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This cheat sheet covers alternating current circuits using impedance, phasors, and resonance in resistor, inductor, and capacitor combinations. Students need these tools because AC circuit quantities change with time and cannot always be added like simple numbers. Phasors make sinusoidal voltage and current easier to compare, while impedance shows how resistors, capacitors, and inductors oppose AC.

The reference is designed for quick review during homework, labs, and exam preparation.

The core idea is that resistance, inductive reactance, and capacitive reactance combine into a complex impedance ZZ. In a series RLC circuit, the impedance magnitude is Z=R2+(XLXC)2|Z| = \sqrt{R^2 + (X_L - X_C)^2} and the resonance frequency is f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}. At resonance, XL=XCX_L = X_C, the phase angle is ϕ=0\phi = 0, and current is maximum in a series circuit.

Power depends on both rms values and phase through P=VrmsIrmscosϕP = V_{\text{rms}} I_{\text{rms}} \cos\phi.

Key Facts

  • Inductive reactance is XL=ωL=2πfLX_L = \omega L = 2\pi fL, so an inductor opposes AC more strongly as frequency increases.
  • Capacitive reactance is XC=1ωC=12πfCX_C = \frac{1}{\omega C} = \frac{1}{2\pi fC}, so a capacitor opposes AC less strongly as frequency increases.
  • For a series RLC circuit, the impedance is Z=R+j(XLXC)Z = R + j(X_L - X_C) and the magnitude is Z=R2+(XLXC)2|Z| = \sqrt{R^2 + (X_L - X_C)^2}.
  • Ohm’s law for AC rms values is Vrms=IrmsZV_{\text{rms}} = I_{\text{rms}} |Z|.
  • The phase angle in a series RLC circuit satisfies tanϕ=XLXCR\tan\phi = \frac{X_L - X_C}{R}.
  • Series resonance occurs when XL=XCX_L = X_C, giving ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}} and f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}.
  • Average power in an AC circuit is P=VrmsIrmscosϕ=Irms2RP = V_{\text{rms}} I_{\text{rms}} \cos\phi = I_{\text{rms}}^2 R for a series RLC circuit.
  • The quality factor for a series RLC circuit can be written as Q=ω0LR=1ω0CRQ = \frac{\omega_0 L}{R} = \frac{1}{\omega_0 C R}.

Vocabulary

Impedance
Impedance ZZ is the total opposition an AC circuit gives to current, including both resistance and reactance.
Reactance
Reactance is the frequency-dependent opposition to AC current caused by inductors or capacitors.
Phasor
A phasor is a rotating vector used to represent the magnitude and phase of a sinusoidal voltage or current.
Resonance
Resonance is the condition in an RLC circuit where XL=XCX_L = X_C and the net reactance is zero.
Phase Angle
The phase angle ϕ\phi measures how far voltage and current are shifted from each other in an AC circuit.
Power Factor
The power factor is cosϕ\cos\phi, the fraction of apparent power converted into average real power.

Common Mistakes to Avoid

  • Adding reactances without signs is wrong because inductive reactance and capacitive reactance act in opposite phasor directions. In a series RLC circuit, use XLXCX_L - X_C, not XL+XCX_L + X_C, for net reactance.
  • Using peak values in rms power formulas is wrong unless the formula is adjusted. For average power, use P=VrmsIrmscosϕP = V_{\text{rms}} I_{\text{rms}} \cos\phi.
  • Forgetting frequency dependence is wrong because XLX_L and XCX_C change when ff changes. Always calculate XL=2πfLX_L = 2\pi fL and XC=12πfCX_C = \frac{1}{2\pi fC} at the given frequency.
  • Assuming resonance means zero impedance is wrong for a series RLC circuit with resistance. At resonance, Z=R|Z| = R, so current is limited by the resistor.
  • Confusing lead and lag is wrong because capacitors and inductors shift current in opposite directions. In a capacitive circuit current leads voltage, while in an inductive circuit current lags voltage.

Practice Questions

  1. 1 A series RLC circuit has R=40 ΩR = 40\ \Omega, L=0.20 HL = 0.20\ \text{H}, C=50 μFC = 50\ \mu\text{F}, and f=60 Hzf = 60\ \text{Hz}. Find XLX_L, XCX_C, and Z|Z|.
  2. 2 A series circuit has R=25 ΩR = 25\ \Omega, XL=80 ΩX_L = 80\ \Omega, and XC=50 ΩX_C = 50\ \Omega. Find the phase angle ϕ\phi and state whether the circuit is inductive or capacitive.
  3. 3 Find the resonance frequency of a series RLC circuit with L=0.10 HL = 0.10\ \text{H} and C=10 μFC = 10\ \mu\text{F} using f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}.
  4. 4 Explain why the current is maximum at resonance in a series RLC circuit even though the inductor and capacitor may each have large reactance.