Quick Recap — Advanced EMI & AC (Multi-step)

  • Rod on rails: ε=BLv\varepsilon=BLv, current BLvR\dfrac{BLv}{R}, force to keep it moving B2L2vR\dfrac{B^2L^2v}{R}, power dissipated (BLv)2R\dfrac{(BLv)^2}{R}.
  • LC oscillations: ω0=1LC\omega_0=\dfrac{1}{\sqrt{LC}}; energy sloshes between 12LI2\tfrac12 LI^2 and q22C\tfrac{q^2}{2C}, total conserved.
  • Series LCR numbers: Z=R2+(XLXC)2Z=\sqrt{R^2+(X_L-X_C)^2}, Irms=VrmsZI_{rms}=\dfrac{V_{rms}}{Z}, P=Irms2RP=I_{rms}^2R, quality factor Q=1RLCQ=\dfrac{1}{R}\sqrt{\dfrac{L}{C}}.
  • Inductor combinations: series L1+L2L_1+L_2; parallel L1L2L1+L2\dfrac{L_1L_2}{L_1+L_2} (no coupling).
  • Induced charge: q=NΔΦRq=\dfrac{N\,\Delta\Phi}{R}; rotating-coil peak emf NBAωNBA\omega.

Worked mini-example. An LC circuit with L=2L=2 H and C=8 μC=8\ \muF oscillates at ω0=1LC=116×106=250\omega_0=\dfrac{1}{\sqrt{LC}}=\dfrac{1}{\sqrt{16\times10^{-6}}}=250 rad/s, i.e. f0=2502π40f_0=\dfrac{250}{2\pi}\approx40 Hz.