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 19.4 - Eccentric Impact - Problems - Page 551: 45

Answer

$v=5.96~ ft/s$

Work Step by Step

We can determine the required velocity as follows: We know that the angular momentum is conserved about D: $H_{D_1}=H_{D_2}$ $\implies mv_1r_1=I_D\omega_2$ [eq(1)] As $I_D=\frac{m(I^2+\omega^2)}{12}+mr_{D/G}^2$ $\implies I_D=\frac{10}{32.2}(\frac{(1)^2+(1)^2}{12})+\frac{10}{32.2}(\sqrt{(0.5)^2+(0.5)^2})^2=0.207 slug/ft^2$ We plug in the known values in eq(1) to obtain: $\frac{10}{32.2}v(0.5)=0.207\omega_2$ $\implies 0.155279v=0.207\omega_2$ [eq(2)] According to the conservation of energy $T_2+V_2=T_3+V_3$ [eq (3)] We know that $T_2=\frac{1}{2}I_D\omega_2^2=(0.1035)\omega_2$ $V_2=mgh_2=10(0.5)=5lb\cdot ft$ Similarly $V_2=mgh_2=(10)(0.5)=5lb\cdot ft$ $T_3=\frac{1}{2}I_D\omega_3^2=\frac{1}{2}(0.207)(0)^2=0lb\cdot ft$ $V_3=mgh_3$ $h_3=\sqrt{(0.5)^2+(0.5)^2}=0.707ft$ $\implies V_3=10(0.707)=7.07\space lb\cdot ft$ We plug in theses values in eq(3) to obtain: $0.1035\omega_2^2+5=0+7.07$ This simplifies to: $\omega_2=4.4721 rad/s$ Now, we plug in the known values in eq(2) to obtain: $0.155279v=0.207(4.4721)$ This simplifies to: $v=5.96~ ft/s$
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