The document discusses electronic devices and circuits, specifically focusing on PN diodes. It describes the theory of PN junctions, how a PN junction forms a diode, and the characteristics and properties of PN diode currents and voltages. It discusses topics like volt-amp characteristics, temperature effects, and switching times of PN diodes. It also provides explanations and circuit diagrams of half-wave and full-wave rectifiers, zener diodes, liquid crystal displays, and series voltage regulators.

1. Electronic devices and circuits
UNIT – I
PN- DIODE

2. SEMICONDUCTOR DIODE
• Theory of p-n junction
• p-n junction as diode
• p-n diode currents
• Volt-amp characteristics
• Diode resistance
• Temperature effect of p-n junction
• Transition and diffusion capacitance of p-n
diode
• Diode switching times

3. Theory of p-n junction
• When a p-type semiconductor material is
suitably joined to n-type semiconductor
the contact surface is called a p-n junction.
• P N
+ +
Depletion region

4. p-n junction as diode
• The p-n junction is also called as
semiconductor diode .
• The left side material is a p-type
semiconductor having –ve acceptor ions
and +vely charged holes. The right side
material is n-type semiconductor having
+ve donor ions and free electrons

5. p-n junction as diode
• Suppose the two pieces are suitably treated to
form pn junction, then there is a tendency for the
free electrons from n-type to diffuse over to the
p-side and holes from p-type to the n-side . This
process is called diffusion
• The left side material is a p-type semiconductor
having –ve acceptor ions and +vely charged
holes. The right side material is n-type
semiconductor having +ve donor ions and free
electrons.

6. p-n junction as diode
• As the free electrons move across the
junction from n-type to p-type, +ve donor
ions are uncovered. Hence a +ve charge
is built on the n-side of the junction. At the
same time, the free electrons cross the
junction and uncover the –ve acceptor
ions by filling in the holes. Therefore a net
–ve charge is established on p-side of the
junction.

7. p-n junction as diode
• When a sufficient number of donor and acceptor
ions is uncovered further diffusion is prevented.
• Thus a barrier is set up against further
movement of charge carriers. This is called
potential barrier or junction barrier Vo. The
potential barrier is of the order of 0.1 to 0.3V.
• Note: outside this barrier on each side of the
junction, the material is still neutral. Only inside
the barrier, there is a +ve charge on n-side and
–ve charge on p-side. This region is called
depletion layer.

8. p-n diode currents
• Diode current equation
• The current in a diode is given by the diode current equation
• I = I0 ( e V/ηVT –1)
Where, I------ diode current
• I0------ reverse saturation current
• V------ diode voltage
• η------- semiconductor constant
• =1 for Ge, 2 for Si.
• VT------ Voltage equivalent of temperature= T/11,600
(Temperature T is in Kelvin)
• Note----- If the temperature is given in 0C then it can be converted to
Kelvin by the help of following relation, 0C+273 = K

9. Volt-amp characteristics
R
A
V diode
VF
Knee voltage
VR
IR(μA )
IF(mA)
Break over
Voltage
V

10. Volt-amp characteristics
• The supply voltage V is a regulated power supply, the
diode is forward biased in the circuit shown. The resistor
R is a current limiting resistor. The voltage across the
diode is measured with the help of voltmeter and the
current is recorded using an ammeter.
• By varying the supply voltage different sets of voltage
and currents are obtained. By plotting these values on a
graph, the forward characteristics can be obtained. It can
be noted from the graph the current remains zero till the
diode voltage attains the barrier potential.
• For silicon diode, the barrier potential is 0.7 V and for
Germanium diode, it is 0.3 V. The barrier potential is also
called as knee voltage or cur-in voltage.

11. Diode equivalent circuit
• It is generally profitable to replace a
device or system by its equivalent circuit.
Once the device is replaced by its
equivalent circuit, the resulting network
can be solved by traditional circuit analysis
technique.
VF rf
Vo
switch
VF

12. Diode resistance
• Static Resistance
– Forward Resistance Rf
– Reverse Resistance Rr
• Dynamic Resistance
– Forward Resistance rf
– Reverse Resistance rr

13. Temperature effect of p-n
junction
• The current in a diode is given by the diode current
equation
• I = I0( e V/ηVT –1)
• Where, I------ diode current
• I0------ reverse saturation current
• V------ diode voltage
• η------- semiconductor constant
• =1 for Ge, 2 for Si.
• VT------ Voltage equivalent of temperature=
T/11,600 (Temperature T is in Kelvin)
• Note----- If the temperature is given in 0C then it can be
converted to Kelvin by the help of following relation,
0C+273 = K

14. HALFWAVE RECTIFIER

15. HALFWAVE RECTIFIER
• The primary of the transformer is connected to
ac supply. This induces an ac voltage across the
secondary of the transformer.
• During the positive half cycle of the input voltage
the polarity of the voltage across the secondary
forward biases the diode. As a result a current IL
flows through the load resistor, RL. The forward
biased diode offers a very low resistance and
hence the voltage

16. HALFWAVE RECTIFIER
• Drop across it is very small. Thus the voltage
appearing across the load is practically the same
as the input voltage at every instant.
• During the negative half cycle of the input
voltage the polarity of the secondary voltage
gets reversed. As a result, the diode is reverse
biased.
• Practically no current flows through the circuit
and almost no voltage is developed across the
resistor. All input voltage appears across the
diode itself.

17. HALFWAVE RECTIFIER
• Hence we conclude that when the input voltage
is going through its positive half cycle, output
voltage is almost the same as the input voltage
and during the negative half cycle no voltage is
available across the load.
• This explains the unidirectional pulsating dc
waveform obtained as output. The process of
removing one half the input signal to establish a
dc level is aptly called half wave rectification.

18. HALFWAVE RECTIFIER
Peak Inverse Voltage
• When the input voltage reaches its maximum
value Vm during the negative half cycle the
voltage across the diode is also maximum. This
maximum voltage is known as the peak inverse
voltage.
Thus for a half wave rectifier
Let Vi be the voltage to the primary of the
transformer. Vi is given by
where Vr is the cut-in voltage of the diode.

19. Half wave waveform

20. HALFWAVE RECTIFIER
Ripple Factor
• Ripple factor is defined as the ratio of rms
value of ac component to the dc
component in the output.
Ripple factor

21. HALFWAVE RECTIFIER
The ripple is

22. HALFWAVE RECTIFIER
Vav the average or the dc content of the
voltage across the load is given by

23. HALFWAVE RECTIFIER
RMS voltage at the load resistance can be
calculated as

24. HALFWAVE RECTIFIER
Ripple Factor

25. HALFWAVE RECTIFIER
Efficiency Efficiency, is the ratio of the dc
output power to ac input power

26. Full Wave Bridge Rectifier

27. The waveform of fullwave rectifier is

28. Zener Diode
• Zener Diode : Works in the break down
region when subjected to reverse bias.
• Large variation in current. Voltage almost
constant.
• Used for voltage regulation. Upper limit of
current depends on the power dissipation
rating of the device.

29. Zener Diode
Zener diode

30. Light Emitting Diode
Light emitting diodes (LEDs)
• The Light Emitting Diode (LED) is a
common light source used in electronic
circuits.
• LED is a semiconductor diode that emits
light when current passes through it.

31. • The circuit symbol is of light emmitting
Diode is

32. • The characteristics of the LED are similar
to other semiconductor diodes except the
operating
• voltage is higher.
• A typical LED has an operating voltage of
2.0V and a maximum current of 30mA.

33. • When the LED is to be operated from a
circuit voltage supply, a resistor will be
required in
• series with the LED to ensure the correct
current and voltage for the LED.
• Consider an LED operating from a +5V
power supply and has 20mA flowing
through it …..
• the value for the resistor (R) will be 150W.

34. LIQUID CRYSTAL DISPLAY
LIQUID CRYSTAL DISPLAY - They are
used for display of numeric and
alphanumeric character in dot matrix and
segmental display.

35. • What is a Liquid Crystal?
Liquid Crystal – a stable phase of matter
characterized by anisotropic properties
without the existence of a 3-dimensional
crystal lattice – generally lying between
the solid and isotropic (“liquid”) phase.

36. • Nematic • Smectic
There are 2 basic phases

37. Liquid Crystal Model

38. Series voltage regulator
In a voltage regulator circuit , if the control
elements are connected in series with load
it is called series voltage regulator .

39. Series voltage regulator

40. • Zener diode is a diode that block current until a
specified voltage is applied. Remember also that
the applied voltage is called the breakdown, or
Zener voltage. Zener diodes are available with
different Zener voltages. When the Zener
voltage is reached, the Zener diode conducts
from its anode to its cathode (with the direction
of the arrow).
• In this voltage regulator, Q1 has a constant
voltage applied to its base.

41. This voltage is often called the reference
voltage. As changes in the circuit output
voltage occur, they are sensed at the
emitter of Q1 producing a corresponding
change in the forward bias of the
transistor.
In other words, Q1 compensates by
increasing or decreasing its resistance in
order to change the circuit voltage
division.

42. V-I Characteristics of Zener
Diode

43. V-I Characteristics of Zener
Diode
• Zener diodes are manufactured to have a
very low reverse bias breakdown voltage
• Since the breakdown at the zener voltage
is so sharp, these devices are often used
in voltage regulators to provide precise
voltage references. The actual zener
voltage is device dependent. For example,
you can buy a 6V zener diode.

44. THANK U