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1
INTRODUCTION
Department of ECE | VISAT, Elanji
2
CLASSIFICATION OF METALS, CONDUCTORS AND
SEMICONDUCTORS
• On the basis of conductivity
• On the basis of energy bands
3
Department of ECE | VISAT, Elanji
*on the basis of conductivity
The solids are broadly classified as:
(i) Metals: They possess very low resistivity (or high
conductivity).
(ii) Semiconductors: They have resistivity or
conductivity intermediate to metals and
insulators.
(iii) Insulators: They have high resistivity (or low
conductivity).
4
Department of ECE | VISAT, Elanji
*on the basis of conductivity
5
Department of ECE | VISAT, Elanji
* On the basis of energy band
6
Department of ECE | VISAT, Elanji
7
Department of ECE | VISAT, Elanji
Difference between energy bands of
(a) metals,
(b) insulators and
(c) semiconductors.
8
Department of ECE | VISAT, Elanji
CLASSIFICATION OF
SEMICONDUCTOR
SEMICONDUCTOR
9
Department of ECE | VISAT, Elanji
INTRINSIC
SEMICONDUCTOR
Three-dimensional diamond-
like crystal structure for Carbon,
Silicon or Germanium
Schematic two-dimensional
representation of Si or Ge structure showing
covalent bonds at low temperature
(all bonds intact). +4 symbol
indicates inner cores of Si or Ge.
10
Department of ECE | VISAT, Elanji
FIGURE 14.5
(a) Schematic model of generation of hole at site 1 and conduction electron due to thermal energy at
moderate temperatures.
(b) Simplified representation of possible thermal motion of a hole. The electron from the lower left hand
covalent bond (site 2) goes to the earlier hole site1, leaving a hole at its site indicating an apparent movement
of the hole from site 1 to site 2.
11
Department of ECE | VISAT, Elanji
FIGURE 14.6 (a) An intrinsic semiconductor at T = 0 K behaves like
insulator. (b) At T > 0 K, four thermally generated electron-hole pairs. The
filled circles represent electrons and empty fields represent holes.
12
Department of ECE | VISAT, Elanji
EXTRINSIC SEMICONDUCTORS
• Current flow and electron flow
• ADDING IMPURITY TO INCREASE NUMBER OF
ELECTRONS OR HOLES
13
Department of ECE | VISAT, Elanji
EXTRINSIC SEMICONDUCTORS
• P type
• N type
14
Department of ECE | VISAT, Elanji
PERIODIC TABLE OF SEMICONDUCTOR
15
Department of ECE | VISAT, Elanji
P TYPE SEMICONDUCTOR
These are materials which have Trivalent impurity atoms (Acceptors) added
and conduct by "hole" movement and are called, P-type Semiconductors.
In these types of materials are:
1. The Acceptors are negatively charged.
2. There are a large number of holes.
3. A small number of free electrons in relation to the number of holes.
4. Doping gives:
•negatively charged acceptors.
•positively charged holes
5. Supply of energy gives:
•positively charged holes.
•negatively charged free electrons.
and both P and N-types as a whole, are electrically neutral on their own.
Antimony (Sb) and Boron (B) are two of the most commonly used doping
agents as they are more feely available compared to others and are also
classed as metalloids.
16
Department of ECE | VISAT, Elanji
P type Semiconductors
• P-TYPE
• Ex: Boron, Aluminium
17
Department of ECE | VISAT, Elanji
N type Semiconductor
These are materials which have Pentavalent impurity atoms (Donors) added
and conduct by "electron" movement and are called, N-type Semiconductors.
• In these types of materials are:
1. The Donors are positively charged.
2. There are a large number of free electrons.
3. A small number of holes in relation to the number of free electrons.
4. Doping gives:
• positively charged donors.
• negatively charged free electrons.
5. Supply of energy gives:
• negatively charged free electrons.
• positively charged holes.
EX: Antimony,Phosphorous 18
Department of ECE | VISAT, Elanji
N type Semiconductor
• N-type
19
Department of ECE | VISAT, Elanji
ENERGY BAND DIAGRAM
.
(b) p-type semiconductor at T > 0K
20
Department of ECE | VISAT, Elanji
PN JUNCTION
21
Department of ECE | VISAT, Elanji
PN Junction Formation Process
PN Junction Formation
22
Department of ECE | VISAT, Elanji
PN Junction at Equilibrium
(a) Diode underequilibrium (V = 0)
(b) Barrierpotential under no bias. 23
Department of ECE | VISAT, Elanji
Semiconductor Diode
24
Department of ECE | VISAT, Elanji
Types of Semiconductor Diode
25
Department of ECE | VISAT, Elanji
P-N JUNCTION DIODE UNDER
FORWARD BIAS
(a) p-n junction diode under forward bias
(b) Barrier potential
(1) without battery
(2) Low battery voltage
(3) High voltage battery.
Forward bias.
26
Department of ECE | VISAT, Elanji
P-N JUNCTION DIODE UNDER
REVERSE BIAS
Click here
27
Department of ECE | VISAT, Elanji
Animation
28
Department of ECE | VISAT, Elanji
V-I CHARACTERISTICS OF DIODE
Experimental circuit arrangement for studying V-I characteristics of
a p-n junction diode
(a) in forward bias
(b) in reverse bias.
(c) Typical V-I characteristics of a silicon diode
29
Department of ECE | VISAT, Elanji
APPLICATION OF
JUNCTION DIODE AS A
RECTIFIER
30
Department of ECE | VISAT, Elanji
Half Wave Rectifier
Click Here
31
Department of ECE | VISAT, Elanji
FULL WAVE CENTRE TAPPED
(a) A Full-wave rectifier Circuit
(b) Input wave forms given to the diode D1 at A and to the
diode D2 at B
(c) Output waveform across the load RL connected in the
full-wave rectifier circuit.
32
Department of ECE | VISAT, Elanji
(a) A full-wave rectifier with capacitor filter,
(b) Input and output voltage of rectifier in (a)
33
Department of ECE | VISAT, Elanji
SPECIAL PURPOSE PN JUNCTION
DIODES
Zener diode
Vi characteristics of Zener diode 34
Department of ECE | VISAT, Elanji
Zener diode as a voltage regulator
35
Department of ECE | VISAT, Elanji
Optoelectronic Junction Devices
PHOTODIODE
36
Department of ECE | VISAT, Elanji
LIGHT EMITTING DIODE
Advantages of LED
(i) Low operational voltage and less power.
(ii) Fast action and no warm-up time required.
(iii) The bandwidth of emitted light is 100 Å to
500 Å or in other words it is nearly (but not
exactly) monochromatic.
(iv) Long life and ruggedness.
(v) Fast on-off switching capability.
37
Department of ECE | VISAT, Elanji
Solar cell
38
Department of ECE | VISAT, Elanji
(a) Schematic representations of a n-p-n
transistor and p-n-p transistor
(b) Symbols for n-p-n and p-n-p transistors. WORKING VIDEO
Junction Transistor
39
Department of ECE | VISAT, Elanji
PNP Transistor
40
Department of ECE | VISAT, Elanji
NPN Transistor
41
Department of ECE | VISAT, Elanji
Basic transistor circuit configurations and
transistor characteristics
42
Department of ECE | VISAT, Elanji
INPUT CHARACTERISTICS
43
Department of ECE | VISAT, Elanji
OUTPUT CHARACTERISTICS
44
Department of ECE | VISAT, Elanji
AC Parameters Of Transistors
(i) Input resistance (ri): This is defined as the ratio of
change in base emitter voltage (ΔVBE) to the
resulting change in base current (ΔIB) at constant
collector-emitter voltage (VCE). This is dynamic (ac
resistance) and as can be seen from the input
characteristic, its value varies with the operating
current in the transistor:
45
Department of ECE | VISAT, Elanji
(ii) Output resistance (ro): This is defined as the ratio of change in collector-
emitter voltage (ΔVCE) to the change in collector current (ΔIC) at a constant base
current IB.
(iii) Current amplification factor (β ): This is defined as the ratio of
the change in collector current to the change in base current at a
constant collector-emitter voltage (VCE) when the transistor is in
active state.
This is also known as small signal current gain and its value is very large. If
we simply find the ratio of IC and IB we get what is called dc β of the
transistor. Hence,
46
Department of ECE | VISAT, Elanji
Transistor as a device
• AMPLIFIER
• SWITCH
• OSCILLATOR
47
Department of ECE | VISAT, Elanji
Transistor as a switch
48
Department of ECE | VISAT, Elanji
Transistor as an Amplifier
(CE-Configuration)
49
Department of ECE | VISAT, Elanji
Feedback amplifier and
transistor oscillator
50
Department of ECE | VISAT, Elanji
51
Department of ECE | VISAT, Elanji
52
Department of ECE | VISAT, Elanji
53
Department of ECE | VISAT, Elanji
54
Department of ECE | VISAT, Elanji
55
Department of ECE | VISAT, Elanji
56
Department of ECE | VISAT, Elanji
57
Department of ECE | VISAT, Elanji
INTEGRATED CIRCUITS
Depending on nature of input signals, IC’s can be grouped in two categories: (a)
linear or analogue IC’s and (b) digital IC’s.
• The linear IC’s process analogue signals which change smoothly and continuously
over a range of values between a maximum and a minimum. The output is more or
less directly proportional to the input, i.e., it varies linearly with the input. Ex:
operational amplifier.
• The digital IC’s process signals that have only two values. They contain circuits
such as logic gates.
Depending upon the level of integration (i.e., the number of circuit components or
logic gates), the ICs are termed as
• Small Scale Integration, SSI (logic gates < 10);
• Medium Scale Integration, MSI (logic gates < 100);
• Large Scale Integration, LSI (logic gates < 1000);
• Very Large Scale Integration, VLSI (logic gates >1000).
58
Department of ECE | VISAT, Elanji
59

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Classification and Working of Semiconductors

  • 1. 1
  • 2. INTRODUCTION Department of ECE | VISAT, Elanji 2
  • 3. CLASSIFICATION OF METALS, CONDUCTORS AND SEMICONDUCTORS • On the basis of conductivity • On the basis of energy bands 3 Department of ECE | VISAT, Elanji
  • 4. *on the basis of conductivity The solids are broadly classified as: (i) Metals: They possess very low resistivity (or high conductivity). (ii) Semiconductors: They have resistivity or conductivity intermediate to metals and insulators. (iii) Insulators: They have high resistivity (or low conductivity). 4 Department of ECE | VISAT, Elanji
  • 5. *on the basis of conductivity 5 Department of ECE | VISAT, Elanji
  • 6. * On the basis of energy band 6 Department of ECE | VISAT, Elanji
  • 7. 7 Department of ECE | VISAT, Elanji
  • 8. Difference between energy bands of (a) metals, (b) insulators and (c) semiconductors. 8 Department of ECE | VISAT, Elanji
  • 10. INTRINSIC SEMICONDUCTOR Three-dimensional diamond- like crystal structure for Carbon, Silicon or Germanium Schematic two-dimensional representation of Si or Ge structure showing covalent bonds at low temperature (all bonds intact). +4 symbol indicates inner cores of Si or Ge. 10 Department of ECE | VISAT, Elanji
  • 11. FIGURE 14.5 (a) Schematic model of generation of hole at site 1 and conduction electron due to thermal energy at moderate temperatures. (b) Simplified representation of possible thermal motion of a hole. The electron from the lower left hand covalent bond (site 2) goes to the earlier hole site1, leaving a hole at its site indicating an apparent movement of the hole from site 1 to site 2. 11 Department of ECE | VISAT, Elanji
  • 12. FIGURE 14.6 (a) An intrinsic semiconductor at T = 0 K behaves like insulator. (b) At T > 0 K, four thermally generated electron-hole pairs. The filled circles represent electrons and empty fields represent holes. 12 Department of ECE | VISAT, Elanji
  • 13. EXTRINSIC SEMICONDUCTORS • Current flow and electron flow • ADDING IMPURITY TO INCREASE NUMBER OF ELECTRONS OR HOLES 13 Department of ECE | VISAT, Elanji
  • 14. EXTRINSIC SEMICONDUCTORS • P type • N type 14 Department of ECE | VISAT, Elanji
  • 15. PERIODIC TABLE OF SEMICONDUCTOR 15 Department of ECE | VISAT, Elanji
  • 16. P TYPE SEMICONDUCTOR These are materials which have Trivalent impurity atoms (Acceptors) added and conduct by "hole" movement and are called, P-type Semiconductors. In these types of materials are: 1. The Acceptors are negatively charged. 2. There are a large number of holes. 3. A small number of free electrons in relation to the number of holes. 4. Doping gives: •negatively charged acceptors. •positively charged holes 5. Supply of energy gives: •positively charged holes. •negatively charged free electrons. and both P and N-types as a whole, are electrically neutral on their own. Antimony (Sb) and Boron (B) are two of the most commonly used doping agents as they are more feely available compared to others and are also classed as metalloids. 16 Department of ECE | VISAT, Elanji
  • 17. P type Semiconductors • P-TYPE • Ex: Boron, Aluminium 17 Department of ECE | VISAT, Elanji
  • 18. N type Semiconductor These are materials which have Pentavalent impurity atoms (Donors) added and conduct by "electron" movement and are called, N-type Semiconductors. • In these types of materials are: 1. The Donors are positively charged. 2. There are a large number of free electrons. 3. A small number of holes in relation to the number of free electrons. 4. Doping gives: • positively charged donors. • negatively charged free electrons. 5. Supply of energy gives: • negatively charged free electrons. • positively charged holes. EX: Antimony,Phosphorous 18 Department of ECE | VISAT, Elanji
  • 19. N type Semiconductor • N-type 19 Department of ECE | VISAT, Elanji
  • 20. ENERGY BAND DIAGRAM . (b) p-type semiconductor at T > 0K 20 Department of ECE | VISAT, Elanji
  • 21. PN JUNCTION 21 Department of ECE | VISAT, Elanji
  • 22. PN Junction Formation Process PN Junction Formation 22 Department of ECE | VISAT, Elanji
  • 23. PN Junction at Equilibrium (a) Diode underequilibrium (V = 0) (b) Barrierpotential under no bias. 23 Department of ECE | VISAT, Elanji
  • 25. Types of Semiconductor Diode 25 Department of ECE | VISAT, Elanji
  • 26. P-N JUNCTION DIODE UNDER FORWARD BIAS (a) p-n junction diode under forward bias (b) Barrier potential (1) without battery (2) Low battery voltage (3) High voltage battery. Forward bias. 26 Department of ECE | VISAT, Elanji
  • 27. P-N JUNCTION DIODE UNDER REVERSE BIAS Click here 27 Department of ECE | VISAT, Elanji
  • 29. V-I CHARACTERISTICS OF DIODE Experimental circuit arrangement for studying V-I characteristics of a p-n junction diode (a) in forward bias (b) in reverse bias. (c) Typical V-I characteristics of a silicon diode 29 Department of ECE | VISAT, Elanji
  • 30. APPLICATION OF JUNCTION DIODE AS A RECTIFIER 30 Department of ECE | VISAT, Elanji
  • 31. Half Wave Rectifier Click Here 31 Department of ECE | VISAT, Elanji
  • 32. FULL WAVE CENTRE TAPPED (a) A Full-wave rectifier Circuit (b) Input wave forms given to the diode D1 at A and to the diode D2 at B (c) Output waveform across the load RL connected in the full-wave rectifier circuit. 32 Department of ECE | VISAT, Elanji
  • 33. (a) A full-wave rectifier with capacitor filter, (b) Input and output voltage of rectifier in (a) 33 Department of ECE | VISAT, Elanji
  • 34. SPECIAL PURPOSE PN JUNCTION DIODES Zener diode Vi characteristics of Zener diode 34 Department of ECE | VISAT, Elanji
  • 35. Zener diode as a voltage regulator 35 Department of ECE | VISAT, Elanji
  • 37. LIGHT EMITTING DIODE Advantages of LED (i) Low operational voltage and less power. (ii) Fast action and no warm-up time required. (iii) The bandwidth of emitted light is 100 Å to 500 Å or in other words it is nearly (but not exactly) monochromatic. (iv) Long life and ruggedness. (v) Fast on-off switching capability. 37 Department of ECE | VISAT, Elanji
  • 38. Solar cell 38 Department of ECE | VISAT, Elanji
  • 39. (a) Schematic representations of a n-p-n transistor and p-n-p transistor (b) Symbols for n-p-n and p-n-p transistors. WORKING VIDEO Junction Transistor 39 Department of ECE | VISAT, Elanji
  • 40. PNP Transistor 40 Department of ECE | VISAT, Elanji
  • 41. NPN Transistor 41 Department of ECE | VISAT, Elanji
  • 42. Basic transistor circuit configurations and transistor characteristics 42 Department of ECE | VISAT, Elanji
  • 45. AC Parameters Of Transistors (i) Input resistance (ri): This is defined as the ratio of change in base emitter voltage (ΔVBE) to the resulting change in base current (ΔIB) at constant collector-emitter voltage (VCE). This is dynamic (ac resistance) and as can be seen from the input characteristic, its value varies with the operating current in the transistor: 45 Department of ECE | VISAT, Elanji
  • 46. (ii) Output resistance (ro): This is defined as the ratio of change in collector- emitter voltage (ΔVCE) to the change in collector current (ΔIC) at a constant base current IB. (iii) Current amplification factor (β ): This is defined as the ratio of the change in collector current to the change in base current at a constant collector-emitter voltage (VCE) when the transistor is in active state. This is also known as small signal current gain and its value is very large. If we simply find the ratio of IC and IB we get what is called dc β of the transistor. Hence, 46 Department of ECE | VISAT, Elanji
  • 47. Transistor as a device • AMPLIFIER • SWITCH • OSCILLATOR 47 Department of ECE | VISAT, Elanji
  • 48. Transistor as a switch 48 Department of ECE | VISAT, Elanji
  • 49. Transistor as an Amplifier (CE-Configuration) 49 Department of ECE | VISAT, Elanji
  • 50. Feedback amplifier and transistor oscillator 50 Department of ECE | VISAT, Elanji
  • 51. 51 Department of ECE | VISAT, Elanji
  • 52. 52 Department of ECE | VISAT, Elanji
  • 53. 53 Department of ECE | VISAT, Elanji
  • 54. 54 Department of ECE | VISAT, Elanji
  • 55. 55 Department of ECE | VISAT, Elanji
  • 56. 56 Department of ECE | VISAT, Elanji
  • 57. 57 Department of ECE | VISAT, Elanji
  • 58. INTEGRATED CIRCUITS Depending on nature of input signals, IC’s can be grouped in two categories: (a) linear or analogue IC’s and (b) digital IC’s. • The linear IC’s process analogue signals which change smoothly and continuously over a range of values between a maximum and a minimum. The output is more or less directly proportional to the input, i.e., it varies linearly with the input. Ex: operational amplifier. • The digital IC’s process signals that have only two values. They contain circuits such as logic gates. Depending upon the level of integration (i.e., the number of circuit components or logic gates), the ICs are termed as • Small Scale Integration, SSI (logic gates < 10); • Medium Scale Integration, MSI (logic gates < 100); • Large Scale Integration, LSI (logic gates < 1000); • Very Large Scale Integration, VLSI (logic gates >1000). 58 Department of ECE | VISAT, Elanji
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