Fundamentals of Physics Extended (10th Edition)

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

Chapter 16 - Waves-I - Problems - Page 477: 75b

Answer

The answer does not depend on the diameter of the wire.

Work Step by Step

Let $A$ be the cross-sectional area of the wire. We can find an expression for the maximum tension: $\tau = (7.00\times 10^8~N/m^2)(A) = (7.00\times 10^8~N/m^2)(\pi~r^2) = (7.00\times 10^8~N/m^2)(\pi)~(\frac{d}{2})^2$ We can find an expression for the linear density: $\mu = \frac{m}{L} = \frac{V~\rho}{L} = \frac{A~L~\rho}{L} = A~\rho = \pi~r^2~\rho = \pi~(\frac{d}{2})^2~\rho$ We can see that $\tau \propto d^2$ and $\mu \propto d^2$ We can write an expression for the maximum wave speed: $v = \sqrt{\frac{\tau}{\mu}}$ $v = \sqrt{\frac{(7.00\times 10^8~N/m^2)(\pi)~(\frac{d}{2})^2}{\pi~(\frac{d}{2})^2~\rho}}$ $v = \sqrt{\frac{(7.00\times 10^8~N/m^2)}{\rho}}$ In this expression, the $d^2$ cancels out of the numerator and the denominator. Therefore, the answer does not depend on the diameter of the wire.
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