Direct Design of Orthogonal Filter Banks and Wavelets by Sequential Convex Quadratic Programming

Size: px
Start display at page:

Download "Direct Design of Orthogonal Filter Banks and Wavelets by Sequential Convex Quadratic Programming"

Transcription

1 Direct Design of Orthogonl Filter Bnks nd Wvelets by Sequentil Convex Qudrtic Progrmming W.-S. Lu Dept. of Electricl nd Computer Engineering University of Victori, Victori, Cnd September 8 1

2 Abstrct Two-chnnel conjugte qudrture (CQ) FIR filter bnks re mong the most populr building blocks for multirte systems s they offer precise perfect reconstruction property. Most design methods for CQ filters re indirect in tht hlfbnd filter with nonnegtivity constrint is designed, followed by spectrum fctoriztion. This tlk describes direct method tht does not require designing the hlfbnd filter nd its fctoriztion, nd integrtes lest-squre nd minimx designs with vnishing moment nd other requirements into single design frmework. Exmples re supplied to help exmine design performnce, efficiency, nd its bility of getting globl solutions.

3 Outline Introduction Erly nd recent work Constrined liner updtes nd convex QP formultion for lest-squres design of conjugte qudrture (CQ) filters Constrined liner updtes nd n second-order cone progrmming (SOCP) formultion for minimx (equiripple) design of CQ filters Experimentl results 3

4 1. Introduction Two-chnnel FIR filter bnk x(n) H (z) F (z) x(n) ^ H 1 (z) F 1 (z) 1 1 Xˆ ( z) = [ F( zh ) ( z) + F1( zh ) 1( z)] X( z) + [ F( zh ) ( z) + F1( zh ) 1( z)] X( z) Perfect reconstruction (PR) conditions F ( z) H ( z) + F( z) H ( z) = z l 1 1 F ( z) H ( z) + F( z) H ( z) = 1 1 4

5 A conjugte qudrture (CQ) filter bnk ssumes H ( z) = z H ( z ), F ( z) = z H ( z ), F( z) = z H ( z ) ( N 1) 1 ( N 1) 1 ( N 1) the nd PR condition is utomticlly stisfied (no lising) nd the 1 st PR condition becomes H ( z) H ( z ) + H ( z) H ( z ) = (PS) 1 1 which is clled the power symmetric (PS) condition becuse it implies 1 ( j( π θ) ) j( π + θ) ( ) H e + H e = for ny θ 5

6 . Erly nd Recent Work Representtive erly nd recent work include Smith nd Brnwell (1984) Mintzer (1985) Vidynthn nd Nguyen (1987) Rioul nd Duhmel (1994) Lwton nd Michelli (1997) Tuqn nd Vidynthn (1998) Dumitrescu nd Popee () Ty (5, 6) 6

7 The most common design technique: A hlf-bnd filter P(z) is zero-phse FIR filter stisfying P(z) + P( z) = If we define P z = H z H z, then the PS condition 1 ( ) ( ) ( ) H ( z) H ( z ) + H ( z) H ( z ) = 1 1 becomes P(z) + P( z) = So P(z) is hlf-bnd filer nd, it is nonnegtive everywhere: ( ) P e = H ( e ) H ( e ) = H ( e ) (P) jω jω jω jω 7

8 Design steps: () Design lowpss hlf-bnd FIR filter P(z) with j nonnegtivity property Pe ( ω ) (b) Perform spectrl decomposition P z H z H z 1 ( ) = ( ) ( ) Vnishing moment (VM): the number of VMs equls to the number of zeros of H t ω = π : dh ( e ) l jω N 1 j l n n l h l n dω ω= π n= = ( ) ( 1) =, for l =, 1,, L 1 8

9 3. Lest-Squres Design of CQ Filters Problem Formultion Let H ( z) h z N 1 n = n with N even, nd h = [h h 1 h N-1 ] T n= A direct pproch: minimizing lest squres type objective function subject to the PS constrint: jω minimize H ( e ) dω h π ω subject to: H ( z) H ( z ) + H ( z) H ( z ) = 1 1 9

10 The objective function is positive definite qudrtic form: π ω ( jω ) T H e dω = h Qh where Q is symmetric positive definite Toeplitz mtrix: Q 1 = toeplitz π ω sinω sin[( N 1) ω] N 1 1

11 The constrint is the PS condition: H ( z) H ( z ) + H ( z) H ( z ) = (PS) 1 1 which is equivlent to set of N/ second-order equlity constrints: N 1 m n n+ m δ n= h h = ( m) for m=,1,,( N )/ where δ ( m) = 1 for m= nd δ ( m) = for m. 11

12 The design problem now becomes polynomil optimiztion problem (POP): N 1 m n= minimize h n n+ m T 1/ hqh= Q h subject to: h h = δ ( m) for m ( N ) / The POP cn be modified to include VM requirement: minimize h N 1 m n= N 1 n= T 1/ hqh= Q h subject to: h h = δ ( m) for m ( N ) / n n+ m n l ( 1) nh = for l=,1,, L 1 n 1

13 The POP cn be further modified to reduce the filter s phse response nonlinerity minimize h N 1 m n= N 1 n= 1/ Q h + w IN I N h n n+ m 1 1 subject to: h h = δ ( m) for m ( N ) / n l ( 1) nh = for l=,1,, L 1 n 13

14 Fetures of these problems: All polynomils re of second-order. The objective function is convex These re nonconvex problems becuse of the N/ second-order equlity constrints (the PS conditions). The PS constrints: exmples 1. N = 4 constrints: h + h + h + h = h h + h h =

15 . N = 1 constrints: h + h + + h = 1 ( terms) 1 19 h h + h h + + h h = h h + h h + + h h = h h + h h + + h h = h h + h h + h h + h h = h h + h h = (18 terms) (16 terms) (14 terms) (4 terms) ( terms) 15

16 Constrined Liner Updtes Suppose we re in the kth itertion of the lgorithm nd we wnt to updte filter coefficients from h (k) to chieve two things: to h (k+1) = h (k) + d to reduce the filter s stopbnd energy hqh T to better stisfy constrints N 1 m n= h h = δ ( m), m N/ 1 n n+ m The stopbnd energy t h (k+1) is equl to The constrints t h (k+1) becomes 1/ ( k ) Q ( d + h ) 16

17 h h + h d + d h + d d = δ ( m) ( k) ( k) ( k) ( k) n n+ m n n+ m n n+ m n n+ m n n n n Imposing constrints on the smllness of increment vector d: di β for i = 1,,, N then the nd -order constrints cn be linerized: h h + h d + d h + d d ( k) ( k) ( k) ( k) n n+ m n n+ m n n+ m n n+ m n n n n ( k ) known term, denoted by s ( m) = δ ( m) for m=,1,,( N )/ very smll, drop ( k) ( k) ( k) ( k) hn hn+ m + hn dn+ m + dnhn+ m n n n liner updtes 17

18 This leds to set of (N )/ liner equtions: n h d + d h = δ ( m) s ( m) u ( m) ( k) ( k) ( k) ( k) n n+ m n n+ m n which cn in mtrix-vector nottion be expressed s C d = u ( k) ( k) The smllness constrint on d is given by d β for 1 i n Ad b i The liner constrint on VMs is given by N 1 n= ( 1) n ( d + h ) = for l L 1 Dd = v n l ( k) ( k) n n 18

19 A Qudrtic Progrmming (QP) Formultion Summrizing the nlysis, the solution strtegy is to itertively updte the filter coefficients from h (k) to h (k+1) = h (k) + d (k) where d (k) is obtined by solving the QP problem 1/ ( k ) minimize Q ( d + h ) d subject to: Ad b ( k) ( k) C u d = ( k ) D v 19

20 If the phse-response nonlinerity is lso concern, we updte h (k) to h (k+1) = h (k) + d (k) by solving the QP problem 1/ ( k) ( k) minimize Q ( d + h ) + w IN I ( ) 1 N d + h 1 d subject to: Ad b ( k) ( k) C u d = ( k ) D v

21 Problem Formultion 4. Minimx Design of CQ Filters The formultion in this cse is chnged to N 1 m n= N 1 n= jω minimize mximize H ( e ) h subject to: h h = δ ( m) for m ( N ) / n n+ m n l ( 1) nh = for l=,1,, L 1 n ω ω π 1

22 Constrined Liner Updtes Like in the lest squres design, the constrined liner updte gives jω minimize mximize H ( e ) d ω ω π subject to: Ad b ( k) ( k) C u d = ( k ) D v

23 Deling with the objective function, we write N 1 jω = n jnω = T ω T n= H ( e ) h e h c( ) jh s( ω) T [ ] [ ] c( ω) = 1 cosω cos( N 1) ω, s( ω) = sinω sin( N 1) ω hence T jω ( T ) ( T ) c( ω) H( e ) = h c( ω) + h s( ω) = h F( ω) h T s( ω) T H (, ) ( ) ( ) ( ) e h + d = F ω h + d = F ω d + g jω ( k) ( k) ( k) ( k) ( k) ( k) 3

24 This converts the minimx problem into minimize η ( k) ( k) subject to: F( ωi) d + g η for { ωi} [ ω, π] Ad b ( k) ( k) C u d = ( k ) D v which is n SOCP problem. 4

25 5. Experimentl Results We performed totl of 18 LS designs with (filter length, stopbnd edge) being (N = 3, ω.58π = ), (N = 64, ω =.57π ), nd (N = 96, ω =.56π ), nd the number of vnishing moments L from, 1,, to 5. The ssocited QP were solved by the Optimiztion Toolbox provided by MthWorks Inc. The design performnce ws evluted in terms of stopbnd energy nd stisfction of the PS conditions. 5

26 Tble 1: Lest squres with N = 3, ω =.58π L Energy in Stopbnd Lrgest Eqution Error

27 LS design with N = 3, ω =.58π, nd L = Normlized frequency 7

28 Tble : Lest squres with N = 64, ω =.57π L Energy in Stopbnd Lrgest Eqution Error

29 LS design with N = 64, ω =.57π, nd L = Normlized frequency 9

30 Tble 3: Lest squres with N = 96, ω =.56π L Energy in Stopbnd Lrgest Eqution Error

31 LS design with N = 96, ω =.56π, nd L = Normlized frequency 31

32 We lso performed totl of 18 minimx designs with (filter length, stopbnd edge) being (N = 3, ω ω =.58π ), (N = 64, ω =.57π ), nd (N = 96, =.56π ), nd the number of vnishing moments L from, 1,, to 5. The ssocited SOCP problems were solved by SeDuMi 1.1R ( freewre mintined by the Advnced Optimiztion Lbortory t McMster). The design performnce ws evluted in terms of instntneous stopbnd energy nd stisfction of the PS conditions. 3

33 Tble 4: Minimx with N = 3, ω =.58π L Instntneous Energy in Stopbnd Lrgest Eqution Error

34 Minimx design with N = 3, ω =.58π, nd L = Normlized frequency 34

35 Tble 5: Minimx with N = 64, ω =.57π L Instntneous Energy in Stopbnd Lrgest Eqution Error

36 Minimx design with N = 64, ω =.57π, nd L = Normlized frequency 36

37 Tble 6: Minimx with N = 96, ω =.56π L Instntneous Energy in Stopbnd Lrgest Eqution Error

38 Minimx design with N = 96, ω =.56π, nd L = Normlized frequency 38

Direct Design of Orthogonal Filter Banks and Wavelets

Direct Design of Orthogonal Filter Banks and Wavelets Direct Design of Orthogonal Filter Banks and Wavelets W.-S. Lu T. Hinamoto Dept. of Electrical & Computer Engineering Graduate School of Engineering University of Victoria Hiroshima University Victoria,

More information

Best Approximation. Chapter The General Case

Best Approximation. Chapter The General Case Chpter 4 Best Approximtion 4.1 The Generl Cse In the previous chpter, we hve seen how n interpolting polynomil cn be used s n pproximtion to given function. We now wnt to find the best pproximtion to given

More information

Numerical Methods I Orthogonal Polynomials

Numerical Methods I Orthogonal Polynomials Numericl Methods I Orthogonl Polynomils Aleksndr Donev Cournt Institute, NYU 1 donev@cournt.nyu.edu 1 MATH-GA 2011.003 / CSCI-GA 2945.003, Fll 2014 Nov 6th, 2014 A. Donev (Cournt Institute) Lecture IX

More information

Matrices, Moments and Quadrature, cont d

Matrices, Moments and Quadrature, cont d Jim Lmbers MAT 285 Summer Session 2015-16 Lecture 2 Notes Mtrices, Moments nd Qudrture, cont d We hve described how Jcobi mtrices cn be used to compute nodes nd weights for Gussin qudrture rules for generl

More information

Advanced Computational Fluid Dynamics AA215A Lecture 3 Polynomial Interpolation: Numerical Differentiation and Integration.

Advanced Computational Fluid Dynamics AA215A Lecture 3 Polynomial Interpolation: Numerical Differentiation and Integration. Advnced Computtionl Fluid Dynmics AA215A Lecture 3 Polynomil Interpoltion: Numericl Differentition nd Integrtion Antony Jmeson Winter Qurter, 2016, Stnford, CA Lst revised on Jnury 7, 2016 Contents 3 Polynomil

More information

1 Online Learning and Regret Minimization

1 Online Learning and Regret Minimization 2.997 Decision-Mking in Lrge-Scle Systems My 10 MIT, Spring 2004 Hndout #29 Lecture Note 24 1 Online Lerning nd Regret Minimiztion In this lecture, we consider the problem of sequentil decision mking in

More information

Designs of Orthogonal Filter Banks and Orthogonal Cosine-Modulated Filter Banks

Designs of Orthogonal Filter Banks and Orthogonal Cosine-Modulated Filter Banks 1 / 45 Designs of Orthogonal Filter Banks and Orthogonal Cosine-Modulated Filter Banks Jie Yan Department of Electrical and Computer Engineering University of Victoria April 16, 2010 2 / 45 OUTLINE 1 INTRODUCTION

More information

Chapter Direct Method of Interpolation More Examples Civil Engineering

Chapter Direct Method of Interpolation More Examples Civil Engineering Chpter 5. Direct Method of Interpoltion More Exmples Civil Engineering Exmple o mximie ctch of bss in lke, it is suggested to throw the line to the depth of the thermocline. he chrcteristic feture of this

More information

Towards Global Design of Orthogonal Filter Banks and Wavelets

Towards Global Design of Orthogonal Filter Banks and Wavelets Towards Global Design of Orthogonal Filter Banks and Wavelets Jie Yan and Wu-Sheng Lu Department of Electrical and Computer Engineering University of Victoria Victoria, BC, Canada V8W 3P6 jyan@ece.uvic.ca,

More information

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies Stte spce systems nlysis (continued) Stbility A. Definitions A system is sid to be Asymptoticlly Stble (AS) when it stisfies ut () = 0, t > 0 lim xt () 0. t A system is AS if nd only if the impulse response

More information

g i fφdx dx = x i i=1 is a Hilbert space. We shall, henceforth, abuse notation and write g i f(x) = f

g i fφdx dx = x i i=1 is a Hilbert space. We shall, henceforth, abuse notation and write g i f(x) = f 1. Appliction of functionl nlysis to PEs 1.1. Introduction. In this section we give little introduction to prtil differentil equtions. In prticulr we consider the problem u(x) = f(x) x, u(x) = x (1) where

More information

Chapter 3 MATRIX. In this chapter: 3.1 MATRIX NOTATION AND TERMINOLOGY

Chapter 3 MATRIX. In this chapter: 3.1 MATRIX NOTATION AND TERMINOLOGY Chpter 3 MTRIX In this chpter: Definition nd terms Specil Mtrices Mtrix Opertion: Trnspose, Equlity, Sum, Difference, Sclr Multipliction, Mtrix Multipliction, Determinnt, Inverse ppliction of Mtrix in

More information

Orthogonal Polynomials

Orthogonal Polynomials Mth 4401 Gussin Qudrture Pge 1 Orthogonl Polynomils Orthogonl polynomils rise from series solutions to differentil equtions, lthough they cn be rrived t in vriety of different mnners. Orthogonl polynomils

More information

Theoretical foundations of Gaussian quadrature

Theoretical foundations of Gaussian quadrature Theoreticl foundtions of Gussin qudrture 1 Inner product vector spce Definition 1. A vector spce (or liner spce) is set V = {u, v, w,...} in which the following two opertions re defined: (A) Addition of

More information

We will see what is meant by standard form very shortly

We will see what is meant by standard form very shortly THEOREM: For fesible liner progrm in its stndrd form, the optimum vlue of the objective over its nonempty fesible region is () either unbounded or (b) is chievble t lest t one extreme point of the fesible

More information

Numerical Integration. 1 Introduction. 2 Midpoint Rule, Trapezoid Rule, Simpson Rule. AMSC/CMSC 460/466 T. von Petersdorff 1

Numerical Integration. 1 Introduction. 2 Midpoint Rule, Trapezoid Rule, Simpson Rule. AMSC/CMSC 460/466 T. von Petersdorff 1 AMSC/CMSC 46/466 T. von Petersdorff 1 umericl Integrtion 1 Introduction We wnt to pproximte the integrl I := f xdx where we re given, b nd the function f s subroutine. We evlute f t points x 1,...,x n

More information

Quadratic Forms. Quadratic Forms

Quadratic Forms. Quadratic Forms Qudrtic Forms Recll the Simon & Blume excerpt from n erlier lecture which sid tht the min tsk of clculus is to pproximte nonliner functions with liner functions. It s ctully more ccurte to sy tht we pproximte

More information

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions Physics 6C Solution of inhomogeneous ordinry differentil equtions using Green s functions Peter Young November 5, 29 Homogeneous Equtions We hve studied, especilly in long HW problem, second order liner

More information

Problem Set 3 Solutions

Problem Set 3 Solutions Chemistry 36 Dr Jen M Stndrd Problem Set 3 Solutions 1 Verify for the prticle in one-dimensionl box by explicit integrtion tht the wvefunction ψ ( x) π x is normlized To verify tht ψ ( x) is normlized,

More information

We know that if f is a continuous nonnegative function on the interval [a, b], then b

We know that if f is a continuous nonnegative function on the interval [a, b], then b 1 Ares Between Curves c 22 Donld Kreider nd Dwight Lhr We know tht if f is continuous nonnegtive function on the intervl [, b], then f(x) dx is the re under the grph of f nd bove the intervl. We re going

More information

Probabilistic Investigation of Sensitivities of Advanced Test- Analysis Model Correlation Methods

Probabilistic Investigation of Sensitivities of Advanced Test- Analysis Model Correlation Methods Probbilistic Investigtion of Sensitivities of Advnced Test- Anlysis Model Correltion Methods Liz Bergmn, Mtthew S. Allen, nd Dniel C. Kmmer Dept. of Engineering Physics University of Wisconsin-Mdison Rndll

More information

Overview of Calculus I

Overview of Calculus I Overview of Clculus I Prof. Jim Swift Northern Arizon University There re three key concepts in clculus: The limit, the derivtive, nd the integrl. You need to understnd the definitions of these three things,

More information

Review of Gaussian Quadrature method

Review of Gaussian Quadrature method Review of Gussin Qudrture method Nsser M. Asi Spring 006 compiled on Sundy Decemer 1, 017 t 09:1 PM 1 The prolem To find numericl vlue for the integrl of rel vlued function of rel vrile over specific rnge

More information

NUMERICAL INTEGRATION

NUMERICAL INTEGRATION NUMERICAL INTEGRATION How do we evlute I = f (x) dx By the fundmentl theorem of clculus, if F (x) is n ntiderivtive of f (x), then I = f (x) dx = F (x) b = F (b) F () However, in prctice most integrls

More information

Discrete Least-squares Approximations

Discrete Least-squares Approximations Discrete Lest-squres Approximtions Given set of dt points (x, y ), (x, y ),, (x m, y m ), norml nd useful prctice in mny pplictions in sttistics, engineering nd other pplied sciences is to construct curve

More information

Lecture 14: Quadrature

Lecture 14: Quadrature Lecture 14: Qudrture This lecture is concerned with the evlution of integrls fx)dx 1) over finite intervl [, b] The integrnd fx) is ssumed to be rel-vlues nd smooth The pproximtion of n integrl by numericl

More information

Abstract inner product spaces

Abstract inner product spaces WEEK 4 Abstrct inner product spces Definition An inner product spce is vector spce V over the rel field R equipped with rule for multiplying vectors, such tht the product of two vectors is sclr, nd the

More information

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004 Advnced Clculus: MATH 410 Notes on Integrls nd Integrbility Professor Dvid Levermore 17 October 2004 1. Definite Integrls In this section we revisit the definite integrl tht you were introduced to when

More information

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.)

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.) MORE FUNCTION GRAPHING; OPTIMIZATION FRI, OCT 25, 203 (Lst edited October 28, 203 t :09pm.) Exercise. Let n be n rbitrry positive integer. Give n exmple of function with exctly n verticl symptotes. Give

More information

Numerical Integration

Numerical Integration Chpter 5 Numericl Integrtion Numericl integrtion is the study of how the numericl vlue of n integrl cn be found. Methods of function pproximtion discussed in Chpter??, i.e., function pproximtion vi the

More information

P 3 (x) = f(0) + f (0)x + f (0) 2. x 2 + f (0) . In the problem set, you are asked to show, in general, the n th order term is a n = f (n) (0)

P 3 (x) = f(0) + f (0)x + f (0) 2. x 2 + f (0) . In the problem set, you are asked to show, in general, the n th order term is a n = f (n) (0) 1 Tylor polynomils In Section 3.5, we discussed how to pproximte function f(x) round point in terms of its first derivtive f (x) evluted t, tht is using the liner pproximtion f() + f ()(x ). We clled this

More information

Instructor: Marios M. Fyrillas HOMEWORK ASSIGNMENT ON INTERPOLATION

Instructor: Marios M. Fyrillas HOMEWORK ASSIGNMENT ON INTERPOLATION AMAT 34 Numericl Methods Instructor: Mrios M. Fyrills Emil: m.fyrills@fit.c.cy Office Tel.: 34559/6 Et. 3 HOMEWORK ASSIGNMENT ON INTERPOATION QUESTION Using interpoltion by colloction-polynomil fit method

More information

Review of Calculus, cont d

Review of Calculus, cont d Jim Lmbers MAT 460 Fll Semester 2009-10 Lecture 3 Notes These notes correspond to Section 1.1 in the text. Review of Clculus, cont d Riemnn Sums nd the Definite Integrl There re mny cses in which some

More information

Department of Chemical Engineering ChE-101: Approaches to Chemical Engineering Problem Solving MATLAB Tutorial VII

Department of Chemical Engineering ChE-101: Approaches to Chemical Engineering Problem Solving MATLAB Tutorial VII Tutoril VII: Liner Regression Lst updted 5/8/06 b G.G. Botte Deprtment of Chemicl Engineering ChE-0: Approches to Chemicl Engineering Problem Solving MATLAB Tutoril VII Liner Regression Using Lest Squre

More information

Lecture 6: Singular Integrals, Open Quadrature rules, and Gauss Quadrature

Lecture 6: Singular Integrals, Open Quadrature rules, and Gauss Quadrature Lecture notes on Vritionl nd Approximte Methods in Applied Mthemtics - A Peirce UBC Lecture 6: Singulr Integrls, Open Qudrture rules, nd Guss Qudrture (Compiled 6 August 7) In this lecture we discuss the

More information

Introduction to Numerical Analysis

Introduction to Numerical Analysis Introduction to Numericl Anlysis Doron Levy Deprtment of Mthemtics nd Center for Scientific Computtion nd Mthemticl Modeling (CSCAMM) University of Mrylnd June 14, 2012 D. Levy CONTENTS Contents 1 Introduction

More information

Interpolation. Gaussian Quadrature. September 25, 2011

Interpolation. Gaussian Quadrature. September 25, 2011 Gussin Qudrture September 25, 2011 Approximtion of integrls Approximtion of integrls by qudrture Mny definite integrls cnnot be computed in closed form, nd must be pproximted numericlly. Bsic building

More information

Engineering Analysis ENG 3420 Fall Dan C. Marinescu Office: HEC 439 B Office hours: Tu-Th 11:00-12:00

Engineering Analysis ENG 3420 Fall Dan C. Marinescu Office: HEC 439 B Office hours: Tu-Th 11:00-12:00 Engineering Anlysis ENG 3420 Fll 2009 Dn C. Mrinescu Office: HEC 439 B Office hours: Tu-Th 11:00-12:00 Lecture 13 Lst time: Problem solving in preprtion for the quiz Liner Algebr Concepts Vector Spces,

More information

Numerical Analysis. Doron Levy. Department of Mathematics Stanford University

Numerical Analysis. Doron Levy. Department of Mathematics Stanford University Numericl Anlysis Doron Levy Deprtment of Mthemtics Stnford University December 1, 2005 D. Levy Prefce i D. Levy CONTENTS Contents Prefce i 1 Introduction 1 2 Interpoltion 2 2.1 Wht is Interpoltion?............................

More information

Predict Global Earth Temperature using Linier Regression

Predict Global Earth Temperature using Linier Regression Predict Globl Erth Temperture using Linier Regression Edwin Swndi Sijbt (23516012) Progrm Studi Mgister Informtik Sekolh Teknik Elektro dn Informtik ITB Jl. Gnesh 10 Bndung 40132, Indonesi 23516012@std.stei.itb.c.id

More information

Definite integral. Mathematics FRDIS MENDELU

Definite integral. Mathematics FRDIS MENDELU Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová Brno 1 Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function defined on [, b]. Wht is the re of the

More information

Numerical Linear Algebra Assignment 008

Numerical Linear Algebra Assignment 008 Numericl Liner Algebr Assignment 008 Nguyen Qun B Hong Students t Fculty of Mth nd Computer Science, Ho Chi Minh University of Science, Vietnm emil. nguyenqunbhong@gmil.com blog. http://hongnguyenqunb.wordpress.com

More information

CMDA 4604: Intermediate Topics in Mathematical Modeling Lecture 19: Interpolation and Quadrature

CMDA 4604: Intermediate Topics in Mathematical Modeling Lecture 19: Interpolation and Quadrature CMDA 4604: Intermedite Topics in Mthemticl Modeling Lecture 19: Interpoltion nd Qudrture In this lecture we mke brief diversion into the res of interpoltion nd qudrture. Given function f C[, b], we sy

More information

Fundamental Theorem of Calculus

Fundamental Theorem of Calculus Fundmentl Theorem of Clculus Recll tht if f is nonnegtive nd continuous on [, ], then the re under its grph etween nd is the definite integrl A= f() d Now, for in the intervl [, ], let A() e the re under

More information

CHAPTER 2d. MATRICES

CHAPTER 2d. MATRICES CHPTER d. MTRICES University of Bhrin Deprtment of Civil nd rch. Engineering CEG -Numericl Methods in Civil Engineering Deprtment of Civil Engineering University of Bhrin Every squre mtrix hs ssocited

More information

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system Complex Numbers Section 1: Introduction to Complex Numbers Notes nd Exmples These notes contin subsections on The number system Adding nd subtrcting complex numbers Multiplying complex numbers Complex

More information

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by.

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by. NUMERICAL INTEGRATION 1 Introduction The inverse process to differentition in clculus is integrtion. Mthemticlly, integrtion is represented by f(x) dx which stnds for the integrl of the function f(x) with

More information

Lecture notes. Fundamental inequalities: techniques and applications

Lecture notes. Fundamental inequalities: techniques and applications Lecture notes Fundmentl inequlities: techniques nd pplictions Mnh Hong Duong Mthemtics Institute, University of Wrwick Emil: m.h.duong@wrwick.c.uk Februry 8, 207 2 Abstrct Inequlities re ubiquitous in

More information

Definite integral. Mathematics FRDIS MENDELU. Simona Fišnarová (Mendel University) Definite integral MENDELU 1 / 30

Definite integral. Mathematics FRDIS MENDELU. Simona Fišnarová (Mendel University) Definite integral MENDELU 1 / 30 Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová (Mendel University) Definite integrl MENDELU / Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function

More information

Multivariate problems and matrix algebra

Multivariate problems and matrix algebra University of Ferrr Stefno Bonnini Multivrite problems nd mtrix lgebr Multivrite problems Multivrite sttisticl nlysis dels with dt contining observtions on two or more chrcteristics (vribles) ech mesured

More information

Numerical Analysis: Trapezoidal and Simpson s Rule

Numerical Analysis: Trapezoidal and Simpson s Rule nd Simpson s Mthemticl question we re interested in numericlly nswering How to we evlute I = f (x) dx? Clculus tells us tht if F(x) is the ntiderivtive of function f (x) on the intervl [, b], then I =

More information

The Wave Equation I. MA 436 Kurt Bryan

The Wave Equation I. MA 436 Kurt Bryan 1 Introduction The Wve Eqution I MA 436 Kurt Bryn Consider string stretching long the x xis, of indeterminte (or even infinite!) length. We wnt to derive n eqution which models the motion of the string

More information

Elements of Matrix Algebra

Elements of Matrix Algebra Elements of Mtrix Algebr Klus Neusser Kurt Schmidheiny September 30, 2015 Contents 1 Definitions 2 2 Mtrix opertions 3 3 Rnk of Mtrix 5 4 Specil Functions of Qudrtic Mtrices 6 4.1 Trce of Mtrix.........................

More information

Jim Lambers MAT 169 Fall Semester Lecture 4 Notes

Jim Lambers MAT 169 Fall Semester Lecture 4 Notes Jim Lmbers MAT 169 Fll Semester 2009-10 Lecture 4 Notes These notes correspond to Section 8.2 in the text. Series Wht is Series? An infinte series, usully referred to simply s series, is n sum of ll of

More information

Orthogonal Polynomials and Least-Squares Approximations to Functions

Orthogonal Polynomials and Least-Squares Approximations to Functions Chpter Orthogonl Polynomils nd Lest-Squres Approximtions to Functions **4/5/3 ET. Discrete Lest-Squres Approximtions Given set of dt points (x,y ), (x,y ),..., (x m,y m ), norml nd useful prctice in mny

More information

Contents. Outline. Structured Rank Matrices Lecture 2: The theorem Proofs Examples related to structured ranks References. Structure Transport

Contents. Outline. Structured Rank Matrices Lecture 2: The theorem Proofs Examples related to structured ranks References. Structure Transport Contents Structured Rnk Mtrices Lecture 2: Mrc Vn Brel nd Rf Vndebril Dept. of Computer Science, K.U.Leuven, Belgium Chemnitz, Germny, 26-30 September 2011 1 Exmples relted to structured rnks 2 2 / 26

More information

Continuous Random Variables

Continuous Random Variables STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 217 Néhémy Lim Continuous Rndom Vribles Nottion. The indictor function of set S is rel-vlued function defined by : { 1 if x S 1 S (x) if x S Suppose tht

More information

STURM-LIOUVILLE THEORY, VARIATIONAL APPROACH

STURM-LIOUVILLE THEORY, VARIATIONAL APPROACH STURM-LIOUVILLE THEORY, VARIATIONAL APPROACH XIAO-BIAO LIN. Qudrtic functionl nd the Euler-Jcobi Eqution The purpose of this note is to study the Sturm-Liouville problem. We use the vritionl problem s

More information

Calculus I-II Review Sheet

Calculus I-II Review Sheet Clculus I-II Review Sheet 1 Definitions 1.1 Functions A function is f is incresing on n intervl if x y implies f(x) f(y), nd decresing if x y implies f(x) f(y). It is clled monotonic if it is either incresing

More information

A Matrix Algebra Primer

A Matrix Algebra Primer A Mtrix Algebr Primer Mtrices, Vectors nd Sclr Multipliction he mtrix, D, represents dt orgnized into rows nd columns where the rows represent one vrible, e.g. time, nd the columns represent second vrible,

More information

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008 Mth 520 Finl Exm Topic Outline Sections 1 3 (Xio/Dums/Liw) Spring 2008 The finl exm will be held on Tuesdy, My 13, 2-5pm in 117 McMilln Wht will be covered The finl exm will cover the mteril from ll of

More information

Math 1B, lecture 4: Error bounds for numerical methods

Math 1B, lecture 4: Error bounds for numerical methods Mth B, lecture 4: Error bounds for numericl methods Nthn Pflueger 4 September 0 Introduction The five numericl methods descried in the previous lecture ll operte by the sme principle: they pproximte the

More information

potentials A z, F z TE z Modes We use the e j z z =0 we can simply say that the x dependence of E y (1)

potentials A z, F z TE z Modes We use the e j z z =0 we can simply say that the x dependence of E y (1) 3e. Introduction Lecture 3e Rectngulr wveguide So fr in rectngulr coordintes we hve delt with plne wves propgting in simple nd inhomogeneous medi. The power density of plne wve extends over ll spce. Therefore

More information

Chapter 6 Techniques of Integration

Chapter 6 Techniques of Integration MA Techniques of Integrtion Asst.Prof.Dr.Suprnee Liswdi Chpter 6 Techniques of Integrtion Recll: Some importnt integrls tht we hve lernt so fr. Tle of Integrls n+ n d = + C n + e d = e + C ( n ) d = ln

More information

A NONLINEAR OPTIMIZATION PROCEDURE FOR GENERALIZED GAUSSIAN QUADRATURES

A NONLINEAR OPTIMIZATION PROCEDURE FOR GENERALIZED GAUSSIAN QUADRATURES A NONLINEAR OPTIMIZATION PROCEDURE FOR GENERALIZED GAUSSIAN QUADRATURES JAMES BREMER, ZYDRUNAS GIMBUTAS, AND VLADIMIR ROKHLIN Abstrct We present new nonliner optimiztion procedure for the computtion of

More information

MAT 772: Numerical Analysis. James V. Lambers

MAT 772: Numerical Analysis. James V. Lambers MAT 772: Numericl Anlysis Jmes V. Lmbers August 23, 2016 2 Contents 1 Solution of Equtions by Itertion 7 1.1 Nonliner Equtions....................... 7 1.1.1 Existence nd Uniqueness................ 7 1.1.2

More information

Data Assimilation. Alan O Neill Data Assimilation Research Centre University of Reading

Data Assimilation. Alan O Neill Data Assimilation Research Centre University of Reading Dt Assimiltion Aln O Neill Dt Assimiltion Reserch Centre University of Reding Contents Motivtion Univrite sclr dt ssimiltion Multivrite vector dt ssimiltion Optiml Interpoltion BLUE 3d-Vritionl Method

More information

B.Sc. in Mathematics (Ordinary)

B.Sc. in Mathematics (Ordinary) R48/0 DUBLIN INSTITUTE OF TECHNOLOGY KEVIN STREET, DUBLIN 8 B.Sc. in Mthemtics (Ordinry) SUPPLEMENTAL EXAMINATIONS 01 Numericl Methods Dr. D. Mckey Dr. C. Hills Dr. E.A. Cox Full mrks for complete nswers

More information

Introduction to Determinants. Remarks. Remarks. The determinant applies in the case of square matrices

Introduction to Determinants. Remarks. Remarks. The determinant applies in the case of square matrices Introduction to Determinnts Remrks The determinnt pplies in the cse of squre mtrices squre mtrix is nonsingulr if nd only if its determinnt not zero, hence the term determinnt Nonsingulr mtrices re sometimes

More information

The Product Rule state that if f and g are differentiable functions, then

The Product Rule state that if f and g are differentiable functions, then Chpter 6 Techniques of Integrtion 6. Integrtion by Prts Every differentition rule hs corresponding integrtion rule. For instnce, the Substitution Rule for integrtion corresponds to the Chin Rule for differentition.

More information

The Regulated and Riemann Integrals

The Regulated and Riemann Integrals Chpter 1 The Regulted nd Riemnn Integrls 1.1 Introduction We will consider severl different pproches to defining the definite integrl f(x) dx of function f(x). These definitions will ll ssign the sme vlue

More information

Section 7.1 Integration by Substitution

Section 7.1 Integration by Substitution Section 7. Integrtion by Substitution Evlute ech of the following integrls. Keep in mind tht using substitution my not work on some problems. For one of the definite integrls, it is not possible to find

More information

CLOSED EXPRESSIONS FOR COEFFICIENTS IN WEIGHTED NEWTON-COTES QUADRATURES

CLOSED EXPRESSIONS FOR COEFFICIENTS IN WEIGHTED NEWTON-COTES QUADRATURES Filomt 27:4 (2013) 649 658 DOI 10.2298/FIL1304649M Published by Fculty of Sciences nd Mthemtics University of Niš Serbi Avilble t: http://www.pmf.ni.c.rs/filomt CLOSED EXPRESSIONS FOR COEFFICIENTS IN WEIGHTED

More information

1. Extend QR downwards to meet the x-axis at U(6, 0). y

1. Extend QR downwards to meet the x-axis at U(6, 0). y In the digrm, two stright lines re to be drwn through so tht the lines divide the figure OPQRST into pieces of equl re Find the sum of the slopes of the lines R(6, ) S(, ) T(, 0) Determine ll liner functions

More information

DOING PHYSICS WITH MATLAB MATHEMATICAL ROUTINES

DOING PHYSICS WITH MATLAB MATHEMATICAL ROUTINES DOIG PHYSICS WITH MATLAB MATHEMATICAL ROUTIES COMPUTATIO OF OE-DIMESIOAL ITEGRALS In Cooper School of Physics, University of Sydney in.cooper@sydney.edu.u DOWLOAD DIRECTORY FOR MATLAB SCRIPTS mth_integrtion_1d.m

More information

Improper Integrals, and Differential Equations

Improper Integrals, and Differential Equations Improper Integrls, nd Differentil Equtions October 22, 204 5.3 Improper Integrls Previously, we discussed how integrls correspond to res. More specificlly, we sid tht for function f(x), the region creted

More information

( ) ( ) Chapter 5 Diffraction condition. ρ j

( ) ( ) Chapter 5 Diffraction condition. ρ j Grdute School of Engineering Ngo Institute of Technolog Crstl Structure Anlsis Tkshi Id (Advnced Cermics Reserch Center) Updted Nov. 3 3 Chpter 5 Diffrction condition In Chp. 4 it hs been shown tht the

More information

Reinforcement Learning

Reinforcement Learning Reinforcement Lerning Tom Mitchell, Mchine Lerning, chpter 13 Outline Introduction Comprison with inductive lerning Mrkov Decision Processes: the model Optiml policy: The tsk Q Lerning: Q function Algorithm

More information

Numerical Integration

Numerical Integration Chpter 1 Numericl Integrtion Numericl differentition methods compute pproximtions to the derivtive of function from known vlues of the function. Numericl integrtion uses the sme informtion to compute numericl

More information

Review of basic calculus

Review of basic calculus Review of bsic clculus This brief review reclls some of the most importnt concepts, definitions, nd theorems from bsic clculus. It is not intended to tech bsic clculus from scrtch. If ny of the items below

More information

The Algebra (al-jabr) of Matrices

The Algebra (al-jabr) of Matrices Section : Mtri lgebr nd Clculus Wshkewicz College of Engineering he lgebr (l-jbr) of Mtrices lgebr s brnch of mthemtics is much broder thn elementry lgebr ll of us studied in our high school dys. In sense

More information

Problem Set 3

Problem Set 3 14.102 Problem Set 3 Due Tuesdy, October 18, in clss 1. Lecture Notes Exercise 208: Find R b log(t)dt,where0

More information

21.6 Green Functions for First Order Equations

21.6 Green Functions for First Order Equations 21.6 Green Functions for First Order Equtions Consider the first order inhomogeneous eqution subject to homogeneous initil condition, B[y] y() = 0. The Green function G( ξ) is defined s the solution to

More information

Partial Derivatives. Limits. For a single variable function f (x), the limit lim

Partial Derivatives. Limits. For a single variable function f (x), the limit lim Limits Prtil Derivtives For single vrible function f (x), the limit lim x f (x) exists only if the right-hnd side limit equls to the left-hnd side limit, i.e., lim f (x) = lim f (x). x x + For two vribles

More information

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah

Jack Simons, Henry Eyring Scientist and Professor Chemistry Department University of Utah 1. Born-Oppenheimer pprox.- energy surfces 2. Men-field (Hrtree-Fock) theory- orbitls 3. Pros nd cons of HF- RHF, UHF 4. Beyond HF- why? 5. First, one usully does HF-how? 6. Bsis sets nd nottions 7. MPn,

More information

Calculus of Variations

Calculus of Variations Clculus of Vritions Com S 477/577 Notes) Yn-Bin Ji Dec 4, 2017 1 Introduction A functionl ssigns rel number to ech function or curve) in some clss. One might sy tht functionl is function of nother function

More information

Integral equations, eigenvalue, function interpolation

Integral equations, eigenvalue, function interpolation Integrl equtions, eigenvlue, function interpoltion Mrcin Chrząszcz mchrzsz@cernch Monte Crlo methods, 26 My, 2016 1 / Mrcin Chrząszcz (Universität Zürich) Integrl equtions, eigenvlue, function interpoltion

More information

PARTIAL FRACTION DECOMPOSITION

PARTIAL FRACTION DECOMPOSITION PARTIAL FRACTION DECOMPOSITION LARRY SUSANKA 1. Fcts bout Polynomils nd Nottion We must ssemble some tools nd nottion to prove the existence of the stndrd prtil frction decomposition, used s n integrtion

More information

Solution to Fredholm Fuzzy Integral Equations with Degenerate Kernel

Solution to Fredholm Fuzzy Integral Equations with Degenerate Kernel Int. J. Contemp. Mth. Sciences, Vol. 6, 2011, no. 11, 535-543 Solution to Fredholm Fuzzy Integrl Equtions with Degenerte Kernel M. M. Shmivnd, A. Shhsvrn nd S. M. Tri Fculty of Science, Islmic Azd University

More information

Lecture 0. MATH REVIEW for ECE : LINEAR CIRCUIT ANALYSIS II

Lecture 0. MATH REVIEW for ECE : LINEAR CIRCUIT ANALYSIS II Lecture 0 MATH REVIEW for ECE 000 : LINEAR CIRCUIT ANALYSIS II Aung Kyi Sn Grdute Lecturer School of Electricl nd Computer Engineering Purdue University Summer 014 Lecture 0 : Mth Review Lecture 0 is intended

More information

Transport Calculations. Tseelmaa Byambaakhuu, Dean Wang*, and Sicong Xiao

Transport Calculations. Tseelmaa Byambaakhuu, Dean Wang*, and Sicong Xiao A Locl hp Adptive Diffusion Synthetic Accelertion Method for Neutron Trnsport Clcultions Tseelm Bymbkhuu, Den Wng*, nd Sicong Xio University of Msschusetts Lowell, 1 University Ave, Lowell, MA 01854 USA

More information

Multi-Armed Bandits: Non-adaptive and Adaptive Sampling

Multi-Armed Bandits: Non-adaptive and Adaptive Sampling CSE 547/Stt 548: Mchine Lerning for Big Dt Lecture Multi-Armed Bndits: Non-dptive nd Adptive Smpling Instructor: Shm Kkde 1 The (stochstic) multi-rmed bndit problem The bsic prdigm is s follows: K Independent

More information

First variation. (one-variable problem) January 14, 2013

First variation. (one-variable problem) January 14, 2013 First vrition (one-vrible problem) Jnury 14, 2013 Contents 1 Sttionrity of n integrl functionl 2 1.1 Euler eqution (Optimlity conditions)............... 2 1.2 First integrls: Three specil cses.................

More information

Physics 202H - Introductory Quantum Physics I Homework #08 - Solutions Fall 2004 Due 5:01 PM, Monday 2004/11/15

Physics 202H - Introductory Quantum Physics I Homework #08 - Solutions Fall 2004 Due 5:01 PM, Monday 2004/11/15 Physics H - Introductory Quntum Physics I Homework #8 - Solutions Fll 4 Due 5:1 PM, Mondy 4/11/15 [55 points totl] Journl questions. Briefly shre your thoughts on the following questions: Of the mteril

More information

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below.

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below. Dulity #. Second itertion for HW problem Recll our LP emple problem we hve been working on, in equlity form, is given below.,,,, 8 m F which, when written in slightly different form, is 8 F Recll tht we

More information

Quantum Physics II (8.05) Fall 2013 Assignment 2

Quantum Physics II (8.05) Fall 2013 Assignment 2 Quntum Physics II (8.05) Fll 2013 Assignment 2 Msschusetts Institute of Technology Physics Deprtment Due Fridy September 20, 2013 September 13, 2013 3:00 pm Suggested Reding Continued from lst week: 1.

More information

New Expansion and Infinite Series

New Expansion and Infinite Series Interntionl Mthemticl Forum, Vol. 9, 204, no. 22, 06-073 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/0.2988/imf.204.4502 New Expnsion nd Infinite Series Diyun Zhng College of Computer Nnjing University

More information

Numerical integration. Quentin Louveaux (ULiège - Institut Montefiore) Numerical analysis / 10

Numerical integration. Quentin Louveaux (ULiège - Institut Montefiore) Numerical analysis / 10 Numericl integrtion Quentin Louveux (ULiège Institut Montefiore) Numericl nlysis 2018 1 / 10 Numericl integrtion We consider definite integrls Z b f (x)dx better to it use if known! A We do not ssume tht

More information

Sturm-Liouville Eigenvalue problem: Let p(x) > 0, q(x) 0, r(x) 0 in I = (a, b). Here we assume b > a. Let X C 2 1

Sturm-Liouville Eigenvalue problem: Let p(x) > 0, q(x) 0, r(x) 0 in I = (a, b). Here we assume b > a. Let X C 2 1 Ch.4. INTEGRAL EQUATIONS AND GREEN S FUNCTIONS Ronld B Guenther nd John W Lee, Prtil Differentil Equtions of Mthemticl Physics nd Integrl Equtions. Hildebrnd, Methods of Applied Mthemtics, second edition

More information

Notes on the Eigenfunction Method for solving differential equations

Notes on the Eigenfunction Method for solving differential equations Notes on the Eigenfunction Metho for solving ifferentil equtions Reminer: Wereconsieringtheinfinite-imensionlHilbertspceL 2 ([, b] of ll squre-integrble functions over the intervl [, b] (ie, b f(x 2

More information