Linear Algebra

Total Page:16

File Type:pdf, Size:1020Kb

Linear Algebra Department of Stat. and OR Refresher course, Summer 2019 Linear Algebra Modified By: Eric Lock (UNC, 2010 & 2011) Original Author: Gen Li (UNC, 2012) Oleg Mayba, Michael Lamm (UNC, 2013) UC Berkeley Wen Jenny Shi (UNC, 2014) Department of Statistics, Meilei Jiang (UNC, 2015 & 2016) 2006, Iain Carmichael (UNC, 2017) DMS Grant No 0130526 Adam Waterbury (UNC, 2018) Brendan Brown (UNC, 2019) Instructor: Brendan Brown (UNC at Chapel Hill) August 9, 2019 Contents 1 Introduction3 2 Vector Spaces4 2.1 Basic Concepts..................................5 2.2 Special Spaces...................................8 2.3 Properties and geometry of inner product spaces................ 12 2.4 Gram-Schmidt Process.............................. 15 2.5 Comments on infinite-dimensional spaces.................... 16 Exercises......................................... 17 3 Matrices and Matrix Algebra 20 3.1 Matrix Operations................................ 20 3.2 Special Matrices.................................. 22 3.3 The Four Fundamental Spaces.......................... 23 3.4 Sample Covariance matrix............................ 25 Exercises......................................... 26 4 Projections and Least Squares Estimation 27 4.1 Projections.................................... 27 4.2 Applications to Statistics: Least Squares Estimator.............. 30 Exercises......................................... 32 5 Linear functionals, riesz representation and hyperplane separation 34 5.1 Linear functionals................................. 34 5.2 Hyperplane separation.............................. 36 6 Matrix Decompositions 39 6.1 Determinants................................... 39 6.2 Eigenvalues and Eigenvectors.......................... 41 6.3 Complex Matrices................................. 45 6.4 Facts that lead up to the spectral theorem................... 45 6.5 Spectral Theorem................................. 47 6.6 Examples: Spectral theory............................ 50 Exercises......................................... 52 7 Tensors 55 7.1 Exercises...................................... 57 8 Singular Value Decomposition 57 8.1 Definition..................................... 57 8.2 Low rank approximation............................. 60 8.3 A few Applications................................ 60 8.4 Principal Components Analysis......................... 62 8.5 The $25,000,000,000 Eigenvector: the Linear Algebra Behind Google.... 65 1 Exercises......................................... 65 9 Matrix functions and differentiation 67 9.1 Basics....................................... 67 9.2 Jacobian and Chain Rule............................. 67 9.3 Matrix functions................................. 69 Exercises......................................... 70 10 Computation 71 10.1 Power method................................... 71 10.2 Gradient Descent................................. 73 11 Statistics: Random Variables 74 11.1 Expectation, Variance and Covariance..................... 74 11.2 Distribution of Functions of Random Variables................. 76 11.3 Derivation of Common Univariate Distributions................ 79 11.4 Random Vectors: Expectation and Variance.................. 82 Exercises......................................... 84 12 Further Applications to Statistics: Normal Theory and F-test 85 12.1 Bivariate Normal Distribution.......................... 85 12.2 F-test....................................... 86 Exercises......................................... 88 13 References 89 2 1 Introduction These notes are intended for use in the warm-up camp for incoming UNC STOR graduate students. Welcome to Carolina! We assume that you have taken a linear algebra course before and that most of the ma- terial in these notes will be a review of what you've already known. If some of the material is unfamiliar, do not be intimidated! We hope you find these notes helpful. If not, you can consult the references listed at the end, or any other textbooks of your choice for more information or another style of presentation (most of the proofs on linear algebra part have been adopted from Strang, the proof of F-test from Montgomery et al, and the proof of bivariate normal density from Bickel and Doksum). Linear algebra is an important and fundamental math tool for probability, statistics, nu- merical analysis and operations research. Lots of material in this notes will show up in your future study and research. There will be 8 algebraic classes in total. In the second week we may cover some topics in computational linear algebra with applications to statistics and machine learning (PCA, PageRank, Spectra Clustering, etc). See the notes and course schedule on the UNC STOR bootcamp webpage. 3 2 Vector Spaces A set V is a vector space over R (or any field) with two operations defined on it: 1. Vector addition, that assigns to each pair of vectors v1; v2 2 V another vector w 2 V (we write v1 + v2 = w) 2. Scalar multiplication, that assigns to each vector v 2 V and each scalar r 2 R (field) another vector w 2 V (we write rv = w) The elements of V are called vectors and must satisfy the following 8 conditions 8 v1; v2; v3 2 V and 8 r1; r2 2 R: 1. Commutativity of vector addition: v1 + v2 = v2 + v1 2. Associativity of vector addition: (v1 + v2) + v3 = v1 + (v2 + v3) 3. Identity element of vector addition: 9 vector 0 2 V , s.t. v + 0 = v, 8 v 2 V 4. Inverse elements of vector addition: 8 v 2 V 9 −v = w 2 V s.t. v + w = 0 5. Compatibility of scalar multiplication with (field) multiplication: r1(r2v) = (r1r2)v, 8 v 2 V 6. Distributivity of scalar multiplication with respect to (field) addition: (r1 + r2)v = r1v + r2v, 8 v 2 V 7. Distributivity of scalar multiplication with respect to vector addition: r(v1 + v2) = rv1 + rv2, 8 r 2 R 8. Identity element of scalar multiplication: 1v = v, 8 v 2 V Vector spaces over fields other than R are defined similarly, with the multiplicative iden- tity of the field replacing 1. We won't concern ourselves with those spaces, except for when we need complex numbers later on. Also, we'll be using the symbol 0 to designate both the number 0 and the vector 0 in V , and you should always be able to tell the difference from the context. Sometimes, we'll emphasize that we're dealing with, say, n × 1 vector 0 by writing 0n×1. Here are some examples of vector spaces 1. Rn with usual operations of element-wise addition and scalar multiplication. An ex- ample of these operations in R2 is illustrated in Figure2. 2. Vector space F[−1;1] of all functions defined on interval [−1; 1], where we define (f+g)(x) = f(x) + g(x) and (rf)(x) = rf(x). 4 - 6 v + w v w - 2w- Figure 1: Vector Addition and Scalar Multiplication 2.1 Basic Concepts Subspace and span We say that S ⊂ V is a subspace of V , if S is closed under vector addition and scalar multiplication, i.e. 1. 8s1; s2 2 S, s1 + s2 2 S 2. 8s 2 S, 8r 2 R, rs 2 S You can verify that if those conditions hold, S is a vector space in its own right (satisfies the 8 conditions above). Note also that S has to be non-empty; the empty set is not allowed as a subspace. Examples: 1. A subset f0g is always a subspace of a vectors space V . Pn 2. Given a set of vectors S ⊂ V , span(S) = fw : w = i=1 rivi; ri 2 R; and vi 2 Sg, the set of all linear combinations of elements of S (see below for definition) is a subspace of V . 3. S = f(x; y) 2 R2 : y = 0g is a subspace of R2 (x-axis). 4. The set of all continuous functions defined on interval [−1; 1] is a subspace of F[−1;1]. For all of the above examples, you should check for yourself that they are in fact subspaces. Given vectors v1; v2; : : : ; vn 2 V , we say that w 2 V is a linear combination of n P v1; v2; : : : ; vn if for some r1; r2; : : : ; rn 2 R, we have w = rivi. If every vector in V is i=1 a linear combination of S = fv1; v2; : : : ; vng, we have span(S) = V , then we say S spans V . Fact: A set S ⊆ V is a subspace if and only if it is closed under linear combinations. Linear independence and dependence Given vectors v1; v2; : : : ; vn 2 V we say that n P v1; v2; : : : ; vn are linearly independent if rivi = 0 =) r1 = r2 = ::: = rn = 0, i.e. the i=1 only linear combination of v1; v2; : : : ; vn that produces 0 vector is the trivial one. We say 5 that v1; v2; : : : ; vn are linearly dependent otherwise. We now prove two results that will be used later and give some practice with linear al- gebra proofs. Theorem: Let I;S ⊂ V be such that I is linearly independent, and S spans V . Then for every x 2 I there exists a y 2 S such that fyg [ Infxg is linearly independent. Proof: We prove this result by contradiction. First two two facts that can be easily verified from the definitions above. 1. If a set J ⊂ V is linearly independent, then J [ fyg is linearly dependent if and only if y 2 span(J). 2. If S; T ⊂ V with T ⊂ span(S) then span(T ) ⊂ span(S). Assume for the sake of contradiction that the claim does not hold. I.e. suppose there there exists a x 2 I such that for all y 2 S fyg[Infxg is linearly dependent. Let I0 = Infxg. Since I is linearly independent it follows that I0 is also linearly independent. Then by the first fact above, the fact that fyg [ I0 is linearly dependent implies y 2 span(I0). Moreover, this holds for all y 2 S so S ⊂ span(I0). By the second fact we then have that span(S) ⊂ span(I0). Now since S spans V it follows that x 2 V = span(S) ⊂ span(I0) = span(Infxg). This means there exists Pn v1; v2; : : : ; vn 2 Infxg and r1; r2; : : : ; rn 2 R such that 0 = x − i=1 rivi, contradicting the assumption that I linearly independent. Corollary: Let I;S ⊂ V be such that I is linearly independent, and S spans V . Then jIj ≤ jSj, where |· j denotes the number of elements of a set (possibly infinite). Proof: If jSj = 1 then the claim holds.
Recommended publications
  • Course Introduction
    Spectral Graph Theory Lecture 1 Introduction Daniel A. Spielman September 2, 2015 Disclaimer These notes are not necessarily an accurate representation of what happened in class. The notes written before class say what I think I should say. I sometimes edit the notes after class to make them way what I wish I had said. There may be small mistakes, so I recommend that you check any mathematically precise statement before using it in your own work. These notes were last revised on September 3, 2015. 1.1 First Things 1. Please call me \Dan". If such informality makes you uncomfortable, you can try \Professor Dan". If that fails, I will also answer to \Prof. Spielman". 2. If you are going to take this course, please sign up for it on Classes V2. This is the only way you will get emails like \Problem 3 was false, so you don't have to solve it". 3. This class meets this coming Friday, September 4, but not on Labor Day, which is Monday, September 7. 1.2 Introduction I have three objectives in this lecture: to tell you what the course is about, to help you decide if this course is right for you, and to tell you how the course will work. As the title suggests, this course is about the eigenvalues and eigenvectors of matrices associated with graphs, and their applications. I will never forget my amazement at learning that combinatorial properties of graphs could be revealed by an examination of the eigenvalues and eigenvectors of their associated matrices.
    [Show full text]
  • Arxiv:1012.3835V1
    A NEW GENERALIZED FIELD OF VALUES RICARDO REIS DA SILVA∗ Abstract. Given a right eigenvector x and a left eigenvector y associated with the same eigen- value of a matrix A, there is a Hermitian positive definite matrix H for which y = Hx. The matrix H defines an inner product and consequently also a field of values. The new generalized field of values is always the convex hull of the eigenvalues of A. Moreover, it is equal to the standard field of values when A is normal and is a particular case of the field of values associated with non-standard inner products proposed by Givens. As a consequence, in the same way as with Hermitian matrices, the eigenvalues of non-Hermitian matrices with real spectrum can be characterized in terms of extrema of a corresponding generalized Rayleigh Quotient. Key words. field of values, numerical range, Rayleigh quotient AMS subject classifications. 15A60, 15A18, 15A42 1. Introduction. We propose a new generalized field of values which brings all the properties of the standard field of values to non-Hermitian matrices. For a matrix A ∈ Cn×n the (classical) field of values or numerical range of A is the set of complex numbers F (A) ≡{x∗Ax : x ∈ Cn, x∗x =1}. (1.1) Alternatively, the field of values of a matrix A ∈ Cn×n can be described as the region in the complex plane defined by the range of the Rayleigh Quotient x∗Ax ρ(x, A) ≡ , ∀x 6=0. (1.2) x∗x For Hermitian matrices, field of values and Rayleigh Quotient exhibit very agreeable properties: F (A) is a subset of the real line and the extrema of F (A) coincide with the extrema of the spectrum, σ(A), of A.
    [Show full text]
  • Spectral Graph Theory: Applications of Courant-Fischer∗
    Spectral graph theory: Applications of Courant-Fischer∗ Steve Butler September 2006 Abstract In this second talk we will introduce the Rayleigh quotient and the Courant- Fischer Theorem and give some applications for the normalized Laplacian. Our applications will include structural characterizations of the graph, interlacing results for addition or removal of subgraphs, and interlacing for weak coverings. We also will introduce the idea of “weighted graphs”. 1 Introduction In the first talk we introduced the three common matrices that are used in spectral graph theory, namely the adjacency matrix, the combinatorial Laplacian and the normalized Laplacian. In this talk and the next we will focus on the normalized Laplacian. This is a reflection of the bias of the author having worked closely with Fan Chung who popularized the normalized Laplacian. The adjacency matrix and the combinatorial Laplacian are also very interesting to study in their own right and are useful for giving structural information about a graph. However, in many “practical” applications it tends to be the spectrum of the normalized Laplacian which is most useful. In this talk we will introduce the Rayleigh quotient which is closely linked to the Courant-Fischer Theorem and give some results. We give some structural results (such as showing that if a graph is bipartite then the spectrum is symmetric around 1) as well as some interlacing and weak covering results. But first, we will start by listing some common spectra. ∗Second of three talks given at the Center for Combinatorics, Nankai University, Tianjin 1 Some common spectra When studying spectral graph theory it is good to have a few basic examples to start with and be familiar with their spectrums.
    [Show full text]
  • Lecture 8: Eigenvalues, Eigenvectors and Spectral Theorem Lecturer: Shayan Oveis Gharan April 20Th Scribe: Sudipto Mukherjee
    CSE 521: Design and Analysis of Algorithms I Spring 2016 Lecture 8: Eigenvalues, Eigenvectors and Spectral Theorem Lecturer: Shayan Oveis Gharan April 20th Scribe: Sudipto Mukherjee Disclaimer: These notes have not been subjected to the usual scrutiny reserved for formal publications. 8.1 Introduction Let M 2 Rn×n be a symmetric matrix. We say λ is an eigenvalue of M with eigenvector v, if Mv = λv: Theorem 8.1. If M is symmetric, then all its eigenvalues are real. Proof. Suppose Mv = λv: We want to show that λ has imaginary value 0. For a complex number x = a + ib, the conjugate of x, is defined as follows: x∗ = a − ib. So, all we need to show is that λ = λ∗. The conjugate of a vector is the conjugate of all of its coordinate. Taking the conjugate transpose of both sides of the above equality, we have v∗M = λ∗v∗; (8.1) where we used that M T = M. So, on one hand, v∗Mv = v∗(Mv) = v∗(λv) = λ(v∗v): and on the other hand, by (8.1) v∗Mv = λ∗v∗v: So, we must have λ = λ∗. 8.2 Characteristic Polynomial If M does not have 0 as one of its eigenvalues, then det(M) 6= 0. An equivalent statement is that, if M all columns of M are linearly independent, then det(M) 6= 0. If λ is an eigenvalue of M, then Mv = λv, so (M − λI)v = 0. In other words, M − λI has a zero eigenvalue and det(M − λI) = 0.
    [Show full text]
  • The Rayleigh Quotient Iteration and Some Generalizations for Nonnormal Matrices B. N. Parlett Mathematics of Computation, Vol. 2
    The Rayleigh Quotient Iteration and Some Generalizations for Nonnormal Matrices B. N. Parlett Mathematics of Computation, Vol. 28, No. 127. (Jul., 1974), pp. 679-693. Stable URL: http://links.jstor.org/sici?sici=0025-5718%28197407%2928%3A127%3C679%3ATRQIAS%3E2.0.CO%3B2-7 Mathematics of Computation is currently published by American Mathematical Society. Your use of the JSTOR archive indicates your acceptance of JSTOR's Terms and Conditions of Use, available at http://www.jstor.org/about/terms.html. JSTOR's Terms and Conditions of Use provides, in part, that unless you have obtained prior permission, you may not download an entire issue of a journal or multiple copies of articles, and you may use content in the JSTOR archive only for your personal, non-commercial use. Please contact the publisher regarding any further use of this work. Publisher contact information may be obtained at http://www.jstor.org/journals/ams.html. Each copy of any part of a JSTOR transmission must contain the same copyright notice that appears on the screen or printed page of such transmission. JSTOR is an independent not-for-profit organization dedicated to and preserving a digital archive of scholarly journals. For more information regarding JSTOR, please contact [email protected]. http://www.jstor.org Tue May 8 02:10:06 2007 MATHEMATICS OF COMPUTATION, VOLUME 28, NUMBER 127, JULY 1974, PAGES 679-693 The Rayleigh Quotient Iteration and Some Generalizations for Nonnormal Matrices* By B. N. Parlett Abstract. The Rayleigh Quotient Iteration (RQI) was developed for real symmetric matrices. Its rapid local convergence is due to the stationarity of the Rayleigh Quotient at an eigenvector.
    [Show full text]
  • Introduction to Spectral Graph Theory
    Introduction to spectral graph theory c A. J. Ganesh, University of Bristol, 2015 1 Linear Algebra Review n×n We write M 2 R to denote that M is an n×n matrix with real elements, n and v 2 R to denote that v is a vector of length n. Vectors are usually taken to be column vectors unless otherwise specified. Recall that a real n×n n n matrix M 2 R represents a linear operator from R to R . In other n words, given any vector v 2 R , we think of M as a function which maps n it to another vector w 2 R , namely the matrix-vector product. Moreover, this function is linear: M(v1 + v2) = Mv1 + Mv2 for any two vectors v1 and v2, and M(λv) = λMv for any real number λ and any vector v. The perspective of matrices as linear operators is important to keep in mind throughout this course. If there is a λ 2 C such that Mv = λv, then we say that v is an (right) eigenvector of M corresponding to the eigenvalue λ. Likewise, w is a left eigenvector of M with eigenvalue λ if wT M = λwT . Here wT denotes the transpose of w. We will write M y and wy to denote the Hermitian conjugates of M and w, namely the complex conjugate of the transpose of M and w respectively. For example, 1 2 + i 1 3 + i M = ) M y = : 3 − i i 2 − i −i In this course, we will mainly be dealing with real vectors and matrices; for these, the Hermitian conjugate is the same as the transpose.
    [Show full text]
  • A Theoretical and Computational Comparison of Approximations Used in Perturbation Analysis of Covariance Matrices Jacques Bénasséni, Alain Mom
    A theoretical and computational comparison of approximations used in perturbation analysis of covariance matrices Jacques Bénasséni, Alain Mom To cite this version: Jacques Bénasséni, Alain Mom. A theoretical and computational comparison of approximations used in perturbation analysis of covariance matrices. 2019. hal-02083181 HAL Id: hal-02083181 https://hal.archives-ouvertes.fr/hal-02083181 Preprint submitted on 28 Mar 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A theoretical and computational comparison of approximations used in perturbation analysis of covariance matrices Jacques B´enass´eni and Alain Mom ∗† Univ Rennes, CNRS, IRMAR - UMR 6625 F-35000 Rennes, France Abstract Covariance matrices play a central role in a wide range of multivariate statistical methods. Therefore, a large amount of work has been devoted to analyzing the sensitivity of their eigenstructure to influential observations. In order to evaluate the effect of deleting one or a small subset of the observations, several approxima- tions to the eigenelements of the perturbed matrix have been proposed. This paper provides a theoretical and numerical comparison of the main approximations. A special emphasis is given to those based on Rayleigh quotients which are seldom used.
    [Show full text]
  • 1 Canonical Forms
    Bindel, Fall 2016 Matrix Computations (CS 6210) Notes for 2016-10-28 1 Canonical forms Abstract linear algebra is about vector spaces and the operations on them, independent of any specific choice of basis. But while the abstract view is useful, when we compute, we are concrete, working with the vector spaces Rn and Cn with a standard norm or inner product structure. A choice of basis (or choices of bases) links the abstract view to a particular representation. When working with an abstract inner product space, we often would like to choose an orthonormal basis, so that the inner product in the abstract space corresponds to the standard dot product in Rn or Cn. Otherwise, the choice of basis may be arbitrary in principle | though, of course, some bases are particularly useful for revealing the structure of the operation. For any given class of linear algebraic operations, we have equivalence classes of matrices that represent the operation under different choices of bases. It is useful to choose a distinguished representative for each of these equivalence classes, corresponding to a choice of basis that renders the struc- ture of the operation particularly clear. These distinguished representatives are known as canonical forms. Many of these equivalence relations have special names, as do many of the canonical forms. For spaces without and with inner product structure, the equivalence relations and canonical forms associated with an operation on V of dimension n and W of dimension n are shown in Figure1. A major theme in the analysis of the Hermitian eigenvalue problem follows from a pun: in the Hermitian case in an inner product space, the equivalence relation for operators (unitary similarity) and for quadratic forms (unitary congruence) are the same thing!.
    [Show full text]
  • 3 Properties of Kernels
    3 Properties of kernels As we have seen in Chapter 2, the use of kernel functions provides a powerful and principled way of detecting nonlinear relations using well-understood linear algorithms in an appropriate feature space. The approach decouples the design of the algorithm from the specification of the feature space. This inherent modularity not only increases the flexibility of the approach, it also makes both the learning algorithms and the kernel design more amenable to formal analysis. Regardless of which pattern analysis algorithm is being used, the theoretical properties of a given kernel remain the same. It is the purpose of this chapter to introduce the properties that characterise kernel functions. We present the fundamental properties of kernels, thus formalising the intuitive concepts introduced in Chapter 2. We provide a characterization of kernel functions, derive their properties, and discuss methods for design- ing them. We will also discuss the role of prior knowledge in kernel-based learning machines, showing that a universal machine is not possible, and that kernels must be chosen for the problem at hand with a view to captur- ing our prior belief of the relatedness of different examples. We also give a framework for quantifying the match between a kernel and a learning task. Given a kernel and a training set, we can form the matrix known as the kernel, or Gram matrix: the matrix containing the evaluation of the kernel function on all pairs of data points. This matrix acts as an information bottleneck, as all the information available to a kernel algorithm, be it about the distribution, the model or the noise, must be extracted from that matrix.
    [Show full text]
  • 8 Norms and Inner Products
    8 Norms and Inner products This section is devoted to vector spaces with an additional structure - inner product. The underlining field here is either F = IR or F = C|| . 8.1 Definition (Norm, distance) A norm on a vector space V is a real valued function k · k satisfying 1. kvk ≥ 0 for all v ∈ V and kvk = 0 if and only if v = 0. 2. kcvk = |c| kvk for all c ∈ F and v ∈ V . 3. ku + vk ≤ kuk + kvk for all u, v ∈ V (triangle inequality). A vector space V = (V, k · k) together with a norm is called a normed space. In normed spaces, we define the distance between two vectors u, v by d(u, v) = ku−vk. Note that property 3 has a useful implication: kuk − kvk ≤ ku − vk for all u, v ∈ V . 8.2 Examples (i) Several standard norms in IRn and C|| n: n X kxk1 := |xi| (1 − norm) i=1 n !1/2 X 2 kxk2 := |xi| (2 − norm) i=1 note that this is Euclidean norm, n !1/p X p kxkp := |xi| (p − norm) i=1 for any real p ∈ [1, ∞), kxk∞ := max |xi| (∞ − norm) 1≤i≤n (ii) Several standard norms in C[a, b] for any a < b: Z b kfk1 := |f(x)| dx a Z b !1/2 2 kfk2 := |f(x)| dx a kfk∞ := max |f(x)| a≤x≤b 1 8.3 Definition (Unit sphere, Unit ball) Let k · k be a norm on V . The set S1 = {v ∈ V : kvk = 1} is called a unit sphere in V , and the set B1 = {v ∈ V : kvk ≤ 1} a unit ball (with respect to the norm k · k).
    [Show full text]
  • The Rayleigh Quotient Iteration and Some Generalizations for Nonnormal Matrices*
    MATHEMATICS OF COMPUTATION, VOLUME 28, NUMBER 127, JULY 1974, PAGES 679-693 The Rayleigh Quotient Iteration and Some Generalizations for Nonnormal Matrices* By B. N. Parlett Abstract. The Rayleigh Quotient Iteration (RQI) was developed for real symmetric matrices. Its rapid local convergence is due to the stationarity of the Rayleigh Quotient at an eigenvector. Its excellent global properties are due to the monotonie decrease in the norms of the residuals. These facts are established for normal matrices. Both properties fail for nonnormal matrices and no generalization of the iteration has recaptured both of them. We examine methods which employ either one or the other of them. 1. History. In the 1870's John William Strutt (third Baron Rayleigh) began his mammoth work on the theory of sound. Basic to many of his studies were the small oscillations of a vibrating system about a position of equilibrium. In terms of suitable generalized coordinates, any set of small displacements (the state of the system) will be represented by a vector q with time derivative q. The potential energy V and the kinetic energy T at each instant t are represented by the two quadratic forms V = i (Mq,q) = \q*Mq, T = £ {Hq,q) = \q*Kq, where M and H are suitable symmetric positive definite matrices, constant in time, and q* denotes the transpose of q. Of principal interest are the smallest natural frequencies w and their corresponding natural modes which can be expressed in the generalized coordinates in the form exp(i«r)x where x is a constant vector (the mode shape) which satisfies (M-o,2H)x=0.
    [Show full text]
  • Eigenvalue Problems
    Eigenvalue Problems Eigenvalue Problems Existence, Uniqueness, and Conditioning Existence, Uniqueness, and Conditioning Computing Eigenvalues and Eigenvectors Computing Eigenvalues and Eigenvectors Outline Scientific Computing: An Introductory Survey Chapter 4 – Eigenvalue Problems 1 Eigenvalue Problems Prof. Michael T. Heath 2 Existence, Uniqueness, and Conditioning Department of Computer Science University of Illinois at Urbana-Champaign 3 Computing Eigenvalues and Eigenvectors Copyright c 2002. Reproduction permitted for noncommercial, educational use only. Michael T. Heath Scientific Computing 1 / 87 Michael T. Heath Scientific Computing 2 / 87 Eigenvalue Problems Eigenvalue Problems Eigenvalue Problems Eigenvalue Problems Existence, Uniqueness, and Conditioning Eigenvalues and Eigenvectors Existence, Uniqueness, and Conditioning Eigenvalues and Eigenvectors Computing Eigenvalues and Eigenvectors Geometric Interpretation Computing Eigenvalues and Eigenvectors Geometric Interpretation Eigenvalue Problems Eigenvalues and Eigenvectors Eigenvalue problems occur in many areas of science and Standard eigenvalue problem : Given n × n matrix A, find engineering, such as structural analysis scalar λ and nonzero vector x such that Eigenvalues are also important in analyzing numerical A x = λ x methods λ is eigenvalue, and x is corresponding eigenvector Theory and algorithms apply to complex matrices as well as real matrices λ may be complex even if A is real With complex matrices, we use conjugate transpose, AH , Spectrum = λ(A) = set of eigenvalues
    [Show full text]