Calculus: Early Transcendentals 8th Edition

Published by Cengage Learning
ISBN 10: 1285741552
ISBN 13: 978-1-28574-155-0

Chapter 16 - Section 16.7 - Surface Integrals - 16.7 Exercise - Page 1133: 14

Answer

$\dfrac{15625\pi \sqrt 2}{6}$

Work Step by Step

Since, $\iint_S F \cdot dS=\iint_S F \cdot n dS$ where, $n$ denotes the unit vector. and $dS=n dA=\pm \dfrac{(r_u \times r_v)}{|r_u \times r_v|}|r_u \times r_v| dA=\pm (r_u \times r_v) dA$ The flux through a surface can be defined only when the surface is orientable. Since, $\iint_S y^2 z^2 dS =\iint_{D} y^2 z^2 \sqrt 2 dx dz$ $=\iint_{D}(x^2+z^2) \times z^2 dx dz$ $=(\sqrt 2) \times \int_{0}^{2 \pi} \int_0^5 (r^2) \cdot (r^{2}) \sin^2 \theta (r dr d\theta)$ $=\sqrt 2 \times \int_{0}^{2 \pi} \sin^2 \theta \times \int_0^5 r^5 dr$ $=\sqrt 2 \times \int_{0}^{2 \pi} (1/2)-\dfrac{ \cos (2 \theta) d \theta}{2} \times ( r^6/6)$ $=\dfrac{15625\pi \sqrt 2}{6}$
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