Multivariable Calculus, 7th Edition

Published by Brooks Cole
ISBN 10: 0-53849-787-4
ISBN 13: 978-0-53849-787-9

Chapter 16 - Vector Calculus - 16.7 Exercises - Page 1145: 13

Answer

$\dfrac{364 \pi \sqrt 2}{3}$

Work Step by Step

The flux through a surface can be defined only when the surface is orientable. We know that $\iint_S F \cdot dS=\iint_S F \cdot n dS$ Here, $n$ denotes the unit vector. Since, $\iint_S x^2z^2 dS =\iiint_{D} (v \sin u)^2 v^2 v\sqrt 2 dA$ $=\int_{1}^{3} \int_{0}^{2 \pi} (\sin^2 u) v^5 \sqrt 2 du dv$ $=( \int_{0}^{2 \pi} \sin^2 u du) \times (\int_{1}^{3} v^5 \sqrt 2 dv)$ $=[(1/2) \int_{0}^{2 \pi} \sin^2 u du] \times (\int_1^3 v^5 \sqrt 2 dv)$ $=(1/2) [u-\dfrac{\sin 2u}{2}]_0^{2 \pi} \times (\dfrac{729\sqrt 2}{6}-\dfrac{\sqrt 2}{6})$ $=\dfrac{364 \pi \sqrt 2}{3}$
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