Prof. D. Wilton ECE Dept. Notes 11 ECE 2317 Applied Electricity and Magnetism Notes prepared by the...
-
Upload
bertram-roberts -
Category
Documents
-
view
217 -
download
0
Transcript of Prof. D. Wilton ECE Dept. Notes 11 ECE 2317 Applied Electricity and Magnetism Notes prepared by the...
Prof. D. WiltonECE Dept.
Notes 11
ECE 2317 ECE 2317 Applied Electricity and MagnetismApplied Electricity and Magnetism
Notes prepared by the EM group,
University of Houston.
Gauss
ExampleExample
Assume D D
infinite uniform line charge
encl
S
D n dS Q
Find the electric field everywhere
x
y
z
S
l = l0 [C/m]
h
r
Example (cont.)Example (cont.)
0
0
2
2
2
c cS S S
l
l
D n dS D dS D dS
D h
D h h
D
Hence
So 0
0
V/m2
lE
ExampleExample
v = 3 2 [C/m3] , < a
Assume D D
non-uniform infinite cylinder of volume charge density
encl
S
D n dS Q
x
y
z
S
h
a
r
Find the electric field everywhere
Example (cont.)Example (cont.)(a) < a
2
0 0 0
0
2
0
4
0
4
2
2 3
32
4
3
2
encl v
V
h
v
v
encl
Q dV
d d dz
h d
h d
h
Q h
S
h
r
Example (cont.)Example (cont.)
Hence
So
4
3
2
32
23
4
cS S S
D n dS D n dS D dS
D h
D h h
D
3
0
3V/m
4E a
ExampleExample
x
y
z
l0 -h
-h
When Gauss’s Law is not useful:
!
!
encl
S
encl
D n dS Q
D D
Q h
(3) E has more than one component
But (1)
(2) (the charge density is not uniform!)
ExampleExample
y
z
x
s = s0 [C/m2]
Assume
zD z D z
encl
S
D n dS Q S
A
r
Find the electric field everywhere
2
top
bottom
z encl
S
z
S
z encl
S
z z encl
z z
z encl
D z n dS Q
D z z dS
D z z dS Q
D A D A Q
D D
AD Q
Example (cont.)Example (cont.)
Assume
S
A
r
D
D
z
0
0 0
0
2
2 2
2
encl s
z encl
s sz
sz z
Q A
AD Q
AD
A
D D
Example (cont.)Example (cont.)
so 0
0
[V/m] 0, 02
sE z z z
S
A
r
( Generally, Ez is continuous except on either side of a surface charge)
ExampleExample
slab of uniform charge
0 0
x
x x
x
E x E x
E x E x
E
Assume
(since Ex(x) is a continuous function)
y
x
30 [C/m ]v
d
rFind the electric field everywhere
Example (cont.)Example (cont.)(a) x > d / 2
0
0
0 ( / 2)
/ 2
t b
x encl
S
x x encl
S S
x x encl v
x v
D x n dS Q
D x x dS D x x dS Q
D x A D A Q A d
D x d
0
0
V/m ( / 2)2
v dE x x d
A
S
xxr
30 [C/m ]v
d
Example (cont.)Example (cont.)
Note: If we define
0
0
0
0
V/m2
Note:
so
effs v
effs
effv s
effs v
d
E x
Q Ad A
d
Q
seff
Q
v0
(sheet formula) then
d
A A
Example (cont.)Example (cont.)
(b) 0 < x < d / 2
0
0
x encl v
x v
D A Q A x
D x
y
x
x = 0
x = xS
r
0
0
V/m 0 / 2v xE x x d
30 [C/m ]vd