Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 20 - Traveling Waves - Exercises and Problems - Page 590: 79

Answer

See the detailed answer below.

Work Step by Step

a) We can find the speed by using the formula of $$v=\sqrt{\dfrac{T_s}{\mu}}$$ where $\mu=m/L$ where $m$ is the mass of the rope and $L$ is the rope's length. Thus, $$v=\sqrt{\dfrac{T_sL}{M}}\tag 1$$ Now we need to find $T_s$ which is seen in the figures below. $$\sum F_y=T_s-mg=ma_y=m(0)=0$$ $$T_s=mg$$ where $m$ is the mass of the part of the rope that is under the point. Hence, $$T_s=\dfrac{yM}{L}g$$ Plugging into (1); $$v=\sqrt{\dfrac{yg\color{red}{\bf\not} M\color{red}{\bf\not} L}{\color{red}{\bf\not} M\color{red}{\bf\not} L}}=\sqrt{yg}$$ $$\boxed{v=\sqrt{yg}}$$ --- b) From the previous result above, where $v=dy/dt$ $$\dfrac{dy}{dt}=\sqrt{yg}$$ Hence, $$dt=\dfrac{dy}{\sqrt{yg}}$$ Integrating both sides: $$\int_0^{\Delta t}dt=\int_0^L\dfrac{dy}{\sqrt{yg}}$$ $$ \Delta t =\frac{1}{\sqrt{g}}\int_0^Ly^{-\frac{1}{2}}{dy}=\frac{2}{\sqrt{g}}y^{\frac{1}{2}}\bigg|_0^L$$ $$ \Delta t =2\sqrt{L/g}$$ Thus, $$\boxed{\Delta t=2\sqrt{\dfrac{L}{g}}}$$
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.