Engineering Mechanics: Statics & Dynamics (14th Edition)

Published by Pearson
ISBN 10: 0133915425
ISBN 13: 978-0-13391-542-6

Chapter 19 - Planar Kinetics of a Rigid Body: Impulse and Momentum - Section 19.2 - Principle of Impulse and Momentum - Problems - Page 536: 16

Answer

$v=7.09ft/s$

Work Step by Step

We can determine the required speed as follows: First, we apply the principle of impulse and momentum to figure (1) $mv_1+\Sigma \int_{0}^{10} F_x dt=mv_2$ $\implies mv_1+A_xt-B_xt=mv_2$ $\implies 0+10A_x-10B_x=\frac{4000}{32.2}v$ $\implies A_x-B_x=12.4224v~~~$[eq(1)] Now, we apply the principle of impulse and momentum to figure (2) $I_A\omega_1+\Sigma\int_{0}^{10}M_A dt=mv_2 r+I_A\omega_2~~~$[eq(2)] We know that $I_A=I_B=mk^2=(\frac{1500}{32.2})(1.25)^2=72.7873slug\cdot ft$ and $\omega_1=0$ Similarly $\int_{0}^{10} M_Adt=Mt-A_x tr=300(10)-A_x(10)(1.5)=3000-15A_x$ From eq(2) $0+3000-1.5A_x=(\frac{1500}{32.2})(1.5v)+72.7873(0.6667v)$ This simplifies to: $A_x=200-7.8935v~~~$[eq(3)] The principle of impulse and momentum for figure (3) is given as $I_B\omega_1+\Sigma\int_{0}^{10} M_B dt=mv_2 r+I_B\omega_2$ As $\omega_1=0$ and $\Sigma\int_{0}^{10} M_B dt=B_x tr=B_x(10)(1.5)=15B_x$ $\implies 0+15B_x=(\frac{1500}{32.2})(1.5)+72.7873(0.6667v)$ This simplifies to: $B_x=7.8935v~~~$[eq(4)] We plug in the known values from eq(3) and eq(4) into eq(1) to obtain: $200-7.8935v-7.8935v=12.4224v$ This simplifies to: $v=7.09ft/s$
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