ECE 472/572 - Digital Image Processing. Roadmap. Questions. Lecture 6 Geometric and Radiometric Transformation 09/27/11
|
|
- Marilynn Bryan
- 5 years ago
- Views:
Transcription
1 ECE 472/572 - Dgtal Image Processng Lecture 6 Geometrc and Radometrc Transformaton 09/27/ Roadmap Introducton Image format vector vs. btmap IP vs. CV vs. CG HLIP vs. LLIP Image acquston Percepton Structure of human ee Brghtness adaptaton and Dscrmnaton Image resoluton Image enhancement Enhancement vs. restoraton Spatal doman methods Pont-based methods Log trans. vs. Power-law Contrast stretchng vs. HE Gra-level vs. Bt plane slcng Image averagng prncple Mask-based methods - spatal flter Smoothng vs. Sharpenng flter Lnear vs. Non-lnear flter Smoothng average vs. Gaussan vs. medan Sharpenng UM vs. st vs. 2nd dervatves Frequenc doman methods Understandng Fourer transform Implementaton n the frequenc doman Low-pass flters vs. hgh-pass flters vs. homomorphc flter Geometrc correcton Affne vs. Perspectve Homogeneous coordnates Inverse vs. forward transform Composte General Model dstorton wth polnomal Least square soluton 2 Questons Affne vs. Perspectve Forward vs. Inverse Composte vs. Sequental Homogeneous coordnate General geometrc s 3
2 Usage Image correcton Color nterpolaton Forensc analss Entertanment effect Affne s " u " a Preserve lnes and parallel lnes a 2 a 3 " x Homogeneous coordnates v a 2 a 22 a General form a a2 a3! a2 a22 a23! 0 0!" Specal matrces R: rotaton, S: scalng, T: translaton, H: shear cosθ snθ 0 sx tx hx 0 R snθ cosθ 0,S 0 s 0,T 0 t,h h
3 3 7 Composte vs. Sequental Orgnal Image fx, R H T S Transformed Image gu, v u v " S T H R x " R H T S C 8 Forward vs. Inverse transforms u v " C x " Forward transform C u v x Inverse transform 9 Examples - Shear h 0.2 hx 0.2 hx h 0.2
4 Examples Translaton + Rotaton theta PI/4 theta PI/4 tx -40, t 60 0 Perspectve Preserve parallel lnes onl when the are parallel to the projecton plane. Otherwse, lnes converge to a vanshng pont General form " a a 2 a 3 a 2 a 22 a 23 a 3 0, a 32 0 a 3 a 32 u " a a 2 a 3 x v " a 2 a 22 a 23,u u " w ",v v " w " w " a 3 a 32 Determne the coeffcents u " a a 2 a 3 x v " a 2 a 22 a 23,u u " w ",v v " w " w " a 3 a 32 8 unknowns, 4-pont least squares 0,0 0,255 0,0 0, ,0 255, ,0 5,5 2 4
5 Example - PT 3 General approaches Fnd teponts Spatal 4 Example CCD buttng msalgnment greater than 50 mcron x-ra senstve scntllator fber optcs CCD arra 242 x 52 9/27/ 5 5
6 Sources of dstortons defects n the producton of fber-optc tapers mperfect compresson and cuttng dfferent lght transfer effcenc across the whole surface 9/27/ 6 Geometrc correcton map close approxmaton P u, v x, control pont nterpolaton T u, v x, x, u, v map exactl 9/27/ 7 Spatal Blnear equaton x ˆ r u,v a u + a 2 v + a 3 uv + a 4 ˆ s u,v b u + b 2 v + b 3 uv + b 4 n-th degree polnomal " x ˆ " ˆ P xu,v d " a krs u r s v P u,v b krs u r s k 0 r+s k v Use nformaton from teponts to solve coeffcents Exact soluton Least square soluton ε mn m 2 2 a, b [ x xˆ + ˆ ] 0 8 6
7 How s t appled? Step : Choose a set of te ponts x, : coordnates of te ponts n the orgnal or dstorted mage u,v : coordnates of te ponts n the corrected mage Step 2: Decde on whch degree of polnomal to use to model the nverse of the dstorton, e.g., x ˆ r u,v a u + a 2 v + a 3 uv + a 4 ˆ s u,v b u + b 2 v + b 3 uv + b 4 Step 3: Solve the coeffcents of the polnomal usng least-squares approach Step 4: Use the derved polnomal model to correct the entre orgnal mage X [ x 0 x x 24 ] T Y [ 0 24 ] T " u 0 v 0 u 0 v 0 u W v u v u 24 v 24 u 24 v 24 A W X,B W Y W W T W W T A [ a a 2 a 3 a 4 ] T B [ b b 2 b 3 b 4 ] T For each u,v n the corrected mage, fnd the correspondng x, n the orgnal mage and use ts ntenst as the ntenst at u,v. 9 Example Geometrc correcton Geometrc correcton of mages from butted CCD arras 20 Example - Color correcton Teponts are colors R, G, B, nstead of spatal coordnates 2 7
8 Example - Image warpng 22 Image warpng Two-pass mesh warpng b Douglas Smthe Reference: G. Wolberg, Dgtal Image Warpng, Example From Joe Howell and Cor McKa, ECE472, Fall
9 Example 2 From Adam Mller, Truman Bonds, Randal Waldrop, ECE472, Fall
Report on Image warping
Report on Image warpng Xuan Ne, Dec. 20, 2004 Ths document summarzed the algorthms of our mage warpng soluton for further study, and there s a detaled descrpton about the mplementaton of these algorthms.
More informationLecture Topics VMSC Prof. Dr.-Ing. habil. Hermann Lödding Prof. Dr.-Ing. Wolfgang Hintze. PD Dr.-Ing. habil.
Lecture Topcs 1. Introducton 2. Sensor Gudes Robots / Machnes 3. Motvaton Model Calbraton 4. 3D Vdeo Metrc (Geometrcal Camera Model) 5. Grey Level Pcture Processng for Poston Measurement 6. Lght and Percepton
More informationFourier Transform. Additive noise. Fourier Tansform. I = S + N. Noise doesn t depend on signal. We ll consider:
Flterng Announcements HW2 wll be posted later today Constructng a mosac by warpng mages. CSE252A Lecture 10a Flterng Exampel: Smoothng by Averagng Kernel: (From Bll Freeman) m=2 I Kernel sze s m+1 by m+1
More informationTutorial 2. COMP4134 Biometrics Authentication. February 9, Jun Xu, Teaching Asistant
Tutoral 2 COMP434 ometrcs uthentcaton Jun Xu, Teachng sstant csjunxu@comp.polyu.edu.hk February 9, 207 Table of Contents Problems Problem : nswer the questons Problem 2: Power law functon Problem 3: Convoluton
More informationThe Fourier Transform
e Processng ourer Transform D The ourer Transform Effcent Data epresentaton Dscrete ourer Transform - D Contnuous ourer Transform - D Eamples + + + Jean Baptste Joseph ourer Effcent Data epresentaton Data
More informationBruce A. Draper & J. Ross Beveridge, January 25, Geometric Image Manipulation. Lecture #1 January 25, 2013
Brce A. Draper & J. Ross Beerdge, Janar 5, Geometrc Image Manplaton Lectre # Janar 5, Brce A. Draper & J. Ross Beerdge, Janar 5, Image Manplaton: Contet To start wth the obos, an mage s a D arra of pels
More information1 Matrix representations of canonical matrices
1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:
More informationCSci 6974 and ECSE 6966 Math. Tech. for Vision, Graphics and Robotics Lecture 21, April 17, 2006 Estimating A Plane Homography
CSc 6974 and ECSE 6966 Math. Tech. for Vson, Graphcs and Robotcs Lecture 21, Aprl 17, 2006 Estmatng A Plane Homography Overvew We contnue wth a dscusson of the major ssues, usng estmaton of plane projectve
More informationAutonomous On-orbit Calibration Approaches for Star Trackers. D. Todd Griffith
Autonomous On-orbt Calbraton Approaches for Star racers D. odd Grffth Colleagues Dr. John L. Junns (Graduate Adsor) Mala Samaan Puneet Sngla eas A&M Unerst Department of Aerospace Engneerng AMU College
More informationChange Detection: Current State of the Art and Future Directions
Change Detecton: Current State of the Art and Future Drectons Dapeng Olver Wu Electrcal & Computer Engneerng Unversty of Florda http://www.wu.ece.ufl.edu/ Outlne Motvaton & problem statement Change detecton
More informationTransform Coding. Transform Coding Principle
Transform Codng Prncple of block-wse transform codng Propertes of orthonormal transforms Dscrete cosne transform (DCT) Bt allocaton for transform coeffcents Entropy codng of transform coeffcents Typcal
More informationCS4495/6495 Introduction to Computer Vision. 3C-L3 Calibrating cameras
CS4495/6495 Introducton to Computer Vson 3C-L3 Calbratng cameras Fnally (last tme): Camera parameters Projecton equaton the cumulatve effect of all parameters: M (3x4) f s x ' 1 0 0 0 c R 0 I T 3 3 3 x1
More informationInvariant deformation parameters from GPS permanent networks using stochastic interpolation
Invarant deformaton parameters from GPS permanent networks usng stochastc nterpolaton Ludovco Bag, Poltecnco d Mlano, DIIAR Athanasos Dermans, Arstotle Unversty of Thessalonk Outlne Startng hypotheses
More informationStructure from Motion. Forsyth&Ponce: Chap. 12 and 13 Szeliski: Chap. 7
Structure from Moton Forsyth&once: Chap. 2 and 3 Szelsk: Chap. 7 Introducton to Structure from Moton Forsyth&once: Chap. 2 Szelsk: Chap. 7 Structure from Moton Intro he Reconstructon roblem p 3?? p p 2
More informationADAPTIVE IMAGE FILTERING
Why adaptve? ADAPTIVE IMAGE FILTERING average detals and contours are aected Averagng should not be appled n contour / detals regons. Adaptaton Adaptaton = modyng the parameters o a prrocessng block accordng
More informationFormulas for the Determinant
page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use
More informationTHE ASTER IMAGES FOR THE ENVIRONMENTAL MONITORING
Dpartmento d Ingegnera per l Ambente e lo Svluppo Sostenble Facoltà d Ingegnera d Taranto POLITECNICO DI BARI THE ASTER IMAGES FOR THE ENVIRONMENTAL MONITORING M. G. Angeln, D. Costantno 4 WORKSHOP TEMATICO
More informationReview: Fit a line to N data points
Revew: Ft a lne to data ponts Correlated parameters: L y = a x + b Orthogonal parameters: J y = a (x ˆ x + b For ntercept b, set a=0 and fnd b by optmal average: ˆ b = y, Var[ b ˆ ] = For slope a, set
More informationCS 468 Lecture 16: Isometry Invariance and Spectral Techniques
CS 468 Lecture 16: Isometry Invarance and Spectral Technques Justn Solomon Scrbe: Evan Gawlk Introducton. In geometry processng, t s often desrable to characterze the shape of an object n a manner that
More informationLectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix
Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could
More informationImage Processing for Bubble Detection in Microfluidics
Image Processng for Bubble Detecton n Mcrofludcs Introducton Chen Fang Mechancal Engneerng Department Stanford Unverst Startng from recentl ears, mcrofludcs devces have been wdel used to buld the bomedcal
More informationVideo Data Analysis. Video Data Analysis, B-IT. Lecture plan:
Vdeo Data Analss Image eatures Spatal lterng Lecture plan:. Medan lterng. Derental lters 3. Image eatures -> > mage edges 4. Edge detectors usng rst-order dervatve 5. Edge detectors usng second-order order
More informationIntegrals and Invariants of Euler-Lagrange Equations
Lecture 16 Integrals and Invarants of Euler-Lagrange Equatons ME 256 at the Indan Insttute of Scence, Bengaluru Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng,
More informationAERODYNAMICS I LECTURE 6 AERODYNAMICS OF A WING FUNDAMENTALS OF THE LIFTING-LINE THEORY
LECTURE 6 AERODYNAMICS OF A WING FUNDAMENTALS OF THE LIFTING-LINE THEORY The Bot-Savart Law The velocty nduced by the sngular vortex lne wth the crculaton can be determned by means of the Bot- Savart formula
More informationConvexity preserving interpolation by splines of arbitrary degree
Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete
More informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationOriginated from experimental optimization where measurements are very noisy Approximation can be actually more accurate than
Surrogate (approxmatons) Orgnated from expermental optmzaton where measurements are ver nos Approxmaton can be actuall more accurate than data! Great nterest now n applng these technques to computer smulatons
More informationρ some λ THE INVERSE POWER METHOD (or INVERSE ITERATION) , for , or (more usually) to
THE INVERSE POWER METHOD (or INVERSE ITERATION) -- applcaton of the Power method to A some fxed constant ρ (whch s called a shft), x λ ρ If the egenpars of A are { ( λ, x ) } ( ), or (more usually) to,
More informationA NOTE ON CES FUNCTIONS Drago Bergholt, BI Norwegian Business School 2011
A NOTE ON CES FUNCTIONS Drago Bergholt, BI Norwegan Busness School 2011 Functons featurng constant elastcty of substtuton CES are wdely used n appled economcs and fnance. In ths note, I do two thngs. Frst,
More informationCOMPUTATIONALLY EFFICIENT WAVELET AFFINE INVARIANT FUNCTIONS FOR SHAPE RECOGNITION. Erdem Bala, Dept. of Electrical and Computer Engineering,
COMPUTATIONALLY EFFICIENT WAVELET AFFINE INVARIANT FUNCTIONS FOR SHAPE RECOGNITION Erdem Bala, Dept. of Electrcal and Computer Engneerng, Unversty of Delaware, 40 Evans Hall, Newar, DE, 976 A. Ens Cetn,
More informationInstituto Tecnológico de Aeronáutica FINITE ELEMENTS I. Class notes AE-245
Insttuto Tecnológco de Aeronáutca FIITE ELEMETS I Class notes AE-5 Insttuto Tecnológco de Aeronáutca 5. Isoparametrc Elements AE-5 Insttuto Tecnológco de Aeronáutca ISOPARAMETRIC ELEMETS Introducton What
More informationError Bars in both X and Y
Error Bars n both X and Y Wrong ways to ft a lne : 1. y(x) a x +b (σ x 0). x(y) c y + d (σ y 0) 3. splt dfference between 1 and. Example: Prmordal He abundance: Extrapolate ft lne to [ O / H ] 0. [ He
More informationThe Geometry of Logit and Probit
The Geometry of Logt and Probt Ths short note s meant as a supplement to Chapters and 3 of Spatal Models of Parlamentary Votng and the notaton and reference to fgures n the text below s to those two chapters.
More informationACTM State Calculus Competition Saturday April 30, 2011
ACTM State Calculus Competton Saturday Aprl 30, 2011 ACTM State Calculus Competton Sprng 2011 Page 1 Instructons: For questons 1 through 25, mark the best answer choce on the answer sheet provde Afterward
More informationProblem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?
Homework 8 solutons. Problem 16.1. Whch of the followng defne homomomorphsms from C\{0} to C\{0}? Answer. a) f 1 : z z Yes, f 1 s a homomorphsm. We have that z s the complex conjugate of z. If z 1,z 2
More informationANALYSIS OF ELECTROMAGNETIC FIELD USING THE CONSTRAINED INTERPOLATION PROFILE METHOD PHÂN TÍCH TRƯỜNG ĐIỆN TỪ SỬ DỤNG PHƯƠNG PHÁP CIP
ANALYSIS OF ELECTROMAGNETIC FIELD USING THE CONSTRAINED INTERPOLATION PROFILE METHOD PHÂN TÍCH TRƯỜNG ĐIỆN TỪ SỬ DỤNG PHƯƠNG PHÁP CIP LÊ VŨ HƯNG Cao đẳng kỹ thuật quốc ga Kushro, Nhật Bản Kushro Natonal
More informationIMGS-261 Solutions to Homework #9
IMGS-6 Solutons to Homework #9. For f [] SINC [] sn[π], use the modulaton theorem to evaluate and sketch π the Fourer transform of f [] f [] f [] (f []) Soluton: We know that F{RECT []} SINC [] so we use
More informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationProblem adapted reduced models based on Reaction-Diffusion Manifolds (REDIMs)
Problem adapted reduced models based on Reacton-Dffuson Manfolds (REDIMs) V Bykov, U Maas Thrty-Second Internatonal Symposum on ombuston, Montreal, anada, 3-8 August, 8 Problem Statement: Smulaton of reactng
More informationRigid body simulation
Rgd bod smulaton Rgd bod smulaton Once we consder an object wth spacal etent, partcle sstem smulaton s no longer suffcent Problems Problems Unconstraned sstem rotatonal moton torques and angular momentum
More informationALGORITHM FOR THE CALCULATION OF THE TWO VARIABLES CUBIC SPLINE FUNCTION
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I. CUZA DIN IAŞI (S.N.) MATEMATICĂ, Tomul LIX, 013, f.1 DOI: 10.478/v10157-01-00-y ALGORITHM FOR THE CALCULATION OF THE TWO VARIABLES CUBIC SPLINE FUNCTION BY ION
More informationTensor Analysis. For orthogonal curvilinear coordinates, ˆ ˆ (98) Expanding the derivative, we have, ˆ. h q. . h q h q
For orthogonal curvlnear coordnates, eˆ grad a a= ( aˆ ˆ e). h q (98) Expandng the dervatve, we have, eˆ aˆ ˆ e a= ˆ ˆ a h e + q q 1 aˆ ˆ ˆ a e = ee ˆˆ ˆ + e. h q h q Now expandng eˆ / q (some of the detals
More informationModelli Clamfim Equazione del Calore Lezione ottobre 2014
CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g
More informationGEMINI GEneric Multimedia INdexIng
GEMINI GEnerc Multmeda INdexIng Last lecture, LSH http://www.mt.edu/~andon/lsh/ Is there another possble soluton? Do we need to perform ANN? 1 GEnerc Multmeda INdexIng dstance measure Sub-pattern Match
More informationModeling curves. Graphs: y = ax+b, y = sin(x) Implicit ax + by + c = 0, x 2 +y 2 =r 2 Parametric:
Modelng curves Types of Curves Graphs: y = ax+b, y = sn(x) Implct ax + by + c = 0, x 2 +y 2 =r 2 Parametrc: x = ax + bxt x = cos t y = ay + byt y = snt Parametrc are the most common mplct are also used,
More informationQuantum Mechanics I - Session 4
Quantum Mechancs I - Sesson 4 Aprl 3, 05 Contents Operators Change of Bass 4 3 Egenvectors and Egenvalues 5 3. Denton....................................... 5 3. Rotaton n D....................................
More information8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before
.1 Arc Length hat s the length of a curve? How can we approxmate t? e could do t followng the pattern we ve used before Use a sequence of ncreasngly short segments to approxmate the curve: As the segments
More information9 Characteristic classes
THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct
More informationA NEW DISCRETE WAVELET TRANSFORM
A NEW DISCRETE WAVELET TRANSFORM ALEXANDRU ISAR, DORINA ISAR Keywords: Dscrete wavelet, Best energy concentraton, Low SNR sgnals The Dscrete Wavelet Transform (DWT) has two parameters: the mother of wavelets
More informationMEM 255 Introduction to Control Systems Review: Basics of Linear Algebra
MEM 255 Introducton to Control Systems Revew: Bascs of Lnear Algebra Harry G. Kwatny Department of Mechancal Engneerng & Mechancs Drexel Unversty Outlne Vectors Matrces MATLAB Advanced Topcs Vectors A
More informationJAB Chain. Long-tail claims development. ASTIN - September 2005 B.Verdier A. Klinger
JAB Chan Long-tal clams development ASTIN - September 2005 B.Verder A. Klnger Outlne Chan Ladder : comments A frst soluton: Munch Chan Ladder JAB Chan Chan Ladder: Comments Black lne: average pad to ncurred
More informationAPPROXIMATE PRICES OF BASKET AND ASIAN OPTIONS DUPONT OLIVIER. Premia 14
APPROXIMAE PRICES OF BASKE AND ASIAN OPIONS DUPON OLIVIER Prema 14 Contents Introducton 1 1. Framewor 1 1.1. Baset optons 1.. Asan optons. Computng the prce 3. Lower bound 3.1. Closed formula for the prce
More informationPHYS 705: Classical Mechanics. Calculus of Variations II
1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary
More informationThe Fundamental Theorem of Algebra. Objective To use the Fundamental Theorem of Algebra to solve polynomial equations with complex solutions
5-6 The Fundamental Theorem of Algebra Content Standards N.CN.7 Solve quadratc equatons wth real coeffcents that have comple solutons. N.CN.8 Etend polnomal denttes to the comple numbers. Also N.CN.9,
More informationAffine transformations and convexity
Affne transformatons and convexty The purpose of ths document s to prove some basc propertes of affne transformatons nvolvng convex sets. Here are a few onlne references for background nformaton: http://math.ucr.edu/
More information5.04, Principles of Inorganic Chemistry II MIT Department of Chemistry Lecture 32: Vibrational Spectroscopy and the IR
5.0, Prncples of Inorganc Chemstry II MIT Department of Chemstry Lecture 3: Vbratonal Spectroscopy and the IR Vbratonal spectroscopy s confned to the 00-5000 cm - spectral regon. The absorpton of a photon
More informationProblems & Techniques
Vsual Moton Estmaton Problems & Technques Prnceton Unversty COS 429 Lecture Oct. 11, 2007 Harpreet S. Sawhney hsawhney@sarnoff.com Outlne 1. Vsual moton n the Real World 2. The vsual moton estmaton problem
More informationCentre of Rotation Determination Using Projection Data in X-ray Micro Computed Tomography
Insttutonen för medcn och vård Avdelnngen för radofysk Hälsounverstetet Centre of Rotaton Determnaton Usng Proecton Data n X-ray Mcro Computed Tomography Brger Olander Department of Medcne and Care Rado
More information5.62 Physical Chemistry II Spring 2008
MIT OpenCourseWare http://ocw.mt.edu 5.62 Physcal Chemstry II Sprng 2008 For nformaton about ctng these materals or our Terms of Use, vst: http://ocw.mt.edu/terms. 5.62 Sprng 2008 Lecture 34 Page Transton
More informationImportant Instructions to the Examiners:
Summer 0 Examnaton Subject & Code: asc Maths (70) Model Answer Page No: / Important Instructons to the Examners: ) The Answers should be examned by key words and not as word-to-word as gven n the model
More informationNumerical Methods. ME Mechanical Lab I. Mechanical Engineering ME Lab I
5 9 Mechancal Engneerng -.30 ME Lab I ME.30 Mechancal Lab I Numercal Methods Volt Sne Seres.5 0.5 SIN(X) 0 3 7 5 9 33 37 4 45 49 53 57 6 65 69 73 77 8 85 89 93 97 0-0.5 Normalzed Squared Functon - 0.07
More informationSome Comments on Accelerating Convergence of Iterative Sequences Using Direct Inversion of the Iterative Subspace (DIIS)
Some Comments on Acceleratng Convergence of Iteratve Sequences Usng Drect Inverson of the Iteratve Subspace (DIIS) C. Davd Sherrll School of Chemstry and Bochemstry Georga Insttute of Technology May 1998
More informationImpulse Noise Removal Technique Based on Fuzzy Logic
Impulse Nose Removal Technque Based on Fuzzy Logc 1 Mthlesh Atulkar, 2 A.S. Zadgaonkar and 3 Sanjay Kumar C V Raman Unversty, Kota, Blaspur, Inda 1 m.atulkar@gmal.com, 2 arunzad28@hotmal.com, 3 sanrapur@redffmal.com
More information= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system.
Chapter Matlab Exercses Chapter Matlab Exercses. Consder the lnear system of Example n Secton.. x x x y z y y z (a) Use the MATLAB command rref to solve the system. (b) Let A be the coeffcent matrx and
More informationHowever, since P is a symmetric idempotent matrix, of P are either 0 or 1 [Eigen-values
Fall 007 Soluton to Mdterm Examnaton STAT 7 Dr. Goel. [0 ponts] For the general lnear model = X + ε, wth uncorrelated errors havng mean zero and varance σ, suppose that the desgn matrx X s not necessarly
More informationTHE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens
THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of
More informationTurbulence. Lecture 21. Non-linear Dynamics. 30 s & 40 s Taylor s work on homogeneous turbulence Kolmogorov.
Turbulence Lecture 1 Non-lnear Dynamcs Strong non-lnearty s a key feature of turbulence. 1. Unstable, chaotc behavor.. Strongly vortcal (vortex stretchng) 3 s & 4 s Taylor s work on homogeneous turbulence
More informationAffine and Riemannian Connections
Affne and Remannan Connectons Semnar Remannan Geometry Summer Term 2015 Prof Dr Anna Wenhard and Dr Gye-Seon Lee Jakob Ullmann Notaton: X(M) space of smooth vector felds on M D(M) space of smooth functons
More informationCOMPLEX NUMBERS AND QUADRATIC EQUATIONS
COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not
More information12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA. 4. Tensor product
12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA Here s an outlne of what I dd: (1) categorcal defnton (2) constructon (3) lst of basc propertes (4) dstrbutve property (5) rght exactness (6) localzaton
More informationTHE VIBRATIONS OF MOLECULES II THE CARBON DIOXIDE MOLECULE Student Instructions
THE VIBRATIONS OF MOLECULES II THE CARBON DIOXIDE MOLECULE Student Instructons by George Hardgrove Chemstry Department St. Olaf College Northfeld, MN 55057 hardgrov@lars.acc.stolaf.edu Copyrght George
More informationMAE140 - Linear Circuits - Winter 16 Final, March 16, 2016
ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have
More informationRECONSTRUCTION OF NON- CARTESIAN DATA USING BURS/RBURS ALGORITHM
EE-591 MAGNETIC RESONANCE IMAGING TERM PROJECT RECONSTRUCTION OF NON- CARTESIAN DATA USING BURS/RBURS ALGORITHM Zheng L Department of Electrcal Engneerng December 5, 2004 1 1. INTRODUCTION There are many
More informationCausal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim
Causal Damonds M. Aghl, L. Bombell, B. Plgrm Introducton The correcton to volume of a causal nterval due to curvature of spacetme has been done by Myrhem [] and recently by Gbbons & Solodukhn [] and later
More informationA New Design Approach for Recursive Diamond-Shaped Filters
A ew Desgn Approach for Recursve Damond-Shaped Flters RADU MATEI Faculty of Electroncs, Telecommuncatons and Informaton Technology Techncal Unversty Gh.Asach Bd. Carol I no., Ias 756 ROMAIA rmate@etc.tuas.ro
More informationNON-LINEAR CONVOLUTION: A NEW APPROACH FOR THE AURALIZATION OF DISTORTING SYSTEMS
NON-LINEAR CONVOLUTION: A NEW APPROAC FOR TE AURALIZATION OF DISTORTING SYSTEMS Angelo Farna, Alberto Belln and Enrco Armellon Industral Engneerng Dept., Unversty of Parma, Va delle Scenze 8/A Parma, 00
More informationLecture 6/7 (February 10/12, 2014) DIRAC EQUATION. The non-relativistic Schrödinger equation was obtained by noting that the Hamiltonian 2
P470 Lecture 6/7 (February 10/1, 014) DIRAC EQUATION The non-relatvstc Schrödnger equaton was obtaned by notng that the Hamltonan H = P (1) m can be transformed nto an operator form wth the substtutons
More informationFeb 14: Spatial analysis of data fields
Feb 4: Spatal analyss of data felds Mappng rregularly sampled data onto a regular grd Many analyss technques for geophyscal data requre the data be located at regular ntervals n space and/or tme. hs s
More informationCS 523: Computer Graphics, Spring Shape Modeling. PCA Applications + SVD. Andrew Nealen, Rutgers, /15/2011 1
CS 523: Computer Graphcs, Sprng 20 Shape Modelng PCA Applcatons + SVD Andrew Nealen, utgers, 20 2/5/20 emnder: PCA Fnd prncpal components of data ponts Orthogonal drectons that are domnant n the data (have
More informationGeometrical Optics Mirrors and Prisms
Phy 322 Lecture 4 Chapter 5 Geometrcal Optc Mrror and Prm Optcal bench http://webphyc.davdon.edu/applet/optc4/default.html Mrror Ancent bronze mrror Hubble telecope mrror Lqud mercury mrror Planar mrror
More informationLinear Approximation with Regularization and Moving Least Squares
Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...
More informationSpatial Statistics and Analysis Methods (for GEOG 104 class).
Spatal Statstcs and Analyss Methods (for GEOG 104 class). Provded by Dr. An L, San Dego State Unversty. 1 Ponts Types of spatal data Pont pattern analyss (PPA; such as nearest neghbor dstance, quadrat
More informationNew Method for Solving Poisson Equation. on Irregular Domains
Appled Mathematcal Scences Vol. 6 01 no. 8 369 380 New Method for Solvng Posson Equaton on Irregular Domans J. Izadan and N. Karamooz Department of Mathematcs Facult of Scences Mashhad BranchIslamc Azad
More informationSignal space Review on vector space Linear independence Metric space and norm Inner product
Sgnal space.... Revew on vector space.... Lnear ndependence... 3.3 Metrc space and norm... 4.4 Inner product... 5.5 Orthonormal bass... 7.6 Waveform communcaton system... 9.7 Some examples... 6 Sgnal space
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationLecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES
COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve
More informationOPTIMISATION. Introduction Single Variable Unconstrained Optimisation Multivariable Unconstrained Optimisation Linear Programming
OPTIMIATION Introducton ngle Varable Unconstraned Optmsaton Multvarable Unconstraned Optmsaton Lnear Programmng Chapter Optmsaton /. Introducton In an engneerng analss, sometmes etremtes, ether mnmum or
More informationx yi In chapter 14, we want to perform inference (i.e. calculate confidence intervals and perform tests of significance) in this setting.
The Practce of Statstcs, nd ed. Chapter 14 Inference for Regresson Introducton In chapter 3 we used a least-squares regresson lne (LSRL) to represent a lnear relatonshp etween two quanttatve explanator
More informationComputational Astrophysics
Computatonal Astrophyscs Solvng for Gravty Alexander Knebe, Unversdad Autonoma de Madrd Computatonal Astrophyscs Solvng for Gravty the equatons full set of equatons collsonless matter (e.g. dark matter
More informationCanonical transformations
Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,
More informationSolutions to Homework 7, Mathematics 1. 1 x. (arccos x) (arccos x) 1
Solutons to Homework 7, Mathematcs 1 Problem 1: a Prove that arccos 1 1 for 1, 1. b* Startng from the defnton of the dervatve, prove that arccos + 1, arccos 1. Hnt: For arccos arccos π + 1, the defnton
More informationGaussian Conditional Random Field Network for Semantic Segmentation - Supplementary Material
Gaussan Condtonal Random Feld Networ for Semantc Segmentaton - Supplementary Materal Ravtea Vemulapall, Oncel Tuzel *, Mng-Yu Lu *, and Rama Chellappa Center for Automaton Research, UMIACS, Unversty of
More informationModal Identification of the Elastic Properties in Composite Sandwich Structures
Modal Identfcaton of the Elastc Propertes n Composte Sandwch Structures M. Matter Th. Gmür J. Cugnon and A. Schorderet School of Engneerng (STI) Ecole poltechnque fédérale f de Lausanne (EPFL) Swterland
More informationDevelopment of a Semi-Automated Approach for Regional Corrector Surface Modeling in GPS-Levelling
Development of a Sem-Automated Approach for Regonal Corrector Surface Modelng n GPS-Levellng G. Fotopoulos, C. Kotsaks, M.G. Sders, and N. El-Shemy Presented at the Annual Canadan Geophyscal Unon Meetng
More informationWorkshop: Approximating energies and wave functions Quantum aspects of physical chemistry
Workshop: Approxmatng energes and wave functons Quantum aspects of physcal chemstry http://quantum.bu.edu/pltl/6/6.pdf Last updated Thursday, November 7, 25 7:9:5-5: Copyrght 25 Dan Dll (dan@bu.edu) Department
More informationNMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582
NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582 4. Moton Knematcs 4.2 Angular Velocty Knematcs Summary From the last lecture we concluded that: If the jonts
More informationC/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1
C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned
More informationAssessing inter-annual and seasonal variability Least square fitting with Matlab: Application to SSTs in the vicinity of Cape Town
Assessng nter-annual and seasonal varablty Least square fttng wth Matlab: Applcaton to SSTs n the vcnty of Cape Town Francos Dufos Department of Oceanography/ MARE nsttute Unversty of Cape Town Introducton
More informationLecture 3. Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab. 13- Jan- 15.
Lecture Caera Models Caera Calbraton rofessor Slvo Savarese Coputatonal Vson and Geoetry Lab Slvo Savarese Lecture - - Jan- 5 Lecture Caera Models Caera Calbraton Recap of caera odels Caera calbraton proble
More informationInner Product. Euclidean Space. Orthonormal Basis. Orthogonal
Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,
More information