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Electromagnetic Induction

A changing magnetic flux induces an EMF β€” this is Faraday's law, the basis of generators, transformers, and electric motors. Lenz's law tells you the direction: the induced current always opposes the change causing it. Self-inductance stores energy in the magnetic field, just as capacitance stores energy in the electric field.

Key Concepts

Faraday's Law
E=βˆ’dΞ¦B/dt\mathcal{E}=-d\Phi_B/dt. The EMF around a loop equals minus the rate of change of magnetic flux through it. In differential form: βˆ‡Γ—Eβƒ—=βˆ’βˆ‚Bβƒ—/βˆ‚t\nabla\times\vec E=-\partial\vec B/\partial t.
Lenz's Law
The induced EMF drives a current that creates a magnetic field opposing the change in flux. This is the minus sign in Faraday's law β€” nature resists changes in flux.
Self-Inductance
L=NΞ¦/IL=N\Phi/I (in henrys). Voltage across an inductor: E=βˆ’L dI/dt\mathcal{E}=-L\,dI/dt. Energy stored: U=12LI2U=\frac{1}{2}LI^2. For a solenoid: L=ΞΌ0n2VcoreL=\mu_0n^2 V_{\rm core}.
Mutual Inductance
M12=N2Ξ¦12/I1M_{12}=N_2\Phi_{12}/I_1. EMF induced in coil 2 by current in coil 1: E2=βˆ’MΒ dI1/dt\mathcal{E}_2=-M\ dI_1/dt. Neumann's formula: M12=M21M_{12}=M_{21} β€” mutual inductance is symmetric.

Key Equations

Faraday's law
E=βˆ’dΞ¦Bdt=βˆ’ddt∫SBβƒ—β‹…daβƒ—\mathcal{E} = -\frac{d\Phi_B}{dt} = -\frac{d}{dt}\int_S\vec{B}\cdot d\vec{a}
Induced EMF equals negative rate of flux change.
Inductance of solenoid
L=ΞΌ0n2β„“A=ΞΌ0n2VL = \mu_0 n^2 \ell A = \mu_0 n^2 V
L for a solenoid of volume V = β„“A, n turns/m.
Magnetic energy
U=12LI2=12ΞΌ0∫B2 dΟ„U = \frac{1}{2}LI^2 = \frac{1}{2\mu_0}\int B^2\,d\tau
Energy stored in the magnetic field of an inductor.
Worked Example

EMF from a Changing Flux

Problem

A rectangular loop (0.20Γ—0.300.20\times0.30 m) lies in the xyxy-plane in a field Bz=0.50tB_z=0.50t T (increasing). Find the induced EMF and current direction (R=2.0 ΩR=2.0\,\Omega).

Solution

Flux: Ξ¦B=Bβ‹…A=0.50tΓ—0.06=0.030t\Phi_B=B\cdot A=0.50t\times0.06=0.030t Wb.

E=βˆ’dΞ¦Bdt=βˆ’0.030Β V\mathcal{E} = -\frac{d\Phi_B}{dt} = -0.030\text{ V}

Magnitude: 30 mV. By Lenz's law, the current flows to oppose increasing +z+z flux β€” counterclockwise when viewed from +z+z.

I=∣E∣/R=0.030/2.0=0.015I=|\mathcal{E}|/R=0.030/2.0=0.015 A.

Answer ∣E∣=30|\mathcal{E}|=30 mV; I=15I=15 mA, counterclockwise.
Practice

Exercises

7 problems
1 of 7

A circular loop (radius R=0.15R=0.15 m) is in a uniform BB that increases at dB/dt=2.0dB/dt=2.0 T/s. Find the induced EMF (in mV).

mV
2 of 7

A solenoid (n=1000n=1000 turns/m, A=5Γ—10βˆ’4A=5\times10^{-4} mΒ², β„“=0.30\ell=0.30 m) has current decreasing at dI/dt=βˆ’2.0dI/dt=-2.0 A/s. Find the induced EMF (in mV). L=ΞΌ0n2β„“AL=\mu_0n^2\ell A.

mV
3 of 7

Energy stored in an inductor: L=0.050L=0.050 H, I=4.0I=4.0 A (in J).

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4 of 7

A rod of length β„“=0.50\ell=0.50 m moves at v=3.0v=3.0 m/s perpendicular to B=0.80B=0.80 T. Find the motional EMF (in V). E=Bvβ„“\mathcal{E}=Bv\ell.

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5 of 7

Two coils have mutual inductance M=0.020M=0.020 H. Current in coil 1 changes at dI1/dt=5.0dI_1/dt=5.0 A/s. Find EMF in coil 2 (in V).

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6 of 7

Inductance of a solenoid: n=2000n=2000/m, A=1.0Γ—10βˆ’3A=1.0\times10^{-3} mΒ², β„“=0.20\ell=0.20 m (in mH).

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7 of 7

A transformer has N1=200N_1=200 turns and N2=50N_2=50 turns. Input voltage V1=120V_1=120 V. Find output voltage V2V_2 (in V). V2/V1=N2/N1V_2/V_1=N_2/N_1.

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Key Takeaways

  • Faraday's law: E=βˆ’dΞ¦B/dt\mathcal{E}=-d\Phi_B/dt. Changing flux induces EMF; Lenz's law gives the direction.
  • Motional EMF: E=Bvβ„“\mathcal{E}=Bv\ell for a rod of length β„“\ell moving at vv in field BB.
  • Self-inductance LL: E=βˆ’L dI/dt\mathcal{E}=-L\,dI/dt; energy U=12LI2U=\frac{1}{2}LI^2.
  • Transformers: V2/V1=N2/N1V_2/V_1=N_2/N_1; power is conserved (ideal transformer).