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EXAMPLE 3-7<br />
Obtain the transfer functions X(s)/U(s) and X2$)/U(s) <strong>of</strong> the mechanical system shown in<br />
unT;"1lnr"tions<br />
<strong>of</strong> motion for the system shown in Figure 3-19 are<br />
mrir: -ktxr - krl*, * x2) - b\*y - i2) + u<br />
mzlz: -k*z - kr(*, - xt) - U(*, - *t)<br />
Simplifying, we obtain<br />
mri, + bit + (kt * k)x1 : b*z * k2x2 I u<br />
m2i2 * b*2 + (k2 * k1)x2 = bit + k2xy<br />
Taking the Laplace transforms <strong>of</strong> these two equations, assuming zero initial conditions, we obtain<br />
lmrs2 + bs + (k, + kr)]xl(s) : (rs + 6)xr1s1+ u(s)<br />
fm2s2 + bs + (k, + h))x21): (rs + k2)xr1)<br />
Solving Equation (3-45) for X2(s) and substituting<br />
into Equation Qa$ and simplifying, we get<br />
from which we obtain<br />
l(mrsz + bs * k,+ k2)(m2s2 .r bs * kz+ h) - (rs + 4)'?)x,1s1<br />
: (m2s2* bs * k2 + h)U (s)<br />
(344)<br />
(3-45)<br />
xr(s) mrsz + bs + kr+ k,<br />
u(s)<br />
(mrs2 + bs + kr+ k2)(m2s2 * bs * k2+ h)-(us + *r)2<br />
(346)<br />
From Equations (3-45) and (3-46) we have<br />
XzG)<br />
u(s)<br />
bs+k2<br />
(m,sz + bs * k1 + kr)(m2s2 + bs + k2 +<br />
t