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Chapter 2: Diode Applications

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Page 1: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Chapter 2:Diode Applications

Page 2: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

LoadLoad--Line AnalysisLine Analysis

The load line plots all possible combinations of diode current (ID) and voltage (VD) for a given circuit. The maximum ID equals E/R, and the maximum VD equals E.

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 22

The point where the load line and the characteristic curve intersect is the Q-point, which identifies ID and VD for a particular diode in a given circuit.

Page 3: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Series Diode ConfigurationsSeries Diode Configurations

Constants• Silicon Diode: VD = 0.7 V• Germanium Diode: VD = 0.3 V

Analysis (for silicon)

Forward BiasForward Bias

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

• VD = 0.7 V (or VD = E if E < 0.7 V)• VR = E – VD

• ID = IR = IT = VR / R

33

Page 4: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Series Diode ConfigurationsSeries Diode Configurations

Diodes ideally behave as open circuits

Analysis• VD = E

• VR = 0 V

Reverse BiasReverse Bias

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

R

• ID = 0 A

44

Page 5: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Parallel ConfigurationsParallel Configurations

V .7V 10DVE

V 9.3R

V

V 0.7O

VD2

VD1

V

V 0.7D

V

−−

=

===

=

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 55

mA 142

mA 28D2

ID1

I

mA 28.33kΩ

V .7V 10

RD

VE

RI

===

=−

=

=

Page 6: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

HalfHalf--Wave RectificationWave Rectification

The diode only conducts when it is forward biased, therefore only half of the AC cycle passes through the

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 66

passes through the diode to the output.

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

Page 7: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

PIV (PRV)PIV (PRV)

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.

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 77

PIV (or PRV) > Vm

• PIV = Peak inverse voltage• PRV = Peak reverse voltage• Vm = Peak AC voltage

Page 8: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

FullFull--Wave RectificationWave Rectification

The rectification process can be improved by using a full-wave rectifier circuit.

Full-wave rectification produces a greater DC output:

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 88

• Half-wave: VVdcdc = 0.318= 0.318VVmm

• Full-wave: VVdcdc = 0.636= 0.636VVmm

DC output:

Page 9: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

FullFull--Wave RectificationWave Rectification

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 99

Bridge RectifierBridge Rectifier

• Four diodes are connected in a bridge configuration

• VDC = 0.636Vm

Page 10: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

FullFull--Wave RectificationWave Rectification

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1010

CenterCenter--Tapped Transformer Tapped Transformer RectifierRectifier

Requires• Two diodes• Center-tapped transformer

VDC = 0.636Vm

Page 11: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Summary of Rectifier CircuitsSummary of Rectifier Circuits

RectifierRectifier Ideal Ideal VVDCDC Realistic Realistic 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 V = 0.636V V = 0.636V – 0.7 V

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1111

Vm = peak of the AC voltage.

IIn the center tapped transformer rectifier circuit, t he peak AC voltage is the transformer secondary voltage to the tap.

Center-Tapped Transformer Rectifier

VDCDC = 0.636Vm VDCDC = 0.636Vm – 0.7 V

Page 12: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Diode ClippersDiode Clippers

The diode in a series clipperseries clipper“clips” any voltage that does not forward bias it:•A reverse-biasing polarity•A forward-biasing polarity less than 0.7 V (for a silicon diode)

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1212

Page 13: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Biased ClippersBiased Clippers

Adding a DC source in series with the clipping diode changes the effective forward bias of the diode.

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1313

Page 14: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Parallel ClippersParallel Clippers

The diode in a parallel clipperparallel clippercircuit “clips” any voltage that forward bias it.

DC biasing can be added in series with the diode to change

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1414

series with the diode to change the clipping level.

Page 15: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Summary of Clipper CircuitsSummary of Clipper Circuits

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1515

more…more…

Page 16: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Summary of Clipper CircuitsSummary of Clipper Circuits

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1616

Page 17: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

ClampersClampers

A diode and capacitor can be combined to “clamp” an AC signal to a specific DC level.

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1717

Page 18: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Biased Clamper CircuitsBiased Clamper Circuits

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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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1818

the DC camping level.

Page 19: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Summary of Clamper CircuitsSummary of Clamper Circuits

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 1919

Page 20: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Zener DiodesZener Diodes

The Zener is a diode operated in reverse bias at the Zener Voltage (Vz).

• When Vi ≥≥≥≥ VZ

– The Zener is on

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2020

– Voltage across the Zener is VZ

– Zener current: IZ = IR – IRL

– The Zener Power: PZ = VZIZ

• When Vi < VZ

– The Zener is off– The Zener acts as an open circuit

Page 21: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Zener Resistor ValuesZener Resistor Values

ZKRL I II −= min

minmax

L

ZL I

VR =

If R 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 maximumvalue of resistance is:

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2121

minmax

L

Z

L

LL R

V R

V I ==

Zi

ZL VV

RVR

−=min

If R 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:

Page 22: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

VoltageVoltage--Multiplier CircuitsMultiplier Circuits

• Voltage Doubler• Voltage Tripler• Voltage Quadrupler

Voltage multiplier circuits use a combination of diodes and capacitors to step up the output voltage of rectifier circuits.

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2222

Page 23: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Voltage DoublerVoltage Doubler

This half-wave voltage doubler’s output can be calculated by:

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2323

This half-wave voltage doubler’s output can be calculated by:

Vout = VC2 = 2Vm

where Vm = peak secondary voltage of the transformer

Page 24: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Voltage DoublerVoltage Doubler

• Positive Half-Cycleo D1 conductso D2 is switched offo Capacitor C1 charges to Vm

• Negative Half-Cycleo D1 is switched offo D2 conductso Capacitor C charges to V

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2424

o Capacitor C2 charges to Vm

Vout = VC2 = 2Vm

Page 25: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

Voltage Tripler and QuadruplerVoltage Tripler and Quadrupler

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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky 2525

Page 26: Electronic devices-and-circuit-theory-10th-ed-boylestad-chapter-2

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

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

– Polarity Reversal– Currents caused by an inductive kick in a relay circuit

• Zener Circuits– Overvoltage Protection– Setting Reference Voltages

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