Series LCR - circuit : -
Suppose a resistance R, an inductance L and capacitance C are connected in series to a source of alternating emf given by

1. Voltage VR = RI Racross the resistance R will be in phase with current I . So phasors VR and I are is same direction. The amplitude of VR is
VR0 = I0R
2. Voltage VL = X LI across the inductance L is ahead of current I in phase by π/2 rad. So phasor VL lies π/2 rad anticlockwise w.r.t. the phasor I . Its amplitude is
V0L = I0XL
3. Voltage Vc = XcI across the capacitance C lags behind the current I in phase by π/2 rad. So phasor VC lies π/2 clockwise w.r.t. the phasor I . Its amplitude is 0 0
V0c = I0 XC

As VL and VC are in opposite directions, their resultant is (VL - VC). By parallelogram law, the resultant of VR and (VL - VC) must be equal to the applied emf ε , given by the diagonal of the parallelogram.

Clearly, √(R2+(XL-XC)2) is the effective resistance of the series LCR - circuit which opposes or impedes the flow of current through it and is called its impedance. It is denoted by Z and its SI unit is ohm (Ω). Thus
