EM Waves ↔ Electrostatics (Chapters: Electric Charges, Gauss's Law)
- Gauss's law for electricity (∮E·dA = q_enc/ε_{0}) is Maxwell's first equation
- Same ε_{0} = /(N·) appears in both displacement current and capacitor formulas
- Capacitor charging → displacement current → this chapter
EM Waves ↔ Magnetism (Chapters: Magnetic Effects of Current)
- Ampere's law is modified by adding displacement current (this chapter)
- Original ∮B·dl = μ_{0}I_c → Modified ∮B·dl = μ_{0}(I_c + ε_{0}dΦ_E/dt)
- Same μ_{0} = 4π×10^{-7} H/m appears in both Biot-Savart and c = 1/√(μ_{0}ε_{0})
EM Waves ↔ Electromagnetic Induction
- Faraday's law (∮E·dl = –dΦ_B/dt) is Maxwell's third equation
- Mutual regeneration of E and B in EM wave is the same coupling as in EM induction
- Transformers and generators use the same Faraday law that Maxwell used in wave equations
EM Waves ↔ Optics (Chapters: Ray Optics, Wave Optics)
- Visible light is an EM wave (λ = 400–700 nm)
- Reflection, refraction, interference, diffraction — all applicable to EM waves
- Refractive index n = c/v arises because EM waves slow down in media (n > 1)
- Dispersion (different speeds in medium) = different refractive indices for different λ
EM Waves ↔ Modern Physics (Chapters: Atoms, Nuclei, Photoelectric Effect)
- Photoelectric effect: light has photon nature; E = hf (photon energy)
- X-rays produced in atoms (inner-shell electron transitions); gamma rays from nuclei
- Radiation from nuclear decay → gamma rays → this chapter
EM Waves ↔ Communication Systems
- Radio waves, microwaves used for communication
- EM spectrum knowledge directly applied in communication chapter
- Frequency allocation: AM radio (kHz), FM radio (MHz), TV (VHF/UHF), mobile (GHz)