Circuits & Electrical Power — formula sheet

First-year EE · DC circuits to machines · 75 formulas · metric edition 1

Ohm's Law
V=IRV = I R
Electric Charge (Q = It)
Q=ItQ = I t
Electrical Power (P = VI)
P=VIP = V I
Electrical Power (P = I²R)
P=I2RP = I^{2} R
Electrical Power (P = V²/R)
P=V2RP = \frac{V^{2}}{R}
Two Resistors in Series
Rt=R1+R2R_{t} = R_{1} + R_{2}
Two Resistors in Parallel
Rt=R1R2R1+R2R_{t} = \frac{R_{1} R_{2}}{R_{1} + R_{2}}
Voltage Divider
Vout=VinR2R1+R2V_{out} = V_{in} \frac{R_{2}}{R_{1} + R_{2}}
Current Divider
I1=ItR2R1+R2I_{1} = I_{t} \frac{R_{2}}{R_{1} + R_{2}}
Resistance of a Wire (R = ρL/A)
R=ρLAR = \frac{\rho L}{A}
Conductor Resistance Temperature Correction
R2=R1[1+α(T2T1)]R_{2} = R_{1} \left[ 1 + \alpha (T_{2} - T_{1}) \right]
Kirchhoff's Voltage Law (Three-Element Loop)
Vs=V1+V2+V3V_{s} = V_{1} + V_{2} + V_{3}
Kirchhoff's Current Law (Node with Three Branches)
Iin=I1+I2+I3I_{in} = I_{1} + I_{2} + I_{3}
Thevenin Resistance from an Open-Circuit and Loaded Measurement
RTh=RL(VOCVL1)R_{Th} = R_{L} \left( \frac{V_{OC}}{V_{L}} - 1 \right)
Norton Current from the Thevenin Equivalent
IN=VThRThI_{N} = \frac{V_{Th}}{R_{Th}}
Maximum Power Transfer to a Matched Load
Pmax=VTh24RThP_{max} = \frac{V_{Th}^{2}}{4 R_{Th}}
Delta to Wye Resistance Transformation
RA=RabRcaRab+Rbc+RcaR_{A} = \frac{R_{ab} R_{ca}}{R_{ab} + R_{bc} + R_{ca}}
Wye to Delta Resistance Transformation
Rab=RARB+RBRC+RCRARCR_{ab} = \frac{R_{A} R_{B} + R_{B} R_{C} + R_{C} R_{A}}{R_{C}}
LED Series Resistor
R=VsVfIR = \frac{V_{s} - V_{f}}{I}
Capacitance (C = Q/V)
C=QVC = \frac{Q}{V}
Energy Stored in a Capacitor
E=12CV2E = \tfrac{1}{2} C V^{2}
Two Capacitors in Series
Ct=C1C2C1+C2C_{t} = \frac{C_{1} C_{2}}{C_{1} + C_{2}}
Two Capacitors in Parallel
Ct=C1+C2C_{t} = C_{1} + C_{2}
RC Time Constant
τ=RC\tau = R C
RC Capacitor Discharge
V=V0et/τV = V_{0} \, e^{-t/\tau}
RL Time Constant (τ = L/R)
τ=LR\tau = \frac{L}{R}
Energy Stored in an Inductor
E=12LI2E = \tfrac{1}{2} L I^{2}
RMS and Peak Voltage
Vrms=Vpeak2V_{rms} = \frac{V_{peak}}{\sqrt{2}}
Inductive Reactance (X_L = 2πfL)
XL=2πfLX_L = 2\pi f L
Capacitive Reactance (X_C = 1/2πfC)
XC=12πfCX_C = \frac{1}{2\pi f C}
Series RL or RC Impedance
Z=R2+X2Z = \sqrt{R^{2} + X^{2}}
Series RLC Impedance
Z=R2+(XLXC)2Z = \sqrt{R^{2} + (X_{L} - X_{C})^{2}}
Phase Angle from Power Factor
φ=arccos(PF)\varphi = \arccos(\text{PF})
LC Resonant Frequency
f=12πLCf = \frac{1}{2\pi\sqrt{LC}}
Q Factor of a Series Resonant Circuit
Q=1RLCQ = \frac{1}{R} \sqrt{\frac{L}{C}}
Bandwidth from Q and Centre Frequency
BW=f0QBW = \frac{f_{0}}{Q}
RC Cutoff Frequency
fc=12πRCf_{c} = \frac{1}{2\pi R C}
RL Cutoff Frequency
fc=R2πLf_{c} = \frac{R}{2\pi L}
Decibel Voltage Gain
GdB=20log10 ⁣(V2V1)G_{dB} = 20 \log_{10}\!\left(\frac{V_{2}}{V_{1}}\right)
Decibel Power Gain
GdB=10log10 ⁣(P2P1)G_{dB} = 10 \log_{10}\!\left(\frac{P_{2}}{P_{1}}\right)
Single-Phase Real Power with Power Factor
P=VIPFP = V I \, \text{PF}
Power Factor from Real and Apparent Power
PF=PS\text{PF} = \frac{P}{S}
Reactive Power (Power Triangle)
Q=S2P2Q = \sqrt{S^{2} - P^{2}}
Three-Phase Real Power
P=3VLILPFP = \sqrt{3} \, V_{L} I_{L} \, \text{PF}
Three-Phase Apparent Power
S=3VLILS = \sqrt{3} \, V_{L} I_{L}
Wye Line and Phase Voltage
VL=3VφV_{L} = \sqrt{3} \, V_{\varphi}
Delta Line and Phase Current
IL=3IφI_{L} = \sqrt{3} \, I_{\varphi}
Power-Factor Correction kvar
Qc=P(tanφ1tanφ2)Q_{c} = P \left( \tan\varphi_{1} - \tan\varphi_{2} \right)
Power-Factor Correction Capacitance
C=Qc2πfV2C = \frac{Q_{c}}{2\pi f V^{2}}
Electrical Energy (E = Pt)
E=PtE = P t
Energy Cost from a Utility Rate
Ce=EpeC_e = E \, p_e
Voltage Drop, Single Phase
Vd=2ρLIAV_{d} = \frac{2 \rho L I}{A}
Voltage Drop, Three Phase
Vd=3ρLIAV_{d} = \frac{\sqrt{3} \, \rho L I}{A}
Percent Voltage Drop
%Vd=100VdVs\%V_{d} = \frac{100 \, V_{d}}{V_{s}}
Peukert's Law (Battery Runtime)
t=H(CIH)kt = H \left( \frac{C}{I H} \right)^{k}
Synchronous Speed from Frequency and Poles
Ns=2fpN_{s} = \frac{2f}{p}
Induction Motor Slip
s=100(NsNr)Nss = \frac{100 \, (N_{s} - N_{r})}{N_{s}}
Motor Torque from Power and Speed
T=P2πNT = \frac{P}{2\pi N}
Motor Efficiency
η=100PoutPin\eta = \frac{100 \, P_{out}}{P_{in}}
Three-Phase Motor Full-Load Current
I=Pout3VPFηI = \frac{P_{out}}{\sqrt{3} \, V \, \text{PF} \, \eta}
Motor Locked-Rotor Starting Current
ILR=1000kP3VI_{LR} = \frac{1000 \, k \, P}{\sqrt{3} \, V}
Transformer Voltage Ratio
VsVp=NsNp\frac{V_{s}}{V_{p}} = \frac{N_{s}}{N_{p}}
Transformer Full-Load Current
IFL=SkVI_{FL} = \frac{S}{k \, V}
Voltage Regulation
%VR=100(VnlVfl)Vfl\%VR = \frac{100 \, (V_{nl} - V_{fl})}{V_{fl}}
Transformer Percent-Impedance Voltage Drop
Vd=%Z100SLSRVRV_{d} = \frac{\%Z}{100} \cdot \frac{S_{L}}{S_{R}} \cdot V_{R}
Available Short-Circuit Current from Percent Impedance
ISC=100IFL%ZI_{SC} = \frac{100 \, I_{FL}}{\%Z}
Generator Sizing from Connected Load
Pg=PcDf(1+m)P_{g} = P_{c} \, D_{f} \left( 1 + m \right)
Coulomb's Law
F=keq1q2r2F = \frac{k_e \, q_{1} q_{2}}{r^{2}}
Magnetic Force on a Moving Charge
F=qvBsinθF = q v B \sin\theta
Magnetic Force on a Current-Carrying Wire
F=BILsinθF = B I L \sin\theta
Force Between Parallel Wires
F=μ0I1I22πdF = \frac{\mu_0 I_1 I_2 \ell}{2\pi d}
Magnetic Field of a Solenoid
B=μ0NILB = \frac{\mu_0 N I}{L}
Magnetic Flux (Φ = BA cos θ)
Φ=BAcosθ\Phi = B A \cos\theta
Faraday's Law of Induction
ε=NΔΦΔt\varepsilon = N \frac{\Delta\Phi}{\Delta t}
Motional EMF (ε = BLv)
ε=BLv\varepsilon = B L v