Exercise Solutions Available
Step-by-step answers for all textbook questions in this chapter
Board Exam Weight: Electromagnetic Induction and Alternating Current carries 8–12 marks in Tamil Nadu Class 12 Physics board exams (Volume 2). NEET typically has 2–4 questions from this chapter.
1. Magnetic Flux
Magnetic flux Φ through a surface of area A when field B makes angle θ with the normal to the surface:
- Maximum when B ⊥ surface (θ = 0°): Φ = BA
- Zero when B ∥ surface (θ = 90°): Φ = 0
2. Faraday's Laws of Electromagnetic Induction
First Law
Whenever the magnetic flux through a circuit changes, an EMF is induced in the circuit.
Second Law
The magnitude of the induced EMF is equal to the rate of change of magnetic flux:
For a coil with N turns, each experiencing the same flux change:
3. Lenz's Law
The direction of the induced EMF (and induced current) is always such that it opposes the cause producing it.
Mathematically, Lenz's law gives the negative sign in Faraday's law:
Physical basis: Lenz's law is a direct consequence of the law of conservation of energy. If the induced current helped the change, it would create energy from nothing.
Example: A north pole approaching a coil → increasing flux → induced current creates a north pole facing the magnet (repelling it). Work must be done to push the magnet against this repulsion — this work appears as electrical energy in the circuit.
4. Self-Inductance
Self-inductance L is the constant of proportionality relating the flux linkage to current:
The induced back-EMF due to changing current:
SI unit: Henry (H). 1 H = 1 V·s/A = 1 Wb/A.
Self-inductance of a solenoid:
where n = N/l = turns per unit length, A = cross-sectional area, l = length.
Energy Stored in an Inductor
An inductor stores energy in its magnetic field (analogous to a capacitor storing energy in its electric field).
5. Mutual Inductance
When two coils are placed close to each other, changing current in coil 1 (primary) induces EMF in coil 2 (secondary):
Induced EMF in secondary:
SI unit: Henry (H). Mutual inductance depends on geometry (number of turns, area, separation) and medium between the coils.
6. AC Generator
Principle: Electromagnetic induction — a coil rotating in a magnetic field generates alternating EMF.
Construction: Rectangular coil (N turns, area A) rotated at angular velocity ω in a uniform field B. Slip rings and brushes collect the output.
EMF generated:
where ε₀ = NBAω is the peak (maximum) EMF.
The EMF varies sinusoidally — it is zero when coil is perpendicular to B and maximum when coil is parallel to B.
RMS (Root Mean Square) Values
For a sinusoidal AC:
RMS values are equivalent to DC values for power calculations.
7. Transformer
Principle: Mutual induction. An AC voltage in the primary coil (Np turns) induces an AC voltage in the secondary coil (Ns turns) through a shared iron core.
Transformer Equation (Ideal)
For an ideal transformer (no losses), power is conserved: VpIp = VsIs, so:
Step-up transformer: Ns > Np → Vs > Vp, but Is < Ip
Step-down transformer: Ns < Np → Vs < Vp, but Is > Ip
Efficiency
For ideal transformer: η = 100%.
Energy Losses in Real Transformers
| Loss | Cause | Remedy |
|---|---|---|
| Copper loss (I²R) | Resistance of coil windings | Use thick copper wire |
| Iron/core loss (eddy currents) | Induced currents in core | Laminated core |
| Hysteresis loss | Repeated magnetisation/demagnetisation | Soft iron core |
| Flux leakage | Not all flux links both coils | Better core design |
8. Worked Numericals
Numerical 1 — Induced EMF (Faraday's Law)
Problem: A coil of 100 turns and area 0.01 m² is placed in a magnetic field perpendicular to the coil. The field increases uniformly from 0 to 2 T in 0.1 s. Find the induced EMF.
The induced EMF is 20 V.
Numerical 2 — Transformer
Problem: A transformer has primary winding of 1000 turns connected to 220 V AC. The secondary has 200 turns. Find (a) secondary voltage and (b) ratio of secondary to primary current.
This is a step-down transformer (output voltage 44 V < input 220 V).
Numerical 3 — Self-Inductance Back EMF
Problem: A coil has self-inductance L = 2 H. The current through it changes uniformly from 0 to 4 A in 2 s. Find the induced back-EMF.
The induced back-EMF is 4 V, opposing the increase in current (Lenz's law).
Numerical 4 — Energy Stored in Inductor
Problem: A coil of self-inductance 4 H carries a current of 3 A. Find the energy stored in the inductor.
The energy stored in the magnetic field of the inductor is 18 J.
9. Board Exam Model Questions
2-Mark Questions
Q1. State Lenz's law and mention its physical basis. Lenz's law: The induced current opposes the change in flux causing it (ε = −dΦ/dt). Physical basis: It is a consequence of the law of conservation of energy. If induced current aided the change, energy would be created without doing work.
5-Mark Questions
By Faraday's law:
where ε₀ = NBAω is the peak EMF.
The EMF is sinusoidal — zero when coil is perpendicular to field (Φ is maximum, rate of change = 0) and maximum when coil is parallel to field (Φ = 0, rate of change is maximum).
Energy losses: (1) Copper loss: I²R heat in windings — reduced by using low-resistance thick conductors. (2) Eddy current loss: currents in core — reduced by laminated core. (3) Hysteresis loss: energy to reverse magnetisation — reduced by soft iron. (4) Flux leakage — reduced by better core geometry.
10. NEET Relevance
| Topic | NEET Frequency |
|---|---|
| Faraday's law — induced EMF calculation | Very High |
| Lenz's law — direction of induced current | High |
| Self-inductance — back EMF, energy | High |
| AC generator — peak and rms EMF | Medium |
| Transformer — turns ratio, power | High |
| Eddy currents | Medium |
NEET Tip: Lenz's law direction questions are common. Practice identifying: what change is happening (flux increasing or decreasing?) → what does the induced current do to oppose it? → use right-hand rule to find current direction.
11. Key Formulae Summary
| Quantity | Formula |
|---|---|
| Magnetic flux | Φ = BA cosθ |
| Induced EMF | ε = −N dΦ/dt |
| Self-inductance | ε = −L dI/dt |
| Solenoid inductance | L = μ₀N²A/l |
| Energy in inductor | U = ½LI² |
| AC generator EMF | ε = ε₀ sinωt, ε₀ = NBAω |
| RMS values | V_rms = V₀/√2 |
| Transformer voltage ratio | Vs/Vp = Ns/Np |
| Transformer current ratio | Is/Ip = Np/Ns |
Constants: μ₀ = 4π×10⁻⁷ T·m/A
