Faraday's Law and Electromagnetic Induction
AP Physics C: Electricity and Magnetism, Electromagnetic Induction unit. Magnetic flux, Faraday's law, Lenz's law for direction, the moving rod on rails, and inductors in LR circuits.
Electromagnetic induction closes AP Physics C: Electricity and Magnetism. It ties together fields, circuits and calculus, which is why it appears on the free response section so often.
Magnetic flux
Φ_B = ∫ B · dA
For a uniform field through a flat loop, Φ_B = BA cos θ, where θ is the angle between the field and the normal to the loop.
Faraday's law
ε = −N dΦ_B/dt
An emf appears whenever the flux changes, and the flux can change in three ways: the field changes, the area changes, or the angle changes. With calculus the rule applies even when the change is not steady: differentiate the flux, then evaluate.
Lenz's law: the direction
The induced current flows so that its own magnetic field opposes the change in flux. It does not oppose the field itself.
- A north pole approaching a loop increases the flux, so the loop makes a field that pushes back: its near face becomes a north pole.
- A north pole moving away decreases the flux, so the induced field points the other way and pulls it back.
Use the right-hand rule to turn the needed field direction into a current direction.
The moving rod
A rod of length L slides at speed v on rails in a field B perpendicular to the circuit, which has resistance R.
- Emf:
ε = BLv. - Current:
I = BLv / R. - Magnetic force on the rod:
F = BIL = B²L²v / R, opposing the motion.
Worked numbers: L = 0.5 m, B = 0.4 T, v = 3 m/s, R = 2 Ω. Then ε = 0.6 V, I = 0.3 A, and F = 0.4 × 0.3 × 0.5 = 0.06 N. The power to keep the rod moving, Fv = 0.18 W, equals the power dissipated, I²R = 0.09 × 2 = 0.18 W: energy is conserved.
Inductors
ε_L = −L dI/dt, stored energyU = ½LI²
In an LR circuit with a battery, the current rises as
I(t) = (ε/R)(1 − e^(−t/τ)), withτ = L/R
Right after the switch closes the inductor blocks any sudden change, so the current starts at zero. After a long time it acts like a wire, and the current is ε/R.
The free response approach
Write the flux as a function of time first, then differentiate. For direction, state in words which change is being opposed before naming clockwise or counterclockwise. For a differential equation, show the loop rule that produces it.
Short Lesson Video
Mock Exam
Practice Quiz
Test yourself: instant results and explanations.
1. A 100-turn coil of area 0.02 m² sits in a field perpendicular to it. The field drops steadily from 0.5 T to 0 in 0.1 s. What is the average induced emf?
2. The north pole of a bar magnet is pushed down toward a horizontal loop lying below it. Seen from above, which way does the induced current flow?
3. An LR circuit has ε = 12 V, R = 4 Ω and L = 2 H. What is its time constant?
4. A loop of area 0.5 m² lies perpendicular to a field B(t) = 0.2t² tesla. What is the magnitude of the emf at t = 3 s?
5. A 0.4 H inductor carries a steady current of 5 A. How much energy is stored in it?
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