1. Alternating Current — Basic Definitions

An alternating current (or voltage) varies sinusoidally with time:

i=I0sin(ωt+ϕ)v=V0sin(ωt+ϕ)

Symbol Name Relation / Value
I0, V0 Peak (maximum) value Amplitude of oscillation
ω Angular frequency ω=2πf=2π/T (rad/s)
f Frequency f=1/T (Hz); mains supply in India: 50 Hz
T Time period T=1/f= 20 ms at 50 Hz
ϕ Initial phase Phase at t=0

2. RMS (Root Mean Square) Value

The RMS value is the effective value of AC — the DC equivalent that produces the exact same heating effect (power dissipation) in a given resistor.

Irms=I020.707I0Vrms=V020.707V0

Derivation: Irms2=i2=I02sin2(ωt)=I02×12=I022Irms=I02

Example: Indian mains voltage is 220 V RMS peak voltage V0=2202 311 V.

3. Average (Mean) Value of AC

The mathematical average of a pure sinusoid over a full cycle is exactly zero (equal positive and negative areas). The average over a half cycle is:

Vhalf=2V0π0.637V0

Form factor: kf=VrmsVhalf=V0/22V0/π=π221.11

Peak factor (crest factor): kp=V0Vrms=21.414

4. AC Generator (Source of AC)

An AC generator (alternator) converts mechanical energy into electrical energy using electromagnetic induction. A coil of N turns, area A, rotating with angular velocity ω in a uniform magnetic field B generates an EMF:

ε=NBAωsin(ωt)=ε0sin(ωt)

where ε0=NBAω is the peak EMF.

Worked example: N=100, B=0.1 T, A=0.5 m2, ω=100π rad/s:

ε0=100×0.1×0.5×100π=500π 1571 V

5. Phasor Representation

A phasor is a rotating vector that graphically represents a sinusoidal quantity. The projection of a phasor onto the vertical axis gives the instantaneous value of that quantity.

  • Length of phasor = peak amplitude (I0 or V0).
  • Phasors rotate anticlockwise with angular frequency ω.
  • The phase difference ϕ between two sinusoids is the angle between their phasors.
  • Voltage leads current by ϕ: The voltage phasor is ϕ ahead of the current phasor.
  • Current leads voltage by ϕ: The current phasor is ϕ ahead of the voltage phasor.

Adding AC voltages: Use phasor addition (vector addition) — never simple algebraic addition — because voltages and currents generally differ in phase.

6. Phase Relationships — Summary

Circuit element Phase of V relative to I Phasor description
Pure resistor (R) In phase (ϕ=0) VR and I phasors completely coincide.
Pure inductor (L) V leads I by 90 (π/2) VL phasor is 90 ahead of I.
Pure capacitor (C) V lags I by 90 (or I leads V by 90) I phasor is 90 ahead of VC.

Memory aids:

  • ELI the ICE man: In an Inductor (L), EMF (E) leads current (I). In a Capacitor (C), current (I) leads EMF (E).