Physics: Principles with Applications (7th Edition)

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

Chapter 4 - Dynamics: Newton's Laws of Motion - Problems - Page 105: 67

Answer

(a) $a = 1.55~m/s^2$ (b) $\mu_k = 0.53$

Work Step by Step

Let $a$ be the acceleration for both blocks. Let $m$ be the mass of each block. Let $F_t$ be the tension in the cord. (a) We can set up a force equation for block B. $ma = \sum F$ $ma = mg - F_t$ $F_t = mg - ma$ We can set up a force equation for block A. Note that we can use the equation for block A to replace $F_T$. $ma = \sum F$ $ma = F_t - mg~sin(\theta) - mg~cos(\theta)\cdot \mu_k$ $ma = mg - ma- mg~sin(\theta) - mg~cos(\theta)\cdot \mu_k$ $2a = g - g~sin(\theta) - g~cos(\theta)\cdot \mu_k$ $a = \frac{g - g~sin(\theta) - g~cos(\theta)\cdot \mu_k}{2}$ $a = \frac{(9.80~m/s^2) - (9.80~m/s^2)~sin(34^{\circ}) - (9.80~m/s^2)~cos(34^{\circ})\cdot (0.15)}{2}$ $a = 1.55~m/s^2$ (b) If the system is not accelerating, then the forces acting on the system in opposite directions must have the same magnitude. $mg~sin(\theta)+mg~cos(\theta)\cdot \mu_k = mg$ $cos(\theta)\cdot \mu_k = 1 - sin(\theta)$ $\mu_k = \frac{1 - sin(\theta)}{cos(\theta)} = \frac{1 - sin(34^{\circ})}{cos(34^{\circ})}$ $\mu_k = 0.53$
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