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caculus 13.9

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13.5 Curl and Divergence
Copyright © Cengage Learning. All rights reserved.
: closed surface
13.5 Curl and Divergence
Copyright © Cengage Learning. All rights reserved.
Vector Forms of Green’s Theorem
Its line integral is
and, regarding F as a vector field on ¡ 3 with third component 0, we have
F = P i + Q j + 0 k.
3
Vector Forms of Green’s Theorem
Then, from equation 16.3 (3)
we have
F = P i + Q j + 0 k.
N
M
4
The Divergence Theorem
We write Green’s Theorem in a vector version as
where C is the positively oriented boundary curve of the plane region D.
If we were seeking to extend this theorem to vector fields on
we might
make the guess that
where S is the boundary surface of the solid region E.
It turns out that Equation 1 is true, under appropriate hypotheses, and is
called the Divergence Theorem.
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13.9 The Divergence Theorem
Copyright © Cengage Learning. All rights reserved.
The Divergence Theorem
The boundary of E is a closed surface, and we use the convention(?), that the
positive orientation is outward; that is, the unit normal vector n is directed
outward from E.
Thus the Divergence Theorem states that, under the given conditions, the flux
of F across the boundary surface of E is equal to the triple integral of the
divergence of F over E.
8
Example 4 (in 13.7)
Find the flux of the vector field F(x, y, z) = z i + y j + x k over the unit sphere x 2 +
y 2 + z 2 =1.
Solution:
We use the parametric representation
9
Example 1(We use the Divergence Theorem)
Find the flux of the vector field F(x, y, z) = z i + y j + x k over the unit sphere x 2 +
y 2 + z 2 =1.
Solution:
First we compute the divergence of F:
The unit sphere S is the boundary of the unit ball B given by
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Example 2
Solution:
11
Example 2
Solution:
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The Divergence Theorem
Let’s consider the region E that lies between the closed surfaces S1 and S2, where
S1 lies inside S2.
Let n1 and n2 be outward normals of S1 and S2.
Then the boundary surface of E is S = S1 ∪ S2 and its normal n is given by n = −n1
on S1 and n = n2 on S2. (See Figure 3.)
Applying the Divergence Theorem to S, we get
Figure 3
13
#2
with upward orientation.
Solution:
( )
(-)
with downward orientation.
D
14
# 37
Solution:
?
= 20
15
Final exam
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Type I
=y
=y
Solution:
Type II
Solution: The region R can be described as
R = {(x, y) | x, y  0, 1  x 2 + y 2  4}
It is the half-ring shown in Fig.,
and in polar coordinates it is given
by 1  r  2, 0     /4.
Type_1
위
아래
Figure 9
Type 1; 위/아래
#. Evaluate the integral by changing to spherical coordinates.
#.
25.
Solution:
R
#.
Solution:
Example 3
Solution:
Using Equation 2, we have
f (1,1,2) - f (0,0,0) = 8
36
Recall (Green’s Theorem)
C:+
37
Example 1
Solution:
n = <0, 1, 1> / 2
curl F ≠ 0
:+
choice!
r (x, y) = < x, y, g(x, y) > = < x, y, 2 - y >
Figure 3
rx × ry =
= < 0, 1, 1 >
38
Example 1
Solution:
curl F ≠ 0
:+
choice!
Figure 3
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①
Example 2 (의도/의미?)
Solution:
뿔룩한 곡면
: + : counterclockwise
(+ orientation)
②
Note that in Example 2 we computed a surface integral simply by knowing the values of F on the
boundary curve C. This means that if we have another oriented surface with the same boundary
40
curve C, then we get exactly the same value for the surface integral!
②
Example 2 (의도/의미?)
Solution:
: + : counterclockwise
(+ orientation)
n = < 0, 0, 1>
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Example 3
: counterclockwise
(+ orientation)
Solution:
n(=k)= < 0, 0, 1>
-n
:+
< 0, 0, -1>
(-1)
42
Recall (Surface Integrals, Flux)
③
+
43
13.7. #31
44
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