Voltage AmpliÞer Frequency Response
|
|
- Gavin Gregory
- 5 years ago
- Views:
Transcription
1 Voltage AmpliÞer Frequency Response Chapter 9 multistage voltage ampliþer 5 V M 7B M 7 M 5 R 35 kω M 6B M 6 Q µa X M 3 Q B Q v OUT V s M 1 M 8 M9 V BIAS M 10 Approaches: 1. brute force OCTC -- do for all capacitances in the circuit. identify the largest contributor(s) and calculate the ThŽvenin resistance associated with them Try second approach: identify four nodes in signal path Lecture 3
2 Qualitative Evaluation of Time Constants Input node: no contribution since R S = 0 Drain of M 1 : Òlow impedance nodeó since R in(cb) = 1/ g m Node X: extremely high resistance... could be a big time constant Source of M 3 : Òlow impedance nodeó since R out(cd) = 1/ g m3 Output node: Òlow impedance nodeó since R o(cc) = 1/ g m4 Note: we are not considering capacitances between nodes here... since we are doing an approximate analysis, we will use MillerÕs theorem to Þnd their effective capacitance to ground Lecture 3
3 Small-Signal Model of Node X Account for all of the capacitances from node X to small-signal ground: 1. Base-collector capacitance C µ of Q (since it is connected to diodeconnected transistors M 6B and M 7B that are in turn connected to V DD ). Gate-drain capacitance C gd6 of M 6 (since it is connected to the same node as C µ ) 3. Gate-drain capacitance C gd3 of M 3 (since it is connected directly to ground) Omitted from Section 10.7Õs analysis: parasitic capacitances to substrate -- C cs and C db6 are both present between node X and ground 4. Effective capacitance due to C gs3 connected between the input and the output of the common-drain stage: C eff = C gs3 ( 1 Ð A vcgs3 ) The gain across C gs3 is about 1, but an accurate calculation would include any backgate effect on M 3 if present. Small-signal model with all (non-parasitic) capacitances X β o r o r oc C µ C gd6 C gd3 (1 A v3 )C gs3 Lecture 3
4 Gain-Bandwidth Product Considering only the time constant from node X 1 ω 3dB [( β o r o g m6 r o6 r o7 )]( C µ C gd6 C gd3 ( 1 Ð A vcgs3 )C gs3 ) Approximate low-frequency gain -- from Chapter 9 A vo Ðg m1 ( β o r o g m6 r o6 r o7 ) Gain-bandwidth product A vo ω g m1 3dB C µ C gd6 C gd3 ( 1 Ð A vcgs3 )C gs3 Lecture 3
5 Magnitude Bode Plot Assuming that the second pole is greater than the unity gain frequency, the Bode plot is V out V s g m1 β o r o 1 1 (r oc β o r o ) {C µ C gd6 C gd3 (1A v3 ) C gs3 } ω g log scale m1 {C µ C gd6 C gd3 (1A v3 ) C gs3 } Lecture 3
6 Differential AmpliÞers General structure: two inputs, two outputs V 1 I 1 I V O1 V O V I1 v i1 = 0 V 1 V IN1 V IN V I v i = 0 V V Consider balanced situation: V I1 = V I and 1 = and devices 1 and are in their constant-current modes. = I 1 I = (V / ) Adjust so V O1 = V O are about 0 V (note the dual supplies) Lecture 3
7 Decomposition of Small-Signal Input Voltages Inputs v i1 and v i are not the Ònatural inputsó to understand how the differential ampliþer works... DeÞne two new voltages differential-mode input voltage = v id = v i1 - v i common-mode input voltage = v ic = (1/)(v i1 v i ) Expressing the inputs v i1 and v i in terms of v id and v ic v id v i1 = v ic v id v i = v ic Ð V V v o1 v o v o1 v o 1 1 v i1 v i v id v id v ic V (a) V (b) Lecture 3
8 Example of Signal Decomposition v i1 = v in and v i = 0 V results in both a differential-modeand a common-mode input to the ampliþer V V v o1 v o v o1 v o 1 1 v in v in v in v in V (a) V (b) Goal: determine the response of the differential ampliþer to v id and v ic separately and then reconstruct the response Lecture 3
9 Small-Signal Model of Bipolar Diff. AmpliÞer DeÞne r ob as the internal (source) resistance of the bias current source V v o1 v o Q 1 Q v i1 v i r ob V Small-signal model with purely differential inputs v o1 v o v id r π g m v π1 R C g m v v π rπ π1 v π v id i 1 i v x r ob Lecture 3
10 Small-Signal Model with Purely Differential Inputs The voltage at v x must be zero for purely differential inputs --> it can be considered a small-signal or incremental ground reference Only need to solve half of the circuit, whose outputs are or - v od / v v od od v id r π g m v π1 R v C g m v π rπ π1 v π v id i 1 i v x Solve left half to Þnd v od v id = Ðg m deþne differential-mode gain a dm by a dm v od = = Ðg v m id Lecture 3
The Miller Approximation
The Miller Approximation The exact analysis is not particularly helpful for gaining insight into the frequency response... consider the effect of C µ on the input only I t C µ V t g m V t R'out = r o r
More informationAssignment 3 ELEC 312/Winter 12 R.Raut, Ph.D.
Page 1 of 3 ELEC 312: ELECTRONICS II : ASSIGNMENT-3 Department of Electrical and Computer Engineering Winter 2012 1. A common-emitter amplifier that can be represented by the following equivalent circuit,
More informationECE-343 Test 1: Feb 10, :00-8:00pm, Closed Book. Name : SOLUTION
ECE-343 Test : Feb 0, 00 6:00-8:00pm, Closed Book Name : SOLUTION C Depl = C J0 + V R /V o ) m C Diff = τ F g m ω T = g m C µ + C π ω T = g m I / D C GD + C or V OV GS b = τ i τ i = R i C i ω H b Z = Z
More informationMultistage Amplifier Frequency Response
Multistage Amplifier Frequency Response * Summary of frequency response of single-stages: CE/CS: suffers from Miller effect CC/CD: wideband -- see Section 0.5 CB/CG: wideband -- see Section 0.6 (wideband
More information6.012 Electronic Devices and Circuits Spring 2005
6.012 Electronic Devices and Circuits Spring 2005 May 16, 2005 Final Exam (200 points) -OPEN BOOK- Problem NAME RECITATION TIME 1 2 3 4 5 Total General guidelines (please read carefully before starting):
More informationBiasing the CE Amplifier
Biasing the CE Amplifier Graphical approach: plot I C as a function of the DC base-emitter voltage (note: normally plot vs. base current, so we must return to Ebers-Moll): I C I S e V BE V th I S e V th
More informationEE105 Fall 2015 Microelectronic Devices and Circuits Frequency Response. Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH)
EE05 Fall 205 Microelectronic Devices and Circuits Frequency Response Prof. Ming C. Wu wu@eecs.berkeley.edu 5 Sutardja Dai Hall (SDH) Amplifier Frequency Response: Lower and Upper Cutoff Frequency Midband
More informationFrequency Response Prof. Ali M. Niknejad Prof. Rikky Muller
EECS 105 Spring 2017, Module 4 Frequency Response Prof. Ali M. Niknejad Department of EECS Announcements l HW9 due on Friday 2 Review: CD with Current Mirror 3 Review: CD with Current Mirror 4 Review:
More informationLecture 37: Frequency response. Context
EECS 05 Spring 004, Lecture 37 Lecture 37: Frequency response Prof J. S. Smith EECS 05 Spring 004, Lecture 37 Context We will figure out more of the design parameters for the amplifier we looked at in
More informationI. Frequency Response of Voltage Amplifiers
I. Frequency Response of Voltage Amplifiers A. Common-Emitter Amplifier: V i SUP i OUT R S V BIAS R L v OUT V Operating Point analysis: 0, R s 0, r o --->, r oc --->, R L ---> Find V BIAS such that I C
More informationECE-343 Test 2: Mar 21, :00-8:00, Closed Book. Name : SOLUTION
ECE-343 Test 2: Mar 21, 2012 6:00-8:00, Closed Book Name : SOLUTION 1. (25 pts) (a) Draw a circuit diagram for a differential amplifier designed under the following constraints: Use only BJTs. (You may
More informationSOME USEFUL NETWORK THEOREMS
APPENDIX D SOME USEFUL NETWORK THEOREMS Introduction In this appendix we review three network theorems that are useful in simplifying the analysis of electronic circuits: Thévenin s theorem Norton s theorem
More informationLecture 24 Multistage Amplifiers (I) MULTISTAGE AMPLIFIER
Lecture 24 Multistage Amplifiers (I) MULTISTAGE AMPLIFIER Outline. Introduction 2. CMOS multi-stage voltage amplifier 3. BiCMOS multistage voltage amplifier 4. BiCMOS current buffer 5. Coupling amplifier
More informationECE-342 Test 3: Nov 30, :00-8:00, Closed Book. Name : Solution
ECE-342 Test 3: Nov 30, 2010 6:00-8:00, Closed Book Name : Solution All solutions must provide units as appropriate. Unless otherwise stated, assume T = 300 K. 1. (25 pts) Consider the amplifier shown
More informationChapter 9 Frequency Response. PART C: High Frequency Response
Chapter 9 Frequency Response PART C: High Frequency Response Discrete Common Source (CS) Amplifier Goal: find high cut-off frequency, f H 2 f H is dependent on internal capacitances V o Load Resistance
More informationECE 546 Lecture 11 MOS Amplifiers
ECE 546 Lecture MOS Amplifiers Spring 208 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine Amplifiers Definitions Used to increase
More informationHomework Assignment 08
Homework Assignment 08 Question 1 (Short Takes) Two points each unless otherwise indicated. 1. Give one phrase/sentence that describes the primary advantage of an active load. Answer: Large effective resistance
More informationECEN 326 Electronic Circuits
ECEN 326 Electronic Circuits Frequency Response Dr. Aydın İlker Karşılayan Texas A&M University Department of Electrical and Computer Engineering High-Frequency Model BJT & MOS B or G r x C f C or D r
More informationECE 255, Frequency Response
ECE 255, Frequency Response 19 April 2018 1 Introduction In this lecture, we address the frequency response of amplifiers. This was touched upon briefly in our previous lecture in Section 7.5 of the textbook.
More informationCE/CS Amplifier Response at High Frequencies
.. CE/CS Amplifier Response at High Frequencies INEL 4202 - Manuel Toledo August 20, 2012 INEL 4202 - Manuel Toledo CE/CS High Frequency Analysis 1/ 24 Outline.1 High Frequency Models.2 Simplified Method.3
More informationElectronics II. Midterm II
The University of Toledo f4ms_elct7.fm - Section Electronics II Midterm II Problems Points. 7. 7 3. 6 Total 0 Was the exam fair? yes no The University of Toledo f4ms_elct7.fm - Problem 7 points Given in
More informationLecture 23 Frequency Response of Amplifiers (I) Common Source Amplifier. December 1, 2005
6.02 Microelectronic Devices and Circuits Fall 2005 Lecture 23 Lecture 23 Frequency Response of Amplifiers (I) Common Source Amplifier December, 2005 Contents:. Introduction 2. Intrinsic frequency response
More information3. Basic building blocks. Analog Design for CMOS VLSI Systems Franco Maloberti
Inverter with active load It is the simplest gain stage. The dc gain is given by the slope of the transfer characteristics. Small signal analysis C = C gs + C gs,ov C 2 = C gd + C gd,ov + C 3 = C db +
More informationAdvanced Current Mirrors and Opamps
Advanced Current Mirrors and Opamps David Johns and Ken Martin (johns@eecg.toronto.edu) (martin@eecg.toronto.edu) slide 1 of 26 Wide-Swing Current Mirrors I bias I V I in out out = I in V W L bias ------------
More informationLecture 5 Review Current Source Active Load Modified Large / Small Signal Models Channel Length Modulation
Lecture 5 Review Current Source Active Load Modified Large / Small Signal Models Channel Length Modulation Text sec 1.2 pp. 28-32; sec 3.2 pp. 128-129 Current source Ideal goal Small signal model: Open
More informationElectronic Circuits Summary
Electronic Circuits Summary Andreas Biri, D-ITET 6.06.4 Constants (@300K) ε 0 = 8.854 0 F m m 0 = 9. 0 3 kg k =.38 0 3 J K = 8.67 0 5 ev/k kt q = 0.059 V, q kt = 38.6, kt = 5.9 mev V Small Signal Equivalent
More informationEE C245 ME C218 Introduction to MEMS Design Fall 2011
EE C245 ME C218 Introduction to MEMS Design Fall 2011 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture EE C245:
More informationThe Devices. Jan M. Rabaey
The Devices Jan M. Rabaey Goal of this chapter Present intuitive understanding of device operation Introduction of basic device equations Introduction of models for manual analysis Introduction of models
More informationHomework Assignment 09
Homework Assignment 09 Question 1 (Short Takes) Two points each unless otherwise indicated. 1. What is the 3-dB bandwidth of the amplifier shown below if r π = 2.5K, r o = 100K, g m = 40 ms, and C L =
More informationElectronic Devices and Circuits Lecture 18 - Single Transistor Amplifier Stages - Outline Announcements. Notes on Single Transistor Amplifiers
6.012 Electronic Devices and Circuits Lecture 18 Single Transistor Amplifier Stages Outline Announcements Handouts Lecture Outline and Summary Notes on Single Transistor Amplifiers Exam 2 Wednesday night,
More informationCommon Drain Stage (Source Follower) Claudio Talarico, Gonzaga University
Common Drain Stage (Source Follower) Claudio Talarico, Gonzaga University Common Drain Stage v gs v i - v o V DD v bs - v o R S Vv IN i v i G C gd C+C gd gb B&D v s vv OUT o + V S I B R L C L v gs - C
More information6.301 Solid State Circuits Recitation 7: Emitter Degeneration, and More on Multistage Amps Prof. Joel L. Dawson
We re going to look at emitter degeneration in detail today. The purpose is in part to review, and in part to help pull together a few of the concepts that we ve dealt with in the class up to this point.
More informationEECS 105: FALL 06 FINAL
University of California College of Engineering Department of Electrical Engineering and Computer Sciences Jan M. Rabaey TuTh 2-3:30 Wednesday December 13, 12:30-3:30pm EECS 105: FALL 06 FINAL NAME Last
More informationEE105 Fall 2014 Microelectronic Devices and Circuits
EE05 Fall 204 Microelectronic Devices and Circuits Prof. Ming C. Wu wu@eecs.berkeley.edu 5 Sutardja Dai Hall (SDH) Terminal Gain and I/O Resistances of BJT Amplifiers Emitter (CE) Collector (CC) Base (CB)
More informationLecture 04: Single Transistor Ampliers
Lecture 04: Single Transistor Ampliers Analog IC Design Dr. Ryan Robucci Department of Computer Science and Electrical Engineering, UMBC Spring 2015 Dr. Ryan Robucci Lecture IV 1 / 37 Single-Transistor
More informationCapacitors Diodes Transistors. PC200 Lectures. Terry Sturtevant. Wilfrid Laurier University. June 4, 2009
Wilfrid Laurier University June 4, 2009 Capacitor an electronic device which consists of two conductive plates separated by an insulator Capacitor an electronic device which consists of two conductive
More informationStep 1. Finding V M. Goal: Þnd V M = input voltage for the output = V M both transistors are saturated at V IN = V M since
Step 1. Finding V M Goal: Þnd V M = input voltage for the output = V M both transistors are saturated at V IN = V M since V DSn = V M - 0 > V M - V Tn V SDp = V DD - V M = (V DD - V M ) V Tp Equate drain
More informationECE 342 Electronic Circuits. Lecture 25 Frequency Response of CG, CB,SF and EF
ECE 342 Electronic Circuits ecture 25 Frequency esponse of CG, CB,SF and EF Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 342 Jose Schutt Aine 1 Common
More informationAt point G V = = = = = = RB B B. IN RB f
Common Emitter At point G CE RC 0. 4 12 0. 4 116. I C RC 116. R 1k C 116. ma I IC 116. ma β 100 F 116µ A I R ( 116µ A)( 20kΩ) 2. 3 R + 2. 3 + 0. 7 30. IN R f Gain in Constant Current Region I I I C F
More informationChapter 13 Small-Signal Modeling and Linear Amplification
Chapter 13 Small-Signal Modeling and Linear Amplification Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock 1/4/12 Chap 13-1 Chapter Goals Understanding of concepts related to: Transistors
More information6.301 Solid State Circuits Recitation 7: Emitter Degeneration, and More on Multistage Amps Prof. Joel L. Dawson
We re going to look at emitter degeneration in detail today. The purpose is in part to review, and in part to help pull together a few of the concepts that we ve dealt with in the class up to this point.
More informationElectronics II. Final Examination
f3fs_elct7.fm - The University of Toledo EECS:3400 Electronics I Section Student Name Electronics II Final Examination Problems Points.. 3 3. 5 Total 40 Was the exam fair? yes no Analog Electronics f3fs_elct7.fm
More informationSwitching circuits: basics and switching speed
ECE137B notes; copyright 2018 Switching circuits: basics and switching speed Mark Rodwell, University of California, Santa Barbara Amplifiers vs. switching circuits Some transistor circuit might have V
More informationEE 330. Lecture 35. Parasitic Capacitances in MOS Devices
EE 330 Lecture 35 Parasitic Capacitances in MOS Devices Exam 2 Wed Oct 24 Exam 3 Friday Nov 16 Review from Last Lecture Cascode Configuration Discuss V CC gm1 gm1 I B VCC V OUT g02 g01 A - β β VXX Q 2
More informationEE115C Winter 2017 Digital Electronic Circuits. Lecture 3: MOS RC Model, CMOS Manufacturing
EE115C Winter 2017 Digital Electronic Circuits Lecture 3: MOS RC Model, CMOS Manufacturing Agenda MOS Transistor: RC Model (pp. 104-113) S R on D CMOS Manufacturing Process (pp. 36-46) S S C GS G G C GD
More informationLecture 10 MOSFET (III) MOSFET Equivalent Circuit Models
Lecture 10 MOSFET (III) MOSFET Equivalent Circuit Models Outline Lowfrequency smallsignal equivalent circuit model Highfrequency smallsignal equivalent circuit model Reading Assignment: Howe and Sodini;
More informationLecture 210 Physical Aspects of ICs (12/15/01) Page 210-1
Lecture 210 Physical Aspects of ICs (12/15/01) Page 210-1 LECTURE 210 PHYSICAL ASPECTS OF ICs (READING: Text-Sec. 2.5, 2.6, 2.8) INTRODUCTION Objective Illustrate the physical aspects of integrated circuits
More informationChapter 10 Feedback. PART C: Stability and Compensation
1 Chapter 10 Feedback PART C: Stability and Compensation Example: Non-inverting Amplifier We are analyzing the two circuits (nmos diff pair or pmos diff pair) to realize this symbol: either of the circuits
More informationLecture 10 MOSFET (III) MOSFET Equivalent Circuit Models
Lecture 1 MOSFET (III) MOSFET Equivalent Circuit Models Outline Lowfrequency smallsignal equivalent circuit model Highfrequency smallsignal equivalent circuit model Reading Assignment: Howe and Sodini;
More informationBipolar junction transistors
Bipolar junction transistors Find parameters of te BJT in CE configuration at BQ 40 µa and CBQ V. nput caracteristic B / µa 40 0 00 80 60 40 0 0 0, 0,5 0,3 0,35 0,4 BE / V Output caracteristics C / ma
More informationMOS Transistor Theory
MOS Transistor Theory So far, we have viewed a MOS transistor as an ideal switch (digital operation) Reality: less than ideal EE 261 Krish Chakrabarty 1 Introduction So far, we have treated transistors
More informationECE 497 JS Lecture - 12 Device Technologies
ECE 497 JS Lecture - 12 Device Technologies Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 NMOS Transistor 2 ρ Source channel charge density
More informationMOS Transistor I-V Characteristics and Parasitics
ECEN454 Digital Integrated Circuit Design MOS Transistor I-V Characteristics and Parasitics ECEN 454 Facts about Transistors So far, we have treated transistors as ideal switches An ON transistor passes
More informationUniversity of Toronto. Final Exam
University of Toronto Final Exam Date - Dec 16, 013 Duration:.5 hrs ECE331 Electronic Circuits Lecturer - D. Johns ANSWER QUESTIONS ON THESE SHEETS USING BACKS IF NECESSARY 1. Equation sheet is on last
More informationECE 438: Digital Integrated Circuits Assignment #4 Solution The Inverter
ECE 438: Digital Integrated Circuits Assignment #4 The Inverter Text: Chapter 5, Digital Integrated Circuits 2 nd Ed, Rabaey 1) Consider the CMOS inverter circuit in Figure P1 with the following parameters.
More informationElectronics II. Final Examination
The University of Toledo f17fs_elct27.fm 1 Electronics II Final Examination Problems Points 1. 11 2. 14 3. 15 Total 40 Was the exam fair? yes no The University of Toledo f17fs_elct27.fm 2 Problem 1 11
More informationFigure 1: MOSFET symbols.
c Copyright 2008. W. Marshall Leach, Jr., Professor, Georgia Institute of Technology, School of Electrical and Computer Engineering. The MOSFET Device Symbols Whereas the JFET has a diode junction between
More informationCircle the one best answer for each question. Five points per question.
ID # NAME EE-255 EXAM 3 November 8, 2001 Instructor (circle one) Talavage Gray This exam consists of 16 multiple choice questions and one workout problem. Record all answers to the multiple choice questions
More informationCharge Storage in the MOS Structure. The Inverted MOS Capacitor (V GB > V Tn )
The Inverted MO Capacitor (V > V Tn ) We consider the surface potential as Þxed (ÒpinnedÓ) at φ s,max = - φ p φ(x).5 V. V V ox Charge torage in the MO tructure Three regions of operation: Accumulation:
More informationLecture 15: MOS Transistor models: Body effects, SPICE models. Context. In the last lecture, we discussed the modes of operation of a MOS FET:
Lecture 15: MOS Transistor models: Body effects, SPICE models Context In the last lecture, we discussed the modes of operation of a MOS FET: oltage controlled resistor model I- curve (Square-Law Model)
More informationEE 466/586 VLSI Design. Partha Pande School of EECS Washington State University
EE 466/586 VLSI Design Partha Pande School of EECS Washington State University pande@eecs.wsu.edu Lecture 8 Power Dissipation in CMOS Gates Power in CMOS gates Dynamic Power Capacitance switching Crowbar
More informationThe BJT Differential Amplifier. Basic Circuit. DC Solution
c Copyright 010. W. Marshall Leach, Jr., Professor, Georgia Institute of Technology, School of Electrical and Computer Engineering. The BJT Differential Amplifier Basic Circuit Figure 1 shows the circuit
More informationLecture Stage Frequency Response - I (1/10/02) Page ECE Analog Integrated Circuits and Systems II P.E.
Lecture 070 Stage Frequency esponse I (/0/0) Page 070 LECTUE 070 SINGLESTAGE FEQUENCY ESPONSE I (EADING: GHLM 488504) Objective The objective of this presentation is:.) Illustrate the frequency analysis
More informationRefinements to Incremental Transistor Model
Refinements to Incremental Transistor Model This section presents modifications to the incremental models that account for non-ideal transistor behavior Incremental output port resistance Incremental changes
More informationThe Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002
Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The Devices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction
More informationThe K-Input Floating-Gate MOS (FGMOS) Transistor
The K-Input Floating-Gate MOS (FGMOS) Transistor C 1 V D C 2 V D I V D I V S Q C 1 C 2 V S V K Q V K C K Layout V B V K C K Circuit Symbols V S Control Gate Floating Gate Interpoly Oxide Field Oxide Gate
More information55:041 Electronic Circuits The University of Iowa Fall Exam 2
Exam 2 Name: Score /60 Question 1 One point unless indicated otherwise. 1. An engineer measures the (step response) rise time of an amplifier as t r = 0.35 μs. Estimate the 3 db bandwidth of the amplifier.
More informationCircuit Topologies & Analysis Techniques in HF ICs
Circuit Topologies & Analysis Techniques in HF ICs 1 Outline Analog vs. Microwave Circuit Design Impedance matching Tuned circuit topologies Techniques to maximize bandwidth Challenges in differential
More informationElectronics II. Final Examination
The University of Toledo f6fs_elct7.fm - Electronics II Final Examination Problems Points. 5. 0 3. 5 Total 40 Was the exam fair? yes no The University of Toledo f6fs_elct7.fm - Problem 5 points Given is
More informationEE 435. Lecture 37. Parasitic Capacitances in MOS Devices. String DAC Parasitic Capacitances
EE 435 Lecture 37 Parasitic Capacitances in MOS Devices String DAC Parasitic Capacitances Parasitic Capacitors in MOSFET (will initially consider two) Parasitic Capacitors in MOSFET C GCH Parasitic Capacitors
More informationand V DS V GS V T (the saturation region) I DS = k 2 (V GS V T )2 (1+ V DS )
ECE 4420 Spring 2005 Page 1 FINAL EXAMINATION NAME SCORE /100 Problem 1O 2 3 4 5 6 7 Sum Points INSTRUCTIONS: This exam is closed book. You are permitted four sheets of notes (three of which are your sheets
More informationLecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics. Lena Peterson
Lecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics Lena Peterson 2015-10-13 Outline (1) Why is the CMOS inverter gain not infinite? Large-signal
More informationEE 230 Lecture 31. THE MOS TRANSISTOR Model Simplifcations THE Bipolar Junction TRANSISTOR
EE 23 Lecture 3 THE MOS TRANSISTOR Model Simplifcations THE Bipolar Junction TRANSISTOR Quiz 3 Determine I X. Assume W=u, L=2u, V T =V, uc OX = - 4 A/V 2, λ= And the number is? 3 8 5 2? 6 4 9 7 Quiz 3
More informationEE C245 ME C218 Introduction to MEMS Design
EE C45 ME C8 Introduction to MEMS Design Fall 007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 9470 Lecture 5: Output t
More informationLecture 23 - Frequency Resp onse of Amplifiers (I) Common-Source Amplifier. May 6, 2003
6.0 Microelectronic Devices and Circuits Spring 003 Lecture 3 Lecture 3 Frequency Resp onse of Amplifiers (I) CommonSource Amplifier May 6, 003 Contents:. Intro duction. Intrinsic frequency resp onse of
More informationECE 342 Electronic Circuits. 3. MOS Transistors
ECE 342 Electronic Circuits 3. MOS Transistors Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu 1 NMOS Transistor Typically L = 0.1 to 3 m, W = 0.2 to
More informationHalf-circuit incremental analysis techniques
6.012 Electronic Devices and Circuits Lecture 19 Differential Amplifier Stages Outline Announcements Handouts Lecture Outline and Summary Design Problem out tomorrow in recitation Review Singletransistor
More information55:041 Electronic Circuits The University of Iowa Fall Final Exam
Final Exam Name: Score Max: 135 Question 1 (1 point unless otherwise noted) a. What is the maximum theoretical efficiency for a class-b amplifier? Answer: 78% b. The abbreviation/term ESR is often encountered
More informationECE 523/421 - Analog Electronics University of New Mexico Solutions Homework 3
ECE 523/42 - Analog Electronics University of New Mexico Solutions Homework 3 Problem 7.90 Show that when ro is taken into account, the voltage gain of the source follower becomes G v v o v sig R L r o
More informationElectronic Circuits 1. Transistor Devices. Contents BJT and FET Characteristics Operations. Prof. C.K. Tse: Transistor devices
Electronic Circuits 1 Transistor Devices Contents BJT and FET Characteristics Operations 1 What is a transistor? Three-terminal device whose voltage-current relationship is controlled by a third voltage
More informationMOSFET: Introduction
E&CE 437 Integrated VLSI Systems MOS Transistor 1 of 30 MOSFET: Introduction Metal oxide semiconductor field effect transistor (MOSFET) or MOS is widely used for implementing digital designs Its major
More informationCMOS Analog Circuits
CMOS Analog Circuits L6: Common Source Amplifier-1 (.8.13) B. Mazhari Dept. of EE, IIT Kanpur 19 Problem statement : Design an amplifier which has the following characteristics: + CC O in R L - CC A 100
More informationQuick Review. ESE319 Introduction to Microelectronics. and Q1 = Q2, what is the value of V O-dm. If R C1 = R C2. s.t. R C1. Let Q1 = Q2 and R C1
Quick Review If R C1 = R C2 and Q1 = Q2, what is the value of V O-dm? Let Q1 = Q2 and R C1 R C2 s.t. R C1 > R C2, express R C1 & R C2 in terms R C and ΔR C. If V O-dm is the differential output offset
More informationSwitched-Capacitor Circuits David Johns and Ken Martin University of Toronto
Switched-Capacitor Circuits David Johns and Ken Martin University of Toronto (johns@eecg.toronto.edu) (martin@eecg.toronto.edu) University of Toronto 1 of 60 Basic Building Blocks Opamps Ideal opamps usually
More informationEE C245 ME C218 Introduction to MEMS Design
EE C45 ME C18 Introduction to MEMS Design Fall 008 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 9470 Lecture 6: Output
More informationLecture 3: CMOS Transistor Theory
Lecture 3: CMOS Transistor Theory Outline Introduction MOS Capacitor nmos I-V Characteristics pmos I-V Characteristics Gate and Diffusion Capacitance 2 Introduction So far, we have treated transistors
More informationTOSHIBA Field Effect Transistor Silicon N Channel MOS Type (π MOSIII) 2SK2610
TOSHIBA Field Effect Transistor Silicon N Channel MOS Type (π MOSIII) Chopper Regulator, DC DC Converter and Motor Drive Applications Unit: mm Low drain source ON resistance : RDS (ON) = 2.3 Ω (typ.) High
More informationChapter 2 Switched-Capacitor Circuits
Chapter 2 Switched-Capacitor Circuits Abstract his chapter introduces SC circuits. A brief description is given for the main building blocks of a SC filter (operational amplifiers, switches, capacitors,
More informationFinal Exam. 55:041 Electronic Circuits. The University of Iowa. Fall 2013.
Final Exam Name: Max: 130 Points Question 1 In the circuit shown, the op-amp is ideal, except for an input bias current I b = 1 na. Further, R F = 10K, R 1 = 100 Ω and C = 1 μf. The switch is opened at
More informationEECS240 Spring Today s Lecture. Lecture 2: CMOS Technology and Passive Devices. Lingkai Kong EECS. EE240 CMOS Technology
EECS240 Spring 2013 Lecture 2: CMOS Technology and Passive Devices Lingkai Kong EECS Today s Lecture EE240 CMOS Technology Passive devices Motivation Resistors Capacitors (Inductors) Next time: MOS transistor
More informationExact Analysis of a Common-Source MOSFET Amplifier
Exact Analysis of a Common-Source MOSFET Amplifier Consider the common-source MOSFET amplifier driven from signal source v s with Thévenin equivalent resistance R S and a load consisting of a parallel
More informationTPC8116-H TPC8116-H. High Efficiency DC/DC Converter Applications Notebook PC Applications Portable Equipment Applications CCFL Inverter Applications
TOSHIBA Field Effect Transistor Silicon P-Channel MOS Type (Ultra-High-Speed U-MOSIII) High Efficiency DC/DC Converter Applications Notebook PC Applications Portable Equipment Applications CCFL Inverter
More informationTSP10N60M / TSF10N60M
TSP10N60M / TSF10N60M 600V N-Channel MOSFET General Description This Power MOSFET is produced using Truesemi s advanced planar stripe DMOS technology. This advanced technology has been especially tailored
More informationUNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences
UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences E. Alon Final EECS 240 Monday, May 19, 2008 SPRING 2008 You should write your results on the exam
More informationfigure shows a pnp transistor biased to operate in the active mode
Lecture 10b EE-215 Electronic Devices and Circuits Asst Prof Muhammad Anis Chaudhary BJT: Device Structure and Physical Operation The pnp Transistor figure shows a pnp transistor biased to operate in the
More informationPOWER SUPPLY INDUCED JITTER MODELING OF AN ON- CHIP LC OSCILLATOR. Shahriar Rokhsaz, Jinghui Lu, Brian Brunn
POWER SUPPY INDUED JITTER MODEING OF AN ON- HIP OSIATOR Shahriar Rokhsaz, Jinghui u, Brian Brunn Rockethips Inc. (A Xilinx, Inc. Division) ABSTRAT This paper concentrates on developing a closed-form small
More information500V N-Channel MOSFET
830 / 830 500V N-Channel MOSFET General Description This Power MOSFET is produced using SL semi s advanced planar stripe DMOS technology. This advanced technology has been especially tailored to minimize
More informationCARLETON UNIVERSITY. FINAL EXAMINATION December DURATION 3 HOURS No. of Students 130
ALETON UNIVESITY FINAL EXAMINATION December 005 DUATION 3 HOUS No. of Students 130 Department Name & ourse Number: Electronics ELE 3509 ourse Instructor(s): Prof. John W. M. ogers and alvin Plett AUTHOIZED
More informationAnalog Integrated Circuit Design Prof. Nagendra Krishnapura Department of Electrical Engineering Indian Institute of Technology, Madras
Analog Integrated Circuit Design Prof. Nagendra Krishnapura Department of Electrical Engineering Indian Institute of Technology, Madras Lecture No - 42 Fully Differential Single Stage Opamp Hello and welcome
More informationELECTRONIC SYSTEMS. Basic operational amplifier circuits. Electronic Systems - C3 13/05/ DDC Storey 1
Electronic Systems C3 3/05/2009 Politecnico di Torino ICT school Lesson C3 ELECTONIC SYSTEMS C OPEATIONAL AMPLIFIES C.3 Op Amp circuits» Application examples» Analysis of amplifier circuits» Single and
More information