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- Electromagnetic Field and Wave
Pham Tan Thi, Ph.D.
Department of Biomedical Engineering
Faculty of Applied Science
Ho Chi Minh University of Technology
- Maxwell’s Equation
Maxwell discovered that the basic principles of electromagnetism can
be expressed in terms of the four equations that now we call Maxwell’s
equations:
(1) Gauss’s law for electric fields;
(2) Gauss’s law for magnetic fields, showing no existence of magnetic
monopole.
(3) Faraday’s law;
(4) Ampere’s law, including displacement current;
- Maxwell’s Equations
Integral form: Differential form:
Gauss’
I Law
Qinside ~ ⇢
~ ~
E · dS = r·E =
"0 "0
Gauss’ Law for Magnetism
I
~ · dS
B ~=0 ~ =0
r·B
Faraday’s Law
I
~ ~ d B @ ~
B
E · dl = ~ =–
r⇥E
dt @t
IAmpere’s Law
~ ~ d E @ ~
E
B · dl = µ0 Ienclosed + µ0 "0 ~ = µ0 J~ + µ0 "0
r⇥B
dt @t
Macroscopic Scale Microscopic Scale
- Gauss’s Law for Electric Field
The flux of the electric field (the area integral of the electric field) over
any closed surface (S) is equal to the net charge inside the surface (S)
divided by the permittivity ε0.
I
~ ~ Qinside
E · dS =
"0
~ Qinside
E · dxdyˆ
n=
~=n
dS ˆ dS = n
ˆ dxdy "0
~ Qinside
E · dxdycos✓ =
"0
dx →
Qinside
dS Edxdy =
dy → "0
2 Qinside
ES = E(4⇡r ) =
"0
Qinside
E= Coulomb’s Law
(4⇡r2 )"0
- Gauss’s Law of Magnetism
Gauss’s law of magnetism states that the net magnetic flux through any
closed surface is zero
I
~ · dS
B ~=0
The number of magnetic field lines that exit equal to the
number for magnetic field lines that enter the closed
surface
→
E
I
~ = Qinside
~ · dS
E
"0
- Faraday’s Law
The electric field around a closed loop is equal to the negative of the
rate of change of the magnetic flux through the area by the loop.
I
~ · d~l = d B ~· d~l = Edlcos✓
~Ed
E
E
dt = Edl
(θ = 0)
d B
E(2⇡R) =
dt
d B
e.m.f =
dt
d B W = F d = Eqd
e.m.f =
dt W
= Ed
d
V = Ed = e.m.f
- Ampère’s Law with Maxwell’s Correction
The line integral of magnetic field over a closed path is equal to the total
current going through any surface bounded by the closed path
I
~ ~ d E
B · dl = µ0 Ienclosed + µ0 "0
dt
1. Time-changing electric fields induces magnetic fields
2. Displacement current
Conduction currents cause Magnetic field
( motion of charged particles)
Time changing electric fields also cause Magnetic field
=> Time changing electric fields is equivalent to a current. We call it
dispalcement current.
- Ampère’s Law with Maxwell’s Correction
The line integral of magnetic field over a closed path is equal to the total
current going through any surface bounded by the closed path
I
~ ~ d E
B · dl = µ0 Ienclosed + µ0 "0
dt
~ · d~l = Bdlcos✓ = Bdl (when θ = 0)
B
I Z
~ ~ d E
B · dl = µ0Bdl
Ienclosed +
= B(2⇡R)
dt
B(2⇡R) = µ0 I
µ0 I
B=
2⇡R
- Ampère’s Law with Maxwell’s Correction
The line integral of magnetic field over a closed path is equal to the total
current going through any surface bounded by the closed path
I
~ ~ d E
B · d l = µ 0 "0 + µ0 Ienclosed
dt
For S1:
I
~ · d~l = µ0 Ienclosed
B
For S2:
I
~ · d~l = 0
B
Two different situations in even one case!
- Ampère’s Law with Maxwell’s Correction
The line integral of magnetic field over a closed path is equal to the total
current going through any surface bounded by the closed path
I
~ ~ d E
B · d l = µ 0 "0 + µ0 Ienclosed
dt
Displacement current
Electric flux is defined as
~ ~ Qinside
E = E · dS =
µ0
For S2:
I ✓ ◆
d Q dQdQ
~ ~
B · dl = µ0 Ienclosed + µ0 "0 = µ 0 "0
dt "0 dt dt
- Recall: Maxwell’s Equations
Integral form: Differential form:
Gauss’
I Law
Qinside ~ ⇢
~ ~
E · dS = r·E =
"0 "0
Gauss’ Law for Magnetism
I
~ · dS
B ~=0 ~ =0
r·B
Faraday’s Law
I
~ ~ d B @ ~
B
E · dl = ~ =–
r⇥E
dt @t
IAmpere’s Law
~ ~ d E @ ~
E
B · dl = µ0 Ienclosed + µ0 "0 ~ = µ0 J~ + µ0 "0
r⇥B
dt @t
Macroscopic Scale Microscopic Scale
- Convert Intergral form to Differential form
I I
Qinside ~ · d~l = d B
~ ~
E · dS = E
"0 dt
ZZZ I I
~ ~ ⇢ d ~d ~~ ~
E · dS = dV ~ ~
E ·E~ ~
dl ·=dl = BdS BdS
V "0 dt dt
Divergence theorem: the flux penetrating a Stokes’ theorem: the circulation of a field E
closed surface S that bounds a volume V is around the loop l that bounds a surface S is
equal to the divergence of the field E inside equal to the flux of curl E over S
the volume I I
ZZZ
~ · dS
~= ~ E ~d~l· =
~ ·E d~l(r ~⇥ E)dS
⇥ E)dS
= (r ~
E (r · E)dV
V
ZZZ !
~ ⇢ @ ~
B
(r · E )dV = 0 ~+
r⇥E dS = 0
V "0 @t
~ ⇢ @ ~
B
r·E = ~ =–
r⇥E
"0 @t
- Divergence Operator
Divergence at a point (x,y,z) is the
measure of the vector flow out of
a surface surrounding that point.
~ =x
E ˆEx + yˆEy + zˆEz
@ @ @
r=xˆ + yˆ + zˆ Fig. 3: No variation →
Fig. 4: Zero divergence
@x @y @z zero divergence
~ = @Ex + @Ey + @Ez
r·E
@x @y @z
≡ (rate of change of E in x direction)
~ @Ex @Ey
+ (rate of change of E in y direction)
r·E =1 +
+ (rate of change of E in z direction)
@x @y
Fig. 5
Fig. 1: Positive Fig. 2: Negative
divergence at P divergence at P
- Curl Operator in a Spherical Coordinate
Curl is a measure of the rotation
of a vector field.
~ =x
E ˆEx + yˆEy + zˆEz
@ @ @
r=x
ˆ + yˆ + zˆ
@x @y @z
2 3
xˆ yˆ zˆ
Fig. 2: How much is the
~ =4 @
r⇥E @ @ 5 Fig. 1: Non-zero curl
@x @y @z curl?
Ex Ey Ez
✓ ◆ ✓ ◆ ✓ ◆
@Ez @Ey @Ex @Ez @Ey @Ex
=x
ˆ + yˆ + zˆ
@y @z @z @x @x @y
≡ (how much does an object in y-z plane rotate)
+ (how much does an object in x-z plane rotate)
+ (how much does an object in x-y plane rotate)
Circulation
Curl =
Area
- Curl Operator in a Cylindrical Coordinate
Curl is a measure of the rotation
of a vector field.
~ = ⇢ˆE⇢ + ˆE + zˆEz
E
1 @ 1 @ @
r= + +
⇢ @⇢ ⇢ @ @z
2 3
1 ˆ 1
⇢⇢ˆ ⇢zˆ
~ = 6@ @ @ 7
r⇥E 4 @⇢ @ @z 5
E⇢ ⇢E Ez
✓ ◆ ✓ ◆ ✓ ◆
~ = ⇢ˆ
r⇥E
@Ez @(⇢E ) ˆ @Ez @E⇢
+
zˆ @(⇢E ) @E⇢ )
⇢ @ @z @⇢ @z ⇢ @ @z
- Differential form: Gauss’ Law for Magnetism
I
~ =0
r·B ⟺ ~ · dS
B ~=0
~ 1 @rBr 1 @B @Bz
~ =
r·B
Bout Bin
=0 r·B = + +
r @r r @ @z
volume ✓ ◆
1 @ µ0 I
= a =0
a @r 2a
B = BA µ0 I
B=
2⇡a
- Differential form: Faraday’s Law
I
@ ~
B d B
~ =–
r⇥E ⟺ ~ · d~l =
E
@t dt
2 3
~ 1 ˆ 1
~ = @ B ⇢⇢ˆ ⇢zˆ
curl of E ~ = 6@ @ @ 7
@t r⇥E 4 @⇢ @ @z 5
Circulation @B~ E0⇢ ⇢E E0 z
=
Area @t zˆ ~⇢
zˆ @ B
~
r⇥E = E =
~
E(2⇡⇢) ~
@B ⇢ ⇢ @t 2
2
=
⇡⇢ @t
~⇢ 1 @ ~
B
~ = @ B ~ =
r⇥E zˆ ⇢
E 2 @t
@t 2
- Differential form: Ampere’s Law with Maxwell’s Corr
I
@ ~
E d E
~ = µ0 J~ + µ0 "0
r⇥B ⟺ ~ ~
B · dl = µ0 Ienclosed +
@t dt
I I
J: Current density J = =
A ⇡R2
~ Circulation
r⇥B = = µ0 J~
Area
B(2⇡R) ~
= µ 0 J
⇡R2
B(2⇡R) Ienclosed
2
= µ0
⇡R ⇡R2
Ienclosed
B = µ0
2⇡R
- Differential form: Ampere’s Law with Maxwell’s Corr
I
@ ~
E d E
~ = µ0 J~ + µ0 "0
r⇥B ⟺ ~ ~
B · dl = µ0 Ienclosed +
@t dt
Start from:
~ = µ0 J~
r⇥B
Take divergence:
~ = µ0 r · J~
r · (r ⇥ B)
!
@⇢ @ ~
@E
~
r·J = = ~ =
("0 r · E) r· "0
@t @t @t
( ⇢ :charge density)
We need to add displacement current term
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