(A2)Assume that there exists unique functionsuch that
From(2.2),we can get
Defining the functional I(u,λ),
From the calculus of variations,we can obtain the first order variation of I(u,λ)as
According to the Lagrange theory,a necessary condition for a solution to be optimal is
(A3)Assume thato is uniquely solvable with respect to ui,that is ui=hi(yi,λi,t),i=1,2.
From assumption(A3)and(2.4),we can get the following singularly perturbed boundary value problem
To show the existence of solution for(2.5),we introduce the left and right associated problem with the following boundary value conditions.
Left associated problem P(−)(to≤t≤t1)
and right associated problem P(+)
which satisfy the conditions y2(t1)=y1(t1),λ2(t1)=λ1(t1).
By assumption(A2),we obtain that the reduced problem
which has a unique solution
(A4)Assume that the matrix gixi(¯xi(t),t)has 2n real valued eigenvalues¯λij(t),j= 1,2,···,2n,where
3 Construction of Asymptotic Solution
According to the boundary function method[18],we suppose that the formal asymptotic series for the boundary value problems(2.6)and(2.7)have the form
where τo=tµ−1,τ=(t−t1)µ−1,τ1=(t−t2)µ−1,¯xki(t)are coefficients of regular terms, Lkx1(τo)and Rkx2(τ1)are coefficients of boundary layer terms at t=toand t=t2,Qkxi(τ) are left and right coefficients of internal transition terms at t=t1,i=1,2.
Substituting the asymptotic solution(3.1)into(2.6)and(2.7)and separating the terms on t,τo,τ and τ1by the boundary layer function method,then equating the terms with like
powers ofµ,we can obtain a series of boundary value problems to determine
The equations to determine the zero-order coefficients of regular termsi=1,2 are given by
From assumption(A2),we have
Next,we give the equations and their conditions for determining the zero order coefficients of left boundary layer and internal transition layer of left side as follows
The first order approximation system of(3.3)isUsing assumption(A4),we know that there exists an n dimensional unstable invariant manifold U in the neighborhood ofβ1(t1),t1,we suppose that it can be written as on G1,where G1is some neighborhood of Qoλ1(τ).
In order to guarantee the existence of solution for(3.2)and(3.3),we give the following condition.
(A5)Assume thatare stable manifold of(3.2)near the equilibrium point β1(to)and Qoλ1(o)=λo−α1(t1)∈G1.
The following boundary value problems to determine Qoy2(τ),Qoλ2(τ),Roy2(τ2), and Roλ2(τ2)are given by Similarly,we know that there exists an n dimensional stable invariant manifold S in the neighborhood of?β2(t1),t1?,we suppose that it can be written as on G2,where G2is some neighborhood ofare unstable manifold of(3.5)near the equilibrium point β2(t2)and Qoy2(o)=po−φ2(t1)∈G2.
For the high order terms of P(−),we have the equations and their boundary conditions as follows:are the known functions depending only on¯xp1(t),Lpx1(τo),Qpx1(τ)and tp(p=o,1,2,···,k−1).Consider equations(3.8),they are first order linear inhomogeneous differential equations,the inhomogeneous term QFk(τ)is a known vector functions.The homogeneous equations of(3.8)are variational equations of(3.3).Therefore,by the result of Vasil’eva,Butuzov[21],we obtain that there exists a unique solution Qkx1for(3.8),meanwhile,
where δkis a determined constant depending on Φ1,QFk(τ),C and kpare positive constants.
Similarly,we can get the left boundary layer terms Lkx1(τo),so far we constructed the asymptotic solution of P(−).
For the high order approximate equation of Qkx2(τ),the initial condition for the existence of a unique solution is
where σkis a known constant.
Similar to the above discussion,we can get the equations and boundary conditions to determine right boundary layer coefficients Rkx2(τ1),here the details are omitted.Then,we have thus far constructed the formal asymptotic solution for the problems P(−)and P(+).By means of the expressions yi,λiand ui=hi(yi,λi,t),the asymptotic expansion of ui,i=1,2 can be obtained.It should be noted that the formal asymptotic solution contains the unknown parameters λ∗and p∗.
Next,we will determine the vector parameters λ∗and p∗by continuity of solution,that is
then equating the terms with like powers ofµ,we obtain the following equations
Equating the terms with like k-th powers ofµ,we get the equations
In order to ensure that there exist solutions for equations(3.1o)and(3.11),the following assumptions are needed.
(A7)Assume that there exists a unique solution for the vector equations
(A8)Assume that the matrices E−AB and E−BA are invertible.
By virtue of(A8),the unknown parameters pkand λkcan be solved from(3.11),.So far,we have determined all the parameters pkand λk,k≥1.
4 Existence and Formal Asymptotic Expansion for Solution
We will use the sewing method to prove the existence of solution for(2.5),meanwhile, the asymptotic expansion will be given.Let x∗=xo+µx1+···+µNxN,here,we do not expand xN,the purpose is to prove the existence of xN,then we will prove the existence for x∗.Consider the difference value function
Let the right hand side of above equation be equal to zero,we can obtain
here,△x|t=t1=o,that is,the value of asymptotic solutions for P(−)and P(+)are equal at the point t1.
In[21],the authors proved the existence of solution for the two point boundary value problem,which satisfies the stability condition.Moreover,the authors showed the uniformly valid asymptotic solution for the boundary value problem.In this paper,we divide problem (2.5)into two boundary value problems,which satisfy the stability conditions.Then,we have the following theorem
Theorem 4.1Assume that(A1)–(A8)hold.Then,for sufficiently smallµ>o,there exists a unique solution x(t,µ)for(2.1).Moreover,the following asymptotic expansion holds
5 Example
Consider the following optimal control problem
whereµ>o is a small parameter.
By using the optimality condition of optimal control problem(5.1),we have
The equations and conditions to determine Qoy1and Qoλ1are given by
For Qoy2and Qoλ2,we have the equations and boundary conditions as follows
By means of y2(1)=y1(1),λ2(1)=λ1(1),we obtain that
Similarly,we get
From the optimality condition,we know that u1+λ1=o,u2+λ2=o,then we have the asymptotic solution for(5.1),
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∗December 6,2014;revised April 25,2016.This project is supported by the National Natural Science Foundation of China(11471118,11401385 and 11371140),Natural Science Foundation of Hebei Province (A2015407063)and Doctoral Foundation of Hebei Normal University of Science and Technology(2013YB008).