Engineering Mechanics: Statics & Dynamics (14th Edition)

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

Chapter 15 - Kinetics of a Particle: Impulse and Momentum - Section 15.3 - Conservation of Linear Momentum for a System of Particles - Problems - Page 265: 55

Answer

$v_c=5.04m/s \leftarrow$

Work Step by Step

We can determine the required final velocity as follows: According to the conservation of energy $T_A+V_A=T_B+V_B$ $\implies \frac{1}{2}(m_c+m_b) v_A^2+(m_c+m_b) gh_A=\frac{1}{2}(m_c+m_b) v_B^2+(m_c+m_b) gh_A$ We plug in the known values to obtain: $\frac{1}{2}(3+0.5)(0)^2+(3+0.5)(9.81)(1.25)=\frac{1}{2}(3+0.5)v_B^2+(3+0.5)(9.81)(0)$ This simplifies to: $v_B=4.95m/s$ Now according to the conservation of linear momentum $(m_c+m_b) v_B=m_cv_c+m_bv_b$ $\implies (3+0.5)(4.95)=3v_c-0.5v_b$ $\implies v_b=6v_c-34.66$eq(1) We know that: $v_{b/c}=v_b-v_c$ $\implies -0.6=-v_b-v_c$ $\implies v_b=0.6-v_c$ From eq(1), we plug in the value of $v_b$ into the above equation to obtain: $6v_c-34.66=0.6-v_c$ This simplifies to: $v_c=5.04m/s \leftarrow$
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