Resonance Circuit: In an alternating current, if the phase of the applied potential difference and the current flowing in the circuit are same, then the circuit is called resonance circuit. The phenomenon shown by these types of circuit is called resonance.
Resonance L.C.R. circuit are of two types:
(i) Series resonance circuit.
(ii) Parallel resonance circuit.
Resonant Frequency for series L-C-R circuit.
We know that the impedance of the circuit is Z=√R2+(ωL−1ωL)2 .......(i)
If V is the potential difference and I is the current and ϕ is the phase difference between then,
tanθ=ωL−1ωCR
Or ϕ=tan⎧⎪
⎪
⎪⎨⎪
⎪
⎪⎩ωL−1ωCR⎫⎪
⎪
⎪⎬⎪
⎪
⎪⎭
In the condition of impedance the current flows through this equation
I=I0sin(ωt−ϕ)
where I0=V0Z=V0√R2+(XL−XC)2
I0=V0√R2+(ωL−1ωC)2 ......(ii)
If ωL=1ωC then from equation (ii)
Z=R (minimum) and I0=V0R (maximum)
Thus, in this condition the impedance is minimum so that the current flowing in the circuit is maximum.
This condition is known as resonance.
In the condition of resonance, ωL=1ωC
ω2=1LC
Or ω=1√LC
2πf=1√LC
f=12π√LC
This is expression for resonant frequency for series L-C-R circuit.