James Clerk Maxwell1831-1879
Maxwell’s Theory• Electricity and magnetism were originally thought to be
unrelated
• Maxwell’s theory showed a close relationship between all electric and magnetic phenomena and proved that electric and magnetic fields play symmetric roles in nature
• Maxwell hypothesized that a changing electric field would produce a magnetic field
• He calculated the speed of light – 3x108 m/s – and concluded that light and other electromagnetic waves consist of fluctuating electric and magnetic fields
James Clerk Maxwell1831-1879
Maxwell’s Theory• Stationary charges produce only electric fields
• Charges in uniform motion (constant velocity) produce electric and magnetic fields
• Charges that are accelerated produce electric and magnetic fields and electromagnetic waves
• A changing magnetic field produces an electric field
• A changing electric field produces a magnetic field
• These fields are in phase and, at any point, they both reach their maximum value at the same time
Modifications to Ampère’s Law• Ampère’s Law is used to analyze magnetic fields
created by currents
• But this form is valid only if any electric fields present are constant in time
• Maxwell modified the equation to include time-varying electric fields and added another term, called the displacement current, Id
• This showed that magnetic fields are produced both by conduction currents and by time-varying electric fields
IsdB 0
dt
d E 00
dt
dI E
d
0
Maxwell’s Equations• In his unified theory of electromagnetism, Maxwell
showed that the fundamental laws are expressed in these four equations:
0q
AdE
0 AdB
dt
dsdE B
IsdB 0
dt
d E 00
Maxwell’s Equations• Gauss’ Law relates an electric field to the charge
distribution that creates it
• The total electric flux through any closed surface equals the net charge inside that surface divided by o
0q
AdE
0 AdB
dt
dsdE B
IsdB 0
dt
d E 00
Maxwell’s Equations• Gauss’ Law in magnetism: the net magnetic flux
through a closed surface is zero
• The number of magnetic field lines that enter a closed volume must equal the number that leave that volume
• If this wasn’t true, there would be magnetic monopoles found in nature
0q
AdE
0 AdB
dt
dsdE B
IsdB 0
dt
d E 00
Maxwell’s Equations• Faraday’s Law of Induction describes the creation of an
electric field by a time-varying magnetic field
• The emf (the line integral of the electric field around any closed path) equals the rate of change of the magnetic flux through any surface bounded by that path
0q
AdE
0 AdB
dt
dsdE B
IsdB 0
dt
d E 00
Maxwell’s Equations• Ampère-Maxwell Law describes the creation of a
magnetic field by a changing electric field and by electric current
• The line integral of the magnetic field around any closed path is the sum of o times the net current through that path and o times the rate of change of electric flux through any surface bounded by that path
0 AdB
0q
AdE
IsdB 0
dt
d E 00
dt
dsdE B
Maxwell’s Equations• Once the electric and magnetic fields are known at
some point in space, the force acting on a particle of charge q can be found
• Maxwell’s equations with the Lorentz Force Law completely describe all classical electromagnetic interactions
0 AdB
IsdB 0
dt
d E 00
0q
AdE
dt
dsdE B
BvqEqF
Maxwell’s Equations• In empty space, q = 0 and I = 0
• The equations can be solved with wave-like solutions (electromagnetic waves), which are traveling at the speed of light
• This result led Maxwell to predict that light waves were a form of electromagnetic radiation
0 AdB
dt
dsdE B
IsdB 0
dt
d E 00
0q
AdE
Electromagnetic Waves• From Maxwell’s equations applied to empty space, the
following relationships can be found:
• The simplest solutions to these partial differential equations are sinusoidal waves – electromagnetic waves:
• The speed of the electromagnetic wave is:
2
2
002
2
t
E
x
E
2
2
002
2
t
B
x
B
00
1
k
v m/s 10 2.99792 8c
)cos();cos( maxmax tkxBBtkxEE
max
max
B
E
B
E
Plane Electromagnetic Waves• The vectors for the electric and magnetic
fields in an em wave have a specific space-time behavior consistent with Maxwell’s equations
• Assume an em wave that travels in the x direction
• We also assume that at any point in space, the magnitudes E and B of the fields depend upon x and t only
• The electric field is assumed to be in the y direction and the magnetic field in the z direction
Plane Electromagnetic Waves• The components of the electric and
magnetic fields of plane electromagnetic waves are perpendicular to each other and perpendicular to the direction of propagation
• Thus, electromagnetic waves are transverse waves
• Waves in which the electric and magnetic fields are restricted to being parallel to a pair of perpendicular axes are said to be linearly polarized waves
John Henry Poynting 1852 – 1914
Poynting Vector• Electromagnetic waves carry energy
• As they propagate through space, they can transfer that energy to objects in their path
• The rate of flow of energy in an em wave is described by a vector, S, called the Poynting vector defined as:
• Its direction is the direction of propagation and its magnitude varies in time
• The SI units: J/(s.m2) = W/m2
• Those are units of power per unit area
1
oμ S E B
Poynting Vector• Energy carried by em waves is shared equally by the
electric and magnetic fields
• The wave intensity, I, is the time average of S (the Poynting vector) over one or more cycles
• When the average is taken, the time average of cos2(kx - ωt) = ½ is involved
2 2max max max max
avg 2 2 2o o o
E B E c BI S
μ μ c μ
Energy Density• The energy density, u, is the energy per unit volume
• It can be shown that
• The instantaneous energy density associated with the magnetic field of an em wave equals the instantaneous energy density associated with the electric field and in a given volume this energy is shared equally by E and B
• The total instantaneous energy density is the sum of the energy densities associated with each field:
u =uE + uB = εoE2 = B2 / μo
221
2 2B E oo
Bu u ε E
μ
Energy Density• When this is averaged over one or more cycles, the
total average becomes
uavg = εo(E2)avg = ½ εoE2max = B2
max / 2μo
• The intensity of an em wave equals the average energy density multiplied by the speed of light
I = Savg = cuavg
• Electromagnetic waves transport linear momentum as well as energy
• As this momentum is absorbed by some surface, pressure is exerted on the surface
Chapter 34Problem 6
An electron moves through a uniform electric field E = (2.50 i^ + 5.00 j^) V/m and a uniform magnetic field B = (0.400 k^) T. Determine the acceleration of the electron when it has a velocity v = 10.0 i^ m/s.
Hertz’s Experiment• In 1887 Hertz was the first to experimentally
generate and detect electromagnetic waves
• An induction coil was connected to two large spheres forming a capacitor
• Oscillations were initiated by short voltage pulses by the coil
• As the air in the gap is ionized, it becomes a better conductor
• At a very high frequencies the discharge between the electrodes exhibited an oscillatory behavior
Heinrich Rudolf Hertz 1857 – 1894
Hertz’s Experiment• The inductor and capacitor formed the
transmitter, equivalent to an LC circuit from a circuit viewpoint
• Several meters away from the transmitter was the receiver (a single loop of wire connected to two spheres) with its own inductance and capacitance
• When the resonance frequencies of the transmitter and receiver matched, energy transfer occurred between them
Heinrich Rudolf Hertz 1857 – 1894
Hertz’s Results• Hertz hypothesized the energy transfer was in the form
of waves (now known to be electromagnetic waves)
• Hertz confirmed Maxwell’s theory by showing the waves existed and had all the properties of light waves (with different frequencies and wavelengths)
• Hertz measured the speed of the waves from the transmitter (used the waves to form an interference pattern and calculated the wavelength)
• The measured speed was very close to 3 x 108 m/s, the known speed of light, which provided evidence in support of Maxwell’s theory
Electromagnetic Waves Produced by an Antenna
• Neither stationary charges nor steady currents can produce electromagnetic waves
• The fundamental mechanism responsible for this radiation: when a charged particle undergoes an acceleration, it must radiate energy in the form of electromagnetic waves
• Electromagnetic waves are radiated by any circuit carrying alternating current
• An alternating voltage applied to the wires of an antenna forces the electric charge in the antenna to oscillate
Electromagnetic Waves Produced by an Antenna
• Half-wave antenna: two rods are connected to an ac 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) and the oscillations continue (d)
Electromagnetic Waves Produced by an Antenna
• 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 lines form concentric circles around the antenna and are perpendicular to the electric field lines at all points
• The antenna can be approximated by an oscillating electric dipole
The Spectrum of EM Waves• Types of electromagnetic
waves are distinguished by their frequencies (wavelengths): c = ƒ λ
• There is no sharp division between one kind of em wave and the next – note the overlap between types of waves
The Spectrum of EM Waves• Radio waves are used in
radio and television communication systems
• Microwaves (1 mm to 30 cm) are well suited for radar systems + microwave ovens are an application
• Infrared waves are produced by hot objects and molecules and are readily absorbed by most materials
The Spectrum of EM Waves• Visible light (a small
range of the spectrum from 400 nm to 700 nm) – part of the spectrum detected by the human eye
• Ultraviolet light (400 nm to 0.6 nm): Sun is an important source of uv light, however most uv light from the sun is absorbed in the stratosphere by ozone
The Spectrum of EM Waves• X-rays – most common
source is acceleration of high-energy electrons striking a metal target, also used as a diagnostic tool in medicine
• Gamma rays: emitted by radioactive nuclei, are highly penetrating and cause serious damage when absorbed by living tissue
Chapter 34Problem 11
In SI units, the electric field in an electromagnetic wave is described by Ey = 100 sin (1.00 × 107 x – ωt). Find (a) the amplitude of the corresponding magnetic field oscillations, (b) the wavelength λ, and (c) the frequency f.