Background Image
Previous Page  8 / 11 Next Page
Information
Show Menu
Previous Page 8 / 11 Next Page
Page Background

J

y

= 274021

;

J

z

= 238845

, and with the usage of a set of units (SI)

the initial values of SC state vector are equal

γ ω

x

ψ ω

y

T

=

= 0

,

1 0

,

005

0

,

1 0

,

002

T

;

ϑ ω

z

T

= 0

,

1 0

,

003

T

. As an

initial approximation of estimation values for the angular velocity vector

let’s choose the beginning of coordinates:

ˆ

ω

x

0

ˆ

ω

y

0

T

= ( 0

,

0 0

,

0 )

T

;

ˆ

ω

z

0

= 0

,

0

.

The simulation results are given in Figure 1, which presents the change

of non-correction components of angular velocity vector (

˜

ω

x

=

ω

x

ˆ

ω

x

,

˜

ω

y

=

ω

y

ˆ

ω

y

,

˜

ω

z

=

ω

z

ˆ

ω

z

) in accordance with the iteration index.

The range of non-connection changes (part

a

and

b

of the figure) is

quite large and correspondingly it is difficult to estimate the convergence

accuracy of SC angular rotation velocity vector using the given dependencies,

that is why starting from the fourth tact of iteration process, the simulation

results are presented in Table 1.

Table 1

Results of simulation

Non-connection component

of angular rotation velocity

vector, 1/s

Iteration index

4

5

6

7

8

9 10

ˆ

ω

x

– 0.0110 0.0343 – 0.0179 0.0089 0.0050 0.0050 0.0050

˜

ω

x

=

ω

x

ˆ

ω

x

0.0160 – 0.0293 0.0229 – 0.0039 0.0000 0.0000 0.0000

ˆ

ω

y

0.0020 0.0020 0.0020 0.0020 0.0020 0.0020 0.0020

˜

ω

y

=

ω

y

ˆ

ω

y

0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000

ˆ

ω

z

0.0030 0.0030 0.0030 0.0030 0.0030 0.0030 0.0030

˜

ω

z

=

ω

z

ˆ

ω

z

0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000

The analysis of the data presented in Figure 1 and Table 1 shows that

during eight iterations angular velocity vector agrees with the real value of

angular velocity vector of a SC.

Conclusion.

In the present article the exact pole placement method

enables the analytical solution of SC angular velocity estimation synthesis

in a mode of orbital stabilization by the results of the local vertical

sensor measurements. The results of mathematical simulation are presented,

confirming the high algorithm efficiency. In accordance with the analysis

of computational expenses of the algorithm based on the expression (16)

and the number of iterations providing the convergence of the process by

the simulation results it may be concluded that its realization is feasible in

real time.

10 ISSN 0236-3933. HERALD of the BMSTU. Series “Instrument Engineering”. 2014. No. 5