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DOI: 10.2478/v10006-010-0017-3

ON ONE ALGORITHM FOR SOLVING THE PROBLEM OF SOURCE FUNCTION RECONSTRUCTION

V

YACHESLAV

MAKSIMOV

Institute of Mathematics and Mechanics

Ural Branch of the Russian Academy of Sciences, 16 S. Kovalevskoi Str., Ekaterinburg, 620219 Russia e-mail:

maksimov@imm.uran.ru

In the paper, the problem of source function reconstruction in a differential equation of the parabolic type is investigated.

Using the semigroup representation of trajectories of dynamical systems, we build a finite-step iterative procedure for solving this problem. The algorithm originates from the theory of closed-loop control (the method of extremal shift). At every step of the algorithm, the sum of a quality criterion and a linear penalty term is minimized. This procedure is robust to perturbations in problems data.

Keywords: reconstruction, source function, feedback control.

1. Introduction and problem formulation

In the theory of differential equations, the following prob- lem is well-known: it is required to determine parameters of a differential equation provided a given function plays the role of its solution. Unknown parameters (generally speaking, not constant and depending on time) can be con- trols, dynamical disturbances, coefficients, some system characteristics and so on. As a rule, such problems are ill-posed. First, a number of parameter values may corre- spond to a given solution. This property rather often re- sults in a new problem of choosing parameters. For exam- ple, in the problem of control reconstruction, the interest is usually in finding a control with an extremal (maximal or minimal) energy resource. Second, the mapping “solu- tion −→ parameter” is discontinuous in the general case.

Therefore, this mapping cannot be used to approximate a desired parameter in the case when a disturbed solution is given instead of an exact one. If some function, which is not a solution, is given instead of a disturbed solution of an equation, additional difficulties arise. Under such con- ditions, the “approximative” feature should be provided by some regularizing procedures. Besides, there exists the problem of sufficiently convenient and constructive description and determination of the mapping “solution

−→ parameter”. Issues of determining some parameters through equation solutions are often called reconstruction (identification) problems. Recently, methods of solving reconstruction problems have been intensively developed.

A considerable number of works is devoted to solving problems of reconstructing right-hand parts (e.g., a source function) of parabolic equations through results of sensor observations. A typical problem from this field is as fol- lows.

Let us imagine a water reservoir occupying an area Ω and n contamination sources located in subareas Ω

1

, . . . , Ω

n

of Ω. It is assumed that an input concentration rate of some contaminant at every point ξ in the source area Ω

j

is modeled as u

j

( t)ω

j

( ξ), where t is current time. The positive function u

j

( t) is a measure of the time- varying intensity of the source located in Ω

j

; u

j

( t) repre- sents the current rate of the contamination inflow in Ω

j

. Let x(t, ξ) be the current concentration of the contaminant at a point ξ in Ω. Some information on the distribution of x(t, ξ) in Ω is registered by m sensors. The sensors reg- ister weighted average concentrations z

1

( t), . . . , z

m

( t) in fixed subareas Θ

1

, . . . , Θ

m

of Ω:

z

k

( t) =



Θk

p

k

( ξ)x(t, ξ) dξ, k = 1, . . . , m,

the positive weight coefficients p

k

( ξ) are supposed to

be given. The problem of reconstructing the right-

hand part (the intensity reconstruction problem) is as

follows. Observing the weighted average concentra-

tions z

1

( t), . . . , z

m

( t) of the contaminant in the areas

Θ

1

, . . . , Θ

m

, reconstruct the intensities of the contam-

ination sources, u

1

( t), . . . , u

n

( t), in the source areas

(2)

Ω

1

, . . . , Ω

m

. This problem has been studied by many au- thors (see, e.g., (Omatu and Seinfeld, 1989; Korbicz and Zgurowski, 1991; Uci´nski, 1999)).

In the present work, a new algorithm for solving such a problem for an abstract parabolic equation is suggested.

A particular case of such an equation is a diffusion equa- tion describing the process of contaminant propagation in the atmosphere or liquid media. This algorithm rests upon constructions of the theory of stable dynamical in- version based on the combination of methods of the theory of ill-posed problems and that of positional control. The essence of the technique described in (Blizorukova and Maksimov, 1998; Digas et al., 2003; Kryazhimskii and Osipov, 1987; Kryazhimskii et al., 1997) is that a recon- struction algorithm is represented as a control algorithm for some auxiliary dynamical system. It should be noted that this technique exploits the idea of stabilizing appro- priate functionals of the Lyapunov type by means of ex- tremal shift (Krasovskii and Subbotin, 1988). Thus, the technique combines the stabilization principle with that of extremal shift in some scheme of control with a model.

In the beginning, some functional treated as a Lyapunov type one is introduced. Then, a control law for an auxil- iary system is chosen. This law uses the idea of extremal shift providing a “weak growth” of the functional in time.

Let us pass to the statement of the problem under in- vestigation. In a real Hilbert space ( H, | · |

H

), the follow- ing parabolic equation is considered:

x(t) + Ax(t) = Bu(t) + f(t), ˙ (1) t ∈ T = [0, ϑ], x(0) = x

0

∈ H.

Here, A : V → V

is a linear continuous symmetric oper- ator satisfying (for some c > 0 and λ ∈ R) the coercivity condition

Ay, y

V

+ λ|y|

2H

≥ cy

2

, ∀y ∈ V.

( V,  · ) is a separable and reflexive Banach space, which is densely and continuously embedded in the space H identified with its conjugate space (H = H

); ·, ·

V

is the duality between V and V

; x(t) is the phase state of the system (1) at the moment t; u(t) ∈ U is a dis- turbance generating the motion x(·); the space of distur- bances (U, | · |

U

) is a Hilbert space with a scalar prod- uct (·, ·)

U

; f(·) ∈ L

2

( T ; H) is a given input action;

B : U → H is a linear continuous operator.

A solution of the system (1) (which is understood in the weak sense) is defined to be a unique continuous func- tion x(·) = x(·; x

0

, u(·)) of the form

x(t) = S(t)x

0

+



t 0

S(t−τ)(Bu(τ)+f(τ)) dτ, t ∈ T.

Here S(t) : H → H (t > 0) is the semigroup of con- tinuous linear operators generated by the operator A. As is

known (Bensoussan et al., 1992), for all u(·) ∈ L

2

( T ; U), f(·) ∈ L

2

( T ; H), x

0

∈ H, there exists a unique solu- tion of the system (1). Below it is assumed that the set of admissible system inputs u(·) is of the form

U

= {u(·) ∈ L

2

( T ; U) : u(t) ∈ P for a. a. t ∈ T }, P ⊂ U is a convex bounded and closed set.

The problem under consideration consists in the fol- lowing. Let Eqn. (1), an action f(·), an initial state x

0

, and the set of admissible inputs U

be known. In addition, at moments t ∈ T , values

z(t) = Gx(t) (2)

are inaccurately measured. Here G is a given linear con- tinuous operator acting from the space of states H into a Hilbert space of measurements H

1

. Results of the mea- surements ξ

h

( t) are, generally speaking, inaccurate:

h

( t) − z(t)|

H1

≤ h, t ∈ T. (3) Here h is the measurement accuracy.

Let U

z

be the set of all admissible inputs u(·) com- patible with some output z(·), i.e.,

U

z

= {u(·) ∈ U

: Gx(t; 0, x

0

, u(·)) = z(t), ∀t ∈ T },

J(u(·)) =



ϑ 0

ω(t, u(t)) dt (4)

is a given performance index. Here ω(·, ·) : T × U → R

+

= [0 , +∞) is a functional, which is convex with re- spect to the second argument. It is assumed that the func- tional J(u(·)) is defined on the set U

and is lower semi- continuous. It is necessary to construct a stable algorithm for calculating an extremal value

J

z0

= min {J(u(·)) : u(·) ∈ U

z

} (5) and an extremal input action u

0

( ·) ∈ U

0

( z), where

U

0

( z) = arg min{J(u(·)) : u(·) ∈ U

z

}.

Since the functional J is convex and the set U

is bounded and closed, the set U

0

( z) is a non-empty convex and closed set. Therefore, the problem in question has a solution. However, the precise calculation of J

z0

and u

0

( ·) is impossible, in particular, due to inaccuracies in mea- suring the values z(t), t ∈ T (see (3)). In this case, it is necessary to design a stable algorithm for approximate determination of the value J

z0

and the extremal input ac- tion u

h

( ·) = u(·; ξ

h

( ·)). The stability of the algorithm is understood in the following sense:

J(u

h

( ·)) → J

z0

, u

h

( ·) → U

0

( z)

weakly in L

2

( T ; U) as h → +0.

(3)

241 The last relation means that any convergent (in L

2

( T ; U))

sequence {u

hl

( ·)}, h

l

→ +0 as l → +∞, converges to some element from the set U

0

( z). Below we present an algorithm for solving the problem considered in the case when the operators A and B, as well as the functional J and the initial state x

0

, are inaccurately known.

Note that the problem of source function reconstruc- tion formulated above can be interpreted as an optimal control problem for the parabolic equation (1) subject to state constraints. Then the performance index takes the form (4), whereas the state constraints are given by (2). A solving algorithm suggested in the paper is oriented to the case of inaccurate data on the problem parameters, i.e., on the system structure, the quality criterion, and the state constraints.

2. Auxiliary results

Before passing on to solving the problem in question, let us give auxiliary statements. Introduce the operator F : L

2

( T ; U) → L

2

( T ; H

1

) and the element b(·) ∈ L

2

( T ; H

1

):

( F u(·))(η) =



η 0

GS(η − t)Bu(t) dt, η ∈ T, u(·) ∈ U

,

b(η) = z(η) − GS(η)x

0

, η ∈ T.

Here the function z is defined by (2). Then the problem of calculating the extremal value J

z0

and extremal input ac- tion u

0

( ·) ∈ U

0

( z) is equivalent to the following extremal problem.

It is required to find

u

0

= arg min {J(u) : u ∈ U

, F u = b}

and

J

0

= min {J(u) : u ∈ U

, F u = b},

where J is the quality criterion (4). Note that the set {u ∈ U

: F u = b} is non-empty. Therefore, there exists a solution to the last problem, and J

0

= J

z0

(see (5)). If the function ω(·, ·) is strictly convex with respect to the second argument, then the set U

0

( z) is a singleton and, in addition, u

0

= u

0

= U

0

( z).

Let non-negative numbers ν

F

, ν

b

, and ν

J

, linear con- tinuous operators F

ν

: L

2

( T ; U) → L

2

( T ; H

1

), elements b

ν

∈ L

2

( T ; H

1

), and convex functionals J

ν

( ·) defined on U

be given in such a way that

|F

ν

u − F u|

L2(T ;H1)

≤ ν

F

, ∀ u ∈ U

, (6)

|b

ν

− b|

L2(T ;H1)

≤ ν

b

, (7)

|J

ν

( u) − J(u)| ≤ ν

J

, ∀ u ∈ U

. (8)

For simplicity, in what follows it is assumed that ν

F

, ν

b

, ν

J

∈ [0, 1).

Our goal is to design an algorithm for approxi- mate determination of the value J

0

and the element u

0

. Namely, it is required to construct an algorithm which, us- ing values F

ν

, b

ν

, and J

ν

known instead of F , b, and J, forms elements {u

j

} ∈ U

, j = 1, . . ., with the properties

|F u

j

− b|

L2(T ;H1)

→ 0, (9) J(u

j

) → J

0

as j → +∞, (10) if ν

F

= ν

jF

→ 0, ν

b

= ν

bj

→ 0, and ν

J

= ν

Jj

→ 0 as j → +∞.

Let us pass on to the description of this algorithm.

Set

K

0

= sup {J(u) : u ∈ U

},

U

γ

= {u ∈ U

: |F u − b|

L2(T ;H1)

≤ γ}, J

0

( γ) = inf{J(u) : u ∈ U

γ

}.

From the results of (Vasiliev, 1981, p. 182), we obtain what follows.

Theorem 1. Let u

j

∈ U

, α

j

> 0, γ

j

> 0, |J

νj

( u) − J(u)| ≤ ν

jJ

∀u ∈ U

,

|F u

j

− b|

2L2(T ;H1)

+ α

j

J(u

j

) − α

j

J

0

≤ γ

j

, ν

jJ

→ 0, α

j

→ +0, γ

j

→ +0, (11)

γ

j

j

→ 0 as j → +∞.

Then we have

(a) J

νj

( u

j

) → J

0

as j → +∞, (b)

J

0

(( γ

j

+ 2 K

0

α

j

)

1/2

) − ν

jJ

≤ J

νj

( u

j

) ≤ J

0

+ γ

j

j

+ ν

Jj

. Any element w

∈ W is called an ε-solution (ε > 0) of the extremal problem ϕ(w) → inf, w ∈ W = ∅, if ϕ(w

) ≤ inf{ϕ(w) : w ∈ W } + ε. We denote by the symbol Y

jν

( δ, α, ε) the set of elements y

i

, i = 0, 1, . . . , j, from U such that

y

0

= 0 , (12)

y

i+1

= y

i

+ u

i

δ, i = 0, 1, . . . , j − 1, (13) where u

i

is an ε-solution of the problem

2 F

ν

y

i

− iδb

ν

, F

ν

u + αJ

ν

( u) → inf, u ∈ U

. (14) Hereinafter, the symbol ·, · denotes the scalar product in L

2

( T ; H

1

).

Let

K

1

= |b|

L2(T ;H1)

, |F u|

L2(T ;H1)

≤ K

2

∀u ∈ U

.

Based on the approach from (Kryazhimskii and Osipov,

1987; Kryazhimskii et al., 1997), the following lemma is

proved.

(4)

Lemma 1. The inequality

|F (y

j

/(δj)) − b|

2L2(T ;H1)

+ α{J(y

j

/(δj)) − J

0

}/(δj) ≤ δ

j

is valid for any j ≥ 1, where

δ

j

= k

1

ν

F

+ k

2

ν

b

+ ( k

3

( ν

F

)

2

+ 2 αν

J

) /(jδ) + k

4

/j + ε/(δj),

k

1

= 4( K

1

+ 2 K

2

) , k

2

= K

2

+ 1 , k

3

= 4 ,

k

4

= ( K

1

+ K

2

)

2

.

Proof. Let us estimate the change of the value Λ

i+1

= |F (y

i

+ δu

i

) − t

i+1

b|

2L2(T ;H1)

+ α

t



i+1

0

J( ˙y(τ)) dτ − αJ(u

0

) t

i+1

= Λ

i

+ μ

i

+ δ

2

|F u

i

− b|

2L2(T ;H1)

, i ≥ 0, where

y(t) = u ˙

i

for t ∈ [t

i

, t

i+1

) , i = 0, 1, . . . , t

i

= iδ, y(0) = 0,

μ

i

= 2 F y

i

− t

i

b, F u

i

− bδ + αδ{J(u

i

) − J(u

0

) }.

Since u

0

is a solution of the problem under consideration, the equality

F u

0

= b is fulfilled. Therefore,

μ

i

= 2 F y

i

− t

i

b, F u

i

− bδ − 2F y

i

− t

i

b, F u

0

− bδ + αδ{J(u

i

) − J(u

0

) }

= 2 F y

i

− t

i

b, F u

i

δ + αδJ(u

i

)

− 2F y

i

− t

i

b, F u

0

δ − αδJ(u

0

) . Moreover,

λ

i

≡ 2F y

i

− t

i

b, F u

i

δ + αJ(u

i

) δ

− 2F

ν

y

i

− t

i

b

ν

, F

ν

u

i

δ + αJ

ν

( u

i

) δ =



3 j=1

λ

(j)

,

λ

(1)i

= 2 F y

i

− t

i

b, (F − F

ν

) u

i

δ,

λ

(2)i

= 2 (F − F

ν

) y

i

− t

i

( b − b

ν

) , F

ν

u

i

δ, λ

(3)i

= α{J(u

i

) − J

ν

( u

i

) }δ.

In addition, by (6) we obtain

|F y

i

|

L2(T ;H1)

= | 

i−1

j=0

F u

j

δ|

L2(T ;H1)

≤ t

i−1

K

2

,

|(F − F

ν

) y

i

|

L2(T ;H1)

=  



i−1 j=0

( F − F

ν

) u

j

δ  

L2(T ;H1)

≤ ν

F

t

i

,

|F

ν

u|

L2(T ;H1)

≤ |(F

ν

− F )u|

L2(T ;H1)

+ |F u|

L2(T ;H1)

≤ K

2

+ ν

F

, u ∈ U

.

Note that, due to the convexity and completeness of the set P , the rule for choosing the elements u

i

implies the inclusion y

i

/(δi) ∈ U

. Thus, we have (see (6)–(8))

λ

(1)i

≤ 2(K

2

+ K

1

) ν

F

δt

i

, λ

(2)i

= 2( ν

F

+ ν

b

)( K

2

+ ν

F

) δt

i

, λ

(3)i

≤ αδν

F

.

Therefore,

λ

i

≤ δν

F

K

1i

+ δν

b

K

2i

+ αν

J

δ, where

K

1i

= 2((2 K

2

+ K

1

) t

i

+ ν

F

) , K

2i

= 2 t

i

( K

2

+ ν

F

) δ.

A similar estimate holds if we replace u

i

by u

0

. Hence, μ

i

≤ 2F

ν

y

i

− t

i

b

ν

, F

ν

u

i

δ − 2F

ν

y

i

− t

i

b

ν

, F

ν

u

0

+ αδ{J

ν

( u

i

) − J

ν

( u

0

) } + 2 {K

1i

ν

F

+ K

2i

ν

b

+ αν

J

}δ.

From (14) we deduce that

μ

i

≤ 2{K

1i

ν

F

+ K

2i

ν

b

+ αν

J

}δ + εδ.

It is easily seen that

|F u

i

− b|

2L2(T ;H1)

δ

2

≤ {(K

2

+ K

1

) δ}

2

. In addition, due to the convexity of J, we obtain

J(y(t)/t) = J  1 t



t 0

y(τ) dτ ˙ 

1 t



t 0

J( ˙y(τ)) dτ.

(15) Accordingly,

Λ

i+1

≤ Λ

i

+ 2 {K

1i

ν

F

+ K

2i

ν

b

+ αν

J

+ {(K

2

+ K

1

) δ}

2

+ εδ

≤ Λ

i

+ 2 {2((2K

2

+ K

1

)( iδ + ν

F

) ν

F

δ + 2 iδ(K

2

+ ν

F

) ν

b

δ + αν

J

δ}

+ {(K

2

+ K

1

) δ}

2

+ εδ, i ≥ 0.

Using (12), we obtain Λ

0

= 0. Then Λ

i+1

≤ 2{((2K

1

+ 4 K

2

) iδ + 2ν

F

) ν

F

δ

+ 2 iδ(K

2

+ ν

F

) ν

b

δ + αν

J

δ}i

+ {(K

1

+ K

2

) δ}

2

i + εδi, i ≥ 0.

(5)

243 Dividing the right-hand and left-hand sides by t

2i+1

and

using (15), we get

|F (y(t

i+1

) /t

i+1

) − b|

2L2(T ;H1)

+ α/t

i+1

{J(y(t

i+1

) /t

i+1

) − J(u

0

) }

≤ 2  2 K

1

+ 4 K

2

δ + 2 ν

F

( i + 1)δ

2

 ν

F

δ + ε/(δ(i + 1))

+ 4( K

2

+ ν

F

) ν

b

+ 2 αν

J

/((i + 1)δ) + ( K

1

+ K

2

)

2

/(i + 1)

= 4 {(K

1

+ 2 K

2

) ν

F

+ ( K

2

+ ν

F

) ν

b

} + 2 {2(ν

F

)

2

+ αν

J

}/((i + 1)δ) + ( K

1

+ K

2

)

2

/(i + 1) + ε/(δ(i + 1)).



The next theorem follows from Theorem 1 and Lemma 1.

Theorem 2. Let

(a) δ

j

→ +0, ε

j

→ +0 as j → +∞;

(b) sequences

j

} and {γ

j

} satisfy the conditions (11);

(c) inequalities

k

1

ν

jF

+ k

2

ν

jb

+ ( k

3

( ν

Fj

)

2

+ 2 α

j

ν

jJ

) /(jδ

j

) + k

4

/j + ε

j

/(δ

j

j) ≤ γ

j

be true;

(d) {y

i

}

ji=0

= Y

jν

( δ

j

, α

j

, ε

j

).

Then the sequence of elements {u

j

}

+∞j=1

, u

j

= y

j

/(δ

j

j) ∈ U

,

satisfying the conditions (9) and (10), solves the problem of approximate calculation of u

0

and J

0

.

As is seen from Lemma 1 and Theorem 2, choosing appropriate relations between the values δ, i, ν

F

, ν

b

, ν

J

, and α, we provide a “slow” growth of the Lyapunov func- tional

Λ( t) = |F (y(t)/t) − b|

2L2(·;H1)

+ α



t 0

J( ˙y(τ)) dτ/t − αJ(u

0

) /t, t > 0.

The rule (14) for choosing controls u

i

is, in essence, a modification of the extremal shift principle from the the- ory of differential games (Krasovskii and Subbotin, 1988).

Let

ν

1

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) = δ

j

+ 2 K

0

α/(δj), ν

2

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) = δ

j

δj/α.

The next inequalities follow from Lemma 1:

|F (y

j

/(δj)) − b|

2L2(T ;H1)

≤ ν

1

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) , (16) J(y

j

/(δj)) − J

0

≤ ν

2

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) . (17)

The following lemma holds.

Lemma 2. Let ν

jF

→ 0, ν

jb

→ 0, ν

jJ

→ 0, α

j

→ +0, α

j

/(δ

j

j) → +0, (δ

j

+ ε

j

)

j

→ +0, ε

j

/(δ

j

j) → +0, ν

jF

j

j

→ 0, ν

bj

j

j

→ 0 as j → +∞.

Then

|F (y

j

/(δ

j

j)) − b|

2L2(T ;H1)

→ 0,

J(y

j

/(δ

j

j)) → J

0

as j → +∞.

Condition 1.

j = j(h) = [1/h], ν

jF

= a

1

h, ν

jb

= a

2

h, ν

jJ

= a

3

h, ε

j

= a

4

δ

j

, α

j

= δ

j1/2

,

δ

j

= h

1−κ

, κ = const ∈ (0, 1).

Here the symbol [1/h] denotes the integer part of 1 /h; a

j

, j = 1, . . . , 4, are some constants. In this case, j = j(h) → +∞ as h → +0 and the elements y

j

/(δ

j

j) depend on h, i.e.,

u

h

= y

j(h)

/(h

1−κ

[1 /h]) ∈ U

. (18) The next statement can be formulated.

Corollary 1. Let Condition 1 be fulfilled and h ∈ (0 , 1 − ε

), ε

= const ∈ (0, 1). Then the inequalities

|F (u

h

) − b|

2L2(T ;H1)

≤ Ch, (19) J(u

h

) − J

0

≤ C

0

h

1/2−κ/2

(20) hold. Here C = C(ε

), C

0

= C

0

( ε

), and the element u

h

is defined by (18).

The validity of Corollary 1 follows from the inequal- ities

ν

1

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) ≤ Ch, ν

2

( α, δ, j, ε, ν

F

, ν

b

, ν

J

) ≤ C

0

h

1/2−κ/2

and the inequalities (16) and (17).

Let a sequence of positive numbers {h

l

}

+∞l=0

, h

l

+0 as l → +∞ be fixed. Let Condition 1 be fulfilled. The symbol y

l

is used for the sequence constructed according to (12)–(14) for j = j

l

= [1 /h

l

], h = h

l

, δ = δ

l

= h

1−κl

, and κ = const ∈ [0, 1). Then the following theorem is valid.

Theorem 3. Let u

l

= y

jl

/(j

l

h

1−κl

), l = 1, 2, . . . . Then any weakly convergent subsequence of the sequence {u

l

}

+∞l=1

weakly converges in L

2

( T ; U) to the set U

0

( z).

If J(u) = |u|

2L2(T ;U)

, then this convergence is strong.

(6)

3. Solving the algorithm

Let us come back to the problem of approximate calculat- ing of the value J

z0

and the extremal input action u

h

( ·).

Let the operators A and B, as well as the initial state x

0

, be inaccurately known. Namely, we have some operators A

ν

: V → V and B

ν

: U → H, and also an element x

ν0

∈ H such that

|B

ν

− B|

L(U;H)

≤ ν

B

, (21)

|x

ν0

− x

0

|

H

≤ ν

x0

. (22) The operator A

ν

generates a semigroup of linear continu- ous operators S

ν

( t), t ≥ 0, such that

sup

t∈T

|S

ν

( t) − S(t)|

L(H;H)

≤ ν

A

.

We also assume that, instead of the functional ω(t, u), we get functionals ω

ν

( t, u) which are convex with respect to u, such that the functionals

J

ν

( u(·)) =



ϑ 0

ω

ν

( t, u(t)) dt, (23)

are defined on the set U

, are lower semicontinuous and satisfy the inequalities

|J

ν

( u(·)) − J(u(·))| ≤ ν

I

, ∀u(·) ∈ U

. Here ν

A

, ν

B

, ν

x0

, and ν

I

∈ [0, 1) are given numbers.

Let the sequence {(y

i

( ·), ψ

i

( ·)}

ji=0

of elements from L

2

( T ; U) × L

2

( T ; H) be defined by the rule:

y

i+1

( ·) = y

i

( ·) + δw

i

( ·) ∈ L

2

( T ; U), y

0

( ·) = 0, (24) ψ

i+1

( ·) = ψ

i

( ·) + δζ

i

( ·) ∈ L

2

( T ; H), (25)

ψ

0

( ·) = 0, i = 0, 1, . . . , j − 1, where w

i

( ·) is a β

0

-solution to the problem



ϑ 0

2( B

ν∗

ψ

i

( t), w(t))

U

+ αω

ν

( t, w(t))

d t → inf,

w(·) ∈ U

; (26)

γ

i

( ·) ∈ C(T, H), |γ

i

( ·) − ¯γ

i

( ·)|

C(T,H)

≤ β

2

, (27) γ ¯

i

( ·) is a solution on T to the Cauchy problem

γ(t) = A ˙

ν

γ(t) + B

ν

w

i

( t), γ(0) = 0; (28)

i

( ·) − ¯ζ

i

( ·)|

C(T,H)

≤ β

1

, (29) ζ ¯

i

( ·) is a solution on T to the Cauchy problem

ζ(t) = −A ˙

ν∗

ζ(t) − G

κ

i

( t), ζ(ϑ) = 0; (30) κ

i

( t) = Gγ

i

( t) − b

ν

( t), t ∈ T. (31)

Here the symbol G

stands for the operator adjoint to G, b

ν

( t) = ξ

h

( t) − GS

ν

( t)x

ν0

.

Note that, in this case, we have ( F

ν

u(·))(η)

=



η 0

GS

ν

( η − t)B

ν

u(t) dt, η ∈ T, u(·) ∈ U

.

Let

ψ

i+1

( ·) = ψ

i

( ·) + δζ

i

( ·) ∈ L

2

( T ; H),

i = 0, 1, . . . , j − 1, (32) where ζ

i

( ·) is a solution on T of the problem

(t) = −A ˙

ν∗

(t) − G

κ

i

( t), (ϑ) = 0, (33) κ

i

( t) = G¯γ

i

( t) − b

ν

( t), t ∈ T. (34) Here ¯ γ

i

( ·) is a solution of the problem (28) on T .

Lemma 3. For any w(·) ∈ U

, the following equality



ϑ 0

2( B

ν∗

ψ

i

( t), w(t))

U

+ αω

ν

( t, w(t)) d t

= 2Ψ

i

( w(·)) + αJ

ν

( w(·)),

i = 0, . . . , j − 1, (35) holds, where

Ψ

i

( w(·)) = F

ν

y

i

( ·) − iδb

ν

, F

ν

w(·). (36) Proof. Taking into account the structure of the func- tional J

ν

( ·) (23), we conclude that (35) is equivalent to the equality



ϑ 0

( B

ν∗

ψ

i

( t), w(t))

U

d t = Ψ

i

( w(·)),

i = 0, . . . , j − 1. (37) Introduce the notation

ν

i

( η) = (F

ν

y

i

( ·))(η) − iδb

ν

( η)

=



η 0

GS

ν

( η − t)B

ν

y

i

( t) dt − iδb

ν

( η), η ∈ T.

(38) Then

Ψ

i

( w(·)) =



ϑ 0

( ν

i

( η) dη,

(7)

245



η t0

GS

ν

( η − t)B

ν

w(t) dt)

H1

d η

=



ϑ 0

( B

ν∗

χ

i

( t), w(t))

U

d t,

where the symbol ( ·, ·)

H1

stands for the scalar product in H

1

,

χ

i

( t) =



ϑ t

S

ν∗

( η − t)G

ν

i

( η) dη. (39)

To prove (35), it is sufficient to show that

ψ

i

( ·) = χ

i

( ·) (40) for i = 0, . . . , j − 1.

Let us prove (40) by induction. For i = 0, we have y

0

( ·) = 0. By virtue of (38) and (39), we obtain χ

0

( ·) = 0 = ψ

0

( ·). Assume that the equalities (40) hold for some i < j − 1. Show that the equality

ψ

i+1

( ·) = χ

i+1

( ·) (41) is also true. From (38) and (24), it follows that

ν

i+1

( η) = ν

i

( η) + δ{Gφ

i

( η) − b

ν

( η)}, (42) where

φ

i

( η) =



η 0

S

ν

( η − t)B

ν

w

i

( t) dt.

Note that φ

i

( ·) is a solution of the Cauchy prob- lem (28), i. e., φ

i

( ·) = ¯γ

i

( ·). Then (see (42) and (33))

ν

i+1

( ·) = ν

i

( ·) + δκ

i

( ·). (43) Further, from (39) and (43), it follows that

χ

i+1

( ·) = χ

i

( ·) + δρ

i

( ·). (44) where

ρ

i

( t) =



ϑ t

S

ν∗

( η − t)G

κ

i

( η) dη.

Consequently, the function ρ

i

( ·) is a solution of the Cauchy problem (33), i.e., ρ

i

( ·) = ¯ζ

i

( ·). Hence, due to

(44), (34), and (40), we get (41).



Introduce the constants

C

1

= sup {|u|

U

: u ∈ U

}, C

2

= ( |B|

L(U;H)

+ 1) C

1

ϑ

1/2

, C

3

= |G|

2L(H;H1)

ϑK

3

, K

3

= sup

t∈T

sup

ν∈(0,1]

|S

ν

( t)|

L(H;H)

.

Lemma 4. Let the elements {y

i

( ·), ψ

i

( ·)} be defined according to (24)–(31). Then {y

i

( ·)}

ji=0

= Y

jν

( δ, α, ε), where

ε = jC

2

δ(β

1

+ C

3

β

2

) + β

0

.

Proof. By definition, w

i

( ·) is a β

0

-solution of the prob- lem (26). Taking into account (35), we show that, for all β

0

, β

1

, β

2

≥ 0, w

i

( ·) is an ε-solution of the problem

i

( w(·)) + αJ

ν

( w(·)) → inf, w(·) ∈ U

. (45) It is sufficient to prove that w

i

( ·) is an ε

i

-solution of the problem (45), where ε

i

= μ

i

+ β

0

,

μ

i

= iC

2

δ(β

1

+ C

3

β

2

) (46) (clearly, ε

i

≤ ε for i ≤ j). For this purpose, it is sufficient to prove that the values of the functionals to be minimized in the problems (26) and (45) (for an arbitrary w(·) ∈ U

) differ by no more than μ

i

or (see (36) and (37)):

ε

i

( w(·)) =  



ϑ 0

2( B

ν∗

ψ

i

( t), w(t))

U

d t



ϑ 0

2( B

ν∗

ψ

i

( t), w(t))

U

d t   ≤ μ

i

. (47) Using the Cauchy-Bunyakovsky inequality, we get

ε

i

( w(·)) ≤  

ϑ

0

|B

ν

|

2L(U;H)

|w(t)|

2U

d t 

1/2

×  

ϑ

0

i

( t) − ψ

i

( t)|

2H

d t 

1/2

≤ (|B|

L(U;H)

+ ν

B

) C

1

ε

(1)i

ϑ

1/2

= C

2

ε

(1)i

, where

ε

(1)i

=

i

( ·) − ψ

i

( ·)|

C(T,H)

. Therefore, for (47) it is sufficient to prove that

ε

(1)i

≤ iδ(β

1

+ C

3

β

2

) . (48) We prove the inequalities (48) by induction. Since ψ

i

( ·) = ψ

i

( ·) = 0, the relation (48) holds for i = 0.

Assume that the relation holds for some i and prove that ε

(1)i+1

≤ (i + 1)δ(β

1

+ C

3

β

2

) . (49) Due to (31) and (34), we have

i

( t) − κ

i

( t)|

H

≤ |G|

L(H;H1)

β

2

, t ∈ T. (50) Then, by virtue of (50), the solution ¯ ζ

i

( ·) of the Cauchy problem (30) solves the Cauchy problem

ζ(t) = −A ˙

ν∗

ζ(t) − G

κ

i

( t) + λ

i

( t), ζ(ϑ) = 0,

(8)

where

λ

i

( t) = G

( κ

i

( t) − κ

i

( t)), |λ

i

( t)|

H

≤ |G|

2L(H;H1)

β

2

. Therefore, the function ζ

i

( ·) = ¯ζ

i

( ·) − ζ

i

( ·) is a solution on T of the Cauchy problem

ζ(t) = −A ˙

ν∗

ζ(t) + λ

i

( t), ζ(ϑ) = 0.

Thus,

|¯ζ

i

( ·) − ζ

i

( ·)|

C(T,H)

≤ ϑβ

2

|G|

2L(H;H1)

sup

t∈T

sup

ν∈[0,1]

|S

ν

( t)|

L(H;H)

= C

3

β

2

.

Hence, using (29), we derive

i

( ·) − ζ

i

( ·)|

C(T ;H)

≤ β

1

+ C

3

β

2

. (51) By virtue of (25) and (32), we conclude from (51) that

ε

(1)i+1

≤ ε

(1)i

+ δ|ζ

i

( ·) − ζ

i

( ·)|

C(T ;H)

≤ ε

(1)i

+ δ(β

1

+ C

3

β

2

) .

This implies (48).



Note that the inequalities

|F u − F

ν

u|

L2(T ;H1)

=

 

ϑ

0

 



η 0

G(S(η−t)B−S

ν

( η−t)B

ν

) u(t) dt  

2

H1

d η 

1/2

≤ ϑ|G|

L(H;H1)

A

|B|

L(U;H)

+ K

3

ν

B

}C

1

≤ ν

F

= C

4

( ν

A

+ ν

B

) ,

(52)

|b

ν

− b|

L2(T ;H1)

=

 

ϑ

0

 G(S

ν

( η)x

ν0

− S(η)x

0

)  

2

L(H;H1)

d η 

1/2

+

 

ϑ

0

h

( t) − z(t)|

2H1

d t 

1/2

≤ ϑ

1/2

( |G|

L(H;H1)

( K

3

ν

x0

+ |x

0

|

H

ν

A

) + h)

≤ ν

b

= C

5

( ν

x0

+ ν

A

+ h)

(53)

are fulfilled. Here

C

4

= ϑ|G|

L(H;H1)

C

1

max {K

3

, |B|

L(U;H)

}, C

5

= ϑ

1/2

( |G|

L(H;H1)

max {K

3

, |x

0

|

H

} + 1).

The next statement follows from Theorems 1 and 2 together with Lemma 4.

Theorem 4. Let ν

jA

→ 0, ν

jB

→ 0, ν

jx0

→ 0, h

j

→ +0, β

0,j

→ +0, β

1,j

→ +0, β

2,j

→ +0 and Conditions (a)–(c) of Theorem 2, where ν

jF

= C

4

( ν

jA

+ ν

jB

), ν

jb

= C

5

( ν

jx0

+ ν

jA

+ h

j

), ε

j

= jC

2

δ

j

( β

1,j

+ C

3

β

2,j

) + β

0,j

, be fulfilled. Let the sequences {y

i

( ·), ψ

i

( ·)}

ji=0

be defined according to (24)–(31), where δ = δ

j

, α = α

j

, h = h

j

, β

0

= β

0,j

, β

1

= β

1,j

, β

2

= β

2,j

, ν = ν

j

, |J

νj

( u(·)) − J(u(·))| ≤ ν

jI

≡ ν

jJ

∀u(·) ∈ U

. Then the sequence of elements {u

j

}

+∞j=1

,

u

j

= y

j

( ·)/(δ

j

j),

satisfies the conditions (9) and (10), i.e., it solves the prob- lem of approximate determination of u

0

and J

0

. In addi- tion, the inequalities (b) of Theorem 1 are valid and any weakly convergent subsequence of the sequence {u

j

}

+∞j=1

weakly converges in L

2

( T ; U) to the set U

0

( z).

Consequently from Theorem 4 and the inequalities (52), (53), the next statement follows.

Corollary 2. Let j = j(h) = [1/h], ν

jA

= k

(1)

h, ν

jB

= k

(2)

h, ν

jx0

= k

(3)

h, δ

j

= h

1−κ

, (κ = const ∈ (0 , 1)), α

j

= h

1/2−κ/2

, β

1,j

= k

(4)

h, β

2,j

= k

(5)

h, β

0,j

= k

(6)

h, ν

jI

= k

(7)

h, and h ∈ (0, 1 − ε

), ε

= const ∈ (0, 1). Then the inequalities (19) and (20), in which C and C

0

are some constants depending on ε

,

u

h

= y

j

( ·)/(h

1−κ

[1 /h]),

are fulfilled. The element y

j

( ·) is defined according to (24)–(31) for j = j(h).

4. Conclusions

In the present work, the problem of source function recon- struction was under investigation. A new algorithm for solving such a problem for an abstract differential equa- tion was suggested. This algorithm relies upon construc- tions of the theory of stable dynamical inversion based on the combination of methods of the theory of ill-posed problems and that of feedback control. The inversion the- ory exploits the idea of stabilizing appropriate functionals of the Lyapunov type by means of the extremal shift.

The work was supported by the Russian Foundation for Basic Research (project 10-01-00002), by the Ural- Siberian Project and by the program of the Presidium of the RAS Mathematical Control Theory.

References

Bensoussan, A., Prato, G.D., Delfour, M. and Mitter, S. (1992).

Representation and Control of Infinite Dimensional Sys- tems, Vol. I, Birkh¨auser, Boston, MA.

Blizorukova, M.S. and Maksimov, V. I. (1998). On the recon-

struction of an extremal input in a system with heredi-

tary, Vestnik PGTU. Matematika i Prikladnaya Matematika

(Mathematics and Applied Mathematics) 4(4): 51–61, (in

Russian).

(9)

247 Digas, B.V., Maksimov, V.I., Lander, A.V. and Bukchin, B.G.

(2003). On an algorithm for solving the inverse problem of ray seismics, in D. Chowdhury (Ed.), Computational Seis- mology and Geodynamics, American Geophysical Union, Washington, DC, pp. 84–92.

Korbicz, J. and Zgurowski, M. (1991). Estimation and Control of Stochastic Distributed-Parameter Systems, Polish Sci- entific Publishers, Warsaw, (in Polish).

Krasovskii, N. and Subbotin, A. (1988). Game-Theoretical Con- trol Problems, Springer, Berlin.

Kryazhimskii, A.V., Maksimov, V.I. and Osipov, Yu.S. (1997).

Reconstruction of extremal disturbances in parabolic equa- tions, Journal of Computational Mathematics and Mathe- matical Physics 37(3): 119–125, (in Russian).

Kryazhimskii, A.V. and Osipov, Yu.S. (1987). To a regulariza- tion of a convex extremal problem with inaccurately given constraints. An application to an optimal control problem with state constraints, in A.I. Korotkii and V.I. Maksimov (Eds.), Some Methods of Positional and Program Control, Ural Scientific Center, Sverdlovsk, pp. 34–54, (in Russian).

Omatu, S. and Seinfeld, J. (1989). Distributed Parameter Systems: Theory and Applications, Oxford Mathematical Monographs, Oxford University Press, New York, NY.

Uci´nski, D. (1999). Measurement Optimization for Parameter Estimation in Distributed Systems, Technical University Press, Zielona G´ora.

Vasiliev, F. (1981). Solution Methods to Extremal Problems, Nauka, Moscow, (in Russian).

Vyacheslav Maksimov graduated in mathemat- ics and mechanics from the Ural State Univer- sity, Ekaterinburg, Russia, in 1972. He received the Candidate and the Doctor of Physics degrees from the Institute of Mathematics and Mechan- ics, Ural Branch of the Russian Academy of Sci- ences, in 1978 and 1992, respectively. Since 1972, he has been with the Institute of Mathemat- ics and Mechanics, Ekaterinburg, Russia. Since 1994, he has been a department head at the same institute and a professor at the Chair of Controlled Systems Modeling of the Ural Federal University, Ekaterinburg, Russia. Since 2005, he has also been the head of the Chair. He is the author of more than 100 techni- cal publications, including three monographs, and his research interests are primarily focused on control theory, distributed parameter systems, mathematical modeling. Dr. Maksimov is a member of the American Mathematical Society and IFIP WG7.2. He has been on editorial boards of various journals.

Received: 14 September 2009

Revised: 19 January 2010

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We propose the Galerkin method with finite-dimensional spaces based on the Lagrangean finite element of degree k £ N (see Sec.. In the case of strong ellipticity