Exercises:
For each vector field F,
find the flux of curl( F) through the paraboloid
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r( u,v) =
á vcos( u) ,vsin( u) ,1-v2
ñ , u in [ 0,2p], v in [ 0,1] |
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first by direct evaluation and then by Stoke's theorem using the
boundary curve T of the surface.
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F( x,y,z) =
á x+y,x-y,z
ñ |
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For each vector field F, find the flux of curl( F) through the upper unit hemisphere first by direct evaluation and
then by Stoke's theorem using the boundary curve T of the
surface.
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F( x,y,z) =
á x+y,x-y,z
ñ |
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F( x,y,z) = |
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x
(x2+y2+z2) 3/2
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y
( x2+y2+z2)3/2
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z
( x2+y2+z2) 3/2
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Use Green's theorem to find the flux of F through the given region in the
xy-plane.
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Region: on and in unit circle |
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Region: on and in unit circle |
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Use Stoke's theorem to evaluate the following line integrals
using either the paraboloid in example 1 or the unit upper hemisphere in
example 4.
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T
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ydx - xdy |
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T
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y2dx - x2dy |
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T
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xydx + xdy |
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C
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ydx + xdy |
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Show that each of the following curves is contained in a
plane by showing that r×v has constant direction.
Then use (1) to find the area enclosed by the curve.
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r( t) =
á 2sin( t), 0, 2cos( t)
ñ , t in [ 0,2p] |
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r( t) =
á 0, 3sin( t), 2cos( t)
ñ , t in [ 0,2p] |
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r( t) =
á 6sin( t), 8sin( t), 10cos( t)
ñ , t in [0,2p] |
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r( t) =
á sin( t), sin( t), cos( t)
ñ, t in [ 0,2p] |
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r( t) =
á cos( t), sin( t), sin( t)
ñ , t in [ 0,2p] |
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r( t) =
á cos(t), sin( t), cos( t)
ñ, t in [ 0,2p] |
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25. Use Stoke's theorem and an appropriate surface to evaluate òC ydx+xdz, where C is the curve parameterized by
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r( t) =
á cos( t) ,1,sin(t)
ñ , t in [ 0,2p] |
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26. Use Stoke's theorem and an appropriate surface to evaluate òC xdx-zdy, where C is the curve parameterized by
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r( t) =
á cos( t) ,1,sin(t)
ñ , t in [ 0,2p] |
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27. Use Stoke's theorem and an appropriate surface to evaluate òC ydx-zdy+xdz, where C is the curve parameterized by
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r( t) =
á cos( t) ,sin(t) ,1+sin( t)
ñ , t in [ 0,2p] |
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28. Use Stoke's theorem and an appropriate surface to evaluate òC xyz dx, where C is the curve parameterized by
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r( t) =
á cos( t) ,sin(t) ,1+sin( t)
ñ , t in [ 0,2p] |
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29. Show that if F is sufficiently smooth on and inside
a sphere centered at the origin, then
ó õ
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ó õ
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Sphere |
curl( F) ·dS = 0 |
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30. Show that the curl of
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F( x,y,z) = |
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-y
x2+y2
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x
x2+y2
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, z |  |
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is zero if ( x,y) ¹ ( 0,0) . Then show that
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T
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F ·dr |
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is not zero. Why does this not violate Stoke's theorem?
31. Apply Stoke's theorem to F( x,y,z) =
á bz-cy,cx-az,ay-bx
ñ to show that if S is a
region in a plane with normal N =
á a,b,c
ñ ,
then
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Area of S = |
±1
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¶S
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( bz-cy) dx+( cx-az) dy+( ay-bx) dz |
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32. Show that Green's theorem can also be written in the form
ó õ
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ó õ
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S |
( Mx+Ny) dA = |  |
¶S
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Mdy - Ndx |
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Then explain why if F( x,y) =
á M(x,y) ,N( x,y)
ñ , then
ó õ
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ó õ
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S |
div( F) dA = |  |
¶S
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F · N ds |
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where N is the unit normal vector to the curve ¶S.
Suppose that r( x,y,z) is the
charge density of an electron cloud and that j( x,y,z) is the current density of the cloud (i.e., the number of ''moving
charges'' per unit volume). Then the resulting Electric Field E( x,y,z,t) and the Magnetic Field H( x,y,z,t) are related to these densities (and each
other) by Maxwell's equations, which in empty space are
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curl( H) = |
4p
c
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j- |
1
c
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¶E
¶t
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where c is the speed of light in a vacuum. Maxwell's
equations are at the heart of the study of electricity and magnetism, and
Stoke's theorem is often used to study Maxwell's equations.
33. Use Stoke's theorem to show that if S is a surface,
then
ó õ
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ó õ
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S |
-1
c
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¶H
¶t
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· dS = | ó (ç) õ
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¶S
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E·dr |
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(Note: This yields the important idea that
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-1
c
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¶
¶t
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( Flux of H through S) = Circulation of E around ¶S |
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34. What type of result can be obtained by applying Stoke's theorem
to Maxwell's equation (4)?
35. It can be shown that div( H) = 0 implies
that there exists a vector field A such that
Use Stoke's theorem to show that
ó õ
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ó õ
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S |
H·dS = |  |
¶S
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A · dr |
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36. Show that if r( x,y) is the charge density of
a 2-dimensional electric field E, then
ó õ
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ó õ
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S |
r( x,y) dA = |
1
4p
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¶S
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E·N ds |
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