Alternating current (AC) is the form of electricity supplied to homes, factories, and laboratories worldwide — because it can be stepped up and down in voltage efficiently using transformers, allowing long-distance power transmission with minimal losses. Unlike direct current (DC), AC reverses direction periodically, making its analysis richer and more mathematical. The foundational concepts — how to characterise AC by its peak and RMS values, how to represent voltages and currents as phasors, and how phase differences arise between voltage and current — underpin everything from impedance calculations to resonance and power factor. For JEE and NEET, this topic provides direct numerical questions on RMS/peak values and conceptual questions on phasor diagrams and phase relationships.
1. Alternating Current — Basic Definitions
An alternating current (or voltage) varies sinusoidally with time:
| Symbol |
Name |
Relation / Value |
| , |
Peak (maximum) value |
Amplitude of oscillation |
|
Angular frequency |
(rad/s) |
|
Frequency |
(Hz); mains supply in India: 50 Hz |
|
Time period |
20 ms at 50 Hz |
|
Initial phase |
Phase at |
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.
Derivation:
Example: Indian mains voltage is 220 V RMS peak voltage 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:
Form factor:
Peak factor (crest factor):
4. AC Generator (Source of AC)
An AC generator (alternator) converts mechanical energy into electrical energy using electromagnetic induction. A coil of turns, area , rotating with angular velocity in a uniform magnetic field generates an EMF:
where is the peak EMF.
Worked example: , , , :
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 ( or ).
- Phasors rotate anticlockwise with angular frequency .
- The phase difference between two sinusoids is the angle between their phasors.
- Voltage leads current by : The voltage phasor is ahead of the current phasor.
- Current leads voltage by : The current phasor is 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 relative to |
Phasor description |
| Pure resistor () |
In phase () |
and phasors completely coincide. |
| Pure inductor () |
leads by () |
phasor is ahead of . |
| Pure capacitor () |
lags by (or leads by ) |
phasor is ahead of . |
Memory aids:
- ELI the ICE man: In an Inductor (L), EMF (E) leads current (I). In a Capacitor (C), current (I) leads EMF (E).
Practice Questions
Q1 (JEE Main / NEET): The peak voltage of Indian household mains supply (220 V rms, 50 Hz) is approximately:
A) 220 V
B) 155 V
C) 311 V
D) 440 V
Answer: C) 311 V.
Explanation:
Q2 (NEET): An AC source has a peak EMF of 200 V at a frequency of 50 Hz. Write the expression for the instantaneous EMF and find the RMS value.
Explanation:
Angular frequency
Instantaneous EMF:
RMS EMF:
Q3 (JEE Main): An AC generator has a coil with turns, area 0.5 m², rotating at in a magnetic field 0.1 T. Find the peak and RMS EMF.
Explanation:
Peak EMF:
RMS EMF:
Q4 (Board / NEET MCQ): In a purely capacitive circuit connected to an AC source, the current:
A) Is in phase with voltage
B) Leads voltage by 90°
C) Lags voltage by 90°
D) Leads voltage by 45°
Answer: B) Leads voltage by 90°.
Explanation: In a pure capacitor, current mathematically leads voltage by (90°) — this is the "ICE" part of the "ELI the ICE man" mnemonic. Physically, the capacitor charges and discharges such that peak current flows when the voltage crosses zero (the steepest rate of change), and current hits zero the moment the capacitor is fully charged (peak voltage).