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A soil reaction on the first (second) leg along the

OY

axis is as follows:

F

N

1(2)

=

F

1(2)

cos

μ

1(2)

.

(9)

The friction force magnitude on the second leg is determined

F

T

2

=

F

2

sin

μ

2

.

For determining the friction force on the first (second) leg, we shall

calculate its velocity along the

OX

axis:

V

x

1(2)

=

V

x

+

δV

x

1(2)

,

(10)

here

V

x

— is a velocity of the spacecraft center of mass along the

OX

axis;

δV

x

1(2)

=

V

y

(

α

1(2)

ϑ

)

— is a velocity of the leg during the shock

absorber length change;

δV

x

2

=

δV

2

cos

γ

2

and

δV

z

2

=

δV

2

sin

γ

2

— is

a displacement projection and a velocity of the second leg along the axes

OX

and

OZ

.

The friction force on the first and second legs can be calculated as

follows:

F

T

1

=

F

T

1

X

=

F

1

sin(

μ

1

)

V

x

1

abs

(

V

x

1

)

.

(11)

The third leg is symmetrical relative to the second leg; therefore, during

the longitudinal motion of the spacecraft landing on the surface of a celestial

body, the soil reaction forces on the second and the third legs are identical.

F

N

2

=

F

N

3

, F

TX

2

=

F

TX

3

.

(12)

Let us consider an example of using the proposed method for calculating

the parameters of the spacecraft longitudinal motion during landing on the

surface of the Moon [9, 10].

The design parameters of the spacecraft and the legs are:

m

= 900

kg,

I

z

= 800

kg

m

2

,

h

0

= 0

.

38

m,

h

1

= 0

.

20

m,

H

= 1

.

06

m,

l

0

= 0

.

8

m,

l

E

= 1

.

0

m,

δ

0

= 0

.

001

m ,

F

0

= 3000

N.

We shall estimate the impact of different forces acting in the shock

absorbers during a vertical landing of the spacecraft under the following

conditions (

y

0

= 1

.

4

m,

V

y

0

= 0

.

1

,

V

x

0

= 0

,

μ

1

=

μ

2

= 0

.

2

,

ϑ

0

= 0

,

θ

0

= 0

). Fig. 5 shows graphs of variance of the soil normal reactions

on the legs of the spacecraft at

F

0

= 4000

N (variant 1),

F

0

= 3000

N

(variant 2),

F

0

= 2000

N (variant 3).

The graphs of variance analysis showed that in the first case, the soil

reaction force on the legs is very high and the strut inclination angle after

the spacecraft landing is rather large (

α

f

= 47

.

8

). In the third case, the

ISSN 0236-3941. HERALD of the BMSTU. Series “Mechanical Engineering”. 2014. No. 1 31