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Page 1: (22) Unit -II Rectifiers, Filters and Regulators Introduction _ Bikila Chalchisa - Academia

2/2/2015 (22) UNIT ­II RECTIFIERS, FILTERS AND REGULATORS Introduction | Bikila Chalchisa ­ Academia.edu

https://www.academia.edu/6317554/UNIT_­II_RECTIFIERS_FILTERS_AND_REGULATORS_Introduction 1/51

UNIT -II RECTIFIERS, FILTERS AND REGULATORS Introduction

22 Home Analytics Upload Papers Rodrigo Search...

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Page 3: (22) Unit -II Rectifiers, Filters and Regulators Introduction _ Bikila Chalchisa - Academia

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Department of Electronics and Communication Engineering  UNIT-III -EDC

___________________________________________________________________________

12 22

0

1( )

2rmsV V d t  

π 

ω 

π 

=

∫  rms rms

  L

V I R=   ×  

3. Ripple Factor ( )γ   : It is defined as ration of R.M.S. value of a.c. component to the d.c.

component in the output is known as “Ripple Factor”.

'rms

dc

V V 

γ   =  

W here

2 2'rms   dcrmsV    V V =   −  

2

1rms

dc

V V 

γ   

−∴ =  

4. Efficiency ( )η  : It is the ratio of d.c output power to the a.c. input power. It

signifies, how efficiently the rectifier circuit converts a.c. power into d.c. power.

It is given bydc

ac

P

Pη  =  

5. Peak Inverse Voltage (PIV): It is defined  as the maximum reverse voltage that adiode can withstand without destroying the junction.

6. Regulation: The variation of the d.c. output voltage as a function of d.c. load current iscalled regulation. The percentage regulation is defined as

% Regulation = 100%no load full load  

 full load 

V V 

V − −

×  

For an ideal power supply, % Regulation is zero.

Using one or more diodes in the circuit, following rectifier circuits can be designed.

1.  Half - Wave Rectifier2.  Full – Wave Rectifier3.  Bridge Rectifier

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99

3.  Bridge Rectifier

HALF-WAVE RECTIFIER:

A Half – wave rectifier is one which converts a.c. voltage into a pulsating voltage using onlyone half cycle of the applied a.c. voltage. The basic half-wave diode rectifier circuit along with itsinput and output waveforms is shown in figure below.

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Department of Electronics and Communication Engineering  UNIT-III -EDC

___________________________________________________________________________

The half-wave rectifier circuit shown in above figure consists of a resistive load; a rectifyingelement i.e., p-n junction diode and the source of a.c. voltage, all connected is series. The a.c.voltage is applied to the rectifier circuit using step-down transformer.

The input to the rectifier circuit, m sinV V t ω =   Where Vm is the peak value of secondary a.c.

voltage

Operation:

For the positive half-cycle of input a.c. voltage, the diode D is forward biased and hence itconducts. Now a current flows in the circuit and there is a voltage drop across RL. The waveformof the diode current (or) load current is shown in figure.

For the negative half-cycle of input, the diode D is reverse biased and hence it does notconduct. Now no current flows in the circuit i.e., i=0 and Vo=0. Thus for the negative half-cycle

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100

conduct. Now no current flows in the circuit i.e., i=0 and Vo=0. Thus for the negative half-cycleno power is delivered to the load.

Analysis:

In the analysis of a HWR, the following parameters are to be analyzed.

i) DC output current ii) DC Output voltageiii) R.M.S. Current iv) R.M.S. voltage

v) Rectifier Efficiency ( )η    vi) Ripple factor ( )γ    

vii) Regulation viii) Transformer Utilization Factor (TUF)ix) Peak Factor (P)

Let a sinusoidal voltage Vi be applied to the input of the rectifier.

Then m sinV V t ω =   Where Vm is the maximum value of the secondary voltage.

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Department of Electronics and Communication Engineering  UNIT-III -EDC

___________________________________________________________________________

Let the diode be idealized to piece-wise linear approximation with resistance Rf   in the

forward direction i.e., in the ON state and Rr (=∞) in the reverse direction i.e., in the OFF state.

Now the current ‘i’ in the diode (or) in the load resistance RL is given by

mI sini t ω =   for 0   t ω π ≤ ≤  

i=0 for 2t π ω π ≤ ≤  

where mI  m

 L f 

 R R=

i) Average (or) DC Output Current (Iav or Idc):

The average dc current Idc is given by

dc I   

2

0

1 ( )

2

  id t π 

ω 

π 

= ∫  

m

2

0

sin ( )1

0 ( )2I   td t    d t 

π 

π 

π 

ω ω    ω π 

= ×+ ∫∫  

m 01 I ( cos )2

  t   π ω π 

= −  

m1 I ( 1 ( 1))2π 

= + − −  

mI

π 

=   ,  = 0.318 mI  

Substituting the value of mI , we get

( )I

 L f 

mdc  R R

π    +=  

V  V 

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 ��������� ������� �� ������������ ����������� ��������� 

101

If RL>>Rf then I   mdc

 L

 Rπ =  = 0.318

m

 L

 R 

ii) Average (or) DC Output Voltage (Vav or Vdc):

The average dc voltage is given by

 Ldc dcV I R=   ×  =

mI L R

π   ×   =

( ) L f 

m   L

 R R

V R

π    + 

(   ) L f 

m   Ldc  R R

V RV π    +⇒   =  

If RL>>Rf thenm

dc

V V 

π =  = 0.318 mI  

mdc

V V 

π ∴ =  

iii) R.M.S. Output Current (Irms):

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Department of Electronics and Communication Engineering  UNIT-III -EDC

___________________________________________________________________________

The value of the R.M.S. current is given by

rms I   

21

22

0

1 ( )2

  i d t π 

ω π 

= ∫  

1

2

222

0

sin ( )1

0 ( )2

1I2

.m

  t d t    d t π 

π 

π 

ω ω    ω π    π 

  • •

=   + ∫∫  

1

22

0

1 cos( )

2

I

2m   t 

d t π 

ω ω 

π 

−= ∫  

122

0

I 1( ) sin4 2

m t t 

π 

ω ω π 

−=  

12 2

sin0I sin20

4 2m   π π π 

+− −=  

12 2I

4m

=  

mI2

=  

mI2rms I    =∴  (or)

(   )2mrms

 R RV  I 

+=  

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Report Work

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 ��������� ������� �� ������������ ����������� ��������� 

102

I2 I (   )2  L f  R R

V  I +

iv) R.M.S. Output Voltage (Vrms):

R.M.S. voltage across the load is given by

rms rms   LV I R=   ×  =

( )2  L f 

m   L

 R R

V R

+  =

2 1   f 

 L

m

 R

 R

+

 

If RL >> Rf   then2m

rmsV 

V    =  

v) Rectifier efficiency( )η  :

The rectifier efficiency is defined as the ration of d.c. output power to the a.c. input power i.e.,

dc

ac

P

Pη ∴ =  

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Department of Electronics and Communication Engineering  UNIT-III -EDC

___________________________________________________________________________

2

22

m   L Ldcdc  I R I RP

π = =  

(   )   (   )2

2

4rms

m

 L L f f ac I 

 I R R R RP   = + = +  

(   )

2

2 22

4 4m

m

 L   L

 L   f  L   f 

dc

ac

 R   R

 R R R R

P   I 

P  I π π η 

=

× =++

∴ =  

2

1 0.406

11

4

 f  f 

 L L

 R R

 R R

π η    ×

++

=⇒   =  

%40.6

1   f 

 L

 R

 R

η +

⇒   =  

Theoretically the maximum value of rectifier efficiency of a half-wave rectifier is 40.6%

when f 

 L

 R

 R= 0.

vi) Ripple Factor ( )γ   :

γ  

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 ��������� ������� �� ������������ ����������� ��������� 

103

The ripple factor γ   is given by

2

1rms

dc

 I  I 

γ   

−=   (or) 

2

1rms

dc

V V 

γ   

−=  

22

 / 

 / 1m

m

 I  I    π 

γ   

−∴ =   =

2

12π 

−   = 1.21

1.21γ  ⇒   =  

vii) Regulation:

The variation of d.c. output voltage as a function of d.c. load current is called regulation.

The variation of Vdc with Idc for a half-wave rectifier is obtained as follows:

mI / I   m

dc L f 

V  R R

π π 

  =+

=  

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___________________________________________________________________________

But Ldc dc

V I R=   ×  

dcV   

m   L

 L f 

 RV  R Rπ 

=+

  1  f m

 L f 

 RV  R Rπ 

= −+

 

dc f m  R

V  I 

π =   −  

dc dc f  mV R

V  I 

π ∴ =   −  

This result shows that Vdc equalsmV 

π  at no load and that the dc voltage decreases linearly

with an increase in dc output current. The larger the magnitude of the diode forward resistance,the greater is this decrease for a given current change.

viii) Transformer Utilization Factor (UTF):

The d.c. power to be delivered to the load in a rectifier circuit decides the rating of thetransformer used in the circuit. So, transformer utilization factor is defined as

( )

dc

ac rated 

PTUF 

P∴ =  

The factor which indicates how much is the utilization of the transformer in the circuit is calledTransformer Utilization Factor (TUF).

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 ��������� ������� �� ������������ ����������� ��������� 

104

Transformer Utilization Factor (TUF).

The a.c. power rating of transformer = Vrms Irms 

The secondary voltage is purely sinusoidal hence its rms value is 12

  times maximum while the

current is half sinusoidal hence its rms value is1

2 of the maximum.

( )ac rated P∴  

mI

22mV 

= ×  mI

2 2mV 

=  

The d.c. power delivered to the load2

dc   L I R=  

m

2I

 L R

π 

=  

( )

dc

ac rated 

PTUF 

P

∴ =  

m

2I

 L R

π 

=m

2 2ImV 

=  

2

2

2

2 2I

Im

m

 L

 L

 R

 Rπ    •

• •

=   (   )mIm   LV R≈Q  

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