Lect 05 Diodes and applications - Part2.pptx

Lecture 05: Diodes Applications
& Special diode types
Prepared By
Dr. Eng. Sherif Hekal
Assistant Professor, CCE department
CCE201: Solid State Electronic Devices
12/10/2022
Lecture 01 1
EEC223: Electronics (1)

Introduction
• In this Lecture we will learn
 application of the diode in the design of rectifier
circuits, which convert ac voltages to dc as needed
for powering electronic equipment.
 a number of other practical and important
applications: limiting and clamping circuits.
 Special diode types: LED, Photo diode, Schottky
diode, Varactor diode, Zener diode.
12/10/2022 2

4.5. Rectifier Circuits
• One important application of
diode is the rectifier –
• Electrical device
which converts
alternating current
(AC) to direct
current (DC)
• One important application of
rectifier is dc power supply. Figure 4.20: Block diagram of a dc
power supply

Oxford University Publishing
Microelectronic Circuits by Adel S. Sedra and Kenneth C. Smith (0195323033)
Figure 4.20: Block diagram of a dc power supply
step #1: Decrease RMS magnitude of AC wave
via power transformer
step #2: convert full-wave AC signal to full-wave
rectified signal (still time-varying and periodic)
step #3: employ low-pass filter to reduce wave
amplitude by > 90%
step #4: employ voltage regulator to eliminate
ripple
step #5: supply dc load
.

4.5.1. The Half-Wave Rectifier
• half-wave rectifier –
utilizes only alternate
half-cycles of the input
sinusoid
• Constant voltage
drop diode model is
employed.
12/10/2022 5
Figure 4.21: (a) Half-wave rectifier (b) Transfer characteristic of the rectifier circuit (c)
Input and output waveforms

4.5.1. The Half-Wave Rectifier
• current-handling capability – what is maximum forward current
diode is expected to conduct?
• peak inverse voltage (PIV) – what is maximum reverse voltage it
is expected to block w/o breakdown?
12/10/2022 6
In selecting diodes for rectifier design, two important parameters must be
specified:
It is usually prudent to select a diode that has a reverse breakdown voltage
at least 50% greater than the expected PIV.

4.5.2. The
Full-Wave Rectifier
• Q: How does full-wave
rectifier differ from
half-wave?
• A: It utilizes both
halves of the input
• One potential is
shown to right.
12/10/2022 7
Figure 4.22: Full-wave rectifier utilizing a
transformer with a center-tapped secondary winding.

12/10/2022 8
Figure 4.22: full-wave rectifier utilizing a transformer with a center-
tapped secondary winding: (a) circuit; (b) transfer characteristic
assuming a constant-voltage-drop model for the diodes; (c) input and
output waveforms.

When instantaneous source voltage is positive, D1
conducts while D2 blocks…
12/10/2022 10

when instantaneous source voltage is negative, D2
conducts while D1 blocks
12/10/2022 11

4.5.2. The Full-Wave Rectifier
• Q: What are most important
observation(s) from this operation?
• A: The direction of current flowing
across load never changes (both halves
of AC wave are rectified). The full-
wave rectifier produces a more
“energetic” waveform than half-wave.
• PIV for full-wave = 2VS – VD
12/10/2022 12

EXERCISE 4.20
12/10/2022 13
For the full-wave rectifier circuit in Fig. 4.22(a), show the following: (a) The
output is zero for an angle of 2 sin−1 (VD ⁄ VS) centered around the zero-
crossing points of the sine-wave input. (b) The average value (dc
component) of vO is 𝑉
𝑜 =
2
𝜋
𝑉𝑆 − 𝑉𝐷 (c) The peak current through each
diode is (𝑉𝑆−𝑉𝐷)/𝑅.

EXERCISE 4.20
12/10/2022 14
𝜋 − 𝜃 𝜋 + 𝜃
𝜃
a. As shown in the diagram, the output is zero between 𝜋 − 𝜃 to 𝜋 + 𝜃 = 2𝜃
Here 𝜃 is the angle at which the input signal reaches 𝑉𝐷
∴ 𝑉𝑆 sin 𝜃 = 𝑉𝐷
∴ 𝜃 = sin−1 𝑉𝐷
𝑉𝑆
The output is zero for an angle of 2𝜃 = 2sin−1 𝑉𝐷
𝑉𝑆

EXERCISE 4.20
12/10/2022 15
𝜋 − 𝜃 𝜋 + 𝜃
𝜃
b. Average value of the output signal is given by
𝑉
o,avg =
1
2𝜋
2 ×
∅
𝜋−∅
(𝑉𝑆 sin ∅ − 𝑉𝐷)d∅
=
1
𝜋
−𝑉𝑆 cos ∅ − 𝑉𝐷∅
=
2𝑉𝑆
𝜋
− 𝑉𝐷







EXERCISE 4.20
12/10/2022 16
C. The peak current occurs when 𝜙 =
𝜋
2
∴ peak current =
𝑉𝑆 sin
𝜋
2
− 𝑉𝐷
𝑅
=
𝑉𝑆 − 𝑉𝐷
𝑅
If 𝑣𝑆 = 12 Vrms ⇒ 𝑡ℎ𝑒𝑛𝑉𝑆 = 12 2
∴ peak current =
12 2 − 0.7
100
= 163 mA
𝜋 − 𝜃 𝜋 + 𝜃
𝜃

4.5.3. The Bridge Rectifier
• An alternative
implementation of
the full-wave
rectifier is bridge
rectifier.
• Shown to right.
12/10/2022 17
Figure 4.23: The bridge rectifier circuit.

12/10/2022 18
when instantaneous source voltage is positive, D1
and D2 conduct while D3 and D4 block

12/10/2022 19
when instantaneous source voltage is positive, D1
and D2 conduct while D3 and D4 block

4.5.3: The Bridge Rectifier (BR)
• Q: What is the main advantage of BR?
• A: No need for center-tapped
transformer.
• Q: What is main disadvantage?
• A: Series connection of TWO diodes
will reduce output voltage.
• PIV = VS – VD
12/10/2022 20

4.5.4. The Rectifier
with a Filter Capacitor
• Pulsating nature of
rectifier output makes
unreliable dc supply.
• As such, a filter
capacitor is employed
to remove ripple.
12/10/2022 21
Figure 4.24: (a) A simple circuit used to illustrate the effect of a filter
capacitor. (b) input and output waveforms assuming an ideal diode.

• step #1: source voltage is
positive, diode is forward
biased, capacitor charges.
reverse, diode is reverse-
biased (blocking),
capacitor cannot
discharge.
positive, diode is forward
biased, capacitor charges
(maintains voltage).
12/10/2022 22
Figure 4.24 (a) A simple circuit used to illustrate the effect…

• Q: Why is this example unrealistic?
• A: Because for any practical
application, the converter would
supply a load (which in turn provides
a path for capacitor discharging).
12/10/2022 23

• Q: What happens when
load resistor is placed
in series with capacitor?
• A: One must now
consider the
discharging of
capacitor across
load.
12/10/2022 24

   
 

 

output voltage for state #1
O I D
t
RC
O peak
v t v t v
v t V e
25
circuit state #2
circuit state #1

   
 



O I
t
RC
O peak
v t v t
v t V e
12/10/2022 26
Figure 4.25: Voltage and Current Waveforms in the Peak Rectifier
Circuit WITH RC >> T. The diode is assumed ideal.

A Couple of Observations
• The diode conducts for a brief interval (Dt) near the
peak of the input sinusoid and supplies the capacitor
with charge equal to that lost during the much longer
discharge interval. The latter is approximately equal
to T.
• Assuming an ideal diode, the diode conduction
begins at time t1 (at which the input vI equals the
exponentially decaying output vO). Diode conduction
stops at time t2 shortly after the peak of vI (the exact
value of t2 is determined by settling of ID).
12/10/2022 27

A Couple of Observations
 
(eq4.27) if is s
1
ll
2
ma
O peak r peak r
V V V V V
  
avg
12/10/2022 28
• During the diode off-interval, the capacitor C discharges through R
causing an exponential decay in the output voltage (vO). At the end of
the discharge interval, which lasts for almost the entire period T,
voltage output is defined as follows – vO(T) = Vpeak – Vr.
• When the ripple voltage (Vr) is small, the output (vO) is almost
constant and equal to the peak of the input (vI). the average output
voltage may be defined as below…

4.6: Limiting and
Clamping Circuits
• Q: What is a limiter circuit?
• A: One which limits
voltage output.
12/10/2022 29
Figure 4.28: General transfer
characteristic for a limiter circuit
𝑣𝑖
𝑣𝑜

4.6. Limiting and
Clamping Circuits
• passive limiter circuit
• has linear range
• has nonlinear range
• K < 1
• examples include
• single limiter operate in uni-
polar manner
• double limiter operate in bi-
polar manner
over linear range
outside linear range
-
constant value(s)
I
O
O
I
I
I
I
Kv
v
L
v Kv
L
v
K
L L
v
K K
L
v
K
L







 

 







 



 30

12/10/2022 31
Figure 4.31: Variety of basic limiting circuits.
single limiters
employ one
diode
double limiters
employ two
diodes of
opposite polarity
linear range may
be controlled via
string of diodes
and dc sources
zener diodes may
be used to
implement soft
limiting

4.6.2. The Clamped
Capacitor or DC Restorer
• Q: What is a dc restorer?
• A: Circuit which removes the
dc component of an AC wave.
• Q: Why is this ability important?
• A: Average value of this output
is effective way to measure duty
cycle
12/10/2022 32
Figure 4.32: The clamped
capacitor or dc restorer with a
square-wave input and no load

4.6.3: The Voltage Doubler
• Q: What is a
voltage doubler?
• A: One which
multiplies the
amplitude of a
wave or signal by
two.
12/10/2022 33
Figure 4.34: Voltage doubler: (a) circuit;
(b) waveform of the voltage across D1.

Special Diode Types
12/10/2022 34

There are two popular types of optoelectronic devices:
light-emitting diode (LED) and photodiode.
The Light-Emitting Diode (LED)
LED is diode that emits light when biased in the forward direction
of p-n junction.
Anode Cathode
The schematic symbol and construction features.
Optical Diodes

LED that are produced in an array of shapes and sizes.
LED characteristics:
characteristic curves are very similar to those for p-n junction diodes
higher forward voltage (VF)
lower reverse breakdown voltage (VBR).

Application
The seven segment display is an example of LEDs use for display of decimal
digits.
The 7-segment LED display.

LED displays are packages of many LEDs arranged in a pattern, the most
familiar pattern being the 7-segment displays for showing numbers (digits 0-9).
LED Displays

Light Spectrum
Red, green and blue LEDs

When a light-emitting diode is forward
biased, electrons are able to recombine with
holes within the device, releasing energy in
the form of photons.
This effect is called electroluminescence and
the color of the light (corresponding to the
energy of the photon) is determined by the
energy gap of the semiconductor.
Fabricating the pn junction using a
semiconductor of the type known as direct-
bandgap materials.

12/10/2022 41
Radiative recombination Non-radiative recombination

12/10/2022 42
Radiative recombination Non-radiative recombination

UV – AlGaN
Blue – GaN, InGaN
Red, green – GaP
Red, yellow – GaAsP
IR- GaAs
LED - Light Emitting Diodes

LED - Colors & voltage drop
Color
Wavelength
(nm)
Voltage (V) Semiconductor Material
Infrared λ > 760 ΔV < 1.9 Gallium arsenide (GaAs) Aluminium gallium arsenide (AlGaAs)
Red 610 < λ < 760 1.63 < ΔV < 2.03 Aluminium gallium arsenide (AlGaAs) Gallium arsenide phosphide
(GaAsP) Aluminium gallium indium phosphide (AlGaInP) Gallium(III)
phosphide (GaP)
Orange 590 < λ < 610 2.03 < ΔV < 2.10 Gallium arsenide phosphide (GaAsP) Aluminium gallium indium
phosphide (AlGaInP)Gallium(III) phosphide (GaP)
Yellow 570 < λ < 590 2.10 < ΔV < 2.18 Gallium arsenide phosphide (GaAsP) Aluminium gallium indium
phosphide (AlGaInP) Gallium(III) phosphide (GaP)
Green 500 < λ < 570 1.9 < ΔV < 4.0 Indium gallium nitride (InGaN) / Gallium(III) nitride (GaN) Gallium(III)
phosphide (GaP)Aluminium gallium indium phosphide (AlGaInP)
Aluminium gallium phosphide (AlGaP)
Blue 450 < λ < 500 2.48 < ΔV < 3.7 Zinc selenide (ZnSe), Indium gallium nitride (InGaN), Silicon carbide
(SiC) as substrate, Silicon (Si)
Violet 400 < λ < 450 2.76 < ΔV < 4.0 Indium gallium nitride (InGaN)
Purple multiple types 2.48 < ΔV < 3.7 Dual blue/red LEDs,blue with red phosphor,or white with purple
plastic
Ultra-
violet
λ < 400 3.1 < ΔV < 4.4 diamond (235 nm), Boron nitride (215 nm) , Aluminium nitride (AlN)
(210 nm) Aluminium gallium nitride (AlGaN) (AlGaInN) — (to
210 nm)
White Broad
spectrum
ΔV = 3.5 Blue/UV diode with yellow phosphor

Never connect an LED directly to a battery or a power supply!
It will be destroyed almost instantly because too much current will
pass through and burn it out.
LEDs must have a resistor in series to limit the current to a safe
value, for quick testing purposes a 1kΩ resistor is suitable for most
LEDs if your supply voltage is 12V or less.
Remember to connect the LED the correct way!
Testing an LED

The most popular type of tri-color LED has a red and a
green LED combined in one package with three leads.
They are called tri-color because mixed red and green
light appears to be yellow.
The diagram shows the organization of a tri-color LED.
Note the different lengths of the three leads.
The central lead (k) is the common cathode for both
LEDs, the outer leads (a1 and a2) are the anodes to the
LEDs allowing each one to be lit separately, or both
together to give the third color.
Tri-color LEDs

An LED must have a resistor connected in series to
limit the current through the LED. The resistor value,
R is given by:
R = (VS - VL) / I
Calculating an LED resistor value
VS = supply voltage
VL = LED voltage (usually 2V, but 4V for blue and white LEDs)
I = LED current (e.g. 20mA), this must be less than the maximum permitted
If the calculated value is not available, choose the nearest standard resistor value
which is greater, to limit the current. Even greater resistor value will increase the
battery life but this will make the LED less bright.
For example
If the supply voltage VS = 9V, and you have a red LED (VL = 2V), requiring a
current I = 20mA = 0.020A,
R = (9V - 2V) / 0.02A = 350, so choose 390 (the nearest greater standard value).

If you wish to have several LEDs on at the same time,
connect them in series.
This prolongs battery life by lighting several LEDs
with the same current as just one LED.
The power supply must have sufficient voltage to
provide about 2V for each LED (4V for blue and
white) plus at least another 2V for the resistor.
To work out a value for the resistor you must add up
all the LED voltages and use this for VL.
Connecting LEDs in series

Example
A red, a yellow and a green LED in series
need a supply voltage of at least
3×2V + 2V = 8V,
so choose a 9V battery. Adjust the resistor
R to have current I=15 mA.

Example
A red, a yellow and a green LED in series need a
supply voltage of at least 3×2V + 2V = 8V,
so choose a 9V battery. Adjust the resistor R to have
current I=15 mA.
VL = 2V + 2V + 2V = 6V (the three LED voltages
added up).
If the supply voltage VS is 9V and the current I
must be 15mA = 0.015A,
Resistor R = (VS - VL) / I = (9 - 6) / 0.015 = 3 /
0.015 = 200,
so choose R = 220Ω (the nearest standard value
which is greater).

Photodiode is a p-n junction that can convert light energy into
electrical energy.
It operates in reverse bias voltage (VR), as shown in Figure, where
Iλ is the reverse light current.
It has a small transparent window that allows light to strike the
p-n junction.
The resistance of a photodiode is calculated by the formula as
follows:

I
V
R R
R 
The Photodiode
Iλ

12/10/2022 52
Alarm System using Photodiode
IR Transmitter Circuit
Photodiode Alarm Circuit

 The Schottky diode’s significant characteristic is its fast switching speed.
 This is useful for high frequencies and digital applications.
 It is not a typical diode in that it does not have a p-n junction.
 Instead, it consists of a doped semiconductor (usually n-type) and
metal bound together.
Schottky diode (a) symbol and (b) basic internal construction
The Schottky Diode

Zener Diode
Zener diode is a p-n junction diode
that is designed to operate in the
reverse breakdown region.
Two things happen when the
reverse breakdown voltage (VBR) is
reached:
The diode current increases
drastically.
The reverse voltage (VR) across
the diode remains relatively
constant.
In other words, the voltage across a
zener diode operated in this region
is relatively constant over a range
of reverse current and nearly equal
to its zener voltage (VZ) rating.
+
−
I
Z
V
Z
Anode (A)
Cathode (K) K
A
Zener diode voltage-curent (V-I) characteristic.
VB
R

Ideal-and-Practical Zener Equivalent Circuits
VF
VR
I
F
IR
V
Z
Ideal model and characteristic curve of a
zener diode in reverse breakdown.
The constant voltage drop =
the nominal zener voltage.
Practical model and characteristic curve of a zener diode, where
the zener impedance (resistance), ZZ is included.
A change in zener current (ΔIZ) produces a
small change in zener voltage (ΔVZ).
Zener Diode

Varactor is a type of p-n junction diode that
operates in reverse bias. The capacitance of
the junction is controlled by the amount of
reverse bias.
Varactor diodes are also referred to as
varicaps or tuning diodes and they are
commonly used in communication systems.
Basic Operation
The capacitance of a reverse-biased
varactor junction is found as:
Reverse-biased varactor diode acts as
a variable capacitor.
Varactor diode symbol
d
A
C


C = the total junction capacitance.
A = the plate area.
ε = the dielectric constant (permittivity).
d = the width of the depletion region
(plate separation).
Varactor (Varicap Diode)

Varactor (Varicap Diode)
When the junction diode is reverse
biased, the insulating barrier
widens reducing diode capacitance.
The barrier forms the dielectric, of
variable width, of a capacitor.
The N and P type cathode and anode are the two plates of the capacitor.
In the diagram, the diode and coil form a resonant circuit.
The capacitance of the diode, and thereby the resonant frequency, is varied
by means of the potentiometer controlling the reverse voltage across the
varicap.
The capacitor prevents the coil shorting out the voltage across the
potentiometer.

Summary (1)
• Rectifiers convert ac voltage into unipolar voltages.
Half-wave rectifiers do this by passing the voltage in
half of each cycle and blocking the opposite-polarity
voltage in the other half of the cycle.
• The bridge-rectifier circuit is the preferred full-wave
rectifier configuration.
12/10/2022 58

Summary (2)
• The variation of the output waveform of the rectifier is
reduced considerably by connecting a capacitor C across
the output load resistance R. The resulting circuit is the
peak rectifier. The output waveform then consists of a
dc voltage almost equal to the peak of the input sine
wave, Vp, on which is superimposed a ripple component
of frequency 2f (in the full-wave case) and of peak-to-
peak amplitude Vr = Vp/2fRC.
12/10/2022 59

Summary (3)
• Combination of diodes, resistors, and possible reference
voltage can be used to design voltage limiters that prevent
one or both extremities of the output waveform from
going beyond predetermined values – the limiting levels.
• Applying a time-varying waveform to a circuit consisting
of a capacitor in series with a diode and taking the output
across the diode provides a clamping function.
• By cascading a clamping circuit with a peak-rectifier
circuit, a voltage doubler is realized. 12/10/2022 60

Summary (4)
• Beyond a certain value of reverse voltage (that depends
on the diode itself), breakdown occurs and current
increases rapidly with a small corresponding increase in
voltage.
• Diodes designed to operate in the breakdown region
are called zener diodes. They are employed in the
design of voltage regulators whose function is to
provide a constant dc voltage that varies little with
variations in power supply voltage and / or load
current.
12/10/2022 61

Lect 05 Diodes and applications - Part2.pptx

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