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This makes it possible to estimate the full loads on the spacecraft landing

gear.

Let us formulate a mathematical model of the spacecraft motion at the

last stage of landing on a small celestial body.

The main assumptions are the following ones:

a) we consider a longitudinal motion of a spacecraft with three legs;

b) aerodynamic forces are neglected;

c) gravitational acceleration is constant;

d) friction in the joints of the legs is neglected;

e) a spacecraft landing site on a celestial body is considered to be rigid.

During the development of a mathematical model of the spacecraft

motion, the following coordinate systems are used:

1) the surface coordinate system (SCS)

X, Y, Z

, associated with the

celestial body surface (

X

and

Z

axes lie in the plane of the landing surface,

X

axis lies in the plane of the first leg);

2) the spacecraft fixed coordinate system (FCS)

X

c

Y

c

Z

c

, directed along

the longitudinal axis of the spacecraft,

X

c

axis is perpendicular to

Y

c

axis

and lies in the plane

XY

of the SCS,

Z

c

completes the right hand triple of

the coordinate system;

3) the gravitational coordinate system (GCS)

X

g

Y

g

Z

g

(

Y

g

axis is

directed along the line of the gravitation force action,

X

g

axis is perpendicular

to

Y

g

axis and lies in the plane

XY

of the SCS).

Fig. 1 shows a top view of the spacecraft. Numbers

1

,

2

,

3

refer to

contact points between the legs and a celestial body; points

P

1

, P

2

, P

3

refer

to locations of the thrusters. Angles

γ

2

, γ

3

denote a rotation of the second

and third legs relative to the axis

O

c

X

c

; points

B

and

D

refer to the struts

attachment.

Fig. 1. Top view of the spacecraft with

three legs

The dimensions of all the legs

are identical. Fig. 2 shows the main

dimensions of the first leg:

l

0

(

AE

)

— is

a projection of the legs

AB

,

AD

on the

plane

X

c

Y

c

;

l

sw

(

АС

)

— is the length

of a rod with a shock absorber;

l

E

is the distance from the center of mass

(CM) of the spacecraft to the point

Е

along the

O

c

X

c

axis;

h

0

, h

1

— are the

distances from the spacecraft CM to

the attachment points of the strut and

the shock absorber, respectively;

H

are the distances from the spacecraft

center of mass to the point

А

along the

ISSN 0236-3941. HERALD of the BMSTU. Series “Mechanical Engineering”. 2014. No. 1 27