Calculus: Early Transcendentals (2nd Edition)

Published by Pearson
ISBN 10: 0321947347
ISBN 13: 978-0-32194-734-5

Chapter 14 - Vector Calculus - 14.3 Conservative Vector Fields - 14.3 Exercises - Page 1085: 47

Answer

$25$

Work Step by Step

For a vector field to be Conservative, $\dfrac{\partial f_1}{\partial y}=\dfrac{\partial f_2}{\partial x}$ and $\dfrac{\partial f_2}{\partial z}=\dfrac{\partial f_3}{\partial y}$ and $\dfrac{\partial f_1}{\partial z}=\dfrac{\partial f_3}{\partial x}$ We are given that the force field as: $F(x,y, z)=(x,y,z)$ So, we can see that $\dfrac{\partial f_1}{\partial y}=0=\dfrac{\partial f_2}{\partial x}$ and $\dfrac{\partial f_2}{\partial z}=0=\dfrac{\partial f_3}{\partial y}$ and $\dfrac{\partial f_1}{\partial z}=0=\dfrac{\partial f_3}{\partial x}$ Next, we will find the potential function for the given vector field as: $\phi(x,y,z)=\dfrac{x^2+y^2+z^2}{2}$ Therefore, the integral can be expressed as: $\int_C F \ dr=\phi(2, 4, 6) -\phi(1, 2, 1) \\=\dfrac{(2)^2+(4)^2+(6)^2}{2}-[\dfrac{(1)^2+(2)^2+(1)^2}{2}]\\ =25$
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