Microelectronic Circuit Design McGraw-Hill Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.

Slides:



Advertisements
Similar presentations
Lecture Metal-Oxide-Semiconductor (MOS) Field-Effect Transistors (FET) MOSFET Introduction 1.
Advertisements

Goals Investigate circuits that bias transistors into different operating regions. Two Supplies Biasing Four Resistor Biasing Two Resistor Biasing Biasing.
Electronic Devices Eighth Edition Floyd Chapter 8.
Transistors (MOSFETs)
Topic 4 Field-Effect Transistors
Chapter 5 Bipolar Junction Transistors
Transistors These are three terminal devices, where the current or voltage at one terminal, the input terminal, controls the flow of current between the.
CURRENT MIRROR/SOURCE EMT451/4. DEFINITION Circuit that sources/sinks a constant current as biasing elements as load devices for amplifier stages.
S. RossEECS 40 Spring 2003 Lecture 20 Today we will Review NMOS and PMOS I-V characteristic Practice useful method for solving transistor circuits Build.
Week 9a OUTLINE MOSFET ID vs. VGS characteristic
Module 3: Part 1 The Field-Effect Transistor (FET)
© Electronics Recall Last Lecture The MOSFET has only one current, I D Operation of MOSFET – NMOS and PMOS – For NMOS, V GS > V TN V DS sat = V GS – V.
Microelectronics Circuit Analysis and Design Donald A. Neamen
Chapter Five The Field-Effect Transistor. Figure 6—2 A three-terminal nonlinear device that can be controlled by the voltage at the third terminal v.
ANALOGUE ELECTRONICS I
Metal-Oxide- Semiconductor (MOS) Field-Effect Transistors (MOSFETs)
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Transistors (MOSFETs)
The Ohmic Region The slope of the characteristic curve in the ohmic region is the dc drain-to- source conductance G DS of the JFET. Thus, the dc drain-to-source.
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.
Chapter 4 DC Biasing – Bipolar Junction Transistors (BJTs)
Semiconductor Devices III Physics 355. Transistors in CPUs Moore’s Law (1965): the number of components in an integrated circuit will double every year;
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 7 Junction Field-Effect Transistors. OBJECTIVES Describe and Analyze: JFET theory JFETS vs. Bipolars JFET Characteristics JFET Biasing JFET Circuits.
Chapter 4 Field-Effect Transistors
McGraw-Hill © 2008 The McGraw-Hill Companies Inc. All rights reserved. Electronics Principles & Applications Seventh Edition Chapter 7 More About Small-Signal.
Microelectronic Circuit Design McGraw-Hill Chapter 5 Bipolar Junction Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock Chap.
Chapter 11 Field effect Transistors: Operation, Circuit, Models, and Applications Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction.
ECE 340 ELECTRONICS I MOS APPLICATIONS AND BIASING.
JFET Biasing ENGI 242/ELEC 222. January 2004ENGI 242/ELEC 2222 JFET Fixed Bias R G is present to limit current in case V GG is connected with wrong polarity.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Chapter 4 Field-Effect Transistors
EE 334 Midterm Review. Diode: Why we need to understand diode? The base emitter junction of the BJT behaves as a forward bias diode in amplifying applications.
1 Fundamentals of Microelectronics  CH1 Why Microelectronics?  CH2 Basic Physics of Semiconductors  CH3 Diode Circuits  CH4 Physics of Bipolar Transistors.
Chapter 4 Field-Effect Transistors
Device Characterization ECE/ChE 4752: Microelectronics Processing Laboratory Gary S. May April 1, 2004.
Chapter 5 Bipolar Junction Transistors
Electronic Circuits Laboratory EE462G Lab #5 Biasing MOSFET devices.
Microelectronic Circuit Design McGraw-Hill Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.
Transistor Circuit DC Bias Part 1 ENGI 242. February 2003ENGI 2422 DC Biasing Circuits Fixed-Bias Circuit Emitter-Stabilized Bias Circuit Collector-Emitter.
Microelectronic Circuit Design, 3E McGraw-Hill Chapter 13 Small-Signal Modeling and Linear Amplification Microelectronic Circuit Design Richard C. Jaeger.
Microelectronic Circuit Design, 3E McGraw-Hill Chapter 14 Single-Transistors Amplifiers Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.
© 2000 Prentice Hall Inc. Figure 5.1 n-Channel enhancement MOSFET showing channel length L and channel width W.
Depletion-type MOSFET bias circuits are similar to JFETs. The only difference is that the depletion-Type MOSFETs can operate with positive values of V.
CHAP3: MOS Field-Effect Transistors (MOSFETs)
Microelectronic Circuit Design, 3E McGraw-Hill Chapter 13 Small-Signal Modeling and Linear Amplification Microelectronic Circuit Design Richard C. Jaeger.
Microelectronic Circuit Design, 3E McGraw-Hill Chapter 13 Small-Signal Modeling and Linear Amplification Microelectronic Circuit Design Richard C. Jaeger.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 7-1 Electronics Principles & Applications Eighth Edition Chapter 7 More About Small-Signal.
Chapter 15 Differential Amplifiers and Operational Amplifier Design
MOSFET DC circuit analysis Common-Source Circuit
JFET Biasing ELEC 121. January 2004ELEC 1212 JFET Fixed Bias R G is present to limit current in case V GG is connected with wrong polarity This would.
Chapter 15 Differential Amplifiers and Operational Amplifier Design
1 DMT 121 – ELECTRONIC DEVICES CHAPTER 5: FIELD-EFFECT TRANSISTOR (FET)
Electronics Principles & Applications Fifth Edition Chapter 7 More About Small-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
Recall Lecture 17 MOSFET DC Analysis 1.Using GS (SG) Loop to calculate V GS Remember that there is NO gate current! 2.Assume in saturation Calculate I.
SMALL SIGNAL FET (Field– Effect Transistors) AMPLIFIER 1.Introduction/Basic 2.FET Small-Signal Model 3.Fixed-Bias Configuration 4.Self-Bias Configuration.
5-1 McGraw-Hill Copyright © 2001 by the McGraw-Hill Companies, Inc. All rights reserved. Chapter Five The Field-Effect Transistor.
6/8/2016Faculty of Engineering Cairo University Chap Lecture 2 Single-Transistor Amplifiers Dr. Ahmed Nader Adapted from presentation by Richard.
BJT Bipolar Junction Transistors (BJT) Presented by D.Satishkumar Asst. Professor, Electrical & Electronics Engineering
ECE 333 Linear Electronics
ITM UNIVERSE,VADODARA ELECTRONIC DEVICES & CIRCUITS TOPIC NAME TRANSISTOR BIASING (DC ANALYSIS) PREPARED BY: NAME: Dilsha Dharmajan Electronics & communication.
MOSFET Basic FET Amplifiers The MOSFET Amplifier
Electronics Technology Fundamentals Chapter 21 Field-Effect Transistors and Circuits.
1 MOS Field-Effect Transistors (MOSFETs). Copyright  2004 by Oxford University Press, Inc. Microelectronic Circuits - Fifth Edition Sedra/Smith2 Figure.
CHAPTER 6 Field Effect Transistors (FETs)
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Microelectronic Circuit Design McGraw-Hill Chapter 3 Solid-State Diodes and Diode Circuits Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.
Microelectronic Circuit Design McGraw-Hill Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.
Chapter 3 Solid-State Diodes and Diode Circuits
Presentation transcript:

Microelectronic Circuit Design McGraw-Hill Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock

Microelectronic Circuit Design McGraw-Hill Bias Analysis Approach Assume an operation region (generally the saturation region) Use circuit analysis to find V GS Use V GS to calculate I D, and I D to find V DS Check validity of operation region assumptions Change assumptions and analyze again if required. NOTE :An enhancement-mode device with V DS = V GS is always in saturation

Microelectronic Circuit Design McGraw-Hill Four-Resistor and Two-Resistor Biasing Provide excellent bias for transistors in discrete circuits. Stabilize bias point with respect to device parameter and temperature variations using negative feedback. Use single voltage source to supply both gate-bias voltage and drain current. Generally used to bias transistors in saturation region. Two-resistor biasing uses lesser components that four- resistor biasing and also isolates drain and gate terminals

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 1 (Constant Gate-Source Voltage Biasing) Problem: Find Q-pt (I D, V DS, V GS ) Approach: Assume operation region, find Q-point, check to see if result is consistent with operation region Assumption: Transistor is saturated, I G =I B =0 Analysis: Simplify circuit with Thevenin transformation to find V EQ and R EQ for gate-bias voltage. Find V GS and then use this to find I D. With I D, we can then calculate V DS.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 1 (Constant Gate-Source Voltage Biasing)(contd.) Since I G =0, Check:V DS >V GS -V TN. Hence saturation region assumption is correct. Q-pt: (50.0  A, 5.00 V) with V GS = 3.00 V Discussion: The Q-point of this circuit is quite sensitive to changes in transistor characteristics, so it is not widely used.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 2 (Load Line Analysis) Problem: Find Q-pt (I D, V DS, V GS ) Approach: Find an equation for the load line. Use this to find Q-pt at intersection of load line with device characteristic. Assumption: Transistor is saturated, I G =I B =0 Analysis: For circuit values above, load line becomes Use this to find two points on the load line.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 2 (Load Line Analysis)(contd.) Check: The load line approach agrees with previous calculation. Q-pt: (50.0  A, 5.00 V) with V GS = 3.00 V Discussion: Q-pt is clearly in the saturation region. Graphical load line is good visual aid to see device operating VDS=10V Plotting on device characteristic yields Q-pt at intersection with V GS = 3V device curve.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 3 (Constant Gate-Source Voltage Biasing with Channel-Length Modulation) Problem: Find Q-pt (I D, V DS, V GS ) of previous example, given =0.02 V -1. Approach: Assume operation region, find Q-point, check to see if result is consistent with operation region Assumption: Transistor is saturated, I G =I B =0 Analysis: Simplify circuit with Thevenin transformation to find V EQ and R EQ for gate-bias voltage. Find V GS and then use this to find I D. With I D, we can then calculate V DS.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 3 (Constant Gate-Source Voltage Biasing with Channel-Length Modulation) Check:V DS >V GS -V TN. Hence saturation region assumption is correct. Q-pt: (54.5  A, 4.55 V) with V GS = 3.00 V Discussion: The bias levels have changed by about 10%. Typically, component values will vary more than this, so there is little value in including effects in most circuits.

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 4 (Four-Resistor Biasing) Problem: Find Q-pt (I D, V DS ) Approach: Assume operation region, find Q-point, check to see if result is consistent with operation region Assumption: Transistor is saturated, I G =I B =0 Analysis: First, simplify circuit, split V DD into two equal-valued sources and apply Thevenin transformation to find V EQ and R EQ for gate-bias voltage

Microelectronic Circuit Design McGraw-Hill Bias Analysis: Example 4 (Four-Resistor Biasing) Since I G =0, Since V GS <V TN for V GS = V and MOSFET will be cut-off, and I D = 34.4  A Also, V DS >V GS -V TN. Hence saturation region assumption is correct. Q-pt: (34.4  A, 6.08 V) with V GS = 2.66 V