Electromagnetic Induction
1. Magnetic Flux & Faraday's Laws
Magnetic Flux (ΦB): Number of magnetic field lines passing normally through a surface.
ΦB = B ⋅ A = BA cosθ
SI Unit: Weber (Wb) or Tesla-meter2 (Tm2).
SI Unit: Weber (Wb) or Tesla-meter2 (Tm2).
Faraday's Laws of Induction
First Law: Whenever magnetic flux linked with a coil changes, an induced EMF is produced.
Second Law: The magnitude of induced EMF is equal to the rate of change of magnetic flux.
Second Law: The magnitude of induced EMF is equal to the rate of change of magnetic flux.
ε = - N (dΦB / dt)
(Negative sign indicates direction - Lenz's Law)
2. Lenz's Law
The direction of induced EMF (or current) is such that it opposes the cause which produces it.
It is based on Conservation of Energy.
Mechanical work done in moving magnet against repulsive/attractive force is converted into Electrical Energy.
Mechanical work done in moving magnet against repulsive/attractive force is converted into Electrical Energy.
- N-pole approaching coil → Face becomes N-pole (Repulsion).
- N-pole receding from coil → Face becomes S-pole (Attraction).
(Asked in NEET 2019, 2022)
3. Motional Electromotive Force
EMF induced in a conductor moving in a magnetic field.
ε = Blv
(B, l, v are mutually perpendicular)
Rotational EMF
Rod of length l rotating with angular velocity ω:
ε = ½ B ω l2 = B A f
(Asked in NEET 2018, 2021)
4. Eddy Currents
Circulating currents induced in bulk pieces of conductors when magnetic flux changes.
Disadvantages: Heat production (Energy loss).
Minimization: Using Laminated cores.
Applications: Magnetic Braking in trains, Induction Furnace, Speedometer.
Minimization: Using Laminated cores.
Applications: Magnetic Braking in trains, Induction Furnace, Speedometer.
(Asked in NEET 2019)
5. Inductance
Self Induction
Production of induced EMF in a coil when current in itself changes.
Φ = LI → ε = -L (dI/dt)
Solenoid: L = μ0 n2 Al
Energy Stored: U = ½ L I2
Solenoid: L = μ0 n2 Al
Energy Stored: U = ½ L I2
Mutual Induction
EMF in secondary coil when current in primary coil changes.
Φs = MIp → εs = -M
(dIp/dt)
Co-axial Solenoids: M = μ0 n1 n2 Al
Coupling Coefficient: k = M / √(L1L2)
Co-axial Solenoids: M = μ0 n1 n2 Al
Coupling Coefficient: k = M / √(L1L2)
(Asked in NEET 2016, 2017, 2023)
6. AC Generator
Converts Mechanical Energy into Electrical Energy (Sine Wave).
Principle: Electromagnetic Induction.
Flux Φ = NBA cos(ωt)
EMF ε = -dΦ/dt = NBAω sin(ωt)
Max EMF ε0 = NBAω
Flux Φ = NBA cos(ωt)
EMF ε = -dΦ/dt = NBAω sin(ωt)
Max EMF ε0 = NBAω
Numericals: Electromagnetic Induction
Q1. A coil of 100 turns and area 0.1 m2 is placed perpendicular to a magnetic field of 0.2 T. The
field acts for 0.1 s and then vanishes. Calculate induced EMF.
Solution:
Initial Flux Φ1 = NBA = 100 × 0.2 × 0.1 = 2 Wb.
Final Flux Φ2 = 0.
Rate of change = (Φ2 - Φ1) / t = (0 - 2) / 0.1 = -20 Wb/s.
|ε| = 20 V.
Initial Flux Φ1 = NBA = 100 × 0.2 × 0.1 = 2 Wb.
Final Flux Φ2 = 0.
Rate of change = (Φ2 - Φ1) / t = (0 - 2) / 0.1 = -20 Wb/s.
|ε| = 20 V.
Q2. A jet plane with wing span 25 m is flying at 1800 km/h. Earth's vertical field is 5 ×
10-4 T. Find voltage between wing tips.
Solution:
v = 1800 × (5/18) = 500 m/s.
l = 25 m, B = 5 × 10-4 T.
ε = B l v
ε = (5 × 10-4) × 25 × 500
ε = 125 × 500 × 10-4
ε = 62500 × 10-4 = 6.25 V.
v = 1800 × (5/18) = 500 m/s.
l = 25 m, B = 5 × 10-4 T.
ε = B l v
ε = (5 × 10-4) × 25 × 500
ε = 125 × 500 × 10-4
ε = 62500 × 10-4 = 6.25 V.
Q3. An inductor of inductance 50 mH carries a current of 2 A. Calculate energy stored in it.
Solution:
U = ½ L I2
U = 0.5 × (50 × 10-3) × 22
U = 0.5 × 0.05 × 4
U = 0.1 Joules.
U = ½ L I2
U = 0.5 × (50 × 10-3) × 22
U = 0.5 × 0.05 × 4
U = 0.1 Joules.
Q4. Current in a coil falls from 5 A to 0 A in 0.1 s. If induced EMF is 200 V, find self impedance
(inductance) of the coil.
Solution:
ε = -L (dI/dt)
200 = -L (0 - 5) / 0.1
200 = L (50)
L = 200 / 50 = 4 H.
ε = -L (dI/dt)
200 = -L (0 - 5) / 0.1
200 = L (50)
L = 200 / 50 = 4 H.
Q5. A 1 m metal rod rotates with frequency 50 Hz with one end hinged at center and other at rim of a
circular ring in B-field 1 T. Find EMF.
Solution:
ε = B A f = B (πl2) f
ε = 1 × 3.14 × (1)2 × 50
ε = 3.14 × 50 = 157 V.
ε = B A f = B (πl2) f
ε = 1 × 3.14 × (1)2 × 50
ε = 3.14 × 50 = 157 V.
Q6. Two concentric circular coils have radii r and R (R >> r). Find mutual
inductance.
Solution:
Assume current I in outer coil R.
Magnetic field at center B = μ0I / 2R.
Flux through inner coil Φ = B × πr2.
Φ = (μ0I / 2R) πr2.
Since Φ = MI, M = μ0 π r2 / 2R.
Assume current I in outer coil R.
Magnetic field at center B = μ0I / 2R.
Flux through inner coil Φ = B × πr2.
Φ = (μ0I / 2R) πr2.
Since Φ = MI, M = μ0 π r2 / 2R.
Q7. A coil of resistance 10 Ω has flux change from 10 Wb to 2 Wb. Calculate charge flowing through it.
Solution:
Δq = ΔΦ / R
ΔΦ = 10 - 2 = 8 Wb.
Δq = 8 / 10 = 0.8 C.
Δq = ΔΦ / R
ΔΦ = 10 - 2 = 8 Wb.
Δq = 8 / 10 = 0.8 C.
Q8. A rectangular coil of 20 turns and area 200 cm2 rotates at 3000 rpm in B=0.5 T. Find max EMF.
Solution:
ε0 = NBAω
ω = 2πf = 2π(3000/60) = 100π rad/s.
A = 200 cm2 = 200 × 10-4 m2.
ε0 = 20 × 0.5 × (2×10-2) × 100π
ε0 = 10 × 0.02 × 314
ε0 = 0.2 × 314 = 62.8 V.
ε0 = NBAω
ω = 2πf = 2π(3000/60) = 100π rad/s.
A = 200 cm2 = 200 × 10-4 m2.
ε0 = 20 × 0.5 × (2×10-2) × 100π
ε0 = 10 × 0.02 × 314
ε0 = 0.2 × 314 = 62.8 V.
Q9. A 0.5 m long conductor moves at 20 m/s perpendicular to B = 2 T. If it is part of a circuit of 5
Ω, find force required to move it.
Solution:
Induced EMF ε = Blv = 2 × 0.5 × 20 = 20 V.
Current I = ε/R = 20/5 = 4 A.
Magnetic Force F = BIl = 2 × 4 × 0.5.
F = 4 N.
Induced EMF ε = Blv = 2 × 0.5 × 20 = 20 V.
Current I = ε/R = 20/5 = 4 A.
Magnetic Force F = BIl = 2 × 4 × 0.5.
F = 4 N.
Q10. A solenoid has 1000 turns wound on a 50 cm long core of radius 2 cm. Calculate self-inductance.
Solution:
L = μ0 n2 Al
n = N/l = 1000 / 0.5 = 2000 turns/m.
A = πr2 = π(0.02)2 = 4π × 10-4 m2.
L = (4π × 10-7) × (2000)2 × (4π × 10-4) × 0.5
L = 4π × 4 × 106 × 2π × 10-4 × 10-7
L = 32 π2 × 10-5 ≈ 320 × 10-5 = 3.2 mH.
L = μ0 n2 Al
n = N/l = 1000 / 0.5 = 2000 turns/m.
A = πr2 = π(0.02)2 = 4π × 10-4 m2.
L = (4π × 10-7) × (2000)2 × (4π × 10-4) × 0.5
L = 4π × 4 × 106 × 2π × 10-4 × 10-7
L = 32 π2 × 10-5 ≈ 320 × 10-5 = 3.2 mH.
Important Formulae
20 NEET Golden Facts
- 1. Induced Charge: Depends only on change in flux (ΔΦ) and resistance, NOT on time rate. q = ΔΦ/R.
- 2. Lenz's Law: It is a consequence of Law of Conservation of Energy.
- 3. Inertia of Electricity: Self-inductance is called electrical inertia because it opposes change in current.
- 4. Sparking: Occurs during 'breaking' of circuit (switch off) due to large induced EMF in inductor.
- 5. Doubling Turns: If turns N are doubled in same length, L becomes 4 times (since L ∝ N2).
- 6. Dead Beat Galvanometer: Coil wound on metallic frame to produce eddy currents which damp oscillations quickly.
- 7. Metal Detector: Works on principle of change in inductance and resonance in AC circuit.
- 8. Free Fall Magnet: Acceleration of magnet falling through a coil is less than g (due to opposing force).
- 9. Cut Ring: If the ring has a cut (open circuit), EMF is induced but no Current flows (No opposition to magnet).
- 10. DC Block: Inductor allows DC to flow easily (f=0, XL=0) but blocks AC.
- 11. Plane Flies: Potential difference develops between wing tips of aircraft flying in Earth's B-field (Vertical component).
- 12. AC Generator: Slip rings produce AC. Split rings (Commutator) produce DC.
- 13. Non-Inductive: Resistance coils are double wound to make net inductance zero.
- 14. Flux Max: Flux is max when θ=0. EMF is max when θ=90 (since EMF ∝ sinθ).
- 15. Iron Core: Putting iron core inside solenoid increases L drastically (by factor μr).
- 16. Dimensions: [L/R] has dimensions of Time. [L] = [ML2T-2A-2].
- 17. Disc Rotation: Metal disc rotating in B-field cuts flux lines → EMF induced between Center and Rim.
- 18. 1 Henry: Current changing at 1 A/s inducing 1 V EMF.
- 19. Coupling: Tight coupling (k=1) means 100% flux linkage. Loose coupling (k<1).
- 20. Fleming's Right Hand: Used to find direction of Induced Current. (Left hand is for Force).
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