Quick Recap — Alternating Current Circuits

  • AC values: I=I0sinωtI=I_0\sin\omega t; Irms=I02I_{rms}=\dfrac{I_0}{\sqrt2}, Vrms=V02V_{rms}=\dfrac{V_0}{\sqrt2}.
  • Reactances: inductive XL=ωLX_L=\omega L (grows with ff); capacitive XC=1ωCX_C=\dfrac{1}{\omega C} (falls with ff).
  • Series LCR: impedance Z=R2+(XLXC)2Z=\sqrt{R^2+(X_L-X_C)^2}; resonance at ω0=1LC\omega_0=\dfrac{1}{\sqrt{LC}}, where XL=XCX_L=X_C, Z=RZ=R (minimum), and current is maximum.
  • Power: P=VrmsIrmscosϕP=V_{rms}I_{rms}\cos\phi, power factor cosϕ=RZ\cos\phi=\dfrac{R}{Z}. A pure inductor or capacitor consumes no average power (wattless current).
  • Ideal transformer: VsVp=NsNp=IpIs\dfrac{V_s}{V_p}=\dfrac{N_s}{N_p}=\dfrac{I_p}{I_s} (power conserved).

Worked mini-example. A series circuit has R=30 ΩR=30\ \Omega, XL=80 ΩX_L=80\ \Omega, XC=40 ΩX_C=40\ \Omega: Z=302+(8040)2=900+1600=50 ΩZ=\sqrt{30^2+(80-40)^2}=\sqrt{900+1600}=50\ \Omega, and cosϕ=3050=0.6\cos\phi=\dfrac{30}{50}=0.6.