Page 422 - Advanced engineering mathematics
P. 422
402 CHAPTER 12 Vector Integral Calculus
F · Tds = (∇× F) · ndσ.
C
We will see this in Section 12.9 as Stokes’s theorem.
SECTION 12.7 PROBLEMS
1. Let C beasimpleclosedpathinthe x, y-plane with 2. Under the conditions of Problem 1, show that
interior D.Let ϕ(x, y) and ψ(x, y) be continuous with
2
2
continuous first and second partial derivatives on C and (ϕ∇ ψ − ψ∇ ϕ)dA
throughout D.Let D
∂ϕ ∂ψ ∂ψ ∂ϕ
= ψ − ϕ dx + ϕ − ψ dy.
2
2
∂ ψ ∂ ψ C ∂y ∂y ∂x ∂x
2
∇ ψ = + .
∂x 2 ∂y 2 3. Let C be a simple closed path in the x, y-plane, with
interior D.Let ϕ be continuous with continuous first
Prove that
and second partial derivatives on C and throughout D.
Let N(x, y) be the unit outer normal to C (outer mean-
2
ϕ∇ ψ dA ing pointing away from D from points on C). Prove that
D
2
∂ψ ∂ψ ϕ N (x, y)ds = ∇ ϕ(x, y)dA.
= −ϕ dx + ϕ dy − ∇ϕ ·∇ψ dA. C D
C ∂y ∂x D
(Recall that ϕ N is the directional derivative of ϕ in the
direction of N.)
12.8 The Divergence Theorem of Gauss
The discussion of the preceding section suggested a possible extension of Green’s theorem to
three dimensions, yielding what is known as the divergence theorem.
THEOREM 12.8 The Divergence Theorem of Gauss
Let be a piecewise smooth closed surface bounding a region M of 3-space. Let have unit
outer normal n.Let F be a vector field with continuous first and second partial derivatives on
and throughout M. Then
F · ndσ = ∇· FdV. (12.10)
M
The theorem is named for the great nineteenth-century German mathematician and scientist
Carl Friedrich Gauss, and is actually a conservation of mass equation. Recall that the diver-
gence of a vector field at a point is a measure of the flow of the field away from that point.
Equation (12.10) states that the flux of the vector field outward from M across exactly bal-
ances the flow of the field from each point in M. Whatever crosses the surface and leaves M must
be accounted for by flow out of M (in the absence of sources or sinks in M).
We will look at two computational examples to get some feeling for equation (12.10), and
then consider applications.
Copyright 2010 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).
Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.
October 14, 2010 14:53 THM/NEIL Page-402 27410_12_ch12_p367-424