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APPhysicsAP Physics C: E&M

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.

  1. Emf: ε = BLv.
  2. Current: I = BLv / R.
  3. 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 energy U = ½LI²

In an LR circuit with a battery, the current rises as

I(t) = (ε/R)(1 − e^(−t/τ)), with τ = 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

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Mock Exam

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Practice Quiz

Test yourself: instant results and explanations.

  1. 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. 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. 3. An LR circuit has ε = 12 V, R = 4 Ω and L = 2 H. What is its time constant?

  4. 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. 5. A 0.4 H inductor carries a steady current of 5 A. How much energy is stored in it?

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