Electromagnetic Theory
• Theoretical understanding of electricity
and magnetism
– Seemed complete by around 1850
– Coulomb’s Law and Gauss’ Law explained electric fields and forces
– Ampère’s Law and Faraday’s Law explained magnetic fields and forces
Unanswered Questions
• What was the nature of electric and
magnetic fields?
• What is the idea of action at a distance?
• How fast do the field lines associated with
a charge react to a movement in the
charge?
• Maxwell’s work led to the discovery of
electromagnetic waves
Discovery of EM Waves
• A time-varying magnetic field gives rise to an electric field
– A magnetic field can produce an electric field
• Maxwell proposed a modification to Ampère’s Law
– A time-varying electric field produces a magnetic field
– This gives a new way to create a magnetic field
– Also gives equations of electromagnetism a symmetry
• James Clerk Maxwell studied some of these questions in the mid-1800’s
Symmetry of E and B
• The correct form of Ampère’s Law (due to Maxwell) says that a changing electric flux produced a magnetic field.
– Since a changing electric flux can be caused by a changing E, there was an indication that a changing
electric field produces a magnetic field
• Faraday’s Law says that a changing magnetic flux produces an induced emf, and an emf is always
associated with an electric field
– Since a changing magnetic flux can be caused by a changing B, we can also say that a changing
Section 23.1
Symmetry of E and B, cont.
Electromagnetic Waves
• Self-sustaining oscillations involving E and B are possible
• The oscillations are an electromagnetic wave
– Electromagnetic waves are also referred to as electromagnetic radiation
• Both the electric and magnetic fields must be changing with time
• Maxwell worked out the details of em waves in great mathematical detail in ~1850
• Experimental proof of the existence of the waves was not found until 1887
Perpendicular Fields
• According to Faraday’s Law, a changing
magnetic flux through a given area produces an electric field
– The direction of the electric field is perpendicular to the magnetic field that
produced it
• Similarly, the magnetic field induced by a
changing electric field is perpendicular to the
electric field that produced it
Properties of EM Waves
• An electromagnetic wave involves both an
electric field and a magnetic field
• These fields are perpendicular to each
other
• The propagation direction of the wave is
perpendicular to both the electric field and
the magnetic field
DEMO 7B‐20
EM Waves are Transverse Waves
• Imagine a snapshot of the electromagnetic wave • The electric field is along the x-axis
• The wave travels in the z-direction
– Determined by the right-hand rule #2
• The magnetic field is along the y-direction
• Because both fields are perpendicular to the direction of propagation, the wave is a transverse wave
Right handed coordinate system
QUIZ 1, OCTOBER 14, 2013 An electromagnetic wave is traveling in +y direction and the magnetic field at a particular point on the y‐axis points in the +z direction at a certain instant in time. At this same point and instant, what is the direction of the electric field? Z B Y a) ‐z b) ‐x c) ‐y d) +x e) None of the above X
Light is an EM Wave
• Maxwell found the speed of an em wave can be expressed in terms of two universal constants
– Permittivity of free space, εo (electrostatic value) – Magnetic permeability of free space, μo
– (magnetostatic value) –
• The speed of an em wave is denoted by c
• Inserting the values, c = 3.00 x 108 m/s
– The value of the speed of an electromagnetic wave is
o o
c
Light as an EM Wave, cont.
• Maxwell answered the question of the
nature of light – it is an electromagnetic
wave
• He also showed that the equations of
electricity and magnetism provide the
theory of light
EM Waves in a Vacuum
• Remember that mechanical waves need a medium to travel through
• Many physicists searched for a medium for em waves to travel through (The ether)
• EM waves can travel through many materials, but they can also travel through a vacuum
• All em waves travel with speed c through a vacuum
• The frequency f and wavelength λ are
EM Waves in Material Substances
• When an em wave travels through a
material substance, its speed depends on
the properties of the substance
• The speed of the wave is always less than
• The speed of the wave depends on the
wave’s frequency
Section 23.2 o o c 1EM Waves Carry Energy
• An em wave carriesenergy in the electric and magnetic fields associated with the wave
• Assume a wave interacts with a charged particle • The particle will
EM Waves Carry Energy, cont.
• As the electric field oscillates, so will the force • The electric force will do work on the charge • The charge’s kinetic energy will increase
• Energy is transferred from the wave to the particle
• The wave has energy
• The total energy per unit volume is the sum of its electric and magnetic energies
• utotal = uelec + umag
Section 23.3 elec o mag o u E and u B 1 2 1 2 2 2
EM Waves Carry Energy, final
• As the wave propagates, the energies per unit volume oscillate (energy densities)
• The electric and magnetic energies are equal and this leads to the proportionality between the peak electric and magnetic fields
o o o o o o E B E c B 2 2 1 1 2 2
Energy Propagation in Electromagnetic Waves Energy transmitted through unit time per unit area 0 0 1 Erms Brms EB P u c A • Intensity I = Average energy flux density (W/m2) Define Poynting vector 0 1 S E B Direction is that of wave propagation average magnitude is the intensity 2 0 2 2 0 0 0 1 1 2 2 2 m m m m S I c E B E B c E c
Intensity of an EM Wave
• The strength of an em wave is usually measured in terms of its intensity
– SI unit is W/m2
• Intensity is the amount of energy transported per unit time across a surface of unit area
• Intensity also equals the energy density multiplied by the speed of the wave
• I = utotal × c = (½ εo c Eo2 + ½ μ
o B2)
the intensity is proportional to the square of the electric and magnetic field amplitudes
TRANSVERSE ELECTROMAGNET WAVE
TEM wave
in y‐z plane In x‐z plane X Y ZSolar Cells
• The intensity of sunlight on a typical sunny day is about 1000 W/m²
• A solar cell converts the energy from sunlight into electrical energy
• Current photovoltaic cells convert only about 15% of the energy that strikes them
• Also must account for nights and cloudy days • Making better and more practical solar cells
EM Waves Carry Momentum
• An electromagnetic wcarries momentum
• Consider the collision
• between w and electron q • The momentum is carried
by the wave before the collision and by the
electron in the wall after the collision
EM Waves Carry Momentum, cont.
• The absorption of the wave occurs through the electric and magnetic forces on charges in the object
• When the charge absorbs an electromagnetic wave, there is a force on the charge in the
direction of propagation of the original wave
• The force on the charge is related to the charge’s
change in momentum: FB = ∆p / ∆t
• According to conservation of momentum, the final momentum on the charge must equal the initial momentum of the electromagnetic wave
Radiation Pressure
• When an electromagnetic wave is absorbed by an object, it exerts a force on the object
• The total force on the object is proportional to its exposed area
• Radiation pressure is the force of the electromagnetic force divided by the area
• This can also be expressed in terms of the intensity
radiation F I P A c Section 23.3
Electromagnetic Spectrum
• All em waves travel through a vacuum at the speed c
– c = 2.99792458 x 108 m/s ~ 3.00 x 108 m/s
– c is defined to have this value and the value of a meter is derived from this speed
• Electromagnetic waves are classified according to their frequency and wavelength
• The wave equation is true for em waves: c = ƒ λ
• The range of all possible electromagnetic waves is called the electromagnetic spectrum
Section 23.4