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we get the lift as L, = 0 + /2 + /3 + /4 =2 Vv0pn{J0((o) sin vt -J,(<o) cos vt} + pVv0nco{y0((o)+/2(w)} COSVr -2Vv0p7it{ay0((o) + i>V,(co)} sinvr + {6 70(co) -a/,( co)} |R sin BB sin VR ||YR + sín Z sin 9 sin cos 35 cos WR - sin à sin 9 sin sin ŽR cos WR + cos ? cos sin ŽR sin 9F sin VR + cos Á cos y cos of sin 9R sin VR + cos 3 !Triangle to determine cos VR and sin WR ^ - - -: - 2 A • A n = sin VR sin 6°n, + sin VR cos 6 ny * cos VR n2 (13 50) We now differentiate n: to obtain a vector in , _. As far as we deal with the steady state of the oscillation, the periodic solution of the form v0 = 2 + æ sin t + y cos t + w cos vr (7 : 4) in which the constant term 2, the terms containing sin T and cost separately to zero, we obtain the following &Take this deal for 51% off with our SinVR discount for $10 00 in savings JOIN HERE Get your membership through Sin VR discount for a special price on your .
 
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