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Diddes lecture

Apr 04, 2018

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Load-Line Analysis

    2

    The load line plots all possible

    combinations of diode current (ID)

    and voltage (VD) for a given circuit.

    The maximumID equalsE/R, and

    the maximum VD equalsE.

    The point where the load line and

    the characteristic curve intersect is

    the Q-point, which identifiesID and

    VD for a particular diode in a given

    circuit.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Series Diode Configurations

    Constants

    Silicon Diode: VD = 0.7 V

    Germanium Diode: VD = 0.3 V

    Analysis (for silicon)

    VD = 0.7 V (or VD =E ifE < 0.7 V)

    VR = EVD

    ID = IR = IT= VR / R

    3

    Forward Bias

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Series Diode Configurations

    Diodes ideally behave as open circuits

    Analysis

    VD = E

    VR = 0 V

    ID= 0 A

    4

    Reverse Bias

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Parallel Configurations

    5

    mA14

    2

    mA28

    D2I

    D1I

    mA28

    .33k

    V.7V10

    R

    DVE

    RI

    V9.3R

    V

    V0.7O

    VD2

    VD1

    V

    V0.7D

    V

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Half-Wave Rectification

    6

    The diode only

    conducts when it is

    forward biased,

    therefore only half

    of the AC cycle

    passes through the

    diode to the

    output.

    The DC output voltage is 0.318Vm, where Vm = the peak AC voltage.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    PIV (PRV)

    7

    Because the diode is only forward biased for one-half of the AC cycle, it is

    also reverse biased for one-half cycle.

    It is important that the reverse breakdown voltage rating of the diode be

    high enough to withstand the peak, reverse-biasing AC voltage.

    PIV (or PRV) > Vm

    PIV = Peak inverse voltage

    PRV = Peak reverse voltage

    Vm

    = Peak AC voltage

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Full-Wave Rectification

    8

    Half-wave: Vdc = 0.318Vm

    Full-wave: Vdc = 0.636Vm

    The rectification process can be improved by

    using a full-wave rectifier circuit.

    Full-wave rectification produces a greaterDC output:

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Full-Wave Rectification

    9

    Bridge Rectifier

    Four diodes are connected in a

    bridge configuration VDC = 0.636Vm

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Full-Wave Rectification

    10

    Center-Tapped Transformer

    Rectifier

    Requires

    Two diodes

    Center-tapped transformer

    VDC = 0.636Vm

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Summary of Rectifier Circuits

    11

    Vm= peak of the AC voltage.

    In the center tapped transformer rectifier circuit, the peak AC voltageis the transformer secondary voltage to the tap.

    Rectifier Ideal VDC Realistic VDC

    Half Wave Rectifier VDC = 0.318Vm VDC = 0.318Vm0.7

    Bridge Rectifier VDC = 0.636Vm VDC = 0.636Vm2(0.7 V)

    Center-Tapped Transformer

    RectifierVDC = 0.636Vm VDC = 0.636Vm0.7 V

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Diode Clippers

    12

    The diode in a series clipperclipsany voltage that does not forward

    bias it:A reverse-biasing polarity

    A forward-biasing polarity less than0.7 V (for a silicon diode)

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Biased Clippers

    13

    Adding a DC source in

    series with the clipping

    diode changes the

    effective forward bias of

    the diode.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Parallel Clippers

    14

    The diode in a parallel clipper

    circuit clips any voltage that

    forward bias it.

    DC biasing can be added inseries with the diode to change

    the clipping level.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Summary of Clipper Circuits

    15

    more

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Summary of Clipper Circuits

    16

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Biased Clamper Circuits

    18

    The input signal can be any type

    of waveform such as sine, square,

    and triangle waves.

    The DC source lets you adjust

    the DC camping level.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Summary of Clamper Circuits

    19

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Zener Diodes

    20

    The Zener is a diode operatedin reverse bias at the Zener

    Voltage (Vz).

    When Vi VZ

    The Zener is on Voltage across the Zener is VZ

    Zener current:IZ=IRIRL The Zener Power:PZ = VZIZ

    When Vi< VZ The Zener is off

    The Zener acts as an open circuit

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Zener Resistor Values

    21

    ZKRLIII

    min

    min

    max

    L

    Z

    L

    I

    VR

    min

    max

    L

    Z

    L

    L

    L

    R

    V

    R

    VI

    Zi

    Z

    LVV

    RVR

    min

    IfR is too large, the Zener diode cannot conduct because the available amount of

    current is less than the minimum current rating,IZK. The minimum current is

    given by:

    Themaximum value of resistance is:

    IfR is too small, the Zener current exceeds the maximum current

    rating,IZM. The maximum current for the circuit is given by:

    The minimum value of resistance is:

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Voltage-Multiplier Circuits

    Voltage Doubler

    Voltage Tripler

    Voltage Quadrupler

    22

    Voltage multiplier circuits use a combination of diodes and

    capacitors to step up the output voltage of rectifier circuits.

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Voltage Doubler

    23

    This half-wave voltage doublers output can be calculated by:

    Vout = VC2 = 2Vm

    where Vm = peak secondary voltage of the transformer

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Voltage Doubler

    24

    Positive Half-Cycle

    o D1 conductso D2 is switched off

    o Capacitor C1 charges to Vm

    Negative Half-Cycle

    o D1 is switched off

    o D2 conductso Capacitor C2 charges to Vm

    Vout = VC2 = 2Vm

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    Copyright 2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 All rights reserved.

    Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky

    Voltage Tripler and Quadrupler

    25

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    Copyright 2009 by Pearson Education, Inc.U S ddl Ri N J 07458 All i ht d

    Electronic Devices and Circuit Theory, 10/eRobert L Boylestad and Louis Nashelsky

    Practical Applications

    Rectifier Circuits Conversions of AC to DC for DC operated circuits

    Battery Charging Circuits

    Simple Diode Circuits

    Protective Circuits against

    Overcurrent

    Polarity Reversal

    Currents caused by an inductive kick in a relay circuit

    Zener Circuits

    Overvoltage Protection

    Setting Reference Voltages

    26