CH 4FullwaveandThreephaserectifiers ConvertingACtoDC 4 1Introduction u u TheaveragecurrentinACsourceiszero

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CH. 4 Full-wave and Threephase rectifiers  (Converting AC to DC) 4 -1 Introduction u u The average current in AC source is zero  in the  full-wave rectifier, thus avoiding  problems  associated with nonzero average  source currents,

CH. 4 Full-wave and Threephase rectifiers  (Converting AC to DC) 4 -1 Introduction u u The average current in AC source is zero  in the  full-wave rectifier, thus avoiding  problems  associated with nonzero average  source currents, particularly in transformers.

4 -2 Single-phase full-wave rectifiers Fig.  4 -1 Bridge rectifier:    The lower peak diode voltage make it more suitable  for high-voltage applications.

4 -2 Single-phase full-wave rectifiers Fig.  4 -1 Bridge rectifier:    The lower peak diode voltage make it more suitable  for high-voltage applications.

Fig.  4 -2 center-tapped transformer  rectifier    With electrical isolation,  only  one diode voltage drop between  the source and load, suitable for  low-voltage, high-current applications

Fig.  4 -2 center-tapped transformer  rectifier    With electrical isolation,  only  one diode voltage drop between  the source and load, suitable for  low-voltage, high-current applications

Resistive load:      power absorbed by the load resistor:   power factor :Pf=1  

Resistive load:      power absorbed by the load resistor:   power factor :Pf=1  

R-L load: Fig. 4 -3

R-L load: Fig. 4 -3

      If L is relatively large, the load current is essentially  dc. ( )   Source harmonics are rich in the odd-numbered harmonics. Filters:reducing the harmonics.

      If L is relatively large, the load current is essentially  dc. ( )   Source harmonics are rich in the odd-numbered harmonics. Filters:reducing the harmonics.

R-L source load: Fig. 4 -5

R-L source load: Fig. 4 -5

 For continuous current operation, the only modification to  the analysis that was done for R-L load is in the  dc term of the Fourier series. The dc component of current in this circuit is.   The sinusoidal terms in the Fourier analysis  are unchanged by the dc source, provided  that the current is continuous.    Discontinuous current is analyzed like 

 For continuous current operation, the only modification to  the analysis that was done for R-L load is in the  dc term of the Fourier series. The dc component of current in this circuit is.   The sinusoidal terms in the Fourier analysis  are unchanged by the dc source, provided  that the current is continuous.    Discontinuous current is analyzed like  section 3 -5.  

 Capacitance output filter: Fig.  4 -6

 Capacitance output filter: Fig.  4 -6

Assuming ideal diodes :the angle where the diodes become reverse  biased, which is the same as for the half-wave  rectifier  and is   =?   solved numerically for   Peak-to-peak variation(ripple):  

Assuming ideal diodes :the angle where the diodes become reverse  biased, which is the same as for the half-wave  rectifier  and is   =?   solved numerically for   Peak-to-peak variation(ripple):  

In practical circuits where ωRC   ,      minimal output voltage occurs at     is half that of the half-wave rectifier.

In practical circuits where ωRC   ,      minimal output voltage occurs at     is half that of the half-wave rectifier.

Fig. 4 -7 (a) Voltage doubler Fig. 4 -7 (b) Dual voltage rectifier      =full-wave rectifier(sw.  open)+       voltage doubler(sw.  closed)

Fig. 4 -7 (a) Voltage doubler Fig. 4 -7 (b) Dual voltage rectifier      =full-wave rectifier(sw.  open)+       voltage doubler(sw.  closed)

L-C filtered output: Fig. 4 -8   C holds the output voltage at a constant level, and the L  smoothes the current from rectifier and reduces the peak  current in diodes.

L-C filtered output: Fig. 4 -8   C holds the output voltage at a constant level, and the L  smoothes the current from rectifier and reduces the peak  current in diodes.

=0 , full-wave rectified Continuous  Current:    The variation in    can be estimate from the first  Ac term (n=2)  in the Fourier series.  The amplitude of the inductor current for n=2 is  

=0 , full-wave rectified Continuous  Current:    The variation in    can be estimate from the first  Ac term (n=2)  in the Fourier series.  The amplitude of the inductor current for n=2 is    where   For Continuous current,      

Discontinuous current:    , When  is positive (   at )

Discontinuous current:    , When  is positive (   at )

 Procedure for determining Vo: (1) Estimate a Value for Vo slightly below Vm, and solve    (2) Solve  numerically, (3) Solve    (4) Slove Vo= (5) Repeat step (1)~(4)

 Procedure for determining Vo: (1) Estimate a Value for Vo slightly below Vm, and solve    (2) Solve  numerically, (3) Solve    (4) Slove Vo= (5) Repeat step (1)~(4)  until the computed Vo in step(4)   equals the estimated Vo in step(1) Output Voltage for discontinuous current is larger than  for continuous current. (see Fig 4 -8(d))

4 -3 controlled full-wave rectifiers Resistive load:  Fig. 4 -10

4 -3 controlled full-wave rectifiers Resistive load:  Fig. 4 -10

           The power delivered to the load  The rms current in source is the same as the rms current in  the load.

           The power delivered to the load  The rms current in source is the same as the rms current in  the load.

R-L load : Fig. 4 -11

R-L load : Fig. 4 -11

discontinuous current :       for    For discontinuous current      Analysis of the controlled full-wave rectifier operating in the  discontinuous current mode is identical to that of the controlled  half-wave rectifier, except that the period for the output current  is .

discontinuous current :       for    For discontinuous current      Analysis of the controlled full-wave rectifier operating in the  discontinuous current mode is identical to that of the controlled  half-wave rectifier, except that the period for the output current  is .

continuous current

continuous current

 Fig 4 -12

 Fig 4 -12

R-L Source load : Fig. 4 -14  The SCRS may be turned on at any time that they are forward  biased, which is at an angle   

R-L Source load : Fig. 4 -14  The SCRS may be turned on at any time that they are forward  biased, which is at an angle   

  For continuous current case,        the average bridge output voltage is average load current is   The ac voltage terms are unchanged from the controlled rectifier  with an R-L load.  The ac current terms are determined from  circuit.  Power absorbed by the dc voltage is      Power absorbed by resistor in the load is

  For continuous current case,        the average bridge output voltage is average load current is   The ac voltage terms are unchanged from the controlled rectifier  with an R-L load.  The ac current terms are determined from  circuit.  Power absorbed by the dc voltage is      Power absorbed by resistor in the load is

Controlled Single-phase converter operating as an inverter: seeing  Fig 4 -14.  4 -15  .  

Controlled Single-phase converter operating as an inverter: seeing  Fig 4 -14.  4 -15  .  

For inverter operation, power is supplied by the dc source, and power is absorbed by the bridge and is transferred to  the ac system.   Vdc and Vo must be negative            rectifier operation      inverter operation  

For inverter operation, power is supplied by the dc source, and power is absorbed by the bridge and is transferred to  the ac system.   Vdc and Vo must be negative            rectifier operation      inverter operation  

4 -4 Three-phase rectifiers Resistive load : Fig 4 -16  

4 -4 Three-phase rectifiers Resistive load : Fig 4 -16  

 上、下半部Diode,每次僅一個ON;同相上、下Diode不可同時ON; Diode ON由瞬間最大線電壓決定。  A transition of the highest line-to-line voltage must take place  every .  Because of the six transitions that occur for each period  of the source voltage, the circuit is called a six-pulse  rectifier.  vo(t)之基頻為 3  Diode 電源頻率之6倍 turn on in the sequence 1, 2,

 上、下半部Diode,每次僅一個ON;同相上、下Diode不可同時ON; Diode ON由瞬間最大線電壓決定。  A transition of the highest line-to-line voltage must take place  every .  Because of the six transitions that occur for each period  of the source voltage, the circuit is called a six-pulse  rectifier.  vo(t)之基頻為 3  Diode 電源頻率之6倍 turn on in the sequence 1, 2, 3, 4, 5, 6, 1, . .

 Each diode conducts one-third of the time, resulting in        Apparent power from the three-phase source is

 Each diode conducts one-third of the time, resulting in        Apparent power from the three-phase source is

Since the output voltage is periodic with period 1/6 of the ac supply voltage, the harmonics in the output are of order 6 kω, k=1, 2, 3, … Adevantage:output is inherently like a dc voltage, and the highfrequency low-amplitude harmonics enable filters to be effective.

Since the output voltage is periodic with period 1/6 of the ac supply voltage, the harmonics in the output are of order 6 kω, k=1, 2, 3, … Adevantage:output is inherently like a dc voltage, and the highfrequency low-amplitude harmonics enable filters to be effective.

 For a dc load current (constant I 0) --- Fig 4. 17

 For a dc load current (constant I 0) --- Fig 4. 17

which consists of terms at fundamental frequency of the ac  1, k=1, 2, 3, … system and harmonics of order 6 k  Filters(Fig. 4 -18)  are frequently necessary to prevent harmonic  currents to enter the ac system.

which consists of terms at fundamental frequency of the ac  1, k=1, 2, 3, … system and harmonics of order 6 k  Filters(Fig. 4 -18)  are frequently necessary to prevent harmonic  currents to enter the ac system.  Resonant filters for 5 th and 7 th harmonics.  High-pass filters for higher order harmonics.

4 -5 Controlled three-phase rectifiers

4 -5 Controlled three-phase rectifiers

 Harmonics for output voltage remain of order 6 k,  functions of .   seeing  Fig. 4 -20 but amplitude are

 Harmonics for output voltage remain of order 6 k,  functions of .   seeing  Fig. 4 -20 but amplitude are

 Twelve-pulse rectifiers:using two six-pulse bridges

 Twelve-pulse rectifiers:using two six-pulse bridges

 The purpose of the   transformer connection is to introduce phase  shift between the source and bridge. This results in inputs to two bridges which are   apart. The two bridge outputs are similar, but also shifted by .  The delay angles for the bridge are typically the same.       The peak output of the twelve-pulse converter occurs midway 

 The purpose of the   transformer connection is to introduce phase  shift between the source and bridge. This results in inputs to two bridges which are   apart. The two bridge outputs are similar, but also shifted by .  The delay angles for the bridge are typically the same.       The peak output of the twelve-pulse converter occurs midway  between alternate peaks of the six-pulse converters.  Adding the  voltages at that point for gives 

 Since a transition between conducting SCRs every  , there a total of 12 such transitions for each period of the  ac source.  The output has harmonic frequencies which are  multiple of 12 times the source fre. (12 k  k=1, 2, …) Cancellation of harmonics 6(2

 Since a transition between conducting SCRs every  , there a total of 12 such transitions for each period of the  ac source.  The output has harmonic frequencies which are  multiple of 12 times the source fre. (12 k  k=1, 2, …) Cancellation of harmonics 6(2 n-1) 1 , n=1, 2, … has resulted from this transformer and converter configuration.

 This principle can be expanded to arrangements of higher pulse  number by incorporating increased number of six-pulse converters  with transformers which have the appropriate phase shifts.  The characteristic ac harmonics of a p-pulse converter will be  pk 1  ,  k=1, 2, 3…  More expense for producing high-voltage transformers with the  appropriate phase shifts.

 This principle can be expanded to arrangements of higher pulse  number by incorporating increased number of six-pulse converters  with transformers which have the appropriate phase shifts.  The characteristic ac harmonics of a p-pulse converter will be  pk 1  ,  k=1, 2, 3…  More expense for producing high-voltage transformers with the  appropriate phase shifts.

Three-phase converter operating as a inverter:  seeing 4 -22.  

Three-phase converter operating as a inverter:  seeing 4 -22.  

 The bridge output voltage Vo must be negative.

 The bridge output voltage Vo must be negative.

4 -6 DC power transmission ․ By using controlled twelve-pulse converter (generally). ․ Used for very long distances of transmission lines. Advantages:(1)   ,  voltage drop↓ in lines ) (2)  

4 -6 DC power transmission ․ By using controlled twelve-pulse converter (generally). ․ Used for very long distances of transmission lines. Advantages:(1)   ,  voltage drop↓ in lines ) (2)   ,  line loss  ( (3) Two conductors required rather than three (4) Transmission towers are smaller. (5 ) Power flow in a dc transmission line is controllable  by adjustment of delay angles at the terminals. (6) Power flow can be modulated during disturbances on     one of the ac system.  System stability increased. (7) The two ac systems that are connected by the dc  line  do not need to be in synchronization. Disadvantages:costly ac-dc converter, filter, and control system  required at each end of the line to interface  with the ac system.

Fig. 4 -23  using six-pulse converter

Fig. 4 -23  using six-pulse converter

For current being ripple free    Power supplied by the converter at terminal 1 is   Power supplied by the converter at terminal 2 is 

For current being ripple free    Power supplied by the converter at terminal 1 is   Power supplied by the converter at terminal 2 is 

Fig. 4 -24  using twelve-pulse converter        (a bipolar scheme)

Fig. 4 -24  using twelve-pulse converter        (a bipolar scheme)

 One of the lines is energized at   and the other is energized  at. In emergency situations, one pole of the line can operate  without the other pole, with current returning through the ground  path.

 One of the lines is energized at   and the other is energized  at. In emergency situations, one pole of the line can operate  without the other pole, with current returning through the ground  path.

4 -7 commutation :effect of source inductance (   Single-phase bridge  rectifier: Fig. 4 -25 )

4 -7 commutation :effect of source inductance (   Single-phase bridge  rectifier: Fig. 4 -25 )

 Assume that the load current is constant Io. Commutation interval starts at ωt= Commutation is completed at ωt=    => Commutation angle: +u

 Assume that the load current is constant Io. Commutation interval starts at ωt= Commutation is completed at ωt=    => Commutation angle: +u

 Average load voltage is   Source inductance lowers the average output voltage of full- wave rectifier.

 Average load voltage is   Source inductance lowers the average output voltage of full- wave rectifier.

Three-phase rectifier:  Fig. 4 -26

Three-phase rectifier:  Fig. 4 -26

 During Commutation from   is , The voltage across La  Current in  starts at I 0 and decreases zero in the   commutation interval

 During Commutation from   is , The voltage across La  Current in  starts at I 0 and decreases zero in the   commutation interval

 During the commutation interval from  output voltage is  ,  the converter   Average output Voltage:  類似 Single-phase rectifier  Source inductance lowers the average output voltage of three- phase rectifiers.

 During the commutation interval from  output voltage is  ,  the converter   Average output Voltage:  類似 Single-phase rectifier  Source inductance lowers the average output voltage of three- phase rectifiers.