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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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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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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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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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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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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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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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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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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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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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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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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
Summary of Clipper Circuits
15
more
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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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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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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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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