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 1146: 47

Answer

$1248 \pi$

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, $dS=n dA=\pm \dfrac{(r_u \times r_v)}{|r_u \times r_v|}|r_u \times r_v| dA=\pm (r_u \times r_v) dA$ $r_s \times r_v=\sqrt 6 (\cos u j+\sin u k)$ and $dS=\sqrt 6 ( \cos u j+\sin u k) dA$ Here, $F(x,y,z) = 26 (yj+zk)$ and $F(r(u,v))=26 \sqrt 6 (\cos u j+\sin u k)$ Rate of heat inflow through the given surface is given by: $\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] $ $=\int_{0}^4 \int_{0}^{2 \pi} 26(6) (\cos^2 u+\sin^2 u) dA$ Hence, $\iint_S F \cdot dS=(26) \cdot (6) \cdot (4) \cdot (2 \pi)=1248 \pi$
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