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Circuit analysis connects voltage, current, resistance, capacitance, and inductance so students can predict how electrical networks behave. This cheat sheet covers both steady DC circuits and sinusoidal AC circuits, which are essential in college physics and engineering. It helps students organize sign conventions, circuit laws, equivalent components, and frequency-dependent behavior in one quick reference. The core tools are Ohm's law, Kirchhoff's junction and loop rules, equivalent resistance and capacitance, and time constants for transient circuits. For AC circuits, phasors and impedance turn sinusoidal circuit problems into algebra with complex quantities. Power calculations depend on whether the circuit is DC, purely resistive AC, or has phase differences between voltage and current.

Key Facts

  • Ohm's law relates voltage, current, and resistance by V=IRV = IR for an ideal resistor.
  • Kirchhoff's current law says the algebraic sum of currents at a junction is zero, so I=0\sum I = 0.
  • Kirchhoff's voltage law says the algebraic sum of potential differences around a closed loop is zero, so ΔV=0\sum \Delta V = 0.
  • Series resistors add directly as Req=R1+R2+R_{\text{eq}} = R_1 + R_2 + \cdots, while parallel resistors satisfy 1Req=1R1+1R2+\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \cdots.
  • Capacitors combine oppositely to resistors: series capacitors satisfy 1Ceq=1C1+1C2+\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} + \cdots, while parallel capacitors add as Ceq=C1+C2+C_{\text{eq}} = C_1 + C_2 + \cdots.
  • The time constant for an RC circuit is τ=RC\tau = RC, and the time constant for an RL circuit is τ=LR\tau = \frac{L}{R}.
  • AC impedance is ZR=RZ_R = R, ZL=iωLZ_L = i\omega L, and ZC=1iωCZ_C = \frac{1}{i\omega C}, where ω=2πf\omega = 2\pi f.
  • Average AC power is Pavg=VrmsIrmscosϕP_{\text{avg}} = V_{\text{rms}} I_{\text{rms}} \cos \phi, where ϕ\phi is the phase angle between voltage and current.

Vocabulary

Node
A node is a connection point in a circuit where two or more elements meet and share the same electric potential.
Loop
A loop is any closed path through a circuit that returns to its starting point.
Impedance
Impedance is the complex opposition to AC current, written as ZZ, and measured in ohms.
Phasor
A phasor is a rotating complex representation of a sinusoidal voltage or current with a fixed amplitude and phase.
Reactance
Reactance is the frequency-dependent part of impedance caused by inductors or capacitors.
Resonance
Resonance occurs in an RLC circuit when inductive and capacitive reactances cancel, so ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}}.

Common Mistakes to Avoid

  • Adding parallel resistors as R1+R2R_1 + R_2 is wrong because parallel branches provide multiple current paths, so use 1Req=1R1+1R2\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2}.
  • Using peak voltage instead of RMS voltage in AC power is wrong unless the formula is written for peak values. For standard power formulas, use Vrms=V02V_{\text{rms}} = \frac{V_0}{\sqrt{2}} and Irms=I02I_{\text{rms}} = \frac{I_0}{\sqrt{2}}.
  • Ignoring phase angle in AC power is wrong for circuits with capacitors or inductors. The correct average power is Pavg=VrmsIrmscosϕP_{\text{avg}} = V_{\text{rms}} I_{\text{rms}} \cos \phi, not just VIVI.
  • Treating capacitors and inductors like resistors in AC is wrong because their opposition depends on frequency. Use XL=ωLX_L = \omega L and XC=1ωCX_C = \frac{1}{\omega C}.
  • Choosing inconsistent loop signs is wrong because it can reverse voltage rises and drops within Kirchhoff's voltage law. Pick a loop direction and apply ΔV=0\sum \Delta V = 0 consistently.

Practice Questions

  1. 1 A 12V12\,\text{V} battery is connected to resistors R1=4ΩR_1 = 4\,\Omega and R2=8ΩR_2 = 8\,\Omega in series. Find ReqR_{\text{eq}} and the current II.
  2. 2 Two resistors, R1=6ΩR_1 = 6\,\Omega and R2=3ΩR_2 = 3\,\Omega, are connected in parallel across a 9V9\,\text{V} source. Find ReqR_{\text{eq}} and the total current.
  3. 3 An AC source has f=60Hzf = 60\,\text{Hz} and is connected to a capacitor C=100μFC = 100\,\mu\text{F}. Calculate the capacitive reactance XC=12πfCX_C = \frac{1}{2\pi f C}.
  4. 4 In a series RLC circuit, explain why the current is largest at resonance even though the circuit contains both an inductor and a capacitor.