Maxwell's equations, displacement current and sources of waves
A mobile tower sends EM waves — Maxwell's equations are behind it. Link to earlier classes : the light, sound and radio waves of classes 9-10 now extend to Maxwell's equations and communication formulas.
Displacement current is the current-like term from a changing electric field that also produces B.
In the figure : A capacitor and the four equations.
Rule 1: Maxwell's equations — Four : Gauss (electric), Gauss (magnetic), Faraday, Ampère-Maxwell. They give c = 1/√(μ₀ε₀).
- Easy : c = 1/√(4π×10⁻⁷ × 8.85×10⁻¹²) = 3.00 × 10⁸ m/s.
- Medium : Changing B ⇒ E (Faraday); changing E ⇒ B (Maxwell).
- Exam (CET) : c = ? (1) 1/√(μ₀ε₀) (2) √(μ₀ε₀) (3) μ₀/ε₀ (4) ε₀/μ₀ → answer 1)
Rule 2: Displacement current — I_d = ε₀ dΦ_E / dt; between capacitor plates I_d equals the conduction current I.
- Easy : I = 2 A in the wire ⇒ I_d = 2 A between the plates.
- Medium : dΦ_E/dt = 10¹¹ V m/s ⇒ I_d = 0.885 A.
- Exam (CET) : Between plates the current is? (1) displacement (2) conduction (3) neither (4) ohmic → answer 1)
Rule 3: Sources of waves — An accelerated charge produces EM waves; a static or uniformly moving one does not. An oscillating charge radiates the same f.
- Easy : Charge oscillating at 1 MHz ⇒ wave of 1 MHz.
- Medium : Steady DC ⇒ no wave.
- Exam (CET) : EM waves come from? (1) accelerated charge (2) static charge (3) uniform motion (4) static magnet → answer 1)
Derivation : Maxwell's correction
- Step 1 : Ampère : ∮B·dl = μ₀ I; between plates I = 0 ⇒ contradiction.
- Step 2 : Between plates E grows : Φ_E = q/ε₀.
- Step 3 : dΦ_E/dt = (1/ε₀) dq/dt = I/ε₀ ⇒ ε₀ dΦ_E/dt = I.
- Step 4 : ∮B·dl = μ₀(I + I_d).
I_d = ε₀ dΦ_E/dt; c = 1/√(μ₀ε₀).
Conduction current is 0 between plates; I_d = I.
Memory clue : "Acceleration = wave".
Spot the difference
| Law | Says |
|---|---|
| Gauss (E) | Charge ⇒ E |
| Gauss (B) | No monopole |
| Faraday | Changing B ⇒ E |
| Ampère-Maxwell | I and changing E ⇒ B |
Practice questions
- 1What is displacement current?
- 2What produces EM waves?
- 3Formula for c?
- 4I = 5 A : I_d between plates?
- 5dΦ_E/dt = 2 × 10¹¹ : I_d?
- 6Source 50 Hz : wave f?
- 7Why correct Ampère's law?
- 8Does steady current radiate?
Show answers (try them yourself first)
- 1A current-like term due to a changing E
- 2An accelerated charge
- 31/√(μ₀ε₀)
- 45 A
- 51.77 A
- 650 Hz
- 7I = 0 between plates
- 8No
Characteristics of electromagnetic waves
Sunlight crosses empty space — no medium needed.
An EM wave is a travelling oscillation of mutually perpendicular E and B.
In the figure : E (blue) and B (red) in phase.
Rule 1: Characteristics — Transverse; E ⊥ B ⊥ propagation; E and B in phase; no medium needed; speed in vacuum c = 3 × 10⁸ m/s.
- Easy : f = 100 MHz ⇒ λ = c/f = 3 m.
- Medium : λ = 600 nm ⇒ f = 5 × 10¹⁴ Hz.
- Exam (CET) : EM wave is? (1) transverse (2) longitudinal (3) mechanical (4) needs a medium → answer 1)
Rule 2: Relation of E and B — E₀ = c B₀; instantaneous E/B = c.
- Easy : E₀ = 300 V/m ⇒ B₀ = 300 ÷ 3×10⁸ = 10⁻⁶ T.
- Medium : B₀ = 2 × 10⁻⁷ T ⇒ E₀ = 60 V/m.
- Exam (CET) : E/B = ? (1) c (2) 1/c (3) c² (4) 1 → answer 1)
Rule 3: Energy and intensity — Energy is shared equally by E and B; I = ½ ε₀ c E₀²; energy density u = ε₀E².
- Easy : E₀ = 300 V/m ⇒ I = ½ × 8.85×10⁻¹² × 3×10⁸ × 300² = 119 W/m².
- Medium : E₀ doubled ⇒ I four times.
- Exam (CET) : I ∝ ? (1) E₀² (2) E₀ (3) 1/E₀ (4) E₀³ → answer 1)
Derivation : E₀ = c B₀
- Step 1 : Faraday : the E loop equals −dΦ_B/dt.
- Step 2 : Wave E = E₀ sin(kx − ωt), B = B₀ sin(kx − ωt).
- Step 3 : k E₀ = ω B₀.
- Step 4 : E₀/B₀ = ω/k = c.
c = E₀/B₀ = fλ = 1/√(μ₀ε₀); I = ½ε₀cE₀².
E and B are in phase (not 90°); all three directions are perpendicular.
Memory clue : "E ⊥ B ⊥ c".
Spot the difference
| Property | EM wave | Sound |
|---|---|---|
| Type | Transverse | Longitudinal |
| Medium | Not needed | Needed |
| Speed in vacuum | 3 × 10⁸ | Cannot travel |
Practice questions
- 1Speed of EM waves in vacuum?
- 2Relation of E, B and c?
- 3Is a medium needed?
- 4f = 30 MHz : λ?
- 5E₀ = 150 V/m : B₀?
- 6λ = 3 cm : f?
- 7B₀ = 4 × 10⁻⁷ T : I?
- 8Ratio of E and B energies?
Show answers (try them yourself first)
- 13 × 10⁸ m/s
- 2E₀ = cB₀
- 3No
- 410 m
- 55 × 10⁻⁷ T
- 610¹⁰ Hz
- 719.1 W/m²
- 81 : 1
The electromagnetic spectrum and its ranges
The rainbow is a tiny part of the full spectrum.
The EM spectrum arranges all EM waves by λ or f.
In the figure : f increases left to right.
Rule 1: Order — From longer to shorter λ : radio, microwave, IR, visible, UV, X-rays, γ-rays.
- Easy : Visible : 400 nm (violet) to 700 nm (red).
- Medium : f = c/λ : 400 nm ⇒ 7.5 × 10¹⁴ Hz.
- Exam (CET) : Highest f? (1) γ (2) radio (3) IR (4) visible → answer 1)
Rule 2: Photon energy — E = h f = h c / λ; E (eV) = 1240 ÷ λ (nm); h = 6.63 × 10⁻³⁴ J s.
- Easy : λ = 620 nm ⇒ E = 2 eV.
- Medium : f = 10¹⁵ Hz ⇒ E = 6.63 × 10⁻¹⁹ J = 4.14 eV.
- Exam (CET) : E ∝ ? (1) f (2) λ (3) f² (4) 1/f → answer 1) Trick : shorter λ ⇒ more E.
Rule 3: Ranges (approx.) — Radio > 0.1 m; microwave 1 mm-0.1 m; IR 700 nm-1 mm; visible 400-700 nm; UV 1-400 nm; X 10⁻³-10 nm; γ < 10⁻² nm.
- Easy : λ = 0.5 mm ⇒ IR.
- Medium : λ = 0.1 nm ⇒ X-rays.
- Exam (CET) : λ = 500 nm? (1) visible (2) UV (3) IR (4) X → answer 1)
Derivation : E (eV) = 1240/λ
- Step 1 : E = hc/λ.
- Step 2 : hc = 6.63×10⁻³⁴ × 3×10⁸ = 1.99×10⁻²⁵ J m.
- Step 3 : In eV ÷ 1.6×10⁻¹⁹ ⇒ 1.24×10⁻⁶ eV m.
- Step 4 : E (eV) = 1240 ÷ λ (nm).
c = fλ; E = hf = 1240/λ (nm) eV.
All travel at the same speed in vacuum; only f and λ differ.
Memory clue : "Rad-Mic-IR-Vis-UV-X-Gam".
Spot the difference
| Band | λ | Photon energy |
|---|---|---|
| Radio | > 0.1 m | Very low |
| Visible | 400-700 nm | 1.8-3.1 eV |
| X-rays | ~ 0.1 nm | ~ 12 keV |
Practice questions
- 1Order of the spectrum?
- 2λ of visible light?
- 3Formula for E?
- 4λ = 400 nm : E (eV)?
- 5f = 3 × 10¹⁵ Hz : λ?
- 6λ = 3 m : f?
- 7λ = 0.2 nm : E (eV)?
- 8Why do γ-rays have more E?
Show answers (try them yourself first)
- 1Radio → γ
- 2400-700 nm
- 3hf
- 43.1 eV
- 5100 nm
- 610⁸ Hz
- 76200 eV
- 8Higher f ⇒ larger E = hf
Sources, properties and uses of the bands
The wave that heats food in an oven is a bit shorter than radio.
Each band has a source and use set by its f.
In the figure : Band and use.
Rule 1: Radio and microwaves — Radio : oscillating circuits, broadcasting. Microwave : klystron/magnetron; radar, ovens, satellites.
- Easy : FM radio ~ 100 MHz; λ = 3 m.
- Medium : Oven 2.45 GHz ⇒ λ = 12.2 cm.
- Exam (CET) : Radar uses? (1) microwaves (2) X (3) γ (4) UV → answer 1)
Rule 2: IR, visible, UV — IR : hot bodies, remotes, thermal imaging. Visible : seen by eye. UV : Sun; sterilising; absorbed by ozone.
- Easy : TV remote = IR.
- Medium : UV to purify water.
- Exam (CET) : The ozone layer absorbs? (1) UV (2) IR (3) radio (4) visible → answer 1)
Rule 3: X and γ rays — X : fast electrons hitting a target; bone imaging. γ : from nuclei; cancer therapy, sterilisation.
- Easy : Bone image = X-rays.
- Medium : From the nucleus = γ.
- Exam (CET) : From the nucleus? (1) γ (2) X (3) UV (4) IR → answer 1)
Derivation : Oven wavelength
- Step 1 : f = 2.45 × 10⁹ Hz.
- Step 2 : λ = c / f.
- Step 3 : = 3 × 10⁸ ÷ 2.45 × 10⁹.
- Step 4 : λ = 12.2 cm.
Radio/micro = messages; IR = heat; X = diagnosis; γ = therapy.
Do not mix X and γ : γ is from the nucleus.
Memory clue : "Rad-Mic-IR-Vis-UV-X-Gam".
Spot the difference
| Band | Source | Use |
|---|---|---|
| Radio | Oscillating circuit | Broadcast |
| Micro | Magnetron | Radar, oven |
| IR | Hot bodies | Remote |
| X | Electron impact | Diagnosis |
| γ | Nucleus | Therapy |
Practice questions
- 1Which wave is used in an oven?
- 2In a TV remote?
- 3Use of X-rays?
- 4f = 90 MHz : λ?
- 5Source of γ?
- 6One use of UV?
- 7Why is IR called heat waves?
- 8Why is ozone important?
Show answers (try them yourself first)
- 1Microwaves
- 2IR
- 3Bones / diagnosis
- 43.33 m
- 5Nucleus
- 6Sterilisation
- 7Hot bodies emit IR
- 8It absorbs UV
Propagation of electromagnetic waves
A radio catches distant stations, but TV fades far from the tower.
Propagation is how a wave reaches the receiver — decided by f.
In the figure : Three modes.
Rule 1: Three modes — Ground wave (< 2 MHz); sky wave (2-30 MHz, reflected by the ionosphere); space wave (> 30 MHz, line of sight).
- Easy : AM radio at 1 MHz ⇒ ground wave.
- Medium : Short wave 10 MHz ⇒ sky wave.
- Exam (CET) : TV at 100 MHz? (1) space (2) ground (3) sky (4) any → answer 1)
Rule 2: Line-of-sight range — d = √(2 R h); two antennas : d = √(2Rh_T) + √(2Rh_R); R = 6.4 × 10⁶ m.
- Easy : h = 100 m ⇒ d = √(2 × 6.4×10⁶ × 100) = 35.8 km.
- Medium : h_T = 100, h_R = 25 ⇒ d = 53.7 km.
- Exam (CET) : h four times ⇒ d? (1) double (2) four times (3) half (4) same → answer 1) Trick : d ∝ √h.
Rule 3: Ionosphere and maximum f — A wave is reflected only if f ≤ f_c = 9 √N_max (N = electrons/m³).
- Easy : N_max = 10¹² ⇒ f_c = 9 MHz.
- Medium : f = 20 MHz > f_c ⇒ passes through.
- Exam (CET) : f > f_c ⇒ ? (1) passes through (2) reflected (3) absorbed (4) scattered → answer 1)
Derivation : d = √(2Rh)
- Step 1 : Tower height h, Earth radius R; tangent length d.
- Step 2 : Pythagoras : (R + h)² = R² + d².
- Step 3 : R² + 2Rh + h² = R² + d² ⇒ d² = 2Rh + h².
- Step 4 : h ≪ R ⇒ d = √(2Rh).
d = √(2Rh); f_c = 9√N.
d ∝ √h, not h; add the two terms for two antennas.
Memory clue : "Low f = ground, medium = sky, high = straight".
Spot the difference
| Mode | f | Use |
|---|---|---|
| Ground | < 2 MHz | AM |
| Sky | 2-30 MHz | Short wave |
| Space | > 30 MHz | TV, FM, satellite |
Practice questions
- 1Three modes of propagation?
- 2Which mode for TV?
- 3Value of R?
- 4h = 64 m : d?
- 5N_max = 4 × 10¹¹ : f_c?
- 6h_T = h_R = 100 m : d?
- 7d = 16 km : h?
- 8Why use satellites for TV?
Show answers (try them yourself first)
- 1Ground, sky, space
- 2Space
- 36.4 × 10⁶ m
- 428.6 km
- 55.69 MHz
- 671.6 km
- 720.0 m
- 8It extends the line of sight
Elements and terms of a communication system
On a phone call your voice travels through wires or waves.
A communication system carries information from a source to a destination.
In the figure : Four main blocks and noise.
Rule 1: Elements — Source → transmitter → channel → receiver → destination; noise enters the channel.
- Easy : Phone : mic = transducer; air = channel.
- Medium : Wires, optical fibre, free space = channel.
- Exam (CET) : Noise enters in the? (1) channel (2) source (3) receiver only (4) none → answer 1)
Rule 2: Key terms — Transducer, signal, attenuation, amplification, range, bandwidth, repeater.
- Easy : Signal weakening in a wire = attenuation.
- Medium : A repeater boosts and resends.
- Exam (CET) : Signal getting weaker? (1) attenuation (2) amplification (3) modulation (4) noise → answer 1)
Rule 3: Bandwidth — Bandwidth = width of frequencies used. Sound 20 Hz-20 kHz; speech ~ 3 kHz; TV ~ 6 MHz.
- Easy : Speech 300 Hz-3.1 kHz ⇒ BW = 2.8 kHz.
- Medium : TV BW = 6 MHz ⇒ more information.
- Exam (CET) : BW = ? (1) f_high − f_low (2) f_high + f_low (3) f_high × f_low (4) f_high ÷ f_low → answer 1)
Derivation : Antenna length
- Step 1 : Effective radiation : l ≈ λ/4.
- Step 2 : λ = c/f.
- Step 3 : f = 1.5 MHz ⇒ λ = 200 m.
- Step 4 : l = λ/4 = 50 m (hence modulation).
Source → Tx → channel → Rx; noise in the channel.
Attenuation ≠ noise : one weakens, one adds.
Memory clue : "Src-Tx-Chan-Rx".
Spot the difference
| Element | Job |
|---|---|
| Transmitter | Prepares/modulates signal |
| Channel | Carries it |
| Receiver | Recovers the signal |
| Repeater | Boosts the signal |
Practice questions
- 1Elements of a communication system?
- 2What is noise?
- 3What is a transducer?
- 4f = 3 MHz : λ/4?
- 5300 Hz-3300 Hz : BW?
- 6How to reduce attenuation?
- 7Why is a direct antenna impractical?
- 8Analog versus digital?
Show answers (try them yourself first)
- 1Source, transmitter, channel, receiver
- 2Unwanted signal
- 3Converts one energy form to another
- 425 m
- 53000 Hz
- 6Repeaters / amplifiers
- 7Large λ ⇒ very long antenna
- 8Continuous versus 0/1
Modulation and demodulation
Many radio stations run together — each with its own carrier f.
Modulation varies a carrier's amplitude or f by the message; demodulation reverses it.
In the figure : The carrier amplitude follows the message.
Modulation and demodulation
In the app you can move this figure with your finger.
Open in the appRule 1: Why modulate — Low-f signals are hard to send directly (huge antenna, mixing). We ride them on a high-f carrier.
- Easy : Speech ~ 3 kHz; carrier 1 MHz.
- Medium : Many stations on different f.
- Exam (CET) : Why modulate? (1) smaller antenna, better propagation (2) lower f (3) less power (4) add noise → answer 1)
Rule 2: Amplitude modulation — The carrier amplitude follows the message. m = A_m / A_c (≤ 1); sidebands f_c ± f_m; BW = 2 f_m.
- Easy : f_c = 1 MHz, f_m = 5 kHz ⇒ 0.995 and 1.005 MHz; BW = 10 kHz.
- Medium : A_c = 10 V, A_m = 6 V ⇒ m = 0.6.
- Exam (CET) : m > 1 ⇒ ? (1) over-modulation (2) good (3) FM (4) same → answer 1)
Rule 3: Power, FM and demodulation — P_t = P_c (1 + m²/2). FM : f varies, amplitude constant — less noise. Demodulation = recovering the message (detector).
- Easy : P_c = 100 W, m = 0.5 ⇒ P_t = 112.5 W.
- Medium : m = 1 ⇒ P_t = 1.5 P_c.
- Exam (CET) : In FM what is constant? (1) amplitude (2) f (3) phase (4) nothing → answer 1)
Derivation : AM sidebands
- Step 1 : Carrier A_c sin ω_c t; message A_m sin ω_m t.
- Step 2 : c_m = (A_c + A_m sin ω_m t) sin ω_c t.
- Step 3 : sin A sin B ⇒ cos(ω_c − ω_m)t and cos(ω_c + ω_m)t.
- Step 4 : Three f : f_c, f_c ± f_m; BW = 2f_m.
m = A_m/A_c; BW = 2f_m; P_t = P_c(1 + m²/2).
m ≤ 1; BW = 2f_m, not f_m.
Memory clue : "Amplitude = AM, Frequency = FM".
Spot the difference
| Feature | AM | FM |
|---|---|---|
| Varies | Amplitude | Frequency |
| Noise | More | Less |
| BW | Small | Large |
Practice questions
- 1What is modulation?
- 2BW of AM?
- 3What is demodulation?
- 4A_c = 8, A_m = 4 : m?
- 5f_c = 800 kHz, f_m = 4 kHz : sidebands?
- 6P_c = 200 W, m = 0.6 : P_t?
- 7Prove BW = 2f_m.
- 8Why is FM less noisy?
Show answers (try them yourself first)
- 1Imposing the message on a carrier
- 22 f_m
- 3Recovering the message
- 40.5
- 5796 and 804 kHz
- 6236 W
- 7sin A sin B expansion
- 8Amplitude is constant; noise changes amplitude
Quick revision of the whole lesson
| Concept | Key formula / fact | Unit / dimensions |
|---|---|---|
| Displacement current | I_d = ε₀ dΦ_E/dt | A; A |
| Speed | c = 1/√(μ₀ε₀) = fλ | m/s; L T⁻¹ |
| E, B | E₀ = cB₀ | V/m; T |
| Intensity | I = ½ε₀cE₀² | W/m²; M T⁻³ |
| Photon | E = hf = 1240/λ eV | J; M L² T⁻² |
| Line of sight | d = √(2Rh) | m; L |
| f_c | 9 √N_max | Hz; T⁻¹ |
| AM | m = A_m/A_c; BW = 2f_m | —; Hz |
| Power | P_t = P_c(1 + m²/2) | W; M L² T⁻³ |
🎯 Most important points for the exam
- I_d = ε₀ dΦ_E/dt; accelerated charge radiates.
- c = E₀/B₀ = fλ; E ⊥ B ⊥ c, in phase.
- Radio → micro → IR → visible → UV → X → γ : f increases.
- E = hf = 1240/λ (nm) eV.
- Ground < 2 MHz, sky 2-30 MHz, space > 30 MHz; d = √(2Rh).
- Source → Tx → channel → Rx; noise in the channel.
- AM : m ≤ 1, BW = 2f_m, P_t = P_c(1 + m²/2).
Maxwell → c → spectrum → uses → propagation → communication → modulation.