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p212c33: 3 A simple Electromagnetic Wave Pulse: E and B constant within a “sheet” moving at velocity v z x y E B v... need to verify consistency with Maxwell’s Equations
Citation preview
p212c33: 1
Electromagnetic Waves
Maxwell’s Equations
om
o
M
Ec
enc
KK
dtdldE
dtdIldB
AdB
QAdE
)(
0
p212c33: 2
“Sourceless” Maxwell’s Equations
AdBdtd
dtdldE
AdEdtd
dtdldB
AdB
AdE
M
E
0
0
p212c33: 3
A simple Electromagnetic Wave
Pulse: E and B constant within a “sheet” moving at velocity v
z
x
y
E
Bv
... need to verify consistency with Maxwell’s Equations
p212c33: 4
E dA
B dA
0
0
Field lines continue forever: each field line which enters (exits) a closed surface must also enter (exit), so net number of field lines entering (exiting) a closed surface must be zero.
p212c33: 5
EvBELvBL
AdEdtdldB
ELvAdEdtd
ELvdtAdEd
BLldB
0)(
dldA
v dt
L
p212c33: 6
dl
v dt
LdA
BvEBLvEL
AdBdtdldE
BLvAdBdtd
BLvdtAdBd
ELldE
0)(
p212c33: 7
BvEBEv
smc
v
BvEvEB
oo
||
featuresimportant other
1099792458.21in vacuumlight of speed
1
Equations sMaxwell' with consistent is Pulse
8
iff
p212c33: 8
x
y
a
x
tB
xE
x
xaBAdB
axExxEldE
AdBdtdldE
zy
z
yy
0lim take
))()((
General relations between (crossed) E and B fields creating EM waves.
p212c33: 9
x
x
y
a
tE
xB
xaEAdE
axBxxBldB
AdEdtdldB
yz
y
zz
0xlim take
))()((
p212c33: 10
1;1
1
Start with
2
2
22
2
2
2
2
2
2
2
2
2
vtE
vxE
tE
xE
xB
ttE
tE
t
tB
xxE
xE
x
tB
xE
tE
xB
yy
yy
zyy
zyy
zy
yz
Classical Wave Equation!
p212c33: 11
Ey
Bz
x
Sinusoidal Electromagnetic Waves
maxmax
max
max
22)sin(ˆ
)sin(ˆ
vBE
vk
f
fk
tkxBzB
tkxEyE
p212c33: 12
Energy in an electromagnetic wave
2
)(sin
WaveHarmonic aFor so
but
21
21
2max
22max
2
2
22
Eu
tkxEEu
Eu
EvEB
BEu
av
p212c33: 13
eous)(instantanIntensity =Vector Poynting
1
:FlowEnergy )(
:Energy
22
2
SS
BES
EBEvEAdt
dUS
AvdtEudVdU
Energy in an electromagnetic wave
p212c33: 14
Intensity222
)(sinˆ
1
2max
2maxmaxmax
2maxmax
IvEv
EBES
tkxBEx
BES
av
Energy Flow and Harmonic Waves
p212c33: 15
Example: A radio station the surface of the earth emits 50 kW sinusoidal waves. Determine the intensity, and the Electric and Magnetic field amplitudes for an orbiting satellite at a distance of 100 km from the station.
p212c33: 16
cS
AFP
cS
AFP
cS
Vp
Sp
avref
avabs
avgavg
2:PressureRadiation
c=
V
Density Momentum
2
2
Momentum in an electromagnetic wave
p212c33: 17
Example: Satellite in previous example has a 2m diameter antenna. What is the force of the radiation on the antenna assuming perfect reflection?
p212c33: 18
Standing Waves:Superposition of equal amplitude traveling waves
of opposite directions.
Lcncf
nL
nL
nx
tkxBtkxBtkxBB
tkxEtkxEtkxEE
nnn 2
;22
when mode waveStanding
2,
23,,
2
E)(for planes nodalsincos2
)sin()sin(cossin2
)sin()sin(
max
maxmax
max
maxmax
p212c33: 19
Example: EM standing waves are set up in a cavity used for electron spin resonance studies. The cavity has two parallel conducting plates separated by 1.50 cm.
a) Calculate the longest wavelength and lowest frequency of EM standing waves between the walls.
b) Where in the cavity is the maximum magnitude electric field and magnetic field?
p212c33: 20
Electromagnetic Spectrum
(see graphic)
in vacuum, v = c = 2.99792458x108 m/s
f = v increasing frequency <=> decreasing wavelength
visible spectrum: 400 nm (violet) to 700 nm (red)
p212c33: 21
Radiation from a Dipole
Q
Q
Ep k
rkr t
Bp k
v rkr t
Ir
02
02
2
4
4
sin sin( )
sin sin( )
sin
p212c33: 22