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 834: 20

Answer

a) $1000\;\rm V$ b) $7\;\rm Mm/s$

Work Step by Step

$$\color{blue}{\bf [a]}$$ We know that $$ \Delta V_C=Ed$$ Plug the known; $$ \Delta V_C = (5\times 10^5)(2\times 10^{-3})$$ $$\Delta V_C=\color{red}{\bf 1000}\;\rm V$$ $$\color{blue}{\bf [b]}$$ since the energy is conserved, $$E_i=E_f$$ $$K_i+U_i=K_f+U_f$$ Assuming the initial potential energy of the electron is zero since it is released from the negative plate $$K_i+0=K_f+U_f$$ where $U_f=q_eV_C$ Hence, $$K_i =K_f+qV_C$$ Recalling that $K=\frac{1}{2}mv^2$ $$\frac{1}{2}m_ev_i^2=\frac{1}{2}m_ev_f^2+qV_C$$ $$ v_i^2= v_f^2+\dfrac{2q_eV_C}{m_e}$$ $$ v_i =\sqrt{ v_f^2+\dfrac{2q_eV_C}{m_e}}$$ Plug the known; $$ v_i =\sqrt{ ( 2.0 \times 10^7 )^2+\dfrac{2 ( 1.6\times10^{-19})(1000)}{(9.11\times10^{-31})}}$$ $$v_i=\color{red}{\bf 7\times 10^6}\;\rm m/s$$
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