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Electromagnetic induction explains how changing magnetic fields create electric fields and currents. This topic connects generators, transformers, motors, wireless charging, and many modern power systems. A cheat sheet helps students keep track of sign conventions, units, and formulas that often look similar but mean different things.

It is especially useful for comparing DC circuit ideas with AC circuits that change over time.

The core ideas include magnetic flux, induced emf, Lenz’s law, and the behavior of inductors and capacitors in alternating current. Faraday’s law states that a changing magnetic flux produces an emf, while Lenz’s law gives the direction of the induced current. In AC circuits, resistance, inductive reactance, and capacitive reactance combine into impedance.

Power in AC circuits depends on rms values and the phase angle between voltage and current.

Key Facts

  • Magnetic flux is ΦB=BAcosθ\Phi_B = BA\cos\theta, where BB is magnetic field, AA is area, and θ\theta is the angle between BB and the area vector.
  • Faraday’s law is E=NΔΦBΔt\mathcal{E} = -N\frac{\Delta \Phi_B}{\Delta t}, where NN is the number of loops and the negative sign shows Lenz’s law.
  • Motional emf for a straight conductor moving perpendicular to a magnetic field is E=Bv\mathcal{E} = B\ell v.
  • Self-induced emf in an inductor is EL=LΔIΔt\mathcal{E}_L = -L\frac{\Delta I}{\Delta t}, where LL is inductance in henrys.
  • For a transformer, VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p} and, for an ideal transformer, VpIp=VsIsV_p I_p = V_s I_s.
  • The rms values for sinusoidal AC are Vrms=Vmax2V_{\mathrm{rms}} = \frac{V_{\max}}{\sqrt{2}} and Irms=Imax2I_{\mathrm{rms}} = \frac{I_{\max}}{\sqrt{2}}.
  • Inductive reactance is XL=2πfLX_L = 2\pi fL, and capacitive reactance is XC=12πfCX_C = \frac{1}{2\pi fC}.
  • The impedance of a series RLC circuit is Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}, and resonance occurs when XL=XCX_L = X_C.

Vocabulary

Magnetic flux
Magnetic flux is the amount of magnetic field passing through an area, calculated by ΦB=BAcosθ\Phi_B = BA\cos\theta.
Induced emf
Induced emf is the voltage produced when magnetic flux through a circuit changes over time.
Lenz’s law
Lenz’s law states that an induced current flows in a direction that opposes the change in magnetic flux that caused it.
Inductance
Inductance is a property of a coil or circuit that measures how strongly it opposes changes in current.
Reactance
Reactance is the opposition to AC current caused by inductors or capacitors, measured in ohms.
Impedance
Impedance is the total opposition to AC current in a circuit, combining resistance and reactance.

Common Mistakes to Avoid

  • Dropping the negative sign in Faraday’s law is a mistake because E=NΔΦBΔt\mathcal{E} = -N\frac{\Delta \Phi_B}{\Delta t} includes Lenz’s law, which determines the direction of the induced effect.
  • Using BABA for magnetic flux without cosθ\cos\theta is a mistake because flux depends on the angle between the magnetic field and the area vector.
  • Confusing peak and rms values is a mistake because AC power calculations usually use VrmsV_{\mathrm{rms}} and IrmsI_{\mathrm{rms}}, not VmaxV_{\max} and ImaxI_{\max}.
  • Adding resistance and reactance directly in a series RLC circuit is a mistake because impedance uses Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}, not R+XL+XCR + X_L + X_C.
  • Assuming a transformer changes power in an ideal circuit is a mistake because an ideal transformer has VpIp=VsIsV_p I_p = V_s I_s, so increasing voltage decreases current.

Practice Questions

  1. 1 A coil with N=200N = 200 turns has its magnetic flux change from 0.030 Wb0.030\ \mathrm{Wb} to 0.010 Wb0.010\ \mathrm{Wb} in 0.50 s0.50\ \mathrm{s}. Find the average induced emf.
  2. 2 A transformer has Np=500N_p = 500 turns and Ns=2500N_s = 2500 turns. If the primary voltage is 120 V120\ \mathrm{V}, what is the secondary voltage for an ideal transformer?
  3. 3 In a series RLC circuit, R=40 ΩR = 40\ \Omega, XL=90 ΩX_L = 90\ \Omega, and XC=60 ΩX_C = 60\ \Omega. Calculate the impedance ZZ.
  4. 4 Explain why an induced current appears in a loop when a magnet is pushed toward it, and describe how Lenz’s law determines the current’s direction.