A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE
S VETLA D IMITROVA M ILUSHEVA D RUMI D IMITROV B AINOV
Averaging method for neutral type impulsive differential equations with supremums
Annales de la faculté des sciences de Toulouse 5
esérie, tome 12, n
o3 (1991), p. 391-403
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- 391 -
Averaging method for
neutral type impulsive differential equations
with supremums
SVETLA DIMITROVA MILUSHEVA and DRUMI DIMITROV
BAINOV(1)
Annales de la Faculte des Sciences de Toulouse Vol. XII, nO 3, 1991
La méthode du centrage pour des equations différentielles impulsives du type neutral avec des supremuns est justifide.
ABSTRACT. - The averaging method for neutral type impulsive differ- ential equations with supremums is justified.
1. Introduction
The papers of
Mil’man, Myshkis ~1~, ~2~
mark thebeginning
of asystem-
atic andprofound investigation
ofimpulsive
differentialequations [3].
. Theintensive
development
of thetheory
of theimpulsive
differentialequations
is conditioned
by
the fact thatby
means of them processes are success-fully
simulated which at certain moments of theirdevelopment undergo
arapid change.
Such processes are observed inmechanics,
radioengineering, biology, population dynamics, biotechnologies,
etc.Parallel with the
development
of thetheory
ofimpulsive
differentialequations
did the firstinvestigations
ofordinary
andpartial
differentialequations
with maxima[4]-[7] begin
in relation to theirapplication
toeconomics and control
theory.
In the mathematical simulation in various
important
branches of controltheory, pharmacokinetics, economics,
etc. one has toanalyse
the influence of both the maximum of the functioninvestigated
and itsimpulsive, by jumps changes. Thus,
forinstance,
if the concentration of the medicinal substance in the bloodplasma
has to be controlled at a venousinjection
1 ~ ) Academy of Medicine, P.O. Box 45, Sofia 1504, Bulgaria
(an impulsive change
of thisconcentration)
of the medicinalsubstance,
onehas to take into account
together
withit,
in view of theoptimal therapy,
themaximum of this concentration too. An
adequate
mathematicalapparatus
for simulation of such processes are the
impulsive
differentialequations
withsupremums.
In the
present pioneer
paper theaveraging
method for neutraltype impulsive
differentialequations
with supremums isjustified.
2. Statement of the
problem
Consider the
impulsive system
of differentialequations
with supremumsof the form
where x = (x1, ... , h is a
positive constant,
_
(c,pl (t),
... is an initialfunction,
: D -~IRn,
k EIN,
,rk are fixed numbers such that D = ro rl ~ ~ ~ r~ ~ ~ ~ and lim Tk = oo and f E
(0, E*, (E*
= const >0)
is a smallparameter.
For any
x ~ D
let thefollowing
limits existThen with the
system (1)
we associate theaveraged system
orordinary
differential
equations
with initial condition
We shall
note,
for the sake ofdefiniteness,
thatspeaking
of a value of apiecewise
continuous function at apoint
ofdiscontinuity
we mean the limitfrom the left of the function
(provided
itexists)
at thispoint. By
the simboldenote summation over all values of k for which the
inequality
0 rk T is
satisfied,
andby
thesymbol ~ ~ ~ ~ ~
the Euclidean norm in IRn.We shall say that condition
(H)
is satisfied if thefollowing
conditionshold:
H1 The function
X(t,
x, y,z)
is continuous in the domainThe functions
cp (t )
andc,p ~t )
arecontinuous,
and( i
=1,
...,n)
have a finite number of extremums in theinterval -h ,
0~,
,h = const >
0,
and E D and~p (t )
ED1
for t E~
- h, 0 ~
. Thefunctions
I k ( z ), k
EIN ,
are continuous in D.H2 There exist
positive
constants M and A such that for any t >0,
~,z’,
y,y’ ED,
z,z’
EDl , k
E IN thefollowing inequalities
holdand for t E
[
-h, 0 ~
thefollowing inequality
is validH3 For ae E D there exist the limits
(2)
and(3).
H4 There exists a
positive
constant 8 such that for k E IN theinequality
Tk -
r~_1 >
0holds,
where To = 0.H5 For any E E
(0, , E* ~,
E* = const > 0system (1)
has aunique
solutionx(t)
which is defined in the interval[0, LE-1 ~,
L - const >0;
and i =
1,
... , n, have a finite number of extremums in each interval of finitelength ; x(t)
andx(t) satisfy respectively
theconditions ~ (0
~--0) = ~p(0)
andx (0
-~0) _
H6 For E = 1 the
Cauchy problem (4), (5)
has aunique
solutionwich is defined in the
interval [ 0, L ] and
t e[ 0,
L] belongs
to thedomain D
together
with somep-neighbourhood
of it(p
= const >0).
3.
Auxiliary
assertionsUnder some natural constraints
imposed
on theright-hand
sides of theequations
insystem (1)
we shall prove a theorem ofproximity
of thesolutions of the initial
system (1)
and theaveraged system (4)
with initial condition(5).
In theproof
of the main result we shall use thefollowing
twolemmas.
LEMMA 1.2014 For the sequence TO, Tl, ... ... let condition H4 hold.
Then
for
any T > 0 andt0 ~
0 thefollowing inequality
is validProof.
- Let n > 2 andT~ to
...Tj+n to
+ T. Then for T > 8 we haveLet
Tj t0 ~ j+1 to
+ Tj+2.
Then for T > 8 we haveThis
completes
theproof
of lemma 1. QLEMMA 2. - For the sequence Tl , ... , Tj~, ... let condition H4 hold. Let the
nonnegative piecewise
continuousfunction u(t) satisfy for
t >to
theinequality
in which c >
0, ,Q
>0,
1 > 0 and Tj~ arepoints of discontinuity of
thefirst
kind
of
thefunction u(t).
. Thenfor
thefunction u(t)
the estimateis
valid,
wherei(to, t)
is the numberof
thepoints
r~belonging
to the interval( to
, t) .
Lemma 2 is
proved by
means of theinequality
of Gronwall-Bellman andby
induction. 0Lemma 2 is a
particular
case of the theorems onintegral inequalities
obtained in
~3~ .
4. Main Results
THEOREM 1. - Let condition
(H)
hold. Thenfor
any r~ > 0 and L > 0 there exists ~0 E( 0 , ~*] (eo
=L))
such thatfor
e E( 0 , ]
andt E
~ 0 , LE-1 ~ ]
theinequality II
-~(t) ()
r~holds,
whereis the solution
of problem (1~~, (5).
Proof.
- From the conditions of theorem 1 is follows that for each com-pact QED
there exists a continuous functiona(T)
whichmonotonically
tends to zero as T ~ oo and is such that for x
E Q
thefollowing inequalities
hold
,, ,,
where
x(t)
_ and =c,p(t)
for t E~
-h, 0 ~.
Subtracting (9)
from(8)
for t > 0 we obtainDenote
successively by ,Q(t), y(t), 6(t)
and~(t)
the addends in theright-
hand side of
(10).
.Without loss of
generality
of theresult,
in the estimation of the functionwe shall assume that
for i =
1,
... , n and k E IN. From the lastassumption
it follows that the supremums in and i =1,
..., n, are reached.Denote
respectively by si (t, h)
andsi (t, t~)
the leftmostpoint
of theinterval
[ t
-h , , t ~, t
>0,
at whichrespectively
and reach theirgreatest
values in this interval. ThenUsing
the conditions of theorem1,
we obtainDenote
by
the second addend in theright-hand
side of( 11 )
andobtain the
following
estimateSet A = 03BBh
(3 B + 6 + 1+03B8
~ /t)M+ / A(L - apply
Minkowski’s
inequality
and for t~ J~
obtainFor
1’(t)
for t EJE, by
the conditions of theorem1,
weget
the estimateIn order to obtain estimates of the functions
~(t)
and((t)
for t E.~E,
we
partition
the interval.~E
into mequal parts by
thepoints ti
= i =0, 1,
... , m.Let t be an
arbitrarily
chosen and fixed number of the intervalJE,
andt E
(ts, , ts+1 ~,
where s E IN and 0 s m - 1.Then, using
conditions of theorem 1 andinequality (6),
we obtainWe pass to the estimation of
~(t).
.Using
the conditions of theorem 1 andinequality (7)
for t E(ts ],
we obtainFrom the results obtained for and
~{t)
for t E(ts ,
it followsthat for
any t
thefollowing
estimates are validFrom
(10)
and the estimates obtained for the functions,Q(t), y(t), 5(t)
and
((t)
it follows that for tE JE
thefollowing inequality
holdsChoose
successively
asufficiently large
mo E IN and asufficiently
smallE1 E
( 0 , E* ~ ] so
that thefollowing inequalities
should holdFor m = mo and E E
( 0 , y ~ ] apply
lemme 1 to the third addend in theright-hand
side ofb(E, m)
and obtainFrom
(12), (13)
and(14)
for m = mo, E E( 0 , ~1] and t
EJe
there follows theinequality
Apply
lemma 2to (15)
and obtainChoose a
sufficiently
small Eo E( 0 , ] so
that for f E( 0 , ~0] to
haveThen for E E
( 0 , ~0] (Eo
=L))
and t EJE
thefollowing inequality
should hold
Hence,
for t EJE, belongs
to the domain D and the estimateII ~(t~ II
~l is valid.This
complestes
theproof
of theorem 1. 0- 403 - References
[1]
MIL’MAN(V.D.)
and MYSHKIS(A.D.) .
2014 On the stability of motion in thepresence of impulses,
Sib. Math. J., 1
(1960)
pp. 233-237(in Russian).
[2]
MIL’MAN(V.D.)
and MYSHKIS(A.D.) .
2014 Random impulses in linear dynamicsystems. Approximate method for solving differential equations, Publ. House Acad. Sci. Ukr. SSR, Kiev
(1963)
pp. 64-81(in Russian).
[3]
LAKSHMIKANTHAM(V.),
BAINOV(D.D.)
and SIMEONOV(P.S.)
.2014 Theory of Impulsi ve Differential Equations,Work Scientific, Singapore, New-Jersey, London, Hong-Kong
(1989),
273 p.[4]
ANGELOV(V.G.)
and BAINOV(D.D.) .
2014 On the functional differential equationswith "maximums",
Appl. Anal. 16
(1883)
pp. 187-194.[5]
BAINOV(D.D.)
and MILUSHEVA(S.D.) .
2014 Justification of the averaging methodfor functional differential equations with maximums, Hardonic J., 6
(1983)
pp. 1034-1039.[6]
BAINOV(D.D.)
and ZAHARIEV(A.I.) .
2014 Oscillating and asymptotic propertiesof a class of functional differential equations with maxima, Czechoslovak Math. J., 34
(109), (1984)
pp. 247-251.[7]
MISHEV(D.P.) .
2014 Oscillatory properties of the solutions of hyperbolic differential equations with "maximums",Hiroshima Math. J., 16