tronics1-clampers clippers multipliers rectifiers zener

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    Chapter 2:

    Diode Applications

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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/e

    Robert L. Boylestad and Louis Nashelsky

    Load-Line AnalysisLoad-Line Analysis

    22

    The load line plots all possible

    combinations of diode current (ID)

    and voltage (VD) for a given

    circuit. The maximumID equals

    E/R, and the maximum VD equals

    E.

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Series Diode ConfigurationsSeries Diode Configurations

    Constants

    Silicon Diode: VD = 0.7 V

    Germanium Diode: VD = 0.3 V

    Analysis (for silicon)

    VD = 0.7 V (or VD =EifE< 0.7 V)

    VR = E VD

    ID = IR = IT= VR / R

    33

    Forward BiasForward 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/e

    Robert L. Boylestad and Louis Nashelsky

    Series Diode ConfigurationsSeries Diode Configurations

    Diodes ideally behave as open circuits

    Analysis

    VD = E

    VR = 0 V

    ID= 0 A

    44

    Reverse BiasReverse 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/e

    Robert L. Boylestad and Louis Nashelsky

    Parallel ConfigurationsParallel Configurations

    55

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Half-Wave RectificationHalf-Wave Rectification

    66

    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/e

    Robert L. Boylestad and Louis Nashelsky

    PIV (PRV)PIV (PRV)

    77

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Full-Wave RectificationFull-Wave Rectification

    88

    Half-wave: VVdcdc = 0.318= 0.318VVmm

    Full-wave: VVdcdc = 0.636= 0.636VVmm

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Full-Wave RectificationFull-Wave Rectification

    99

    Bridge RectifierBridge 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/e

    Robert L. Boylestad and Louis Nashelsky

    Full-Wave RectificationFull-Wave Rectification

    1010

    Center-Tapped TransformerCenter-Tapped Transformer

    RectifierRectifier

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Summary of Rectifier CircuitsSummary of Rectifier Circuits

    1111

    Vm= peak of the AC voltage.

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

    RectifierRectifier IdealIdeal VVDCDC RealisticRealistic VVDCDC

    Half Wave Rectifier VDCDC = 0.318Vm VDCDC = 0.318Vmm 0.7

    Bridge Rectifier VDCDC = 0.636Vm VDCDC = 0.636Vm 2(0.7 V)

    Center-Tapped Transformer

    RectifierVDCDC = 0.636Vm VDCDC = 0.636Vm 0.7 V

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    Important Equations

    TRANSFORMER EQUATIONS

    =

    =

    = 0.707

    HALF-WAVE RECTIFIER EQUATIONS (TRANSFORMER COUPLED)

    = 0.7 = /

    = = / = = /

    = = /2 = = /2

    PIV=V2 fout= fin

    Efficiency of Rectification = n = (/)100%CENTER-TAPPED FULL-WAVE RECTIFIER EQUATIONS (TRANSFORMER COUPLED)

    = /20.7 = /

    = = 2/ = = 2/

    =

    =

    /2

    =

    =

    /2

    PIV=V2 0.7 fout= 2fin

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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/e

    Robert L. Boylestad and Louis Nashelsky

    Diode ClippersDiode Clippers

    1212

    The diode in a series clipperseries 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/e

    Robert L. Boylestad and Louis Nashelsky

    Biased ClippersBiased Clippers

    1313

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Parallel ClippersParallel Clippers

    1414

    The diode in a parallel clipperparallel 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/e

    Robert L. Boylestad and Louis Nashelsky

    Summary of Clipper CircuitsSummary of Clipper Circuits

    1515

    moremore

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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/e

    Robert L. Boylestad and Louis Nashelsky

    Summary of Clipper CircuitsSummary of Clipper Circuits

    1616

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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/e

    Robert L. Boylestad and Louis Nashelsky

    ClampersClampers

    1717

    A diode and capacitor can be

    combined to clamp an AC

    signal to a specific DC 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/e

    Robert L. Boylestad and Louis Nashelsky

    Biased Clamper CircuitsBiased Clamper Circuits

    1818

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Summary of Clamper CircuitsSummary of Clamper Circuits

    1919

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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/e

    Robert L. Boylestad and Louis Nashelsky

    Zener DiodesZener Diodes

    2020

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Zener Resistor ValuesZener Resistor Values

    2121

    ZKRLIII

    min

    min

    max

    L

    Z

    L

    I

    VR

    min

    max

    L

    Z

    L

    L

    L

    R

    V

    R

    VI

    Zi

    Z

    L

    VV

    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:

    The maximum 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/e

    Robert L. Boylestad and Louis Nashelsky

    Voltage-Multiplier CircuitsVoltage-Multiplier Circuits

    Voltage Doubler

    Voltage Tripler

    Voltage Quadrupler

    2222

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Voltage DoublerVoltage Doubler

    2323

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Voltage DoublerVoltage Doubler

    2424

    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/e

    Robert L. Boylestad and Louis Nashelsky

    Voltage Tripler and QuadruplerVoltage Tripler and Quadrupler

    2525

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    Copyright 2009 by Pearson Education, Inc.

    S R 0 4 8 A

    Electronic Devices and Circuit Theory, 10/e

    R b t L B l t d d L i N h l k

    Practical ApplicationsPractical 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

    2626