emlab 1 5. conductors and dielectrics. emlab 2 contents 1.current and current density 2.continuity...
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EMLAB
1
5. Conductors and dielectrics
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EMLAB
2Contents
1. Current and current density
2. Continuity of current
3. Metallic conductors
4. Conductor properties and boundary conditions
5. The method of images
6. Semiconductors
7. Dielectric materials
8. Boundary conditions for dielectric materials
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EMLAB
3
Current and voltage
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EMLAB
55.1 Current and current density
dt
dQI
I
S
dII aJSJ
nJ ˆS
I
n
• Current is electric charges in motion, and is defined as the rate of movement of charges passing a given reference plane.
• In the above figure, current can be measured by counting charges passing through surface S in a unit time.
S
• In field theory, the interest is usu-ally in event occurring at a point rather than within some large region.
•For this purpose, current density measured at a point is used, which is current divided by the area.
I
J
S
Current
Current density
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EMLAB
6Current density from velocity and charge density
tv
S
vJ
S
IS
t
QI
tSVQ
,
volume)(
Charges with density ρ
With known charge density and velocity, cur-rent density can be calculated.
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EMLAB
7Continuity equation : Kirchhoff ’s current law
Q I
J
tSq nJ ˆ
Charges going out through dS.
nFor steady state, charges do not accumulate at any nodes, thus ρ become constant.
.currentSteady;0
t
J
t
dt
dddt
dd
dddtdQ
VVVC
VC
J
JaJ
aJ
dS
t
J t
dQI
nn
differential form
integral form
Kirchhoff ’s current law
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EMLAB
8
+
-
Electron energy level
- -
- -
- -
1 atom
Electrons in an isolated atom
Tightly bound electron
Energy levels and the radii of the electron orbit are quantized and have discrete values. For each energy level, two electrons are accommodated at most.
-
-
More freely moving electron
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EMLAB
9
+-
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Atoms in a solid are arranged in a lattice structure. The electrons are attracted by the nuclei. The amount of attractions differs for various material.
Electrons in a solid
Freely moving elec-tron
Tightly bound elec-tron
-
Electron energy level
To accommodate lots of electrons, the discrete energy levels are broad-ened.
extE
External E-field
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EMLAB
10
-
Energy level of insula-tor atoms
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-
Energy level of con-ductor atom
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Insulator and conductorInsulator atoms Conductor atoms
Occupied energy level
Empty energy level
External E-field External E-field
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EMLAB
11Movement of electrons in a conductor
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EMLAB
12
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EMLAB
13
+-
+-
+-
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+-
+-
+-
E
EEF eq
Ev e
EE ee nene ))((
vJ
EJ
: Electric conductivity
; Ohm’s law
Electron flow in metal : Ohm’s law
• n: Electron density (number of electrons per unit vol-ume.
• μ : mobility
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EMLAB
14
J
AB
BA
A
B
A
B
B
ABA dddV LJ
rJ
rErE
BABABA LS
IL
JV
S
lRIRVBA ,
Example : calculation of resistance
SSd
d
d
d
I
VR
aE
rE
aJ
rE
S
AB
S
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EMLAB
15Conductivities of materials
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EMLAB
16
E
-q1+q1
Conductor
1. Tangential component of an external E-field causes a positive charge (+q) to move in the di-rection of the field. A negative charge (-q) moves in the opposite direction.
2. The movement of the surface charge compensates the tangential electric field of the external field on the surface, thus there is no tangential electric field on the surface of a conductor.
3. The uncompensated field component is a normal electric field whose value is proportional to the surface charge density.
4. With zero tangential electric field, the conductor surface can be assumed to be equi-potential.
0
Sn
t
ˆ
0
nE
E
-q1
Conductor
EE in
Electric field on a conductor due to external field
normal component
tangential component
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EMLAB
17Charges on a conductor
1. In equilibrium, there is no charge in the interior of a conductor due to repulsive forces between like charges.
2. The charges are bound on the surface of a conduc-tor.
3. The electric field in the interior of a conductor is zero.
4. The electric field emerges on the positive charges and sinks on negative charges.
5. On the surface, tangential component of electric field becomes zero. If non-zero component exist, it induces electric current flow which generates heats on it.
0inE
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EMLAB
18Image method
• If a conductor is placed near the charge q1,
the shape of electric field lines changes due to the induced charges on the conductor.
• The charges on the conductor redistribute themselves until the tangential electric field on the surface becomes zero.
•If we use simple Coulomb’s law to solve the problem, charges on the conductors as well as the charge q1 should be taken into account. As
the surface charges are unknown, this approach is difficult.
• Instead, if we place an imaginary charge whose value is the negative of the original charge at the opposite position of the q1, the
tangential electric field simply becomes zero, which solves the problem.
+q1
Perfect electric conductor
0ˆ0tan nEEn
-q1
0ˆ0tan nEE
Image charge
+q1
- - - -
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EMLAB
19
+q1
도체
0ˆ0tan nEE
n
-q1
0ˆ0tan nEE
Image charge
+q1
0
zya
ˆa2
4
q)0x(
zy)ax(
zˆyˆ)ax(ˆ
4
q
zy)ax(
zˆyˆ)ax(ˆ
4
q
tan
2/32220
1
2/32220
1
2/32220
1
E
xE
zyx
zyxE
z
x)0,0,a(
)0,0,a(
)0,0,a(
• The electric field due to a point charge is in-fluenced by a nearby PEC whose charge distri-bution is changed. In this case, an image charge method is useful in that the charges on the PEC need not be taken into account.
•As shown in the figure on the right side, the presence of an image charge satisfies the boundary condition imposed on the PEC sur-face, on which tangential electric field be-comes zero.
• This method is validated by the uniqueness theorem which states that the solution that sat-isfy a given boundary condition and differen-tial equation is unique.
z
x
Example : a point charge above a PEC plane
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EMLAB
20
molecule
Dielectric material
The charges in the molecules force the molecules aligned so that externally applied electric field be decreased.
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EMLAB
21Dielectric material
S
0
S0 ˆ
zE
d
zx
S
0E -+
-+
S S
pE
inESˆ zD Sˆ zD
• D (electric flux density) is related with free charges, so D is the same despite of the dielectric material.
• But the strength of electric field is changed by the induced dipoles inside.
EED )1( e0
(1) No material (2) With dielectric material
inine
einine
inein
ineppin
EEED
EEEE
EEE
EEEEE
)1(
1)1(
,
000
00
0
0
0E
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EMLAB
22
+q
-q
)cosr,sinr,0( P
)2/d,0,0(Q
)2/d,0,0(Q
)d,0,0(d
d
.momentdipole;1
drp qqN
iii
θ
z
Electric dipole
sinˆcos2ˆ4
cos
4
ˆ
4
cos
4
4
11
444
30
20
20
20
0000
θrE
rp
r
qdV
rr
qd
r
PQPQq
PQPQ
PQPQq
PQPQ
q
PQ
q
PQ
qV
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EMLAB
23
S
d
xS
0E -+
-+
S S
pE
inE0E
0
S0 ˆ
zE
r
S
0
zE
-+
-+
Electric field in dielectric material
Induced dipole 에 의해 물질 내부 전기장 세기 줄어듦 . 도체 양단의 전압을 측정하면 전압이 줄어듦 .
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EMLAB
24
-+ -+
+q1-
+
-+ -
+
- +
-+
-+
-+
-+
-+
-+
-+
-+
-+
-+
-+
-+
-+
- +
-+-
+ -+
- +
-+
-+
-+
-+ -
+
-+
-+ -
+
-+-+
-+
-+
-+
-+
-+
-+
-+ -
+-+
-+
-+
-+
-+
-+
-+
Gauss’ law in Dielectric material
PED
aDaPE
aPaE
in
SS
in
SS
in
dd
dd
0
free0
freeboundfreetotal0
q
qqqQ
-+
- +
DipoleLength : d
d
SSS
S
ddNdNqdqNVq
ddSdV
aPapan
an
ˆ)()(
ˆ
bound
V
ineEP 0
Induced dipole
p
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EMLAB
25Relative permittivity
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EMLAB
26Boundary conditions
(1) Boundary condition on tangential electric field component
Tangential boundary condition can be derived from the result of line integrals on a closed path.
1C
τEτE
τEτEsE
ˆˆ
)wˆwˆ(d0V
21
C
21
1
unit vector tangential to the surface
t2t1 EE
(2) Boundary condition on normal component of electric field
Boundary condition on normal component can be obtained from the result of surface integrals on a closed surface.
density) charge surface(ˆˆ
0ˆ
,0 If
ˆ)ˆˆ(
12
side curved
side curved12
S
S VV
h
h
h
ShhS
ddda
nDnD
τD
τDnDnD
DD
Sn11n22Sn1n2 EEDDS
n
Unit vector normal to the surface
S
h
Medium #1
Medium #2
Medium #1
Medium #2
τ
w
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EMLAB
27
E
-q1+q1
Conductor
1. Tangential component of an external E-field causes a positive charge (+q) to move in the di-rection of the field. A negative charge (-q) moves in the opposite direction.
2. The movement of the surface charge compensates the tangential electric field of the external field on the surface, thus there is no tangential electric field on the surface of a conductor.
3. The uncompensated field component is a normal electric field whose value is proportional to the surface charge density.
4. With zero tangential electric field, the conductor surface can be assumed to be equi-potential.
0
Sn
t
ˆ
0
nE
E
-q1
Conductor
EE in
Example – conductor surface
normal component
tangential component
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EMLAB
28
1E
2E21
21
: component normal
:component tangential
nn
tt
DD
EE
1
2
12
2
2
11
21
2
112
1211
222
2222
1112221n12n21n2n
11221t2t
cossinE
cossincossin
coscos
sinsin
EEEEE
EEEEDD
EEEE1
2
Surface charge density of dielectric interface can not be infinite.
Example – dielectric interface
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EMLAB
29Example – dielectric interface
0
z
D
z
D
y
D
x
D zzyxD
Sz
z
D
CD
The normal component of D is equal to the surface charge density.
x
yz
Szz DD 21
Szz EE 2211
11
22
1122
0dddEdEdV SS
zzd
rE
SSdQ ssS )ˆ)(ˆ( zzaD
1
1
2
21
12
2
dd
S
dd
S
V
QC
SS
s
Capacitance :
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EMLAB
30
0C drE 0 E
Static electric field : Conservative property
정전기장에 의한 potential difference VAB 는 시작점과 끝점이 고정된 경우 , 적분
경로와 상관없이 동일한 값을 갖는다 .
21 CC
BA ddV rErE
AAV
BBV
1C
2C
3C
021
CC
Cddd rErErE
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EMLAB
31
n
CndrE
C
drE
nC
임의의 닫혀진 경로에 대한 선적분은 매우 작은 폐곡선의 선적분의 합으로 분해할 수 있다 .
Stokes’ theorem
aErE ddSC
• 벡터함수를 임의의 닫혀진 경로에 대한 선적분을 하는 경우 그
경로로 둘러싸인 면에 대한 면적분으로 바꿀 수 있다 .
• 이 때 피적분 함수는 원래 함수의 ‘ curl’ 로 바꿔야 한다 .
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EMLAB
32Line integral over an infinitesimally small closed path
xy
yEy
yEyx
xEx
xE
dxy
yEdyx
xEdxy
yEdyx
xE
dxEdyEdxEdyEd
xxyy
xyxy
xyxyCn
2222
2222
1
4
4
3
3
2
2
1
1
4
4
3
3
2
2
1rE
S
xy dyxy
E
x
EaE
yx
d
y
E
x
EnC
S
xyz
rEE
0Lim)(
),,( zyx y
x
z
yxz ˆ)( E
zyxE ˆˆˆ zyx EEE
y
E
x
E
x
E
z
E
z
E
y
E xyzxyz zyxE ˆˆˆ