What is a Series RLC Circuit?
A series RLC circuit is one the resistor, inductor and capacitor are connected in series across a voltage supply. The resulting circuit is called series RLC circuit. A circuit and phasor diagram for a series RLS circuit has been shown below.
Phasor Diagram of Series RLC Circuit
The phasor diagram of series RLC circuit is drawn by combining the phasor diagram of resistor, inductor and capacitor. Before doing so, one should understand the relationship between voltage and current in case of resistor, capacitor and inductor.


 Resistor
In case of resistor, the voltage and the current are in same phase or we can say that the phase angle difference between voltage and current is zero.  Inductor
In inductor, the voltage and the current are not in phase. The voltage leads that of current by 90° or in the other words, voltage attains its maximum and zero value 90° before the current attains it.  Capacitor
In case of capacitor, the current leads the voltage by 90° or in the other words, voltage attains its maximum and zero value 0° after the current attains it i.e the phasor diagram of capacitor is exactly opposite of inductor.
 Resistor

NOTE: For remembering the phase relationship between voltage and current, learn this simple word called ‘CIVIL’, i.e in capacitor current leads voltage and voltage leads current in inductor.
RLC Circuit
For drawing the phasor diagram of series RLC circuit, follow these steps:
Step – I. In case of series RLC circuit; resistor, capacitor and inductor are connected in series; so, the current flowing in all the elements are same i.e I_{ r } = I_{l} = I_{c} = I. For drawing the phasor diagram, take current phasor as reference and draw it on horizontal axis as shown in diagram.
Step – II. In case of resistor, both voltage and current are in same phase. So draw the voltage phasor, V_{R} along same axis or direction as that of current phasor i.e V_{R} is in phase with I.
Step – III. We know that in inductor, voltage leads current by 90° so draw V_{l} (voltage drop across inductor) perpendicular to current phasor in leading direction.
Step – IV. In case of capacitor, the voltage lags behind the current by 90° so draw V_{c} (voltage drop across capacitor) perpendicular to current phasor in downwards direction.
Step – V. For drawing the resultant diagram, draw V_{c} in upwards direction. Now draw resultant, V_{s} which is vector sum of voltage V_{r} and V_{L} – V_{C}.
Impedance for a Series RLC Circuit
The impedance Z of a series RLC circuit is defined as opposition to the flow of current, due to circuit resistance R, inductive reactance, X_{L} and capacitive reactance, X_{C}. If the inductive reactance is greater than the capacitive reactance, i.e X_{L} > X_{C}, then the RLC circuit has lagging phase angle and if the capacitive reactance is greater than the inductive reactance, i.e X_{C} > X_{L} then the RLC circuit have leading phase angle and if both inductive and capacitive are the same, i.e X_{L} = X_{C} then circuit will behave as purely resistive circuit.
We know that,
Substituting the values V_{S}^{2} = (IR)^{2} + (I X_{L} – I X_{C} )^{2}
From this impedance triangle: by using Pythagoras theorem we get;
Variation in Resistance, Reactance and Impedance with Frequency
In series RLC circuit, three types of impedance are involved
 Electrical resistance – Resistance is independent of frequency, so it remains constant with change in frequency.
 Inductive reactance, X_{L} – We know that X_{L} = 2πfL. So, inductive reactance varies directly with frequency. So the graph between frequency and inductive reactance is a straight line passing through the centre as shown by curve
a
.  Capacitive reactance, X_{C} – From the formula of capacitive reactance, X_{C} = 1/ 2πfC so, capacitive reactance varies inversely with frequency. Since the net reactance is ( X_{L} – X_{C}). So for drawing curve of ( X_{L } – X_{C}), firstly draw the graph of ( X_{C}) which is shown by curve
b
and then draw a curve for net reactance which is shown as curvec
.  The total impedance of circuit is shown by curve
d
which is obtained by adding constant resistor value to the net reactance.