Electromagnetic Induction
NCERT Class 12 Physics Chapter 6
Electromagnetic Induction for Class 12 Physics, JEE and NEET: Faraday’s and Lenz’s laws, motional emf, eddy currents, inductance and the AC generator.
8 topics Updated 8 Nov 2026
For: Class 12, JEE and NEET, unless a topic says otherwise
In the syllabus: JEE Class 12 syllabus, NEET Class 12 syllabus
With your textbook
NCERT Physics Part I (Class 12), Chapter 6 “Electromagnetic Induction”, reprint 2026-27.
Open the official NCERT chapter (PDF, 2.4 MB, ncert.nic.in) (opens in a new tab)
Checked on 19 Oct 2026.
Learn in this order
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The experiments of Faraday and Henry
Magnet and coil, two coils, a key, and the flux change behind them.
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Magnetic flux
Definition, Φ = BA cos θ and the area vector, SI unit weber, dimensions, curved surfaces, with solved examples.
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Faraday’s law of induction
Statement, ε = −dΦ/dt and its minus sign, N-turn coils, average emf, with examples.
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Lenz’s law and conservation of energy
The induced current opposes the change in flux, magnet-and-coil cases, open circuits and conservation of energy.
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Motional electromotive force
Definition, ε = Blv derived from Faraday’s law and the Lorentz force, rods on rails, rotating rods and wheels.
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Eddy currents
Current loops induced in bulk metal, magnetic braking, damping, induction heating, and why transformer cores are laminated.
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Inductance
Coaxial solenoids, a solenoid’s self-inductance, back emf, energy stored ½LI and solved examples.
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AC generator
Working principle, a coil turning in a magnetic field, emf ε = NBAω sin ωt, its derivation and the peak emf.
Key formulas in this chapter
Experiments of Faraday and Henry
- flux through a plane area: ΦB = BA cos θ
- Faraday’s law: ε = −dΦB/dt
- N-turn coil: ε = −N dΦB/dt
Magnetic flux
- ΦB = B · A = BA cos θ
- general surface: ΦB = ∫ B · dA
- unit: 1 Wb = 1 T m
Faraday’s law of induction
- ε = −dΦB/dt
- N turns: ε = −N dΦB/dt
- signed average: εavg = −N ΔΦB/Δt
- resistive approximation: I = ε/R
Lenz’s law
- ε = −dΦB/dt (the sign is Lenz’s law)
- resistive loop, fixed field direction: flux magnitude rising → induced field against B
- resistive loop, fixed field direction: flux magnitude falling → induced field along B
Motional emf
- ε = Blv
- with resistance R: I = Blv/R, F = IlB
- rod of length l turning at ω about one end: ε = Bωl2/2
Eddy currents
- emf round a closed path: ε = −dΦB/dt
- resistive ring, uniform normal field: |ε| = πr2 |dB/dt|
- heating in a path of resistance R: P = ε2/R
Inductance
- mutual: N1Φ_1 = MI2, ε1 = −M dI2/dt
- coaxial solenoids: M = μ0 n1 n2 π r1^2 l
- self: NΦB = LI, ε = −L dI/dt
- solenoid: L = μr μ0 n2 A l
- linear inductor: W = LI2/2; vacuum: uB = B2/(2μ0)
AC generator
- ΦB = BA cos ωt
- ε = NBAω sin ωt
- ε0 = NBAω, ω = 2πν
More in Physics
- Units and Measurement
- Motion in a Straight Line
- Motion in a Plane
- Laws of Motion
- Work, Energy and Power
- Systems of Particles and Rotational Motion
- Gravitation
- Mechanical Properties of Solids
- Mechanical Properties of Fluids
- Thermal Properties of Matter
- Thermodynamics
- Kinetic Theory
- Oscillations
- Waves
- Electric Charges and Fields
- Electrostatic Potential and Capacitance
- Current Electricity
- Moving Charges and Magnetism
- Magnetism and Matter
- Alternating Current
- Electromagnetic Waves
- Ray Optics and Optical Instruments
- Wave Optics
- Dual Nature of Radiation and Matter
- Atoms
- Nuclei
- Semiconductor Electronics: Materials, Devices and Simple Circuits