Garret Sobczyk s 2x2 Matrix Derivation
|
|
- Archibald Phillip Perry
- 5 years ago
- Views:
Transcription
1 Garret Sobczyk s x Matrix Derivation Krt Nalty May, 05 Abstract Using matrices to represent geometric algebras is known, bt not necessarily the best practice. While I have sed small compter programs to scan throgh candidate matrices to find representations, I have not been able to derive sch matrices from first principles. Garret Sobczyk at however, has. I repeat his derivation here, for x matrix representation of the D geometric algebra, inclding more intermediate steps for easier nderstanding. D Eclidean Geometric Algebra Basis Start with a two dimensional, Eclidean geometric algebra. We have two vector directions, and e which correspond to or standard x and y directions. Or geometric mltivector elements are scalars, vectors and e, and a single bivector e =. In this algebra, scalar mltiplication is commtative and associative, vectors sqare to scalar one, and the prodct of two vectors reslting in a bivector is anti-commtative, associative and sqares to negative one. The order sensitive mltiplication table for this algebra is shown below. e e e e e e e e e e e e -
2 Given this notation, the generic D mltivector can be written as g = α + x + ye + β e Sobczyk now introdces a linear combination of two of these basis, where he rotates the scalar and e elements 5 degrees, and applies a small scaling factor. = + e = e Adding these two basis recovers th, sbtracting these two basis recovers e. Each of the basis sqare to themselves, making these combinations idempotents like 0 0 = 0 and =. More fn, the prodct of these two basis is zero, making these combinations mtal annihilators. These two properties of projection and annihilation greatly simplify power series formlas, as fond in exponentiation. + = + e = + e = + e = e = + e + e e + e e e = = e notice below e e = = + e + e e = e + e e = e e = + e + = e + = = 0 = = Having seen how the and basis work among themselves, let s write ot the preprodct and postprodct expressions among the,, and e terms. = + e = + e = + e = + e = e = e = e = = e =
3 Now for e, e = + e e = e + e e e = e + e = e + e e e = e e = e e e e = e e Finally for the bivector e, = e e e = e + = e + = e = e = = = = e = + e e = e + e e e = e + e = e + e e e = e e = e e e e = e e So, a little smmary sheet... = e e e = e = e + = e + = e = = = = = + e / = e / + = = e = = = 0 = 0 = = = = e = e = e = e = e = e = e = e = Sobczyk now presents two matrix expressions sing geometric algebra elements. + + e e + = + e = Sobcyzk calls the right hand matrix the spectral basis for D. The next matrix expression is + = + = + = + = 3
4 Now the fn begins. Start with the tre statement for the generic mltivector g = g. [ ] [ ] g = g = + g + Being an associative algebra, we can refactor or mltiplications, keeping the order intact. g = g = [ + g ] g = g = + g ge g g e We now want to examine the middle three prodct terms. Begin by looking at each term in the center matrix. g = α + x + ye + β e g = α + x + ye + β e = x + α + βe + y e g = α + x + ye + β e = x + α βe y e g = x + α βe y e = α + x ye β e We now postmltiply by, and separate prodct terms to isolate leading and terms. Start with g. g = α + x + ye + β e = α + x + ye + β e = α + x + y + β = α + x + y + β = α + y + x + β Now, premltiply by, project and annihilate. g = α + y + x + β = α + y + x + β = α + y + 0 x + β = α + y
5 In a similar fashion, we process g g = x + α + βe + y e = x + α + βe + y e = x + α + β + y = x + β + α + y = x + β + α + y Now, premltiply by, project and annihilate. g = x + β + α + y = x + β We now rapidly do the remaining terms. g = x + α βe y e = x + α βe y e = x + α β y = x β + α y Now, premltiply by, project and annihilate. Finish with g = x β + α y = x β g = α + x ye β e = α + x ye β e = α + x y β = α + x y β = α y + x β Now, premltiply by, project and annihilate. g = α y + x β = α y 5
6 We ths have the nice reslt that g ge g g = + α + y x β x + β α y Plling ot the common factor, we have g ge α + y g ge + = x + β x β α y This real matrix is the D Eclidean geometric algebra, with respect to the spectral basis. I point ot that being an array of scalars real nmbers, not geometrical objects, this matrix commtes with the geometric nmber. α + y x β α + y x β α + y x β = x + β α y x + β α y + = x + β α y + Sobczyk ses the notation [g] for this real matrix. α + y x β [g] = x + β α y So, a little recap is in order before we proceed. g = g = + [ g ] which becomes g = + [g] Sobczyk now does a preprodct and postprodct on g. g = + [g] g = e We now sandwich mltiply by, and find e [g] 6
7 g + = e e [g] On the right hand side of the eqation, I bring the left into the matrix. g + + = + [g] + + Now I drag the across the terms, creating elements. g + e + = [g] + We now bring the term left of the [g] in the matrix from the right. g + + = + [g] + We project and annihilate. g = 0 e [g] Refactor ot the term g + = 0 0 e [g] And now absorb the nit matrix. g + = [g] e Since the [g] matrix consists of real nmbers, the mltivector and scalar array [g] commte, nlike the mltivector and the mltivector g. So, we move to the right hand side of [g], and repeat the previos steps. g + = [g] e 7
8 Bring the left into the matrix. g + + = [g] + Drag across. g + e + = [g] Bring in the right. g + + = [g] + Project and annihilate. g = [g] 0 Factor and absorb. g + = [g] We have the very pretty reslt 0 0 = [g] = [g] g + = [g] = [g] To get a stand alone formla for [g], Sobczyk develops a formla for [g], then adds the terms [g] + [g] = + [g] = [g] = [g]. To develop the formla for [g], Sobczyk once again does a sandwich prodct with conjgation with respect to. g + = [g] Doing the right hand side first, we drag across. [g] = [g] 8
9 Since [g] is a scalar array, [g] and commte. [g] = [g] = [g] Now, since sqares to one, we have [g] = [g] = [g] = [g] We now work on the left side. g + = [g] = [g] Drag across the terms. g e = [g] Bring into the colmn and row matrices. e g e = [g] Clean p the sqares e g = [g] Do the order sensitive matrix prodcts e ge g g g = [g] We now have the generic reslt g ge e ge [g] = g ge + + g g g 9
10 Consistency Check We previosly evalated g ge g g α + y = x + β x β α y We want to verify e ge g g g α + y = x + β x β α y Repeating from previosly g = α + x + ye + β e g = α + x + ye + β e = x + α + βe + y e g = α + x + ye + β e = x + α βe y e g = x + α βe y e = α + x ye β e We start with the g term. g = α + x ye β e g = α + x ye β e = α + x + y + β = α + x + y + β = α + y + x + β Project and annihilate, and get the expected reslt. Contine with the g term. g = α + y g = x + α + βe + y e g = x + α + βe + y e g = x + α β y g = x + α β y g = x β + α y 0
11 Project and annihilate, and get the expected reslt. g = x β Contine with the g term. g = x + α βe y e g = x + α βe y e g = x + α + β + y g = x + α + β + y g = x + β + α + y Project and annihilate, and get the expected reslt. Finish with the g term. g = x + β g = α + x + ye + β e g = α + x + ye + β e g = α + x y β g = α + x y β g = α y + x β Project and annihilate, and get the expected reslt. g = α y Conclsion Garret Sobczyk has demonstrated why a matrix representation for D Eclidean geometric algebra is α + y x β [g] = x + β α y
Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled.
Jnction elements in network models. Classify by nmber of ports and examine the possible strctres that reslt. Using only one-port elements, no more than two elements can be assembled. Combining two two-ports
More informationLINEAR COMBINATIONS AND SUBSPACES
CS131 Part II, Linear Algebra and Matrices CS131 Mathematics for Compter Scientists II Note 5 LINEAR COMBINATIONS AND SUBSPACES Linear combinations. In R 2 the vector (5, 3) can be written in the form
More informationLesson 81: The Cross Product of Vectors
Lesson 8: The Cross Prodct of Vectors IBHL - SANTOWSKI In this lesson yo will learn how to find the cross prodct of two ectors how to find an orthogonal ector to a plane defined by two ectors how to find
More informationFEA Solution Procedure
EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations
More informationImage and Multidimensional Signal Processing
Image and Mltidimensional Signal Processing Professor William Hoff Dept of Electrical Engineering &Compter Science http://inside.mines.ed/~whoff/ Forier Transform Part : D discrete transforms 2 Overview
More informationSetting The K Value And Polarization Mode Of The Delta Undulator
LCLS-TN-4- Setting The Vale And Polarization Mode Of The Delta Undlator Zachary Wolf, Heinz-Dieter Nhn SLAC September 4, 04 Abstract This note provides the details for setting the longitdinal positions
More informationCONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4
CONTENTS INTRODUCTION MEQ crriclm objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4 VECTOR CONCEPTS FROM GEOMETRIC AND ALGEBRAIC PERSPECTIVES page 1 Representation
More informationHomework 5 Solutions
Q Homework Soltions We know that the colmn space is the same as span{a & a ( a * } bt we want the basis Ths we need to make a & a ( a * linearly independent So in each of the following problems we row
More informationSection 7.4: Integration of Rational Functions by Partial Fractions
Section 7.4: Integration of Rational Fnctions by Partial Fractions This is abot as complicated as it gets. The Method of Partial Fractions Ecept for a few very special cases, crrently we have no way to
More informationLecture 3. (2) Last time: 3D space. The dot product. Dan Nichols January 30, 2018
Lectre 3 The dot prodct Dan Nichols nichols@math.mass.ed MATH 33, Spring 018 Uniersity of Massachsetts Janary 30, 018 () Last time: 3D space Right-hand rle, the three coordinate planes 3D coordinate system:
More informationPhysicsAndMathsTutor.com
C Integration - By sbstittion PhysicsAndMathsTtor.com. Using the sbstittion cos +, or otherwise, show that e cos + sin d e(e ) (Total marks). (a) Using the sbstittion cos, or otherwise, find the eact vale
More informationAPPENDIX B MATRIX NOTATION. The Definition of Matrix Notation is the Definition of Matrix Multiplication B.1 INTRODUCTION
APPENDIX B MAIX NOAION he Deinition o Matrix Notation is the Deinition o Matrix Mltiplication B. INODUCION { XE "Matrix Mltiplication" }{ XE "Matrix Notation" }he se o matrix notations is not necessary
More informationVectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2
MATH 307 Vectors in Rn Dr. Neal, WKU Matrices of dimension 1 n can be thoght of as coordinates, or ectors, in n- dimensional space R n. We can perform special calclations on these ectors. In particlar,
More informationSTEP Support Programme. STEP III Hyperbolic Functions: Solutions
STEP Spport Programme STEP III Hyperbolic Fnctions: Soltions Start by sing the sbstittion t cosh x. This gives: sinh x cosh a cosh x cosh a sinh x t sinh x dt t dt t + ln t ln t + ln cosh a ln ln cosh
More informationDecision Making in Complex Environments. Lecture 2 Ratings and Introduction to Analytic Network Process
Decision Making in Complex Environments Lectre 2 Ratings and Introdction to Analytic Network Process Lectres Smmary Lectre 5 Lectre 1 AHP=Hierar chies Lectre 3 ANP=Networks Strctring Complex Models with
More informationBLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students
BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they
More informationGeometry of Span (continued) The Plane Spanned by u and v
Geometric Description of Span Geometr of Span (contined) 2 Geometr of Span (contined) 2 Span {} Span {, } 2 Span {} 2 Geometr of Span (contined) 2 b + 2 The Plane Spanned b and If a plane is spanned b
More informationLecture Notes: Finite Element Analysis, J.E. Akin, Rice University
9. TRUSS ANALYSIS... 1 9.1 PLANAR TRUSS... 1 9. SPACE TRUSS... 11 9.3 SUMMARY... 1 9.4 EXERCISES... 15 9. Trss analysis 9.1 Planar trss: The differential eqation for the eqilibrim of an elastic bar (above)
More informationThe Lehmer matrix and its recursive analogue
The Lehmer matrix and its recrsive analoge Emrah Kilic, Pantelimon Stănică TOBB Economics and Technology University, Mathematics Department 0660 Sogtoz, Ankara, Trkey; ekilic@etedtr Naval Postgradate School,
More informationSolving a System of Equations
Solving a System of Eqations Objectives Understand how to solve a system of eqations with: - Gass Elimination Method - LU Decomposition Method - Gass-Seidel Method - Jacobi Method A system of linear algebraic
More informationSources of Non Stationarity in the Semivariogram
Sorces of Non Stationarity in the Semivariogram Migel A. Cba and Oy Leangthong Traditional ncertainty characterization techniqes sch as Simple Kriging or Seqential Gassian Simlation rely on stationary
More informationA FIRST COURSE IN THE FINITE ELEMENT METHOD
INSTRUCTOR'S SOLUTIONS MANUAL TO ACCOMANY A IRST COURS IN TH INIT LMNT MTHOD ITH DITION DARYL L. LOGAN Contents Chapter 1 1 Chapter 3 Chapter 3 3 Chapter 17 Chapter 5 183 Chapter 6 81 Chapter 7 319 Chapter
More informationDesigning of Virtual Experiments for the Physics Class
Designing of Virtal Experiments for the Physics Class Marin Oprea, Cristina Miron Faclty of Physics, University of Bcharest, Bcharest-Magrele, Romania E-mail: opreamarin2007@yahoo.com Abstract Physics
More information10.2 Solving Quadratic Equations by Completing the Square
. Solving Qadratic Eqations b Completing the Sqare Consider the eqation ( ) We can see clearl that the soltions are However, What if the eqation was given to s in standard form, that is 6 How wold we go
More informationAdvanced topics in Finite Element Method 3D truss structures. Jerzy Podgórski
Advanced topics in Finite Element Method 3D trss strctres Jerzy Podgórski Introdction Althogh 3D trss strctres have been arond for a long time, they have been sed very rarely ntil now. They are difficlt
More informationSYMMETRY OF THE TRIPLE OCTONIONIC PRODUCT
UDC 5 SYMMETRY OF THE TRIPLE OCTONIONIC PRODUCT г M V Kharinov (997 Rssia St Petersbrg line of VI 9 SPIIRS) e-mail khar@iiasspbs The Hermitian decomposition of a linear operator is generalized to the case
More information1 Undiscounted Problem (Deterministic)
Lectre 9: Linear Qadratic Control Problems 1 Undisconted Problem (Deterministic) Choose ( t ) 0 to Minimize (x trx t + tq t ) t=0 sbject to x t+1 = Ax t + B t, x 0 given. x t is an n-vector state, t a
More informationThe Cross Product of Two Vectors in Space DEFINITION. Cross Product. u * v = s ƒ u ƒƒv ƒ sin ud n
12.4 The Cross Prodct 873 12.4 The Cross Prodct In stdying lines in the plane, when we needed to describe how a line was tilting, we sed the notions of slope and angle of inclination. In space, we want
More informationIllustrations of a Modified Standard Model: Part 1-The Solar Proton- Proton Cycle
Illstrations of a Modified : Part 1-The Solar Proton- Proton Cycle by Roger N. Weller, (proton3@gmail.com), Febrary 23, 2014 Abstract A proposed modification of the, when applied to the Solar Proton-Proton
More informationControl Systems
6.5 Control Systems Last Time: Introdction Motivation Corse Overview Project Math. Descriptions of Systems ~ Review Classification of Systems Linear Systems LTI Systems The notion of state and state variables
More informationSECTION 6.7. The Dot Product. Preview Exercises. 754 Chapter 6 Additional Topics in Trigonometry. 7 w u 7 2 =?. 7 v 77w7
754 Chapter 6 Additional Topics in Trigonometry 115. Yo ant to fly yor small plane de north, bt there is a 75-kilometer ind bloing from est to east. a. Find the direction angle for here yo shold head the
More informationDecoder Error Probability of MRD Codes
Decoder Error Probability of MRD Codes Maximilien Gadolea Department of Electrical and Compter Engineering Lehigh University Bethlehem, PA 18015 USA E-mail: magc@lehigh.ed Zhiyan Yan Department of Electrical
More informationTechnical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty
Technical Note EN-FY160 Revision November 30, 016 ODiSI-B Sensor Strain Gage Factor Uncertainty Abstract Lna has pdated or strain sensor calibration tool to spport NIST-traceable measrements, to compte
More informationChapter 5 Dot, Inner and Cross Products. 5.1 Length of a vector 5.2 Dot Product 5.3 Inner Product 5.4 Cross Product
Chapter 5 Dot Inner and Cross Prodcts 5. Length of a ector 5. Dot Prodct 5.3 Inner Prodct 5.4 Cross Prodct 5. Length and Dot Prodct in R n Length: The length of a ector ( n in R n is gien by n Notes: The
More information4.4 Moment of a Force About a Line
4.4 Moment of a orce bot a Line 4.4 Moment of a orce bot a Line Eample 1, page 1 of 3 1. orce is applied to the end of gearshift lever DE. Determine the moment of abot shaft. State which wa the lever will
More informationIntrodction Finite elds play an increasingly important role in modern digital commnication systems. Typical areas of applications are cryptographic sc
A New Architectre for a Parallel Finite Field Mltiplier with Low Complexity Based on Composite Fields Christof Paar y IEEE Transactions on Compters, Jly 996, vol 45, no 7, pp 856-86 Abstract In this paper
More information1 The space of linear transformations from R n to R m :
Math 540 Spring 20 Notes #4 Higher deriaties, Taylor s theorem The space of linear transformations from R n to R m We hae discssed linear transformations mapping R n to R m We can add sch linear transformations
More informationStudy on the Mathematic Model of Product Modular System Orienting the Modular Design
Natre and Science, 2(, 2004, Zhong, et al, Stdy on the Mathematic Model Stdy on the Mathematic Model of Prodct Modlar Orienting the Modlar Design Shisheng Zhong 1, Jiang Li 1, Jin Li 2, Lin Lin 1 (1. College
More information3.4-Miscellaneous Equations
.-Miscellaneos Eqations Factoring Higher Degree Polynomials: Many higher degree polynomials can be solved by factoring. Of particlar vale is the method of factoring by groping, however all types of factoring
More informationOptimization via the Hamilton-Jacobi-Bellman Method: Theory and Applications
Optimization via the Hamilton-Jacobi-Bellman Method: Theory and Applications Navin Khaneja lectre notes taken by Christiane Koch Jne 24, 29 1 Variation yields a classical Hamiltonian system Sppose that
More informationDifferentiation of Exponential Functions
Differentiation of Eponential Fnctions The net derivative rles that o will learn involve eponential fnctions. An eponential fnction is a fnction in the form of a constant raised to a variable power. The
More informationDecoder Error Probability of MRD Codes
Decoder Error Probability of MRD Codes Maximilien Gadolea Department of Electrical and Compter Engineering Lehigh University Bethlehem, PA 18015 USA E-mail: magc@lehighed Zhiyan Yan Department of Electrical
More informationCurves - Foundation of Free-form Surfaces
Crves - Fondation of Free-form Srfaces Why Not Simply Use a Point Matrix to Represent a Crve? Storage isse and limited resoltion Comptation and transformation Difficlties in calclating the intersections
More informationMean Value Formulae for Laplace and Heat Equation
Mean Vale Formlae for Laplace and Heat Eqation Abhinav Parihar December 7, 03 Abstract Here I discss a method to constrct the mean vale theorem for the heat eqation. To constrct sch a formla ab initio,
More informationLinear System Theory (Fall 2011): Homework 1. Solutions
Linear System Theory (Fall 20): Homework Soltions De Sep. 29, 20 Exercise (C.T. Chen: Ex.3-8). Consider a linear system with inpt and otpt y. Three experiments are performed on this system sing the inpts
More informationPulses on a Struck String
8.03 at ESG Spplemental Notes Plses on a Strck String These notes investigate specific eamples of transverse motion on a stretched string in cases where the string is at some time ndisplaced, bt with a
More informationPhysicsAndMathsTutor.com
. Two smooth niform spheres S and T have eqal radii. The mass of S is 0. kg and the mass of T is 0.6 kg. The spheres are moving on a smooth horizontal plane and collide obliqely. Immediately before the
More informationThe Brauer Manin obstruction
The Braer Manin obstrction Martin Bright 17 April 2008 1 Definitions Let X be a smooth, geometrically irredcible ariety oer a field k. Recall that the defining property of an Azmaya algebra A is that,
More informationAssignment Fall 2014
Assignment 5.086 Fall 04 De: Wednesday, 0 December at 5 PM. Upload yor soltion to corse website as a zip file YOURNAME_ASSIGNMENT_5 which incldes the script for each qestion as well as all Matlab fnctions
More informationWhen are Two Numerical Polynomials Relatively Prime?
J Symbolic Comptation (1998) 26, 677 689 Article No sy980234 When are Two Nmerical Polynomials Relatively Prime? BERNHARD BECKERMANN AND GEORGE LABAHN Laboratoire d Analyse Nmériqe et d Optimisation, Université
More information3.3 Operations With Vectors, Linear Combinations
Operations With Vectors, Linear Combinations Performance Criteria: (d) Mltiply ectors by scalars and add ectors, algebraically Find linear combinations of ectors algebraically (e) Illstrate the parallelogram
More informationSecond-Order Wave Equation
Second-Order Wave Eqation A. Salih Department of Aerospace Engineering Indian Institte of Space Science and Technology, Thirvananthapram 3 December 016 1 Introdction The classical wave eqation is a second-order
More informationNilpotents and Idempotents in 2D and 3D Euclidean Geometric Algebra
Nilpotents and Idempotents in D and D Euclidean Geometric Algebra Kurt Nalty July 11, 015 Abstract I present general homework level formulas for nilpotents (non-zero expressions which square to zero) and
More informationStair Matrix and its Applications to Massive MIMO Uplink Data Detection
1 Stair Matrix and its Applications to Massive MIMO Uplink Data Detection Fan Jiang, Stdent Member, IEEE, Cheng Li, Senior Member, IEEE, Zijn Gong, Senior Member, IEEE, and Roy S, Stdent Member, IEEE Abstract
More informationDepartment of Industrial Engineering Statistical Quality Control presented by Dr. Eng. Abed Schokry
Department of Indstrial Engineering Statistical Qality Control presented by Dr. Eng. Abed Schokry Department of Indstrial Engineering Statistical Qality Control C and U Chart presented by Dr. Eng. Abed
More informationHigher Maths A1.3 Recurrence Relations - Revision
Higher Maths A Recrrence Relations - Revision This revision pack covers the skills at Unit Assessment exam level or Recrrence Relations so yo can evalate yor learning o this otcome It is important that
More informationVectors. Vectors ( 向量 ) Representation of Vectors. Special Vectors. Equal vectors. Chapter 16
Vectors ( 向量 ) Chapter 16 2D Vectors A vector is a line which has both magnitde and direction. For example, in a weather report yo may hear a statement like the wind is blowing at 25 knots ( 海浬 ) in the
More informationCS 450: COMPUTER GRAPHICS VECTORS SPRING 2016 DR. MICHAEL J. REALE
CS 45: COMPUTER GRPHICS VECTORS SPRING 216 DR. MICHEL J. RELE INTRODUCTION In graphics, we are going to represent objects and shapes in some form or other. First, thogh, we need to figre ot how to represent
More informationControl Systems Design
ELEC4410 Control Systems Design Lectre 16: Controllability and Observability Canonical Decompositions Jlio H. Braslavsky jlio@ee.newcastle.ed.a School of Electrical Engineering and Compter Science Lectre
More informationIntegration of Basic Functions. Session 7 : 9/23 1
Integration o Basic Fnctions Session 7 : 9/3 Antiderivation Integration Deinition: Taking the antiderivative, or integral, o some nction F(), reslts in the nction () i ()F() Pt simply: i yo take the integral
More informationDiscussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli
1 Introdction Discssion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli Søren Johansen Department of Economics, University of Copenhagen and CREATES,
More informationQuadratic and Rational Inequalities
Chapter Qadratic Eqations and Ineqalities. Gidelines for solving word problems: (a) Write a verbal model that will describe what yo need to know. (b) Assign labels to each part of the verbal model nmbers
More informationAffine Invariant Total Variation Models
Affine Invariant Total Variation Models Helen Balinsky, Alexander Balinsky Media Technologies aboratory HP aboratories Bristol HP-7-94 Jne 6, 7* Total Variation, affine restoration, Sobolev ineqality,
More information4 Primitive Equations
4 Primitive Eqations 4.1 Spherical coordinates 4.1.1 Usefl identities We now introdce the special case of spherical coordinates: (,, r) (longitde, latitde, radial distance from Earth s center), with 0
More informationSimplified Identification Scheme for Structures on a Flexible Base
Simplified Identification Scheme for Strctres on a Flexible Base L.M. Star California State University, Long Beach G. Mylonais University of Patras, Greece J.P. Stewart University of California, Los Angeles
More informationEffects Of Symmetry On The Structural Controllability Of Neural Networks: A Perspective
16 American Control Conference (ACC) Boston Marriott Copley Place Jly 6-8, 16. Boston, MA, USA Effects Of Symmetry On The Strctral Controllability Of Neral Networks: A Perspective Andrew J. Whalen 1, Sean
More informationThe Dual of the Maximum Likelihood Method
Department of Agricltral and Resorce Economics University of California, Davis The Dal of the Maximm Likelihood Method by Qirino Paris Working Paper No. 12-002 2012 Copyright @ 2012 by Qirino Paris All
More information3 2D Elastostatic Problems in Cartesian Coordinates
D lastostatic Problems in Cartesian Coordinates Two dimensional elastostatic problems are discssed in this Chapter, that is, static problems of either plane stress or plane strain. Cartesian coordinates
More informationSection 9. Paraxial Raytracing
OPTI-/ Geometrical and Instrmental Optics Copright 8 John E. Greivenkamp 9- Section 9 Paraxial atracing YNU atrace efraction (or reflection) occrs at an interface between two optical spaces. The transfer
More informationEfficiency Increase and Input Power Decrease of Converted Prototype Pump Performance
International Jornal of Flid Machinery and Systems DOI: http://dx.doi.org/10.593/ijfms.016.9.3.05 Vol. 9, No. 3, Jly-September 016 ISSN (Online): 188-9554 Original Paper Efficiency Increase and Inpt Power
More informationQUANTILE ESTIMATION IN SUCCESSIVE SAMPLING
Jornal of the Korean Statistical Society 2007, 36: 4, pp 543 556 QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Hosila P. Singh 1, Ritesh Tailor 2, Sarjinder Singh 3 and Jong-Min Kim 4 Abstract In sccessive
More informationFRTN10 Exercise 12. Synthesis by Convex Optimization
FRTN Exercise 2. 2. We want to design a controller C for the stable SISO process P as shown in Figre 2. sing the Yola parametrization and convex optimization. To do this, the control loop mst first be
More informationEvaluation of the Fiberglass-Reinforced Plastics Interfacial Behavior by using Ultrasonic Wave Propagation Method
17th World Conference on Nondestrctive Testing, 5-8 Oct 008, Shanghai, China Evalation of the Fiberglass-Reinforced Plastics Interfacial Behavior by sing Ultrasonic Wave Propagation Method Jnjie CHANG
More informationCONSIDER an array of N sensors (residing in threedimensional. Investigating Hyperhelical Array Manifold Curves Using the Complex Cartan Matrix
IEEE JOURNAL OF SELECTED TOPICS IN SIGNAL PROCESSING (SPECIAL ISSUE), VOL.?, NO.?,???? 1 Investigating yperhelical Array Manifold Crves Using the Complex Cartan Matrix Athanassios Manikas, Senior Member,
More informationOn the tree cover number of a graph
On the tree cover nmber of a graph Chassidy Bozeman Minerva Catral Brendan Cook Oscar E. González Carolyn Reinhart Abstract Given a graph G, the tree cover nmber of the graph, denoted T (G), is the minimm
More informationDigital Image Processing. Lecture 8 (Enhancement in the Frequency domain) Bu-Ali Sina University Computer Engineering Dep.
Digital Image Processing Lectre 8 Enhancement in the Freqenc domain B-Ali Sina Uniersit Compter Engineering Dep. Fall 009 Image Enhancement In The Freqenc Domain Otline Jean Baptiste Joseph Forier The
More informationsin u 5 opp } cos u 5 adj } hyp opposite csc u 5 hyp } sec u 5 hyp } opp Using Inverse Trigonometric Functions
13 Big Idea 1 CHAPTER SUMMARY BIG IDEAS Using Trigonometric Fnctions Algebra classzone.com Electronic Fnction Library For Yor Notebook hypotense acent osite sine cosine tangent sin 5 hyp cos 5 hyp tan
More informationsin xdx = cos x + c We also run into antiderivatives for tan x, cot x, sec x and csc x in the section on Log integrals. They are: cos ax sec ax a
Trig Integrals We already know antiderivatives for sin x, cos x, sec x tan x, csc x, sec x and csc x cot x. They are cos xdx = sin x sin xdx = cos x sec x tan xdx = sec x csc xdx = cot x sec xdx = tan
More informationCRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE. Jingbo Xia
CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE Jingbo Xia Abstract. Let H 2 (S) be the Hardy space on the nit sphere S in C n. We show that a set of inner fnctions Λ is sfficient for the prpose of determining
More informationLecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2
BIJU PATNAIK UNIVERSITY OF TECHNOLOGY, ODISHA Lectre Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 Prepared by, Dr. Sbhend Kmar Rath, BPUT, Odisha. Tring Machine- Miscellany UNIT 2 TURING MACHINE
More informationMath 144 Activity #10 Applications of Vectors
144 p 1 Math 144 Actiity #10 Applications of Vectors In the last actiity, yo were introdced to ectors. In this actiity yo will look at some of the applications of ectors. Let the position ector = a, b
More informationElectron Phase Slip in an Undulator with Dipole Field and BPM Errors
CS-T--14 October 3, Electron Phase Slip in an Undlator with Dipole Field and BPM Errors Pal Emma SAC ABSTRACT A statistical analysis of a corrected electron trajectory throgh a planar ndlator is sed to
More informationGraphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007
Graphs and Networks Lectre 5 PageRank Lectrer: Daniel A. Spielman September 20, 2007 5.1 Intro to PageRank PageRank, the algorithm reportedly sed by Google, assigns a nmerical rank to eery web page. More
More informationUNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL
8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a
More informationMEG 741 Energy and Variational Methods in Mechanics I
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationUncertainty Analysis of the Thunder Scientific Model 1200 Two-Pressure Humidity Generator
Uncertainty Analysis of the hnder cientific Model 100 wo-ressre Hmidity Generator 1.0 Introdction escribed here is the generated hmidity ncertainty analysis, following the Gidelines of NI and NL International
More informationElements of Coordinate System Transformations
B Elements of Coordinate System Transformations Coordinate system transformation is a powerfl tool for solving many geometrical and kinematic problems that pertain to the design of gear ctting tools and
More informationStudy on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom
EPJ Web of Conferences 80, 0034 (08) EFM 07 Stdy on the implsive pressre of tank oscillating by force towards mltiple degrees of freedom Shigeyki Hibi,* The ational Defense Academy, Department of Mechanical
More informationFEA Solution Procedure
EA Soltion Procedre (demonstrated with a -D bar element problem) MAE 5 - inite Element Analysis Several slides from this set are adapted from B.S. Altan, Michigan Technological University EA Procedre for
More informationIntro to path analysis Richard Williams, University of Notre Dame, https://www3.nd.edu/~rwilliam/ Last revised April 6, 2015
Intro to path analysis Richard Williams, Uniersity of Notre Dame, https://3.nd.ed/~rilliam/ Last reised April 6, 05 Sorces. This discssion dras heaily from Otis Ddley Dncan s Introdction to Strctral Eqation
More information1. Introduction 1.1. Background and previous results. Ramanujan introduced his zeta function in 1916 [11]. Following Ramanujan, let.
IDENTITIES FOR THE RAMANUJAN ZETA FUNCTION MATHEW ROGERS Abstract. We prove formlas for special vales of the Ramanjan ta zeta fnction. Or formlas show that L(, k) is a period in the sense of Kontsevich
More informationA Characterization of the Domain of Beta-Divergence and Its Connection to Bregman Variational Model
entropy Article A Characterization of the Domain of Beta-Divergence and Its Connection to Bregman Variational Model Hyenkyn Woo School of Liberal Arts, Korea University of Technology and Edcation, Cheonan
More informationOptimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance
Optimal Control of a Heterogeneos Two Server System with Consideration for Power and Performance by Jiazheng Li A thesis presented to the University of Waterloo in flfilment of the thesis reqirement for
More informationKonyalioglu, Serpil. Konyalioglu, A.Cihan. Ipek, A.Sabri. Isik, Ahmet
The Role of Visalization Approach on Stdent s Conceptal Learning Konyaliogl, Serpil Department of Secondary Science and Mathematics Edcation, K.K. Edcation Faclty, Atatürk University, 25240- Erzrm-Trkey;
More informationOn relative errors of floating-point operations: optimal bounds and applications
On relative errors of floating-point operations: optimal bonds and applications Clade-Pierre Jeannerod, Siegfried M. Rmp To cite this version: Clade-Pierre Jeannerod, Siegfried M. Rmp. On relative errors
More information10.4 Solving Equations in Quadratic Form, Equations Reducible to Quadratics
. Solving Eqations in Qadratic Form, Eqations Redcible to Qadratics Now that we can solve all qadratic eqations we want to solve eqations that are not eactl qadratic bt can either be made to look qadratic
More informationChapter 2 Difficulties associated with corners
Chapter Difficlties associated with corners This chapter is aimed at resolving the problems revealed in Chapter, which are cased b corners and/or discontinos bondar conditions. The first section introdces
More information1. INTRODUCTION. A solution for the dark matter mystery based on Euclidean relativity. Frédéric LASSIAILLE 2009 Page 1 14/05/2010. Frédéric LASSIAILLE
Frédéric LASSIAILLE 2009 Page 1 14/05/2010 Frédéric LASSIAILLE email: lmimi2003@hotmail.com http://lmi.chez-alice.fr/anglais A soltion for the dark matter mystery based on Eclidean relativity The stdy
More information