Electromagnetic Field Theory: A Problem Solving Approach Part 7 - Pdf 16

The
Curl
and
Stokes'
Theorem
35
as
1
1
aA,
a
(Vx
A)@
=
lim
r
(rA
o)
a,-o
r
sin
0
Ar
A
r
sin
08 a
r
(19)
The
4

[A,
1
-Ar,_-,])
r
Ar
AO
\
r
Ar
r
AO
(20)
as
Ad
1
a
BA
(Vx
A),
=
lim
-(rAe)
-
(21)
Ar o
r
Ar
AO
r
aOr

Stokes'
Theorem
We
now
piece
together
many
incremental
line
contours
of
the
type
used
in
Figures
1-19-1-21
to
form
a
macroscopic
surface
S
like
those
shown
in
Figure
1-23.
Then

small
surface
elements
C
C= I(VxA)'dS
J's
36
Review
of
Vector
Analysis
Figure
1-23
Many
incremental
line
contours
distributed
over
any
surface,
have
nonzero contribution
to
the
circulation
only
along
those
parts

adjacent
contours
but
which
are
twice
traversed
in
opposite directions
yielding
no
net
line
integral
contribution,
as
illustrated
in
Figure
1-23.
Only
those
contours
with
a
side
on
the open boundary
L
have

to
a
surface
integral
over
any
area
S
bounded
by
the
contour
A
*
dl=
J(Vx
A)*
dS
(25)
Note
that
there
are
an infinite
number
of
surfaces
that
are
bounded

plane
shown
in
Figure
1-24
with
a
vector
The
Curl
and
Stokes'
Theorem
37
zi
-1 ri - i
Figure
1-24
Stokes'
theorem
for
the
vector
given
in
Example
1-7
can be
applied
to

(b)
for the
hemispherical surface
bounded
by
the
contour,
and
(c)
for
the
cylindrical
surface
bounded
by
the
contour.
SOLUTION
For
the
contour
shown
dl=
R
do
i"
so
that
A
*

was
entirely
in
the
xy
plane.
The
curl
of
A
is
VxA=i
aA,
=y2i,
ax
ay
38
Review
of
Vector
Analysis
(a)
For
the
circular
area
in
the plane
of
the

0
2i,
iR
sin
0
dO
d
From Table
1-2
we
use
the
dot
product
relation
i= • i,
=
cos
0
which
again
gives
the
circulation
as
/2
COs
20
w/2
C=

the
upper
circular
area
that
is
perpendicular
to
Vx
A.
The
integral
is
then
the
same
as
part
(a)
as
V
X
A
is
independent
of
z.
1-5-4
Some
Useful

0]
We
integrate
the
normal
component
of
the
vector
V
x
(Vf)
over
a
surface
and
use
Stokes'
theorem
JVx
(Vf).dS=
Vf
dl=
(26)
where
the
zero
result
is
obtained

of
dS
in
(26)
must
be
zero
vx(Vf)=O
The
identity
is
also
easily
proved
by
direct
computation
using
the
determinantal
relation
in
Section
1-5-1
defining the
I
Problems
39
curl
operation:

ayaz
azay
azax
axaz
axay
ayax)
(28)
Each
bracketed
term
in
(28)
is
zero
because
the
order
of
differentiation
does
not
matter.
(b)
The
Divergence
of
the
Curl
of
a

closed
surface
while
Stokes'
theorem
is
true
in
general
for
an
open
surface.
Stokes'
theorem
for
a
closed
surface
requires
the
contour
L to
shrink
to
zero
giving
a
zero
result for the

which
proves
the
identity
because
the
volume
is
arbitrary.
More
directly
we
can
perform
the
required
differentiations
V.
(VxA)
a,
aA,
aA,
\
a
aA
aA)
a
aA,
aA\
-ax\y

azay)
\azax
ax(z
where
again
the
order
of
differentiation
does
not
matter.
PROBLEMS
Section
1-1
1.
Find
the
area of
a
circle
in
the
xy
plane
centered
at
the
origin
using:

a.
Which
coordinate
system
is
easier
to
use?
2.
Find
the
volume
of
a
sphere
of
radius
R
centered
at
the
origin
using:
(a)
rectangular
coordinates
x
2
+y
2

Which
coordinate
system
is
easiest?
Section
1-2
3.
Given
the
three
vectors
A
=
3ix
+
2i,
-
i.
B
=
3i,
-
4i,
-
5i,
C=
i.
-i,
+i,

(e)
Ax
(B
x
C),
B(A
C)-
C(A
-
B)
[Are
they
equal?]
(f)
What
is
the
angle between
A
and
C
and
between
B
and
AxC?
4.
Given
the
sum

and
B,
show
that
the
component
of
B
parallel
to
A
is
B'A
Bll
=
A
A*A
(Hint:
Bi
=
aA.
What
is
a?)
(b)
If
the
vectors
are
A

between
each
of
the
following
vectors:
A
=
4i.
-
2i,
+
2i,
B=
-6ix
+
3i,
-
3i,
C=
i.
+
3,+i,
7.
Given
the
two
vectors
A=3i,+4i,
and

+A,i,
+Aii
the
directional
cogines
are
defined
as
the
cosines
of
the
angles
between
A
and
each
of
the Cartesian
coordinate
axes.
Find
each
of
these
directional
cosines
and
show
that

in
terms
of
the
lengths
of
A
and
B
and
the
enclosed
angle
0c.
The
result
is
known
as
the
law
of
cosines.
(Hint:
C
C =
(B
-
A)
(B

Review
of
Vector
Analysis
10.
(a)
Prove
that
the
dot
and
cross
can be
interchanged
in
the
scalar
triple
product
(AxB)
.C=(BxC)
A=
(CxA)
B
(b)
Show
that
this
product
gives

of
(a)
and
find
the
volume
of
the paral-
lelepiped
formed
by
the
vectors.
(d)
Prove
the
vector
triple
product
identity
A
x
(B
x
C)
=
B(A- C)- C(A
B)
I(A
x

using
Cartesian
coordinates
in
terms
of
their
angles
0
and
4
from
the
x
axis.
(b)
Using
the
results
of
(a)
derive
the
trigonometric
expansions
sin(O
+) =
sin
0
cos

functions
where
a
and
b
are
constants:
(a)
f =
axz
+bx-y
(b)
f=
(a/r)
sin
4
+brz
2
cos
30
(c)
f
=
ar
cos
0
+
(b/r
2
)

following vectors:
(a)
A=
xi,
+
i,+zi,
=
ri,
(b)
A=
(xy
2)[i.
+i,
+
i]
(c)
A=
rcos
Oi,+[(z/r)
sin
0)]i,
(d)
A=
r
2
sin
0
cos
4
[i,

constant
unit
vector.)
(b)
tVxFdV=
-FxdS
(Hint:
LetA=ixF.)
(c)
Using
the
results
of
(a)
show
that
the
normal
vector
integrated
over
a
surface
is
zero:
dS=
0
(d)
Verify
(c)

dS=
J[fV2g-
gV2f]
dV
(Hint:
V
(fVg)=
fV
2
g+
Vf
Vg.)
17.
(a)
Find
the
area element
dS
(magnitude
and
diirection)
on
each of
the
four
surfaces
of
the
pyramidal
figure

as
4 =
IV -
AdV
2J
-4
b
Section
1-5
18.
Find
the
curl
of
the
following
vectors:
(a)
A=
x
2
yi
+2
Yi,
+yi
A


Nhờ tải bản gốc

Tài liệu, ebook tham khảo khác

Music ♫

Copyright: Tài liệu đại học © DMCA.com Protection Status