Consider a resistance R, an inductor of self inductance L and a capacitor of capacitance C connected in series across an AC source. The applied voltage is given by,
v = v0sinωt ……(1)

Where, v is the instantaneous value, v is the peak value and ω = 2πf, f being the frequency of AC.
If i be the instantaneous current at time t, the instantaneous voltages across R, L and C are respectively iR, iXL and iXC. The vector sum of the voltage amplitudes across R, L, C equals the amplitude v0 of the voltage applied.

Let vR, vL and VC be the voltage amplitudes .across R, L and C respectively and I0 the current amplitude. Then vR = I0R is in phase with i0.
vL = i0XL = I0(ωL) leads i0 by 90°
vc = i0Xc = i0(\(\frac{1}{\omega C}\)) lags behind io by 90°
The current in a pure resistor is phase with the voltage, whereas the current in a pure inductor lags the voltage by rad. The current in a pure capacitor leads the voltage by rad.
For vL > vc, phase angle Φ between the voltage and the current is positive.
From the right angled triangle OAP,
OP2 = OA2 + AP2 = OA2 + OB2 (Q AP = OB)
v2 = v2R + (VL – Vc)2 = (iR)2 + (iXL – iXc)2
= i2(R2 + (XL – Xc)2)

Where Z is the impedance of the circuit. Phase angle between v & i.
