This unit covers series and parallel resonance, quality factor, bandwidth, self and mutual inductance, and coefficient of coupling. It discusses resonance occurring when the applied voltage and source current are in phase, making the circuit purely resistive. At resonance, the power factor is unity. Series resonance occurs when the inductive and capacitive reactances are equal in magnitude but cancel each other out. This happens at the resonant frequency. Applications of series resonance circuits include AC mains filters and radio/TV tuning circuits. The bandwidth, selectivity, and quality factor of series resonance circuits are also defined in relation to the resonant frequency, current, and cutoff frequencies.

1. UNIT-III
RESONANCE & COUPLED CIRCUITS

2. This unit covers
 Series & Parallel Resonance
 Quality Factor
 Bandwidth
 Self & Mutual Inductance
 Coefficient of coupling
 Tuned Circuits – Single Tuned Circuits

3. Resonance
 When a Sinusoidal forcing function produces a response of
Maximum Amplitude.
An Ac Circuit comprising of R,L and C is said to be in Resonance
when the Applied voltage ( Source Voltage ) and the Source
Current are in phase ( i.e., Purely Resistive Circuit )
At Resonance P.F = Unity
The driving point impedance (or admittance) is completely
real when this condition exists.

4. Resonance in Electric Circuits
Series Resonance
Parallel Resonance

5. Series Resonance Circuits
 The resonance of a series RLC circuit occurs
when the inductive and capacitive
reactances are equal in magnitude but
cancel each other. XL = XC
 The point at which this occurs is called the
Resonant Frequency
 Series Resonance circuits are one of the most
important circuits used in electrical and
electronic circuits.
 Since “Z” is minimum “Current “ is Maximum

6. Series Resonance Circuits
 Series Resonant Circuit has the capability to draw Heavy
currents & Power from the mains ( Acceptor Circuit )

7. Uses of Series Resonance Circuits
AC mains filters
Noise filters
radio and television tuning circuits producing a very
selective tuning circuit for the receiving of the different
frequency channels.

8. Inductive Reactance against Frequency
F is Infinity XL is also Infinity => Circuit element Acts Like O.C
F is Zero XL is also Zero => Circuit Element Acts Like S.C
( XL ∝ ƒ )

9. Capacitive Reactance against Frequency
F (or) C is Increases => XC is Decreases
F approaches to ∞, XC reduces to zero => Causes Circuit
element to act like a Perfect Conductor ( 0Ω )
( XC ∝ ƒ -1 )

10. Series Resonance Frequency
Electrical resonance occurs in an AC circuit when the two reactances
which are opposite and equal cancel each other out as XL = XC and
the point on the graph at which this happens is were the two
reactance curves cross each other.

11. Series Resonance Frequency
In a series resonant circuit, the resonant frequency, ƒr point can be
calculated as follows.

12. Impedance in a Series Resonance Circuit
Note that when the capacitive reactance dominates the circuit the
impedance curve has a hyperbolic shape to itself
but when the inductive reactance dominates the circuit the curve is
non-symmetrical due to the linear response of XL.

13. Impedance in a Series Resonance Circuit
If the circuits impedance is at its minimum at resonance then
consequently, the circuits admittance must be at its maximum and
one of the characteristics of a series resonance circuit is that
admittance is very high.
But this can be a bad thing because a very low value of resistance at
resonance means that the circuits current may be dangerously high.

14. Impedance in a Series Resonance Circuit
If at resonance the two reactances are equal and
cancelling, the two voltages representing VL and VC must
also be opposite and equal in value thereby cancelling
each other out because with pure components the phasor
voltages are drawn at +90o and -90o respectively. Then in a
series resonance circuit VL = -VC therefore, V = VR.

15. Bandwidth of a Series Resonance Circuit

16. Selectivity ( Q )
 selectivity of the circuit is a measure of its ability to reject
any frequencies either side of these points.
 A more selective circuit will have a narrower bandwidth
whereas a less selective circuit will have a wider
bandwidth.
 The selectivity of a series resonance circuit can be
controlled by adjusting the value of the resistance only,
keeping all the other components the same, since
 Q = (XL or XC)/R.

17. Relationship between resonance, bandwidth, selectivity and
quality factor for a series resonance circuit being defined as:
1). Resonant Frequency, (ƒr)

18. Relationship between resonance, bandwidth, selectivity and
quality factor for a series resonance circuit being defined as:
2). Current, (I)

19. Relationship between resonance, bandwidth, selectivity and
quality factor for a series resonance circuit being defined as:
3). Lower cut-off frequency, (ƒL)

20. Relationship between resonance, bandwidth, selectivity and
quality factor for a series resonance circuit being defined as:
4). Upper cut-off frequency, (ƒH)

21. Relationship between resonance, bandwidth, selectivity and
quality factor for a series resonance circuit being defined as:
5). Bandwidth, (BW)
6). Quality Factor, (Q)

22. Problems