7696081262
Z. KORUBA ET AL.
Ivz — (A< T IprĘpv cos 'dpy T IprripV sin dpv) sin lfipv +
“I- (+ ^prQpv ) COS Ippy
Ivxz — (At>£' T Ipr£pv
• cos if)pV sin ippv |
COS 0pv 1 prrjp , sin “9pv |
mw = 50 kg |
Iw^ = lOkgm2 |
Iwt]'v — 7 kgm |
Iw{' = 12 kgm2 |
mpr = 30 kg |
Iprtw = 0.6 kgm2 |
Iprr)pv = 4kgm |
= 3.5 kgm2 |
Launcher suspension parameters
kv ii = 30000 N/m |
cv u = 150Ns/m |
kv\2 = 30000 N/m |
cwi 2 = 150Ns/m |
kv 13 = 30000 N/m |
Cui3 = 150Ns/m |
kv i4 = 30000 N/m |
Cyi4 = 150Ns/m |
Missile parameters |
mp = 12 kg |
Ipxp = 0.01 kgm2 |
Ipyp = 2 kgm2 |
IPzr = 2 kgm2 |
Geometrie characteristics |
l\ = 0.3 m |
I2 = 0.3 m |
d\ = 0.2 m |
d2 = 0.2 m |
lp = 1.6 m |
s
00
0
II
n. |
Thrust and operation time of the missile starter motor Pss = 4000 N tss = 0.07 s
4.2. Kinematic excitations
The terrain unevenness, i.e. a bump, was assumed to be a kinematic exci-tation. The basie motion of the vehicle carrying the launcher was defined as
Sn = tgb)
where
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