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Physics Helpline
L K Satapathy
Alternating Current Theory 5
Resonance in LCR Series Circuit
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
Resonance in LCR series circuit
2
2
. . . (1)
1
o o
o
E E
i
Z
R L
C


 
 
  
 
Current amplitude & voltage amplitude are related as
1 1
0o o
o
L
C LC
 

   
. . . (2)m o
o
E
i
R
 Maximum current amplitude is
It is maximum when frequency of AC
such that
o 
[Derived in AC Theory 4]
The variation of Io with  is shown in the figure
Each curve corresponds to a particular value of R
We observe that the value of decreases as R increasesm
oi

oi
o
1R
2R
3R
 1 2 3R R R 
1( )m
oi
2( )m
oi
3( )m
oi
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
Let current amplitude for some value of  be
. . . (3)
2 2
m
o o
o
i E
i
R
 
 Power of the circuit becomes half the maximum power
We have two such frequencies symmetric about1 2&  o
1
2&
o
o
where   
  
  
  
 Half power band width 1 2 2    
oi
m
oi
12
m
oi
2
2 
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
1 2
2
1
1
, . . . (4)
1
o
o
E
For i
R L
C
 


 
 
  
 
2
2
1
1
(3) & (4)
21
o oE E
R
R L
C


 
 
  
 
2
2
1
1
1
2R L R
C


 
    
 
2
2 2
1
1
1
2R L R
C


 
    
 
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
2
2
1
1
1
L R
C


 
   
 
1
1
1
L R
C


  
1
( )
( )
o
o
L R
C
 
 
    
 
1
1
1
o
o
o
o
L R
C


 


 
    
    
 
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
1
1
o
o
o
o
L
L R


 

 
    
    
 
1
o
o
L
C


 
 
 

1
1 1o o
o o
L L R
 
 
 

    
       
   
1 1o o
o o
L L R
 
 
 
    
       
   
1
o





 
 
2
o
o
L R




  
2 [ ]Bandwid
R
L
th  
Physics Helpline
L K Satapathy
Cells in Parallel
Alternating Current Theory 5
1
2
o o
o
L
Q
R CR
 
 
  

We define Quality factor
 When the value of Q is larger
Band width 2 is smaller
Resonance is sharper
The circuit will be more selective
2 o
Q

  
This phenomenon is used in Radio Tuners
Physics Helpline
L K Satapathy
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www.physics-helpline.com
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Alternating Current Theory 5/ Resonance

  • 1. Physics Helpline L K Satapathy Alternating Current Theory 5 Resonance in LCR Series Circuit
  • 2. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 Resonance in LCR series circuit 2 2 . . . (1) 1 o o o E E i Z R L C            Current amplitude & voltage amplitude are related as 1 1 0o o o L C LC        . . . (2)m o o E i R  Maximum current amplitude is It is maximum when frequency of AC such that o  [Derived in AC Theory 4] The variation of Io with  is shown in the figure Each curve corresponds to a particular value of R We observe that the value of decreases as R increasesm oi  oi o 1R 2R 3R  1 2 3R R R  1( )m oi 2( )m oi 3( )m oi
  • 3. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 Let current amplitude for some value of  be . . . (3) 2 2 m o o o i E i R    Power of the circuit becomes half the maximum power We have two such frequencies symmetric about1 2&  o 1 2& o o where              Half power band width 1 2 2     oi m oi 12 m oi 2 2 
  • 4. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 1 2 2 1 1 , . . . (4) 1 o o E For i R L C              2 2 1 1 (3) & (4) 21 o oE E R R L C            2 2 1 1 1 2R L R C            2 2 2 1 1 1 2R L R C           
  • 5. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 2 2 1 1 1 L R C           1 1 1 L R C      1 ( ) ( ) o o L R C            1 1 1 o o o o L R C                    
  • 6. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 1 1 o o o o L L R                    1 o o L C          1 1 1o o o o L L R                         1 1o o o o L L R                        1 o          2 o o L R        2 [ ]Bandwid R L th  
  • 7. Physics Helpline L K Satapathy Cells in Parallel Alternating Current Theory 5 1 2 o o o L Q R CR         We define Quality factor  When the value of Q is larger Band width 2 is smaller Resonance is sharper The circuit will be more selective 2 o Q     This phenomenon is used in Radio Tuners
  • 8. Physics Helpline L K Satapathy For More details: www.physics-helpline.com Subscribe our channel: youtube.com/physics-helpline Follow us on Facebook and Twitter: facebook.com/physics-helpline twitter.com/physics-helpline