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    Single-Phase ControlledRectifiers

    JM610

    Electrical Engineering Department

    Kota Bharu Polytechnic

    Mohd Azlan bin Ashari

    1

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    SINGLE PHASE

    CONTROLLED RECTIFIER

    1. HALFWAVE CONTROLLED

    RECTIFIER

    2. FULLWAVE HALFCONTROLLED

    RECTIFIER

    3. FULLWAVE FULLY CONTROLLEDRECTIFIER

    2

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    Normal rectifiers are considered as uncontrolledrectifiers.

    Once the source and load parameters are

    established, the dc level of the output and power

    transferred to the load are fixed quantities.

    A way to control the output is to use SCR instead of

    diode. Two condition must be met before SCR can

    conduct: The SCR must be forward biased (VSCR>0)

    Current must be applied to the gate of SCR

    The Half-wave Controlled Rectifier

    3

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    The simplest controlled rectifier uses a single device, such as a

    thyristor, to produce variable voltage d.c. from fixed voltage a.c.

    mains. The circuit arrangement is shown below

    4

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    The thyristor is turned on in the positivehalf-cycle, some time after supply voltage

    zero, by the application of a gate pulse

    with delay angle a. In the negative half-

    cycle, the thyristor is reverse biased and

    cannot switch on. The larger the delay

    angle, the smaller is the average load

    voltage.

    5

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    Voltage waveforms

    for two delay angles are shown below

    6

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    Controlled, Half-wave R load

    ]cos1[

    2

    )sin(2

    1

    ,""

    a

    a

    s

    mDCaveo

    V

    tdtVVVV

    voltageoutputDCAverage

    a

    a

    2

    )2sin(1

    2

    )()]sin([2

    1,

    resistor,byabsorbedpowerAverage

    0

    2

    ,

    22

    m

    mrmso

    rms

    V

    tdtVVwhere

    R

    VRIP rms

    A gate signal isapplied at t = a,

    where a is the

    delay/firing angle.

    R

    V

    R

    VI srms

    o

    rmso 2

    ,

    ,

    m

    7

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    Example

    Design a circuit to produce an average voltage

    of 40V across 100 load resistor from a 120Vrms

    60 Hz ac source. Determine the power absorbed

    by the resistor and the power factor.

    Briefly describe what happen if the circuit is

    replaced by diode to produce the same average

    output.

    8

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    Example (Cont) Solution

    rad

    VV

    o

    s

    o

    07.12.61

    ]cos1[2

    212040

    ]cos1[2

    a

    a

    a

    In such that to achieved 40Vaverage voltage, the delay angle

    must be

    If an uncontrolled diode is used,

    the average voltage would be

    That means, some reducing

    average resistor to the design mustbe made.A series resistor or

    inductor could be added to an

    uncontrolled rectifier, while

    controlled rectifier has advantage

    of not altering the load or

    introducing the losses

    V

    VV m

    rmso

    6.75

    2

    )07.1(2sin07.11

    2

    2120

    2

    )2sin(1

    2,

    a

    a

    WR

    V

    P

    rms

    1.57100

    6.75 22

    63.0

    100

    6.75)120(

    1.57

    pf

    VV

    V so 54)120(2

    m

    m

    9

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    Half - Wave Controlled

    Rectifier Circuit with an RLLoad

    10

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    Figure 1 : Half-wave controlled

    Rectifier with RL Load

    11

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    Let vs(t) be Vm sin (t). At t =

    0, the current through the

    circuit is zero. As t becomes >0, vs becomes positive. If a

    diode instead of an SCR has

    been used, the diode would

    start conduction at t = 0. With

    an SCR, the conduction doesnot start till the SCR is

    triggered. Let the SCR be

    triggered when t = a. Then a

    is called the firing angle and

    the SCR continues to conduct.

    When t = , the source

    becomes zero, but at this instant,

    the current through the circuit is

    not zero and there is some

    energy stored in the inductor.

    When vs becomes negative, the

    current through the circuit would

    not become zero suddenly

    because of the inductor. The

    inductor acts as a source andkeeps the SCR forward-biased till

    the energy stored in the inductor

    becomes zero. Let the current

    through the circuit become zero

    at t = b and the value ofb > .Forb < t < 2, the current

    through the circuit is zero

    12

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    With an Inductive (RL) Load

    13

    13

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    14

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    15

    With I nductive Load and

    Freewheeling Diode

    15

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    FULL-WAVE HALF-CONTROLLED BRIDGE

    RECTIFIER WITH RESISTIVE LOAD

    The half-controlled is the easiest to implement since the two thyristors

    can be arranged to have a common cathode.

    The firing circuit can have a common train of pulses and only the

    forward-biased device will switch on at the arrival of a pulse on the two

    gates.

    Figure 1 : Circuit Diagram16

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    In the positive half-cycle, T1 is turned on at delay anglea, and current flows to the load through the path T1, load

    and D1. The supply voltage then passes through zeroand reverses; since the load is resistive, T1 and D1

    would turn-off.

    Figure 2 : The flow of load current during +ve half cycle

    17

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    At delay angle + a, T2 is fired, and load current flowsthrough T2, load and D2. Once again, the supply voltagepasses through zero, and T2 and D2 would turn-off

    Figure 3 : The flowing of load current during ve half cycle

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    Figure 4 : The input and output waveforms

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    Average load voltage (V av)

    The average load voltage is found by calculating the area under the

    voltage curve and then dividing by the length of the base. For any delay

    angle a, the average load voltage is given by

    20

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    In the circuit in Fig. 1, the load is replaced by a large inductance.The assumption is that the load inductance is high enough to causecontinuous steady load current.

    .

    HALF-CONTROLLED BRIDGE WITH

    HIGHLY INDUCTIVE LOAD

    Inductive

    load

    Figure 5 : Half-controlled bridge rectifier with inductive load

    21

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    Operation:

    In the positive half-cycle, T1 is turned on at delay angle a, andcurrent flows to the load through the path T1, load and D1. Thesupply voltage passes through zero and reverses; if this was aresistive load T1 would turn-off. However, due to the inductivestored energy, the load voltage reverses in order to keep the loadcurrent flowing, D2 is forward-biased and conducts, and clamps thebottom of the load to virtually zero voltage. Energy stored in the loadinductance keeps load current flowing through the path of D2, T1and the load until T2 is fired at t = ( a + )

    The flow of load current

    during ( a < t < )

    The flow of load current

    during ( < t < a ) 22

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    At delay angle + a, T2 is fired, T1 is reverse-biased and turns off,and load current flows through T2, load and D2. Once again, thesupply voltage passes through zero, and load inductive energyforward biases D1 to keep load current flowing. T1 is then fired, T2turns off and the cycle is repeated.

    .

    The flow of load current during ( a) < t < 2

    The flow of load current during 2 < t < ( 2 a)

    23

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    Input supply

    Load voltage

    Load current

    Input current

    Current flow due

    to inductive load

    Figure 6 : Waveforms 24

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    Average load voltage

    A full-wave half-controlled bridge has a supply voltage of 220V at 50Hz. The

    firing angle delay a = 90o . Determine the values of average and rms

    currents load power and power factor for a resistive load of R = 100,

    Example :

    25

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    HALF-CONTROLLED BRIDGE WITH FLYWHEEL

    DIODE AND INDUCTIVE LOAD

    Although the half-controlled bridge has a fly-wheel diode action built in, it

    uses one of the thyristors in the fly-wheeling path. If a third diode isused, connected directly across the inductive load, then when the load

    voltage attempts to reverse, this diode is forward-biased and the

    inductive stored energy circulates the load current in the closed path of

    the load and third diode

    Figure 7 : circuit diagram

    26

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    The advantage of this method is that at mains voltage zero the conducting

    thyristor turns off instead of hanging on for fly-wheel diode action, and thisreduces the thyristor duty cycle.

    The circuit arrangement shown in figure 7 and resulting waveforms are shown

    in Figure 7b. It is clear from observation of the waveforms that values of

    average and rms voltage and current are unaffected by the addition of the third

    diode.

    27

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    Input supply

    Load voltage

    Load current

    Input current

    Current flow due

    to inductive load

    Figure 7b : Waveforms 28

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    FULL-WAVE FULLY CONTROLLED BRIDGE

    WITH RESISTIVE LOAD

    During the positive half-cycle, T1 and T3 are turned on simultaneously at the delay

    angle ofa, and current flows to the load through the path T1, load and T3. The

    supply voltage then passes through zero and reverses; since the load is resistive,

    T1 and T3 would turn-off.

    At delay angle of ( + a), T2 and T4 are fired simultaneously, and load current

    flows through T2, load and T4. Once again, the supply voltage passes through

    zero, T2 and T3 would turn off.

    The waveforms are shown in figure 8. 29

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    Figure 8Average load voltage

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    FULL-WAVE FULLY CONTROLLED BRIDGE

    WITH INDUCTIVE LOAD

    In the positive half-cycle, T1 and T3 are turned on at delay angle a, and current

    flows to the load through the path T1, load and T3. When the supply voltage

    passes through zero and reverses. the stored energy in the load is regenerating

    back to the supply; T1 and T3 are maintained in conduction state. Energy stored

    in the load inductance keeps load current flowing through the path of T1, load

    and T3 until (T2 and T4) are fired at delay angle of ( a).

    .

    The flow of load current

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    When T2 and T4 are fired at delay angle of ( a), current flows to the load

    through the path T2, load and T4 until T1 and T3 are fired at the next cycle.

    The flow of load current

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    supply voltage

    Output voltage

    Output current

    supply current

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    Average Load Voltage :

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