When the circuit current in the RLC series circuit is in phase with the applied voltage, the circuit is said to be in Series Resonance.
Resonance in AC Circuit
An ac circuit containing reactive elements(L and C) is said to be in resonance when the circuit power factor is unity. Resonance means to be in step with. When applied voltage and circuit current in an ac circuit are in step with(i.e phase angle is Zero or power factor is unity) the circuit is said to be in electrical resonance. If a condition exists in a series a.c circuit, it is called series resonance. If the condition exists in a parallel a.c circuit, it is called parallel resonance. The frequency at which resonance occurs is called resonant frequency(fr).
An R-L-C series ac circuit is said to be in resonance when the circuit power factor is unity i.e XL=XC. The frequency fr at which it occurs is called resonant frequency. The resonance i.e (XL=XC) in an RLC series circuit can be achieved by changing the supply frequency because XL & XC are frequency dependent. At a certain frequency fr, XL becomes equal to XC and the resonance takes place.
At a series resonance,
From the above, we can conclude that,
- Increasing either inductance or the capacitance caused the resonant frequency to decrease.
- For a given value of inductance and capacitance, there is only one resonant frequency.
- There are an infinite number of inductor and capacitor combinations for any specified resonant frequency.
Graphical Explanation of Series Resonance
When the frequency of the applied voltages changes the impedance of the circuit varies because both(XL=2πfL) & (XC=1/2πfC) are frequency dependent. Since XL=2πfL, XL ∝ f so that variation of XL with f is a straight line passing through the origin. Again, XC=1/2πfC so that XC ∝ 1/f variation of XC with f is a curve approaching the two axes.
The resistance R is independent of the frequency and is thus represented by a line parallel to the frequency axis. The difference between XL-XC is represented by the dotted lines. The difference reduces to Zero at point A called fr and series resonance occurs. At series resonance, Zr=R of the circuit is minimum so that the current is maximum. At frequencies above and below the resonant frequency, the current is less than the maximum current.
At series resonance,
Effects of Series Resonance
when series resonance occurs, the effect on the circuit is the same as though neither inductance nor capacitance is present. The current under this condition is dependent only on the resistance of the circuit and voltage across it.
- The impedance of the circuit is minimum and is equal to the resistance of the circuit i.e. Zr=R.
- The current in the circuit is maximum as it is limited by the resistance of the circuit alone
. As the current is at its maximum value, the power of the circuit will also be at its maximum value.
- Since at series resonance, the current flowing in the circuit is very large, the voltage drops across L and C are also very large. These drops are much greater than the applied voltage. However, the voltage drop across the L-C combination as a whole will be Zero because these drops are equal in magnitude but 180° out of phase with each other.
Q-Factor of Series Resonant circuit
The Q-factor of a series resonant circuit can also be expressed in terms of L and C.
The value of the Q-factor depends entirely upon the design of the coil (i.e R-L part of R-L-C circuit) because resistance arises in this rather than in a capacitor. With a well-designed coil, the Q-factor can be 200 or more. The Q factor of a series circuit indicates how many times potential differences across L or C are greater than the applied voltage at resonance.
The bandwidth of a series circuit
The bandwidth of a series circuit is defined as the range of frequencies over which circuit current is equal to or greater than 70.7% maximum current(Ir, current at resonance).
In an R-L-C series circuit changes with frequency. For any frequency lying between f1 and f2, the circuit current is equal to or greater than 70.07% maximum current (i.e Ir=V/R). Therefore f2-f1 is the bandwidth of the circuit.
where f1 and f2 are the limiting frequencies at which the current is exactly equal to 70.7% of the maximum value. The frequency f1 is the lower cut-off frequency and the frequency f2 is called upper cut-off frequency. The bandwidth of a series circuit means that the circuit will offer very low impedance to this frequency range.
Features of Series Resonance