Transcript E&M Waves

Chapter 21
Electromagnetic Waves
Exam II
Curve: +30
General Physics
Electromagnetic Waves
Ch 21, Secs 8–12
General Physics
James Clerk Maxwell
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1831 – 1879
Electricity and magnetism were
originally thought to be
unrelated
In 1865, James Clerk Maxwell
provided a mathematical theory
that showed a close
relationship between all electric
and magnetic phenomena
Electromagnetic theory of light
General Physics
Maxwell’s Starting Points
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Electric field lines originate on
positive charges and terminate
on negative charges
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Magnetic field lines always form
closed loops – they do not begin
or end anywhere
General Physics
Can electric fields
form closed loops?
1.
2.
Yes
No
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Maxwell’s Starting Points
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A varying magnetic field induces
an emf and hence an electric
field (Faraday’s Law)
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Magnetic fields are generated by
moving charges or currents
(Ampère’s Law)
General Physics
Maxwell’s Hypothesis
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Turning Faraday’s Law upside
down, Maxwell hypothesized that
a changing electric field would
produce a magnetic field
(Maxwell-Ampère’s Law)
General Physics
Maxwell Equations
closed surface
enclosed charge
closed loop
• Conservation of energy
closed surface
closed loop
linked flux
no mag. charge
linked current + flux
• Conservation of charge
Lorentz force law
General Physics
Maxwell’s Predictions
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Maxwell concluded that visible light and all other
electromagnetic (EM) waves consist of fluctuating
electric and magnetic fields, with each varying
field inducing the other
Accelerating charges generate these time varying
E and B fields
Maxwell calculated the speed at which these
electromagnetic waves travel in a vacuum –
speed of light c = 3.00 x 108 m/s
General Physics
Hertz’s Confirmation of
Maxwell’s Predictions
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1857 – 1894
First to generate and detect
electromagnetic waves in a
laboratory setting
Showed radio waves could
be reflected, refracted and
diffracted
The unit Hz is named for
him
General Physics
Hertz’s Experimental Apparatus
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An induction coil is
connected to two large
spheres forming a capacitor
Oscillations are initiated by
short voltage pulses
The oscillating current
(accelerating charges)
generates EM waves
General Physics
Hertz’s Experiment
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Several meters away from
the transmitter is the
receiver
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This consisted of a single
loop of wire connected to
two spheres
When the oscillation frequency of the transmitter
and receiver matched, energy transfer occurred
between them
General Physics
Hertz’s Conclusions
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Hertz hypothesized the energy transfer was in
the form of waves
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These are now known to be electromagnetic waves
Hertz confirmed Maxwell’s theory by showing the
waves existed and had all the properties of light
waves (e.g., reflection, refraction, diffraction)
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They had different frequencies and wavelengths which
obeyed the relationship v = f λ for waves
v was very close to 3 x 108 m/s, the known speed of
light
General Physics
EM Waves by an Antenna
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Two rods are connected to an oscillating source, charges oscillate
between the rods (a)
As oscillations continue, the rods become less charged, the field
near the charges decreases and the field produced at t = 0
moves away from the rod (b)
The charges and field reverse (c) – the oscillations continue (d)
General Physics
EM Waves by an Antenna, final
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Because the oscillating charges in the
rod produce a current, there is also a
magnetic field generated
As the current changes, the magnetic
field spreads out from the antenna
The magnetic field is perpendicular to
the electric field
General Physics
Electromagnetic Waves,
Summary
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A changing magnetic field produces an
electric field
A changing electric field produces a
magnetic field
These fields are in phase
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At any point, both fields reach their maximum
value at the same time
General Physics
Electromagnetic Waves are
Transverse Waves
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The E and B fields are
perpendicular to each other
Both fields are
perpendicular to the
direction of motion
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Therefore, EM waves are
transverse waves
Active Figure: A Transverse Electromagnetic Wave
General Physics
Properties of EM Waves
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Electromagnetic waves are transverse waves
They travel at the speed of light
c
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This supports the fact that light is an EM wave
General Physics
Properties of EM Waves, 2
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The ratio of the electric field to the magnetic field is
equal to the speed of light
E Emax
c 
B Bmax
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Electromagnetic waves carry energy as they travel
through space, and this energy can be transferred to
objects placed in their path
General Physics
Properties of EM Waves, 3
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Energy carried by EM waves is shared
equally by the electric and magnetic fields
Average power per unit area
2
max
2
max
Pave
Emax Bmax E
cB
I 
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A
20
20c 20
General Physics
Properties of EM Waves, final
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Electromagnetic waves transport linear
momentum as well as energy
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For complete absorption of energy U
p = U/c  F = Pave/c
For complete reflection of energy U
p = (2U)/c  F = 2Pave/c
Radiation pressures (forces) can be
determined experimentally
General Physics
Determining Radiation Pressure
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This is an apparatus for
measuring radiation
pressure
In practice, the system is
contained in a vacuum
The pressure is
determined by the angle
at which equilibrium
occurs
General Physics
Summary of Properties of
Electromagnetic (EM) Waves
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They travel at the speed of light
They are transverse waves
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Ratio of E and B field magnitudes: E/B=c
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E, B perpendicular to each other and velocity
Electric and magnetic fields carry equal energy
They carry both energy and momentum
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Can deliver U and p to a surface
General Physics
The Spectrum of EM Waves
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Forms of electromagnetic waves
exist that are distinguished by
their frequency and wavelength
 c = ƒλ
Wavelengths for visible light
range from 400–700 nm
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a small portion of the spectrum
Wavelengths
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1
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km = 10-3 m (radio) electronic
m = 10-6 m (visible, IR)
nm = 10-9 m (UV, X-ray)
Å = 10-10 m (X-ray) atomic
fm =10-15 m (-ray) nuclear
General Physics