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 1134: 47

Answer

$1248 \pi$

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. $r_s \times r_v=\sqrt 6 (\cos u j+\sin u k)$ and $dS=\sqrt 6 ( \cos u j+\sin u k) dA$ Here, $F(r(u,v))=26 \sqrt 6 (\cos u j+\sin u k)$ $\iint_S F \cdot dS= \int_{0}^4 \int_{0}^{2 \pi} 26 \sqrt 6 (\cos u j+\sin u k) [\sqrt 6 ( \cos u j+\sin u k) dA] $ $=\int_{0}^4 \int_{0}^{2 \pi} 26(6) (\cos^2 u+\sin^2 u) dA$ $=(26) \cdot (6) \cdot (4) \cdot (2 \pi)$ Hence, the rate of heat inflow is $1248 \pi$
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