Physics: Principles with Applications (7th Edition)

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

Chapter 18 - Electric Currents - General Problems - Page 525: 91

Answer

$f=1-\frac{V}{V_0}$.

Work Step by Step

Assume the tank is empty. The entire wire of length $\ell$ is non-superconducting. Suppose its resistivity is $\rho$. The resistance of the wire, with an empty tank, is $R_0=\rho\frac{\ell}{A}=\frac{V_0}{I}$. Now, let a length x of the wire become superconducting. That part of the wire has zero resistance. Only the length $\ell-x$ has resistance. The wire’s overall resistance is $R=\rho\frac{\ell-x}{A}=\rho\frac{\ell}{A}\frac{\ell-x}{\ell}=R_0\frac{\ell-x}{\ell}$. The current is held steady, so we calculate the voltage using Ohm’s Law. $$V=IR=\frac{V_0}{R_0}R_0\frac{\ell-x}{\ell}=V_0(1-\frac{x}{\ell})=V_0(1-f)$$ We solve for the relationship between f and V. $$f=1-\frac{V}{V_0}$$ We see that measuring the voltage V reveals the fraction of the tank that is filled with liquid helium.
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