EM Waves
🟢 Lite — Quick Review (1h–1d)
Rapid summary for last-minute revision before your NEET attempt.
Electromagnetic (EM) waves are transverse waves produced by accelerating charges, made of mutually perpendicular, in-phase electric (E) and magnetic (B) fields that travel in vacuum at c = 3 × 10⁸ m/s. The propagation direction is given by the Poynting vector S = (1/μ₀)(E × B).
- Speed in vacuum: c = 1/√(μ₀ε₀), where μ₀ = 4π × 10⁻⁷ T·m/A and ε₀ = 8.854 × 10⁻¹² C²/(N·m²).
- Amplitude relation: E₀ = cB₀, so B₀ is far smaller than E₀ in SI units.
- Spectrum order (↑λ, ↓ν): γ-rays → X-rays → UV → visible → IR → microwaves → radio.
NEET pointer: Expect one conceptual MCQ — usually spectrum ordering, wavelength range of visible light (400–750 nm), or the displacement current term.
🟡 Standard — Regular Study (2d–2mo)
Standard content for students with a few days to months.
Origin and Maxwell’s prediction
A stationary charge produces only a static E-field; a steady current produces only a static B-field. Only an accelerating charge generates a self-sustaining disturbance where a changing E-field produces a B-field and vice versa. Maxwell captured this reciprocity through the displacement current term (ε₀ dΦ_E/dt) added to Ampère’s law — without it, his equations would forbid wave solutions.
Structure of a plane EM wave
In a plane wave travelling along +x, the fields take the form: E = E₀ sin(kx − ωt) ŷ, B = B₀ sin(kx − ωt) ẑ.
The three vectors E, B and the propagation direction form a right-handed system, so the direction is E × B, not E · B. E and B oscillate in phase — they reach zero and maximum together.
Energy and intensity
The wave carries energy density u = ½ε₀E² + B²/(2μ₀). The average intensity (energy flux) is I = ½ ε₀ c E₀², and the momentum delivered on absorption is p = U/c.
The electromagnetic spectrum
| Region | Approx. λ | Typical source / use |
|---|---|---|
| γ-rays | < 10⁻¹² m | Radioactive nuclei |
| X-rays | 10⁻¹⁰–10⁻⁸ m | Medical imaging |
| UV | 10⁻⁸–4 × 10⁻⁷ m | Sun, sterilisation |
| Visible | 4 × 10⁻⁷–7.5 × 10⁻⁷ m | Optics, human vision |
| Infrared | 7.5 × 10⁻⁷–10⁻³ m | Thermal radiation |
| Microwaves | 10⁻³–10⁻¹ m | Radar, ovens |
| Radio | > 10⁻¹ m | Communication |
Exam trap: “A steady current radiates EM waves.” False — acceleration is essential. Also, microwaves sit between IR and radio, never near UV.
🔴 Extended — Deep Study (3mo+)
Comprehensive coverage for students on a longer study timeline.
Edge cases and subtleties
In a dielectric medium the wave slows to v = c/n, where n is the refractive index, while the frequency stays fixed — wavelength shrinks to λ/n. The in-phase E–B relation still holds, but the amplitude ratio becomes E₀ = vB₀, not cB₀. In a conductor the fields penetrate only to the skin depth δ = √(2/(ωμσ)), beyond which the wave is exponentially attenuated.
Connection to modern physics
Quantum-mechanically, an EM wave of frequency ν is a stream of photons with energy E = hν and momentum p = h/λ. This duality is why a single Young-style double-slit experiment cannot decide whether light is a wave or a particle — both frameworks coexist. The Compton shift Δλ = (h/mc)(1 − cos θ) for scattered X-rays is direct evidence of photon momentum.
Common mistakes
- Writing E · B for the propagation direction — propagation is E × B.
- Saying radio waves have higher frequency than X-rays — the order is reversed.
- Believing Maxwell’s equations are only for static fields — the displacement current is what makes the wave equation ∂²E/∂x² = μ₀ε₀ ∂²E/∂t² fall out.
- Confusing phase velocity with signal velocity in a dispersive medium.
Worked micro-example
A radio antenna broadcasts at 100 MHz. The wavelength is λ = c/ν = (3 × 10⁸)/(10⁸) = 3 m, placing it firmly in the VHF band. If the radiated E-field amplitude is 0.1 V/m, then B₀ = E₀/c = (0.1)/(3 × 10⁸) ≈ 3.33 × 10⁻¹⁰ T.
Practice prompts
- Show, starting from Faraday’s and Ampère–Maxwell laws, that E(x, t) = E₀ sin(kx − ωt) satisfies a wave equation with speed 1/√(μ₀ε₀).
- Arrange the following in order of decreasing photon energy: microwaves, green light, X-rays, UV. Justify using E = hν.
NEET strategy: This chapter rarely crosses one question, so spend ~30 minutes mastering spectrum ordering, the c = 1/√(μ₀ε₀) relation, and the displacement current idea. Skip lengthy derivations — focus on the five boxed formulas and the spectrum table.
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Sources & verification
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- Reviewed by Pushkar Saini · last updated
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