A circuit that contains pure resistance R ohms connected in series with a pure capacitor of capacitance C farads is known as RC Series Circuit. A sinusoidal voltage is applied to and current I flows through the resistance (R) and the capacitance (C) of the circuit.The RC Series circuit is shown in the figure below
- VR – voltage across the resistance R
- VC – voltage across the capacitor C
- V – total voltage across the RC Series circuit
- Phasor Diagram of RC Series Circuit
- Steps to draw a Phasor Diagram
- Phase angle
- Power in RC Series Circuit
- Waveform and Power Curve of the RC Series Circuit
Phasor Diagram of RC Series Circuit
The phasor diagram of the RC Series circuit is shown below
Steps to draw a Phasor Diagram
The following steps are used to draw the phasor diagram of RC Series circuit
- Take the current I (r.m.s value) as a reference vector
- Voltage drop in resistance VR = IR is taken in phase with the current vector
- Voltage drop in capacitive reactance VC = IXC is drawn 90 degrees behind the current vector, as current leads voltage by 90 degrees in pure capacitive circuit)
- The vector sum of the two voltage drops is equal to the applied voltage V (r.m.s value).
Now, VR = IR and VC = IXC
Where, XC = I/2πfC
From the phasor diagram shown above it is clear that the current in the circuit leads the applied voltage by an angle ϕ and this angle is called the phase angle.
Power in RC Series Circuit
Therefore, the instantaneous power is given by p = vi
Putting the value of v and i from the equation (1) and (2) in p = vi
The Average power consumed in the circuit over a complete cycle is given by
Where, cosϕ is called the power factor of the circuit.
Putting the value of V and cosϕ from the equation (3) the value of power will be
Waveform and Power Curve of the RC Series Circuit
The waveform and power curve of the RC Circuit is shown below
The various points on the power curve is obtained from the product of the instantaneous value of voltage and current. The power is negative between the angle (180◦ – ϕ) and 180◦ and between (360◦ -ϕ) and 360◦ and in the rest of the cycle the power is positive. Since the area under the positive loops is greater than that under the negative loops, therefore the net power over a complete cycle is positive.