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 28 - The Electric Potential - Exercises and Problems - Page 835: 46

Answer

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Work Step by Step

We know that during the acceleration of the protons, they must be gaining kinetic energy while losing potential energy until they leave the electric field area that pushes them to accelerate, and then the beam will move at a constant speed. In other words, since the protons are accelerating, they must be traveling through a decreasing potential. Hence, $$\Delta K=-\Delta U_e$$ $$ K_f-K_i=-\Delta U_e$$ where $K_i=0$, and $U_{ef}=0$ $$ K_f-0=-\Delta U_e$$ $$ K_f = -q\Delta V$$ Hence, $$q=\dfrac{K_f}{|-\Delta V|}$$ For one patient, it is desired to deposit 0.10 J of proton energy. $$q=\dfrac{0.10}{|-1\times 10^7|}=\color{red}{\bf 10}\;\rm nC$$ where $q=Ne$ whereas $e$ is the charge of one proton and $N$ is the number of them. Hence, $$N=\dfrac{q}{e}=\dfrac{10\times 10^{-9}}{1.6\times 10^{-19}}$$ $$N=\bf 6.25\times 10^{10}\;\rm e^-$$
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