University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 13 - Gravitation - Problems - Exercises - Page 431: 13.81

Answer

$\frac{2GMm}{a^{2}}[1-\frac{x}{\sqrt {x^{2}+a^{2}}}]$

Work Step by Step

We can view the disk as being made up of smaller concentric disks of radius $r$ and thickness $dr.$ The area of each ring is $dA = 2πrdr$ and the mass is $dM = \frac{M}{πa^{2}}dA = \frac{2Mr}{a^{2}}dr$. Then the force exerted by this ring on the mass $m$ is . . . $dF = \frac{(GmdM)x}{(r^{2}+x^{2})^{3/2}} = \frac{2GmMx}{a^{2}}\frac{rdr}{(r^{2}+x^{2})^{3/2}} $ The total force is the contribution of all the forces from all the disks. So we integrate from 0 to a: $F = \int dF =\int_{0}^{a} \frac{2GmMx}{a^{2}}\frac{rdr}{(r^{2}+x^{2})^{3/2}} $ Clearly, $\frac{2GmMx}{a^{2}}$ is a constant quantity, so we bring it outside the integral. $F = \frac{2GmMx}{a^{2}}\int_{0}^{a} \frac{rdr}{(r^{2}+x^{2})^{3/2}} $ Then we evaluate the integral (using the substitution $u^{2} = r^{2} + x^{2}$). This yields . . . $F = \frac{2GmMx}{a^{2}}[\frac{1}{x}-\frac{1}{\sqrt {a^{2}+x^{2}}}] = \frac{2GMm}{a^{2}}[1-\frac{x}{\sqrt {x^{2}+a^{2}}}] $ To verify this result and to check if it gives us the correct result as x grows very large, we can rewrite the term within brackets as . . . $\frac{x}{\sqrt {x^{2} + a^{2}}} = \frac{1}{\sqrt {1 + (a/x)^{2}}} = (1+(a/x)^2)^{-1/2}$ Using the binomial expansion, if $x>>a$, this expression simplifies to $F=\frac{GMm}{x^{2}}$—as we should expect! So the result is correct.
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