ADVANCED TOPICS ON VIDEO PROCESSING
|
|
- Antony Rich
- 5 years ago
- Views:
Transcription
1 ADVANCED TOPICS ON VIDEO PROCESSING Image Spatial Processig
2 FILTERING EXAMPLES
3 FOURIER INTERPRETATION
4 FILTERING EXAMPLES
5 FOURIER INTERPRETATION
6 FILTERING EXAMPLES
7 FILTERING EXAMPLES
8 FOURIER INTERPRETATION
9 FILTERING EXAMPLES
10 FOURIER INTERPRETATION
11 LINEAR AND NON LINEAR OPERATIONS Media Filter: (6899 (6, 8, 9, 9,,,, 3, 5) = Miimum = 6; Maximum: 5 Average o earest eighbours:
12 LOW PASS GAUSSIAN FILTER
13 MEDIAN FILTERING
14 HI PASS FILTERING FOR HIGH FREQUENCIES
15 EXAMPLE
16 D DERIVATIVES
17 GRADIENT METHODS D example >ThresThres hold? ye Si s Yes No No edge Yes No No edge
18 D CASE The irst derivative is substituted by the gradiet x y x, y i x x Omidirectioal detector, x, y y Based o ƒ(x,y) : isotropic i behaviour Directioal detector Based o a orieted derivative: ex.: a possible horizotal edge detector is y i y
19 D APPROACH
20 EDGE THINNING ) i has a local horizotal max but ot a vertical oe i ( ) the that poit is a edge poit i (x,y ), the, that poit is a edge poit i x K K ( typical value) y ( x y ) ( x, y ), ) i has a local vertical max but ot a horizotal oe i (x,y ), the, that poit is a edge poit i y K x ( ) ( ) x, y x, y o K(typical value)
21 DIRECTIONAL CASE.
22 EXAMPLE: ISOTROPIC CASE.
23 DISCRETIZATION DISCRETIZATION The gradiet operator ca be discretized as: The gradiet operator ca be discretized as:, ), ( ) ( y x y x, ), ( ), ( y y x y y x ), ( ), ( ), ( y x Which is based o a discretizatio o directioal derivatives: derivatives: ), ( ), ( ), ( y x
24 FINITE IMPULSE RESPONSE MODEL Discrete sc ete operators ope ato s or o derivative de at e estimatio est at o ca ca be estimated est ated as FIR ilters. y (, ) (, ) * hy (, ) x (, ) (, ) * hx (, ) (, ) hx (, ) x (, )
25 DISCRETE DIFFERENTIAL OPERATORS Pixel dierece: lumiace dierece betwee to eighbour pixels alog orthogoal directios. x y Separable ilters ( j, k) ( j, k) ( j, k ) ( j, k) ( j, k) ( j, k) h x h y
26 EXAMPLE: PIXEL DIFFERENCE
27 SEPARATED PIXEL DIFFERENCE I arther pixels are chose there is a higher oise rejectio, ad there is o phase traslatio i edge deiitio. x ( j, k) ( j, k ) ( j, k ) ( j, k ) ( j, k ) ( j, k ) y h x h y
28 EX.: SEPARATED PIXEL DIFFERENCE
29 ROBERTS EDGE EXTRACTION ROBERTS EDGE EXTRACTION ), ( ), ( ), ( k j k j k j x ), ( ), ( ), ( k j k j k j y h h h x h y
30 EX.: ROBERTS METHOD
31 PREWITT METHOD PREWITT METHOD Estimatio ca be improved ivolvig more samples or te Estimatio ca be improved ivolvig more samples or te gradiet operator 3x3,, * x K = vertical low pass* horizotal high pass,,,, vertical low pass horizotal high pass,, * K,,,, y = vertical high pass* horizotal low pass
32 GRADIENT ESTIMATION Gradiet modulus = the value o the higher g directioal derivative Gradiet phase = orietatio o the higher directioal derivative Squared lattice =eight possible directios h, E h, NE h, N h, NW
33 GRADIENT ESTIMATION h, W h, SW h, h, S SE
34 EX.: PREWITT METHOD 3X3 3
35 SOBEL METHOD Same dimesios o Prewitt ilter Dieret weight or cetral poit i dieret directios. h r h c Sobel or exagoal grids. h
36 EX.: SOBEL METHOD
37 COMPARISON Roberts Sobel Prewitt
38 FREI-CHEN OPERATOR Isotropic operator similar il to Prewitt dieret weight or the cetral poit i the 4 directios. The gradiet has the same value or horizotal, vertical ad diagoal edges. h r h c
39 EX.: METODO O DI FREI-CHEN
40 EXTENDED OPERATORS EXTENDED OPERATORS A li it th ti d th d i th i k i A limit or the aoremetioed methods is their weakess i accurate edge detectio whe SNR is very low. A possible solutio i to exted their size: the result will be a A possible solutio i to exted their size: the result will be a less accurate edge positioig but oise rejectio will be higher. higher. PREWITT METHOD 7X7 Extesio o Prewitt 3X3 Extesio o Prewitt 3X3 Normalized impulse respose: h r r
41 EX.: PREWITT 7X7 METHOD
42 ABDOU 7X7 METHOD ABDOU 7X7 METHOD I ilt k th t i li d i l i ht Is a ilter mask that gives a liear decreasig sample weight as they are arther rom the edge. Its behaviour is close to a trucated pyramid trucated pyramid. The ormalized impulse respose is: h r 3 3 r
43 EX.: ABDOU 7X7 METHOD
44 FURTHER EXTENDED OPERATORS It tspossbetoobta is possible to obtai exteded etededgadet gradiet ilters teso or low SNR coditios covolvig a 3x3 operator with a low-pass ilter. h( j, k) h ( j, k)* h ( j, k) G H G (j,k) is oe o the previously cosidered ilters, H PB (j,k) is the impulse respose or a low-pass ilter. PG
45 EXAMPLE Prewitt 3X3 covoled with: h * 9...ad we get the Smoothed Prewitt 5X5 h
46 LAPLACIAN BASED METHODS D Case Fi d i g th d d i ti di g t Fid zero-crossig o the secod derivative, correspodig to ilectio poits.
47 LAPLACIAN For the D case the d order dieretial operator is the Laplacia ( x, y) ( x, y) ( x, y) ( ( x, y)) x y Isotropic operator More sesible to oise with respect to gradiet False edges ca be geerated due to oise. Thier edges are produced.
48 ALGORITHM: CASE D Gradiet estimatio O( x, y) ( xy, ) ( x, y) =? Yes O ( x, y ) Yes threshold edge No No
49 ZERO-CROSSING WITHOUT THRESHOLD Sobel vs. Laplacia
50 LAPLACIAN DISCRETIZATION Ca be see as the covolutio o (, ) with the impulse respose h(, ) o a liear system.
51 4 NEIGHBOURS METHOD 4 NEIGHBOURS METHOD S bl li d ilt Separable ormalized ilter Uit gai or cotiuous compoet The sig o h( ) ca be chaged itho t chages i The sig o h(, ) ca be chaged without chages i the ial result (sice we are lookig or zeros o laplacia) 4 4 ), ( h
52 EX.: 4 NEIGHBOURS METHOD
53 LAPLACIAN DISCRETIZATION LAPLACIAN DISCRETIZATION The laplacia ca be approximated with iite diereces ), ( ), ( ), ( ), ( k j k j y x y x diereces ), ( ), ( ), ( k j k j y x x x ) ( ), ( ), ( ), ( ), ( k j k j k j x y x x x xx ), ( ), ( ), ( k j k j k j
54 DISCRETIZATION EXAMPLES DISCRETIZATION EXAMPLES Prewitt method Not separable ilter h (, ) Neighbours method ( ) 8 8 Neighbours method Similar to Prewitt but with a separable ormulatio 4 ) ( h ), ( h
55 EX.: 8 NEIGHBOURS METHOD
56 EX.: PREWITT NOT SEPARABLE
57 NOISE PRESENCE Whe oise is sigiicat these ilters could ot be accurate or diagoal edges. The Prewitt ilter ca work eve i regios with high desity o edges. h(, ) 4 8 Sice ege are directioal ad oise ca geerate lumiace variatios, zero-crossig or laplacia could id o-correct edges.
58 EX.: LAPLACIAN FOR DIAGONAL EDGES
59 SUPER-RESOLUTION RESOLUTION (LAPLACIAN) First method. Give two eighbour pixels, mark as possible edge poit the itrapixels poits i the laplacia values i the two pixels have dieret sigs. Assume as eective edge the poit, amog them, with the largest gradiet. Apply this aalysis to all the pixels couples. LAPLACIAN I 4 I3 I I5 I I I 6 I7 I8 Sig aalysis Magitude compariso
60 Fˆ SUPERRESOLUTION Secod method: aalytical approach Approximate the cotiuous orm o uctio (, ) with a D polyomial i order to describe the laplacia i a aalytical way. Polyomial example: ( r, c) K Kr K3c K4r K5rc K6c K7r c K8rc K9r c where K i are the weights obtaied rom the discrete image. r ad c the become cotiuous variables associtated to a discrete image matrix. ( W ) Polyomial ormulatio ca be oud with small eorts. rc, ( W )
61 SUPERRESOLUTION Method d3: edge ittig Based o the compariso with a edge model based o the image correlatio. sx ( ) a per x < x a+h per x x x L Exemple: compariso with a step uctio E ( x) s( x) the edge is accepted i the MSE is below a threshold. x L dx
62 SUPERRESOLUTION sxy (, ) Case D a or (x cos +y si )< a+h or (x cos +y si ) Compare (x,y) with a D step, where ad speciy the distace ad the agle, i polar coordiates o the edge poit rom the ceter o the cosidered circular regio. The edge is accepted i the MSE is below a Threshold MSE ( x, y) s( x, y) dxdy circle
63 GAUSSIAN FILTERING Why we should use a gaussia uctio? Sice the Fourier trasorm o a Gaussia is still e gaussia, g, The cut-o requecy ca be expressed as a uctio o the width o the impulse respose It has a low aliasig The ilter is separable ad isotropic at the same time h( x, y ) h ( x)h ( y ) h ( x) e x / The oise sesitivityy ((umerous zero crossig) g) decrease as the ilter stregth (width) icrease.
64 LOG OPERATOR The low pass gaussia ilter has a variable cut-o requecy. x y h( x, y) exp H ( x, y ) exp ( x y ) It ollows that the stadard deviatio is iversely proportioal to the ilter width.
65 LOG LOG operator g ( x, y ) ( x, y ) * h ( x, y ) Laplacia ad ilterig are iterchageable sice both o them are liear g ( x, y ) ( x, y ) * h ( x, y ) x y x y exp h ( x, y ) 4 x y h( x, y ) exp x y
66 DIFFERENCE OF GAUSSIANS Thee LOG, OG, Laplacia ap ac a oo a Gaussia Gauss a co correspods espo ds to o thee derivative o a gaussia with respect to The laplacia ca be approximated with the dierece o two gaussia ilters with dieret.
67 DOG APPLICATION
FIR Filter Design: Part I
EEL3: Discrete-Time Sigals ad Systems FIR Filter Desig: Part I. Itroductio FIR Filter Desig: Part I I this set o otes, we cotiue our exploratio o the requecy respose o FIR ilters. First, we cosider some
More informationWhere do eigenvalues/eigenvectors/eigenfunctions come from, and why are they important anyway?
Where do eigevalues/eigevectors/eigeuctios come rom, ad why are they importat ayway? I. Bacgroud (rom Ordiary Dieretial Equatios} Cosider the simplest example o a harmoic oscillator (thi o a vibratig strig)
More informationFFTs in Graphics and Vision. The Fast Fourier Transform
FFTs i Graphics ad Visio The Fast Fourier Trasform 1 Outlie The FFT Algorithm Applicatios i 1D Multi-Dimesioal FFTs More Applicatios Real FFTs 2 Computatioal Complexity To compute the movig dot-product
More informationThe Discrete-Time Fourier Transform (DTFT)
EEL: Discrete-Time Sigals ad Systems The Discrete-Time Fourier Trasorm (DTFT) The Discrete-Time Fourier Trasorm (DTFT). Itroductio I these otes, we itroduce the discrete-time Fourier trasorm (DTFT) ad
More informationAssignment 1 : Real Numbers, Sequences. for n 1. Show that (x n ) converges. Further, by observing that x n+2 + x n+1
Assigmet : Real Numbers, Sequeces. Let A be a o-empty subset of R ad α R. Show that α = supa if ad oly if α is ot a upper boud of A but α + is a upper boud of A for every N. 2. Let y (, ) ad x (, ). Evaluate
More informationPAPER : IIT-JAM 2010
MATHEMATICS-MA (CODE A) Q.-Q.5: Oly oe optio is correct for each questio. Each questio carries (+6) marks for correct aswer ad ( ) marks for icorrect aswer.. Which of the followig coditios does NOT esure
More informationProblem Cosider the curve give parametrically as x = si t ad y = + cos t for» t» ß: (a) Describe the path this traverses: Where does it start (whe t =
Mathematics Summer Wilso Fial Exam August 8, ANSWERS Problem 1 (a) Fid the solutio to y +x y = e x x that satisfies y() = 5 : This is already i the form we used for a first order liear differetial equatio,
More informationMon Apr Second derivative test, and maybe another conic diagonalization example. Announcements: Warm-up Exercise:
Math 2270-004 Week 15 otes We will ot ecessarily iish the material rom a give day's otes o that day We may also add or subtract some material as the week progresses, but these otes represet a i-depth outlie
More information(c) Write, but do not evaluate, an integral expression for the volume of the solid generated when R is
Calculus BC Fial Review Name: Revised 7 EXAM Date: Tuesday, May 9 Remiders:. Put ew batteries i your calculator. Make sure your calculator is i RADIAN mode.. Get a good ight s sleep. Eat breakfast. Brig:
More informationTime-Domain Representations of LTI Systems
2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable
More informationFilter banks. Separately, the lowpass and highpass filters are not invertible. removes the highest frequency 1/ 2and
Filter bas Separately, the lowpass ad highpass filters are ot ivertible T removes the highest frequecy / ad removes the lowest frequecy Together these filters separate the sigal ito low-frequecy ad high-frequecy
More informationCALCULUS AB SECTION I, Part A Time 60 minutes Number of questions 30 A CALCULATOR MAY NOT BE USED ON THIS PART OF THE EXAM.
AP Calculus AB Portfolio Project Multiple Choice Practice Name: CALCULUS AB SECTION I, Part A Time 60 miutes Number of questios 30 A CALCULATOR MAY NOT BE USED ON THIS PART OF THE EXAM. Directios: Solve
More informationCS537. Numerical Analysis and Computing
CS57 Numerical Aalysis ad Computig Lecture Locatig Roots o Equatios Proessor Ju Zhag Departmet o Computer Sciece Uiversity o Ketucky Leigto KY 456-6 Jauary 9 9 What is the Root May physical system ca be
More informationFundamental Concepts: Surfaces and Curves
UNDAMENTAL CONCEPTS: SURACES AND CURVES CHAPTER udametal Cocepts: Surfaces ad Curves. INTRODUCTION This chapter describes two geometrical objects, vi., surfaces ad curves because the pla a ver importat
More informationComplex Analysis Spring 2001 Homework I Solution
Complex Aalysis Sprig 2001 Homework I Solutio 1. Coway, Chapter 1, sectio 3, problem 3. Describe the set of poits satisfyig the equatio z a z + a = 2c, where c > 0 ad a R. To begi, we see from the triagle
More information6.003 Homework #12 Solutions
6.003 Homework # Solutios Problems. Which are rue? For each of the D sigals x [] through x 4 [] below), determie whether the coditios listed i the followig table are satisfied, ad aswer for true or F for
More informationCS321. Numerical Analysis and Computing
CS Numerical Aalysis ad Computig Lecture Locatig Roots o Equatios Proessor Ju Zhag Departmet o Computer Sciece Uiversity o Ketucky Leigto KY 456-6 September 8 5 What is the Root May physical system ca
More information6.003 Homework #12 Solutions
6.003 Homework # Solutios Problems. Which are rue? For each of the D sigals x [] through x 4 [] (below), determie whether the coditios listed i the followig table are satisfied, ad aswer for true or F
More informationMTH Assignment 1 : Real Numbers, Sequences
MTH -26 Assigmet : Real Numbers, Sequeces. Fid the supremum of the set { m m+ : N, m Z}. 2. Let A be a o-empty subset of R ad α R. Show that α = supa if ad oly if α is ot a upper boud of A but α + is a
More informationCS475 Parallel Programming
CS475 Parallel Programmig Dieretiatio ad Itegratio Wim Bohm Colorado State Uiversity Ecept as otherwise oted, the cotet o this presetatio is licesed uder the Creative Commos Attributio.5 licese. Pheomea
More informationFrequency Response of FIR Filters
EEL335: Discrete-Time Sigals ad Systems. Itroductio I this set of otes, we itroduce the idea of the frequecy respose of LTI systems, ad focus specifically o the frequecy respose of FIR filters.. Steady-state
More informationOutline. L7: Probability Basics. Probability. Probability Theory. Bayes Law for Diagnosis. Which Hypothesis To Prefer? p(a,b) = p(b A) " p(a)
Outlie L7: Probability Basics CS 344R/393R: Robotics Bejami Kuipers. Bayes Law 2. Probability distributios 3. Decisios uder ucertaity Probability For a propositio A, the probability p(a is your degree
More informationThis chapter describes different methods to discretize the diffusion equation. f z 2 = 0. y ) x f
Chapter 8 Diusio Equatio This chapter describes dieret methods to discretize the diusio equatio 2 t α x 2 + 2 y 2 + 2 z 2 = 0 which represets a combied boudary ad iitial value problem, i.e., requires to
More informationSection 7. Gaussian Reduction
7- Sectio 7 Gaussia eductio Paraxial aytrace Equatios eractio occurs at a iterace betwee two optical spaces. The traser distace t' allows the ray height y' to be determied at ay plae withi a optical space
More informationLecture 11. Solution of Nonlinear Equations - III
Eiciecy o a ethod Lecture Solutio o Noliear Equatios - III The eiciecy ide o a iterative ethod is deied by / E r r: rate o covergece o the ethod : total uber o uctios ad derivative evaluatios at each step
More informationContinuous Data that can take on any real number (time/length) based on sample data. Categorical data can only be named or categorised
Questio 1. (Topics 1-3) A populatio cosists of all the members of a group about which you wat to draw a coclusio (Greek letters (μ, σ, Ν) are used) A sample is the portio of the populatio selected for
More information2D DSP Basics: 2D Systems
- Digital Image Processig ad Compressio D DSP Basics: D Systems D Systems T[ ] y = T [ ] Liearity Additivity: If T y = T [ ] The + T y = y + y Homogeeity: If The T y = T [ ] a T y = ay = at [ ] Liearity
More informationIndian Institute of Information Technology, Allahabad. End Semester Examination - Tentative Marking Scheme
Idia Istitute of Iformatio Techology, Allahabad Ed Semester Examiatio - Tetative Markig Scheme Course Name: Mathematics-I Course Code: SMAT3C MM: 75 Program: B.Tech st year (IT+ECE) ate of Exam:..7 ( st
More informationLesson 03 Heat Equation with Different BCs
PDE & Complex Variables P3- esso 3 Heat Equatio with Differet BCs ( ) Physical meaig (SJF ) et u(x, represet the temperature of a thi rod govered by the (coductio) heat equatio: u t =α u xx (3.) where
More informationPRELIM PROBLEM SOLUTIONS
PRELIM PROBLEM SOLUTIONS THE GRAD STUDENTS + KEN Cotets. Complex Aalysis Practice Problems 2. 2. Real Aalysis Practice Problems 2. 4 3. Algebra Practice Problems 2. 8. Complex Aalysis Practice Problems
More informationSalmon: Lectures on partial differential equations. 3. First-order linear equations as the limiting case of second-order equations
3. First-order liear equatios as the limitig case of secod-order equatios We cosider the advectio-diffusio equatio (1) v = 2 o a bouded domai, with boudary coditios of prescribed. The coefficiets ( ) (2)
More informationThe z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j
The -Trasform 7. Itroductio Geeralie the complex siusoidal represetatio offered by DTFT to a represetatio of complex expoetial sigals. Obtai more geeral characteristics for discrete-time LTI systems. 7.
More informationPhys. 201 Mathematical Physics 1 Dr. Nidal M. Ershaidat Doc. 12
Physics Departmet, Yarmouk Uiversity, Irbid Jorda Phys. Mathematical Physics Dr. Nidal M. Ershaidat Doc. Fourier Series Deiitio A Fourier series is a expasio o a periodic uctio (x) i terms o a iiite sum
More informationNumerical Methods! for! Elliptic Equations-II! Multigrid! Methods! f Analytic Solution of! g = bk. da k dt. = α. ( t)
http://www.d.edu/~gtryggva/cfd-course/! umerical Methods! or! Elliptic Equatios-II! Grétar Tryggvaso! Sprig 13! Examples o elliptic equatios! Direct Methods or 1D problems! Elemetary Iterative Methods!
More informationCov(aX, cy ) Var(X) Var(Y ) It is completely invariant to affine transformations: for any a, b, c, d R, ρ(ax + b, cy + d) = a.s. X i. as n.
CS 189 Itroductio to Machie Learig Sprig 218 Note 11 1 Caoical Correlatio Aalysis The Pearso Correlatio Coefficiet ρ(x, Y ) is a way to measure how liearly related (i other words, how well a liear model
More informationMorphological Image Processing
Morphological Image Processig Biary dilatio ad erosio Set-theoretic iterpretatio Opeig, closig, morphological edge detectors Hit-miss filter Morphological filters for gray-level images Cascadig dilatios
More informationCorrelation. Two variables: Which test? Relationship Between Two Numerical Variables. Two variables: Which test? Contingency table Grouped bar graph
Correlatio Y Two variables: Which test? X Explaatory variable Respose variable Categorical Numerical Categorical Cotigecy table Cotigecy Logistic Grouped bar graph aalysis regressio Mosaic plot Numerical
More informationPH 411/511 ECE B(k) Sin k (x) dk (1)
Fall-27 PH 4/5 ECE 598 A. La Rosa Homework-3 Due -7-27 The Homework is iteded to gai a uderstadig o the Heiseberg priciple, based o a compariso betwee the width of a pulse ad the width of its spectral
More information5. Fast NLMS-OCF Algorithm
5. Fast LMS-OCF Algorithm The LMS-OCF algorithm preseted i Chapter, which relies o Gram-Schmidt orthogoalizatio, has a compleity O ( M ). The square-law depedece o computatioal requiremets o the umber
More informationFormation of A Supergain Array and Its Application in Radar
Formatio of A Supergai Array ad ts Applicatio i Radar Tra Cao Quye, Do Trug Kie ad Bach Gia Duog. Research Ceter for Electroic ad Telecommuicatios, College of Techology (Coltech, Vietam atioal Uiversity,
More informationSIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road QUESTION BANK (DESCRIPTIVE)
QUESTION BANK 8 SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayaavaam Road 5758 QUESTION BANK (DESCRIPTIVE) Subject with Code : (6HS6) Course & Brach: B.Tech AG Year & Sem: II-B.Tech&
More informationPhysics 7440, Solutions to Problem Set # 8
Physics 7440, Solutios to Problem Set # 8. Ashcroft & Mermi. For both parts of this problem, the costat offset of the eergy, ad also the locatio of the miimum at k 0, have o effect. Therefore we work with
More informationRandom Variables, Sampling and Estimation
Chapter 1 Radom Variables, Samplig ad Estimatio 1.1 Itroductio This chapter will cover the most importat basic statistical theory you eed i order to uderstad the ecoometric material that will be comig
More informationPH 411/511 ECE B(k) Sin k (x) dk (1)
Fall-26 PH 4/5 ECE 598 A. La Rosa Homework-2 Due -3-26 The Homework is iteded to gai a uderstadig o the Heiseberg priciple, based o a compariso betwee the width of a pulse ad the width of its spectral
More informationProblem Set 4 Due Oct, 12
EE226: Radom Processes i Systems Lecturer: Jea C. Walrad Problem Set 4 Due Oct, 12 Fall 06 GSI: Assae Gueye This problem set essetially reviews detectio theory ad hypothesis testig ad some basic otios
More informationChapter 2 The Monte Carlo Method
Chapter 2 The Mote Carlo Method The Mote Carlo Method stads for a broad class of computatioal algorithms that rely o radom sampligs. It is ofte used i physical ad mathematical problems ad is most useful
More informationAccuracy. Computational Fluid Dynamics. Computational Fluid Dynamics. Computational Fluid Dynamics
http://www.d.edu/~gtryggva/cfd-course/ Computatioal Fluid Dyamics Lecture Jauary 3, 7 Grétar Tryggvaso It is clear that although the umerical solutio is qualitatively similar to the aalytical solutio,
More informationTMA4205 Numerical Linear Algebra. The Poisson problem in R 2 : diagonalization methods
TMA4205 Numerical Liear Algebra The Poisso problem i R 2 : diagoalizatio methods September 3, 2007 c Eiar M Røquist Departmet of Mathematical Scieces NTNU, N-749 Trodheim, Norway All rights reserved A
More informationSolutions to quizzes Math Spring 2007
to quizzes Math 4- Sprig 7 Name: Sectio:. Quiz a) x + x dx b) l x dx a) x + dx x x / + x / dx (/3)x 3/ + x / + c. b) Set u l x, dv dx. The du /x ad v x. By Itegratio by Parts, x(/x)dx x l x x + c. l x
More informationApproximate solutions for an acoustic plane wave propagation in a layer with high sound speed gradient
Proceedigs o Acoustics Victor Harbor 7- ovember, Victor Harbor, Australia Approximate solutios or a acoustic plae wave propagatio i a layer with high soud speed gradiet Alex Zioviev ad Adria D. Joes Maritime
More information10-701/ Machine Learning Mid-term Exam Solution
0-70/5-78 Machie Learig Mid-term Exam Solutio Your Name: Your Adrew ID: True or False (Give oe setece explaatio) (20%). (F) For a cotiuous radom variable x ad its probability distributio fuctio p(x), it
More informationDynamic Response of Second Order Mechanical Systems with Viscous Dissipation forces
Hadout #b (pp. 4-55) Dyamic Respose o Secod Order Mechaical Systems with Viscous Dissipatio orces M X + DX + K X = F t () Periodic Forced Respose to F (t) = F o si( t) ad F (t) = M u si(t) Frequecy Respose
More informationTopic 9 - Taylor and MacLaurin Series
Topic 9 - Taylor ad MacLauri Series A. Taylors Theorem. The use o power series is very commo i uctioal aalysis i act may useul ad commoly used uctios ca be writte as a power series ad this remarkable result
More informationBivariate Sample Statistics Geog 210C Introduction to Spatial Data Analysis. Chris Funk. Lecture 7
Bivariate Sample Statistics Geog 210C Itroductio to Spatial Data Aalysis Chris Fuk Lecture 7 Overview Real statistical applicatio: Remote moitorig of east Africa log rais Lead up to Lab 5-6 Review of bivariate/multivariate
More informationWe are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n
Review of Power Series, Power Series Solutios A power series i x - a is a ifiite series of the form c (x a) =c +c (x a)+(x a) +... We also call this a power series cetered at a. Ex. (x+) is cetered at
More informationNANYANG TECHNOLOGICAL UNIVERSITY SYLLABUS FOR ENTRANCE EXAMINATION FOR INTERNATIONAL STUDENTS AO-LEVEL MATHEMATICS
NANYANG TECHNOLOGICAL UNIVERSITY SYLLABUS FOR ENTRANCE EXAMINATION FOR INTERNATIONAL STUDENTS AO-LEVEL MATHEMATICS STRUCTURE OF EXAMINATION PAPER. There will be oe 2-hour paper cosistig of 4 questios.
More informationChapter 6 Principles of Data Reduction
Chapter 6 for BST 695: Special Topics i Statistical Theory. Kui Zhag, 0 Chapter 6 Priciples of Data Reductio Sectio 6. Itroductio Goal: To summarize or reduce the data X, X,, X to get iformatio about a
More informationTopic 9: Sampling Distributions of Estimators
Topic 9: Samplig Distributios of Estimators Course 003, 2016 Page 0 Samplig distributios of estimators Sice our estimators are statistics (particular fuctios of radom variables), their distributio ca be
More informationDiscrete Orthogonal Moment Features Using Chebyshev Polynomials
Discrete Orthogoal Momet Features Usig Chebyshev Polyomials R. Mukuda, 1 S.H.Og ad P.A. Lee 3 1 Faculty of Iformatio Sciece ad Techology, Multimedia Uiversity 75450 Malacca, Malaysia. Istitute of Mathematical
More informationOutline. Linear regression. Regularization functions. Polynomial curve fitting. Stochastic gradient descent for regression. MLE for regression
REGRESSION 1 Outlie Liear regressio Regularizatio fuctios Polyomial curve fittig Stochastic gradiet descet for regressio MLE for regressio Step-wise forward regressio Regressio methods Statistical techiques
More informationAxis Aligned Ellipsoid
Machie Learig for Data Sciece CS 4786) Lecture 6,7 & 8: Ellipsoidal Clusterig, Gaussia Mixture Models ad Geeral Mixture Models The text i black outlies high level ideas. The text i blue provides simple
More informationFourier Series and Transforms
Fourier Series ad rasorms Orthogoal uctios Fourier Series Discrete Fourier Series Fourier rasorm Chebyshev polyomials Scope: wearetryigto approimate a arbitrary uctio ad obtai basis uctios with appropriate
More informationEigenvalues and Eigenvectors
5 Eigevalues ad Eigevectors 5.3 DIAGONALIZATION DIAGONALIZATION Example 1: Let. Fid a formula for A k, give that P 1 1 = 1 2 ad, where Solutio: The stadard formula for the iverse of a 2 2 matrix yields
More informationTHE KALMAN FILTER RAUL ROJAS
THE KALMAN FILTER RAUL ROJAS Abstract. This paper provides a getle itroductio to the Kalma filter, a umerical method that ca be used for sesor fusio or for calculatio of trajectories. First, we cosider
More informationLast time: Moments of the Poisson distribution from its generating function. Example: Using telescope to measure intensity of an object
6.3 Stochastic Estimatio ad Cotrol, Fall 004 Lecture 7 Last time: Momets of the Poisso distributio from its geeratig fuctio. Gs () e dg µ e ds dg µ ( s) µ ( s) µ ( s) µ e ds dg X µ ds X s dg dg + ds ds
More informationLecture 22: Review for Exam 2. 1 Basic Model Assumptions (without Gaussian Noise)
Lecture 22: Review for Exam 2 Basic Model Assumptios (without Gaussia Noise) We model oe cotiuous respose variable Y, as a liear fuctio of p umerical predictors, plus oise: Y = β 0 + β X +... β p X p +
More informationName: Math 10550, Final Exam: December 15, 2007
Math 55, Fial Exam: December 5, 7 Name: Be sure that you have all pages of the test. No calculators are to be used. The exam lasts for two hours. Whe told to begi, remove this aswer sheet ad keep it uder
More informationLecture III-2: Light propagation in nonmagnetic
A. La Rosa Lecture Notes ALIED OTIC Lecture III2: Light propagatio i omagetic materials 2.1 urface ( ), volume ( ), ad curret ( j ) desities produced by arizatio charges The objective i this sectio is
More informationMihai V. Putz: Undergraduate Structural Physical Chemistry Course, Lecture 6 1
Mihai V. Putz: Udergraduate Structural Physical Chemistry Course, Lecture 6 Lecture 6: Quatum-Classical Correspodece I. Bohr s Correspodece Priciple Turig back to Bohr atomic descriptio it provides the
More informationFINALTERM EXAMINATION Fall 9 Calculus & Aalytical Geometry-I Questio No: ( Mars: ) - Please choose oe Let f ( x) is a fuctio such that as x approaches a real umber a, either from left or right-had-side,
More informationCO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS
CO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS C.PRAX ad H.SADAT Laboratoire d'etudes Thermiques,URA CNRS 403 40, Aveue du Recteur Pieau 86022 Poitiers Cedex,
More information1.3 Convergence Theorems of Fourier Series. k k k k. N N k 1. With this in mind, we state (without proof) the convergence of Fourier series.
.3 Covergece Theorems of Fourier Series I this sectio, we preset the covergece of Fourier series. A ifiite sum is, by defiitio, a limit of partial sums, that is, a cos( kx) b si( kx) lim a cos( kx) b si(
More informationImage Spaces. What might an image space be
Image Spaces What might a image space be Map each image to a poit i a space Defie a distace betwee two poits i that space Mabe also a shortest path (morph) We have alread see a simple versio of this, i
More information11 Correlation and Regression
11 Correlatio Regressio 11.1 Multivariate Data Ofte we look at data where several variables are recorded for the same idividuals or samplig uits. For example, at a coastal weather statio, we might record
More informationGrouping 2: Spectral and Agglomerative Clustering. CS 510 Lecture #16 April 2 nd, 2014
Groupig 2: Spectral ad Agglomerative Clusterig CS 510 Lecture #16 April 2 d, 2014 Groupig (review) Goal: Detect local image features (SIFT) Describe image patches aroud features SIFT, SURF, HoG, LBP, Group
More informationSolutions to Homework 1
Solutios to Homework MATH 36. Describe geometrically the sets of poits z i the complex plae defied by the followig relatios /z = z () Re(az + b) >, where a, b (2) Im(z) = c, with c (3) () = = z z = z 2.
More informationImage pyramid example
Multiresolutio image processig Laplacia pyramids Discrete Wavelet Trasform (DWT) Quadrature mirror filters ad cojugate quadrature filters Liftig ad reversible wavelet trasform Wavelet theory Berd Girod:
More informationMath Solutions to homework 6
Math 175 - Solutios to homework 6 Cédric De Groote November 16, 2017 Problem 1 (8.11 i the book): Let K be a compact Hermitia operator o a Hilbert space H ad let the kerel of K be {0}. Show that there
More informationResponse Variable denoted by y it is the variable that is to be predicted measure of the outcome of an experiment also called the dependent variable
Statistics Chapter 4 Correlatio ad Regressio If we have two (or more) variables we are usually iterested i the relatioship betwee the variables. Associatio betwee Variables Two variables are associated
More information1 Inferential Methods for Correlation and Regression Analysis
1 Iferetial Methods for Correlatio ad Regressio Aalysis I the chapter o Correlatio ad Regressio Aalysis tools for describig bivariate cotiuous data were itroduced. The sample Pearso Correlatio Coefficiet
More informationLinear regression. Daniel Hsu (COMS 4771) (y i x T i β)2 2πσ. 2 2σ 2. 1 n. (x T i β y i ) 2. 1 ˆβ arg min. β R n d
Liear regressio Daiel Hsu (COMS 477) Maximum likelihood estimatio Oe of the simplest liear regressio models is the followig: (X, Y ),..., (X, Y ), (X, Y ) are iid radom pairs takig values i R d R, ad Y
More informationPractical Spectral Anaysis (continue) (from Boaz Porat s book) Frequency Measurement
Practical Spectral Aaysis (cotiue) (from Boaz Porat s book) Frequecy Measuremet Oe of the most importat applicatios of the DFT is the measuremet of frequecies of periodic sigals (eg., siusoidal sigals),
More information10.6 ALTERNATING SERIES
0.6 Alteratig Series Cotemporary Calculus 0.6 ALTERNATING SERIES I the last two sectios we cosidered tests for the covergece of series whose terms were all positive. I this sectio we examie series whose
More informationCALCULUS BASIC SUMMER REVIEW
CALCULUS BASIC SUMMER REVIEW NAME rise y y y Slope of a o vertical lie: m ru Poit Slope Equatio: y y m( ) The slope is m ad a poit o your lie is, ). ( y Slope-Itercept Equatio: y m b slope= m y-itercept=
More informationSolutions Numerical Simulation - Homework, 4/15/ The DuFort-Frankel method is given by. f n. x 2. (a) Truncation error: Taylor expansion
Solutios Numerical Simulatio - Homework, 4/15/211 36. The DuFort-Frakel method is give by +1 1 = αl = α ( 2 t 2 1 1 +1 + +1 (a Trucatio error: Taylor epasio i +1 t = m [ m ] m= m! t m. (1 i Sice we cosider
More informationMIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS
MIDTERM 3 CALCULUS MATH 300 FALL 08 Moday, December 3, 08 5:5 PM to 6:45 PM Name PRACTICE EXAM S Please aswer all of the questios, ad show your work. You must explai your aswers to get credit. You will
More information18.S096: Homework Problem Set 1 (revised)
8.S096: Homework Problem Set (revised) Topics i Mathematics of Data Sciece (Fall 05) Afoso S. Badeira Due o October 6, 05 Exteded to: October 8, 05 This homework problem set is due o October 6, at the
More informationStochastic Processes
Stochastic Processes Review o Elemetar Probabilit Lecture I Hamid R. Rabiee Fall 20 Ali Jalali Outlie Histor/Philosoph Radom Variables Desit/Distributio Fuctios Joit/Coditioal Distributios Correlatio Importat
More informationAlgebra of Least Squares
October 19, 2018 Algebra of Least Squares Geometry of Least Squares Recall that out data is like a table [Y X] where Y collects observatios o the depedet variable Y ad X collects observatios o the k-dimesioal
More informationIntroduction to Optimization Techniques. How to Solve Equations
Itroductio to Optimizatio Techiques How to Solve Equatios Iterative Methods of Optimizatio Iterative methods of optimizatio Solutio of the oliear equatios resultig form a optimizatio problem is usually
More information3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,
3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [
More informationg p! where ω is a p-form. The operator acts on forms, not on components. Example: Consider R 3 with metric +++, i.e. g µν =
Chapter 17 Hodge duality We will ext defie the Hodge star operator. We will defieit i a chart rather tha abstractly. The Hodge star operator, deoted i a -dimesioal maifold is a map from p-forms to ( p)-forms
More informationNBHM QUESTION 2007 Section 1 : Algebra Q1. Let G be a group of order n. Which of the following conditions imply that G is abelian?
NBHM QUESTION 7 NBHM QUESTION 7 NBHM QUESTION 7 Sectio : Algebra Q Let G be a group of order Which of the followig coditios imply that G is abelia? 5 36 Q Which of the followig subgroups are ecesarily
More informationOrthogonal transformations
Orthogoal trasformatios October 12, 2014 1 Defiig property The squared legth of a vector is give by takig the dot product of a vector with itself, v 2 v v g ij v i v j A orthogoal trasformatio is a liear
More informationApply change-of-basis formula to rewrite x as a linear combination of eigenvectors v j.
Eigevalue-Eigevector Istructor: Nam Su Wag eigemcd Ay vector i real Euclidea space of dimesio ca be uiquely epressed as a liear combiatio of liearly idepedet vectors (ie, basis) g j, j,,, α g α g α g α
More informationOrthogonal Gaussian Filters for Signal Processing
Orthogoal Gaussia Filters for Sigal Processig Mark Mackezie ad Kiet Tieu Mechaical Egieerig Uiversity of Wollogog.S.W. Australia Abstract A Gaussia filter usig the Hermite orthoormal series of fuctios
More informationCHAPTER 6d. NUMERICAL INTERPOLATION
CHAPER 6d. NUMERICAL INERPOLAION A. J. Clark School o Egieerig Departmet o Civil ad Evirometal Egieerig by Dr. Ibrahim A. Assakka Sprig ENCE - Computatio Methods i Civil Egieerig II Departmet o Civil ad
More informationSCORE. Exam 2. MA 114 Exam 2 Fall 2016
MA 4 Exam Fall 06 Exam Name: Sectio ad/or TA: Do ot remove this aswer page you will retur the whole exam. You will be allowed two hours to complete this test. No books or otes may be used. You may use
More informationContinuous Domain Analysis of Graph Laplacian Regularization for Image Denoisng. Presenter: Gene Cheung National Institute of Informatics
Cotiuous Domai Aalysis of Graph Laplacia Regularizatio for Image Deoisg Preseter: Gee Cheug atioal Istitute of Iformatics [1] Jiahao Pag, Gee Cheug, Wei Hu, Oscar C. Au, "Redefiig Self-Similarity i atural
More informationLog1 Contest Round 1 Theta Equations & Inequalities. 4 points each. 5 points each. 7, a c d. 9, find the value of the product abcd.
013 01 Log1 Cotest Roud 1 Theta Equatios & Iequalities Name: poits each 1 Solve for x : x 3 38 Fid the greatest itegral value of x satisfyig the iequality x x 3 7 1 3 3 xy71 Fid the ordered pair solutio
More information