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 553: 52

Answer

$\omega_1=3.9778 rad/s$

Work Step by Step

The required angular velocity can be determined as follows: According to the conservation of angular momentum equation $mv_1 r_1+I\omega_1=mv_2r_2+I\omega_2$ [eq(1)] We know that $v_1=\omega_1r$ and $v_2=\omega_2 r=0.15\omega_2$ Similarly $I=mk_G^2=50(0.125)^2=0.78125Kg/m^2$ Now from eq(1), we have $50(0.15\omega_1)(0.15-0.025)+0.78125\omega_1=50(0.15\omega_2)(0.15)+0.78125\omega_2$ This simplifies to: $\omega_1=1.109\omega_2$ [eq(2)] Now, we apply the conservation of energy equaiton $T_2+V_2=T_3+V_3$ [eq(3)] As $T_2=\frac{1}{2}mv_2^2+\frac{1}{2}I\omega_2^2$ $\implies T_2=\frac{50}{2}(0.15\omega_2)^2+\frac{0.78125}{2}\omega_2^2=0.953125\omega_2^2$ Similarly $V_2=0J$ $T_3=\frac{1}{2}mv_3^2+\frac{1}{2}I\omega_3^2=\frac{50}{2(0.15\times 0)^2}+(\frac{0.78125}{2})(0)^2=0J$ and $V_3=mgh_3=50(9.81)(0.025)=12.2625J$ We plug in the known values in eq(3) to obtain: $0.953125\omega_2^2+0=0+12.2625$ This simplifies to: $\omega_2=3.5868rad/s$ Now from eq(2), we obtain: $\omega_1=1.109\times 3.5868=3.9778 rad/s$
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