MECHANICAL DEPARTMENT
Elements of Electrical Engineering
ACTIVE LEARNING ASSIGNMENT
Topic: Resonance in series and parallel circuits
Guided by: Prof. Rahish
Group Members
 Hardik Panchal (130120119115)
 Vivek Panchal (130120119122)
 Parth Panchal (130120119120)
Content
 Series Resonance
 Parallel Resonance
 Important Parameters
 Resonance Frequency, o
 Half-power frequencies, 1 and 2
 Bandwidth, 
 Quality Factor, Q
 Application
Introduction
 Resonance is a condition in an RLC circuit in which
the capacitive and reactive reactance are equal in
magnitude, thereby resulting in a purely resistive
impedance.
 Resonance circuits are useful for constructing
filters and used in many application.
Series Resonance Circuit
At Resonance
 At resonance, the impedance consists only resistive
component R.
 The value of current will be maximum since the total
impedance is minimum.
 The voltage and current are in phase.
 Maximum power occurs at resonance since the power
factor is unity.
Series Resonance
CLTotal jX-jXRZ 
R
V
Z
V
I m
Total
s
m 
Total impedance of series RLC Circuit is
At resonance
The impedance now reduce to
CL XX 
RZTotal 
)X-j(XRZ CLTotal 
The current at resonance
Resonance Frequency
Resonance frequency is the frequency where the
condition of resonance occur.
Also known as center frequency.
Resonance frequency
rad/s
LC
1
ωo 
Hz
LC2
1

of
Half-power Frequency
rad/s
LC
1
2L
R
2L
R
ω
2
2 











rad/s
LC
1
2L
R
2L
R
ω
2
1 














Half-power frequencies is the frequency when the
magnitude of the output voltage or current is decrease
by the factor of 1 / 2 from its maximum value.
Also known as cutoff frequencies.
Bandwidth, 
rad/s)( 12 cc ωωβ 
rad/s
L
R
β 
Bandwidth,  is define as the difference between the
two half power frequencies.
The width of the response curve is determine by the
bandwidth.
Current Response Curve
Voltage Response Curve
Quality Factor (Q-Factor)
The ratio of resonance frequency to the bandwidth
The “sharpness” of response curve could be measured
by the quality factor, Q.
R
L
Q oo 



Q-Factor Vs Bandwidth
 Higher value of
Q, smaller the
bandwidth. (Higher
the selectivity)
 Lower value of Q larger
the bandwidth. (Lower
the selectivity)
Parallel Resonance
Parallel Resonance
The total admittance
ωL
ωC
1

Resonance occur when
)ωω L1/Cj(
R
1
YTotal 
321Total YYYY 
C)(-j/
1
L)(j
1
R
1
YTotal


Cj
ωL
j-
R
1
YTotal ω
At Resonance
 At resonance, the impedance consists only
conductance G.
 The value of current will be minimum since the
total admittance is minimum.
 The voltage and current are in phase.
Parameters in Parallel Circuit
rad/s
LC
1
2RC
1
2RC
1
ω
2
1 














Parallel resonant circuit has same parameters as the
series resonant circuit.
rad/s
LC
1
ωo 
rad/s
LC
1
2RC
1
2RC
1
ω
2
2 












Resonance frequency
Half-power frequencies
Parameters in Parallel Circuit
RC
β
ω
Q o
o

RC
1
12  ωωβ
Bandwidth
Quality Factor
Resonance in series and parallel circuits

Resonance in series and parallel circuits

  • 1.
    MECHANICAL DEPARTMENT Elements ofElectrical Engineering ACTIVE LEARNING ASSIGNMENT Topic: Resonance in series and parallel circuits Guided by: Prof. Rahish
  • 2.
    Group Members  HardikPanchal (130120119115)  Vivek Panchal (130120119122)  Parth Panchal (130120119120)
  • 3.
    Content  Series Resonance Parallel Resonance  Important Parameters  Resonance Frequency, o  Half-power frequencies, 1 and 2  Bandwidth,   Quality Factor, Q  Application
  • 4.
    Introduction  Resonance isa condition in an RLC circuit in which the capacitive and reactive reactance are equal in magnitude, thereby resulting in a purely resistive impedance.  Resonance circuits are useful for constructing filters and used in many application.
  • 5.
  • 6.
    At Resonance  Atresonance, the impedance consists only resistive component R.  The value of current will be maximum since the total impedance is minimum.  The voltage and current are in phase.  Maximum power occurs at resonance since the power factor is unity.
  • 7.
    Series Resonance CLTotal jX-jXRZ R V Z V I m Total s m  Total impedance of series RLC Circuit is At resonance The impedance now reduce to CL XX  RZTotal  )X-j(XRZ CLTotal  The current at resonance
  • 8.
    Resonance Frequency Resonance frequencyis the frequency where the condition of resonance occur. Also known as center frequency. Resonance frequency rad/s LC 1 ωo  Hz LC2 1  of
  • 9.
    Half-power Frequency rad/s LC 1 2L R 2L R ω 2 2             rad/s LC 1 2L R 2L R ω 2 1               Half-power frequencies is the frequency when the magnitude of the output voltage or current is decrease by the factor of 1 / 2 from its maximum value. Also known as cutoff frequencies.
  • 10.
    Bandwidth,  rad/s)( 12cc ωωβ  rad/s L R β  Bandwidth,  is define as the difference between the two half power frequencies. The width of the response curve is determine by the bandwidth.
  • 11.
  • 12.
  • 13.
    Quality Factor (Q-Factor) Theratio of resonance frequency to the bandwidth The “sharpness” of response curve could be measured by the quality factor, Q. R L Q oo    
  • 14.
    Q-Factor Vs Bandwidth Higher value of Q, smaller the bandwidth. (Higher the selectivity)  Lower value of Q larger the bandwidth. (Lower the selectivity)
  • 15.
  • 16.
    Parallel Resonance The totaladmittance ωL ωC 1  Resonance occur when )ωω L1/Cj( R 1 YTotal  321Total YYYY  C)(-j/ 1 L)(j 1 R 1 YTotal   Cj ωL j- R 1 YTotal ω
  • 17.
    At Resonance  Atresonance, the impedance consists only conductance G.  The value of current will be minimum since the total admittance is minimum.  The voltage and current are in phase.
  • 18.
    Parameters in ParallelCircuit rad/s LC 1 2RC 1 2RC 1 ω 2 1                Parallel resonant circuit has same parameters as the series resonant circuit. rad/s LC 1 ωo  rad/s LC 1 2RC 1 2RC 1 ω 2 2              Resonance frequency Half-power frequencies
  • 19.
    Parameters in ParallelCircuit RC β ω Q o o  RC 1 12  ωωβ Bandwidth Quality Factor