1. Maxwell’s Equations and Electromagnetic Waves
Chapter 29
Maxwell’s Equations and Electromagnetic Waves

2. 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
James Clerk Maxwell
He calculated the speed of light – 3x108 m/s – and concluded that light and other electromagnetic waves consist of fluctuating electric and magnetic fields

3. 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
James Clerk Maxwell

4. 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
Applying Ampère’s law to a circuit with a changing current results in an ambiguity
The result depends on which surface is used to determine the encircled current.

5. Modifications to Ampère’s Law
Maxwell used this ambiguity, along with symmetry considerations, to conclude that a changing electric field, in addition to current, should be a source of magnetic field
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

6. Maxwell’s Equations
In his unified theory of electromagnetism, Maxwell showed that the fundamental laws are expressed in these four equations:

7. 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 eo

8. 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

9. 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

10. 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 mo times the net current through that path and eomo times the rate of change of electric flux through any surface bounded by that path

11. 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

12. 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

13. 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:

14. 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

15. 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

16. Poynting Vector Electromagnetic waves carry energy
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

17. 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

18. Chapter 29 Problem 29
What would be the average intensity of a laser beam so strong
that its electric field produced dielectric breakdown of air (which
requires Ep = 3 MV/m)?

19. Polarization of Light
An unpolarized wave: each atom produces a wave with its own orientation of E, so all directions of the electric field vector are equally possible and lie in a plane perpendicular to the direction of propagation
A wave is said to be linearly polarized if the resultant electric field vibrates in the same direction at all times at a particular point
Polarization can be obtained from an unpolarized beam by selective absorption, reflection, or scattering

20. Polarization by Selective Absorption
The most common technique for polarizing light
Uses a material that transmits waves whose electric field vectors in the plane are parallel to a certain direction and absorbs waves whose electric field vectors are perpendicular to that direction

21. Polarization by Selective Absorption
The intensity of the polarized beam transmitted through the second polarizing sheet (the analyzer) varies as S = So cos2 θ, where So is the intensity of the polarized wave incident on the analyzer
This is known as Malus’ Law and applies to any two polarizing materials whose transmission axes are at an angle of θ to each other
Étienne-Louis Malus
1775 – 1812

22. Chapter 29 Problem 40
A polarizer blocks 75% of a polarized light beam. What’s the angle between the beam’s polarization and the polarizer’s axis?

23. 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

24. 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)

25. 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

26. 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

27. 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

28. 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

29. 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

30. Answers to Even Numbered Problems
Chapter 29:
Problem 14
3.9 μA

31. Answers to Even Numbered Problems
Chapter 29:
Problem 22
3 m
6 cm
500 nm
3 Å

32. Answers to Even Numbered Problems
Chapter 29:
Problem 32
160 W/m2
350 V/m
1.2 μT

33. Answers to Even Numbered Problems
Chapter 29:
Problem 36
3.1 cm