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Chapter 3 SPECIAL PURPOSE DIODE 1

Chapter 3portal.unimap.edu.my/portal/page/portal30/Lecturer Notes... · Chapter 3 SPECIAL PURPOSE DIODE 1. ... department of Physics. He developed the Zener Diode in 1950 and employed

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Chapter 3

SPECIAL PURPOSE DIODE

1

Inventor of Zener Diode

Clarence Melvin Zener was a professor at Carnegie Mellon University in the

department of Physics. He developed the Zener Diode in 1950 and employed it

in modern computer circuits.

2

A Zener is a diode operated in reversebias at the

Zener voltage (VZ).

Common Zener voltages are between 1.8 V and 200 V

Zener Diode

3

Zener Region

The Zener region is in the diode’s

reverse-bias region.

At some point the reverse bias

voltage is so large the diode breaks

down and the reverse current

increases dramatically.increases dramatically.

• The maximum reverse voltage that

won’t take a diode into the zener

region is called the peak inverse

voltage or peak reverse voltage.

• The voltage that causes a diode to enter

the zener region of operation is called

the zener voltage (VZ).

4

Zener Region

Approximate equivalent circuits for the Zener diode in the three

possible regions of application.

5

Zener DiodeTemperature Coefficient

6

Zener Diode

7

Table 1

Zener Diode (Fixed Vi and R)

8

Zener Diode (Fixed Vi, Variable RL)

I

VZRLmax =

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:

ILmin = IR − IZK

The maximum value of resistance is:

LminI

L Lmin

LmaxR R

I ==VL VZ

Zi

RVZ

V −VRLmin =

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:

9

Zener Diode (Variable Vi, Fixed RL)

10

Optical Diodes

There are two popular types of optoelectronic devices:

• light-emitting diode (LED)

• Photodiode

An LED emits photons when it is forward biased. These can be in

the infrared or visible spectrum.

LED is diode that emits light when biased in the forward direction of LED is diode that emits light when biased in the forward direction of

p-n junction.

The forward bias voltage is usually in the range of 2 V to 3V.

11

Anode Cathode

Light-Emitting Diode (LED)

Fig.3–1: The schematic symbol and construction features.

12

Light-Emitting Diode (LED)

Fig.3–2: 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).13

The basic operation of LED is as illustrated in Fig.

3-3:

“When the device is forward-biased, electrons

cross the p-n junction from the n-type material

and recombine with holes in the p-type material.

These free electrons are in the conduction band

and at a higher energy than the holes in the

Light-Emitting Diode (LED)

and at a higher energy than the holes in the

valence band.

When recombination takes place, the recombining

electrons release energy in the form photons.

A large exposed surface area on one layer of the

semiconductive material permits the photons to be

emitted as visible light.”

This process is called electroluminescence.

Various impurities are added during the doping

process to establish the wavelength of the emitted

light. The wavelength determines the color of

visible light.

Fig.3–3: Electroluminescence in a

forward-biased LED.

14

ApplicationThe seven segment display is an example of LEDs use for display of decimal

digits.

Light-Emitting Diode (LED)

Fig.3-4: The 7-segment LED display.15

Multiple diodes can be packaged

together in an integrated circuit (IC).

Common

Anode

Diode Arrays

Common

Cathode

A variety of combinations exist.

16

Photodiode is a p-n junction that can

convert light energy into electrical energy.

It operates in reverse bias voltage (VR), as

shown in Fig. 3-18, where Iλis the reverse

light current.

Photodiode

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:

λI

VR R

R =

Fig.3-5: Photodiode.

17

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

Fig.3-6: Varactor diode symbol

Varactor Diode

Basic Operation

The capacitance of a reverse-biased varactor

junction is found as:

Fig.3-7: Reverse-biased varactor

diode acts as a variable capacitor.

d

AC

ε=

where, C = the total junction capacitance.A = the plate area.ε = the dielectric constant

(permittivity).d = the width of the depletion region

(plate separation). 18

The ability of a varactor to act as a voltage-controlled capacitor is demonstrated in

Fig. 3-7.

Varactor Diode

Fig.3-8: Varactor diode capacitance varies with reverse voltage.

As the reverse-bias voltage increases, the depletion region widens, increasing the

plate separation, thus decreasing the capacitance.

When the reverse-bias voltage decreases, the depletion region narrows, thus

increasing the capacitance. 19

A major application of varactor is in tuning circuits, for example, VHF, UHF, and

satelite receivers utilize varactors. Varactors are also used in cellular communications.

When used in a parallel resonant circuit, as shown in Fig. 3-11, the varactor acts as a

variable capacitor, thus allowing the resonant frequency to be adjusted by a variable

voltage level.

Varactor Diode Application

Fig.3-9: A resonant band-pass filter.

20

The Schottky Diode

A Schottky diode symbol is shown in Fig. 3-10(a). 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

Other Types of Diodes

Instead, it consists of a doped semiconductor (usually n-type) and metal bound

together, as shown in Fig. 3-10(b).

Fig.3-10: (a) Schottky diode symbol and (b) basic internal construction of a

Schottky diode. 21

The Laser Diode

The laser diode (light amplification by stimulated emission of radiation) produces a

monochromatic (single color) light. Laser diodes in conjunction with photodiodes are

used to retrieve data from compact discs.

Other Types of Diodes

Fig.3-11: Basic laser diode construction and operation.

22

The PIN Diode

The pin diode is also used in mostly microwave frequency applications. Its

variable forward series resistance characteristic is used for attenuation,

modulation, and switching. In reverse bias it exhibits a nearly constant

capacitance.

Other Types of Diodes

Fig.3-12: PIN diode23

Current Regulator Diode

Current regulator diodes keeps a constant current value over a specified range of

forward voltages ranging from about 1.5 V to 6 V.

Other Types of Diodes

Fig.3-13: Symbol for a current regulator diode.

24

Although power supply outputs generally use IC regulators, zener diodes can be used as a

voltage regulator when less precise regulation and low current is acceptable.

The meter readings of 15.5

V for no-load check and

14.8 V for full-load test

indicate approximately the

expected output voltage of

Troubleshooting

Fig.3-14: Zener-regulated power supply test.

expected output voltage of

15 V.

A properly functioning

zener will work to

maintain the output

voltage within certain

limits despite changes in

load.

25

In no-load check, output voltage is 24 V as shown in Fig. 3-15(a). This

indicates an open circuit between the output terminal and ground. Therefore,

there is no voltage dropped between the filtered output of the power supply and

the output terminal.

In full-load check, output

voltage is 14.8 V due to the

voltage-divider action of the

Case-1: Diode Zener Open

Figure 3-15: Indications of an open zener.

voltage-divider action of the

180 Ω series resistor and the

291 Ω load.

The result for full-load check is

too close to the normal reading

to be reliable fault indication

and thus, the no-load check is

used to verify the problem.

26

As indicated in Fig. 3-16, no-load check that result in an output voltage greater

than the maximum zener voltage but less than the power supply output voltage

indicates that the zener has failed. The 20 V output in this case is 4.5 V higher

than the expected value of 15.5 V. That additional voltage indicates the zener is

faulty or the wrong type has been installed.

Case-2: Incorrect Zener Voltage

Fig. 3-16: Indication of excessive zener impedance. 27