Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 4 - Forces and Newton's Laws of Motion - Problems - Page 119: 116

Answer

(a) $a=3.68m/s^2$ (b) $a=11.8m/s^2$ (c) The difference in the results comes from the difference in mass in 2 cases.

Work Step by Step

(a) The heavier block will fall down while the lighter block will be pulled up. As these blocks act as a system, their movement has similar acceleration $a$. The weight of the heavier block pulls it downward, while the tension $T$ in the rope holds it upward. According to Newton's 2nd Law, as the block falls with acceleration $a$, $$W-T=Ma$$ $$908-T=\frac{908}{9.8}a=92.65a (1)$$ Similarly, the weight of the lighter block pulls it downward, while the tension $T$ in the rope holds it upward. According to Newton's 2nd Law, as the block is pulled up with acceleration $a$, $$T-W=ma$$ $$T-412=\frac{412}{9.8}a=42.04a(2)$$ We solve equations (1) and (2) and get $a=3.68m/s^2$ (b) The removal of the heavier block means we have to revisit equation (1) $W-T=Ma$ We assume the pulling hand has zero mass, which means $M=0$ and $W=0$. If we call the pulling force $P$, we get, as a result $$P-T=0$$ $$P=T=908N$$ The tension in the rope is $908N$. Apply this back to equation $T$: $$42.04a=908-412=496N$$ $$a=11.8m/s^2$$ (c) The difference in the results comes from the difference in mass in 2 cases as we have seen. This leads to different tension values in the rope, which lead to different acceleration in the end.
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.