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Volume 2007, Article ID 40160,17pages doi:10.1155/2007/40160

Research Article

Necessary Conditions of Optimality for Second-Order Nonlinear

Impulsive Differential Equations

Y. Peng, X. Xiang, and W. Wei

Received 2 February 2007; Accepted 5 July 2007

Recommended by Paul W. Eloe

We discuss the existence of optimal controls for a Lagrange problem of systems governed by the second-order nonlinear impulsive differential equations in infinite dimensional spaces. We apply a direct approach to derive the maximum principle for the problem at hand. An example is also presented to demonstrate the theory.

Copyright © 2007 Y. Peng et al. This is an open access article distributed under the Cre-ative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

It is well known that Pontryagin maximum principle plays a central role in optimal control theory. In 1960, Pontryagin derived the maximum principle for optimal control problems in finite dimensional spaces (see [1]). Since then, the maximum principle for optimal control problems involving first-order nonlinear impulsive differential equations in finite (or infinite) dimensional spaces has been extensively studied (see [2–10]). How-ever, there are a few papers addressing the existence of optimal controls for the systems governed by the second-order nonlinear impulsive differential equations. By reducing wave equation to the customary vector form, Fattorini obtained the maximum principle for time optimal control problem of the semilinear wave equations (see [6, Chapter 6]). Recently, Peng and Xiang [11,12] applied the semigroup theory to establish the existence of optimal controls for a class of second-order nonlinear differential equations in infinite dimensional spaces.

LetYbe a reflexive Banach space from which the controlsutake the values. We denote a class of nonempty closed and convex subsets ofYbyPf(Y). Assume that the multifunc-tionω:I=[0,T]→Pf(Y) is measurable andω(·)⊂EwhereEis a bounded set ofY, the admissible control setUad= {u∈Lp([0,T],Y)|u(t)∈ω(t) a.e}.Uad= ∅(see [13,

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technique to derive the maximum principle for a Lagrange problem of systems governed by a class of the second-order nonlinear impulsive differential equation in infinite di-mensional spaces. Consider the following second-order nonlinear impulsive differential equations:

¨

x(t)=Ax˙(t) +ft,x(t), ˙x(t)+B(t)u(t), t∈(0,T]\Θ,

x(0)=x0,Δlxti=Ji0

xti, ti∈Θ,i=1, 2,. . .,n, ˙

x(0)=x1,Δlx˙ti=Ji1

˙

xti, ti∈Θ,i=1, 2,. . .,n,

(1.1)

where theAis the infinitesimal generator of aC0-semigroup in a Banach spaceX=

{ti∈I|0=t0< t1<···< tn< tn+1=T},Ji0,Ji1(i=1, 2,. . .,n) are nonlinear maps, and Δlx(ti)=x(ti+ 0)−x(ti),Δlx˙(ti)=x˙(ti+ 0)−x˙(ti). We denote the jump in the statex, ˙x at timeti, respectively, withJi0,Ji1determining the size of the jump at timeti.

As a first step, we use the semigroup{S(t), t≥0} generated byA to construct the semigroup generated by the operator matrixA(seeLemma 2.2). Then, the existence and uniqueness ofPCl-mild solution for (1.1) are proved. Next, we consider a Lagrange prob-lem of system governed by (1.1) and prove the existence of optimal controls. In order to derive the optimality conditions for the system (1.1), we consider the associated adjoint equation and convert it to a first-order backward impulsive integro-differential equa-tion with unbounded impulsive condiequa-tions. We note that the resulting integro-differential equation cannot be turned into the original problem by simple transformations=T−t

(see (4.9)). Subsequently, we introduce a suitable mild solution for adjoint equation and give a generalized backward Gronwall inequality to find a priori estimate on the solution of adjoint equation. Finally, we make use of Yosida approximation to derive the optimal-ity conditions.

The paper is organized as follows. InSection 2, we give associated notations and pre-liminaries. InSection 3, the mild solution of second-order nonlinear impulsive diff eren-tial equations is introduced and the existence result is also presented. In addition, the existence of optimal controls for a Lagrange problem (P) is given. InSection 4, we dis-cuss corresponding the adjoint equation and directly derive the necessary conditions by the calculus of variations and the Yosida approximation. At last, an example is given for demonstration.

2. Preliminaries

In this section, we give some basic notations and preliminaries. We present some ba-sic notations and terminologies. Let £(X) be the class of (not necessary bounded) linear operators in Banach spaceX. £b(X) stands for the family of bounded linear operators in X. ForA∈£(X), letρ(A) denote the resolvent set and R(λ,A) the resolvent corre-sponding toλ∈ρ(A). DefinePCl(I,X) (PCr(I,X))= {x:I→X|xis continuous att∈

I\Θ,xis continuous from left (right) and has right- (left-) hand limits atti∈Θ}.PC1l(I,

X)= {x∈PCl(I,X)|x˙∈PCl(I,X)},PCr1(I,X)= {x∈PCr(I,X)|x˙∈PCr(I,X)}. Set

xPC=max

sup t∈I

x(t+ 0), sup

t∈I

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It can be seen that endowed with the norm · PC( · PC1)PCl(I,X)(PC1l(I,X)) and

PCr(I,X)(PCr1(I,X)) are Banach spaces.

In order to construct theC0-semigroup generated byA, we need the following lemma

([14, Theorem 5.2.2]).

Lemma2.1. LetAbe a densely defined linear operator inXwithρ(A)= ∅. Then the Cauchy problem

˙

x(t)=Ax(t), t >0,

x(0)=x0 (2.2)

has a unique classical solution for eachx0∈D(A)if, and only if,Ais the infinitesimal

gen-erator of aC0-semigroup{S(t),t≥0}inX.

In the following lemma we construct theC0-semigroup generated byA.

Lemma 2.2 [12, Lemma 1]. SupposeA is the infinitesimal generator of a C0-semigroup

{S(t),t≥0}onX. ThenA=(0 I

0A)is the infinitesimal generator of aC0-semigroup{S(t),t≥

0}onX×X, given by

S(t)=

I 0tS(τ)

0 S(t) . (2.3)

Proof. Obviously,Ais a densely defined linear operator inX×Xwithρ(A)= ∅ accord-ing to assumption.

Consider the following initial value problem:

¨

x(t)=Ax˙(t), t∈(0,T], x(0)=x0, x˙(0)=x1∈D(A). (2.4)

It is to see that the classical solution of (2.4) can be given by

x(t)=x0+

t

0S(τ)x1, x˙(t)=S(t)x1. (2.5)

Settingv0(t)=x(t), v1(t)=x˙(t), v(t)=(vv01((tt))), v0=(xx01)∈D(A)=X×D(A), (2.4)

can be rewritten as

˙

v(t)=Av(t), t∈(0,T], v(0)=v0∈D(A), (2.6)

and (2.6) has a unique classical solutionvgiven by

v(t)=

I 0tS(τ)

0 S(t) v0. (2.7)

UsingLemma 2.1,Agenerates aC0-semigroup{S(t),t≥0}.

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Lemma2.3 [7, Lemma 3.2]. SupposeAis the infinitesimal generator of a compact semigroup {S(t),t≥0}inX. Then the operatorQ:Lp([0,T],X)→C([0,T],X)withp >1given by

(Q f)(t)= t

0S(t−τ)f(τ) (2.8)

is strongly continuous.

Lemma2.4 [15, Lemma 1.1]. Letϕ∈C([0,T],X)satisfy the following inequality:

ϕ(t)a+bt

0

ϕ(s)ds+ct

0

ϕs

Bds ∀t∈[0,t], (2.9)

wherea,b,c≥0are constants, andϕsB=sup0≤τ≤sϕ(τ). Then

ϕ(t)ae(b+c)t. (2.10)

3. Existence of optimal controls

In this section, we not only present the existence ofPCl-mild solution of the controlled system (1.1) but also give the existence of optimal controls of systems governed by (1.1).

We consider the following controlled system:

¨

x(t)=Ax˙(t) +ft,x(t), ˙x(t)+B(t)u(t), t∈(0,T]\Θ,

Δlxti=Ji0

xti, Δlx˙ti=Ji1

˙

xti, ti∈Θ,

x(0)=x0, x˙(0)=x1, u∈Uad,

(3.1)

and naturally introduce its mild solution.

Definition 3.1. A functionx∈PC1

l(I,X) is said to be aPCl-mild solution of the system (3.1) ifxsatisfies the following integral equation:

x(t)=x0+

t

0S(s)x1ds+

t

0

t

τS(s−τ)

,x(τ), ˙x(τ)+B(τ)u(τ)ds dτ

+

0<ti<t

J0

i

xti

+

t

ti

Ss−ti

J1

i

˙

xti

ds

.

(3.2)

For the forthcoming analysis, we need the following assumptions: [B]:B∈L∞(I, £(Y,X));

[F]: (1) f :I×X×X→Xis measurable int∈Iand locally Lipschitz continuous with respect to last two variables, that is, for allx1,x2,y1,y2∈X, satisfyingx1,x2,y1,

y2 ≤ρ, we have

f t,x1,y1

−ft,x2,y2≤L(ρ)x1−x2+y1−y2; (3.3)

(2) there exists a constanta >0 such that

f(t,x,y)a

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[J]: (1)Ji0(J1

i) :X→X(i=1, 2,. . .,n) map bounded set ofXto bounded set ofX; (2) There exist constantse0i,e1i 0 such that mapsJi0,Ji1:X→Xsatisfy

J0

i(x)−Ji0(y)≤e0ix−y, Ji1(x)−Ji1(y)≤e1ix−y ∀x,y∈X(i=1, 2,. . .,n). (3.5)

Similar to the proof of existence of mild solution for the first-order impulsive evolution equation (see [16]), one can verify the basic existence result. Here, we have to deal with spacePC1

l(I,X) instead.

Theorem3.2. Suppose thatAis the infinitesimal generator of aC0-semigroup. Under

as-sumptions [B], [F], and [J](1), the system (3.1) has a uniquePCl-mild solution for every

u∈Uad.

Proof. Consider the mapHgiven by

(Hx)(t)=x0+

t

0S(s)x1ds+

t

0

t

τS(s−τ)

,x(τ), ˙x(τ)+B(τ)u(τ)ds dτ (3.6)

on

Bx0,x1, 1

=x∈C10,T1

,X|x˙(t)−x1+x(t)−x01, 0≤t≤T1

, (3.7)

whereT1would be chosen. Using assumptions and properties of semigroup, we can show

thatHis a contraction map and obtain local existence of mild solution for the following differential equation without impulse:

¨

x(t)=Ax˙(t) +ft,x(t), ˙x(t)+B(t)u(t), t∈(0,T],

x(0)=x0, x˙(0)=x1, u∈Uad.

(3.8)

The global existence comes from a priori estimate of mild solution in spaceC1(I,X) which

can be proved by Gronwall lemma.

Step by step, the existence ofPCl-mild solution of (3.1) can be derived.

Letxudenote thePC

l-mild solution of system (3.1) corresponding to the controlu∈

Uad, then we consider the Lagrange problem (P):

findu0U

adsuch that

Ju0J(u), ∀uU

ad, (3.9)

where

J(u)= T

0 l

t,xu(t), ˙xu(t),u(t)dt. (3.10)

Suppose that

[L]: (1) the functionall:I×X×X×Y→R∪ {∞}is Borel measurable;

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(4) there exist constantsb≥0,c >0 andϕ∈L1(I,R) such that

l(t,x,y,u)≥ϕ(t) +bx+y+cuYp ∀x,y∈X,u∈Y. (3.11)

Now we can give the following result on existence of the optimal controls for problem (P).

Theorem3.3. Suppose thatAis the infinitesimal generator of a compact semigroup. Under assumptions [F], [L], and [J](2), the problem(P)has a solution.

Proof. If inf{J(u)|u∈Uad} =+, there is nothing to prove.

We assume that inf{J(u)|u∈Uad} =m <+. By assumption [L], we havem >−∞.

By definition of infimum, there exists a sequence{un} ⊂U

ad such thatJ(un)→m.

Since{un}is bounded inLp(I,Y), there exists a subsequence, relabeled as{un}, andu0

Lp(I,Y) such that

un w−→u0 inL

p(I,Y). (3.12)

SinceUadis closed and convex, from the Mazur lemma, we haveu0∈Uad.

Supposexnis thePC

l-mild solution of (3.1) corresponding toun(n=0, 1, 2,. . .). Then

xnsatisfies the following integral equation

xn(t)=x0+

t

0S(s)x1ds+

t

0

t

τS(s−τ)

,xn(τ), ˙xn(τ)+B(τ)un(τ)ds dτ

+

0<ti<t

J0

i

xnt

i

+

0<ti<t

t

ti

Ss−ti

J1

i

˙

xnt i

ds.

(3.13)

Using the boundedness of{un}andTheorem 3.2, there exists a numberρ >0 such that

xn PC1

l(I,X)≤ρ. Define

ηn(t)=

t

0

t

τS(s−τ)B(τ)u

n(τ)ds dτ

t

0

t

τS(s−τ)B(τ)u

0(τ)ds dτ. (3.14)

According toLemma 2.3, we have

ηn−→0 inC(I,X) asun w−→u0. (3.15)

By assumptions [F], [J](2),Theorem 3.2, and Gronwall lemma with impulse (see [17, Lemma 1.7.1]), there exists a constantM >0 such that

xn(t)x0(t)+x˙n(t)x˙0(t)Mη

nC1(I,X), (3.16)

that is,

xn−→x0 inPC1

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SincePC1

l(I,X)L1(I,X), using the assumption [L] and Balder’s theorem (see [18]),

we can obtain

m=lim n→∞

T

0 l

t,xn(t),un(t)dt≥ T

0 l

t,x0(t),u0(t)dt=Ju0≥m. (3.18)

This means thatJattains its minimum atu0U

ad.

4. Necessary conditions of optimality

In this section, we present necessary conditions of optimality for Lagrange problem (P). Let (x0,u0) be an optimal pair.

[F]f satisfies the assumptions [F], f is continuously Frechet differentiable atx0and

˙

x0, respectively,f0

x ∈L1(I, £(X)),fx˙0∈L∞(I, £(X)), fx0(ti±0)= fx0(ti), fx˙0(ti±0)=fx˙0(ti) forti∈Θ, where fx0(t)=fx(t,x0(t), ˙x0(t)), fx˙0(t)=fx˙(t,x0(t), ˙x0(t)).

[L]lis continuously Frechet differentiable onx, ˙xandu, respectively,l0

x(·)∈L1(I,

X∗),l0 ˙

x(·)∈W1,1(I,X∗),l0u(·)∈L1(I,Y∗),lx0˙(T)∈X∗,lx0˙(ti±0)=l0x˙(ti) forti∈Θ, where

l0

x(·)=lx(·,x0(·), ˙x0(·),u0(·)), l0x˙(·)=lx˙(·,x0(·), ˙x0(·),u0(·)), lu0(·)=lu(·,x0(·), ˙x0(·),

u0(·)).

[J] J0

i(Ji1) is continuously Frechet differentiable on x0( ˙x0), and Ji10x˙(ti)D(A∗)

D(A∗), whereJix00(ti)=Jix0(x0(ti)),Ji10x˙(ti)=Ji1x˙( ˙x0(ti)) (i=1, 2,. . .,n).

In order to derive a priori estimate on solution of adjoint equation, we need the fol-lowing generalized backward Gronwall lemma.

Lemma4.1. Letϕ∈C(I,X∗)satisfy the following inequality:

ϕ(t)

X∗≤a+b T

t

ϕ(s)

X∗ds+c T

t

ϕs

B0ds ∀t∈I, (4.1)

wherea,b,c≥0are constants, andϕsB0=sups≤τ≤Tϕ(τ)X∗. Then ϕ(t)

X∗≤aexp

(b+c)(T−t). (4.2)

Proof. Settingϕ(T−t)(t) fort∈I,ψtB=sup0≤τ≤tϕ(τ)X∗, we have

ψ(t)

X∗≤a+b t

0

ψ(s)

X∗ds+c t

0

ψs

Bds. (4.3)

UsingLemma 2.4, we obtain

ψ(t)

X∗≤aexp

(b+c)t; (4.4)

further,

ϕ(t)

X∗≤aexp

(b+c)(T−t). (4.5)

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LetXbe a reflexive Banach space, letA∗be the adjoint operator ofA, and let{S∗(t),t

0}be the adjoint semigroup of{S(t),t≥0}. It is aC0-semigroup and its generator is just

A∗(see [14, Theorem 2.4.4]).

We consider the following adjoint equation:

ϕ(t)= −A∗ϕ(t)−f0

Lemma4.2. Assume thatXis a reflexive Banach space. Under the assumptions [F∗], [L∗], [J∗], the evolution (4.6) has a uniquePCr-mild solutionϕ∈PCr1(I,X∗).

Proof. Consider the following equation:

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where

giψsi,ψsi=A∗+fx˙0

tiJi10x˙

ti−Jix00

tiA∗+ fx˙0

tiψsi

+J00

ix

ti

ψti

−J00

ix

ti

l0

˙

x

ti

,

F(s)=

T

T−s

f0

x (θ)ψ(T−θ) +l0x(θ)−l0

˙

x(θ)

+l0

˙

x(T).

(4.11)

Obviously, ifϕis the classical solution of (4.9), then it must be thePCr-mild solution of (4.6). Now we show that (4.9) has a unique classical solutionϕ∈PC1(I,X)PC(I, D(A∗)).

Fors∈[0,sn], prove that the following equation:

ψ(s)=A∗ψ(s) +f0

˙

x (T−s)ψ(s) +F(s),

ψ(0)=0, (4.12)

has a unique classical solutionψ∈C1([0,s

n],X∗)C([0,sn],D(A∗)) given by

ψ(s)= s

0S

(sτ)f0

˙

x (T−τ)ψ(τ) +F(τ)

dτ. (4.13)

By following the same procedure as in [16, Theorem 4.A], one can verify that (4.12) has a unique mild solutionψ∈C([0,sn],X∗) given by expression (4.13).

By the definition ofF, it is easy to see thatF∈L1([0,sn],X∗)

C((0,sn),X∗). Using (4.13) and the basic properties ofC0-semigroup, we obtainψ(s)∈D(A∗) fors∈[0,sn] and

ψ(s)= f0

˙

x (T−s)ψ(s) +F(s) +A∗

s

0S

(sτ)f0

˙

x (T−τ)ψ(τ) +F(τ)

dτ. (4.14)

This impliesψ∈C1((0,s

n),X∗) andψ(sn−)(sn). Using [14, Theorem 5.2.13], (4.12) has a unique classical solutionψ∈C1((0,s

n),X∗)

C([0,sn],D(X∗)) given by the expres-sion (4.13). In addition, the expressions (4.13) and (4.12) implyψ(0)=0,ψ(0)=l0

˙

x(T), andψ(sn−0),ψ(sn−0) exist. Furthermore,ψ∈C1([0,sn],X∗)C([0,sn],D(A∗)).

By assumption [J], we have

ψ0

n=ψ

sn+Jn10x˙

tnψsn∈D(A∗), ψn1

sn+gnψsn,ψsn∈X∗. (4.15)

Fors∈(sn,sn−1], consider the following equation:

ψ(s)=A∗+f0

˙

x (T−s)

ψ(s) +

T−sn

T−s

f0

x (θ)ψ(T−θ) +l0x(θ)−l0

˙

x(θ)

+ψ1

n,

ψsn+

=ψn0,

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that is, study the following equation:

By following the same procedure as on time interval [0,sn], it has a unique classical solu-tion given by

It has a unique classical solution given by

ψ(s)=S∗s−si

Repeating the procedure till the time interval which is expanded, and combining all of the solutions on [ti,ti+1] (i=0, 1,. . .,n), we obtain classical solution of (4.10) given by For simplicity, we have the following result.

Remark 4.3. ThePC-mild solutionϕof (4.6) can be rewritten as

ϕ(t)=

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Theorem4.4. Suppose bothXandY be reflexive Banach spaces. Under the assumption of Theorem 3.2and assumptions [B], [F∗], [L∗], and [J∗], then, in order that the pair{x0,u0}

be optimal, it is necessary that there exists a functionϕ∈PC1

r(I,X∗)

PCr(I,D(A∗))such

that the following evolution equations and inequality hold:

¨

l-mild solution of (3.1) corresponding to the control. Using assump-tion [J],Jis Gateaux differentiable, and the G-derivative ofJatu0in the directionuu0

can be given by

lim tionu−u0which satisfies the following equation:

¨

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by

Sinceu0is the optimal control, we have the following inequality:

T

Due to the reflexivity of Banach spaceX, we have the Yosida approximationλkR(λk,

A∗)→I∗asλk→ ∞, whereR(λk,A∗) is the resolvent ofA∗forλk∈ρ(A∗) andI∗stands for the identity operator inX∗. Consider the Yosida approximation of f0

x , fx˙0,lx0,l0

Consider the following evolution equation:

ϕk(t)= −A∗(t)ϕk(t)

Similar to the proof ofLemma 4.2, one can show that (4.31) has a unique class solution

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Next, show that

ϕk−→ϕ inPCr1

I,X∗asλk−→ ∞. (4.34)

Employing the method of proof forLemma 4.2, there exists a numberM0>0 such that

ϕPC1(I,X),ϕkPC1(I,X)≤M0 (k=1, 2,. . .). (4.35)

Setting

Fk(t)=

T

t

fk∗

x (s)ϕk(s) +lkx(s)−lk

˙

x(s)

ds+lk

˙

x(T) (k=0, 1,···),

ak=lxk−l

k

˙

x −lx0+l0

˙

xL1(I,X∗)+l

k

˙

x(T)−l0x˙(T)X∗+M0fxk∗−fx0∗L1(I,£(X∗)),

(4.36)

it follows that

Fk(t)F0(t)

X∗

≤ak+fx0∗L1(I,£(X∗))(ϕk)t−ϕtB0+f 0

x L1(I,£(X∗))ϕk(t)−ϕ(t)X∗.

(4.37)

Fort∈[tn,T], we have

ϕk(t)ϕ(t)

X∗≤αTak+αθ

T

t

ϕk(τ)ϕ(τ)

X∗dτ+αθ T

t

ϕk

τ−ϕτB0,

(4.38)

whereθ= f0

x L1([0,T],£(X∗)),α=sup{U∗(t,s)£(X∗)|0≤s≤t≤T}. ByLemma 4.1,

we obtain

ϕk(t)ϕ(t)

X∗≤akαTe2αTθ. (4.39)

Further,

ϕ

k(t)−ϕ(t)X∗≤λake2αTθ, (4.40)

whereω=sup0tTA∗(t)

£(D(A∗),X),λ=(1 +T)(1 +αω+ 2αθ). Hence ϕk(t)ϕ(t)

X∗+ϕk(t)−ϕ(t)X∗≤2λake2αTθ fort∈

tn,T

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Using (4.8), (4.33), and (4.41), we have

By the same procedure, there existsγ >0 such that

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forλk∈ρ(A∗)>0. Taking the limitk→ ∞, we find that

T

0

ϕ(t),B(t)u(t)−u0(t)

X∗,Xdt

= T

0

l0

x(t)−l˙x0˙(t),y(t)

X∗,Xdt+

l0 ˙

x(T),y(T)

X∗,X

n

i=1

l0

˙

x

tilytiX,X.

(4.49)

Further,

T

0

lu

t,x0(t),u0(t)+B(t)ϕ(t),u(t)u0(t)

Y∗,Ydt≥0, ∀u∈Uad. (4.50)

Thus, we have proved all the necessary conditions of optimality given by (4.23)–(4.25).

At the end of this section, an example is given to illustrate our theory. Consider the following problem:

2

∂t2x(t,y)

=Δ∂t∂x(t,y)+x2(t,y) + 1 +

∂tx(t,y) 2

+ 1 +u(t,y), y∈Ω,t∈(0, 1]\

1 3,

2 3

,

x(0,y)=0, x i

3+ 0,y

−x

i

30,y

=x

i

3,y

, i=1, 2, y∈Ω,

∂tx(t,y)|t=0=0,

∂tx(t,y)|t=i/3+0

∂tx(t,y)|t=i/30=

∂tx(t,y)|t=i/3, i=1, 2, y∈Ω, x(t,y)|[0,1]×∂Ω=0, ∂t∂x(t,y)|[0,1]×∂Ω=0,

(4.51)

with the cost function

J(u)= 1

0

Ω

x(t,ξ)2

dξ dt+

1

0

Ω

∂t∂x(t,ξ)

2

dξ dt+

1

0

Ω

u(t,ξ)2

dξ dt, (4.52)

whereΩ⊂R3is bounded domain,ΩC3.

For the problem (4.51), one can show the following theorem.

Theorem4.5. In order that the pair{x0,u0} ∈PC1

l([0, 1], L2(Ω))×L2([0, 1],L2(Ω))be

optimal, it is necessary that there exists aϕ∈PC1

(16)

evolution equations and inequality hold:

2

∂t2x

0(t,y)=Δ

∂tx

0(t,y) +x0(t,y)2+ 1 +

∂tx0(t,y) 2

+ 1 +u0(t,y),

y∈Ω,t∈(0, 1]\ 1

3, 2 3

,

x0(0,y)=0, x0

i

3+ 0,y

−x0

i

30,y

=x0

i

3,y

, i=1, 2, y∈Ω,

∂tx

0(t,y)

t=0=0,

∂tx

0(t,y)|

t=i/3+0

∂tx

0(t,y)|

t=i/30=

∂tx

0(t,y)|

t=i/3,

i=1, 2, y∈Ω,

x0(t,y)|

[0,1]×∂Ω=0, ∂t∂x0(t,y)|[0,1]×Ω=0;

2

∂t2ϕ(t,y)= −

∂t

Δϕ(t,y) + (∂/∂t)x

0(t,y)ϕ(t,y)

(∂/∂t)x0(t,y)2+ 1

+ x

0(t,y)ϕ(t,y)

x0(t,y)2+ 1+ 2x

0(t,y) 2

∂t2x

0(t,y), yΩ,t[0, 1)\

1

3, 2 3

,

ϕ

i

30,y

−ϕ

i

3+ 0,y

(t,y)|t=i/3, i=1, 2,y∈Ω,

∂tϕ(t,y)|t=i/30

∂tϕ(t,y)|t=i/3+0= ∂t

ϕ(t,y) + 2x0(t,y)

t=i/3, i=1, 2, y∈Ω,

ϕ(1,y)=0,

∂tϕ(t,y)|t=1=2

∂tx(t,y)|t=1, y∈Ω, ϕ(t,y)|[0,1]×∂Ω=0, ∂t∂ϕ(t,y)|[0,1]×∂Ω=0; 1

0

Ω

2u0(t,ξ) +ϕ(t,ξ),u(t,ξ)−u0(t,ξ)L2(Ω),L2(Ω)dξ dt≥0, ∀u∈Uad.

(4.53)

Acknowledgment

This work is supported by the National Science Foundation Of China under Grant no. 10661004 and the Science and Technology Committee of Guizhou Province under Grant no. 20052001.

References

[1] L. S. Pontryagin, “The maximum principle in the theory of optimal processes,” inProceedings of the 1st International Congress of the IFAC on Automatic Control, Moscow, Russia, June-July 1960. [2] N. U. Ahmed, “Optimal impulse control for impulsive systems in Banach spaces,”International

Journal of Differential Equations and Applications, vol. 1, no. 1, pp. 37–52, 2000.

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[4] A. G. Butkovski˘ı, “The maximum principle for optimum systems with distributed parameters,” Avtomatika i Telemehanika, vol. 22, pp. 1288–1301, 1961 (Russian).

[5] A. I. Egorov, “The maximum principle in the theory of optimal regulation,” inStudies in Integro-Differential Equations in Kirghizia, No. 1 (Russian), pp. 213–242, Izdat. Akad. Nauk Kirgiz. SSR, Frunze, Russia, 1961.

[6] H. O. Fattorini,Infinite Dimensional Optimization and Control Theory, vol. 62 ofEncyclopedia of Mathematics and Its Applications, Cambridge University Press, Cambridge, UK, 1999.

[7] X. Li and J. Yong,Optimal Control Theory for Infinite Dimensional Systems, Systems & Control: Foundations & Applications, Birkh¨auser, Boston, Mass, USA, 1995.

[8] W. Wei and X. Xiang, “Optimal control for a class of strongly nonlinear impulsive equations in Banach spaces,”Nonlinear Analysis, vol. 63, no. 5–7, pp. e53–e63, 2005.

[9] X. Xiang and N. U. Ahmed, “Necessary conditions of optimality for differential inclusions on Banach space,”Nonlinear Analysis, vol. 30, no. 8, pp. 5437–5445, 1997.

[10] X. Xiang, W. Wei, and Y. Jiang, “Strongly nonlinear impulsive system and necessary conditions of optimality,”Dynamics of Continuous, Discrete & Impulsive Systems A, vol. 12, no. 6, pp. 811– 824, 2005.

[11] Y. Peng and X. Xiang, “Second order nonlinear impulsive evolution equations with time-varying generating operators and optimal controls,” to appear inOptimization.

[12] Y. Peng and X. Xiang, “Necessary conditions of optimality for second order nonlinear evolution equations on Banach spaces,” inProceedings of the 4th International Conference on Impulsive and Hyprid Dynamical Systems, pp. 433–437, Nanning, China, 2007.

[13] S. Hu and N. S. Papageorgiou,Handbook of Multivalued Analysis. Vol. I: Theory, vol. 419 of Mathematics and Its Applications, Kluwer Academic Publishers, Dordrecht, The Netherlands, 1997.

[14] N. U. Ahmed,Semigroup Theory with Applications to Systems and Control, vol. 246 ofPitman Research Notes in Mathematics Series, Longman Scientific & Technical, Harlow, UK; John Wiley & Sons, New York, NY, USA, 1991.

[15] X. Xiang and H. Kuang, “Delay systems and optimal control,”Acta Mathematicae Applicatae Sinica, vol. 16, no. 1, pp. 27–35, 2000.

[16] X. Xiang, Y. Peng, and W. Wei, “A general class of nonlinear impulsive integral differential equations and optimal controls on Banach spaces,”Discrete and Continuous Dynamical Systems, vol. 2005, supplement, pp. 911–919, 2005.

[17] T. Yang,Impulsive Control Theory, vol. 272 ofLecture Notes in Control and Information Sciences, Springer, Berlin, Germany, 2001.

[18] E. J. Balder, “Necessary and sufficient conditions forL1-strong-weak lower semicontinuity of

integral functionals,”Nonlinear Analysis, vol. 11, no. 12, pp. 1399–1404, 1987.

Y. Peng: Department of Mathematics, Guizhou University, Guiyang, Guizhou 550025, China Email address:[email protected]

X. Xiang: Department of Mathematics, Guizhou University, Guiyang, Guizhou 550025, China Email address:[email protected]

References

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