Transistor configurations: There are three main ways to place a FET/BJT in an architecture:

Similar documents
INF 5460 Electronic noise Estimates and countermeasures. Lecture 13 (Mot 10) Amplifier Architectures

Supplementary Information

ECSE Partial fraction expansion (m<n) 3 types of poles Simple Real poles Real Equal poles

1 Notes on Little s Law (l = λw)

Comparing Different Estimators for Parameters of Kumaraswamy Distribution

Capítulo. of Particles: Energy and Momentum Methods

Applications of force vibration. Rotating unbalance Base excitation Vibration measurement devices

Extremal graph theory II: K t and K t,t

Auchmuty High School Mathematics Department Sequences & Series Notes Teacher Version

Big O Notation for Time Complexity of Algorithms

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Section 8 Convolution and Deconvolution

Spectrum of The Direct Sum of Operators. 1. Introduction

An Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants

ECE-314 Fall 2012 Review Questions

The Eigen Function of Linear Systems

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

Lecture 17: Kinetics of Phase Growth in a Two-component System:

S n. = n. Sum of first n terms of an A. P is

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of

PI3B V, 16-Bit to 32-Bit FET Mux/DeMux NanoSwitch. Features. Description. Pin Configuration. Block Diagram.

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

Exercise 3 Stochastic Models of Manufacturing Systems 4T400, 6 May

Progression. CATsyllabus.com. CATsyllabus.com. Sequence & Series. Arithmetic Progression (A.P.) n th term of an A.P.

Electrical Engineering Department Network Lab.

ECE 350 Matlab-Based Project #3

ECE 145B / 218B, notes set 5: Two-port Noise Parameters

Non-sinusoidal Signal Generators

The Non-Truncated Bulk Arrival Queue M x /M/1 with Reneging, Balking, State-Dependent and an Additional Server for Longer Queues

MATH Midterm Solutions

SHOCK AND VIBRATION RESPONSE SPECTRA COURSE Unit 21 Base Excitation Shock: Classical Pulse

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

Solution. 1 Solutions of Homework 6. Sangchul Lee. April 28, Problem 1.1 [Dur10, Exercise ]

B. Maddah INDE 504 Simulation 09/02/17

BEST LINEAR FORECASTS VS. BEST POSSIBLE FORECASTS

ABSOLUTE INDEXED SUMMABILITY FACTOR OF AN INFINITE SERIES USING QUASI-F-POWER INCREASING SEQUENCES

COST OPTIMIZATION OF SLAB MILLING OPERATION USING GENETIC ALGORITHMS

The Central Limit Theorems for Sums of Powers of Function of Independent Random Variables

Fresnel Dragging Explained

FBD of SDOF Base Excitation. 2.4 Base Excitation. Particular Solution (sine term) SDOF Base Excitation (cont) F=-(-)-(-)= 2ζω ωf

Mathematical Statistics. 1 Introduction to the materials to be covered in this course

On The Estimation of Two Missing Values in Randomized Complete Block Designs

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

Calculus Limits. Limit of a function.. 1. One-Sided Limits...1. Infinite limits 2. Vertical Asymptotes...3. Calculating Limits Using the Limit Laws.

F D D D D F. smoothed value of the data including Y t the most recent data.

ES 330 Electronics II Homework 03 (Fall 2017 Due Wednesday, September 20, 2017)

= 5! 3! 2! = 5! 3! (5 3)!. In general, the number of different groups of r items out of n items (when the order is ignored) is given by n!

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

Sampling. AD Conversion (Additional Material) Sampling: Band limited signal. Sampling. Sampling function (sampling comb) III(x) Shah.

S, we call the base curve and the director curve. The straight lines

Relations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems

4. Fundamental of A.C. Circuit

GENERALIZED FRACTIONAL INTEGRAL OPERATORS AND THEIR MODIFIED VERSIONS

4. Biasing Transistor Circuits

An interesting result about subset sums. Nitu Kitchloo. Lior Pachter. November 27, Abstract

On imploding cylindrical and spherical shock waves in a perfect gas

Math 2414 Homework Set 7 Solutions 10 Points

The Nehari Manifold for a Class of Elliptic Equations of P-laplacian Type. S. Khademloo and H. Mohammadnia. afrouzi

Notes 03 largely plagiarized by %khc

6.003: Signals and Systems Lecture 20 April 22, 2010

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

PI3B

Computer Propagation Analysis Tools

CS623: Introduction to Computing with Neural Nets (lecture-10) Pushpak Bhattacharyya Computer Science and Engineering Department IIT Bombay

Angle Modulation: NB (Sinusoid)

Reinforcement learning

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

6.2 Improving Our 3-D Graphics Pipeline

Sampling Example. ( ) δ ( f 1) (1/2)cos(12πt), T 0 = 1

Algebra 2A. Algebra 2A- Unit 5

(a) Unde zeo-bias conditions, thee ae no lled states on one side of the junction which ae at the same enegy as the empty allowed states on the othe si

CSE 202: Design and Analysis of Algorithms Lecture 16

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming*

COS 522: Complexity Theory : Boaz Barak Handout 10: Parallel Repetition Lemma

Available online at J. Math. Comput. Sci. 2 (2012), No. 4, ISSN:

The sudden release of a large amount of energy E into a background fluid of density

King Fahd University of Petroleum & Minerals Computer Engineering g Dept

Cameras and World Geometry

Review - Week 10. There are two types of errors one can make when performing significance tests:

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

ECE594I Notes set 13: Two-port Noise Parameters

The Production of Polarization

C(p, ) 13 N. Nuclear reactions generate energy create new isotopes and elements. Notation for stellar rates: p 12

Orthotropic Materials

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

Low-complexity Algorithms for MIMO Multiplexing Systems

Fourier transform. Continuous-time Fourier transform (CTFT) ω ω

Fujii, Takao; Hayashi, Fumiaki; Iri Author(s) Oguro, Kazumasa.

Determining solar characteristics using planetary data

Effect of Heat Exchangers Connection on Effectiveness

Linear Time Invariant Systems

Generalized Fibonacci-Type Sequence and its Properties

Communication Systems Lecture 25. Dong In Kim School of Info/Comm Engineering Sungkyunkwan University

The analysis of the method on the one variable function s limit Ke Wu

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Solutions Manual 4.1. nonlinear. 4.2 The Fourier Series is: and the fundamental frequency is ω 2π

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

Supplementary materials. Suzuki reaction: mechanistic multiplicity versus exclusive homogeneous or exclusive heterogeneous catalysis

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch

Transcription:

F3 Mo 0. Amplifie Achiecues Whe a asiso is used i a amplifie, oscillao, file, seso, ec. i will also be a eed fo passive elemes like esisos, capacios ad coils o povide biasig so ha he asiso has he coec wokig poi. These passive elemes will ifluece o he oise. he followig we will look a some achiecues ad how hey affec he equivale ipu oise. Tasiso cofiguaios: Thee ae hee mai ways o place a FT/BJT i a achiecue: BJT FT : ommo mie : ommo ouce B: ommo Base G: ommo Gae : ommo olleco D: ommo Dai / has he lages powe amplificaio. /D is used o achieve high ipu impedace ad low oupu impedace. G/B is used by achieve low ipu impedace ad high oupu impedace.

Whe he i is calculaed fo he gae/bias i is almos equal fo all cofiguaios. Hece he i, ad calculaed fo / ca also be used i /D ad B/G cofiguaios. This assumes ha he fequecy is so low ha he ieal colleco-base feedback capaciace ca be igoed. NB! Alhough he ipu oise is he same his does o apply o he oupu oise.

0- ommo-mie The figue shows a asiso ha is biased fo low oise opeaio bewee 0Hz ad 0kHz. The oise values ae as follows: 0Hz 0kHz V V pa 0.3pA 0 000 6700 NF@0.8dB 0.3dB mall sigal equivale schemaic fo he cicui is show o he ex page.

The schemaic shows a hybid- model ogehe wih passive bias elemes. The volage gai : Z i L Z Z i Z i D D is he volage gai fom Vs o Vo. The fis paehesis is he volage gai wihi he asiso ( is /B) while he secod paehesis is he ewok i fo of he base.

i x Z Z The ipu esisace Zi cosiss also of he esisace you ca see hough he base o emie. (+=/B). L 0 i The load esisace cosiss of boh he colleco bias esisace, he asiso ieal esisace ad he ipu esisace of he ex sage: i. Z jx. The emie impedace cosiss of a eal pa ad a imagiay pa (a esisace ad a capaciace i paallel). Z jx The souce impedace is a esisace i seies wih a capacio. f we assume igoable loss i biasig, couplig ad feedback we ca simplify he expessio fo o: L Z Z x

f Zs << ad Z << e he expessio is simplified o: L m e L g We simplify ad igoe he exeal load ad simplifies L so ha: L fo ' We will he have he followig expessio fo he equivale ipu oise: ' D D D s i jx he expessio, we ecogise he fis lie (say fom secio. 7.3). Las em is also kow. The secod las em, howeve, eed some commes. The volage ove will o be fo highe fequecies, because will "aemp o sho-cicui" his. We choose o model he hemal oise i as a cue oise of size =/. The oise cue ove ad will be:

' j Back o he expessio fo i: ' D D D s i jx Fom he expessio we fid ha o have low oise: D should be lage elaive o. should be gea. s should be small. should be small (less ha ). should be high. should be lage. should be lage. f he A-couplig is o eeded is emove D ad. has he geaes powe amplificaio ad oise fom sages followig he amplifie ca pobably be igoed. The ipu esisace vaies wih.

hoice of capaciace value. has a high pass effec wih 3dB limi equal o he sum of he souce esisace ad esisace o he amplifie (icludig bias). Wih egad o oise /() should be much less ha a he lowes eleva fequecy. This is because hese ae added ad deemies he coibuio of : (+j/()). Obviously he las em should be ied made small (</00) elaive o. NB! Hece due o oise mus o be used ieioally fo file fucios! should sho-cicui emie A-wise o goud. The impedace of should be small i elaio o he ieal esisace i he emie: e. Basically oise i has he same weigh as he oise i he souce. Howeve, will educe he coibuio fom. he expessio below is he oise coibuio fom i he umeao.

ommo-emie wih oe volage supply. Hee a poi A is esablished supplyig a sable D poeial fo he base ad ha A-wise is sho cicuied o goud hough B.

The oise schemaic is as follows: quivale ipu oise ca be expessed as: ' D D B B B B A A D D s i jx addiio o he kow ems, we have ow a ew em i squae paehesis due o he base bias ewok. The paehesis is weighed wih he /D aio. The D-volage a he base is deemied by he elaioship bewee A ad B as follows: B A B A V V

The coibuig oise fom he esisos A ad B should be elaively small. A good saig poi is o chose B so lage ha he oise i he eleva fequecy age saisfies he iequaliy: A xa B xb D A B B B Noise i he amplifie is give i he followig able: 0Hz 0kHz 4.5V 4.5V 0.3pA 0.pA 0 0k 45 NF@0 0.68dB 0.35dB 80 i 780

Noise i cascaded sages We have peviously sudied he oise figue fo cascaded amplifies. We will ow look a he equivale ipu oise: The expessio fo equivale ipu oise ca be expessed as follows... i o 3 3 s o Hee o is he oupu esisace of sage. imilaly fo o, o3 ec. i is as ealie he volage gai. As peviously if he gai is lage eough i he fis sage oise fom subseque sages ca be igoed.

Thee ae hee mehods oe ca use fo oise aalysis of moe complex sysems such as cascaded ewok: Maual ewok aalysis (had calculaios), use a simulao as say LTspice, o measue he sysem afe ealisaio. Ticks fo simulaio (ad measueme): f oe is usue of he impac of oise fom a souce: simulae oly wih his souce ad measue esuls o he ed.

ombied achiecues: ommo-ouce --- ommo-mie couple povides high ipu impedace ad high volage gai. he example is a JFT bu he cosideaios applies o MOFTs also.

The oise figues fo his cicui ae as follows: 0Hz 0kHz 8V 4V 7fA 7fA 0.M 570k NF@0 0.03dB 0.05dB The volage amplificaio fo he -sage is: g ml gm Z L ad Z is give by: L D d i ad L D d i The oal volage gai is: g ml c g mz x Whe >> D ad >> o we have ha: g md c e

To educe he -oise coibuio fom he FT we icease D. Bu his assumes a smalle D which meas less oal gai. The expessio fo he equivale ipu oise fo his cicui is: c D D G G G G s i jx G mus be lage compaed o G mus be lage compaed o mus be sufficiely lage should be lage ad c should be gea.

ommo-colleco --- ommo-emie couple - has oly a lile lage ha a pue sage bu ca offe highe ipu esisace ad lowe ipu capaciace. Fis sage has a gai of appox.. The oal gai is: x L x L c Z whee x L Z The expessio fo c ca be simplified whe L>>(+x+) ad >>x+z: e c

quivale ipu oise is: ' ' c s i is he gai i he fis sage wih as load. ' e x ad D should he emie esisace be lage.

ommo-mie --- ommo base couple -B has low ipu capaciace ad high oupu impedace. Due o he low ipu esisace of he secod sage he volage gai of he fis sage will be low. This educes he high fequecy feedback (Mille effec) hough as discussed befoe. The ipu capaciace is hus much less ha fo a egula sep. Q povides powe amplificaio bu o volage gai (ie Q povides a cue gai.) Q povides a lage volage gai. is used o povide exa colleco cue o Q whe hee is a eed fo lage gai-badwidh.

The oal powe gai ca be expessed as: B x x L B x x L c Z Z Z Z whee e B x L Z Whe =0 ad >>/ we ca simplify c o: e c The equivale ipu oise is: c B B B A B A B L s i Z

egaed BJT cascade amplifie Hee Q acs as a -sage ad Q as a B-sage. Q3 is load. The oal volage gai is: 3 e o c The equivale ipu oise is: 3 c o B e s i Z Hee is =e/e. ice he colleco cues ae equal so will =. ZB is he impedace o VBB (should be low). ice e also is small he coibuio fom should also be igoable.

The oise volage fom Q3 is: 3 3 3 o The gai i Q3 is: c e o 3 3 Wih hese simplificaios he expessio fo he equivale ipu oise is educed o: 3 3 3 s s i

Diffeeial amplifie The wo ipu sigals V ad V ca be defied elaive o a commo value (commo-mode) V, ad a diffeece value VD. V V V, ad V D V V We will he have: V V D V, ad V V D V The oise schemaic looks as follows: The equivale ipu oise is: i s s

Diffeeial coecio: We assume ha he posiive ad egaive ipu has he same oise chaaceisics ad adds ogehe he ad -values fo he amplifie. T T Whe we pu ogehe wih he souce esisace, we obai he equivale ipu oise: s i

Noise model fo he diffeeial amplifie. xample of diffeeial sage: a) Volage gai of diffeeial sigal: dm V V o s V V o s g m Hee is gm=/e fo each of he asisos. Assumig ideical asisos ad ==, == ad ==. Fo he ypical cases whee =0 ad << we ca simplify dm o: dm e

b) Gai fo he commo volage sigal: m s s o o cm g V V V V Whe is lage we ge: cm c) Diffeeial volage gai bewee oupus wih commo ipu sigal: m m m m o o dc g g g g V V V deally if he ipus wee compleely symmeical dc should be 0. Whe his is o he case oe ca educe dc say by iceasig.

i: dc V V dm i Hee is V ad V oise o he volage supplies.

egaed BJT diffeeial amplifie ca be elaively lage vaiaio i pocess paamees fo iegaed cicuis fom poducio o poducio. Howeve bewee he elemes o he same cicui he vaiaio will be lile. This is exploied by basig desigs moe o he symmey bewee he elemes ha o hei acual values. O iegaed cicuis he commo-mode oise ejecio is impoved. O he ohe had, o iegaed cicuis equies compomises ha may give moe oise ha whe opimizig a pocess fo a sigle isolaed compoe. xamples of hese compomises ae: log isulaio diffuse sessios, acive loads, ad powe souces.

The figue shows he iegaed vesio of he diffeeial amplifie we sudied peviously. quivale ipu oise: e dc V V s s s s i 5 4 3 ice commo-mode ejecio is high ad all acive cicuis have appoximaely he same geomey ad oise mechaisms, i will be educed o: 4 i

Paallel amplifie sages Wha whe seveal amplifies ae placed i paallel? chemaically, we ca daw oise souces as follows: We have: N ' ad ' N A ew opimal souce esisace ca be defied as: ' o ' ' o N Gai is give by: A' v NA v A sigifica coibuio o he -oise i a BJT is he base esisace x. The base esisace ca be educed by placig he base coacs all he way aoud he emie ad he closes possible o he emie. FTs i is deemied by he chael

esisaces, ad by gm. Low esisace ad high gm ca be achieved by havig a lage W/L aio. By paallelisig boh he ad he Mille effec is iceased.