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: 22

Answer

$\pi$

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. Here, $\iint_S F \cdot n dS=\iint_D (vi+u \sin v j+u \cos v k) \cdot (\sin v i-\cos v j+uk) dA$ $= \int_{0}^{1} \int_0^{\pi} v \sin v -u \sin v \cos v +u^2 \cos v dv du$ $= \int_{0}^{1} [(- v \cos v + \sin v) +\dfrac{u \cos 2 v}{4} +u^2 \sin v]_0^{\pi} du$ or, $= \int_{0}^{1} \pi du$ Hence, $Flux=\pi$
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