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Useful formulas

DC (Direct current) circuits

 V = I \times R \;\; \mathrm{(Ohm's} \; \mathrm{Law)}

 P = I V = I^2 R = \frac{V^2}{R} \,\!

 V = \sqrt{PR}

where V = voltage difference (SI unit: volt), I = electric current (SI unit: ampere), R = resistance (SI unit: ohm), P = power (SI unit: watt).

AC (Alternating current) circuits

 V = \frac{P}{I\;\cos\phi}

 V = \frac{\sqrt{P\;Z}}{\sqrt{\cos\phi}} \!\

 V = \frac{I\;R}{\cos\phi}

Where V=voltage, I=current, R=resistance, P=true power, Z=impedance, φ=phase difference between I and V.

AC conversions

 V_{avg} = 0.637\,V_{pk} = \frac{2}{\pi} V_{pk} = \frac{\omega}{\pi}\int_0^{\pi/\omega} V_{pk} \sin(\omega t - k x) {\rm{d}}x \!\

 V_{rms} = 0.707\,V_{pk} = \frac{1}{\sqrt{2}} V_{pk} = V_{pk} \sqrt{\langle \sin^2(\omega t - k x) \rangle} \!\

 V_{pk} = 0.5\,V_{ppk} \!\

 V_{avg} = 0.319\,V_{ppk}\!\

 V_{rms} = 0.354\,V_{ppk} = \frac{1}{2 \sqrt{2}} V_{ppk}\!\

 V_{avg} = 0.900\,V_{rms} = \frac{2 \sqrt{2}}{\pi} V_{rms}\!\

Where Vpk=peak voltage, Vppk=peak-to-peak voltage, Vavg=average voltage over a half-cycle, Vrms=effective (root mean square) voltage, and we assumed a sinusoidal wave of the formVpksin(ωt  kx), with a period T = 2π / ω, and where the angle brackets (in the root-mean-square equation) denote a time average over an entire period.

Total voltage

Voltage sources and drops in series:

 V_T = V_1 + V_2 + V_3 + ... + V_n \!\

Voltage sources and drops in parallel:

 V_T = V_1 = V_2 = V_3 = ... = V_n \!\

Where  n \!\  is the nth voltage source or drop

Voltage drops

Across a resistor (Resistor R):

 V_R = IR_R  \!\

Across a capacitor (Capacitor C):

 V_C = IX_C  \!\

Across an inductor (Inductor L):

 V_L = IX_L  \!\

Where V=voltage, I=current, R=resistance, X=reactance.

 


   

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