In alternating current (AC) circuits, the magnitude and direction of current and voltage vary sinusoidally with time. To simplify their analysis, the concept of rotating vectors, known as phasors, is used. Phasors allow us to represent sinusoidal quantities as rotating vectors in a complex plane, making the analysis of AC circuits easier and more intuitive.
A phasor is a rotating vector that represents a sinusoidal quantity. The length of the phasor corresponds to the peak value of the sine wave, and its angular position represents the phase of the wave at any given time.
The general expression for an AC voltage or current is:
V(t) = V₀ sin(ωt + φ)
Where:
- V₀ = Peak voltage
- ω = Angular frequency
- φ = Phase angle
- t = Time
In phasor notation, this can be represented as:
V = V₀ e^(j(ωt + φ))
where j is the imaginary unit.
1. Simplifies the addition and subtraction of sinusoidal waveforms.
2. Converts differential equations into simple algebraic equations.
3. Provides a visual representation of phase differences between waveforms.
Read Also: AC Voltage Applied to an Inductor – Class 12 Physics Notes
1. Draw a reference axis.
2. Represent the voltage or current as a vector with magnitude V₀.
3. The angle between the phasor and the reference axis corresponds to the phase angle φ.
4. As time progresses, the phasor rotates counter-clockwise at an angular velocity ω.
1. Analyzing series and parallel AC circuits.
2. Determining impedance and phase relationships.
3. Analyzing resonance in LCR circuits.
4. Calculating power in AC circuits.
Phasors are an essential tool for understanding and analyzing alternating current circuits. By representing sinusoidal quantities as rotating vectors in the complex plane, phasors simplify the mathematical analysis of AC circuits and help in visualizing phase relationships.