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Class 12 · Physics · Part 1

Chapter 8: Electromagnetic Waves

Revision notes, practice numericals, a question bank, assertion and reason questions and answers to the NCERT questions. Tap a group to open it; opening one closes the others.

8.1Displacement currentMaxwell's modification of Ampere's law

The problem

  • When a capacitor is being charged, a current I flows in the wires, but no charge crosses the gap between the plates. Ampere's law ∮B·dl = μ₀ I gives different answers depending on whether the surface used passes between the plates or not.
  • Maxwell's fix: a changing electric field also acts as a source of magnetic field. The displacement current is I_d = ε₀ dΦ_E / dt.
  • The Ampere–Maxwell law: ∮ B · dl = μ₀ (I_c + I_d) = μ₀ I_c + μ₀ε₀ dΦ_E/dt.
  • In a charging capacitor the displacement current in the gap equals the conduction current in the wires, so the current is continuous and Kirchhoff's junction rule holds at each plate when both are counted.
I (conduction)E changing: displacement current I_dI_d = ε₀ dΦ_E/dt = I
Displacement current: the changing electric field between the plates acts like a current and continues the circuit.

Field between circular plates

  • Between circular plates of radius R carrying a displacement current I_d, the field at distance r from the axis is B = μ₀ I_d r / 2π R² for r < R (it rises in proportion to r) and B = μ₀ I_d / 2π r for r > R.
8.2Maxwell's equationsThe four laws

Summary

  • Gauss's law (electricity): ∮E·dA = q/ε₀. Gauss's law (magnetism): ∮B·dA = 0.
  • Faraday's law: ∮E·dl = −dΦ_B/dt. Ampere–Maxwell law: as above.
  • A changing magnetic field produces an electric field and a changing electric field produces a magnetic field. Together they predict waves, travelling at c = 1/√(μ₀ε₀) = 3 × 10⁸ m s⁻¹, the speed of light. Hertz produced and detected such waves in 1887.
8.3Electromagnetic wavesProperties

Nature of the wave

  • Accelerated (oscillating) charges radiate EM waves, with the frequency of the oscillation.
  • The wave is transverse: E and B are perpendicular to each other and to the direction of travel (along E × B). They are in phase.
  • A wave along z: E = E₀ sin (kz − ωt) along x, B = B₀ sin (kz − ωt) along y. In vacuum E₀ / B₀ = c.
  • Here ω = 2π ν, k = 2π / λ, and c = ν λ = ω / k.
  • No medium is needed. In a medium of refractive index n: v = c / n = 1/√(με), the frequency stays the same and the wavelength becomes λ/n.
zE (in x–z plane)B (in y–z plane)E ⟂ B ⟂ direction of travel; E₀ = c B₀
An electromagnetic wave: E and B are in phase, perpendicular to each other and to the direction of travel.

Energy and momentum

  • The energy densities of the electric and magnetic parts are equal on average: u_E = ½ ε₀ E² , u_B = B² / 2μ₀. The average total is u = ½ ε₀ E₀².
  • The intensity is I = u c = ½ ε₀ c E₀².
  • A wave carrying energy U has momentum p = U / c. The radiation pressure is I / c on an absorber and 2I / c on a perfect reflector (normal incidence).
8.4The electromagnetic spectrumFrom gamma rays to radio waves

The bands

  • In order of increasing wavelength: gamma rays, X-rays, ultraviolet, visible (about 400–700 nm), infrared, microwaves, radio waves. All travel at c in vacuum. The photon energy E = h ν = h c / λ is greatest for gamma rays.
γ-rays<10⁻¹² mX-rays10⁻¹² to10⁻⁸ mUV10⁻⁸ to4×10⁻⁷ mVisible400 to700 nmInfrared7×10⁻⁷ to10⁻³ mMicrowave10⁻³ to0.3 mRadio>0.3 mshorter λ, higher ν, higher photon energylonger λ, lower ν
The electromagnetic spectrum: from gamma rays (shortest wavelength) to radio waves (longest).

Sources and uses

  • Radio waves (above about 0.1 m): oscillating circuits; broadcasting and communication; some are reflected by the ionosphere.
  • Microwaves (mm to cm): special tubes; radar, communication, microwave ovens (they match a frequency absorbed by water molecules).
  • Infrared: hot bodies and vibrating molecules; heating, remote controls, night vision, the greenhouse effect.
  • Visible light: atoms (electron transitions); vision.
  • Ultraviolet: the Sun, special lamps; sterilising water, LASIK; absorbed by the ozone layer.
  • X-rays: fast electrons hitting a metal target; medical diagnosis, security checks.
  • Gamma rays: radioactive nuclei; cancer treatment and sterilisation.
Quick referenceFormulas at a glanceRevise before the exam

Key results

  • I_d = ε₀ dΦ_E/dt; ∮B·dl = μ₀(I + I_d)
  • c = 1/√(μ₀ε₀); c = νλ; E₀ = cB₀
  • I = ½ε₀cE₀²; u_E = u_B; p = U/c; pressure I/c or 2I/c
  • E = hν = 1240 eV nm / λ

Common mistakes

  • Saying that EM waves need a medium or are longitudinal.
  • Using the unit nT as T (1 nT = 10⁻⁹ T).
  • Forgetting that the frequency, not the wavelength, stays the same when the wave changes medium.
  • Thinking displacement current is a flow of charge across the gap.