we get1 1 1
1
( )
( )
(
( )
( ))
.
( )
( ( ( )))
t s t
t t t
z
s
w t
Mp s
q s
s
s
a
τ
τ
g x
δ
s
∆
≥
∫
+
∫
∆ ∆ −
∫
∆
(3.14)As the function
( )
( ( ( )))
z t
g x
δ
t
∆
is positive for t∈[t , )1 ∞T, then
1
( )
lim
( ( ( )))
t t tz
s
s
g x
δ
s
∆ →∞
∫
∆
exists. Assume that 1( )
=
<
.
lim
( ( ( )))
t t tz
s
s
k
g x
δ
s
∆
→∞
∫
∆
∞
Taking into account (H23), and from (3.14) we get,
=
)
(
limsup
∞
∞ →t
w
twhich gives a contradiction, because
w
is negative for all t∈[t , )1 ∞ T. Thus,.
=
)))
(
(
(
)
(
lim
1∞
∆
∆ ∞→
∫
g
x
s
s
s
z
t t tδ
(3.15) Consequently, 1 1 1( )
1
( )
lim
( ( ( )))
( ( ( )))
t t t t tz
s
s
z
s
s
g x
δ
s
g x
δ
t
∆ ∆ →∞
∆ ≤
∆
∫
∫
)).
(
)
(
(
)))
(
(
(
1
=
1 1t
z
t
z
t
x
g
δ
−
From (3.15), we get
.
=
)
(
lim
∞
∞ →z
t
t
(3.16)
Since
z
(
t
)
=
x
(
t
)
+
b
(
t
)
x
(
α
(
t
))
+
c
(
t
)
x
(
β
(
t
))
andx
is non-negative, we have).
(
))
(
(1
)
(
t
p
t
x
t
z
≤
+
Thus from (3.16), we have
.
=
)
(
lim
∞
∞ →x
t
t
This completes the proof of the theorem.
© 2018, IJMA. All Rights Reserved 294
Remark 3.3: In this paper we obtained conditions for the non-existence of solutions in the classes
M
+,M
− and theexistence of solutions in the classes OS and WOS. It would be interesting to extend the results of this paper to the following equation
(a(t)(x(t) b(t)x( (t)) c(t)x( (t))) )+ α + β ∆ ∆+p(t)f (x( (t)))γ +q(t)g(x( (t))) = r(t)δ for t∈[t , )0 ∞ T
where
r
(
t
)
is a rd-continuous function.REFERENCES
1. M. Bohner, and A. Peterson, Dynamic Equations on Time Scales: An Introduction With Applications, Birkhäuser, Boston, 2001.
2. M. Bohner, and A. Peterson, Advances in Dynamic Equations on Time Scales, Birkhäuser, Boston, 2003. 3. S. Hilger, Analysis on measure chains: a unified approach to continuousand discrete calculus, Results. Math.
18 (1990), 18–56.
4. S. Panigrahi, J. R. Graef and P. R. Reddy, Oscillation Results for fourth order nonlinear neutral dynamic equations, Commu. Math. Anal., 15 (2013), 11–28.
5. J. R. Graef, S. Panigrahi, and P. Rami Reddy, On oscillatory and asymptotic behavior of fourth order nonlinear neutral delay dynamic equations with positive and negative coefficients, Math. Slovaca, 64 (2014), No. 2, 347–366.
6. E. Thandapani, S. Padmavathi, and S. Pinelas, Classifications of solutions of second-order nonlinear neutral differential equations of mixed type, Advances in Difference Equations, 226 (2012), (1-13).
7. M. Cecchi, and M. Marini, Oscillatory and non-oscillatory behavior of a second order functional differential equation, Rocky Mountain Journal of Mathematics 22 (1992) No. 4, 1259–1276.
8. R. P. Agarwal, M. M. S. Manuel, and E. Thandapani, Oscillatory and non-oscillatory behavior of second order neutral delay difference equations, Math. Comput. Modelling 24 (1996) No. 1. 5–11.
9. Sabah Hafez Abdallah, Oscillatory and non-oscillatory behavior of second order neutral delay differential equations, Appl. Math. Comput. 135 (2003) 333–344.
10. P. Rami Reddy, N. Sikender, and M. V. Krishna, Classification of solutions of second order neutral delay dynamic equations IOSR Jornal of Mathematics (IOSR - JM), e-ISSN: 2278-5728, p-ISSN: 2319-765X. Volume 12, Issue 5 Ver. I (Sep. - Oct.2016), 72-81.
11. N. Sikender, M. V. Krishna, and P. Rami Reddy Classification of solutions of second order neutral delay dynamic equations with positive and negative coefficients International Jornal of Mathematics Trends and Technology (IJMTT), e-ISSN: 2278-5728, Volume 37, Number I- September 2016, 20-28.
12. E. Boe, H. C. Chang, Dynamics of delayed systems under feedback control, Chem. Eng. Sci. 44 (1989), 1281-1294.
13. R. D. Driver, A mixed neutral systems, Nonlinear Analysis; Theory Methods and Applications (1984), 155-158.
14. J. K. Hale, Theory of Functional Differential Equations, Springer-Verlag, New York,1977 15. E. P. Popov, Automatic regulation and Control, Nauka Mascow (in Russian), 1966.
16. Da-Xue Chen, Pei-Xin Qu, Yong-Hong Lan, Oscillation of second-order nonlinear dynamic equations with positive and negative coefficients, Advances in Difference Equations 2013, 2013:168.
17. S.Padhi, Oscillation and asymptotic behavior of solutions of second order neutral differential equation with positive and negative coefficients, Fasc. Math., 38 (2007), 105-111.
18. S. Padhi, Oscillation and asymptotic behavior of solutions of second order homogeneous neutral differential equations with positive and negative coefficients, Funct. Differ. Equ. 14 (2007), 363-371.
19. E. Thandapani, V. Muthulakshmi, John R. Graef, Classification of solutions of second order nonlinear neutral delay differential equations with positive and negative coefficients, International J. Pure Appl. Math. 64 No. (2010), 159-170.
Source of support: Nil, Conflict of interest: None Declared.