Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.

Slides:



Advertisements
Similar presentations
TRANSISTOR BJT : DC BIASING.
Advertisements

Bipolar Junction Transistor Circuit Analysis
Lecture 07 DC and AC Load Line
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Recommended Books Robert Boylestad and Louis Nashelsky, “Electronic Devices and Circuit Theory”, Prentice Hall, 7th Edition or Latest. Thomas L. Floyd,
COMSATS Institute of Information Technology Virtual campus Islamabad
BIPOLAR JUNCTION TRANSISTORS (BJTs)
Pnp transistor ECE Electronics - Dr. S. Kozaitis- Florida Institute of Technology – Fall 2002.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
COMSATS Institute of Information Technology Virtual campus Islamabad
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Chapter 7 DC Biasing Circuits
Transistors They are unidirectional current carrying devices with capability to control the current flowing through them The switch current can be controlled.
Bipolar Junction Transistors
Dr. Nasim Zafar Electronics 1: EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Chapter 4 DC Biasing – Bipolar Junction Transistors (BJTs)
Electronic Devices and Circuit Theory
BJT Fixed Bias ENGI 242 ELEC 222. January 2004ENGI 242/ELEC 2222 BJT Biasing 1 For Fixed Bias Configuration: Draw Equivalent Input circuit Draw Equivalent.
Chapter 6: Bipolar Junction Transistors
Department of Electronics and Communication Engineering, Manipal Institute of Technology, Manipal, INDIA Subject Code : ECE – 101/102 BASIC ELECTRONICS.
COMSATS Institute of Information Technology Virtual campus Islamabad
Voltage Divider Bias ENGI 242 ELEC February 2005ENGI 242/ELEC 2222 BJT Biasing 3 For the Voltage Divider Bias Configurations Draw Equivalent Input.
0 Chap. 4 BJT transistors Widely used in amplifier circuits Formed by junction of 3 materials npn or pnp structure.
Chapter 4 DC Biasing–BJTs. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices and.
Chapter 5 Transistor Bias Circuits
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Biasing Biasing: Application of dc voltages to establish a fixed level of current and voltage. BJT Biasing Circuits: Fixed Bias Circuit Fixed Bias with.
BJT amplifier & small-signal concept
Introduction to BJT Amplifier BJT (Review). Still remember about BJT? The emitter current (i E ) is the sum of the collector current (i C ) and the base.
Chapter 5 Transistor Bias Circuits. Objectives  Discuss the concept of dc biasing of a transistor for linear operation  Analyze voltage-divider bias,
Transistor Circuit DC Bias Part 1 ENGI 242. February 2003ENGI 2422 DC Biasing Circuits Fixed-Bias Circuit Emitter-Stabilized Bias Circuit Collector-Emitter.
1 TRANSISTOR AMPLIFIER CONFIGURATION -BJT Common-Emitter Amplifier- By: Syahrul Ashikin Azmi School of Electrical System Engineering.
Recall Last Lecture Introduction to BJT 3 modes of operation Cut-off Active Saturation Active mode operation of NPN.
Chapter 4 Bipolar Junction Transistors
Chapter 5 Transistor Bias Circuits
1 LECTURE 1: SMALL-SIGNAL HYBRID-Π EQUIVALENT CIRCUIT OF BIPOLAR TRANSISTOR (BJT) By: Syahrul Ashikin Azmi PPKSE.
Chapter 4(b) DC Biasing – Bipolar Junction Transistors (BJTs)
Chapter 4 DC Biasing–BJTs. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices and.
Prepared by: Garima Devpriya ( ) Jamila Kharodawala ( ) Megha Sharma ( ) ELECTRONICS DEVICES AND CIRCUITS G.H.Patel.
Load Line & BJT Biasing. DC Biasing To establish a constant dc collector current in the BJT. Biasing is required to operate the transistor in the linear.
BJT Bipolar Junction Transistors (BJT) Presented by D.Satishkumar Asst. Professor, Electrical & Electronics Engineering
Lecture 10:Load Line & BJT Biasing CSE251. DC Biasing To establish a constant dc collector current in the BJT. Biasing is required to operate the transistor.
Chapter 5 Transistor Bias Circuits. Objectives  Discuss the concept of dc biasing of a transistor for linear operation  Analyze voltage-divider bias,
The Bipolar Junction Transistor
Emitter-Stabilized Bias Circuit Load Line Analysis.
BJT transistors Summary of DC problem 2 Bias transistors so that they operate in the linear region B-E junction forward biased, C-E junction reversed.
ITM UNIVERSE,VADODARA ELECTRONIC DEVICES & CIRCUITS TOPIC NAME TRANSISTOR BIASING (DC ANALYSIS) PREPARED BY: NAME: Dilsha Dharmajan Electronics & communication.
Electronics Technology Fundamentals Chapter 19 Bipolar Junction Transistor Operation and Biasing.
Chapter 4 DC Biasing–BJTs. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices and.
DC Biasing - BJTs Chapter 4 Boylestad Electronic Devices and Circuit Theory.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Chapter 4 Bipolar junction transistor Ir. Dr. Rosemizi Abd Rahim 1 Ref: Electronic Devices and Circuit Theory, 10/e, Robert L. Boylestad and Louis Nashelsky.
Chapter 5 Transistor bias circuits Ir. Dr. Rosemizi Abd Rahim 1 Ref: Electronic Devices and Circuit Theory, 10/e, Robert L. Boylestad and Louis Nashelsky.
Chapter 4 DC Biasing–BJTs
Recall Lecture 10 Introduction to BJT 3 modes of operation
Recall Last Lecture Biasing of BJT Three types of biasing
Lecture 07 DC and AC Load Line
Lecture 10 Bipolar Junction Transistor (BJT)
Chapter 4(c) DC Biasing – Bipolar Junction Transistors (BJTs)
Chapter 1 – Revision Part 2
ME3000 ANALOG ELECTRONICS [Slide 3] DC Biasing BY DREAMCATCHER
Electronics Fundamentals
Recall Lecture 10 Introduction to BJT 3 modes of operation
Recall Last Lecture Voltage Transfer Characteristic
ChapTer FoUr DC BIASING - BIPOLAR JUNCTION TRANSISTORS (BJTs)
ChapTer FoUr DC BIASING - BIPOLAR JUNCTION TRANSISTORS (BJTs)
DC Biasing Circuits.
Presentation transcript:

Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad

Potential-Divider-Biasing Circuits: Examples and Exercises.. Lecture No: 19 Contents:  Base-Biased (Fixed Bias) Transistor Circuits.  Voltage-Divider-Bias transistor Circuits.  Examples and Exercises. Nasim Zafar2

References:  Microelectronic Circuits: Adel S. Sedra and Kenneth C. Smith.  Integrated Electronics : Jacob Millman and Christos Halkias (McGraw-Hill).  Introductory Electronic Devices and Circuits Robert T. Paynter  Electronic Devices : Thomas L. Floyd ( Prentice Hall ). Nasim Zafar3

Basic Circuits of BJT: NPN Transistor Nasim Zafar4 I E = I C + I B

Transistor Output Characteristics: 5Nasim Zafar

Transistor Output Characteristics: Load Line – Biasing and Stability:  Active region: – BJT acts as a signal amplifier. – B-E junction is forward biased and C-B junction is reverse biased.  Graphical construction for determining the dc collector current I C and the collector-to-emitter voltage V CE.  The requirement is to set the Q-point such that that it does not go into the saturation or cutoff regions when an a ac signal is applied.  Maximum signal swing depends on the bias voltage. Nasim Zafar6

The DC Operating Point: Biasing and Stability  Active region - Amplifier: BJT acts as a Signal Amplifier. 1. B-E Junction Forward Biased V BE ≈ 0.7 V for Si 2. B-C Junction Reverse Biased 3. KCL: I E = I C + I B C B E IBIB IEIE ICIC C B E IBIB IEIE ICIC 7Nasim Zafar

The DC Operating Point: Biasing and Stability Slope of the Load Line: V CC = V CE + V RC V CE = V CC - V RC V CE = V CC - I C R C 8Nasim Zafar

9 Current Equations in a BJT: NPN Transistor  Collector Current  Base Current  Emitter Current 9Nasim Zafar

1. Fixed-Biased Transistor Circuits. Base-Biased (Fixed Bias) Transistor Circuit: Single Power Supply 10Nasim Zafar

11 Base-Biased (Fixed Bias) Transistor Circuit: Advantage: Circuit simplicity. Disadvantage: Q-point shifts with temp. Applications: Switching circuits only. Circuit Recognition: A single resistor R B between the base terminal and V CC. No emitter resistor. Nasim Zafar Circuit Characteristics - 1:

12 Base-Biased (Fixed Bias) Transistor Circuit: Circuit Characteristics - 2: Load line equations: Q-point equations: Nasim Zafar

13 Base-Biased (Fixed Bias) Transistor Circuit: Q-point equations: Nasim Zafar 1. Base–Emitter Loop: V CC = V BE + I B R B

14 Base-Biased (Fixed Bias) Transistor Circuit:  = dc current gain = h FE Nasim Zafar 2. Collector–Emitter Loop: V CC = V CE + V RC V CE = V CC - I C R

15 Circuit 19.1; Example 19.1 Nasim Zafar

16 Example 19.2 Construct the DC Load line for circuit 19.1; shown in slide 12, and plot the Q-point from the values obtained in Example Determine whether the circuit is midpoint biased. Nasim Zafar The circuit is midpoint biased.

17 Example 19.3 (Q-point Shift.) The transistor of Circuit 19.1, has values of h FE = 100 when T = 25 °C and h FE = 150 when T = 100 °C. Determine the Q-point values of I C and V CE at both of these temperatures. Temp(°C)I B (mA)I C (mA)V CE (V) Nasim Zafar

3. 2. Voltage-Divider-Bias Circuits. 18Nasim Zafar

Voltage-Divider Bias Circuits: NPN Transistor.  Voltage-divider biasing is the most common form of transistor biasing used. A thorough understanding of the dc analysis of this circuit is essential for an electronic technician.  In the Circuit, R1 and R2 set up a voltage divider on the base. Notice the similarity to the emitter-biased circuit. Nasim Zafar19

20 Voltage-Divider Bias Characteristics-(1) Circuit Recognition: The voltage divider in the base circuit. Advantages: The circuit Q- point values are stable against changes in h FE. Disadvantages: Requires more components than most other biasing circuits. Applications: Used primarily to bias linear amplifier. Nasim Zafar

21 Voltage-Divider Bias Characteristics-(2) The Thevenin voltage: Nasim Zafar

22 Voltage-Divider Bias Characteristics-(3) Load line equations: Q-point equations (assume that h FE R E > 10R 2 ): Nasim Zafar

23 Circuit 19.2; Example 19.4 (a). Determine the values of I CQ and V CEQ for the circuit 19.2 shown in Fig below: Because I I E (or h FE >> 1), Nasim Zafar

24 Circuit 19.2; Example 19.4 (b). Verify that I 2 > 10 I B. Nasim Zafar

25 Example 19.5 A voltage-divider bias circuit has the following values: R 1 = 1.5 kW, R 2 = 680 W, R C = 260 W, R E = 240 W and V CC = 10 V. Assuming the transistor is a 2N3904, determine the value of I B for the circuit. Nasim Zafar

26 Load Line for Voltage Divider Bias Circuit. Example 19.5 Nasim Zafar

27 Which value of h FE do we use? Transistor specification sheet may list any combination of the following h FE : max. h FE, min. h FE, or typ. h FE. Use typical value if there is one. Otherwise, use Nasim Zafar

28 Stability of Voltage Divider Bias Circuit:  The Q-point of voltage divider bias circuit is less dependent on h FE than that of the base bias (fixed bias).  For example, if I E is exactly 10 mA, the range of h FE is 100 to 300. Then I CQ hardly changes over the entire range of h FE. Nasim Zafar

Voltage-Divider Bias Circuit: Circuit-19.3; Problem 19.6 (a).  Find the operating point Q for this circuit.  The use of Thevenin equivalent circuit for the base makes the circuit simpler. Nasim Zafar29

Determination of V BB – The Thevenin Voltage V CC = I.(R 1 + R 2 ) -- Eq. (1) V Thev = I.R 2 Eq. (2) -- Eq. (3) Nasim Zafar30

Circuit-19.3; Problem 19.6 (a) Determination of V BB From Eq (3) V Thev = 2 Volts Nasim Zafar31

Circuit-19.3; Problem 19.6 (b). Determination of V RE Input Loop with R E V BB = V BE + V RE V RE = V BB – V BE V RE = 2V - 0.7V V RE = 1.3V Nasim Zafar32

Circuit-19.3; Problem 19.6 (c). Determination of I E V RE = I E R E Nasim Zafar33

Circuit-19.3; Problem 19.6 (d). Determination of V RC Since I E ≈ I C I E = 1.3mA Therefore, I C = 1.3mA V RC = I C R C = (1.3mA)(4x10 3 Ω) V RC = 5.2V Nasim Zafar34

Circuit-19.3; Problem 19.6 (e). Determination of V CE Output Loop V CC =V RC +V CE +V RE V CE = V CC -V RC -V RE V CE = 12V - 5.2V - 1.3V V CE = 5.5V Nasim Zafar35

Results of Problem 19.6 I E = I C = 1.3mA V RC = 5.2V V CE = 5.5V V RE = 1.3V V BB = 2V β dc was never used in a calculation. Hence, voltage-divider biased circuits are immune to changes in β dc. A single voltage source supplies both voltages, V CC and V BB Nasim Zafar36

Review of equations: In Review V RE = V BB – V BE I E ≈ I C Nasim Zafar37

Summary:  Voltage-divider biased circuits are immune to changes in β dc.  A single voltage source supplies both voltages, V CC and V BB  The circuit Q-point values are stable against changes in h FE.  Use of the Thevenin equivalent circuit for the base makes the circuit simpler.  Make the current in the voltage divider about 10 times IB, to simplify the analysis.  For design, solve for the resistor values (IC and VC specified). Nasim Zafar38

Nasim Zafar39

Circuit 19.4; Problem 19.7 (a). Given: V B = 3V and I = 0.2mA. IBIB I (a) RB1 and RB2 form a voltage divider. Assume I >> IB I = V CC /(R B1 + R B2 ) 0.2mA = 9 /(R B1 + R B2 ) 40 Nasim Zafar

Circuit 19.4; Problem 19.7 (b). Given: V B = 3V and I = 0.2mA. R B1 = 30K , and R B2 = 15K . IBIB I V B = V CC [R B2 /(R B1 + R B2 )] 3 = 9 [R B2 /(R B1 + R B2 )], Solve for R B1 and R B2. 41 Nasim Zafar (b) Determination of the Thevenin voltage:

Prob (c). Find the operating point The use of Thevenin equivalent circuit for the base makes the circuit simpler. V BB = V B = 3V R BB = R B1 || R B2 = 30K  15K  10K  42Nasim Zafar

Problem 19.7 (d). Write B-E loop and C-E loop B-E loop C-E loop B-E Voltage Loop: V BB = V RBB + V BE + V R E V BB = I B R BB + V BE + I E R E I E =2.09 mA C-E Voltage Loop: V CC = I C R C + V CE + I E R E V CE =4.8 V This is how all DC circuits are analyzed and designed! 43Nasim Zafar

44

Example 19.7 Stage 2 C-E loop I E2 I C2 V CC = I E2 R E2 + V EC2 +I C2 R C2 15 = 2.8(2) + V EC (2.7) solve for V EC2 V CE2 = 1.84V 45Nasim Zafar

Example 19.7 C-E loop neglect IB2 because it is IB2 << IC1 I E1 I C1 V CC = I C1 R C1 + V CE1 +I E1 R E1 15 = 1.3(5) + V CE1 +1.3(3) VCE1= 4.87V 46Nasim Zafar

Example 19.7 Stage 2 B-E loop I B2 I E2 V CC = I E2 R E2 + V EB +I B2 R BB2 + V BB2 15 = I E2 (2K) +.7 +I B2 (5K) (3) Use I B2  I E2 /  solve for I E2 IE2 = 2.8mA 47Nasim Zafar

Example stage amplifier, 1st stage has an npn transistor; 2nd stage has an pnp transistor. I C =  I B I C  I E V BE = 0.7 (npn) = -0.7 (pnp)  = 100 Find I C1, I C2, V CE1, V CE2 Use Thevenin circuits. 48Nasim Zafar

Example 19.7 R BB1 = R B1 ||R B2 = 33K V BB1 = V CC [R B2 /(R B1 +R B2 )] V BB1 = 15[50K/150K] = 5V Stage 1 B-E loop V BB1 = I B1 R BB1 + V BE +I E1 R E1 Use I B1  I E1 /  5 = I E1 33K / I E1 3K I E1 = 1.3mA I B1 I E1 49Nasim Zafar