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2)

the solution

η

(

t

)

of the Cauchy problem

˙

η

=

q

(

B

1

(

t

)

, . . . , B

m

(

t

)

, η

)

, η

(0) =

η

0

(5)

is determined at all

t

[0

, t

]

and satisfies the condition

η

(

t

) =

η

.

(6)

In paper [9] it is also shown that the control

u

=

u

(

t

)

, which is the

solution to the terminal problem, is found according to the equality

u

(

t

) =

g

1

(

B

1

(

t

)

, . . . , B

m

(

t

)

, η

(

t

))

×

×

 

B

(

r

1

)

1

(

t

)

f

1

(

B

1

(

t

)

, . . . , B

m

(

t

)

, η

(

t

))

. . .

B

(

r

m

)

m

(

t

)

f

m

(

B

1

(

t

)

, . . . , B

m

(

t

)

, η

(

t

))

 

,

(7)

while the relations

z

i

=

B

i

(

t

)

,

i

= 1

, m

,

η

=

η

(

t

)

,

t

[0

, t

]

are the

parametric equations of that phase trajectory of system (2) which connects

states (3) and (4).

According to [9], we shall find functions

B

1

(

t

)

, . . . , B

m

(

t

)

from

theorem 2 in the form of

B

i

(

t

) =

b

i

(

t

) +

c

i

d

i

(

t

)

,

i

= 1

, m,

where

b

i

(

t

)

,

d

i

(

t

)

C

r

i

([0

, t

])

, the vector-functions

b

i

(

t

) =

b

i

(

t

)

, b

0

i

(

t

)

, . . . , b

(

r

i

1)

i

(

t

)

T

satisfy the conditions

b

i

(0) =

z

i

0

, b

i

(

t

) =

z

i

, i

= 1

, m,

while the vector-functions

d

i

(

t

) =

d

i

(

t

)

, d

0

i

(

t

)

, . . . , d

(

r

i

1)

i

(

t

)

T

satisfy the

conditions

d

i

(0) = 0

, d

i

(

t

) = 0

, i

= 1

, m,

(8)

It is necessary to find

c

i

R

.

It is possible, for example, to take interpolation polynomials of

2

r

i

1

degrees as functions

b

i

(

t

)

,

i

= 1

, m

, and to take any functions, for which

correlations (8) are fulfilled as functions

d

i

(

t

)

,

i

= 1

, m

. With the given

set of functions

B

i

(

t

)

, condition 1 of theorem 2 is fulfilled for any

c

i

R

.

Numbers

c

i

should be selected in such a way that condition 2 of theorem 2

was fulfilled. If there exist such numbers as

c

1

=

c

1

, . . . , c

m

=

c

m

that the

solution

η

(

t

)

of the Cauchy problem (5) satisfies the additional requirement

ISSN 1812-3368. Herald of the BMSTU. Series “Natural Sciences”. 2014. No. 5

19