Physics: Principles with Applications (7th Edition)

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

Chapter 27 - Early Quantum Theory and Models of the Atom - General Problems - Page 801: 77

Answer

$4.0\times10^{-14}m$.

Work Step by Step

We are told to ignore the recoil of the nucleus. At the closest approach, the kinetic energy of the system is zero. The final potential energy of the two charges equals the kinetic energy of the incoming $\alpha$ particle. $$KE_{\alpha}=\frac{1}{4\pi \epsilon_o}\frac{(2e)(79e)}{r_{min}}$$ $$ r_{min}=\frac{1}{4\pi \epsilon_o}\frac{(2e)(79e)}{ KE_{\alpha}}$$ $$ =(9.00\times10^9Nm^2/C^2)\frac{(2)(79)(1.60\times10^{-19}C)^2}{(4.8MeV)(1.60\times10^{-13}J/MeV)}$$ $$=4.74\times10^{-14}m$$ The distance to the surface is this center-to-center spacing minus the radius of the gold nucleus, $4.74\times10^{-14}m-7.0\times10^{-15}m=4.0\times10^{-14}m$.
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