Journal
of
Applied Mathematics and Stochastic Analysis, 11:2(1998),
193-208.OSCILLATION CRITERIA FOR HIGH ORDER DELAY PARTIAL DIFFERENTIAL EQUATIONS
1XINZHI LIU and XILIN FU
2University
of Waterloo, Department of
Applied MathematicsWaterloo, Ontario,
Canada N2L 3G1(Received October, 1996;
RevisedJanuary, 1997)
This paper studies a class ofhighorder delay partial differential equations.
Employing high order delay differential inequalities, several oscillation cri- teria are established for such equations subject to two different boundary conditions.
Two
examples arealso given.Key
words:Oscillation,
Higher Order Delay Partial DifferentialEqua-
tions, Differential Inequality, Eventual Positive Solutions.AMS
subjectclassifications: 35B05. 34L40.1. Introduction
The oscillation theory of delay differential equations has been studied by numerous authors and the number of papers published in this area is enormous. For an ex- cellent exposition of the basic theory, see
[5]. In
recent years, there has been an in- creasing interest in oscillation theory ofdelay partial differential equations, see[6-10]
and references therein.
However,
the corresponding theory is still in its initialstage
of development.In
this paper, weshall investigate a class ofhigh order delay partial differential equations which will bedescribed in Section 2.In
Section3,
weshall esta- blish several oscillation criteria for high order delay partialdifferential equations sub- ject to two kinds ofboundaryconditions,
employingGreen’s
theorem and high order delay differential inequalities.We
then develop, in Section4,
some results on even- tual positive and eventual negative solutions of high order differential inequalities, which enable us, in addition to their independent interests, to obtain in Section5,
further oscillation criteria for high order delay partial differential equations.To
illu- strateourresults,
two examples are also given.1Research
supported by NSERC-Canada.2On
leave fromShandong
Normal University, Jinan, Shandong250014, PR
China.Printed in the U.S.A.()1998by North Atlantic SciencePublishingCompany 193
2. Prehminaries
We
shall consider the following nonlinear high order delay partial differential equationff-m[u + A(t)u(x, v)] + p(x, t)u + q(x, t)f(u(x,
tr))
= a(t)Au + E aj(t)Au(x, aj(t)),(x,t)e x R+ G, (2.1)
j=l
where m is an even positive integer,
" >
0 and a>
0 are constants.Let
fl be abounded domain in
R
n with piecewise boundaryOF/,
A is the Laplacian inRn;
A
Ecm[R + ,R];
a, ajC[R + ,R + ],
j1, 2,..., ;
p,qC[R +
x,R + ], f C[R, R],
rjC[R
+,R +
is nondecreasing int, rj(t) <
t and limr(t) +
cx3,j
1, 2,..., .
t--.+
We
shall consider two kinds ofboundaryconditionsOu )u o, (, ) e O R +
and
ON t- 7(x’ (B1)
0, (, ) e 0e a
+,(B)
where
N
is the unit exterior normal vector to0, 7(x, t)
is anonnegative continuous functionon c3 xR +.
Definition 2.1: The solution
u(x,t)
of system(2.1)
satisfying certain boundaryconditions is called oscillatory in the domain
G
if for each positive number #, there exists apoint(Xo, to)
2 xlit, + cx)
such thatU(Xo, to) O.
3. Oscillation Criteria
In
this section we shall establish oscillation criteria for problem(2.1)
with boundarycondition
(B1)
and(B2)
separately. The basic idea ofour approach is to reduce the study of high order delay partial differential equations to that of high order delay differential inequalities.Theorem 3.1:
Assume
that the following condition(H)
holds.(H) f(u)
is convex inR +
andf( u) = f(u) < O,
uER + If
the high order delaydifferential
inequalitiesd--t-[U(t
d,+ (t)U(t r)] + P(t)U(t) + Q(t)f(U(t o’)) _<
0(3.1)
has no eventually positivesolutions,
then all solutionsof
the problem(2.1)
under(B1)
are oscillatory in
G,
whereP(t)
min_p(x, t), Q(t)
min_q(x, t).
xEfl xEfl
Proof:
Let u(x,t)
be a nonoscillatory solution of the problem(2.1)
under(B1).
We
may assume thatu(x,t)>
0 for(x,t)E x[it, +x),
where it is a positive number to>
it, such thatand
(,
t-) > 0, (,
t) >
0u(x,rj(t)) > O, (x,t) e ]x[t
o,+oo),
j- 1,2,...,g.Oscillation Criteria
for
High Order DelayPDEs
195Integrating both sides ofsystem
(2.1)
with respectto x over thedomainf2,
weobtaindm u(x, t)dx + a(t) u(x
tr)dx + p(x, t)u(x t)dx
dtm
+ J q(x, t)f(u(x,
tr))dx
a(t)/Au(x, t)dx + E aj(t)J Au(x,
aj(t))dx,
t_
t0.t j=l Ft
From Green’s Theorem,
itfollows thatand
/ /
-/7(,j(t))(,y(t))d8 <_ o,
j-1,2,...,t,
t>_ to,
o
(3.3)
(3.4)
where dS is the surface integral element on
0ft.
using
Jensen’s
inequality, we haveSince
if(u)
is convex inR
+, thenf (u(x,
t)dx _ all [o1 u(x,
t)dx (3.)
where
a] f
dx. Combining(3.2)-(3.5)
yields+ P(t) u(x,t)dx + Q(t)f a
_ a(t) / 7(x, t)u(x, t)dS E.aj(t) / 7(x, j(t))u(x, aj(t))dS
<_O, t>_t
o.Thus,
we see that thefunction1
/ u(x t)dx
u(t) al (3.6)
is a positive solution ofthe inequality
(3.1)
for t_> to,
which contradicts the condition of the theorem.If
u(x, t) <
0 for(x, t) [#, + c),
then set(., t) (., t), (., t) [, + ).
Note
that sincef(-u)= -f(u),
uE(0, + c),
it is easy to check that(x,t)is
apositive solution of the problem
(2.1)
under(B1)
which is impossible. This com- pletes the proofofTheorem 3.1.The following fact will be used in the proof of Theorem3.2. Consider the Dirich- let problem
Au+u-0 in
,
ulo-O,
where
,-
constant.It
is well known that the smallest eigenvalue0
and the cor-responding eigenfunction
(x)
are positive.Theorem 3.2:
Assume
that the condition(H)
holds.If
the high order delaydifferential
inequalitydm [V(t) + A(t)V(t v)] + (A0a(t) + P(t))V(t) + Q(t)f(V(t r)) <
0(3.7)
dtm
has no eventually positive
solutions,
then all solutionsof
the problem(2.1)
underare oscillatory in
G.
Proof:
Let u(x,t)
be a solution of the problem(2.1)
under(B2)
having no zerosin the domain
fix[#, +c),
for some#>0. Ifu(x,t)>0
for(x,t) EFt[#,+cx3),
then there exists a to
>
tt such thatu(x,
tr) > O, u(x,
tr) >
0 andu(x, aj(t)) > 0, (x, t)
flx[to, +
j
1,2,...,t.
Multiplying both sides of
(2.1)
by theeigenfunction(I)(x)
and integrating withrespect to x over the domainfl,
we havedrn
+ I p(x, t)u(x, t)qP(x)dx + / q(x, t)f(u(x,
t(r))O(x)dx
a(t)J Au(x, t)(x)dx + E aj(t)] Au(x,rj(t))(x)dx,
t>
tO.(3.8)
fl 3--1
Using
Green’s Theorem,
we obtainAu(x, t) ((x)dx
Oscillation Criteria
for
High OrderDelayPDEs
197= / (3.9)
Au(x, crj(t)). (b(x)dx
o i u(x, rj(t))(b(x)dx,
j1, 2,..., . (3.10)
Using
Jensen’s
inequality, wehavef(u(x,
tcr))O(x)dx
>_ (x)dx. f
f ((x)dx
Combining
(3.8)-(3.10)
yields(3.11)
- Ja(t) i u(x, t)((x)dx,
t>_ to,
i.e.,
the inequality(3.7)
has positive solutionf
] u(x, t)((x)dx,
t>_ to, v(t) r
J((x)dx
which contradictsthe condition of the theorem.
If
u(x, t) <
0 for(x, t)
E x[#, + oc),
then -u is a positive solution of the problem(2.1)
under(B2)
which also provides a contradiction. The proof of Theorem 3.2 iscomplete.4. High Order Delay Differential Inequalities
From
the discussion in Section 3 it followsthat the problem ofestablishingoscillation criteria for the system(2.1)
can be reduced to the investigation of the properties of the solution ofhigh order delay differential inequalitiesfor the form-m[y(t)
m+ (t)y(t 7")] + Q(t)f(y(t or)) <_ O,
t>_ to, (4.1)
and dm
d--[y(t + (t)y(t 7")] + Q(t)f(y(t r)) O,
t>_
to.(4.2)
Along
with(4.1)
and(4.2),
we consider the high orderdelay differentialequation dTMdtm[y(t + (t)y(t ’)] + Q(t)f(y(t )) o,
t>_ to, (4.3)
where m is an even positive integer,
" >
0 and r>
0 areconstants;
cm[[to,+ c), R], Q C[[,
0,+ ), R +
fo om*o > 0, f e C[R, R]. We
hfirst consider thecase
A(t) >_
0.Assume
thaty(t)
isa nonoscillatory solution of equation(4.3). Let z(t) y(t) + A(t)y(t-
We
shall usethe following lemma.Lemma
4.1"If z(t)
isof definite
sign and not identically zerofor
all sufficiently large t; there exist aT >_
to and an integerk,
O<_
k<_
m, with rn+
k evenfor
z(t)z(m)(t) >_ O,
orrn+
k oddfor z(t)z(m)(t) <_ O,
thenz(t)z(i)(t) >
0 on[r, + c) for
0< <_ k,
(- 1)
i-kz(t)z(i)(t) >
0 on[7", + oc) for
k<_ <_
m.Theorem4.1-
Assume
thatf(- y) f(y) for
yR
+, and that0
_< A(t) <_ 1, Q(t) >_ O,
t>_ to; (4.4) f(Y)
y>
e constant> O,
y(0, + oz) (4.5) If
Q(s)[1 A(s cr)]ds +
cx,(4.6)
then
(i)
the inequality(4.1)
has no eventuallypositivesolutions;
(ii)
the inequality(4.2)
has no eventually negative solutions; and(iii)
all solutionsof
the equation(4.3)
are oscillatory.Proof:
Let y(t)
be an eventually positive solution of the inequality(4.1). Then,
there exists at > to,
such thaty(t) > 0, y(t- r) >
0 andy(t- r) >
0 for all t>_
t1.Setting
z(t) y(t)+ A(t)y(t- 7-),
t>_ tl, (4.7)
wehave
z(t) > O,
t>_
t1.From (4.1), (4.4)
and(4.5)it
follows thatOscillation Criteria
for
High OrderDelay PDEs
199z(rn)(t) <_ -Q(t)f(y(t- r)) <_ -eQ(t)y(t- or) <_ O,
t>_
t1.Thus,
it follows fromLemma 4.1,
that there exists an odd number k and a t2_
t1such that
z()(t) > o, o <_ <_ ,
t>_ t
and
(-1) i-kz(i)(t)>0,
k< <_
m, t>_
t2.It
is easyto see thatz’(t) > O,
z(m-1)(t) > 0,
t_
t2.(4.8)
Using
(4.5)and (4.7),
we have0
>_ z(m)(t) + Q(t)f(y(t
>_ z(rn)(t) + Q(t) y(t
z(m)(t) + eQ(t)[z(t r) A(t r)y(t
vr)],
t_>
t2.Note z(t) >_ y(t)
for t>_ t2,
thus weobtain0
>_ z(m)(t) + eQ(t)[z(t r) A(t r)z(t
rr)],
t>_
t2.Since
z(t)
is increasing for t>_ t2,
we havez(m)(t) + eQ(t)[1 (t a)]z(t a) _< O,
t>_
t2.(4.9)
Integrating both sides of
(4.9)
from t2 tot(t > t2)
weget
z(m
1)(t) _
z(m1)(t2) ez(t
2r) J Q(s)[1 A(s r)]ds.
2
Since z(m-
a)(t) >
0 for t_> t2,
the above inequality leads to a contradiction in view of(4.6).
This proves assertion(i).
Assertion
(it)
follows from the fact that ify(t)
is an eventually negative solution of(4.2),
theny(t)
is an eventually positivesolution of(4.1).
Theproofoftheasser-tion
(iii)
is obvious.Theorem4.2:
Assume
that condition(4.4) holds; f(- y) f(y) > O,
y ER
+, and thatf(y)
is a monotone increasingfunction
inR +. If for
any c> O,
Q(s)f([1 A(s r)]c)ds +
oc,(4.10)
then conclusions
(i)-(iii) of
Theorem 4.1 remain true.Proof:
Let y(t)
be an eventually positive solution of inequality(4.1).
there exists a tI
>
to suchthatThen,
y(t) > 0, y(t-r) >
0 andy(t-r) >
0 for all t_> ta.
The following inequalities can be proved by the
analogous arguments
as in the proof of Theorem 4.1:z(m)(t) O,
t1;
z’(t) >0,
z(m-l)>0,
t>_t
2>_tl,
with
z(t)
defined by(4.7). We
havez(t) >
0 for t>_
tI andz(t- r) < z(t) < y(t) + (t)z(t- r),
t>_ t2,
[1- (t)]z(t- r) <_ y(t),
t>_
t2.Choose a
t* >
t2 such thatz(t-r) > O, t>_t*.
Since
f(y)
isincreasing, we obtain0
>_ z(m)(t) + Q(t)f(y(t o)
>_ z(m)(t) + Q(t)f[(1 i(t er)]z(t
rer)),
t_> t*.
Note
that sincez(t*-v- r) < z(t- t-r)
for t> t*,
wehavez(m)(t) + Q(t)f([1 A(t r)]c) _< O,
t>_ t*,
where c
z(t*-r- r) > O.
Integrating the above inequality fromt*
tot(t > t*),
weget
z(m z(ra
1)(t*) + / Q(s)f([1 A(s r)]c)ds <_ O.
t*
This leads to a contradiction in view of
(4.10),
since z(m-1)(t) >
0 for t>_
t2. Thisproves the assertion
(i).
We
can prove assertion(ii)
and(iii)
by the samearguments
as in the proof of Theorem 4.1. This completes the proof.Theorem 4.3:
Assume
thatf(- y) -f(y) .for
yER+
and that(4.4)
and(4.5)
hold.
If
there exists a monotonically increasingfunction cl[[t0, + oo), (0, + oo)]
such that
+oo
[e(s)Q(s)(1 (s-r))-c’(s)]ds +oo (4.11)
for
any numberc> O,
then conclusions(i)-(iii) of
Theorem 4.1 remain true.Proof:
Let y(t)
be an eventually positive solution of the inequality(4.1). Then,
there exists a tI>_
to such thaty(t) > O, y(t- r) >
O andy(t-er) >
O for all t>_
t1.The following inequalities can be proved by the
analogous arguments
as in the proofOscillation Criteria
for
High Order DelayPDEs
201 ofTheorem 4.1:z(t) > o, z(’)(t) _< o,
Z’(t) > O,
Z(m-1)(t) > O,
t_
t2_ tl;
z(m)(t) + eQ(t)[1 A(t a)]z(t a) _< O,
t>_ tz.
Thus,
there existsT >
t2 such thatz(T- r) >
0 andZ(m-
1)(t)
_(Z(m-1)(T),
t>_ T; (4.12)
z(m)(t) + ez(T r)Q(t)[1 (t r)] _< 0,
t>_
t.(4.13)
Set
(m 1)(t)_(t).z (t).
z(T r)
thenweobviously have
(t) >
0 forall t>_ T.
Note
that(t)
is a montonically increasing functions and using(4.12)
and(4.13),
weobtain
’(t)z(m-1)(t) (t)z(m)(t)
9’(t)
z(T r) + z(T
(r)
z(m 1)( ez(T r)Q(t)[1 A(t r)]
< z(T T) )’(t) + (t) z(T )
t> T.
Set
we have
z(m-1)(T)
z(T (r) =c>0;
’(t) <_ -[e(t)Q(t)(1 A(t r)) c’(t)],
t>_ T.
Integrating both sides to the above inequality from
T
tot(t > T),
weget (t) <_ (T) / [e(s)Q(s)(1 A(s r)) c’(s)]ds,
T
which is impossiblein view of assumption
(4.11).
This proves assertion(i).
We
can prove assertion(ii)
and(iii)
by the samearguments
as in the proofofTheorem 4.1. The proofofTheorem 4.3 iscomplete.
Theorem 4.4:
Assume
thatA(t) A
constant> O, f(- y) f(y) >
0for
y
R+
andthatf(y)
is an increasingfunction
andsatisfies:
f(x + y) <_ f(x) + f(y), f(kx) <_ kf(x) for
x> O,
y> O,
k> O. (4.14)
If Q(t)
isperiodic with period andsatisfies
Q(s)ds +
oo,(4.15)
then conclusions
(i)-(iii) of
Theorem4.1 remain true.Proof:
Let y(t)
be an eventually positive solution of the inequality(4.1). Then,
there exists a tI
>
to such thaty(t) > O, y(t- 7") > O
andy(t-cr) > O
for all t>_
tIand for
z(t) v(t) + v(t- ).
we have
z(t) > O, z(m)(t) <_ O,t _> tl;
z’(t) >0,
z(m-1)(t) > O, t_>t2_>t
1.Set
a(t) z(t) + z(t- 7") y(t) + 2Ay(t- 7") + A2y(t 2v),
t>_
t2.(4.16)
Then,
there exists at3>
t1such thatand
.(t) > 0..(t- ) > 0..’(t) > 0.
t>_ t
ce
(m-1)(t)>0,
c(m-1)(t-7")>0, t>_t
3.From (4.1)
and(4.16)it
follows that.(")(t) v(")(t) + v()(t- ) + [v(’)(t- ) + v(")(t- 2)]
<_ Q(t)f(y(t r)) Q(t r)f(y(t
7-r)). (4.17)
Choose
T >_
t3 such thaty(t-
27"-(r) > O,
t>_ T.
Since
Q(t)is
periodic with period r, weget
by(4.14), (4.16)
and(4.17)"
a(m)(t) + a(m)(t r) + Q(t)f(a(t r))
< Q(t)f(y(t a)) 2AQ(t v)f(y(t
va)) A2Q(t 2v)f(y(t
2"+ Q(t)f(y(t a) + 2Ay(t
ra) + A2y(t
2ra))
< Q(t)f(y(t ag)) 2AQ(t)f(y(t
rr)) A2Q(t)f(y(t
2ra))
+ Q(t)f(y(t )) 2AQ(t)f(y(t
rr)) + A2Q(t)f(y(t
2r)) O,
t>_ T.
(4.18)
Since a and
f
are increasing, wehave0
< c(T- (r) < a(s- a),
s> T
andI(a(T- )) <_ f(a(s- a)),s >_
T.Oscillation Criteria
for
High Order DelayPDEs
203Integrating both sides of
(4.18)
fromT
tot(t > T),
weget
0
>_
ce(m1)(t)
ce(m1)(T) -t- c
(m1)(t 7")
,kce(m1)(T 7")
+ f Q(s)f(a(s-a))ds
T
_>
c(m1)(t c(
m+ 1)(T f(a(T- -- ce( r))
TM/
T1)(t Q(s)ds. 7") c(
TM1)(T 7")
This leads to a contradiction in view of
(4.15),
sincec(m-1)(t)>0
andCe(m
--1)(t- 7") >
0 for t_>
t3. This proves assertion(i).
We
can proves assertion(ii)
and(iii)
by the samearguments
as in the proofofTheorem 4.1. This completes the proof of Theorem4.4.
We
shall consider next the case ofA(t)<
0. The following lemma is a special case ofTheorem 2 in[3].
Lemma
4.2:[3] Assume
thatfl
EC[[t
0,+ o),R +]
such thatand
Then,
the inequalitylim inf
/3(s)ds >-
t-5
limt__,+inf / fl(s)ds > O.
t_
_
x(m)(t)- m(t)x(t- mS) <_
0(4.19)
has no eventually negative bounded solutions.
We
introducethe followingnotations:cQ(t)
+ > o
Theorem 4.5:
Assume
that the condition(4.5) holds, >
7",f(-y)- -f(y) for
y +, and that there exist constants,kl,,k
2 andM
such that1
<_ "1 /(t) /2 < O,
t>_
to(4.21)
and
Q(t) >_ M > O,
t>_
toif
limt__,+ooinf J
t-5fl(s)ds > 1,
then conclusions
(i)
and(iii) of
Theorem 4.1 remain true.Proof:
Let y(t)
be an eventually positive solution of the inequality(4.1). Then,
there exists a tI>_
t0 such thaty(t) > O, y(t- r) >
0 andy(t- r) >
0 for all t>_
t1.Set We
havez(t) y(t) + ;(t)y(t- r).
z(m)(t) <_ -Q(t)f(y(t- r)) <_ -cq(t)y(t- r) <_ O,
t>_
t1.We
claim thatz(t) < O,
t>_
t1.(4.23)
If
true,
from(4.1)
it follows thatz(m)(t) <_ eQ(t)y(t r) <_ eMy(t r),
t<_
t1.(4.24)
Thus,
we see that z(m-1)(t)
is strictly decreasing on(tl, + oo)
andz(i)(t)
are strictlymonotonically functions on
It, + c), 0, 1,...,
m 2.Then,
we havelim z(m-
1)(t)
oo(4.25)
or
lim z(m
1)(t) r < +
oe.(4.26)
If
(4.25) holds,
then wehavelim
z(i)(t)
c,O, 1,...,
m 1.Hence (4.23)
is true.If
(4.26) holds,
then integrating both sides of(4.24)
from tI to t and lettingt---,
+
cx, weget
eMy(s- a)ds <_ z(
m1)(tl)-
r/,(4.27)
I
which implies that y E
Ll[tl, + oo). In
viewof(4.2),
we obtainz E
Ll[tl, -t- oo).
Note
thatz(t)
ismontonicallyfunction,
we see thatlim
z(t) O. (4.28)
Oscillation Criteria
for
High Order DelayPDEs
205Thus r/- 0.
From (4.28),
it follows thatz(i)(t)z(i+l)(t)<O,
i-0,1,...,m-1, t>t1.Equations
(4.28)
and(4.29)imply
that(4.23)is
true.Now
wehave(4.29)
v() < ()v(- ) < v(- ) < v(- ),
which implies that
y(t)
is a boundedfunction. Thusz(t)is
bounded. Sincez(t + ) ( + )(t ) + (t + -)
>_ (t- + )(t- ) o
t>_
weh&ve
Q() ).z(t-a + r) < Q(t)y(t- ),
t>
t1.(4.30)
(t-+r
From (4.24)
and(4.30),
itfollows that) z(t-(q-v)) < O, t>tl,
z()(t) -(t- + )
z(m)(t)- flm(t)z(t- mS) O,
t t1.(4.31)
In
view of(4.22),
byLemma
4.2 we see that the inequality(4.31)
has no eventuallynegative bounded
solutions,
which contradicts the fact thatz(t)<
0 andz(t)
isbounded. This proves assertion
(i). We
can prove assertion(ii)
and(iii)
by thesame
arguments
as inthe proofofTheorem4.1. The proofis thereforecomplete.5. Further Oscillation Criteria
In
this section we shall establish some further oscillation criteria for the higher order delay hyperbolic boundary valueproblem(2.1)
under(B1)and (2.1)
under(B2)
usingthe results obtained in the last two sections.
Theorem 5.1:
Assume
that conditions(U)
and(4.5) hold,
and that 0<_ ;(t) <_
1.II
min_q(x,s)[1-)(s-)]ds- (5.1)
x
then
(i) a
omio.of ro6tm (2.) . (B)
aocilmou
i. a.d(ii)
all solutionsof
the problem(2.1)
under(B2)
are oscillatory inG.
Proof:
Let u(x,t)
be a nonoscillatory solution of the problem(2.1)
under(B1).
We
may assume thatu(x,t)>O
for(x,t) Efx[#,+c),
where # is a positive number.By
the analogousarguments
as in the proof of Theorem3.1,
we can see that the functionU(t)
defined by(3.6)
is apositive solution of the inequality(3.1)
fort
>_
to>_
#, which implies that the functionU(t)
defined by(3.6)
also is a positivesolution of the inequality
m[U(t)
d-+ A(t)U(t v)] +
zflmin_q(x, t)f(U(t )) _<
0.(5.2)
However,
by Theorem4.1,
we see that the inequality(5.2)
has no eventually positivesolutions.
Thus,
we obtain acontradiction.If
u(x,t)<O
for(x,t)x[#,+c),
then -u is an eventually positive solution of the problem(2.1)
under(B1)
which is impossible. This proves assertion(i).
The assertion
(ii)
can be proved by theanalogous arguments
as in the proof of assertion(i).
The proofofTheorem 5.1 is complete.Using Theorem
4.2-4.5,
respectively, it is easy to obtain the corresponding results for problem(2.1)
under(B)or (2.1)
under(B2)also. We
merely statethem below.Theorem 5.2:
Assume
that the condition(H) holds,
and that 0< (t) <
1,f(y)
is a monotone increasing
function
inR +. If for
any c> O,
min_
q(x, s)f([1 A(s r)]c)ds +
oc,then
all solutions
of
the problem(2.1)
under(B1)
are oscillatory inG
and allsolutionsof
the problem(2.1)
under(B2)
are oscillatory inG.
Theorem 5.3:
Assume
that conditions(H)
and(4.5) hold,
and that 0<_ A(t) <_
1.If
there exists a monotonically increasingfunction
ECI[R + (- ,-t-cx)]
such that[(s)min_ a(x, s)(1 i(s )) c’(s)]ds
4-c,(5.4)
xE
for
any number c> O,
then(i)
all solutionsof
the problem(2.1)
under(B1)
are oscillatory inG
and(ii)
all solutionsof
the problem(2.1)
under(B2)
are oscillatory inG.
Theorem 5.4:
Assume
that condition(H) holds, A(t)
=_.
constant> O,
andthat
f(y)
is an increasingfunction
andsatisfies (4.14). /f q(x,t)
isperiodic in t with periodr andsatisfies
+oo
min_q(x,s)ds-+oc, (5.5)
then x
(i)
all solutionsof
the problem(2.1)
under(B1)
are oscillatory inG
and(ii)
allsolutionsof
the problem(2.1)
under(B2)
are oscillatory inG.
Theorem 5.5:
Assume
that conditions(H)
and(4.5) hold, >
v, and that there exist constants"1,’2,
andM
such thatand
-l
<_ _< (t) _< 2 <0, tER+
min
q(x,t) > M > O,
tR +.
xEft
inf
fl (s)ds > 1,
lir +
Oscillation Criteria
for
High Order DelayPDEs
207 then() (ii)
where
and
all solutions
of
the problem(2.1)
under(B1)
are oscillatory inG
and all solutionsof
the problem(2.1)
under(B2)
are oscillatory inG,
cmin_
q(x, t)
’(t) -a(t-+-)
xEftm Finally, wediscuss two examples.
Example 5.1" Consider theequation
Ot6 + (1
-e)u(x,t- -)] +
3u+ 2u(x,t- )exp[3t +
x+ u2(x,t-)]
Xu + (2 +
ost)x(,
t), (, t) e (0,,) (0, + )
and a boundarycondition of type
(B1)
,,(o, t) + (o, t) 0, (,, t) + ,,(,, t) o,
t> o.
Here,
m-6;n-X;,g-
1;gt-(0,’);r-
’;a;7(x,t)-
1 forA(t)
1 et;
q(z,t)--2e
z+3t,min q(t)--2eat; f(u)--ue
u2 : [o,]It is easy to see that the function
f(u)
satisfies condition(H)
and-boo
/ m.in .q(x,s)[1-A(s-r)]ds- Then,
all conditions of Theorem 5.1 are fulfilled.(5.7)
and(5.8)
are oscillatoryin(0, rr)
x(0, + oo).
Example 5.2: Consider the equation (94
-[u u(x,
t2r)] +
2u+ 4(2
sinx)u(x,
t4’)
etAu
-k3An(x,
t), (x, t)i(O, 7r) (0,
q-oo)
(5.8)
t>0;
_s+n"
2e3s.e
gds +
oo.Hence,
all solutions ofproblems
(5.9)
and aboundary condition ofthe type
(B2)
,,(o, t) u(,, t) o,
t>
0.(5.10)
Here,
m4;n 1;e 1;f2 -(0, 7r); A(t) 1;r 2rr;r 4rr;q(z,t) r4(2 sinx);
f(u)
u.In
thiscase,5 r-mr rr and --2
emin
q(x, t)
e[0,,]
4(t)-
A(t-
O"q-7") 71"4’
where e 1.
It
is easy to see thatinf
fl (s)ds
lim inf rds- > -.
limt-
+
oo t+
oot-r _"
2
The hypotheses of Theorem 5.5 are satisfied and hence all solutions of the problem
(5.9)
and(5.10)
are oscillatory in(0, r)
x(0,
/c).
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