Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 7 - Kinetic Energy and Work - Problems - Page 172: 21a

Answer

Let T as the cord's force. Applying Newton's Second Law, we have: Net force = $T-mg=ma$. Then $$T=m(a+g)$$ Because of $a=-\frac{g}{4}$ $$T=m(a+g)=m(-\frac{g}{4}+g)=m\frac{3g}{4}$$ By definition, $W=Fdcos\theta$. The angle between $T$ and displacement $d$ is $180^{\circ}$, thus $$W_{T}=Tdcos\theta=-m\frac{3g}{4}d$$ is the work done on the block by the cord.

Work Step by Step

Let the cord's force be F. Block's acceleration $=\frac{g}{4}$ Net force = $Ma=M\frac{g}{4}$ Block is going down so, weight($Mg$) is greater. Therefore; $Mg-F = M\frac{g}{4}$ $F = \frac{-3Mg}{4}$ Substituting the formula of $F$ above in $W=Fd$ and simplifying: $W=Fd=\frac{-3Mg}{4}\times d =\frac{-3Mgd}{4}$
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