Semiconductor Diode
Diode is a two terminals nonlinear circuit element.
It has non-linear V-I characteristics whereas resistor has a linear
relationship. P-N junction is formed by simply joining a p-type material and an n-type
material together. Semiconductor diode is made by biasing the P-N junction.
Figure:
(a) P-N junction (b) Diode Symbol and direction.
Joining a p-type material (holes as a majority
carrier) with an n-type material (electrons as a majority carrier) and no bias
is applied to its terminal; this creates a depletion region between the P-N junctions
due to its charge carrier. There is no current flow and diode voltage is zero.
Figure:
(a) Charge distribution under no applied bias (b) Diode symbol and direction.
Reverse bias is introduced by applying an external
voltage such that the positive terminal is connected to the n-type material and
the negative terminal is connected to the p-type material. The negative potential to the p-type material and
the positive terminal to the n-type material create a large number of negative
ions and positive ions respectively. The depletion region becomes wider and there
is no majority carrier flow. Reverse bias current flows due to the majority
carrier and it is called reverse saturation current Is.
Figure:
(a) Internal distribution of charge under reverse bias condition (b) Diode
symbol and direction.
Forward bias is created by applying an external voltage such that the positive terminal is connected to the p-type material and the negative terminal is connected to the n type material. The depletion region is smaller because of the majority carrier flow.
The positive and negative potential to the p-type
material and n-type material break the charge barrier and the diode current
flow. The characteristic of a diode is determined by the Shockley’s equation:
ID=
IS (e^(Vd/nVt) -1) A
Where, ID=Diode current
IS=Reverse
saturation current
Vd =Externally
applied voltage
n= Ideality factor
Vt= Thermal
voltage
Figure:
Si semiconductor diode characteristics
Vt= (KTk/q) (v)
Where, K= Boltzmann’s constant= 1.38˟10-23
J/K
Tk= Absolute
temperature in kelvin = 273+̊C
q= Magnitude of electronic
charge= 1.6˟10-19
C.
v At a temperature 27̊C, determine
the thermal voltage Vt.
Solution:
Tk=
(273+27)K=300 K
Vt= KTk/q =(1.38˟10-23 ˟ 300)/1.6˟10-19
=25.875 mV=26 mV
Application
of semiconductor diode:
Diode is generally used as
1. Rectifier
2. Clipper
3. Clamper
4. Voltage
multiplier
5. Logic
gate maker
For the reverse bias potential in a diode, there is
a sharp change in voltage-current relationship. The current increases at a very
rapid rate in negative voltage region. The reverse bias potential draws an
abrupt change in the characteristics curve is called breakdown potential VBV.
This occurs because the valance electrons absorb the sufficient energy to leave
the parent atom (called ionization process).
The sharp change in the characteristics at any level
of the negative potential is called the Zener region. Zener Breakdown occurs
because there is a strong electric field in the region of the junction that can
disrupt the bounding forces within the atom and generate carriers.
The maximum reverse bias potential that can be
applied before entering the Breakdown region is called the peak inverse voltage
(PIV) or the peak reverse voltage (PRV).
Different semiconductor diode starts to flow current
at a different maximum forward bias potential, which is called knee voltage Vk.
Table:
Knee voltage of semiconductor diode
Semiconductor
|
Vk(V)
|
Ge
|
0.3
|
Si
|
0.7
|
GaAs
|
1.2
|
Temperature
effect
In the forward bias region the characteristics of a
silicon diode shift to the left at a rate of 2.5 mV per centigrade degree
increase in temperature. In the reverse bias region the reverse current of a
silicon diode doubles for every 10 degree centigrade rise in temperature.
The
semiconductor diode acts as a switch. The only difference is that the diode
current flows in a one direction whereas a switch allows the current flow in
both directions.
Diode
equivalent circuit:
The transition capacitance is the predominant
capacitive effect in the reverse bias region whereas the diffusion capacitance
is the predominant capacitive effect in the forward bias region.
Figure:
Transition and diffusion capacitance in the semiconductor diode.
Zener
diode:
Diode showing the sharp change in the characteristics
of a P-N junction is called Zener diode. The higher is the number of adding
impurities the lower is the Zener potential. Zener diode is always set to the
reverse biased.
Figure:
Zener diode characteristics, symbol and direction.
Application
of Zener diode:
ü As
a voltage regulator
ü As
a protective device
ü To
generate square wave
ü To
use in transistor circuit
Difference
between conventional diode and Zener diode:
Diode
|
Zener
diode
|
It
has no definite breakdown voltage.
|
It
has Zener voltage.
|
It
has slightly less impurity material than Zener impurity.
|
It
contains much more impurities than conventional diode impurities.
|
It
does not work at Breakdown region.
|
It
works at breakdown region.
|
It
is connected at forward bias in a circuit.
|
It
is connected at reverse Biased only.
|
It is damaged by the application of extra peak
inverse voltage.
|
It is conducted at a certain amount of reverse
voltage.
|
LED
(light Emitting Diode)
One types of diode that glow visible lights
v It
converts forward current into light.
v At
the modified p-n junction of the LED, the electron changes its energy level;
then the energy is transformed into heat and photon.
SBD
(Schottky-Barrier Diode)
The SBD is formed by bringing material into contract
with a moderately doped n-type semiconductor material.
v The
diode current flows from the metal anode to the semiconductor cathode.
v The
diode acts as an open circuit in the other.
v Current
is conducted by majority carriers (electrons).
v The
forward voltage drop of a conducting SBD is lower than that of a p-n junction
diode.
v Metal
is commonly deposited on the semiconductor surface in order to make terminals
for the semiconductor devices and to connect different devices in an integrated
circuit chip.
Diode
Testing
Ø By
Digital Display Meter (DDM): Determining the ‘ON’ state by estimating the
specific diode forward bias voltage.
Ø By
Ohmmeter Testing: Determining the resistivity for relatively low (short
circuit) or high (open circuit) value with ‘ON’ or ‘OFF’ state respectively.
The ‘ON’ state shows its polarity.
Ø By
Curve Tracer: Tracing diode characteristic curve by positioning the exact
polarity (ON) mode.
Analyze
yourself:
Q1. What do you mean by diode? Draw
the diode characteristic curve.
|
Q2. What is p-n junction? Describe
reverse biasing.
|
Q3. Define: Zener region,
Breakdown voltage, PIV, Knee voltage. Write down the uses of diode.
|
Q4. Draw the diode equivalent
circuits. Distinguish between switch and diode.
|
Q4. Broadly explain the Zener
diode. Differentiate between Zener diode & conventional diode.
|
Q5. Write short note on: 1. LED 2.
SBD 3. Diode testing
|
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