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 833: 14

Answer

a) $\text{Into a region of higher potential.}$ b) $3340\;\rm V$

Work Step by Step

$$\color{blue}{\bf [a]}$$ We know that the proton slows down as it travels and we know that the proton is a positively charged particle. This means that the electron is moving toward a higher potential region. $$\color{blue}{\bf [b]}$$ We know that the potential difference is given by $$\Delta V=\dfrac{\Delta U}{q_p}\tag 1$$ And since the energy is conserved, $$E_i=E_f$$ $$K_i+U_i=K_f+U_f$$ The final speed of the electron is zero, so $K_f=0$ $$K_i+U_i=0+U_f$$ Hence, $$\Delta U=K_i=\frac{1}{2}m_pv_p^2$$ Plug into (1), $$\Delta V=\dfrac{\frac{1}{2}m_pv_p^2}{q_p} $$ Plug the known; $$\Delta V=\dfrac{\frac{1}{2}(1.67\times 10^{-27})(800,000)^2}{(1.6\times 10^{-19})} $$ $$\Delta V=\color{red}{\bf 3340}\;\rm V$$
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