Application of Residue Theorem to evaluate real integrations.pptx
Β
Basic electronics - Bi Junction Terminals 02.pptx
1. Chapter 2: BJT and its
applications
Module 2 : Transistor Biasing
Reference:
Robert L. Boylestad, Louis Nashelsky, Electronic Devices & Circuits
Theory, 11th Edition, PHI, 2012
Department of Electronics & Communication Engineering 1
2. Objectives
β’ Discuss the concept of biasing of the transistor.
β’ Analyse the fixed and self bias circuits.
β’ Identify the circuit parameters that effect Q point.
Department of Electronics & Communication Engineering 2
3. Operating Point / Quiescent Point
For the BJT to operate effectively , it has to be properly biased.
Set a certain value of I and V in the BJTβ Biasing
These values correspond to a point on the BJT output characteristics
Department of Electronics & Communication Engineering 3
4. Transistor circuit in Common Emitter Configuration
Applying external dc voltages to ensure
that transistor operates in the desired region.
Applying KVL to the output loop,
ππΆπΆ - πΌπΆπ πΆ -ππΆπΈ=0
ππΆπΈ = ππΆπΆ - πΌπΆπ πΆ ------(1)
πΌπΆ = -
ππΆπΈ
π πΆ
+
ππΆπΆ
π πΆ
---------(2)
Department of Electronics & Communication Engineering 4
5. From equation (1), when πΌπΆ=0,
ππΆπΈ = ππΆπΆ -------------(3)
From equation (2) when ππΆπΈ=0,
πΌπΆ =
ππΆπΆ
π πΆ
-------------(4)
Equation (3) and (4) form the
extremities of πΌπΆ and ππΆπΈ
Line joining these two points β DC Load Line
Department of Electronics & Communication Engineering 5
6. The point where DC load line cuts the output characteristics is called
Quiescent Point (Q Point) / Operating point
Depending on the requirement, Q point can be moved to Saturation, Active
or Cut-off region
To set the Q Point, biasing is necessary
Note: When no biasing is applied, Q point is at the origin
Department of Electronics & Communication Engineering 6
8. Variation in load line with circuit parameters
Department of Electronics & Communication Engineering 8
9. Fixed Bias / Base Current Bias
Applying KVL to input loop,
ππΆπΆ-πΌπ΅π π΅-ππ΅πΈ=0
πΌπ΅ =
ππΆπΆβππ΅πΈ
π π΅
Applying KVL to output loop,
ππΆπΆ-πΌπΆπ πΆ-ππΆπΈ=0
ππΆπΈ = ππΆπΆ-πΌπΆπ πΆ
Department of Electronics & Communication Engineering 9
10. πΌπΆ = Ξ²*πΌπ΅
ππΆπΆ is constant
ππ΅πΈ = 0.7 (for Si)
By selecting proper π π΅ , πΌπ΅ can be
fixed.
ππΆπΈ can also be fixed by selecting
appropriate π πΆ
Department of Electronics & Communication Engineering 10
12. To draw DC Load Line
ππΆπΈπππ₯ = ππΆπΆ =10V
πΌπΆπππ₯ =
ππΆπΆ
π πΆ
= 5mA
Department of Electronics & Communication Engineering 12
π°πͺπππ
ππΆπΈπππ₯
5mA
10V
6.04V
1.978mA
15. Self Bias / Voltage Divider Bias
Uses two resistors π 1 and π 2 instead
of π π΅
π πΈ is the emitter feedback resistance
connected between emitter and
ground.
The circuit can be simplified using
Theveninβs Theorem
Department of Electronics & Communication Engineering 15
18. Theveninβs Resistance
Department of Electronics & Communication Engineering 18
π ππ» is the resistance seen between AB with
ππΆπΆ replaced by a short circuit
π ππ» =
π 1π 2
π 1+π 2
19. Theveninβs Voltage
Department of Electronics & Communication Engineering 19
πππ» is the open circuit voltage
between AB
πππ» =
ππΆπΆβπ 2
π 1+π 2
A
B
20. Self bias circuit with input loop replaced by Theveninβs equivalent
circuit
Apply KVL to the input loop,
πππ» - πΌπ΅π ππ» - ππ΅πΈ - πΌπΈπ πΈ = 0
Substitute πΌπΈ = Ξ² + 1 πΌπ΅
πΌπ΅=
πππ»βππ΅πΈ
π ππ» + (Ξ²+1)π πΈ
Department of Electronics & Communication Engineering 20
21. Since Ξ²+1 β Ξ² and Ξ²π πΈ>> π ππ»
πΌπ΅=
πππ»βππ΅πΈ
Ξ²π πΈ
Collector current πΌπΆ= Ξ²*πΌπ΅
πΌπΆ=
πππ»βππ΅πΈ
π πΈ
πΌπΆ is now independent of Ξ² , where Ξ² is a temperature dependent factor
Department of Electronics & Communication Engineering 21
22. Applying KVL to the output loop,
ππΆπΆ-πΌπΆπ πΆ-ππΆπΈ-πΌπΈπ πΈ=0
ππΆπΈ = ππΆπΆ-πΌπΆπ πΆ-πΌπΈπ πΈ
Department of Electronics & Communication Engineering 22