Introduction to Electrodynamics 4e

Published by Pearson Education
ISBN 10: 9332550441
ISBN 13: 978-9-33255-044-5

Chapter 9 - Section 1.1 - Waves in One Dimension - Problem - Page 390: 2

Answer

$f$ satisfies the wave equation and $f$ can be represented as the sum of a wave traveling to the left and a wave traveling to the right as $$f(z, t) = \frac{A}{2} [\sin(kz+kvt)+\sin(kz-kvt)] $$

Work Step by Step

Wave equation is given by: $$ \frac{\partial^2 f}{\partial z^2} = \frac{1}{v^2}\frac{\partial^2 f}{\partial t^2} $$ For $f(z, t) = A \sin(kz)\cos(kvt) $ $$ \frac{\partial f}{\partial z} = Ak\cos(kz)cos(kvt) $$ $$ \frac{\partial^2 f}{\partial z^2} = -Ak^2\sin(kz)\cos(kvt)\qquad ...(1)$$ $$ \frac{\partial f}{\partial t} = -Akv\sin(kz)\sin(kvt) $$ $$ \frac{\partial^2 f}{\partial t^2} = -Ak^2v^2\sin(kz)\cos(kvt)\qquad ...(2)$$ From equation $(1) \text{ and } (2)$, $$ \frac{\partial^2 f_1}{\partial z^2} = \frac{1}{v^2}\frac{\partial^2 f_1}{\partial t^2} $$ Hence $f$ satisfies the wave equation. Using the Trigonometry Identity, $$\sin(A)\cos(B) = \frac{1}{2}[\sin(A+B)+\sin(A-b)]$$ we get, $$f(z, t) = A \sin(kz)\cos(kvt) $$ $$f(z, t) = \frac{A}{2} [\sin(kz+kvt)+\sin(kz-kvt)] $$ Hence, $f$ can be represented as the sum of a wave traveling to the left and a wave traveling to the right.
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