01
CONCEPT
Nature of EM Waves & Their Direction
In one line
A changing electric field makes a changing magnetic field, and a changing magnetic field makes a changing electric field. Together they travel as a transverse wave.
A changing electric field makes a changing magnetic field, and a changing magnetic field makes a changing electric field. Together they travel as a transverse wave.
NATURE
32.1.1 What is an EM wave?
- E and B oscillate with time and keep creating each other.
- They need no material medium; they travel through vacuum at speed c.
- They are transverse; polarization proves this.
- They carry energy and momentum.
- They carry no charge, so E and B fields do not deflect them.
- The electric vector causes the optical effects, so it is called the light vector.
E and B oscillate in phase, at right angles to each other and to c
PHASE
32.1.2 E and B together
- E and B are always in phase: both reach maximum and zero together.
- E ⊥ B, and both are ⊥ to the direction of travel.
DIRECTION
32.1.3 Direction of propagation
E, B and c form a right-handed set
| E along | B along | Wave travels along |
|---|---|---|
| +x | +y | +z |
| +y | +z | +x |
| +z | +x | +y |
- Use î × ĵ = k̂, ĵ × k̂ = î, k̂ × î = ĵ.
- Reversing the order gives a minus sign.
- Unit vector along travel: k̂ = Ê × B̂.
FINDING B
32.1.4 B from k and E
- k is the propagation vector, along the direction of travel.
- A wave along y can have only x and z components of E and B.
- For valid E and B directions: E · B = 0, and E × B is along the travel.
02
CONCEPT
Wave Equation, E0 = cB0 & Force on a Charge
In one line
The two fields follow the same sine wave. The ratio of their amplitudes is always the wave speed: E0 = cB0.
The two fields follow the same sine wave. The ratio of their amplitudes is always the wave speed: E0 = cB0.
WAVE EQUATION
32.2.1 Wave along +x
- E0, B0: amplitudes of the fields.
- Other forms: sin(ωt − kx), or sin ω(t − xc).
READING IT
32.2.2 What the equation tells you
| In the phase | Meaning |
|---|---|
| kx − ωt | travels along +x |
| kx + ωt | travels along −x |
| number with x | k, and λ = 2πk |
| number with t | ω, and f = ω2π |
| number in front | amplitude |
AMPLITUDES
32.2.3 E0 = cB0
- True at every point and every instant, not only at the peaks.
- So BE = 1c.
- The frequency is not needed to find one field from the other.
WRITING THE OTHER FIELD
32.2.4 B from E, or E from B
- Step 1: amplitude from E0 = cB0.
- Step 2: keep the same phase: same sin or cos, same bracket.
- Step 3: direction from E × B = direction of travel.
FORCE ON A CHARGE
32.2.5 Lorentz force
- Electric force: FE = qE.
- Magnetic force, v ⊥ B: FB = qvB.
- Since E = cB:
03
CONCEPT
Displacement Current, Maxwell’s Equations & Production
In one line
Maxwell found that a changing electric field also makes a magnetic field. He called this term the displacement current.
Maxwell found that a changing electric field also makes a magnetic field. He called this term the displacement current.
AMPERE’S LAW
32.3.1 Where it fails
- Holds only for steady current.
- Take a capacitor being charged by a battery.
Loop l₁ is around the wire; loop l₂ is between the plates
- Loop l₁: ∮B · dl = μ0i.
- Loop l₂: no current passes, so the law gives 0.
- But a magnetic field is found between the plates. So the law fails.
DISPLACEMENT CURRENT
32.3.2 Ampere-Maxwell law
- ic: conduction current, from flow of charges.
- id: from the changing electric field. It has the dimension of current.
- Between the plates, id = current in the connecting wires.
CAPACITOR RESULTS
32.3.3 Working forms
- E is uniform, so a part of area A0 carries id × A0A.
- Leaky capacitor: conduction and displacement currents cancel, so B = 0 between the plates.
CONDUCTING MEDIUM
32.3.4 Comparing the two currents
MAXWELL’S EQUATIONS
32.3.5 The four laws
| Law | Equation |
|---|---|
| Gauss (electrostatics) | ∮E · ds = qε0 |
| Gauss (magnetism) | ∮B · ds = 0 |
| Faraday (EMI) | ∮E · dl = −dφBdt |
| Ampere-Maxwell | ∮B · dl = μ0(ic + ε0dφEdt) |
- For static fields ∮E · dl = 0; Faraday’s form is needed when B changes.
PRODUCTION
32.3.6 What makes an EM wave?
- Stationary charge: only an E field.
- Uniform velocity: steady E and B, no wave.
- Accelerated charge: radiates an EM wave.
- A charge oscillating harmonically gives a wave of the same frequency.
- An LC oscillator gives waves of a chosen frequency:
LC oscillator feeding an antenna
HISTORY
32.3.7 Who did what
| Name | Work |
|---|---|
| Maxwell | first predicted EM waves |
| Hertz | produced and detected them, λ about 6 m |
| J. C. Bose | produced λ from 5 mm to 25 mm |
| Marconi | transmitted them over a few km |
JEE · NEET
Corner
Hertz’s experiment
Hertz’s set-up
- Plates P₁ and P₂ act as a capacitor.
- Wires joining spheres S₁, S₂ to the plates give a low inductance.
- High voltage makes a spark across the gap; the spark sets up oscillations.
- The oscillations send out EM waves, picked up by the receiver ring.
04
CONCEPT
Speed of EM Waves in a Medium
In one line
In vacuum every EM wave travels at c. In a medium it slows down by the factor n = √(μrεr).
In vacuum every EM wave travels at c. In a medium it slows down by the factor n = √(μrεr).
VACUUM
32.4.1 Speed in free space
- Same in all directions.
- Does not depend on the motion of the source.
- Same for all wavelengths in vacuum.
MEDIUM
32.4.2 Speed in a medium
- μ = μrμ0, ε = εrε0.
- Dielectric constant k is the same as εr.
- Speed in a medium depends on wavelength (dispersion), not on intensity.
REFRACTIVE INDEX
32.4.3 Link with n
- Non-magnetic medium, μr = 1:
FROM THE EQUATION
32.4.4 Reading v from a wave
- Find v from the two numbers in the phase.
- Then n = cv, and εr = n² (non-magnetic).
- Time for an echo: t = 2dv.
ENTERING A MEDIUM
32.4.5 What changes
| Quantity | In the medium |
|---|---|
| frequency | unchanged |
| speed | v = cn |
| wavelength | λm = λn |
| wave number | km = nk |
JEE · NEET
Corner
Wave impedance
- Hindrance a medium offers to the wave.
- H is the magnetic intensity: H = Bμ.
05
CONCEPT
Energy Density
In one line
The energy of an EM wave is shared equally by its electric and magnetic fields.
The energy of an EM wave is shared equally by its electric and magnetic fields.
AT ANY INSTANT
32.5.1 Energy per unit volume
- Using E = cB, these two are always equal.
- Same result in a medium, with ε and μ.
AVERAGE VALUES
32.5.2 Over one cycle
| Quantity | Value |
|---|---|
| average electric | 14ε0E0² |
| average magnetic | B0²4μ0 |
| total average | 12ε0E0² = B0²2μ0 |
- The average of sin²ωt is one half.
- Ratio of average electric to average magnetic = 1.
- Ratio of average electric to total average = 12.
ENERGY IN A VOLUME
32.5.3 Total energy
- Same energy in a smaller volume needs a larger E0: E0² ∝ 1V.
- Half the diameter of a cylinder: V becomes one fourth, so E0 doubles.
HOW IT VARIES
32.5.4 Oscillation of energy
- u ∝ E² ∝ sin²ωt.
- So the energy in a small volume oscillates at twice the frequency of the wave.
06
CONCEPT
Intensity
In one line
Intensity is the energy crossing unit area per unit time, on a surface perpendicular to the direction of travel.
Intensity is the energy crossing unit area per unit time, on a surface perpendicular to the direction of travel.
DEFINITION
32.6.1 Energy flow
All the energy in a column of length cΔt crosses area A in time Δt
- Unit: W/m². Also called energy flux.
- E and B contribute equally: ratio 1 : 1.
FROM AMPLITUDES
32.6.2 Working formula
- ε0c = 2.655 × 10−3 in SI: a handy number.
- √2Iε0c has the unit of electric field, N/C.
- In terms of rms: I = ε0Erms²c.
LASER BEAM
32.6.3 Power and area
IN A MEDIUM
32.6.4 Refractive index n
- With a fraction reflected: Itransmitted = (1 − r)I.
POINT SOURCE
32.6.5 Bulb, lamp, LED
Power spreads over a sphere
- Prad = efficiency × rated power.
- I ∝ 1r², and E0 ∝ 1r.
- All points at the same r have the same I, whatever the angle.
- Intensity due to the electric field alone = I2.
JEE · NEET
Corner
Poynting vector
- Rate of energy flow per unit area; unit W/m².
- Points along the direction of travel.
- Its direction does not oscillate; its size swings between 0 and Smax.
- Sav is the intensity I.
07
CONCEPT
Momentum & Radiation Pressure
In one line
EM waves have no rest mass, yet they carry momentum, so they push on any surface they strike.
EM waves have no rest mass, yet they carry momentum, so they push on any surface they strike.
MOMENTUM
32.7.1 Carried by the wave
Momentum given: absorbing Uc, reflecting 2Uc
| Surface | Momentum delivered |
|---|---|
| fully absorbing | Uc |
| fully reflecting | 2Uc |
| fraction r reflected | (1 + r)Uc |
FORCE
32.7.2 On a surface of area A
- Energy per second on the surface = IA.
- Force = momentum delivered per second.
| Surface | Force F |
|---|---|
| absorbing | IAc |
| reflecting | 2IAc |
| fraction r reflected | (1 + r)IAc |
- The time of exposure does not change the force or the pressure.
- It only changes the total momentum: p = F × t.
RADIATION PRESSURE
32.7.3 Force per unit area
- Check the units: change W/cm² to W/m² when A is in m².
- I can be found first from the amplitude of E.
IN A MEDIUM
32.7.4 Wave speed v
JEE · NEET
Corner
Force on a reflecting hemisphere
- Point source of power P at the centre, inner surface fully reflecting.
- Sideways parts of the force cancel; only the axial part adds up over projected area πR².
08
CONCEPT
Electromagnetic Spectrum: Order & Ranges
In one line
The whole ordered range of frequencies and wavelengths of EM waves is the EM spectrum.
The whole ordered range of frequencies and wavelengths of EM waves is the EM spectrum.
ORDER
32.8.1 Shortest to longest wavelength
The EM spectrum
- Wavelength rises left to right; frequency and photon energy fall.
- All of them travel at the same speed c in vacuum.
RANGES
32.8.2 Wavelength of each part
| Wave | Wavelength |
|---|---|
| Radio | above 0.1 m |
| Microwave | 0.1 m to 1 mm |
| Infrared | 1 mm to 700 nm |
| Visible | 700 nm to 400 nm |
| Ultraviolet | 400 nm to 1 nm |
| X-rays | 1 nm to 10−3 nm |
| Gamma rays | below 10−3 nm |
VISIBLE LIGHT
32.8.3 VIBGYOR
- Violet has the shortest wavelength (about 400 nm).
- Red has the longest wavelength (about 700 nm).
- Blue photon has more energy than yellow.
PHOTON ENERGY
32.8.4 Finding the region
- A photon of about 10 keV gives λ near 0.1 nm: X-ray region.
NOT EM WAVES
32.8.5 Watch out
- α-rays and β-rays are charged particles.
- Cathode rays are electrons.
- Sound is a mechanical wave.
- Heat rays are infrared, so they are EM waves.
09
CONCEPT
Production, Uses & the Atmosphere
In one line
Each part of the spectrum has its own source and its own uses. The atmosphere decides which of them reach us.
Each part of the spectrum has its own source and its own uses. The atmosphere decides which of them reach us.
PRODUCTION
32.9.1 Source of each wave
| Wave | Produced by |
|---|---|
| Radio | rapid acceleration of electrons in aerials |
| Microwave | klystron valve, magnetron |
| Infrared | vibration of atoms and molecules |
| Visible | outer electrons changing levels |
| Ultraviolet | inner electrons, arc lamps |
| X-rays | inner shell electrons, X-ray tube |
| Gamma rays | radioactive decay of the nucleus |
USES
32.9.2 What each wave does
| Wave | Uses |
|---|---|
| Radio | AM and FM, TV, communication |
| Microwave | radar, aircraft navigation, oven |
| Infrared | physiotherapy, muscular strain, night and fog photography, remote control |
| Visible | to see objects |
| Ultraviolet | sterilizing, water purification, food preservation, Lasik surgery, finger prints |
| X-rays | medical diagnosis, crystal structure |
| Gamma rays | nuclear structure, cancer treatment |
WORTH REMEMBERING
32.9.3 Common questions
- Microwave oven: its frequency matches the resonant frequency of water molecules.
- Human body radiates all the time, in the infrared.
- X-rays study crystals: their λ is close to the atomic spacing.
- To observe a particle, choose λ of the order of its size.
- Radio waves diffract more than microwaves: longer λ.
- Object much smaller than λ: the wave is scattered.
- Optical waves have shorter λ than microwaves.
GREENHOUSE EFFECT
32.9.4 Warming of the earth
Infrared from the earth is sent back
- Infrared from the earth is reflected back by low clouds and CO₂.
- So the cause is infrared rays.
OZONE LAYER
32.9.5 The UV shield
- Absorbs most of the sun’s ultraviolet rays.
- Blocks wavelengths below about 3 × 10−7 m.
- This protects living cells.
RADIO PROPAGATION
32.9.6 How signals travel
Ground wave and sky wave
- Ground wave: follows the surface of the earth.
- Sky wave: reflected back by the ionosphere.
- AM band: frequency up to 30 MHz. Amplitude of the carrier follows the signal.
- FM band: 80 MHz to 200 MHz. Frequency of the carrier follows the signal.
JEE · NEET
Corner
Layers of the atmosphere
Layers above the earth
- 78% N₂, 21% O₂, traces of other gases.
- Troposphere: temperature falls from 290 K to 220 K with height.
- Stratosphere: temperature 220 K to 200 K.
- Mesosphere: temperature falls to 180 K.
- Ionosphere: ions, electrons and neutral molecules.
- Kennelly-Heaviside layer: about 110 km up, very high electron density.
Radio bands
| Band | Frequency |
|---|---|
| VLF | 10 kHz to 30 kHz |
| LF | 30 kHz to 300 kHz |
| MF (MW) | 300 kHz to 3000 kHz |
| HF (SW) | 3 MHz to 30 MHz |
| VHF | 30 MHz to 300 MHz |
| UHF | 300 MHz to 3000 MHz |
| SHF (micro) | 3000 MHz to 300000 MHz |
TV signals and antenna height
Range of a tall antenna
- TV signals are frequency modulated.
- h = antenna height, R = radius of the earth.
- Population covered = area × population density.
EXAM-DAY CARD
Just see this before the exam
E0B0 = c
wave
id = ε0dφEdt
displacement current
n = √μrεr
medium
I = 12ε0E0²c
intensity
P = Ic or 2Ic
radiation pressure
γ X UV V IR M R
spectrum
FORMULA SHEET
Whole chapter on one page
Wave
travel along E × B
Ey = E0 sin(kx − ωt)
k = 2πλ, c = ωk = fλ
E0 = cB0
Maxwell
id = ε0dφEdt = CdVdt
∮B·dl = μ0(ic + id)
Jc to Jd = σ to ωε
ν = 12π√(LC)
Medium
c = 1√μ0ε0
v = c√μrεr
n = cv = √μrεr
f same, λm = λn
Energy
uE = 12ε0E², uB = B²2μ0
uE = uB
uav = 12ε0E0²
U = uavV
Intensity
I = uavc = 12ε0E0²c
I = cB0²2μ0
point source: I = P4πr²
laser: I = PA
Pressure
absorbing: p = Uc, P = Ic
reflecting: p = 2Uc, P = 2Ic
F = (1 + r)IAc
λ(nm) ≈ 1240E(eV)
TOP MISTAKES
Avoid these = easy marks
MISTAKE ✗
Direction of travel from B × E
Using c in a medium
Total uav = ¼ε0E0²
Reflecting surface: F = IAc
CORRECT ✓
Always use E × B
v = cn, and frequency stays the same
¼ is electric alone; total is ½ε0E0²
Reflecting: F = 2IAc