ECE 2C, notes set 7: Basic Transistor Circuits; High-Frequency Response

Size: px
Start display at page:

Download "ECE 2C, notes set 7: Basic Transistor Circuits; High-Frequency Response"

Transcription

1 class notes, M. odwell, copyrhted 013 EE, notes set 7: Basc Transstor rcuts; Hh-Frequency esponse Mark odwell Unversty of alforna, Santa Barbara , fax

2 oals class notes, M. odwell, copyrhted 013 These notes : calculate crcut transfer functons H ( s. Low - frequency rolloff. Hh - frequency rolloff. Frequency response.transent reponse. oals : Becoe Becoe expert n crcut analyss. expert n LaPlace ethods. Transstor crcuts ake ood exercses they are real, nterestn, useful. : LaPlace analyss: portant n ost partsof electrcal enneern

3 Feld-Effect Transstor Hh-Frequency Model class notes, M. odwell, copyrhted 013 Physcalorn of these capactances For ecec, we sply take ths odel wll as ven. be covered n later classes.

4 Feld-Effect Transstor Hh-Frequency Model class notes, M. odwell, copyrhted 013 sb db arses ostly fro ate - channel capactance Partly due to ate -source frnn felds, and nterconnect vas. d arses n part fro ate - channel capactance Partly due to ate -source frnn felds and nterconnect vas. sb and db are source - bulk (substrate and dran - bulk PNjuncton capactances. Many of these capactances vary wthbas voltae.

5 Basc oon-source Aplfer class notes, M. odwell, copyrhted 013 Ths crcut : 1950's - style basn n and and wll wll reduce reduce the crcut an at low frequences. the crcut an at hh frequences.

6 Basc oon-source Aplfer class notes, M. odwell, copyrhted 013 Sall -snal equvalent crcut : n and and wll wll reduce reduce the crcut an at low frequences. the crcut an at hh frequences.

7 Basc oon-source Aplfer class notes, M. odwell, copyrhted 013 Let us frst consder responseat hh frequences. We wll therefore teporarly nelect n and.

8 Nodal Analyss: How to solve crcuts class notes, M. odwell, copyrhted 013 Label all crcut nodes. For each :s the voltae known? known voltae (blue, unknown voltae (red Tosolve crcut # of Wrte the equatons ust be *lnearly ndependent *. Alwaysves : equatons # of node currents 0 at each node whch you do not know the voltae. the needed set of unknowns # of unknown node voltaes lnearly ndependent equatons.

9 oon-source Aplfer: Splfyn class notes, M. odwell, copyrhted 013 onvert the erator froa Thevenn to a Norton odel : And then use parallel resstor forulas :

10 class notes, M. odwell, copyrhted 013 oon-source: Nodal Analyss n n n n n ( ( ( zero: s currents at Su of 0 ( ( 0 ( ( ( zero: s currents at Su of n n n

11 class notes, M. odwell, copyrhted 013 oon-source: Nodal Analyss 0 ( ( ( ( n n 0 n

12 class notes, M. odwell, copyrhted 013 oon-source: Nodal Analyss 0 n n n 0 / / n

13 class notes, M. odwell, copyrhted 013 oon-source: Nodal Analyss 0 ( and ( where ( ( ( ( ( ( s N s D s s D s N s s H s

14 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 D( s D( s D( s

15 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 oranze nto powersof D( s s s s :

16 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 Separate nto a constant carryn unts ultpled by a untless frequency response: D( s / 1 s s D( s 1 s 1 s s (1 s

17 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 Follow the sae rules for the nuerator : N( s 0 1 /

18 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 N( s D( s 1 1 s / (1 s N( s D( s 1 s 1 / (1 s So ( s ( s H ( s 1 s 1 / (1 s

19 oon-source: Nodal Analyss class notes, M. odwell, copyrhted 013 H H ( s noralzed ( s H 1 d band s (1 s H noralzed ( s 1 / H d band ( n, Ap n, Ap n, Ap n, Ap n, Ap

20 oon-source Nodal Analyss: the answer class notes, M. odwell, copyrhted 013 H H where H d band noralzed d band ( s H noralzed 1 b1s 1 a s a 1 n, Ap ( s s n, Ap s the d - band an. s the aplfer frequency response. Frst - order te constant : a 1 Second and b 1 - order (te / constant : a

21 oents on the analyss class notes, M. odwell, copyrhted 013

22 Fndn Poles: Separated Pole Approxaton class notes, M. odwell, copyrhted 013

23 Fndn Poles: Separated Pole Approxaton class notes, M. odwell, copyrhted 013

24 Aplfer Frequency esponse class notes, M. odwell, copyrhted 013

25 Exaple class notes, M. odwell, copyrhted 013

26 Frequency esponse Exaple (1: D class notes, M. odwell, copyrhted 013 * weare norn the (1 bas analyss. Don ths causes soe sall error. If we do not, the D analyss nvolves solvn quadratc forulas. sall snal analyss. Hard. In EE137A we wll learn soe trcks calculate ths quckly yet farly accurately. Donot nore the (1 DS DS ter n the to ter n the FET : ( c th ox W / L 0.3 1/ 10 Analyss: I D ( ( current throuh D ( c DS 1 th ox W 0.5. ( I 0.3 ( 100 k, DD DD I 1A/ / L D D DS 1/ ( ( c 50 A D L / I D ox 50 k 1 1A W th / L 1A/ Desn condtons I DS D DD A 3.3 ( ter nored 50 A 1/ 1/ ( / 50 A 5 k 0.5/1 A 50 k, 0. ( /10 A.78 M,

27 class notes, M. odwell, copyrhted 013 Frequency esponse Exaple (: oponent alues M 5 k k ds 0.47 S 5S 50 k 50 k FET : I D ds ( c ox (A/ I D ds W / L 1A ( I D (1 50 A (1 I ( (1 0.7/ S DS th I D DS 50 A 10 D 1 5S 00 k ( c ox W / L ( th (1 DS

28 class notes, M. odwell, copyrhted 013 Frequency esponse Exaple (3: oponent alues 00k 100 k 5 k 50k 5.5k 50 k.78m 438k 0.47 S

29 class notes, M. odwell, copyrhted 013 Frequency esponse Exaple (4: oponent alues 1pF 0.5 pf 0.47 S 8k.6k

30 class notes, M. odwell, copyrhted 013 Frequency esponse Exaple (5: (te n constants H H H d band noralzed d band H noralzed 1 b1s ( s 1 a s a ( s s a a a 1 8k1pF 8k0.5pF 0.47S8k.6k0.5pF.6k0.5pF 0.36s / a a 1, a / a 1 8k.6k1pF0.5pF/0.36s 1.4ns so, separated pole approxaton works. b 1 / 0.5pF/0.47S 0.53 ns

31 class notes, M. odwell, copyrhted 013 Frequency esponse Exaple (6: Transfer Functon a 1 ( s 1 b1s 8.65 ( s (1 a s(1 ( a 0.36s, a / a ns, b / a 1 1 s 0.53 ns f f p1 z ( jf 8.65 ( jf (1 jf khz, f 0.36s ps 1 / f p p1 jf / f z (1 jf ns 11 MHz 99 MHz(zeron the rht half / f p of thes - plane

32 class notes, M. odwell, copyrhted 013 The Mller Effect

33 The Mller Approxaton class notes, M. odwell, copyrhted 013

34 The Mller Approxaton class notes, M. odwell, copyrhted 013

35 The Mller Approxaton class notes, M. odwell, copyrhted 013 efer back to the coon - source analyss You wll.e. see (1 (1 v A

36 class notes, M. odwell, copyrhted 013 Usn Mller Approxaton to Understand esponse

37 class notes, M. odwell, copyrhted 013 Usn Mller Approxaton to Understand esponse Low - frequency an fro Approxate: replace wth ller to s ( 1 ller 1/ f ( (1 pole ller

38 Mller and Exact Solutons class notes, M. odwell, copyrhted 013 Exact soluton a a 1

39 class notes, M. odwell, copyrhted 013 Further oents eardn Mller Approxaton

40 class notes, M. odwell, copyrhted 013 Frequency/Transent eponse: eal, Iportant

Week 9: Multivibrators, MOSFET Amplifiers

Week 9: Multivibrators, MOSFET Amplifiers ELE 2110A Electronc Crcuts Week 9: Multbrators, MOSFET Aplfers Lecture 09-1 Multbrators Topcs to coer Snle-stae MOSFET aplfers Coon-source aplfer Coon-dran aplfer Coon-ate aplfer eadn Assnent: Chap 14.1-14.5

More information

ES 330 Electronics II Homework 04 (Fall 2017 Due Wednesday, September 27, 2017)

ES 330 Electronics II Homework 04 (Fall 2017 Due Wednesday, September 27, 2017) Pae1 Nae Solutons ES 330 Electroncs II Hoework 04 (Fall 2017 Due Wednesday, Septeer 27, 2017) Prole 1 onsder the FET aplfer of F. 7.10 for the case of t =0.4, kn = 5 A/ 2, GS =0.6, DD = 1.8 and RD = 10

More information

Lecture 14: More MOS Circuits and the Differential Amplifier

Lecture 14: More MOS Circuits and the Differential Amplifier Lecture 4: More MOS rcuts an the Dfferental Aplfer Gu-Yeon We Dson of nneern an Apple Scences Harar Unersty uyeon@eecs.harar.eu We Oerew Rean S&S: hapter 5.0, 6.~, 6.6 ackroun Han seen soe of the basc

More information

Our focus will be on linear systems. A system is linear if it obeys the principle of superposition and homogenity, i.e.

Our focus will be on linear systems. A system is linear if it obeys the principle of superposition and homogenity, i.e. SSTEM MODELLIN In order to solve a control syste proble, the descrptons of the syste and ts coponents ust be put nto a for sutable for analyss and evaluaton. The followng ethods can be used to odel physcal

More information

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax .9.1: AC power analyss Reson: Deceber 13, 010 15 E Man Sute D Pullan, WA 99163 (509 334 6306 Voce and Fax Oerew n chapter.9.0, we ntroduced soe basc quanttes relate to delery of power usng snusodal sgnals.

More information

Lecture #4 Capacitors and Inductors Energy Stored in C and L Equivalent Circuits Thevenin Norton

Lecture #4 Capacitors and Inductors Energy Stored in C and L Equivalent Circuits Thevenin Norton EES ntro. electroncs for S Sprng 003 Lecture : 0/03/03 A.R. Neureuther Verson Date 0/0/03 EES ntroducton to Electroncs for omputer Scence Andrew R. Neureuther Lecture # apactors and nductors Energy Stored

More information

Fermi-Dirac statistics

Fermi-Dirac statistics UCC/Physcs/MK/EM/October 8, 205 Fer-Drac statstcs Fer-Drac dstrbuton Matter partcles that are eleentary ostly have a type of angular oentu called spn. hese partcles are known to have a agnetc oent whch

More information

Complex Numbers, Signals, and Circuits

Complex Numbers, Signals, and Circuits Complex Numbers, Sgnals, and Crcuts 3 August, 009 Complex Numbers: a Revew Suppose we have a complex number z = x jy. To convert to polar form, we need to know the magntude of z and the phase of z. z =

More information

Chapter 10 Sinusoidal Steady-State Power Calculations

Chapter 10 Sinusoidal Steady-State Power Calculations Chapter 0 Snusodal Steady-State Power Calculatons n Chapter 9, we calculated the steady state oltages and currents n electrc crcuts dren by snusodal sources. We used phasor ethod to fnd the steady state

More information

MAE140 - Linear Circuits - Winter 16 Final, March 16, 2016

MAE140 - Linear Circuits - Winter 16 Final, March 16, 2016 ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 00 Crcut Analyss Lesson 3 Chapter : AC Power Analyss (nstant & Ae Power; Max Ae Power Transfer; Effecte or RMS alue, Power Factor, Coplex Power, Power Trangle, Power Factor Correcton Danel M. Ltynsk,

More information

Excess Error, Approximation Error, and Estimation Error

Excess Error, Approximation Error, and Estimation Error E0 370 Statstcal Learnng Theory Lecture 10 Sep 15, 011 Excess Error, Approxaton Error, and Estaton Error Lecturer: Shvan Agarwal Scrbe: Shvan Agarwal 1 Introducton So far, we have consdered the fnte saple

More information

Selected Student Solutions for Chapter 2

Selected Student Solutions for Chapter 2 /3/003 Assessment Prolems Selected Student Solutons for Chapter. Frst note that we know the current through all elements n the crcut except the 6 kw resstor (the current n the three elements to the left

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electronc Crcuts Feedback & Stablty Sectons of Chapter 2. Kruger Feedback & Stablty Confguraton of Feedback mplfer Negate feedback β s the feedback transfer functon S o S S o o S S o f S S S S fb

More information

Microelectronics Circuit Analysis and Design. NMOS Common-Source Circuit. NMOS Common-Source Circuit 10/15/2013. In this chapter, we will:

Microelectronics Circuit Analysis and Design. NMOS Common-Source Circuit. NMOS Common-Source Circuit 10/15/2013. In this chapter, we will: Mcrelectrncs Crcut Analyss and Desn Dnald A. Neaen Chapter 4 Basc FET Aplfers In ths chapter, we wll: Inestate a snle-transstr crcut that can aplfy a sall, te-aryn nput snal Deelp sall-snal dels that are

More information

Final Exam Solutions, 1998

Final Exam Solutions, 1998 58.439 Fnal Exa Solutons, 1998 roble 1 art a: Equlbru eans that the therodynac potental of a consttuent s the sae everywhere n a syste. An exaple s the Nernst potental. If the potental across a ebrane

More information

System in Weibull Distribution

System in Weibull Distribution Internatonal Matheatcal Foru 4 9 no. 9 94-95 Relablty Equvalence Factors of a Seres-Parallel Syste n Webull Dstrbuton M. A. El-Dacese Matheatcs Departent Faculty of Scence Tanta Unversty Tanta Egypt eldacese@yahoo.co

More information

ECSE Linearity Superposition Principle Superposition Example Dependent Sources. 10 kω. 30 V 5 ma. 6 kω. 2 kω

ECSE Linearity Superposition Principle Superposition Example Dependent Sources. 10 kω. 30 V 5 ma. 6 kω. 2 kω S-00 Lnearty Superposton Prncple Superposton xample Dependent Sources Lecture 4. sawyes@rp.edu www.rp.edu/~sawyes 0 kω 6 kω 8 V 0 V 5 ma 4 Nodes Voltage Sources Ref Unknown Node Voltage, kω If hae multple

More information

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab Bose State Unersty Department of Electrcal and omputer Engneerng EE 1L rcut Analyss and Desgn Lab Experment #8: The Integratng and Dfferentatng Op-Amp rcuts 1 Objectes The objectes of ths laboratory experment

More information

MAE140 - Linear Circuits - Fall 13 Midterm, October 31

MAE140 - Linear Circuits - Fall 13 Midterm, October 31 Instructons ME140 - Lnear Crcuts - Fall 13 Mdterm, October 31 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electronc Crcuts Feedback & Stablty Sectons of Chapter 2. Kruger Feedback & Stablty Confguraton of Feedback mplfer S o S ε S o ( S β S ) o Negate feedback S S o + β β s the feedback transfer functon

More information

MAE140 - Linear Circuits - Winter 16 Midterm, February 5

MAE140 - Linear Circuits - Winter 16 Midterm, February 5 Instructons ME140 - Lnear Crcuts - Wnter 16 Mdterm, February 5 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator

More information

Week 11: Differential Amplifiers

Week 11: Differential Amplifiers ELE 0A Electronc rcuts Week : Dfferental Amplfers Lecture - Large sgnal analyss Topcs to coer A analyss Half-crcut analyss eadng Assgnment: hap 5.-5.8 of Jaeger and Blalock or hap 7. - 7.3, of Sedra and

More information

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng EE59 Spring Parallel LSI AD Algoriths Lecture I interconnect odeling ethods Zhuo Feng. Z. Feng MTU EE59 So far we ve considered only tie doain analyses We ll soon see that it is soeties preferable to odel

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 00 Crcut Analyss Lesson 3 Chapter : AC Power Analyss (nstant & Ae Power; Max Ae Power Transfer; Effecte or RMS alue, Power Factor, Coplex Power, Power Trangle, Power Factor Correcton Danel M. Ltynsk,

More information

1 cos. where v v sin. Range Equations: for an object that lands at the same height at which it starts. v sin 2 i. t g. and. sin g

1 cos. where v v sin. Range Equations: for an object that lands at the same height at which it starts. v sin 2 i. t g. and. sin g SPH3UW Unt.5 Projectle Moton Pae 1 of 10 Note Phc Inventor Parabolc Moton curved oton n the hape of a parabola. In the drecton, the equaton of oton ha a t ter Projectle Moton the parabolc oton of an object,

More information

The Impact of the Earth s Movement through the Space on Measuring the Velocity of Light

The Impact of the Earth s Movement through the Space on Measuring the Velocity of Light Journal of Appled Matheatcs and Physcs, 6, 4, 68-78 Publshed Onlne June 6 n ScRes http://wwwscrporg/journal/jap http://dxdoorg/436/jap646 The Ipact of the Earth s Moeent through the Space on Measurng the

More information

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab Bose State Unersty Department of Electrcal and omputer Engneerng EE 1L rcut Analyss and Desgn Lab Experment #8: The Integratng and Dfferentatng Op-Amp rcuts 1 Objectes The objectes of ths laboratory experment

More information

Key component in Operational Amplifiers

Key component in Operational Amplifiers Key component n Operatonal Amplfers Objectve of Lecture Descrbe how dependent voltage and current sources functon. Chapter.6 Electrcal Engneerng: Prncples and Applcatons Chapter.6 Fundamentals of Electrc

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d)

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d) Massachusetts Insttute of Technology Department of Electrcal Engneerng and Computer Scence 6.002 í Electronc Crcuts Homework 2 Soluton Handout F98023 Exercse 21: Determne the conductance of each network

More information

Estimating Delays. Gate Delay Model. Gate Delay. Effort Delay. Computing Logical Effort. Logical Effort

Estimating Delays. Gate Delay Model. Gate Delay. Effort Delay. Computing Logical Effort. Logical Effort Estmatng Delas Would be nce to have a back of the envelope method for szng gates for speed Logcal Effort ook b Sutherland, Sproull, Harrs Chapter s on our web page Gate Dela Model Frst, normalze a model

More information

On Pfaff s solution of the Pfaff problem

On Pfaff s solution of the Pfaff problem Zur Pfaff scen Lösung des Pfaff scen Probles Mat. Ann. 7 (880) 53-530. On Pfaff s soluton of te Pfaff proble By A. MAYER n Lepzg Translated by D. H. Delpenc Te way tat Pfaff adopted for te ntegraton of

More information

Exercises for Frequency Response. ECE 102, Winter 2011, F. Najmabadi

Exercises for Frequency Response. ECE 102, Winter 2011, F. Najmabadi Eercses r Frequency espnse EE 0, Wnter 0, F. Najabad Eercse : A Mdy the crcut belw t nclude a dnant ple at 00 Mz ( 00 Ω, k, k, / 00 Ω, λ 0, and nre nternal capactances the MOS. pute the dnant ple n the

More information

Start with the equation of motion for a linear multi-degree of freedom system with base ground excitation:

Start with the equation of motion for a linear multi-degree of freedom system with base ground excitation: SE 80 Earthquake Enneern November 3, 00 STEP-BY-STEP PROCEDURE FOR SETTING UP A SPREADSHEET FOR USING NEWMARK S METHOD AND MODAL ANALYSIS TO SOLVE FOR THE RESPONSE OF A MULTI-DEGREE OF FREEDOM (MDOF) SYSTEM

More information

Chemical Engineering 160/260 Polymer Science and Engineering. Lecture 10 - Phase Equilibria and Polymer Blends February 7, 2001

Chemical Engineering 160/260 Polymer Science and Engineering. Lecture 10 - Phase Equilibria and Polymer Blends February 7, 2001 Checal Engneerng 60/60 Polyer Scence and Engneerng Lecture 0 - Phase Equlbra and Polyer Blends February 7, 00 Therodynacs of Polyer Blends: Part Objectves! To develop the classcal Flory-Huggns theory for

More information

Chapter 12 Lyes KADEM [Thermodynamics II] 2007

Chapter 12 Lyes KADEM [Thermodynamics II] 2007 Chapter 2 Lyes KDEM [Therodynacs II] 2007 Gas Mxtures In ths chapter we wll develop ethods for deternng therodynac propertes of a xture n order to apply the frst law to systes nvolvng xtures. Ths wll be

More information

CHAPTER 7 CONSTRAINED OPTIMIZATION 1: THE KARUSH-KUHN-TUCKER CONDITIONS

CHAPTER 7 CONSTRAINED OPTIMIZATION 1: THE KARUSH-KUHN-TUCKER CONDITIONS CHAPER 7 CONSRAINED OPIMIZAION : HE KARUSH-KUHN-UCKER CONDIIONS 7. Introducton We now begn our dscusson of gradent-based constraned optzaton. Recall that n Chapter 3 we looked at gradent-based unconstraned

More information

Gradient Descent Learning and Backpropagation

Gradient Descent Learning and Backpropagation Artfcal Neural Networks (art 2) Chrstan Jacob Gradent Descent Learnng and Backpropagaton CSC 533 Wnter 200 Learnng by Gradent Descent Defnton of the Learnng roble Let us start wth the sple case of lnear

More information

OPTIMUM DESIGN OF FREQUENCY SELECTIVE AMPLIFIER INTENDED FOR CHOPPER STABILIZED APLICATIONS. Andrei DANCHIV, Mircea BODEA, Claudius DAN

OPTIMUM DESIGN OF FREQUENCY SELECTIVE AMPLIFIER INTENDED FOR CHOPPER STABILIZED APLICATIONS. Andrei DANCHIV, Mircea BODEA, Claudius DAN OPTMUM DESGN OF FEQUENY SELETE AMPLFE NTENDED FO OPPE STABLZED APLATONS Anre DAN Mrcea BODEA lauus DAN POLTENA Unversty of Bucharest Electroncs Teleco. an T Dept. str. ulu Manu nr. -3 67 Bucharest oana

More information

ELECTRONICS. EE 42/100 Lecture 4: Resistive Networks and Nodal Analysis. Rev B 1/25/2012 (9:49PM) Prof. Ali M. Niknejad

ELECTRONICS. EE 42/100 Lecture 4: Resistive Networks and Nodal Analysis. Rev B 1/25/2012 (9:49PM) Prof. Ali M. Niknejad A. M. Nknejad Unversty of Calforna, Berkeley EE 100 / 42 Lecture 4 p. 1/14 EE 42/100 Lecture 4: Resstve Networks and Nodal Analyss ELECTRONICS Rev B 1/25/2012 (9:49PM) Prof. Al M. Nknejad Unversty of Calforna,

More information

ELECTRONIC DEVICES. Assist. prof. Laura-Nicoleta IVANCIU, Ph.D. C13 MOSFET operation

ELECTRONIC DEVICES. Assist. prof. Laura-Nicoleta IVANCIU, Ph.D. C13 MOSFET operation ELECTRONIC EVICES Assst. prof. Laura-Ncoleta IVANCIU, Ph.. C13 MOSFET operaton Contents Symbols Structure and physcal operaton Operatng prncple Transfer and output characterstcs Quescent pont Operatng

More information

Projectile Motion. Parabolic Motion curved motion in the shape of a parabola. In the y direction, the equation of motion has a t 2.

Projectile Motion. Parabolic Motion curved motion in the shape of a parabola. In the y direction, the equation of motion has a t 2. Projectle Moton Phc Inentor Parabolc Moton cured oton n the hape of a parabola. In the drecton, the equaton of oton ha a t ter Projectle Moton the parabolc oton of an object, where the horzontal coponent

More information

MAE140 - Linear Circuits - Fall 10 Midterm, October 28

MAE140 - Linear Circuits - Fall 10 Midterm, October 28 M140 - Lnear rcuts - Fall 10 Mdterm, October 28 nstructons () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator

More information

Special Relativity and Riemannian Geometry. Department of Mathematical Sciences

Special Relativity and Riemannian Geometry. Department of Mathematical Sciences Tutoral Letter 06//018 Specal Relatvty and Reannan Geoetry APM3713 Seester Departent of Matheatcal Scences IMPORTANT INFORMATION: Ths tutoral letter contans the solutons to Assgnent 06. BAR CODE Learn

More information

Limit Cycle Bifurcations in a Class of Cubic System near a Nilpotent Center *

Limit Cycle Bifurcations in a Class of Cubic System near a Nilpotent Center * Appled Mateatcs 77-777 ttp://dxdoorg/6/a75 Publsed Onlne July (ttp://wwwscrporg/journal/a) Lt Cycle Bfurcatons n a Class of Cubc Syste near a Nlpotent Center * Jao Jang Departent of Mateatcs Sanga Marte

More information

Chapter 8 Deflection. Structural Mechanics 2 Dept of Architecture

Chapter 8 Deflection. Structural Mechanics 2 Dept of Architecture Chapter 8 Deflection Structural echanics Dept of rchitecture Outline Deflection diagras and the elastic curve Elastic-bea theory The double integration ethod oent-area theores Conjugate-bea ethod 8- Deflection

More information

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner.

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner. (C) 998 Gerald B Sheblé, all rghts reserved Lnear Prograng Introducton Contents I. What s LP? II. LP Theor III. The Splex Method IV. Refneents to the Splex Method What s LP? LP s an optzaton technque that

More information

VI. Transistor Amplifiers

VI. Transistor Amplifiers VI. Transstor Amplfers 6. Introducton In ths secton we wll use the transstor small-sgnal model to analyze and desgn transstor amplfers. There are two ssues that we need to dscuss frst: ) What are the mportant

More information

Copyright 2004 by Oxford University Press, Inc.

Copyright 2004 by Oxford University Press, Inc. JT as an Amplfer &a Swtch, Large Sgnal Operaton, Graphcal Analyss, JT at D, asng JT, Small Sgnal Operaton Model, Hybrd P-Model, TModel. Lecture # 7 1 Drecton of urrent Flow & Operaton for Amplfer Applcaton

More information

Solutions to Practice Problems

Solutions to Practice Problems Phys A Solutons to Practce Probles hapter Inucton an Maxwell s uatons (a) At t s, the ef has a agntue of t ag t Wb s t Wb s Wb s t Wb s V t 5 (a) Table - gves the resstvty of copper Thus, L A 8 9 5 (b)

More information

,..., k N. , k 2. ,..., k i. The derivative with respect to temperature T is calculated by using the chain rule: & ( (5) dj j dt = "J j. k i.

,..., k N. , k 2. ,..., k i. The derivative with respect to temperature T is calculated by using the chain rule: & ( (5) dj j dt = J j. k i. Suppleentary Materal Dervaton of Eq. 1a. Assue j s a functon of the rate constants for the N coponent reactons: j j (k 1,,..., k,..., k N ( The dervatve wth respect to teperature T s calculated by usng

More information

arxiv: v2 [math.co] 3 Sep 2017

arxiv: v2 [math.co] 3 Sep 2017 On the Approxate Asyptotc Statstcal Independence of the Peranents of 0- Matrces arxv:705.0868v2 ath.co 3 Sep 207 Paul Federbush Departent of Matheatcs Unversty of Mchgan Ann Arbor, MI, 4809-043 Septeber

More information

Advanced Circuits Topics - Part 1 by Dr. Colton (Fall 2017)

Advanced Circuits Topics - Part 1 by Dr. Colton (Fall 2017) Advanced rcuts Topcs - Part by Dr. olton (Fall 07) Part : Some thngs you should already know from Physcs 0 and 45 These are all thngs that you should have learned n Physcs 0 and/or 45. Ths secton s organzed

More information

ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES

ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES Journal of Algebra, Nuber Theory: Advances and Applcatons Volue 3, Nuber, 05, Pages 3-8 ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES Feldstrasse 45 CH-8004, Zürch Swtzerland e-al: whurlann@bluewn.ch

More information

Chapter 1. Theory of Gravitation

Chapter 1. Theory of Gravitation Chapter 1 Theory of Gravtaton In ths chapter a theory of gravtaton n flat space-te s studed whch was consdered n several artcles by the author. Let us assue a flat space-te etrc. Denote by x the co-ordnates

More information

Multipoint Analysis for Sibling Pairs. Biostatistics 666 Lecture 18

Multipoint Analysis for Sibling Pairs. Biostatistics 666 Lecture 18 Multpont Analyss for Sblng ars Bostatstcs 666 Lecture 8 revously Lnkage analyss wth pars of ndvduals Non-paraetrc BS Methods Maxu Lkelhood BD Based Method ossble Trangle Constrant AS Methods Covered So

More information

Preference and Demand Examples

Preference and Demand Examples Dvson of the Huantes and Socal Scences Preference and Deand Exaples KC Border October, 2002 Revsed Noveber 206 These notes show how to use the Lagrange Karush Kuhn Tucker ultpler theores to solve the proble

More information

Transfer Characteristic

Transfer Characteristic Eeld-Effect Transstors (FETs 3.3 The CMS Common-Source Amplfer Transfer Characterstc Electronc Crcuts, Dept. of Elec. Eng., The Chnese Unersty of Hong Kong, Prof. K.-L. Wu Lesson 8&9 Eeld-Effect Transstors

More information

College of Engineering Department of Electronics and Communication Engineering. Test 1 With Model Answer

College of Engineering Department of Electronics and Communication Engineering. Test 1 With Model Answer Name: Student D Number: Secton Number: 01/0/03/04 A/B Lecturer: Dr Jamaludn/ Dr Jehana Ermy/ Dr Azn Wat Table Number: College of Engneerng Department of Electroncs and Communcaton Engneerng Test 1 Wth

More information

Slobodan Lakić. Communicated by R. Van Keer

Slobodan Lakić. Communicated by R. Van Keer Serdca Math. J. 21 (1995), 335-344 AN ITERATIVE METHOD FOR THE MATRIX PRINCIPAL n-th ROOT Slobodan Lakć Councated by R. Van Keer In ths paper we gve an teratve ethod to copute the prncpal n-th root and

More information

CHAPTER 6 CONSTRAINED OPTIMIZATION 1: K-T CONDITIONS

CHAPTER 6 CONSTRAINED OPTIMIZATION 1: K-T CONDITIONS Chapter 6: Constraned Optzaton CHAPER 6 CONSRAINED OPIMIZAION : K- CONDIIONS Introducton We now begn our dscusson of gradent-based constraned optzaton. Recall that n Chapter 3 we looked at gradent-based

More information

Physics 4B. A positive value is obtained, so the current is counterclockwise around the circuit.

Physics 4B. A positive value is obtained, so the current is counterclockwise around the circuit. Physcs 4B Solutons to Chapter 7 HW Chapter 7: Questons:, 8, 0 Problems:,,, 45, 48,,, 7, 9 Queston 7- (a) no (b) yes (c) all te Queston 7-8 0 μc Queston 7-0, c;, a;, d; 4, b Problem 7- (a) Let be the current

More information

6.01: Introduction to EECS I Lecture 7 March 15, 2011

6.01: Introduction to EECS I Lecture 7 March 15, 2011 6.0: Introducton to EECS I Lecture 7 March 5, 20 6.0: Introducton to EECS I Crcuts The Crcut Abstracton Crcuts represent systems as connectons of elements through whch currents (through arables) flow and

More information

PHY2049 Exam 2 solutions Fall 2016 Solution:

PHY2049 Exam 2 solutions Fall 2016 Solution: PHY2049 Exam 2 solutons Fall 2016 General strategy: Fnd two resstors, one par at a tme, that are connected ether n SERIES or n PARALLEL; replace these two resstors wth one of an equvalent resstance. Now

More information

Electrical Circuits II (ECE233b)

Electrical Circuits II (ECE233b) Electrcal Crcuts (ECE33b SteadyState Power Analyss Anests Dounas The Unersty of Western Ontaro Faculty of Engneerng Scence SteadyState Power Analyss (t AC crcut: The steady state oltage and current can

More information

EE 330 Lecture 24. Small Signal Analysis Small Signal Analysis of BJT Amplifier

EE 330 Lecture 24. Small Signal Analysis Small Signal Analysis of BJT Amplifier EE 0 Lecture 4 Small Sgnal Analss Small Sgnal Analss o BJT Ampler Eam Frda March 9 Eam Frda Aprl Revew Sesson or Eam : 6:00 p.m. on Thursda March 8 n Room Sweene 6 Revew rom Last Lecture Comparson o Gans

More information

= m 1. sin π( ai z ) )

= m 1. sin π( ai z ) ) EXACT COVERING SYSTEMS AND THE GAUSS-LEGENDRE MULTIPLICATION FORMULA FOR THE GAMMA FUNCTION John Beeee Unversty of Alaska Anchorage July 0 199 The Gauss-Legendre ultplcaton forula for the gaa functon s

More information

Physics Courseware Electronics

Physics Courseware Electronics Physcs ourseware Electroncs ommon emtter amplfer Problem 1.- In the followg ommon Emtter mplfer calculate: a) The Q pot, whch s the D base current (I ), the D collector current (I ) and the voltage collector

More information

Applied Mathematics Letters

Applied Mathematics Letters Appled Matheatcs Letters 2 (2) 46 5 Contents lsts avalable at ScenceDrect Appled Matheatcs Letters journal hoepage: wwwelseverco/locate/al Calculaton of coeffcents of a cardnal B-splne Gradr V Mlovanovć

More information

ECEN326: Electronic Circuits Fall 2017

ECEN326: Electronic Circuits Fall 2017 EEN36: Electronic ircuits Fall 07 ecture 5: Frequency esponse a Palero Analo & Mixed-al enter Texas A&M University Announceents HW5 due / Exa /6 9:0-0:0 (0 extra utes) losed book w/ one standard note sheet

More information

Electrical Circuits 2.1 INTRODUCTION CHAPTER

Electrical Circuits 2.1 INTRODUCTION CHAPTER CHAPTE Electrcal Crcuts. INTODUCTION In ths chapter, we brefly revew the three types of basc passve electrcal elements: resstor, nductor and capactor. esstance Elements: Ohm s Law: The voltage drop across

More information

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions.

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions. Lesson 0: Collsons, Rotatonal netc Energy, Torque, Center o Graty (Sectons 7.8 Last te we used ewton s second law to deelop the pulse-oentu theore. In words, the theore states that the change n lnear oentu

More information

A Radon-Nikodym Theorem for Completely Positive Maps

A Radon-Nikodym Theorem for Completely Positive Maps A Radon-Nody Theore for Copletely Postve Maps V P Belavn School of Matheatcal Scences, Unversty of Nottngha, Nottngha NG7 RD E-al: vpb@aths.nott.ac.u and P Staszews Insttute of Physcs, Ncholas Coperncus

More information

EE C245 ME C218 Introduction to MEMS Design

EE C245 ME C218 Introduction to MEMS Design EE C45 ME C8 Introducton to MEM Desgn Fall 7 Prof. Clark T.C. Nguyen Dept. of Electrcal Engneerng & Computer cences Unersty of Calforna at Berkeley Berkeley, C 947 Dscusson: eew of Op mps EE C45: Introducton

More information

Physics 114 Exam 2 Spring Name:

Physics 114 Exam 2 Spring Name: Physcs 114 Exam Sprng 013 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red wth the amount beng

More information

Lecture-24. Enzyme kinetics and Enzyme inhibition-ii

Lecture-24. Enzyme kinetics and Enzyme inhibition-ii Lecture-24 Enzye knetcs and Enzye nhbton-ii Noncopette Inhbton A noncopette nhbtor can bnd wth enzye or wth enzye-substrate coplex to produce end coplex. Hence the nhbtor ust bnd at a dfferent ste fro

More information

PHYS 1443 Section 002 Lecture #20

PHYS 1443 Section 002 Lecture #20 PHYS 1443 Secton 002 Lecture #20 Dr. Jae Condtons for Equlbru & Mechancal Equlbru How to Solve Equlbru Probles? A ew Exaples of Mechancal Equlbru Elastc Propertes of Solds Densty and Specfc Gravty lud

More information

Physics 114 Exam 2 Fall 2014 Solutions. Name:

Physics 114 Exam 2 Fall 2014 Solutions. Name: Physcs 114 Exam Fall 014 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red. Unless otherwse ndcated,

More information

Scattering by a perfectly conducting infinite cylinder

Scattering by a perfectly conducting infinite cylinder Scatterng by a perfectly conductng nfnte cylnder Reeber that ths s the full soluton everywhere. We are actually nterested n the scatterng n the far feld lt. We agan use the asyptotc relatonshp exp exp

More information

PROBABILITY AND STATISTICS Vol. III - Analysis of Variance and Analysis of Covariance - V. Nollau ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE

PROBABILITY AND STATISTICS Vol. III - Analysis of Variance and Analysis of Covariance - V. Nollau ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE V. Nollau Insttute of Matheatcal Stochastcs, Techncal Unversty of Dresden, Gerany Keywords: Analyss of varance, least squares ethod, odels wth fxed effects,

More information

Chapter One Mixture of Ideal Gases

Chapter One Mixture of Ideal Gases herodynacs II AA Chapter One Mxture of Ideal Gases. Coposton of a Gas Mxture: Mass and Mole Fractons o deterne the propertes of a xture, we need to now the coposton of the xture as well as the propertes

More information

The Parity of the Number of Irreducible Factors for Some Pentanomials

The Parity of the Number of Irreducible Factors for Some Pentanomials The Party of the Nuber of Irreducble Factors for Soe Pentanoals Wolfra Koepf 1, Ryul K 1 Departent of Matheatcs Unversty of Kassel, Kassel, F. R. Gerany Faculty of Matheatcs and Mechancs K Il Sung Unversty,

More information

Quick Visit to Bernoulli Land

Quick Visit to Bernoulli Land Although we have een the Bernoull equaton and een t derved before, th next note how t dervaton for an uncopreble & nvcd flow. The dervaton follow that of Kuethe &Chow ot cloely (I lke t better than Anderon).

More information

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F) EN40: Dynacs and Vbratons Hoework 4: Work, Energy and Lnear Moentu Due Frday March 6 th School of Engneerng Brown Unversty 1. The Rydberg potental s a sple odel of atoc nteractons. It specfes the potental

More information

Generalized Thévenin/ Helmholtz and Norton/ Mayer Theorems of Electric Circuits With Variable Resistances

Generalized Thévenin/ Helmholtz and Norton/ Mayer Theorems of Electric Circuits With Variable Resistances WSES TRSTOS on RUTS and SSTEMS Penn lexandr eneralzed Thévenn/ Helholtz and orton/ Mayer Theores of Electrc rcuts Wth arable Resstances PE EXDR "D htu" nsttute of Electronc Engneerng and anotechnologes

More information

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2013

University of Washington Department of Chemistry Chemistry 452/456 Summer Quarter 2013 Lecture 8/8/3 Unversty o Washngton Departent o Chestry Chestry 45/456 Suer Quarter 3 A. The Gbbs-Duhe Equaton Fro Lecture 7 and ro the dscusson n sectons A and B o ths lecture, t s clear that the actvty

More information

% & 5.3 PRACTICAL APPLICATIONS. Given system, (49) , determine the Boolean Function, , in such a way that we always have expression: " Y1 = Y2

% & 5.3 PRACTICAL APPLICATIONS. Given system, (49) , determine the Boolean Function, , in such a way that we always have expression:  Y1 = Y2 5.3 PRACTICAL APPLICATIONS st EXAMPLE: Gven system, (49) & K K Y XvX 3 ( 2 & X ), determne the Boolean Functon, Y2 X2 & X 3 v X " X3 (X2,X)", n such a way that we always have expresson: " Y Y2 " (50).

More information

Surface Charge and Resistors

Surface Charge and Resistors Surface Charge and Resstors Just after connecton: E may be the same everywhere nav naue thn thck na na thn thck ue ue After steady state s reached: thn thck na thn thck na thn thck ue thn ue thck E thn

More information

+ v i F02E2P2 I. Solution (a.) The small-signal transfer function of the stages can be written as, V out (s) V in (s) = g m1 /g m3.

+ v i F02E2P2 I. Solution (a.) The small-signal transfer function of the stages can be written as, V out (s) V in (s) = g m1 /g m3. ECE 6440 Summer 003 Page 1 Homework Assgnment No. 7 s Problem 1 (10 ponts) A fourstage rng oscllator used as the VCO n a PLL s shown. Assume that M1 and M are matched and M3 and M4 are matched. Also assume

More information

EE 434 Lecture 16. Small signal model Small signal applications in amplifier analysis and design

EE 434 Lecture 16. Small signal model Small signal applications in amplifier analysis and design EE 434 Lecture 16 Sall sinal odel Sall sinal applications in aplifier analysis and desin Quiz 13 The of an n-channel OS transistor that has a quiescent current of 5A was easured to be 10A/. If the lenth

More information

Computational and Statistical Learning theory Assignment 4

Computational and Statistical Learning theory Assignment 4 Coputatonal and Statstcal Learnng theory Assgnent 4 Due: March 2nd Eal solutons to : karthk at ttc dot edu Notatons/Defntons Recall the defnton of saple based Radeacher coplexty : [ ] R S F) := E ɛ {±}

More information

CHAPTER 10 ROTATIONAL MOTION

CHAPTER 10 ROTATIONAL MOTION CHAPTER 0 ROTATONAL MOTON 0. ANGULAR VELOCTY Consder argd body rotates about a fxed axs through pont O n x-y plane as shown. Any partcle at pont P n ths rgd body rotates n a crcle of radus r about O. The

More information

EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING

EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING TaChang Chen Unersty of Washngton, Bothell Sprng 2010 EE215 1 WEEK 8 FIRST ORDER CIRCUIT RESPONSE May 21 st, 2010 EE215 2 1 QUESTIONS TO ANSWER Frst order crcuts

More information

1.4 Small-signal models of BJT

1.4 Small-signal models of BJT 1.4 Small-sgnal models of J Analog crcuts often operate wth sgnal levels that are small compared to the bas currents and voltages n the crcut. Under ths condton, ncremental or small-sgnal models can be

More information

Atmospheric Radiation Fall 2008

Atmospheric Radiation Fall 2008 MIT OpenCourseWare http://ocw.t.edu.85 Atospherc Radaton Fall 8 For nforaton about ctng these aterals or our Ters of Use, vst: http://ocw.t.edu/ters. .85, Atospherc Radaton Dr. Robert A. McClatchey and

More information

Lecture 8: Small signal parameters and hybrid-π model Lecture 9, High Speed Devices 2016

Lecture 8: Small signal parameters and hybrid-π model Lecture 9, High Speed Devices 2016 Lecture 8: Small sgnal parameters and hbrdπ model π 08006 Lecture 9, Hgh Speed Deces 06 Lecture 8: Small sgnal parameters and hbrdπ model Lterature: Twoport networks Transstors for hgh frequences How to

More information

Chapter 13. Gas Mixtures. Study Guide in PowerPoint. Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and Michael A.

Chapter 13. Gas Mixtures. Study Guide in PowerPoint. Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and Michael A. Chapter 3 Gas Mxtures Study Gude n PowerPont to accopany Therodynacs: An Engneerng Approach, 5th edton by Yunus A. Çengel and Mchael A. Boles The dscussons n ths chapter are restrcted to nonreactve deal-gas

More information

BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS. Dariusz Biskup

BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS. Dariusz Biskup BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS Darusz Bskup 1. Introducton The paper presents a nonparaetrc procedure for estaton of an unknown functon f n the regresson odel y = f x + ε = N. (1) (

More information

Mixed Signal IC Design Notes set 4: Broadband Design Techniques

Mixed Signal IC Design Notes set 4: Broadband Design Techniques Mixed Sal C Des Notes set 4: Broadband Des Techniques Mark odwell University of California, Santa Barbara rodwell@ece.ucsb.edu 805-893-3244, 805-893-3262 fax Gett ore bandwidth At this pot we have learned

More information