R ENDICONTI
del
S EMINARIO M ATEMATICO
della
U NIVERSITÀ DI P ADOVA
S HAIR A HMAD A. S. V ATSALA
Comparison results of reaction-diffusion equations with delay in abstract cones
Rendiconti del Seminario Matematico della Università di Padova, tome 65 (1981), p. 19-34
<http://www.numdam.org/item?id=RSMUP_1981__65__19_0>
© Rendiconti del Seminario Matematico della Università di Padova, 1981, tous droits réservés.
L’accès aux archives de la revue « Rendiconti del Seminario Matematico della Università di Padova » (http://rendiconti.math.unipd.it/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions).
Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
Comparison Equations
with Delay in Abstract Cones.
SHAIR AHMAD
(*) -
A. S. VATSALA(**)
1. Introduction.
Differential
equations
and differentialinequalities containing
func-tionals is of
great importance
inproblems
of biomathematical medi-cine, chemistry,
y heat flow andpopulation growth. Many
of theseapplications
lead to anequation,
which is ofparabolic structure,
in the sense that theequation
would beparabolic
if the function in itwere
replaced by
a known function. Aspecial
case ofthis,
which isknown as reaction diffusion
equation
occurs in studies ofpopulation genetics [2, 9],
conduction of nerveimpulses [2, 4],
chemical reac-tions
[1, 3]
and several otherbiological questions [1, 8].
In this paper we
give comparison
theorems related toparabolic
differential
inequalities
withdelay
and flow in variance results for theparabolic
differentialequation
withdelay
in a Banach space.We have also included a
generalization
of the classical Miiller’s the-orem. Our results are
generalizations
of the results in[5].
See also[7]
for different
type
ofcomparison
theoremsconcerning parabolic
dif-ferential
inequalities
withdelay
in Rn.2.
Preliminary
results.Let Q be a bounded domain in Rn and let G =
[to
- T,to]
X S~and H =
(to, Suppose
theboundary
aH of H issplit (*)
Indirizzodegli
A.A:Department
of Mathematics,University
of Miami, Coral Gables, Fl. 33124, U.S.A.(**) Department
of Mathematics, Oklahoma StateUniversity, Stillwater,
Oklahoma 74078.
into two
parts 8Hi
such that 8H =8Ho LJ 2H1,
8Q cand
8Ho m
0.Let .E be a real Banach space with
1/ .11.
A one k is a proper sub- set of .E such that if v, w E ER+,
then v+
w, lv E k.Throughout
this paper we will consider a closed cone k and its interior k0 and we assume that k° is
nonempty.
The cone k induces apartial ordering
on E defined
by uv
iff v - u E k and uvLet k* be the set of all continuous linear functionals c on E such that
c(~) ~ 0
for all u and letk*
be the set of all continuous linear functionals c on E such thatc(u)
> 0 for all u E T~°.Let i > 0 be a
given
real number and C =C ~[-
T,0], E]
andCp = C C[- i, 7 0] x D, E]
denote the Banach spaces of continuous func- tions with the normof T
EC, g~( ’ , x)
ECp given by
respectively.
A vector v is said to be an outernormal at
( t, x)
E if( t, x - hv)
EE t for small h > 0. The outernormal derivative is then
given by
We shall
always
assume that an outernorinal exists onaHl
and the functions inquestion
have outernormal derivatives onOH1.
If u E
V H, E]
andu(t -f- s, x)
Eep
for t Eoo)
and also if8E[-T,O]
the
partial
derivativesayat, ux(= ayax), a2UIaX2)
exist andare continuous in
H,
then we shall saythat u(t, x ) belongs
to class Z.From now on we denote
u(t +
s,x)
asut(., x).
We state below Mazur’s theorem which is needed in our compar- ison theorems.
THEOREM 2.1
(Mazur).
Let k be a cone withnonempty
in-terior k°. Then
(i) ~c
E k isequivalent
to > 0 for all c E k*.(ii) u
E akimplies
that there existsa c E ko
such thatc(u)
= 0.A function is said to be
quasimonotone nondecreasing
in u forfiged t,
x, qbelonging
to[to, 00), Q, en respectively,
if for any u, v EE,
Uan vx E Uxan vxx EEn’
such that u ~ v,
c(u)
=c(v),
=c(vx)
for i= I ,
... , n, andimplies
For the case = Rn and k =
R+,
thequasimonotone
conditionon
f implies
thatf i (t,
x, u, ux,~( ’ , x))
=fi (t~ x~ ‘l’~, ?,~x 9 ‘uxx ~ q( . , z))
for
each i,
A function is said to be
monotone
nondecreasing
ing~( ~ , x)
if for U EE, Ua; E En, En’, g~( ~ , x) ~ ~( ~ , x) implies
that forc E ko
REMARK 2.1. We
give
similar definitions ofquasimonotonicity
and
monotonicity
of a function3. In this section we
develop
thetheory
of differentialinequal-
ities related to
parabolic
differentialequations
withdelay.
THEOREM 3.1.
Suppose
that( i ) f is quasi-
monotone
nondecreasing
in u relative to k and monotonenondecreasing
in
gg(-, x)
relative to7~,
andwhere 1
Then
v(t, x) w(t, x)
on[to, oo)
XQ,
if one of theinequalities
in(i)
is strict.
PROOF. Assume that one of the
inequalities
in(i)
is strict. Con- siderm(t, x)
=v(t, x)
-w(t, x).
It isenough
to show thatm(t, x)
0.If it were not
true,
there would exist a(t, , x1 )
and c E7~o
such thatm(t, x) 0
on[to, tl)
XQ, m(t1, x,)
0 andc(m(tl, x))
0. It is easy to see that the functionx))
has its maximum at x. which isequal
to zero.Clearly
because of( ii ) ( a )
and(b).
Also
(tal,
y for we would then haveThis contradicts
(ii) (c). Hence, (tl, x,)
E H. Let c Ek)
be such thatm(t1, xl) 0, c(m(tl, x,))
=0, xi))
= 0 and for i =1, 2,
..., n, andi.
and
m tl( ~ , x) ~ 0.
This im-plies
thatand
x) x). Thus,
in view of(i),
it follows thatusing quasimonotonicity of f
in u relative to k andmonotonicity
off
in
g~( ~ , x)
relative to 1~. That isx,))
0. Howeverfor h > 0
sufficiently
small. It there-fore follows that
c((omfot)(t1, 0153l))>O,
which leads to a contradiction.This
completes
theproof.
REMARK 3.1. The conclusion of the above theorem is not valid if one of the
inequalities
in(i)
is not strict.However,
we candispense
with the strict
inequality
needed in Theorem 3.1 of(i), (ii)
if in ad-ditio n
f
satisfies thefollowing condition,
(Co)
z > 0 onGuÏl-oHl,
onaH,
and for
sufficiently
small E >0,
eitheron
where v, w E Z.
THEOREM 3.2. Let the
assumptions (i)
of Theorem 3.1 hold.Sup-
pose further that the condition
Co
is satisfied. Then the relationsimply v(t, x) x)
on[to, oo)
X,52.
PROOF. Assume that the condition
(a)
ofCo
holds. Consider v = v - 8z where E > 0 issufficiently
small. We haveusing Co(a).
Alsov(t, x) w(t, x)
on G u andThus,
thefunctions v, 2v satisfy
theassumptions
of Theorem3.1,
hence
v(t, x) 16(t, x)
on H.Taking
the limit as e - 0yields
thedesired result and the
proof
iscomplete.
REMARK 3.2. If
8Hi
isempty
so thataHo
=aH,
the assump- tion( Co)
in Theorem 3.2 can bereplaced by
a weakerhypothesis, namely
a one-sidedLipschitz’s
condition of the formfor u > v and
g~( ~, x) ~ y~( ~, x).
In this case, it is
enough
to set v = v -ee2Ltyo,
yo E ko(where
8 > 0 is
sufficiently small)
so thatx ) w(t, x )
on aH andvt,( ’ ~ x) wto( ’ ~ x)
Even when
dH1
is notempty,
the condition(Ci)
isenough
prov- ided(ii) (c)
isstrengthened
to+ Q (t, x, v) c 8wj8v + Q (t,
x,w)
onaHl
whereQ E C[H X E, E]
and isstrictly increasing
in u.To see
this,
observe that 0 v and henceQ(t,
x,0) Q(t,
x,v)
whichgives
the desired strictinequality
needed in theproof.
4. In this section we
give
somecomparison
theorems related tothe
system
satisfying
the initialboundary
conditions0 A closed set is said to be flow invariant relative to the
system (4.1)-(4.2)
if for every solutionu(t, z)
of(4.1)-(4.2)
we havepo( . , z)
anduo (t, x) c F implies u(t, .r)
c- F onj7.
The function
f(t,
x, uy uxx,gg(*7 .r))
is said to bequasi-nonpositive (quasinonnegative)
if(u > 0),
=0, =0, ~
=1, 2, ..., n
and
I - -il I l I I --, --
-
for A E Rn and also for
(cp( ~ , x)) ~ 0, (9~(’?~)>~) for
someimplies
THEOREM 4.1. Assume that
f
isquasinonpositive
and that the condition holds with v = it, where u =u (t, x )
is any solution of(4.1)-(4.2).
Then the closed setQ
is flow invariant relative to thesystem (4.1)-(4.2)
whereQ
=[~c E E, u 0].
PROOF. We set
m(t, x)
==x)
whereu(t, x)
is any solution of(4.1)-(4.2)
such thatx), x)
EQ
and 8 > 0 is suf-ficiently
small and z E Z is as inCO(a).
We wish to showm(t, x) ~
0on
H.
Ifnot,
there would exist a(tl, x1),
ti >to,
I Xl c S2 and c Ek:
such that
It is easy to see that the function has its maximum at Xl
which is
equal
to zero.Clearly,
y or Let(tl,
E H and cE k:
be such thatx1) 0, c(m(t1,x1))
=0,
==
0, i
=1,
... ,n, .L kikjc(mxixj(t1, x1))0, k
E Rn. Theni,~ =1
by Co(a)
and the factf
isquasinonpositive,
we obtainbut
This leads to a contradiction.
Hence, (t1, x,) 0
H.Thus, m(t, x)
0on H which
implies,
as e ~0,
the flow invariance ofQ,
which completes
theproof.
REMARK 4.1. Theorem 3.2 can be obtained as a consequence of Theorem 4.1. For this purpose we set d = so that
where
Clearly _dto( ~ , x) ~ 0,
andd(t, x) c 0
on8Ho showing
on
ago .
It caneasily
be seen .~’ isquasinonpositive
andthat .F satisfies condition
Co(a) with f replaced by
F and vreplaced by
d.Hence,
the conclusion follows.COROLLARY 4.1. Assume
that f
isquasinonnegative
and that the conditionCo(b)
holds with w =u(t, x).
Then the closed setQ
is flowinvariant relative to
(4.1)-(4.2)
whereQ = [~ E E, u > 0 ]
if~c t a ( ~ , x )
and
x)
EQ.
0
COROLLARY 4.2.
Suppose
that condition( Co)
holds with v = w = ~.Assume also the
following
conditionholds;
ut( ~, z)) > 0,
then the closed setW,
where w =[u
EE, a
ub,
a, is flow invariant relative to(4.1)-(4.2).
REMARK 4.2. If
dH0
=afl,
then the initialboundary
con-ditions can be written as for and
(aulat) ( t, x)
= 0 on8Hi .
We shall next consider a
comparison
result whichyields
upper and lower bounds for solutions of(4.1)-(4.2)
in terms of solutions ofordinary delay
differentialequations.
THEOREM 4.2. Assume that
(i) ~ _ u(t, x)
is any solution of(4.1)-(4.2)
and the condition( Co )
holds with v = w = u ;(ii) e, E’]~
u,g2(t, u, q)
arequasimo-
notone
nondecreasing
in u relative to k and monotonedecreasing
in cp relative to k and for if
c(uxi)=0, i==1,2,...,n and
(iii) r(t),
are solutions ofsuch that
ro(to)
= andsuch that
oo(to)
=yo(0) respectively existing
on[to, oo)
such thatwhere is any solution of
( 4.1 ) - ( 4.2 ) ,
thenPROOF.
Setting
we see that m satisfieswhere
We shall show that
(4.3)-(4.4)
satisfies theassumptions
of The-orem 4.1. Let
e(m)
==0, m,(-, ~)0, e(mx,)
=0,
i ==1, 2,
...~ ~yn
and for some This
implies
thati.l=l
t and
c(u)
=c(r)
andconsequently
thequasi- monotonicity
of gl in u andmonotonicity of
g, in Tyield
zc,Ut))
r,
rt)).
It now follows from(ii)
andproving
1~’ isquasinonpositive.
We have
This proves .F’ satisfies the condition
(Co) (a)
yvith v = m.Thus, by
Theorem 4.1 it follows that
m(t, x) ~ 0
on H which provesx) c r(t)
on H.
On similar lines we can show that
e (t) x) by setting
m =This proves the theorem.
COROLLARY 4.3. If H is flow invariant relative to the
system (4.1)- (4.2),
y there exists functions gl, g2satisfying
theassumptions
of The-orem 4.2
provided
E = Rn and K =PROOF. We construct g2 as follows: for
each i,
and
f
iselliptic
for each i.Next we
give
acomparison
theorem which is an extension of the classical result of Miiller[6]
which is valid when .E and k =1~+ .
THEOREM 4.5. Assume that
(i)
foreach i,
1 (1,vx, vxx, q)
forwhenever
.~i
isquasimonotone nondecreasing
in u and monotonenondecreasing in ga
and there exists a such that z > 0 on
[to, co)
XQ,
0 forx E
S2, ~ x) ~ y
> 0 on8Hi ,
and for allsufficiently
small s >0,
(iii) u (t, x)
is any solution of(4.1)-(4.2)
such that 9and on
8Hi ,
thenon
(W.J H.
PROOF. We shall first assume
that v, w satisfy
strictinequalities
and prove the conclusion for strict
inequalities.
We let m = ~ - wand n = ~ - v on
[to, oo)
X Q. We show m 0 n. Ifnot,
therewould exist a
(tl, Xl)
anda j
such that eitherc 0,
=0,
7 n’ ’
Suppose
the first alternative holds.Certainly
t1 >to by (iii). Hence,
atwhich leads to a contradiction. A similar
proof
holds when the second alternative is true.Thus,
weget m(t, x)
0n(t, x)
on G U j7 andthis proves the claim for strict
inequalities.
_Consider now w = w
+
= v - Ez on G u H. LetPi(t,
x,o)
== max
wi(t, x),
minwt( ’ , x)}].
Then it is clear that if iand 9-9
issuch that
replace by
andwi ,
it follows thata = P(t, z, W) , q = Pi( . , z, §5 ) satisfy
i and Gi = wi .Hence, using (i)
and(ii)
weget
Here we have used that
Li
isquasimonotone nondecreasing
in u andmonotone
decreasing in q
and -c Ezt
forall j .
Since Uto also v on
8Ho ,
and81Yf 8v
on
8Hi .
Weget immediately v(t, x)
-sz(t, x) u(t, x) w(t, x) + + x )
on G U H forarbitrary e
> 0.Letting 8
-0,
we obtainthe stated
result, completing
theproof.
COROLLARY 4.4. Let the
assumptions (i), (ii)
of Theorem 4.2 hold without gl , g2being quasimonotone nondecreasing
in it and withoutbeing
monotonedecreasing
in cpoSuppose
that the conditions(ii), (iii)
of Theorem 4.5 are satisfied. Assume further that for
each i,
and
Then on (7uR. Note that the
f unctions v, w
donot
depend
on the space variable x in theforegoing corollary.
5. Consider the reaction-diffusion
equation
of thespecial
formin with the initial function
and the Neumann
boundary
conditionIn
(5.1)
L1 denotes theLaplace operator
inand A is a
diagonal
matrix.Consider the standard cone in
..RN, namely
Clearly
the setgenerates
the cone k. Let us note that weakcoupling
of thesystem (5.1) suggests
the choice of thisspecial
cone.Thus,
theinequality implies
thecomponentwise inequalities
==1, 2,
... , N.THEOREM 5.1. Assume that
(i)_A ~ 0
andu(t, x)
is any solution of(5.1)
to(5.3) existing
on
B+ x D9
(ii) xt)
satisfies aLipschitz
condition for a constantL ~ 0;
(iii)
Theboundary
8Q isregular, i.e. ,
y there exists h E Z such thaton D,
on oil andhae, hxx
are bounded.Then the
following
conclusions are valid.(b)
IfF(t,
u,g~)
isquasimonotone nondecreasing
in u and mono-tone
nondecreasing in p
relative to that is foreach i,
-Fi(t9
u, isnondecreasing
in andnondecreasing
inx)
and if the solutions
r(t),
ofy’ - F(t,
y,y,)
withro(.)
=~o( ~ )
=q~o(s)
exist onR+,
then ’provided
that onD.
(e)
If ~c,q)
isquasimonotone nondecreasing
in it and mono-tone
decreasing
in (f,F(t, 0, 0)
=0,
thenimplies
thatu(t, x) ~
0 on~
XDy
implies
thatimplies
that onR+ X S2,
wherer(t)
is the same func-tion assumed in
( b ) .
(d)
IfF(t,
u,u,) is
notquasimonotone
in u, nor monotonein 92
and if the closed set W =
[u
is flow invariant relative to(5.1)
to(5.3),
then the estimate(5.4)
holds wherer(t), e(t)
are nowbeing
solutions ofwhere
_(e)
IfF(t,
u,q)
is notquasimonotone
in u nor monotonein lp
and W is not known to be flow
invariant,
then(5.4)
holds and ifr(t), satisfy
the relationsfor all a such that 0~==~
lp)
for all 0’ such and J; = ri, forPROOF. The conclusion
( a )
follows fromCorollary
4.1. Theorem 4.2yields (b)
with the choice .F = gi = g2.Uniqueness
of solutions ofy’ - pet, Y, yi) together
with the factpet, 0, 0)
= 0implies (c).
Corol-lary (4.3) gives
the conclusion(d)
whereas(e)
follows fromCorollary
4.4.REFERENCES
[1]
R. ARIS, The mathematicaltheory of diffusion
and reaction inpermeable catalysts,
Clarendon Press, Oxford,England,
1975.[2]
D. G. ARONSON - H. F. WEINBERGER, Nonlineardiffusion in population genetics,
combustion and nervepropagation,
Lecture Notes, vol. 446,Sprin- ger-Verlag,
New York, 1975.[3]
P. C. FIFE, Patternformation in reacting
anddiffusing
systems, J. Chem.Phys.,
64(1976),
pp. 554-564.[4]
R. FITZHUGH, Mathematical modelsof
excitation andpropagation
in nerves,Biological Engineering,
H. P. Schwann, Ed., McGraw-Hill, New York,1969.
[5]
V. LAKSHMIKANTHAM,Comparison
resultsfor
reaction anddiffusion
equa-tion in a Banach space, Technical
report
94, Univ. of Texas atArlington.
[6]
M. MULLER,Über
dasfundamental
theorem in der theorie dergewohnlichen differential gleichungen,
Math. Z., 26 (1926), pp. 619-645.[7]
R. REDHEFFER - W. WALTER,Comparison
theoremsfor parabolic func-
tional
equalities.
[8]
A. M. TURING, On the chemical basisfo morphogenesis,
Phil. Trans.Roy.
Soc. London Ser. B, 237 (1952), pp. 37-52.
[9]
P. E. WALTMAN, Theequations of growth,
Bull. Math.Biophys.,
26 (1964), pp. 39-43.Manoscritto