Conjugate Gradient (CG) Method
|
|
- Lillian Thompson
- 5 years ago
- Views:
Transcription
1 Optimization II
2 Conugate Gaient CG Metho Anothe metho oes not equie explicit secon eivatives, an oes not even stoe appoximation to Hessian matix CG geneates sequence of conugate seach iections, implicitly accumulating infomation about Hessian matix Fo quaatic obective function, CG is theoetically exact afte at most n iteations, whee n is the imension of poblem Numeical Methos Wen-Chieh Lin 2
3 Conugate Diections x 1 x f x x x 1 Pic a set of iections: 0, 1,, n-1 ae exactly one step along each iection Solution is foun within n steps wo poblems: how o we etemine these iections? how to we etemine the step size along each iections? Numeical Methos Wen-Chieh Lin 3
4 How o we etemine the optimal step size? Suppose we now the CG iections fo now, we want to now the optimal step size in each CG iection? Numeical Methos Wen-Chieh Lin 4
5 Conugacy A-othogonality If we tae the optimal step size along each conugate iection f f x 1 0 x 1 0 x 1 1 wo vectos v an u ae conugate o A- othogonal if va u=0 0 0 Ae 1 x Ae x 1 Numeical Methos Wen-Chieh Lin A x * x 1 1
6 A-othogonality vs. Othogonality A-othogonal vectos othogonal vectos Numeical Methos Wen-Chieh Lin 6
7 Optimal Step Size 0 Ae 1 e 1 must be A - othogonal to Use this conition, can you eive α? Numeical Methos Wen-Chieh Lin 7
8 Algoithm Suppose we can come up with a set of A- othogonal iections { } 1. ae x x A 1 Numeical Methos Wen-Chieh Lin 8
9 Why oes it wo? We nee to pove that x* can be foun in n steps if we tae α step size along at each step n 1 e0 i i i0 n 1 Ae0 i0 i s ae linealy inepenent if s ae conugate A i Ae A 0 See poof in next slie Ae 0 A e A A ecall Ae A Ae Numeical Methos Wen-Chieh Lin 9
10 Poof that x x e x 1 1 x * x x * e 1 e e e e 1 e e e e 0 e 1 1 e Numeical Methos Wen-Chieh Lin 10
11 A-othogonality cont. 0 Ae 1 e e Numeical Methos Wen-Chieh Lin 11
12 Eo tem vanishes afte n steps e e n1 0 Afte n steps, e n = 0 1 n 1 0 he eo at step is equal to 1 e 0 + total path of pevious -1 steps tavele 2 total path of next n- steps that ae going to be tavele Numeical Methos Wen-Chieh Lin 12
13 Seach Diections We now how to etemine the optimal step size along each iection We still nee to figue out what seach iections ae What o we now about 0, 1,, n-1? hey ae A-othogonal to each othe: i A = 0 i is A-othogonal to e i+1 Numeical Methos Wen-Chieh Lin 13
14 Gam-Schmit Conugation Suppose we have a set of linealy inepenent vectos u 0, u 1,, u n-1 o constuct i, tae u i an subtact out any components that ae not A-othogonal to the pevious vectos: 1 = u 1 - u + Numeical Methos Wen-Chieh Lin 14
15 Gam-Schmit Conugation he seach iections can be epesente as 1 u i i an 0 u 0 i0 Use the same tic to get i of the summation A u A A 0 u A A u A A by A-othogonality of vectos Numeical Methos Wen-Chieh Lin 15
16 Dawbacs of Gam-Schmit Conugation All the ol seach vectos must be ept in memoy to constuct each new one! 1 u i i an 0 u 0 i0 Remey conugate gaients Numeical Methos Wen-Chieh Lin 16
17 Conugate Gaients If we pic a set of u s intelligently, we might be able to save both time an space It tuns out that esiuals s is an excellent choice fo u s esiual is othogonal to the pevious seach iection esiuals wo fo steepest escent Numeical Methos Wen-Chieh Lin 17
18 Conugate Gaients cont. Gam-Schmit Conugation 1 u i i an 0 u 0 i0 In conugate gaient metho, seach iections ae constucte by conugation of the esiuals setting u Numeical Methos Wen-Chieh Lin 18
19 Numeical Methos Wen-Chieh Lin 19 Conugate Gaients cont. ae an subtact out any components that ae not A-othogonal to the pevious vectos 1 0 i i i i i i 1 0 A A A 0 A A by A-othogonality of vectos A A
20 Conugate Gaients cont. is A-othogonal to all the pevious seach iections except fo -1 1 A A 1 0, if if 1 1 We on t nee to stoe pevious seach iections now! Poof: A 0 when 1 Numeical Methos Wen-Chieh Lin 20
21 Numeical Methos Wen-Chieh Lin 21 Poof: Othogonality Poof: is othogonal to all the pevious seach iections 0, 1,, -1 Fom hee, we can pove 1 n i i i e 1 if 0 n i i i A Ae if 0 i i if 0 see page of Shewchu s pape
22 Geometic Intepetation 0 if 0 Ae 1 u 1 i0 i i Numeical Methos Wen-Chieh Lin 22
23 Numeical Methos Wen-Chieh Lin 23 othewise A Poof: A-Othogonality is A-othogonal to all the pevious seach iections except fo Ae e A A 1 A
24 Numeical Methos Wen-Chieh Lin 24 Conugate Gaients Recall in slie 19, , A A A A A fom last slie A Ae Fom slie 9:
25 Numeical Methos Wen-Chieh Lin 25 Conugate Gaients Put it all togethe Ax b A 1 A x x
26 Each new esiual is othogonal to all the pevious esiual an seach iections Each new seach iection is constucte fom the esiual to be A-othogonal to all pevious esiuals an seach iections Numeical Methos Wen-Chieh Lin 26
27 Example: Minimize fx,y=1.5*x^2+2*x*y+3*y^2-2*x+8*y 3 2 A b 8 ugategaient/ Numeical Methos Wen-Chieh Lin 27
Conjugate Gradient Methods. Michael Bader. Summer term 2012
Gadient Methods Outlines Pat I: Quadatic Foms and Steepest Descent Pat II: Gadients Pat III: Summe tem 2012 Pat I: Quadatic Foms and Steepest Descent Outlines Pat I: Quadatic Foms and Steepest Descent
More informationScientific Computing II
Scientific Computing II Conjugate Gadient Methods Michael Bade Summe 2014 Conjugate Gadient Methods, Summe 2014 1 Families of Iteative Solves elaxation methods: Jacobi-, Gauss-Seidel-Relaxation,... Ove-Relaxation-Methods
More informationSolutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook
Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)
More information15.081J/6.251J Introduction to Mathematical Programming. Lecture 6: The Simplex Method II
15081J/6251J Intoduction to Mathematical Pogamming ectue 6: The Simplex Method II 1 Outline Revised Simplex method Slide 1 The full tableau implementation Anticycling 2 Revised Simplex Initial data: A,
More informationMethod for Approximating Irrational Numbers
Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations
More informationA Two-Dimensional Bisection Envelope Algorithm for Fixed Points
A Two-imensional Bisection Envelope Algoithm fo Fied Points Kis Siosi and Spence Shellman Fom pulished Jounal of Compleity 8, 64-659(00 Intoduction How we solve fo two-dimensional f ( domain: [0, ]X[0,
More information18.06 Problem Set 4 Solution
8.6 Poblem Set 4 Solution Total: points Section 3.5. Poblem 2: (Recommended) Find the lagest possible numbe of independent vectos among ) ) ) v = v 4 = v 5 = v 6 = v 2 = v 3 =. Solution (4 points): Since
More informationTemporal-Difference Learning
.997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation
More informationEquilibria of a cylindrical plasma
// Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the
More informationMAC Module 12 Eigenvalues and Eigenvectors
MAC 23 Module 2 Eigenvalues and Eigenvectos Leaning Objectives Upon completing this module, you should be able to:. Solve the eigenvalue poblem by finding the eigenvalues and the coesponding eigenvectos
More information10/04/18. P [P(x)] 1 negl(n).
Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationGreen s Identities and Green s Functions
LECTURE 7 Geen s Identities and Geen s Functions Let us ecall The ivegence Theoem in n-dimensions Theoem 7 Let F : R n R n be a vecto field ove R n that is of class C on some closed, connected, simply
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More informationPHYS 705: Classical Mechanics. Small Oscillations
PHYS 705: Classical Mechanics Small Oscillations Fomulation of the Poblem Assumptions: V q - A consevative system with depending on position only - The tansfomation equation defining does not dep on time
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationLocalization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix
Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani
More informationGeneral Relativity Homework 5
Geneal Relativity Homewok 5. In the pesence of a cosmological constant, Einstein s Equation is (a) Calculate the gavitational potential point souce with = M 3 (). R µ Rg µ + g µ =GT µ. in the Newtonian
More information15. SIMPLE MHD EQUILIBRIA
15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium
More informationEquilibrium Reconstruction with Grad-Shafranov Equation
Equilibium Reconstuction with Gad-Shafanov Equation Qian Peng (qp215) Apil 14, 211 1 Gad-Shafanov equation [1]Fo axial symmetic case, the tooidal B eld is B to = F φ. Whee 2π F (, θ) is the total poloidal
More informationPHYS Summer Professor Caillault Homework Solutions
PHYS 1111 - Summe 2007 - Pofesso Caillault Homewok Solutions Chapte 3 13. Pictue the Poblem: The whale dives along a staight line tilted 20.0 below hoizontal fo 150 m as shown in the figue. Stategy: Resolve
More informationPart V: Closed-form solutions to Loop Closure Equations
Pat V: Closed-fom solutions to Loop Closue Equations This section will eview the closed-fom solutions techniques fo loop closue equations. The following thee cases will be consideed. ) Two unknown angles
More informationAuchmuty High School Mathematics Department Advanced Higher Notes Teacher Version
The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!
More information6.4 Period and Frequency for Uniform Circular Motion
6.4 Peiod and Fequency fo Unifom Cicula Motion If the object is constained to move in a cicle and the total tangential foce acting on the total object is zeo, F θ = 0, then (Newton s Second Law), the tangential
More informationPH126 Exam I Solutions
PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium
More informationSemi-Lagrangian simulations of the diocotron instability
Semi-Lagangian simulations of the diocoton instability Eic Madaule, Seve Adian Histoaga, Michel Mehenbege, Jéôme Péti To cite this vesion: Eic Madaule, Seve Adian Histoaga, Michel Mehenbege, Jéôme Péti.
More informationConservative Averaging Method and its Application for One Heat Conduction Problem
Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem
More informationCOLLAPSING WALLS THEOREM
COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned
More informationTopic 4a Introduction to Root Finding & Bracketing Methods
/8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline
More informationCartesian Coordinate System and Vectors
Catesian Coodinate System and Vectos Coodinate System Coodinate system: used to descibe the position of a point in space and consists of 1. An oigin as the efeence point 2. A set of coodinate axes with
More informationInternet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks
Intenet Appendix fo A Bayesian Appoach to Real Options: The Case of Distinguishing Between Tempoay and Pemanent Shocks Steven R. Genadie Gaduate School of Business, Stanfod Univesity Andey Malenko Gaduate
More informationEM Boundary Value Problems
EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do
More informationQualifying Examination Electricity and Magnetism Solutions January 12, 2006
1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and
More informationAnalytical time-optimal trajectories for an omni-directional vehicle
Analytical time-optimal tajectoies fo an omni-diectional vehicle Weifu Wang and Devin J. Balkcom Abstact We pesent the fist analytical solution method fo finding a time-optimal tajectoy between any given
More information6 Matrix Concentration Bounds
6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom
More informationNew problems in universal algebraic geometry illustrated by boolean equations
New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic
More informationQIP Course 10: Quantum Factorization Algorithm (Part 3)
QIP Couse 10: Quantum Factoization Algoithm (Pat 3 Ryutaoh Matsumoto Nagoya Univesity, Japan Send you comments to yutaoh.matsumoto@nagoya-u.jp Septembe 2018 @ Tokyo Tech. Matsumoto (Nagoya U. QIP Couse
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More informationMULTILAYER PERCEPTRONS
Last updated: Nov 26, 2012 MULTILAYER PERCEPTRONS Outline 2 Combining Linea Classifies Leaning Paametes Outline 3 Combining Linea Classifies Leaning Paametes Implementing Logical Relations 4 AND and OR
More informationHua Xu 3 and Hiroaki Mukaidani 33. The University of Tsukuba, Otsuka. Hiroshima City University, 3-4-1, Ozuka-Higashi
he inea Quadatic Dynamic Game fo Discete-ime Descipto Systems Hua Xu 3 and Hioai Muaidani 33 3 Gaduate School of Systems Management he Univesity of suuba, 3-9- Otsua Bunyo-u, oyo -0, Japan xuhua@gssm.otsua.tsuuba.ac.jp
More informationDuality between Statical and Kinematical Engineering Systems
Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.
More informationSCHAUDER ESTIMATES FOR ELLIPTIC AND PARABOLIC EQUATIONS. Xu-Jia Wang The Australian National University
SCHAUDER ESTIMATES FOR ELLIPTIC AND PARABOLIC EQUATIONS Xu-Jia Wang The Austalian National Univesity Intouction The Schaue estimate fo the Laplace equation was taitionally built upon the Newton potential
More informationMoment-free numerical approximation of highly oscillatory integrals with stationary points
Moment-fee numeical appoximation of highly oscillatoy integals with stationay points Sheehan Olve Abstact We pesent a method fo the numeical quadatue of highly oscillatoy integals with stationay points.
More information556: MATHEMATICAL STATISTICS I
556: MATHEMATICAL STATISTICS I CHAPTER 5: STOCHASTIC CONVERGENCE The following efinitions ae state in tems of scala anom vaiables, but exten natually to vecto anom vaiables efine on the same obability
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationHOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS?
6th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE HOW TO TEACH THE FUNDAMENTALS OF INFORMATION SCIENCE, CODING, DECODING AND NUMBER SYSTEMS? Cecília Sitkuné Göömbei College of Nyíegyháza Hungay Abstact: The
More informationarxiv: v1 [math.co] 1 Apr 2011
Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and
More informationInseting this into the left hand side of the equation of motion above gives the most commonly used algoithm in classical molecula dynamics simulations
Chem465 in 2000 Univesity of Washington Lectue notes Hannes Jonsson Classical dynamics When we ae dealing with heavy atoms and high enough enegy o tempeatue, it is often suciently accuate to neglect quantum
More informationPhysics Courseware Physics II Electric Field and Force
Physics Cousewae Physics II lectic iel an oce Coulomb s law, whee k Nm /C test Definition of electic fiel. This is a vecto. test Q lectic fiel fo a point chage. This is a vecto. Poblem.- chage of µc is
More informationDirected Regression. Benjamin Van Roy Stanford University Stanford, CA Abstract
Diected Regession Yi-hao Kao Stanfod Univesity Stanfod, CA 94305 yihaoao@stanfod.edu Benjamin Van Roy Stanfod Univesity Stanfod, CA 94305 bv@stanfod.edu Xiang Yan Stanfod Univesity Stanfod, CA 94305 xyan@stanfod.edu
More informationDouble-angle & power-reduction identities. Elementary Functions. Double-angle & power-reduction identities. Double-angle & power-reduction identities
Double-angle & powe-eduction identities Pat 5, Tigonomety Lectue 5a, Double Angle and Powe Reduction Fomulas In the pevious pesentation we developed fomulas fo cos( β) and sin( β) These fomulas lead natually
More information4.[1pt] Two small spheres with charges -4 C and -9 C are held 9.5 m apart. Find the magnitude of the force between them.
. [pt] A peson scuffing he feet on a wool ug on a y ay accumulates a net chage of - 4.uC. How many ecess electons oes this peson get? Coect, compute gets:.63e+4. [pt] By how much oes he mass incease? Coect,
More informationHomework # 3 Solution Key
PHYSICS 631: Geneal Relativity Homewok # 3 Solution Key 1. You e on you hono not to do this one by hand. I ealize you can use a compute o simply look it up. Please don t. In a flat space, the metic in
More informationAs is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.
Appendix A Vecto Algeba As is natual, ou Aeospace Stuctues will be descibed in a Euclidean thee-dimensional space R 3. A.1 Vectos A vecto is used to epesent quantities that have both magnitude and diection.
More informationGRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1
Einstein Classes, Unit No. 0, 0, Vahman Ring Roa Plaza, Vikas Pui Extn., New Delhi -8 Ph. : 96905, 857, E-mail einsteinclasses00@gmail.com, PG GRAVITATION Einstein Classes, Unit No. 0, 0, Vahman Ring Roa
More informationNotation. 1 Vectors. 2 Spherical Coordinates The Problem
Notation 1 Vectos As aleady noted, we neve wite vectos as pais o tiples of numbes; this notation is eseved fo coodinates, a quite diffeent concept. The symbols we use fo vectos have aows on them (to match
More informationPROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.
POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and
More informationA STUDY OF HAMMING CODES AS ERROR CORRECTING CODES
AGU Intenational Jounal of Science and Technology A STUDY OF HAMMING CODES AS ERROR CORRECTING CODES Ritu Ahuja Depatment of Mathematics Khalsa College fo Women, Civil Lines, Ludhiana-141001, Punjab, (India)
More informationThe Laws of Motion ( ) N SOLUTIONS TO PROBLEMS ! F = ( 6.00) 2 + ( 15.0) 2 N = 16.2 N. Section 4.4. Newton s Second Law The Particle Under a Net Force
SOLUTIONS TO PROBLEMS The Laws of Motion Section 4.3 Mass P4. Since the ca is moving with constant speed and in a staight line, the esultant foce on it must be zeo egadless of whethe it is moving (a) towad
More informationElectric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions
Poblem 1: Electic Potential an Gauss s Law, Configuation Enegy Challenge Poblem Solutions Consie a vey long o, aius an chage to a unifom linea chage ensity λ a) Calculate the electic fiel eveywhee outsie
More informationKinematics in 2-D (II)
Kinematics in 2-D (II) Unifom cicula motion Tangential and adial components of Relative velocity and acceleation a Seway and Jewett 4.4 to 4.6 Pactice Poblems: Chapte 4, Objective Questions 5, 11 Chapte
More informationL p Theory for the Multidimensional Aggregation Equation
L p Theoy fo the Multiimensional Aggegation Equation Anea L. Betozzi, Thomas Lauent* & Jesus Rosao Novembe 19, 29 Abstact We consie well-poseness of the aggegation equation tu + iv(uv) =, v = K u with
More informationPsychometric Methods: Theory into Practice Larry R. Price
ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include
More informationInformation Retrieval (Relevance Feedback & Query Expansion)
Infomation Retieval (Relevance Feedback & Quey Epansion) Fabio Aiolli http://www.math.unipd.it/~aiolli Dipatimento di Matematica Univesità di Padova Anno Accademico 1 Relevance feedback and quey epansion
More informationGradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function
Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong
More informationDynamic Visualization of Complex Integrals with Cabri II Plus
Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape
More informationPushdown Automata (PDAs)
CHAPTER 2 Context-Fee Languages Contents Context-Fee Gammas definitions, examples, designing, ambiguity, Chomsky nomal fom Pushdown Automata definitions, examples, euivalence with context-fee gammas Non-Context-Fee
More informationEasy. P4.2 Since the car is moving with constant speed and in a straight line, the. resultant force on it must be regardless of whether it is moving
Chapte 4 Homewok Solutions Easy P4. Since the ca is moving with constant speed and in a staight line, the zeo esultant foce on it must be egadless of whethe it is moving (a) towad the ight o the left.
More informationThe Strain Compatibility Equations in Polar Coordinates RAWB, Last Update 27/12/07
The Stain Compatibility Equations in Pola Coodinates RAWB Last Update 7//7 In D thee is just one compatibility equation. In D polas it is (Equ.) whee denotes the enineein shea (twice the tensoial shea)
More informationEN40: Dynamics and Vibrations. Midterm Examination Thursday March
EN40: Dynamics and Vibations Midtem Examination Thusday Mach 9 2017 School of Engineeing Bown Univesity NAME: Geneal Instuctions No collaboation of any kind is pemitted on this examination. You may bing
More information1D2G - Numerical solution of the neutron diffusion equation
DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both
More informationSyntactical content of nite approximations of partial algebras 1 Wiktor Bartol Inst. Matematyki, Uniw. Warszawski, Warszawa (Poland)
Syntactical content of nite appoximations of patial algebas 1 Wikto Batol Inst. Matematyki, Uniw. Waszawski, 02-097 Waszawa (Poland) batol@mimuw.edu.pl Xavie Caicedo Dep. Matematicas, Univ. de los Andes,
More informationOn the Quasi-inverse of a Non-square Matrix: An Infinite Solution
Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J
More information5.61 Physical Chemistry Lecture #23 page 1 MANY ELECTRON ATOMS
5.6 Physical Chemisty Lectue #3 page MAY ELECTRO ATOMS At this point, we see that quantum mechanics allows us to undestand the helium atom, at least qualitatively. What about atoms with moe than two electons,
More informationCHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations
1 CHAPTER DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE 1 Deivation of Machine Equations A moel of a phase PM machine is shown in Figue 1 Both the abc an the q axes ae shown
More informationworking pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50
woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,
More informationApplication 4.3B Comets and Spacecraft
Application 4.3B Comets and Spacecaft The investigations outlined hee ae intended as applications of the moe sophisticated numeical DE solves that ae "built into" computing systems such as Maple, Mathematica,
More informationQuantum Fourier Transform
Chapte 5 Quantum Fouie Tansfom Many poblems in physics and mathematics ae solved by tansfoming a poblem into some othe poblem with a known solution. Some notable examples ae Laplace tansfom, Legende tansfom,
More informationAQI: Advanced Quantum Information Lecture 2 (Module 4): Order finding and factoring algorithms February 20, 2013
AQI: Advanced Quantum Infomation Lectue 2 (Module 4): Ode finding and factoing algoithms Febuay 20, 203 Lectue: D. Mak Tame (email: m.tame@impeial.ac.uk) Intoduction In the last lectue we looked at the
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More informationSecret Exponent Attacks on RSA-type Schemes with Moduli N = p r q
Secet Exponent Attacks on RSA-type Schemes with Moduli N = p q Alexande May Faculty of Compute Science, Electical Engineeing and Mathematics Univesity of Padebon 33102 Padebon, Gemany alexx@uni-padebon.de
More informationCOMP Parallel Computing SMM (3) OpenMP Case Study: The Barnes-Hut N-body Algorithm
COMP 633 - Paallel Computing Lectue 8 Septembe 14, 2017 SMM (3) OpenMP Case Study: The Banes-Hut N-body Algoithm Topics Case study: the Banes-Hut algoithm Study an impotant algoithm in scientific computing»
More informationThe Substring Search Problem
The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is
More informationPhys 201A. Homework 5 Solutions
Phys 201A Homewok 5 Solutions 3. In each of the thee cases, you can find the changes in the velocity vectos by adding the second vecto to the additive invese of the fist and dawing the esultant, and by
More informationEE 5337 Computational Electromagnetics
Instucto D. Ramond Rumpf (95) 747 6958 cumpf@utep.edu EE 5337 Computational Electomagnetics Lectue # WEM Etas Lectue These notes ma contain copighted mateial obtained unde fai use ules. Distibution of
More informationUniversity Physics (PHY 2326)
Chapte Univesity Physics (PHY 6) Lectue lectostatics lectic field (cont.) Conductos in electostatic euilibium The oscilloscope lectic flux and Gauss s law /6/5 Discuss a techniue intoduced by Kal F. Gauss
More informationComputing Approximate GCD of Multivariate Polynomials by Structure Total Least Norm 1)
MM Reseach Pepints, 388 41 MMRC, AMSS, Academia Sinica No 23, Decembe 24 Computing Appoximate GCD of Multivaiate Polynomials by Stuctue Total Least Nom 1) Lihong Zhi and Zhengfeng Yang Key Laboatoy of
More informationMCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.
MCVU Final Eam Review Answe (o Solution) Pactice Questions Conside the function f () defined b the following gaph Find a) f ( ) c) f ( ) f ( ) d) f ( ) Evaluate the following its a) ( ) c) sin d) π / π
More informationON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},
ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability
More information(read nabla or del) is defined by, k. (9.7.1*)
9.7 Gadient of a scala field. Diectional deivative Some of the vecto fields in applications can be obtained fom scala fields. This is vey advantageous because scala fields can be handled moe easily. The
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
More informationThat is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.
PHY 8 Test Pactice Solutions Sping Q: [] A poton an an electon attact each othe electically so, when elease fom est, they will acceleate towa each othe. Which paticle will have a lage acceleation? (Neglect
More informationUnobserved Correlation in Ascending Auctions: Example And Extensions
Unobseved Coelation in Ascending Auctions: Example And Extensions Daniel Quint Univesity of Wisconsin Novembe 2009 Intoduction In pivate-value ascending auctions, the winning bidde s willingness to pay
More informationThe energy spaces of the tangent point energies
The enegy spaces of the tangent point enegies Simon Blatt August 3, 2 In this small note, we will give a necessay and sucient condition unde which the tangent point enegies intoduced by Heiko von de Mosel
More informationThe geometric construction of Ewald sphere and Bragg condition:
The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in
More informationUsing Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu
Available at https://edupediapublicationsog/jounals Volume 3 Issue 4 Febuay 216 Using Laplace Tansfom to Evaluate Impope Integals Chii-Huei Yu Depatment of Infomation Technology, Nan Jeon Univesity of
More informationMarkscheme May 2017 Calculus Higher level Paper 3
M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted
More informationMAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates,
MAE B Homewok Solution #6 Winte Quate, 7 Poblem a Expecting a elocity change of oe oe a aial istance, the conition necessay fo the ow to be ominate by iscous foces oe inetial foces is O( y ) O( ) = =
More informationPROBLEM (page 126, 12 th edition)
PROBLEM 13-27 (page 126, 12 th edition) The mass of block A is 100 kg. The mass of block B is 60 kg. The coefficient of kinetic fiction between block B and the inclined plane is 0.4. A and B ae eleased
More informationMATHEMATICAL TOOLS. Contents. Theory Exercise Exercise Advance Level Problems Answer Key
MATHEMATICAL TOOLS Contents Topic Page No. Theoy - 6 Eecise - 7 - Eecise - - 7 Avance Level Poblems 8 - Answe Key - 9 Syllabus Diffeentiation, Integation & Vecto Name : Contact No. ARRIDE LEARNING ONLINE
More information