Radial Basis Functions I

Size: px
Start display at page:

Download "Radial Basis Functions I"

Transcription

1 Radial Basis Functions I Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo November 14, 2008

2 Today Reformulation of natural cubic spline interpolation Scattered data interpolation with RBF s Franke s example using Gaussian Non-singularity via nonnegative Fourier Transform RBF interpolation with polynomial precision Positive definite matrices on a subspace.

3 Cubic Splines Given a < b and x = [x 0,..., x N+1 ] with a =: x 0 < x 1 < < x N < x N+1 := b. Cubic Splines: S 2 3(x) := {g C 2 [a, b] : g (xj,x j+1 ) Π 3, for j = 0,..., N Π d := span{x k : 0 k d} polynomials of degree d. Unique representation of g S 2 3 in terms of truncated powers x 3 + := max{x 3, 0}. x 3 + C 2 (R). g(x) = N k=1 c k(x x k ) k=0 a kx k, x [a, b]. S 2 3(x) is a linear space of functions of dimension N + 4.

4 Natural Cubic Splines NS 2 3(x) := {g S 2 3(x) : g (a,x1 ), g (xn,b) Π 1}. Truncated power representation g NS 2 3(x) g(x) = N k=1 c k(x x k ) a 0 + a 1 x, x [a, b], N k=1 c k = 0, N k=1 c kx k = 0. Proof Choosing x (a, x 1 ) shows that a 2 = a 3 = 0 in the truncated power representation. Choosing x (x N, b) shows the orthogonality conditions. remove + s: g(x) = N k=1 c k(x x k ) 3 + a 0 + a 1 x, x (x N, b). Expand (x xk ) 3 = x 3 3x k x 2 + 3xk 2x x k 3 Expanded Sum: k c k(x x k ) 3 = x 3 k c k 3( k c kx k )x 2 + 3( k c kxk 2)x ( k c kxk 3).

5 Radial basis function representation truncated power representation: g NS 2 3(x) g(x) = N k=1 c k(x x k ) a 0 + a 1 x, x [a, b], N k=1 c k = 0, N k=1 c kx k = 0. Replace x+ 3 by 1 2 ( x 3 + x 3 ) in truncated power representation. g(x) = 1 N 2 k=1 c k x x k N 2 k=1 c k(x x k ) 3 + a 0 + a 1 x, x [a, b], g(x) = 1 N 2 k=1 c k x x k 3 + 3( N 2 k=1 c kxk 2)x 1 ( N 2 k=1 c kxk 3) + a 0 + a 1 x, x [a, b], radial basis function representation g(x) = N k=1 c k x x k 3 + d 0 + d 1 x, x [a, b], N k=1 c k = 0, N k=1 c kx k = 0.

6 Natural cubic spline interpolation in a radial basis formulation Find P f NS 2 3(x) such that P f (x j ) = f j, j = 1,..., N. N k=1 c kϕ( x j x k ) + d 0 + d 1 x j = f j, j = 1,..., N k c k = 0, k c kx k = 0. Matrix form [ ] [ ] A B T c = B 0 d N + 2 equations in N + 2 unknowns. [ ] [ ] f 1 1, A = [ϕ( x 0 j x k )], B =. x 1 x N

7 Radial Function in R s Definition Let s N and a norm on R s. A function Φ : R s R is called radial if Φ(x) = ϕ( x ), x R s, for some univariate function ϕ : [0, ) R. The norm is often the Euclidian norm 2. = 2 when nothing else is said. Radial: Φ(x) = ϕ(r) for all x with x = r.

8 Gaussian, ϕ(r) = e ε2 r 2, ε = 2, Φ(x) = ϕ( x ) = e ε2 x 2

9 Distance, ϕ(r) = r Φ(x) = ϕ( x ) = x 2 + y 2

10 Thin Plate,ϕ(r) = r 2 log r Φ(x) = ϕ( x ) = 1 2 (x 2 + y 2 ) log(x 2 + y 2 ). 4 Φ(x) = 0.

11 RBF Interpolation without polynomial precision Given N, s N and distinct points x 1,..., x N R s, ordinate-values f j = f (x j ) representing an unknown function f. A radial function Φ : R s R given by Φ(x) = ϕ( x ) Linear combinations P f (x) := N k=1 c KΦ(x x k ) Find c = [c 1,..., c N ] such that P f (x j ) := N c k Φ(x j x k ) = f j, k=1 j = 1,..., N Matrix Problem Ac = f, where A = [ϕ( x j x k )] R N,N, f = [f 1,..., f N ] T.

12 N = 2 [ ] ϕ( x1 x A = 1 ) ϕ( x 1 x 2 ). ϕ( x 2 x 1 ) ϕ( x 2 x 2 ) ϕ(r) = e ε2 r 2, A = [ ] 1 a, a = e a 1 ε2 x 1 x 2 2 < 1 if ε 0. A is symmetric and positive definite. (Positive eigenvalues by Gerschgorin or strict diagonal dominance). [ ] 0 b ϕ(r) = r, A =, b = x b 0 1 x 2. A is symmetric with one positive and one negative eigenvalue. Nonsingular, but indefinite. Same for thin plate

13 Franke s test function

14 Franke s test function f (x, y) :=0.75 Exp ( ((9 x 2) 2 + (9 y 2) 2 )/4 ) Exp ( ((9 x + 1) 2 /49 + (9 y + 1) 2 /10) ) + Exp ( ((9 x 7) 2 + (9 y 3) 2 )/4 ) 0.2 Exp ( ((9 x 4) 2 + (9 y 7) 2 ) )

15 Halton Points x 1,..., x N uniformly distributed points in (0, 1) s. can be downloaded by searching for haltonseq.m Halton Points in R 2

16 Gaussian Example Φ(x) = e ε2 x 2, ε = (left) and 1089 right) Halton Points f sampled from Franke s test function. Matlab program RBFInterpolation2D.m by Fasshauer RBF interpolant false colored by maximum error. RBF interpolant false colored by maximum error Error Error

17 Discussion Dense linear system Non-singular? Extremely ill-conditioned for ε not large. Polynomials of low degree not reproduced. But.. Can work for scattered data in high space dimension without triangulating the data.

18 Non-singularity via Fourier Transform Definition For a function f L 1 (R s ) we define the (symmetric) Fourier transform of f by ˆf (ω) := 1 (2π) s/2 R s f (x)e iω x dx, ω R s. (1) and the inverse Fourier transform 1 f (x) = ˆf (ω)e iω x dω, (2π) s/2 R s x R s. (2) Φ(x) := e ε2 x 2 ˆΦ(ω) := e ω 2 /(4ε 2) 0.

19 Non-negative Fourier transform Theorem Let Φ(x) = ϕ( x ) be a radial function with nonnegative Fourier transform not identically zero. For any distinct points x 1,..., x N the matrix is positive definite. A := [ϕ( x j x k )] R N,N,

20 Proof c T Ac = N j=1 N c j c k Φ(x j x k ) k=1 1 = c (2π) s/2 j c k ˆΦ(ω)e j,k R iω (x j x k ) dω s 1 ( ) = cj e iω x j c (2π) s/2 k e iω x k ˆΦ(ω)dω = 1 (2π) s/2 R s j,k R s j c j e iω x j 2 ˆΦ(ω)dω 0. Equality j c j e iω x j = 0, ω R s, c = 0.

21 Discussion The Fourier transform can be used for some other examples. But, The distance function and thin plate and other examples are not integrable so do not have a Fourier transform Can use nonnegativity of the generalized Fourier transform. We will instead look at the connection between positive definite matrices and completely monotone functions.

22 Polynomial reproduction Gaussian, distance and thin plate do not reproduce polynomials can add terms to achieve this. Example x = (x, y) R 2, add 1, x, y to reproduce linear polynomials P f (x) := N k=1 c kϕ( x x k ) + d 1 + d 2 x + d 3 y, need 3 extra conditions k c k = 0, k c kx k = 0, k c ky k = 0

23 Linear system N k=1 c kϕ( x j x k ) + d 1 + d 2 x j + d 3 y j = f j, j = 1,..., N k c k = 0, k c kx k = 0, k c ky k = 0 [ A B T B 0 ] [ ] c = d [ ] f, A = [ϕ( x 0 j x k )], B T = S 1 := {c R N : Bc = 0}, is a subspace of R N. 1 x 1 y x N y N

24 Positive definite on a subspace Definition Suppose A R N,N and S a subspace of R N. We say that A is positive definite on S if A T = A and c T Ac > 0 for all nonzero c S. If A is positive definite on S = ker(b) := {c R N : Bc = 0} and B R M,N has linearly independent rows then the block matrix [ ] A B T is nonsingular. B 0

25 Proof [ A B T B 0 ] [ ] c = 0 Ac + BT d = 0 d Bc = 0 ct Ac + c T B T d = 0 c T B T = 0. So c = 0 and then d = 0 since 0 = Ac + B T d = B T d and B has linearly independent rows.

26 Positive and negative eigenvalues Theorem If A R N,N is positive definite on the subspace S := {c R N : k c k = 0} and i a ii 0, then A has N 1 positive eigenvalues and one negative eigenvalue. Proof S is a subspace of R N of dimension N 1. Since A is symmetric it has real eigenvalues. Let λ 1 λ 2 λ N be the eigenvalues of A. Recall Courant-Fischer s characterization In particular λ k = max min c T Ac. dim T =k c T c =1 λ N 1 min c T Ac > 0. c S c =1 But i λ i = i a ii 0 so λ N < 0.

27 Non-singularity without polynomial precision Corollary Let Φ(x) := ϕ( x ) be a radial function. If A = [ϕ( x j x k )] R N,N is positive definite on the subspace S := {c R N : k c k = 0} and ϕ(0) = 0 then A is non-singular with N 1 positive eigenvalues and one negative eigenvalue. Proof. This follows immediately from the previous theorem.

28 Distance matrix ϕ(r) = r, Φ(x) = ϕ( x ) = x. A = [ x j x k ] and a jj = x j x j = 0, j = 1,..., N since ϕ(0) = 0 so j a jj 0. We show next time that A is positive definite on S := {c R N : k c k = 0}. It will then follow that the distance matrix is non-singular with N 1 positive and one negative eigenvalue.

Least Squares. Tom Lyche. October 26, Centre of Mathematics for Applications, Department of Informatics, University of Oslo

Least Squares. Tom Lyche. October 26, Centre of Mathematics for Applications, Department of Informatics, University of Oslo Least Squares Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo October 26, 2010 Linear system Linear system Ax = b, A C m,n, b C m, x C n. under-determined

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 9: Conditionally Positive Definite Radial Functions Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH

More information

Scattered Data Interpolation with Polynomial Precision and Conditionally Positive Definite Functions

Scattered Data Interpolation with Polynomial Precision and Conditionally Positive Definite Functions Chapter 3 Scattered Data Interpolation with Polynomial Precision and Conditionally Positive Definite Functions 3.1 Scattered Data Interpolation with Polynomial Precision Sometimes the assumption on the

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 34: Improving the Condition Number of the Interpolation Matrix Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu

More information

Lecture 1 INF-MAT3350/ : Some Tridiagonal Matrix Problems

Lecture 1 INF-MAT3350/ : Some Tridiagonal Matrix Problems Lecture 1 INF-MAT3350/4350 2007: Some Tridiagonal Matrix Problems Tom Lyche University of Oslo Norway Lecture 1 INF-MAT3350/4350 2007: Some Tridiagonal Matrix Problems p.1/33 Plan for the day 1. Notation

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 33: Adaptive Iteration Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH 590 Chapter 33 1 Outline 1 A

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 33: Adaptive Iteration Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH 590 Chapter 33 1 Outline 1 A

More information

Orthogonal Transformations

Orthogonal Transformations Orthogonal Transformations Tom Lyche University of Oslo Norway Orthogonal Transformations p. 1/3 Applications of Qx with Q T Q = I 1. solving least squares problems (today) 2. solving linear equations

More information

The Singular Value Decomposition and Least Squares Problems

The Singular Value Decomposition and Least Squares Problems The Singular Value Decomposition and Least Squares Problems Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo September 27, 2009 Applications of SVD solving

More information

Orthonormal Transformations and Least Squares

Orthonormal Transformations and Least Squares Orthonormal Transformations and Least Squares Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo October 30, 2009 Applications of Qx with Q T Q = I 1. solving

More information

Kernel B Splines and Interpolation

Kernel B Splines and Interpolation Kernel B Splines and Interpolation M. Bozzini, L. Lenarduzzi and R. Schaback February 6, 5 Abstract This paper applies divided differences to conditionally positive definite kernels in order to generate

More information

Lecture 1 INF-MAT : Chapter 2. Examples of Linear Systems

Lecture 1 INF-MAT : Chapter 2. Examples of Linear Systems Lecture 1 INF-MAT 4350 2010: Chapter 2. Examples of Linear Systems Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo August 26, 2010 Notation The set of natural

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 2 Part 3: Native Space for Positive Definite Kernels Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2014 fasshauer@iit.edu MATH

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 2: Radial Basis Function Interpolation in MATLAB Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH 590

More information

Chapter 3 Transformations

Chapter 3 Transformations Chapter 3 Transformations An Introduction to Optimization Spring, 2014 Wei-Ta Chu 1 Linear Transformations A function is called a linear transformation if 1. for every and 2. for every If we fix the bases

More information

1. Select the unique answer (choice) for each problem. Write only the answer.

1. Select the unique answer (choice) for each problem. Write only the answer. MATH 5 Practice Problem Set Spring 7. Select the unique answer (choice) for each problem. Write only the answer. () Determine all the values of a for which the system has infinitely many solutions: x +

More information

Orthonormal Transformations

Orthonormal Transformations Orthonormal Transformations Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo October 25, 2010 Applications of transformation Q : R m R m, with Q T Q = I 1.

More information

Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm

Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo November 13, 2009 Today

More information

Lecture Notes for Inf-Mat 3350/4350, Tom Lyche

Lecture Notes for Inf-Mat 3350/4350, Tom Lyche Lecture Notes for Inf-Mat 3350/4350, 2007 Tom Lyche August 5, 2007 2 Contents Preface vii I A Review of Linear Algebra 1 1 Introduction 3 1.1 Notation............................... 3 2 Vectors 5 2.1 Vector

More information

Linear Algebra Massoud Malek

Linear Algebra Massoud Malek CSUEB Linear Algebra Massoud Malek Inner Product and Normed Space In all that follows, the n n identity matrix is denoted by I n, the n n zero matrix by Z n, and the zero vector by θ n An inner product

More information

Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices

Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo November 8, 2009 Today

More information

Inner products. Theorem (basic properties): Given vectors u, v, w in an inner product space V, and a scalar k, the following properties hold:

Inner products. Theorem (basic properties): Given vectors u, v, w in an inner product space V, and a scalar k, the following properties hold: Inner products Definition: An inner product on a real vector space V is an operation (function) that assigns to each pair of vectors ( u, v) in V a scalar u, v satisfying the following axioms: 1. u, v

More information

Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm

Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm Computing Eigenvalues and/or Eigenvectors;Part 2, The Power method and QR-algorithm Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo November 19, 2010 Today

More information

Kernel Method: Data Analysis with Positive Definite Kernels

Kernel Method: Data Analysis with Positive Definite Kernels Kernel Method: Data Analysis with Positive Definite Kernels 2. Positive Definite Kernel and Reproducing Kernel Hilbert Space Kenji Fukumizu The Institute of Statistical Mathematics. Graduate University

More information

Compensation. June 29, Arizona State University. Edge Detection from Nonuniform Data via. Convolutional Gridding with Density.

Compensation. June 29, Arizona State University. Edge Detection from Nonuniform Data via. Convolutional Gridding with Density. Arizona State University June 29, 2012 Overview gridding with density compensation is a common method for function reconstruction nonuniform Fourier data. It is computationally inexpensive compared with

More information

Lecture 2 INF-MAT : , LU, symmetric LU, Positve (semi)definite, Cholesky, Semi-Cholesky

Lecture 2 INF-MAT : , LU, symmetric LU, Positve (semi)definite, Cholesky, Semi-Cholesky Lecture 2 INF-MAT 4350 2009: 7.1-7.6, LU, symmetric LU, Positve (semi)definite, Cholesky, Semi-Cholesky Tom Lyche and Michael Floater Centre of Mathematics for Applications, Department of Informatics,

More information

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics MATH M Test #1. July 11, 2013 Solutions

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics MATH M Test #1. July 11, 2013 Solutions YORK UNIVERSITY Faculty of Science Department of Mathematics and Statistics MATH 222 3. M Test # July, 23 Solutions. For each statement indicate whether it is always TRUE or sometimes FALSE. Note: For

More information

Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices

Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices Computing Eigenvalues and/or Eigenvectors;Part 1, Generalities and symmetric matrices Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo November 9, 2008 Today

More information

A Field Extension as a Vector Space

A Field Extension as a Vector Space Chapter 8 A Field Extension as a Vector Space In this chapter, we take a closer look at a finite extension from the point of view that is a vector space over. It is clear, for instance, that any is a linear

More information

A new stable basis for radial basis function interpolation

A new stable basis for radial basis function interpolation A new stable basis for radial basis function interpolation Stefano De Marchi and Gabriele Santin Department of Mathematics University of Padua (Italy) Abstract It is well-known that radial basis function

More information

RKHS, Mercer s theorem, Unbounded domains, Frames and Wavelets Class 22, 2004 Tomaso Poggio and Sayan Mukherjee

RKHS, Mercer s theorem, Unbounded domains, Frames and Wavelets Class 22, 2004 Tomaso Poggio and Sayan Mukherjee RKHS, Mercer s theorem, Unbounded domains, Frames and Wavelets 9.520 Class 22, 2004 Tomaso Poggio and Sayan Mukherjee About this class Goal To introduce an alternate perspective of RKHS via integral operators

More information

x x2 2 + x3 3 x4 3. Use the divided-difference method to find a polynomial of least degree that fits the values shown: (b)

x x2 2 + x3 3 x4 3. Use the divided-difference method to find a polynomial of least degree that fits the values shown: (b) Numerical Methods - PROBLEMS. The Taylor series, about the origin, for log( + x) is x x2 2 + x3 3 x4 4 + Find an upper bound on the magnitude of the truncation error on the interval x.5 when log( + x)

More information

Numerical Methods I Solving Square Linear Systems: GEM and LU factorization

Numerical Methods I Solving Square Linear Systems: GEM and LU factorization Numerical Methods I Solving Square Linear Systems: GEM and LU factorization Aleksandar Donev Courant Institute, NYU 1 donev@courant.nyu.edu 1 MATH-GA 2011.003 / CSCI-GA 2945.003, Fall 2014 September 18th,

More information

Applied Linear Algebra in Geoscience Using MATLAB

Applied Linear Algebra in Geoscience Using MATLAB Applied Linear Algebra in Geoscience Using MATLAB Contents Getting Started Creating Arrays Mathematical Operations with Arrays Using Script Files and Managing Data Two-Dimensional Plots Programming in

More information

DS-GA 1002 Lecture notes 10 November 23, Linear models

DS-GA 1002 Lecture notes 10 November 23, Linear models DS-GA 2 Lecture notes November 23, 2 Linear functions Linear models A linear model encodes the assumption that two quantities are linearly related. Mathematically, this is characterized using linear functions.

More information

D. Shepard, Shepard functions, late 1960s (application, surface modelling)

D. Shepard, Shepard functions, late 1960s (application, surface modelling) Chapter 1 Introduction 1.1 History and Outline Originally, the motivation for the basic meshfree approximation methods (radial basis functions and moving least squares methods) came from applications in

More information

Lecture 2 INF-MAT : A boundary value problem and an eigenvalue problem; Block Multiplication; Tridiagonal Systems

Lecture 2 INF-MAT : A boundary value problem and an eigenvalue problem; Block Multiplication; Tridiagonal Systems Lecture 2 INF-MAT 4350 2008: A boundary value problem and an eigenvalue problem; Block Multiplication; Tridiagonal Systems Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University

More information

Solutions for Math 225 Assignment #5 1

Solutions for Math 225 Assignment #5 1 Solutions for Math 225 Assignment #5 1 (1) Find a polynomial f(x) of degree at most 3 satisfying that f(0) = 2, f( 1) = 1, f(1) = 3 and f(3) = 1. Solution. By Lagrange Interpolation, ( ) (x + 1)(x 1)(x

More information

Lecture 22: Section 4.7

Lecture 22: Section 4.7 Lecture 22: Section 47 Shuanglin Shao December 2, 213 Row Space, Column Space, and Null Space Definition For an m n, a 11 a 12 a 1n a 21 a 22 a 2n A = a m1 a m2 a mn, the vectors r 1 = [ a 11 a 12 a 1n

More information

MATH 2331 Linear Algebra. Section 2.1 Matrix Operations. Definition: A : m n, B : n p. Example: Compute AB, if possible.

MATH 2331 Linear Algebra. Section 2.1 Matrix Operations. Definition: A : m n, B : n p. Example: Compute AB, if possible. MATH 2331 Linear Algebra Section 2.1 Matrix Operations Definition: A : m n, B : n p ( 1 2 p ) ( 1 2 p ) AB = A b b b = Ab Ab Ab Example: Compute AB, if possible. 1 Row-column rule: i-j-th entry of AB:

More information

Here each term has degree 2 (the sum of exponents is 2 for all summands). A quadratic form of three variables looks as

Here each term has degree 2 (the sum of exponents is 2 for all summands). A quadratic form of three variables looks as Reading [SB], Ch. 16.1-16.3, p. 375-393 1 Quadratic Forms A quadratic function f : R R has the form f(x) = a x. Generalization of this notion to two variables is the quadratic form Q(x 1, x ) = a 11 x

More information

Lecture 15 Review of Matrix Theory III. Dr. Radhakant Padhi Asst. Professor Dept. of Aerospace Engineering Indian Institute of Science - Bangalore

Lecture 15 Review of Matrix Theory III. Dr. Radhakant Padhi Asst. Professor Dept. of Aerospace Engineering Indian Institute of Science - Bangalore Lecture 15 Review of Matrix Theory III Dr. Radhakant Padhi Asst. Professor Dept. of Aerospace Engineering Indian Institute of Science - Bangalore Matrix An m n matrix is a rectangular or square array of

More information

Scientific Computing: Dense Linear Systems

Scientific Computing: Dense Linear Systems Scientific Computing: Dense Linear Systems Aleksandar Donev Courant Institute, NYU 1 donev@courant.nyu.edu 1 Course MATH-GA.2043 or CSCI-GA.2112, Spring 2012 February 9th, 2012 A. Donev (Courant Institute)

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 1 Part 3: Radial Basis Function Interpolation in MATLAB Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2014 fasshauer@iit.edu

More information

University of Houston, Department of Mathematics Numerical Analysis, Fall 2005

University of Houston, Department of Mathematics Numerical Analysis, Fall 2005 4 Interpolation 4.1 Polynomial interpolation Problem: LetP n (I), n ln, I := [a,b] lr, be the linear space of polynomials of degree n on I, P n (I) := { p n : I lr p n (x) = n i=0 a i x i, a i lr, 0 i

More information

MAT Linear Algebra Collection of sample exams

MAT Linear Algebra Collection of sample exams MAT 342 - Linear Algebra Collection of sample exams A-x. (0 pts Give the precise definition of the row echelon form. 2. ( 0 pts After performing row reductions on the augmented matrix for a certain system

More information

Chapter 4 Euclid Space

Chapter 4 Euclid Space Chapter 4 Euclid Space Inner Product Spaces Definition.. Let V be a real vector space over IR. A real inner product on V is a real valued function on V V, denoted by (, ), which satisfies () (x, y) = (y,

More information

LECTURE NOTES ELEMENTARY NUMERICAL METHODS. Eusebius Doedel

LECTURE NOTES ELEMENTARY NUMERICAL METHODS. Eusebius Doedel LECTURE NOTES on ELEMENTARY NUMERICAL METHODS Eusebius Doedel TABLE OF CONTENTS Vector and Matrix Norms 1 Banach Lemma 20 The Numerical Solution of Linear Systems 25 Gauss Elimination 25 Operation Count

More information

Chap 3. Linear Algebra

Chap 3. Linear Algebra Chap 3. Linear Algebra Outlines 1. Introduction 2. Basis, Representation, and Orthonormalization 3. Linear Algebraic Equations 4. Similarity Transformation 5. Diagonal Form and Jordan Form 6. Functions

More information

1. What is the determinant of the following matrix? a 1 a 2 4a 3 2a 2 b 1 b 2 4b 3 2b c 1. = 4, then det

1. What is the determinant of the following matrix? a 1 a 2 4a 3 2a 2 b 1 b 2 4b 3 2b c 1. = 4, then det What is the determinant of the following matrix? 3 4 3 4 3 4 4 3 A 0 B 8 C 55 D 0 E 60 If det a a a 3 b b b 3 c c c 3 = 4, then det a a 4a 3 a b b 4b 3 b c c c 3 c = A 8 B 6 C 4 D E 3 Let A be an n n matrix

More information

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )

More information

12. Cholesky factorization

12. Cholesky factorization L. Vandenberghe ECE133A (Winter 2018) 12. Cholesky factorization positive definite matrices examples Cholesky factorization complex positive definite matrices kernel methods 12-1 Definitions a symmetric

More information

Recall the convention that, for us, all vectors are column vectors.

Recall the convention that, for us, all vectors are column vectors. Some linear algebra Recall the convention that, for us, all vectors are column vectors. 1. Symmetric matrices Let A be a real matrix. Recall that a complex number λ is an eigenvalue of A if there exists

More information

Linear Algebra Practice Problems

Linear Algebra Practice Problems Linear Algebra Practice Problems Math 24 Calculus III Summer 25, Session II. Determine whether the given set is a vector space. If not, give at least one axiom that is not satisfied. Unless otherwise stated,

More information

Cheat Sheet for MATH461

Cheat Sheet for MATH461 Cheat Sheet for MATH46 Here is the stuff you really need to remember for the exams Linear systems Ax = b Problem: We consider a linear system of m equations for n unknowns x,,x n : For a given matrix A

More information

Basic Concepts in Linear Algebra

Basic Concepts in Linear Algebra Basic Concepts in Linear Algebra Grady B Wright Department of Mathematics Boise State University February 2, 2015 Grady B Wright Linear Algebra Basics February 2, 2015 1 / 39 Numerical Linear Algebra Linear

More information

Chapter 7 Iterative Techniques in Matrix Algebra

Chapter 7 Iterative Techniques in Matrix Algebra Chapter 7 Iterative Techniques in Matrix Algebra Per-Olof Persson persson@berkeley.edu Department of Mathematics University of California, Berkeley Math 128B Numerical Analysis Vector Norms Definition

More information

Scalable kernel methods and their use in black-box optimization

Scalable kernel methods and their use in black-box optimization with derivatives Scalable kernel methods and their use in black-box optimization David Eriksson Center for Applied Mathematics Cornell University dme65@cornell.edu November 9, 2018 1 2 3 4 1/37 with derivatives

More information

Approximation by Conditionally Positive Definite Functions with Finitely Many Centers

Approximation by Conditionally Positive Definite Functions with Finitely Many Centers Approximation by Conditionally Positive Definite Functions with Finitely Many Centers Jungho Yoon Abstract. The theory of interpolation by using conditionally positive definite function provides optimal

More information

Review of Basic Concepts in Linear Algebra

Review of Basic Concepts in Linear Algebra Review of Basic Concepts in Linear Algebra Grady B Wright Department of Mathematics Boise State University September 7, 2017 Math 565 Linear Algebra Review September 7, 2017 1 / 40 Numerical Linear Algebra

More information

Linear Algebra. Session 8

Linear Algebra. Session 8 Linear Algebra. Session 8 Dr. Marco A Roque Sol 08/01/2017 Abstract Linear Algebra Range and kernel Let V, W be vector spaces and L : V W, be a linear mapping. Definition. The range (or image of L is the

More information

13-2 Text: 28-30; AB: 1.3.3, 3.2.3, 3.4.2, 3.5, 3.6.2; GvL Eigen2

13-2 Text: 28-30; AB: 1.3.3, 3.2.3, 3.4.2, 3.5, 3.6.2; GvL Eigen2 The QR algorithm The most common method for solving small (dense) eigenvalue problems. The basic algorithm: QR without shifts 1. Until Convergence Do: 2. Compute the QR factorization A = QR 3. Set A :=

More information

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics MATH M Test #2 Solutions

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics MATH M Test #2 Solutions YORK UNIVERSITY Faculty of Science Department of Mathematics and Statistics MATH 3. M Test # Solutions. (8 pts) For each statement indicate whether it is always TRUE or sometimes FALSE. Note: For this

More information

ACM106a - Homework 2 Solutions

ACM106a - Homework 2 Solutions ACM06a - Homework 2 Solutions prepared by Svitlana Vyetrenko October 7, 2006. Chapter 2, problem 2.2 (solution adapted from Golub, Van Loan, pp.52-54): For the proof we will use the fact that if A C m

More information

Math 240 Calculus III

Math 240 Calculus III The Calculus III Summer 2015, Session II Wednesday, July 8, 2015 Agenda 1. of the determinant 2. determinants 3. of determinants What is the determinant? Yesterday: Ax = b has a unique solution when A

More information

Preliminary/Qualifying Exam in Numerical Analysis (Math 502a) Spring 2012

Preliminary/Qualifying Exam in Numerical Analysis (Math 502a) Spring 2012 Instructions Preliminary/Qualifying Exam in Numerical Analysis (Math 502a) Spring 2012 The exam consists of four problems, each having multiple parts. You should attempt to solve all four problems. 1.

More information

Wavelet Bi-frames with Uniform Symmetry for Curve Multiresolution Processing

Wavelet Bi-frames with Uniform Symmetry for Curve Multiresolution Processing Wavelet Bi-frames with Uniform Symmetry for Curve Multiresolution Processing Qingtang Jiang Abstract This paper is about the construction of univariate wavelet bi-frames with each framelet being symmetric.

More information

D. Shepard, Shepard functions, late 1960s (application, surface modelling)

D. Shepard, Shepard functions, late 1960s (application, surface modelling) Chapter 1 Introduction 1.1 History and Outline Originally, the motivation for the basic meshfree approximation methods (radial basis functions and moving least squares methods) came from applications in

More information

Lecture4 INF-MAT : 5. Fast Direct Solution of Large Linear Systems

Lecture4 INF-MAT : 5. Fast Direct Solution of Large Linear Systems Lecture4 INF-MAT 4350 2010: 5. Fast Direct Solution of Large Linear Systems Tom Lyche Centre of Mathematics for Applications, Department of Informatics, University of Oslo September 16, 2010 Test Matrix

More information

AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES

AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES JOEL A. TROPP Abstract. We present an elementary proof that the spectral radius of a matrix A may be obtained using the formula ρ(a) lim

More information

Spring, 2012 CIS 515. Fundamentals of Linear Algebra and Optimization Jean Gallier

Spring, 2012 CIS 515. Fundamentals of Linear Algebra and Optimization Jean Gallier Spring 0 CIS 55 Fundamentals of Linear Algebra and Optimization Jean Gallier Homework 5 & 6 + Project 3 & 4 Note: Problems B and B6 are for extra credit April 7 0; Due May 7 0 Problem B (0 pts) Let A be

More information

Linear Systems of n equations for n unknowns

Linear Systems of n equations for n unknowns Linear Systems of n equations for n unknowns In many application problems we want to find n unknowns, and we have n linear equations Example: Find x,x,x such that the following three equations hold: x

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 6: Scattered Data Interpolation with Polynomial Precision Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 7: Conditionally Positive Definite Functions Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH 590 Chapter

More information

Radial basis functions topics in slides

Radial basis functions topics in slides Radial basis functions topics in 40 +1 slides Stefano De Marchi Department of Mathematics Tullio Levi-Civita University of Padova Napoli, 22nd March 2018 Outline 1 From splines to RBF 2 Error estimates,

More information

Algebra C Numerical Linear Algebra Sample Exam Problems

Algebra C Numerical Linear Algebra Sample Exam Problems Algebra C Numerical Linear Algebra Sample Exam Problems Notation. Denote by V a finite-dimensional Hilbert space with inner product (, ) and corresponding norm. The abbreviation SPD is used for symmetric

More information

Math 577 Assignment 7

Math 577 Assignment 7 Math 577 Assignment 7 Thanks for Yu Cao 1. Solution. The linear system being solved is Ax = 0, where A is a (n 1 (n 1 matrix such that 2 1 1 2 1 A =......... 1 2 1 1 2 and x = (U 1, U 2,, U n 1. By the

More information

Chapter 6: Orthogonality

Chapter 6: Orthogonality Chapter 6: Orthogonality (Last Updated: November 7, 7) These notes are derived primarily from Linear Algebra and its applications by David Lay (4ed). A few theorems have been moved around.. Inner products

More information

Symmetric Matrices and Eigendecomposition

Symmetric Matrices and Eigendecomposition Symmetric Matrices and Eigendecomposition Robert M. Freund January, 2014 c 2014 Massachusetts Institute of Technology. All rights reserved. 1 2 1 Symmetric Matrices and Convexity of Quadratic Functions

More information

ELE/MCE 503 Linear Algebra Facts Fall 2018

ELE/MCE 503 Linear Algebra Facts Fall 2018 ELE/MCE 503 Linear Algebra Facts Fall 2018 Fact N.1 A set of vectors is linearly independent if and only if none of the vectors in the set can be written as a linear combination of the others. Fact N.2

More information

Problem # Max points possible Actual score Total 120

Problem # Max points possible Actual score Total 120 FINAL EXAMINATION - MATH 2121, FALL 2017. Name: ID#: Email: Lecture & Tutorial: Problem # Max points possible Actual score 1 15 2 15 3 10 4 15 5 15 6 15 7 10 8 10 9 15 Total 120 You have 180 minutes to

More information

MATH 20F: LINEAR ALGEBRA LECTURE B00 (T. KEMP)

MATH 20F: LINEAR ALGEBRA LECTURE B00 (T. KEMP) MATH 20F: LINEAR ALGEBRA LECTURE B00 (T KEMP) Definition 01 If T (x) = Ax is a linear transformation from R n to R m then Nul (T ) = {x R n : T (x) = 0} = Nul (A) Ran (T ) = {Ax R m : x R n } = {b R m

More information

OR MSc Maths Revision Course

OR MSc Maths Revision Course OR MSc Maths Revision Course Tom Byrne School of Mathematics University of Edinburgh t.m.byrne@sms.ed.ac.uk 15 September 2017 General Information Today JCMB Lecture Theatre A, 09:30-12:30 Mathematics revision

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 5: Completely Monotone and Multiply Monotone Functions Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu MATH

More information

Linear Algebra Review. Vectors

Linear Algebra Review. Vectors Linear Algebra Review 9/4/7 Linear Algebra Review By Tim K. Marks UCSD Borrows heavily from: Jana Kosecka http://cs.gmu.edu/~kosecka/cs682.html Virginia de Sa (UCSD) Cogsci 8F Linear Algebra review Vectors

More information

Math 4A Notes. Written by Victoria Kala Last updated June 11, 2017

Math 4A Notes. Written by Victoria Kala Last updated June 11, 2017 Math 4A Notes Written by Victoria Kala vtkala@math.ucsb.edu Last updated June 11, 2017 Systems of Linear Equations A linear equation is an equation that can be written in the form a 1 x 1 + a 2 x 2 +...

More information

Computational Methods CMSC/AMSC/MAPL 460. Eigenvalues and Eigenvectors. Ramani Duraiswami, Dept. of Computer Science

Computational Methods CMSC/AMSC/MAPL 460. Eigenvalues and Eigenvectors. Ramani Duraiswami, Dept. of Computer Science Computational Methods CMSC/AMSC/MAPL 460 Eigenvalues and Eigenvectors Ramani Duraiswami, Dept. of Computer Science Eigen Values of a Matrix Recap: A N N matrix A has an eigenvector x (non-zero) with corresponding

More information

Remark 1 By definition, an eigenvector must be a nonzero vector, but eigenvalue could be zero.

Remark 1 By definition, an eigenvector must be a nonzero vector, but eigenvalue could be zero. Sec 5 Eigenvectors and Eigenvalues In this chapter, vector means column vector Definition An eigenvector of an n n matrix A is a nonzero vector x such that A x λ x for some scalar λ A scalar λ is called

More information

MATH 304 Linear Algebra Lecture 34: Review for Test 2.

MATH 304 Linear Algebra Lecture 34: Review for Test 2. MATH 304 Linear Algebra Lecture 34: Review for Test 2. Topics for Test 2 Linear transformations (Leon 4.1 4.3) Matrix transformations Matrix of a linear mapping Similar matrices Orthogonality (Leon 5.1

More information

Meshfree Approximation Methods with MATLAB

Meshfree Approximation Methods with MATLAB Interdisciplinary Mathematical Sc Meshfree Approximation Methods with MATLAB Gregory E. Fasshauer Illinois Institute of Technology, USA Y f? World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI

More information

MTH 464: Computational Linear Algebra

MTH 464: Computational Linear Algebra MTH 464: Computational Linear Algebra Lecture Outlines Exam 2 Material Prof. M. Beauregard Department of Mathematics & Statistics Stephen F. Austin State University March 2, 2018 Linear Algebra (MTH 464)

More information

Review problems for MA 54, Fall 2004.

Review problems for MA 54, Fall 2004. Review problems for MA 54, Fall 2004. Below are the review problems for the final. They are mostly homework problems, or very similar. If you are comfortable doing these problems, you should be fine on

More information

Applied Linear Algebra in Geoscience Using MATLAB

Applied Linear Algebra in Geoscience Using MATLAB Applied Linear Algebra in Geoscience Using MATLAB Contents Getting Started Creating Arrays Mathematical Operations with Arrays Using Script Files and Managing Data Two-Dimensional Plots Programming in

More information

Chapters 5 & 6: Theory Review: Solutions Math 308 F Spring 2015

Chapters 5 & 6: Theory Review: Solutions Math 308 F Spring 2015 Chapters 5 & 6: Theory Review: Solutions Math 308 F Spring 205. If A is a 3 3 triangular matrix, explain why det(a) is equal to the product of entries on the diagonal. If A is a lower triangular or diagonal

More information

Positive Definite Kernels: Opportunities and Challenges

Positive Definite Kernels: Opportunities and Challenges Positive Definite Kernels: Opportunities and Challenges Michael McCourt Department of Mathematical and Statistical Sciences University of Colorado, Denver CUNY Mathematics Seminar CUNY Graduate College

More information

MATH 590: Meshfree Methods

MATH 590: Meshfree Methods MATH 590: Meshfree Methods Chapter 14: The Power Function and Native Space Error Estimates Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Fall 2010 fasshauer@iit.edu

More information

arxiv: v1 [math.pr] 22 May 2008

arxiv: v1 [math.pr] 22 May 2008 THE LEAST SINGULAR VALUE OF A RANDOM SQUARE MATRIX IS O(n 1/2 ) arxiv:0805.3407v1 [math.pr] 22 May 2008 MARK RUDELSON AND ROMAN VERSHYNIN Abstract. Let A be a matrix whose entries are real i.i.d. centered

More information

MATH 320: PRACTICE PROBLEMS FOR THE FINAL AND SOLUTIONS

MATH 320: PRACTICE PROBLEMS FOR THE FINAL AND SOLUTIONS MATH 320: PRACTICE PROBLEMS FOR THE FINAL AND SOLUTIONS There will be eight problems on the final. The following are sample problems. Problem 1. Let F be the vector space of all real valued functions on

More information

Interpolation by Basis Functions of Different Scales and Shapes

Interpolation by Basis Functions of Different Scales and Shapes Interpolation by Basis Functions of Different Scales and Shapes M. Bozzini, L. Lenarduzzi, M. Rossini and R. Schaback Abstract Under very mild additional assumptions, translates of conditionally positive

More information

Input: A set (x i -yy i ) data. Output: Function value at arbitrary point x. What for x = 1.2?

Input: A set (x i -yy i ) data. Output: Function value at arbitrary point x. What for x = 1.2? Applied Numerical Analysis Interpolation Lecturer: Emad Fatemizadeh Interpolation Input: A set (x i -yy i ) data. Output: Function value at arbitrary point x. 0 1 4 1-3 3 9 What for x = 1.? Interpolation

More information