Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 8 - Rotational Motion - General Problems - Page 227: 87

Answer

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Work Step by Step

a. The kinetic energy of the system is the total kinetic energy of the two masses, because the rod is “very light”, i.e., massless. Let 1 represent the heavier mass and 2 the lighter mass. $$KE=\frac{1}{2}I_1\omega_1^2+\frac{1}{2}I_2\omega_2^2$$ $$KE=\frac{1}{2}m_1r_1^2\omega_1^2+\frac{1}{2}m_2r_2^2\omega_2^2$$ $$KE=\frac{1}{2}(m_1+m_2)r^2\omega^2=\frac{1}{2}(7.00kg)(0.210m)^2(5.60rad/s)^2=4.84J$$ b. The net force on each object is its mass multiplied by its acceleration, which is centripetal acceleration $\omega^2 r$. $$F_{net,1}=m_1\omega_1^2r_1=(4.00kg)(5.60rad/s)^2(0.210m)=26.3N$$ $$F_{net,2}=m_2\omega_2^2r_2=(3.00kg)(5.60rad/s)^2(0.210m)=19.8N$$
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