DC and AC Load Line DC biasing circuits DC and AC equivalent circuit

Slides:



Advertisements
Similar presentations
Lecture 07 DC and AC Load Line
Advertisements

Class-A and Class-B Amplifiers
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)
POWER AMPLIFIER (Additional Lecture Notes)
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 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Chapter 5 Transistor Bias Circuits
Chapter 4 DC Biasing–BJTs. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices and.
1 2. Design of BJT amplifiers 2.1 Types of BJT amplifiersTypes of BJT amplifiers 2.2 BJT amplifier biasing designBJT amplifier biasing design 2.3 BJT Optimum.
Prepared by: Garima Devpriya ( ) Jamila Kharodawala ( ) Megha Sharma ( ) ELECTRONICS DEVICES AND CIRCUITS G.H.Patel.
Chapter 4 DC Biasing–BJTs. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices and.
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 13 Small-Signal Modeling and Linear Amplification
Chapter 4 DC Biasing–BJTs
LECTURE 1: BASIC BJT AMPLIFIER -AC ANALYSIS-
Recall Lecture 10 Introduction to BJT 3 modes of operation
Recall Last Lecture Biasing of BJT Applications of BJT
Recall Last Lecture Biasing of BJT Three types of biasing
Gandhinagar Institute of Technology
Recall Last Lecture Biasing of BJT Three types of biasing
Amplifier: An amplifier is an electronic device that increases voltage, current or power of a signal. According to the class of operation, the amplifiers.
Bipolar Junction Transistor Circuit Analysis
Lecture 07 DC and AC Load Line
EKT104 ANALOG ELECTRONIC CIRCUITS [LITAR ELEKTRONIK ANALOG] BASIC BJT AMPLIFIER (PART I) DR NIK ADILAH HANIN BINTI ZAHRI
Recall Last Lecture Biasing of BJT Three types of biasing
TRANSISTOR BIASING & STABILIZATION.
Lecture 10 Bipolar Junction Transistor (BJT)
Transistor Bias Circuits
(15A04301) ELECTRONIC DEVICES AND CIRCUITS
Prepared By: Branch: Electronics and Communication. Semester: 3
EELE 2321 – Electronics Spring, 2013 Bipolar Junction Transistor (BJT) Structure Eng. Wazen M. Shbair.
Transistor Biasing The basic function of transistor is amplification. The process of raising the strength of weak signal without any change in its general.
BRANCH:- IC SEM :- 3 1.
Chapter 4(c) DC Biasing – Bipolar Junction Transistors (BJTs)
Amplifier Group Members: Shrivastav Mehul S. Katara Sandeep.
SMALL SIGNAL ANALYSIS OF CB AMPLIFIER
SMALL SIGNAL ANALYSIS OF CE AMPLIFIER
Principles & Applications Small-Signal Amplifiers
Recall Lecture 13 Biasing of BJT Voltage Divider Biasing Circuit.
Small-Signal Modeling and Linear Amplification
GUIDED BY: Prof. Nipa Modi
ac Load Line Analysis Maximum Symmetrical Swing
The Currents of a BJT The collector current. The base Current.
Chapter 1 – Revision Part 2
Lecture 07 Bipolar Junction Transistors (2)
POWER AMPLIFIERS.
Chapter 5 Transistor Bias Circuits
Govt. Polytechnic, Dhangar
Recall Last Lecture Voltage Transfer Characteristic
Recall Lecture 11 DC Analysis and Load Line
Recall Last Lecture Voltage Transfer Characteristic
Lecture’s content Objectives BJT – Small Signal Amplifier
Bipolar Junction Transistor
Recall Lecture 10 Introduction to BJT 3 modes of operation
Chapter 5 Transistor Bias Circuits
Lecture VI Power Amplifiers Class A & Class AB
Recall Last Lecture Voltage Transfer Characteristic
Bipolar Junction Transistor Circuit Analysis
TRANSISTOR AMPLIFIER CONFIGURATION -BJT Common-Emitter Amplifier-
Lecture’s content Objectives BJT – Small Signal Amplifier
Chapter 3 – Transistor Amplifiers – Part 1
ChapTer FoUr DC BIASING - BIPOLAR JUNCTION TRANSISTORS (BJTs)
ChapTer FoUr DC BIASING - BIPOLAR JUNCTION TRANSISTORS (BJTs)
TRANSISTOR BIASING & STABILIZATION
Electronic PRINCIPLES
DC Biasing Circuits.
Recall Lecture 11 DC Analysis and Load Line
Presentation transcript:

DC and AC Load Line DC biasing circuits DC and AC equivalent circuit Q-point (Static operation point) DC and AC load line Saturation Cutoff Condition Compliance Ref:080314HKN EE3110 DC and AC Load Line 1

Book Reference Electronic Devices and Circuit Theory by Robert Boylestad & Louis Nashelsky ( Prentice Hall ) Electronic Devices by Thomas L. Floyd ( Prentice Hall ) Ref:080314HKN EE3110 DC and AC Load Line 2

DC Biasing Circuits The ac operation of an amplifier depends on the initial dc values of IB, IC, and VCE. By varying IB around an initial dc value, IC and VCE are made to vary around their initial dc values. DC biasing is a static operation since it deals with setting a fixed (steady) level of current (through the device) with a desired fixed voltage drop across the device. Ref:080314HKN EE3110 DC and AC Load Line 3

Purpose of the DC biasing circuit To turn the device “ON” To place it in operation in the region of its characteristic where the device operates most linearly, i.e. to set up the initial dc values of IB, IC, and VCE Ref:080314HKN EE3110 DC and AC Load Line 4

Voltage-Divider Bias The voltage – divider (or potentiometer) bias circuit is by far the most commonly used. RB1, RB2  voltage-divider to set the value of VB , IB C3  to short circuit ac signals to ground, while not effect the DC operating (or biasing) of a circuit (RE  stabilizes the ac signals)  Bypass Capacitor Ref:080314HKN EE3110 DC and AC Load Line 5

Graphical DC Bias Analysis Ref:080314HKN EE3110 DC and AC Load Line 6

DC Load Line The straight line is know as the DC load line Its significance is that regardless of the behavior of the transistor, the collector current IC and the collector-emitter voltage VCE must always lie on the load line, depends ONLY on the VCC, RC and RE (i.e. The dc load line is a graph that represents all the possible combinations of IC and VCE for a given amplifier. For every possible value of IC, and amplifier will have a corresponding value of VCE.) It must be true at the same time as the transistor characteristic. Solve two condition using simultaneous equation  graphically  Q-point !! What is IC(sat) and VCE(off) ? Ref:080314HKN EE3110 DC and AC Load Line 7

Q-Point (Static Operation Point) When a transistor does not have an ac input, it will have specific dc values of IC and VCE. These values correspond to a specific point on the dc load line. This point is called the Q-point. The letter Q corresponds to the word (Latent) quiescent, meaning at rest. A quiescent amplifier is one that has no ac signal applied and therefore has constant dc values of IC and VCE. Ref:080314HKN EE3110 DC and AC Load Line 8

Q-Point (Static Operation Point) The intersection of the dc bias value of IB with the dc load line determines the Q-point. It is desirable to have the Q- point centered on the load line. Why? When a circuit is designed to have a centered Q-point, the amplifier is said to be midpoint biased. Midpoint biasing allows optimum ac operation of the amplifier. Ref:080314HKN EE3110 DC and AC Load Line 9

DC Biasing + AC signal When an ac signal is applied to the base of the transistor, IC and VCE will both vary around their Q-point values. When the Q-point is centered, IC and VCE can both make the maximum possible transitions above and below their initial dc values. When the Q-point is above the center on the load line, the input signal may cause the transistor to saturate. When this happens, a part of the output signal will be clipped off. When the Q-point is below midpoint on the load line, the input signal may cause the transistor to cutoff. This can also cause a portion of the output signal to be clipped. Ref:080314HKN EE3110 DC and AC Load Line 10

DC Biasing + AC signal Ref:080314HKN EE3110 DC and AC Load Line 11

DC and AC Equivalent Circuits Bias Circuit DC equivalent circuit AC equivalent circuit Ref:080314HKN EE3110 DC and AC Load Line 12

AC Load Line The ac load line of a given amplifier will not follow the plot of the dc load line. This is due to the dc load of an amplifier is different from the ac load. Ref:080314HKN EE3110 DC and AC Load Line 13

AC Load Line What does the ac load line tell you? The ac load line is used to tell you the maximum possible output voltage swing for a given common-emitter amplifier. In other words, the ac load line will tell you the maximum possible peak-to-peak output voltage (Vpp ) from a given amplifier. This maximum Vpp is referred to as the compliance of the amplifier. (AC Saturation Current Ic(sat) , AC Cutoff Voltage VCE(off) ) Ref:080314HKN EE3110 DC and AC Load Line 14

AC Saturation Current and AC Cutoff Voltage Ref:080314HKN EE3110 DC and AC Load Line 15

Amplifier Compliance The ac load line is used to tell the maximum possible output voltage swing for a given common-emitter amplifier. In another words, the ac load line will tell the maximum possible peak- to-peak output voltage (VPP) from a given amplifier. This maximum VPP is referred to as the compliance of the amplifier. The compliance of an amplifier is found by determine the maximum possible of IC and VCE from their respective values of ICQ and VCEQ. Ref:080314HKN EE3110 DC and AC Load Line 16

Maximum Possible Compliance Ref:080314HKN EE3110 DC and AC Load Line 17

Compliance The maximum possible transition for VCE is equal to the difference between VCE(off) and VCEQ. Since this transition is equal to ICQrC, the maximum peak output voltage from the amplifier is equal to ICQrC. Two times this value will give the maximum peak-to-peak transition of the output voltage: VPP = the output compliance, in peak-to-peak voltage ICQ = the quiescent value of IC rC = the ac load resistance in the circuit VPP = 2ICQrC (A) Ref:080314HKN EE3110 DC and AC Load Line 18

Compliance When IC = IC(sat)­, VCE is ideally equal to 0V. When I­C = ICQ, VCE is at VCEQ. Note that when IC makes its maximum possible transition (from ICQ to IC(sat)), the output voltage changes by an amount equal to VCEQ. Thus the maximum peak-to-peak transition would be equal to twice this value: Equation (A) sets the limit in terms of VCE(off). If the value obtained by this equation is exceed, the output voltage will try to exceed VCE(off), which is not possible. This is called cutoff clipping, because the output voltage is clipped off at the value of VCE(off). Equation (B) sets of the limit in terms of IC(sat). If the value obtained by this equation is exceed, the output will experience saturation clipping. (B) VPP = 2VCEQ Ref:080314HKN EE3110 DC and AC Load Line 19

Cutoff and Saturation Clipping When determining the output compliance for a given amplifier, solve both equation (A) and (B). The lower of the two results is the compliance of the amplifier. Ref:080314HKN EE3110 DC and AC Load Line 20

Example For the voltage-divider bias amplifier shown in the figure, what is the ac and dc load line. Determine the maximum output compliance. Ref:080314HKN EE3110 DC and AC Load Line 21