Nothing Special   »   [go: up one dir, main page]

B-Stad CH 02

Download as ppt, pdf, or txt
Download as ppt, pdf, or txt
You are on page 1of 27

Electronic Devices and Circuit Theory

Boylestad

Diode Applications
Chapter 2

Ch.2 Summary

Load-Line 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.
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.
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Series Diode Configurations


Forward Bias
Constants Silicon Diode: VD = 0.7 V

Germanium Diode: VD = 0.3 V


Analysis (for silicon) VD = 0.7 V (or VD = E if E < 0.7 V) VR = E VD ID = IR = IT = VR / R
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Series Diode Configurations


Reverse Bias
Diodes ideally behave as open circuits

Analysis VD = E VR = 0 V ID = 0 A

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Parallel Diode Configurations


V 0.7 V D V V V 0.7 V D1 D2 o V 9.3 V R E V 10 V .7 V D I 28 mA R R .33 k I D1 I D2 28 mA 2 14 mA

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Half-Wave Rectification
The diode conducts only 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.
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

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.

PIV (or PRV) > Vm


Where PIV = Peak inverse voltage
PRV = Peak reverse voltage Vm = Peak AC voltage
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Full-Wave Rectification
The rectification process can be improved by using a full-wave rectifier circuit.
Full-wave rectification produces a greater DC output:

Half-wave: Vdc = 0.318Vm


Full-wave: Vdc = 0.636Vm
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Full-Wave Rectification

Bridge Rectifier
A full-wave rectifier with four diodes that are connected in a bridge configuration

VDC = 0.636Vm
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Full-Wave Rectification

Center-Tapped Transformer Rectifier


Requires two diodes and a center-tapped transformer

VDC = 0.636Vm
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Summary of Rectifier Circuits


In the center tapped transformer rectifier circuit, the peak AC voltage is the transformer secondary voltage to the tap.
Rectifier Half Wave Rectifier Bridge Rectifier Center-Tapped Transformer Rectifier Ideal VDC VDC= 0.318Vm VDC = 0.636Vm VDC = 0.636Vm Realistic VDC VDC = 0.318Vm 0.7 VDC = 0.636Vm 2(0.7 V) VDC = 0.636Vm 0.7 V

Vm = the peak AC voltage


Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Diode Clippers
The diode in a series 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)

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

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

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Parallel Clippers
The diode in a parallel clipper circuit clips any voltage that forward biases it.
DC biasing can be added in series with the diode to change the clipping level.

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Summary of Clipper Circuits

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Summary of Clipper Circuits

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Summary of Clipper Circuits

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

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

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Biased Clamper Circuits


The input signal can be any type of waveform such as a sine, square, or triangle wave.

The DC source lets you adjust the DC camping level.


Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Summary of Clamper Circuits

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Zener Diodes
The Zener is a diode that is operated in reverse bias at the Zener Voltage (Vz).
When Vi VZ The Zener is on 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
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Zener Resistor Values


If R is too large, the Zener diode cannot conduct because IZ < IZK. The minimum current is given by:

ILmin IR IZK

The maximum value of resistance is:

RLmax

VZ ILmin IL max VL V Z RL RL min

If R is too small, IZ > IZM . The maximum allowable current for the circuit is given by:

The minimum value of resistance is:


Electronic Devices and Circuit Theory
Boylestad

RL min

RVZ Vi VZ

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Voltage-Multiplier Circuits
Voltage multiplier circuits use a combination of diodes and capacitors to step up the output voltage of rectifier circuits. Three common voltage multipliers are the:

Voltage Doubler
Voltage Tripler Voltage Quadrupler
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Voltage Doubler

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

Vout = VC2 = 2Vm


where Vm = peak secondary voltage of the transformer
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Voltage Doubler
Positive Half-Cycle
D1 conducts D2 is switched off Capacitor C1 charges to Vm D1 is switched off D2 conducts Capacitor C2 charges to Vm

Negative Half-Cycle

Vout = VC2 = 2Vm

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

Voltage Tripler and Quadrupler

Electronic Devices and Circuit Theory


Boylestad

2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

Ch.2 Summary

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
Electronic Devices and Circuit Theory
Boylestad 2013 by Pearson Higher Education, Inc Upper Saddle River, New Jersey 07458 All Rights Reserved

You might also like