GEOMETRY FOR 3D COMPUTER VISION

Size: px
Start display at page:

Download "GEOMETRY FOR 3D COMPUTER VISION"

Transcription

1 GEOMETRY FOR 3D COMPUTER VISION 1/29 Válav Hlaváč Czeh Tehnial University, Faulty of Eletrial Engineering Department of Cybernetis, Center for Mahine Pereption Praha 2, Karlovo nám. 13, Czeh Republi LECTURE PLAN 1. Brief introdution to my group Center for Mahine Pereption. 2. Mathematial model of a single perspetive amera. 3. Epipolar onstraint. 4. Correspondene problem. 5. Results: state-of-the-art stereo, unalibrated 3D reonstrution, VR model.

2 CENTER FOR MACHINE PERCEPTION Researh group, head Prof. Válav Hlaváč, established 1986 as omputer vision lab, under the name CMP sine staff (11 2 Prof., 1 Asso. Prof., 3 PhD, 7 MS); out of it 2 mathematiians, 2 physiists, 8 engineers) + 8 full time PhD students. Interests: omputer vision, pattern reognition, mathematial models for treating unertainty. Links to industry mainly via a spin-off ompany Neovision Prague (10 people). E.g. Samsung, Boeing, Texas Instruments, Robert Bosh, Kyoera, Hitahi. 2/29

3 MAIN RUNNING PROJECTS AtIPret (R&D, , IST ) Interpreting and Understanding Ativities of Expert Operators for Teahing and Eduation (V. Hlaváč, J. Matas). ISAAC (Trial, 2002, IST ) Inspeting Sewerage Systems And Image Analysis by Computer (V. Hlaváč). Reonstrution of 3D sene from multiple unalibrated views (V. Hlaváč). Computational stereo (R. Šára). Omni-diretional vision. (T. Pajdla). Authentiation based on fae reognition (J. Matas). Pattern reognition theory (V. Hlaváč). 3/29

4 V. Hlaváč, books 4/29 Šonka M., Hlaváč V., Boyle R.B.: Image Analysis, Proessing and Mahine Vision, 2nd edition, PWS Boston, USA, 1999 (China edition 2002), 800 p, USD 105. Shlesinger M.I., Hlaváč V.: Ten Letures on Statistial and Strutural Pattern Reognition Kluwer, Dordreht, May 2002, EUR 165.

5 BASICS OF PROJECTIVE GEOMETRY Pinhole model - the simplest geometrial model of human eye, photographi and TV amera. 5/29 Perspetive projetion, also entral projetion. Parallel lines in the world do not remain parallel in the image (e.g., view along the straight setion of a railroad). Foal point Image plane Horizon Vanishing point Optial axis Base plane

6 PROJECTIVE SPACE 6/29 Consider (n + 1) dimensional vetor spae without its origin, R n+1 {(0,..., 0)}. Define an equivalene relation [x 1,..., x n+1 ] T [x 1,..., x n+1] T iff α 0 : [x 1,..., x n+1 ] T = α [x 1,..., x n+1] T Projetive spae P n is the quotient spae of this equivalene relation. Points in the projetive spae are expressed in homogeneous o-ordinates (alled also projetive oordinates) x = [x 1,..., x n, 1] T.

7 RELATION BETWEEN EUCLIDEAN AND PROJECTIVE SPACES 7/29 Consider Eulidean spae R n. The one-to-one mapping from the R n into P n [x 1,..., x n ] T [x 1,..., x n, 1] T Projetive points [x 1,..., x n, 0] T do not have an Eulidean ounterpart and represent points at infinity in a partiular diretion. Consider [x 1,..., x n, 0] T as a limiting ase of [x 1,..., x n, α] T that is projetively equivalent to [x 1 /α,..., x n /α, 1] T, and assume that α 0. This orresponds to a point in R n going to infinity in the diretion of the radius vetor [x 1 /α,..., x n /α] R n.

8 PROJECTIVE TRANSFORMATION (also CO-LINEATION) 8/29 Co-lineation is any mapping P n P n. Defined by a regular (n + 1) (n + 1) matrix A, ỹ = A x. Matrix A is defined up to a sale fator. Co-lineations map hyperplanes to hyperplanes. A speial ase is the mapping of lines to lines that is often used in omputer vision.

9 SINGLE PERSPECTIVE CAMERA, pinhole model Optial axis Z w O w Y w 9/29 X w Sene point X X w World Eulidean oordinate system t X Foal point C Z O Camera Eulidean oordinate system Y R Image affine oordinate system Z w i X f Optial ray X Image plane i π O i u v Y i U, u ~ Prinipal point = [0, 0, - f ] U 0 U 0a = [u, v, 0] 0 0 T T

10 CAMERA: P 3 P 2 10/29 A sene point X w in the world Eulidean o-ordinate system is a 3 1 vetor. The same point X in the amera Eulidean o-ordinate system is transformed by translation t (vetor) and rotation R (orthogonal matrix). X = x y z = R (X w t)

11 CAMERA: P 3 P 2 (2) 11/29 The point X is projeted to the image plane π as point U. Z x z X f - f x z U = [ fx z, fy z, f ] T, U0a = [u 0, v 0, 0] T.

12 CAMERA: P 3 P 2 (3) 12/29 Projeted point in the 2D image plane π in homogeneous o-ordinates ũ = U V W = = a b u 0 0 v fa fb u 0 0 f v fx z fy z 1 x z y z 1 2D Eulidean ounterpart is u = [u, v] T = [ U W, V W ]T.

13 CALIBRATION MATRIX K 13/29 z ũ = z fa fb u 0 0 f v x z y z 1 = fa fb u 0 0 f v x y z = fa fb u 0 0 f v R (X w t) = KR (X w t) Calibration parameters: intrinsi (matrix K) vs. extrinsi (vetor t, matrix R).

14 PROJECTION MATRIX M 14/29 ũ = U V W = 1 z KR (X w t) = [KR K R t] = M [ Xw 1 ] [ Xw 1 ] = M X w

15 SINGLE CAMERA CALIBRATION, overview 15/29 Intrinsi parameters only - seeking matrix K. Intrinsi + extrinsi parameters - seeking matrix M. 1. Known sene: A set of n non-degenerate (not o-planar) points in the 3D world (e.g., a alibration objet), and the orresponding 2D image points are known. Eah orrespondene between a 3D sene and 2D image point provides one equation [ ] Xj α j ũ j = M Unknown sene: More views are needed to alibrate the amera. The intrinsi amera parameters will not hange for different views, and the orrespondene between image points in different views must be established.

16 CALIBRATION FROM UNKNOWN SCENE (ont.) X 16/29 K R, t K Known amera motion: Three ases aording to the known motion onstraint: (a) Both rotation and translation, general ase. (b) Pure rotation () Pure translation, a linear solution proposed by [Pajdla, Hlaváč 1995]. 2. Unknown amera motion: The most general ase, sometimes alled amera self-alibration. At least three views are needed and the solution is nonlinear. Numerially hard.

17 CAMERA CALIBRATION FROM A KNOWN SCENE (1) 17/29 Typially a two stage proess. 1. Estimate the projetion matrix M is estimated from the o-ordinates of points with known sene positions. 2. The extrinsi and intrinsi parameters are estimated from M. Note: The seond step is not always needed the ase of stereo vision is an example.

18 CAMERA CALIBRATION FROM A KNOWN SCENE (2) Eah orrespondene between sene point X = [x, y, z] T and 2D image point [u, v] T gives one equation αu αv α αu αv α = = m 11 m 12 m 13 m 14 m 21 m 22 m 23 m 24 m 31 m 32 m 33 m 34 x y z 1 m 11 x + m 12 y + m 13 z + m 14 m 21 x + m 22 y + m 23 z + m 24 m 31 x + m 32 y + m 33 z + m 34 18/29

19 CAMERA CALIBRATION FROM A KNOWN SCENE (3) 19/29 u(m 31 x + m 32 y + m 33 z + m 34 ) = m 11 x + m 12 y + m 13 z + m 14 v(m 31 x + m 32 y + m 33 z + m 34 ) = m 21 x + m 22 y + m 23 z + m 24 Two linear equations, eah in 12 unknowns m 11,..., m 34, for eah known orresponding sene and image point (atually only 11 unknowns due to unknown saling). 6 orresponding points needed, at least. If n suh points are available, we an write it as a 2n 12 matrix. x y z ux uy uz u x y z. 1 vx vy vz v m 11 m 12. m 34 = 0 Overonstraint linear system. Robust least squares. Result = M.

20 SVD Singular Value Deomposition SVD is a linear algebra tehnique for solving linear equations in the least square sense. SVD works for singular matries or matries numerially lose to singular. Contained, e.g., in MATLAB. Any m n matrix A, m n an be fatorized as A = UDV T. U has orthonormal olumns, D is non-negative diagonal, and V T has orthonormal rows. SVD loates the losest possible solution in a least square sense. Sometimes need for the losest singular matrix to the original matrix A this dereases the rank from n to n 1. Replae the smallest diagonal element of D by zero. This new matrix is the losest to the original one with respet to the Frobenius norm (whih is alulated as a sum of the squared values of all matrix elements). 20/29

21 SEPARATION OF EXTRINSIC PARAMETERS FROM M Given: projetion matrix M 21/29 Output: rotation matrix R and translation vetor t). M = [KR KR t] = [A b] The 3 3 submatrix is denoted as A, and the rightmost olumn as b. Translation vetor t is easy; A = KR, t = A 1 b. Rotation matrix R. Reall that the alibration matrix K is upper triangular and the rotation matrix is orthogonal. The QR fatorization method or SVD will deompose A into a produt and hene reover K and R.

22 RADIAL DISTORTION AND DE-CENTERING 22/29 PINCUSHION BARREL Often modelled as rotationally symmetri by polynomials. u, v - orret image o-ordinates ũ, ṽ - measured unorreted image o-ordinates û 0, ˆv 0 - estimate of the position of the prinipal point ũ = x û 0, ṽ = y ˆv 0

23 RADIAL DISTORTION (2) 23/29 u = ũ + δu, v = ṽ + δv δu = (ũ u p )(κ 1 r 2 + κ 2 r 4 + κ 3 r 6 ) δv = (ṽ v p )(κ 1 r 2 + κ 2 r 4 + κ 3 r 6 ) r 2 is the square of the radial distane from the enter of the image. r 2 = (ũ u p ) 2 + (ũ u p ) 2 u p, v p are orretions to û 0, ˆv 0 u 0 = û 0 + u p v 0 = ˆv 0 + v p

24 GEOMETRY OF 2 CAMERAS 24/29 Epipoles e, e, epipolar lines l, l. e, e, l, l, C, C, X lie in a single plane. Epipolar geometry. Seeking orrespondenes between two 1D signals. Bilinear relation between u, u.

25 FUNDAMENTAL MATRIX (1) 25/29 Left projetion u and right projetion u of the sene point X. u [K 0] [ X 1 ] u [K R K R t] = K X, [ X 1 = K (R X R t) = K X ] Coplanarity of X, X and t. Distinguish o-ordinates of the left and right ameras by the subsript L, R. Vetor produt.

26 FUNDAMENTAL MATRIX (2) 26/29 Coordinates rotation X R = R X L, and hene X L = R 1 X R. Coplanarity onstraint X T L (t X L) = 0. Preparing for substitution X L = K 1 u, X R = (K ) 1 u, and X L = R 1 (K ) 1 u. Epipolar onstraint in vetor form (K 1 u) T (t R 1 (K ) 1 u ) = 0. Equation is homogeneous with respet to t, so the sale is not determined. Absolute sale annot be reovered without yardstik.

27 FUNDAMENTAL MATRIX (3) 27/29 Replaement of a vetor produt by a matrix multipliation. The translation vetor is t = [t x, t y, t z ] T, and a skew symmetri matrix S(t) (i.e., S T = S) an be reated from it if t 0. S(t) = 0 t z t y t z 0 t x t y t x 0 Note that rank(s) = 2 if and only if t 0.

28 FUNDAMENTAL MATRIX (4) 28/29 The vetor produt an be replaed by the multipliation of two matries. For any regular matrix A, we have t A = S(t) A. Thus we an rewrite the epipolar onstraint in a vetor form (K 1 u) T (S(t) R 1 (K ) 1 u ) = 0, u T (K 1 ) T S(t)R 1 (K ) 1 u = 0.

29 FUNDAMENTAL MATRIX (5) 29/29 The middle part an be onentrated into a single matrix F alled the fundamental matrix of two views, F = (K 1 ) T S(t)R 1 (K ) 1. With the substitution for F we finally get the bilinear relation (sometimes named after Longuet-Higgins) between any two views u T F u = 0. It an be seen that the fundamental matrix F aptures all information that an be reovered from a pair of images if the orrespondene problem is solved.

30

31

32 Foal point Image plane Horizon Vanishing point Optial axis Base plane

33 Optial axis Z w O w Y w Sene point X w X X w World Eulidean oordinate system t X Foal point C Z O Camera Eulidean oordinate system Y R Image affine oordinate system Z w i X f Optial ray X Image plane i π O i u v Y i U, u ~ Prinipal point = [0, 0, - f ] U 0 U 0a = [u, v, 0] 0 0 T T

34 Z x z X f - f x z

35 X K R, t K 1 2

36

37 PINCUSHION BARREL

38

v = fy c u = fx c z c The Pinhole Camera Model Camera Projection Models

v = fy c u = fx c z c The Pinhole Camera Model Camera Projection Models The Pinhole Camera Model Camera Projetion Models We will introdue dierent amera projetion models that relate the loation o an image point to the oordinates o the orresponding 3D points. The projetion models

More information

University of Cambridge Engineering Part IIB Module 4F12: Computer Vision Handout 3: Projection

University of Cambridge Engineering Part IIB Module 4F12: Computer Vision Handout 3: Projection University of Cambridge Engineering Part IIB Module 4F2: Computer Vision Handout 3: Projetion Roberto Cipolla Otober 2009 Projetion Orthographi projetion Reall that omputer vision is about disovering from

More information

Lecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont.

Lecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont. Stat60/CS94: Randomized Algorithms for Matries and Data Leture 7-09/5/013 Leture 7: Sampling/Projetions for Least-squares Approximation, Cont. Leturer: Mihael Mahoney Sribe: Mihael Mahoney Warning: these

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

TENSOR FORM OF SPECIAL RELATIVITY

TENSOR FORM OF SPECIAL RELATIVITY TENSOR FORM OF SPECIAL RELATIVITY We begin by realling that the fundamental priniple of Speial Relativity is that all physial laws must look the same to all inertial observers. This is easiest done by

More information

Ayan Kumar Bandyopadhyay

Ayan Kumar Bandyopadhyay Charaterization of radiating apertures using Multiple Multipole Method And Modeling and Optimization of a Spiral Antenna for Ground Penetrating Radar Appliations Ayan Kumar Bandyopadhyay FET-IESK, Otto-von-Guerike-University,

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

Study of EM waves in Periodic Structures (mathematical details)

Study of EM waves in Periodic Structures (mathematical details) Study of EM waves in Periodi Strutures (mathematial details) Massahusetts Institute of Tehnology 6.635 partial leture notes 1 Introdution: periodi media nomenlature 1. The spae domain is defined by a basis,(a

More information

LECTURE NOTES FOR , FALL 2004

LECTURE NOTES FOR , FALL 2004 LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as

More information

Sensitivity analysis for linear optimization problem with fuzzy data in the objective function

Sensitivity analysis for linear optimization problem with fuzzy data in the objective function Sensitivity analysis for linear optimization problem with fuzzy data in the objetive funtion Stephan Dempe, Tatiana Starostina May 5, 2004 Abstrat Linear programming problems with fuzzy oeffiients in the

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

F = F x x + F y. y + F z

F = F x x + F y. y + F z ECTION 6: etor Calulus MATH20411 You met vetors in the first year. etor alulus is essentially alulus on vetors. We will need to differentiate vetors and perform integrals involving vetors. In partiular,

More information

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined How should a snake turn on ie: A ase study of the asymptoti isoholonomi problem Jianghai Hu, Slobodan N. Simić, and Shankar Sastry Department of Eletrial Engineering and Computer Sienes University of California

More information

Takeshi Kurata Jun Fujiki Katsuhiko Sakaue. 1{1{4 Umezono, Tsukuba-shi, Ibaraki , JAPAN. fkurata, fujiki,

Takeshi Kurata Jun Fujiki Katsuhiko Sakaue. 1{1{4 Umezono, Tsukuba-shi, Ibaraki , JAPAN. fkurata, fujiki, Ane Eiolar Geometry via Fatorization Method akeshi Kurata Jun Fujiki Katsuhiko Sakaue Eletrotehnial Laboratory {{4 Umezono, sukuba-shi, Ibaraki 305-8568, JAPAN fkurata, fujiki, sakaueg@etl.go.j Abstrat

More information

CSE 252B: Computer Vision II

CSE 252B: Computer Vision II CSE 252B: Computer Vision II Lecturer: Serge Belongie Scribe: Tasha Vanesian LECTURE 3 Calibrated 3D Reconstruction 3.1. Geometric View of Epipolar Constraint We are trying to solve the following problem:

More information

Lecture 5. Epipolar Geometry. Professor Silvio Savarese Computational Vision and Geometry Lab. 21-Jan-15. Lecture 5 - Silvio Savarese

Lecture 5. Epipolar Geometry. Professor Silvio Savarese Computational Vision and Geometry Lab. 21-Jan-15. Lecture 5 - Silvio Savarese Lecture 5 Epipolar Geometry Professor Silvio Savarese Computational Vision and Geometry Lab Silvio Savarese Lecture 5-21-Jan-15 Lecture 5 Epipolar Geometry Why is stereo useful? Epipolar constraints Essential

More information

Math 220A - Fall 2002 Homework 8 Solutions

Math 220A - Fall 2002 Homework 8 Solutions Math A - Fall Homework 8 Solutions 1. Consider u tt u = x R 3, t > u(x, ) = φ(x) u t (x, ) = ψ(x). Suppose φ, ψ are supported in the annular region a < x < b. (a) Find the time T 1 > suh that u(x, t) is

More information

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach Measuring & Induing Neural Ativity Using Extraellular Fields I: Inverse systems approah Keith Dillon Department of Eletrial and Computer Engineering University of California San Diego 9500 Gilman Dr. La

More information

The gravitational phenomena without the curved spacetime

The gravitational phenomena without the curved spacetime The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,

More information

Singular Event Detection

Singular Event Detection Singular Event Detetion Rafael S. Garía Eletrial Engineering University of Puerto Rio at Mayagüez Rafael.Garia@ee.uprm.edu Faulty Mentor: S. Shankar Sastry Researh Supervisor: Jonathan Sprinkle Graduate

More information

After the completion of this section the student should recall

After the completion of this section the student should recall Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition

More information

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances An aptive Optimization Approah to Ative Canellation of Repeated Transient Vibration Disturbanes David L. Bowen RH Lyon Corp / Aenteh, 33 Moulton St., Cambridge, MA 138, U.S.A., owen@lyonorp.om J. Gregory

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

Modeling superlattice patterns using the interference of sharp focused spherical waves

Modeling superlattice patterns using the interference of sharp focused spherical waves Modeling superlattie patterns using the interferene of sharp foused spherial waves Fidirko N.S. Samara State Aerospae University Abstrat. In this paper, modelling of pseudonondiffrational beams forming

More information

HOW TO FACTOR. Next you reason that if it factors, then the factorization will look something like,

HOW TO FACTOR. Next you reason that if it factors, then the factorization will look something like, HOW TO FACTOR ax bx I now want to talk a bit about how to fator ax bx where all the oeffiients a, b, and are integers. The method that most people are taught these days in high shool (assuming you go to

More information

Discrete Bessel functions and partial difference equations

Discrete Bessel functions and partial difference equations Disrete Bessel funtions and partial differene equations Antonín Slavík Charles University, Faulty of Mathematis and Physis, Sokolovská 83, 186 75 Praha 8, Czeh Republi E-mail: slavik@karlin.mff.uni.z Abstrat

More information

V. Interacting Particles

V. Interacting Particles V. Interating Partiles V.A The Cumulant Expansion The examples studied in the previous setion involve non-interating partiles. It is preisely the lak of interations that renders these problems exatly solvable.

More information

Solutions for Math 225 Assignment #2 1

Solutions for Math 225 Assignment #2 1 Solutions for Math 225 Assignment #2 () Determine whether W is a subspae of V and justify your answer: (a) V = R 3, W = {(a,, a) : a R} Proof Yes For a =, (a,, a) = (,, ) W For all (a,, a ), (a 2,, a 2

More information

Name Solutions to Test 1 September 23, 2016

Name Solutions to Test 1 September 23, 2016 Name Solutions to Test 1 September 3, 016 This test onsists of three parts. Please note that in parts II and III, you an skip one question of those offered. Possibly useful formulas: F qequb x xvt E Evpx

More information

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION 4 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION Jiri Nozika*, Josef Adame*, Daniel Hanus** *Department of Fluid Dynamis and

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

A Characterization of Wavelet Convergence in Sobolev Spaces A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat

More information

Moments and Wavelets in Signal Estimation

Moments and Wavelets in Signal Estimation Moments and Wavelets in Signal Estimation Edward J. Wegman 1 Center for Computational Statistis George Mason University Hung T. Le 2 International usiness Mahines Abstrat: The problem of generalized nonparametri

More information

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip

Q2. [40 points] Bishop-Hill Model: Calculation of Taylor Factors for Multiple Slip 27-750, A.D. Rollett Due: 20 th Ot., 2011. Homework 5, Volume Frations, Single and Multiple Slip Crystal Plastiity Note the 2 extra redit questions (at the end). Q1. [40 points] Single Slip: Calulating

More information

3D from Photographs: Camera Calibration. Dr Francesco Banterle

3D from Photographs: Camera Calibration. Dr Francesco Banterle 3D from Photographs: Camera Calibration Dr Francesco Banterle francesco.banterle@isti.cnr.it 3D from Photographs Automatic Matching of Images Camera Calibration Photographs Surface Reconstruction Dense

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

COMPLEX INDUCTANCE AND ITS COMPUTER MODELLING

COMPLEX INDUCTANCE AND ITS COMPUTER MODELLING Journal of ELECTRICAL ENGINEERING, VOL. 53, NO. 1-2, 22, 24 29 COMPLEX INDUCTANCE AND ITS COMPUTER MODELLING Daniel Mayer Bohuš Ulryh The paper introdues the onept of the omplex indutane as a parameter

More information

MOLECULAR ORBITAL THEORY- PART I

MOLECULAR ORBITAL THEORY- PART I 5.6 Physial Chemistry Leture #24-25 MOLECULAR ORBITAL THEORY- PART I At this point, we have nearly ompleted our rash-ourse introdution to quantum mehanis and we re finally ready to deal with moleules.

More information

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices AAS 03-190 Conformal Mapping among Orthogonal, Symmetri, and Skew-Symmetri Matries Daniele Mortari Department of Aerospae Engineering, Texas A&M University, College Station, TX 77843-3141 Abstrat This

More information

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

A Practical Method for Decomposition of the Essential Matrix

A Practical Method for Decomposition of the Essential Matrix Applied Mathematical Sciences, Vol. 8, 2014, no. 176, 8755-8770 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2014.410877 A Practical Method for Decomposition of the Essential Matrix Georgi

More information

Relativistic Dynamics

Relativistic Dynamics Chapter 7 Relativisti Dynamis 7.1 General Priniples of Dynamis 7.2 Relativisti Ation As stated in Setion A.2, all of dynamis is derived from the priniple of least ation. Thus it is our hore to find a suitable

More information

Multiple View Geometry in Computer Vision

Multiple View Geometry in Computer Vision Multiple View Geometry in Computer Vision Prasanna Sahoo Department of Mathematics University of Louisville 1 Scene Planes & Homographies Lecture 19 March 24, 2005 2 In our last lecture, we examined various

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

SYNTHETIC APERTURE IMAGING OF DIRECTION AND FREQUENCY DEPENDENT REFLECTIVITIES

SYNTHETIC APERTURE IMAGING OF DIRECTION AND FREQUENCY DEPENDENT REFLECTIVITIES SYNTHETIC APERTURE IMAGING OF DIRECTION AND FREQUENCY DEPENDENT REFLECTIVITIES LILIANA BORCEA, MIGUEL MOSCOSO, GEORGE PAPANICOLAOU, AND CHRYSOULA TSOGKA Abstrat. We introdue a syntheti aperture imaging

More information

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach Amerian Journal of heoretial and Applied tatistis 6; 5(-): -8 Published online January 7, 6 (http://www.sienepublishinggroup.om/j/ajtas) doi:.648/j.ajtas.s.65.4 IN: 36-8999 (Print); IN: 36-96 (Online)

More information

Chapter 2. Conditional Probability

Chapter 2. Conditional Probability Chapter. Conditional Probability The probabilities assigned to various events depend on what is known about the experimental situation when the assignment is made. For a partiular event A, we have used

More information

Chapter 26 Lecture Notes

Chapter 26 Lecture Notes Chapter 26 Leture Notes Physis 2424 - Strauss Formulas: t = t0 1 v L = L0 1 v m = m0 1 v E = m 0 2 + KE = m 2 KE = m 2 -m 0 2 mv 0 p= mv = 1 v E 2 = p 2 2 + m 2 0 4 v + u u = 2 1 + vu There were two revolutions

More information

4.4 Solving Systems of Equations by Matrices

4.4 Solving Systems of Equations by Matrices Setion 4.4 Solving Systems of Equations by Matries 1. A first number is 8 less than a seond number. Twie the first number is 11 more than the seond number. Find the numbers.. The sum of the measures of

More information

Normative and descriptive approaches to multiattribute decision making

Normative and descriptive approaches to multiattribute decision making De. 009, Volume 8, No. (Serial No.78) China-USA Business Review, ISSN 57-54, USA Normative and desriptive approahes to multiattribute deision making Milan Terek (Department of Statistis, University of

More information

Answers to Coursebook questions Chapter J2

Answers to Coursebook questions Chapter J2 Answers to Courseook questions Chapter J 1 a Partiles are produed in ollisions one example out of many is: a ollision of an eletron with a positron in a synhrotron. If we produe a pair of a partile and

More information

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data Comparison of Alternative Equivalent Ciruits of Indution Motor with Real Mahine Data J. radna, J. auer, S. Fligl and V. Hlinovsky Abstrat The algorithms based on separated ontrol of the motor flux and

More information

Remarks Around Lorentz Transformation

Remarks Around Lorentz Transformation Remarks Around Lorentz Transformation Arm Boris Nima arm.boris@gmail.om Abstrat After diagonalizing the Lorentz Matrix, we find the frame where the Dira equation is one derivation and we alulate the speed

More information

Parameterized Special Theory of Relativity (PSTR)

Parameterized Special Theory of Relativity (PSTR) Apeiron, Vol. 19, No., April 01 115 Parameterized Speial Theory of Relativity (PSTR) Florentin Smarandahe University of New Mexio Gallup, NM 87301, USA smarand@unm.edu We have parameterized Einstein s

More information

Lecture 3 - Lorentz Transformations

Lecture 3 - Lorentz Transformations Leture - Lorentz Transformations A Puzzle... Example A ruler is positioned perpendiular to a wall. A stik of length L flies by at speed v. It travels in front of the ruler, so that it obsures part of the

More information

Estimating the probability law of the codelength as a function of the approximation error in image compression

Estimating the probability law of the codelength as a function of the approximation error in image compression Estimating the probability law of the odelength as a funtion of the approximation error in image ompression François Malgouyres Marh 7, 2007 Abstrat After some reolletions on ompression of images using

More information

Math 151 Introduction to Eigenvectors

Math 151 Introduction to Eigenvectors Math 151 Introdution to Eigenvetors The motivating example we used to desrie matrixes was landsape hange and vegetation suession. We hose the simple example of Bare Soil (B), eing replaed y Grasses (G)

More information

Wave Propagation through Random Media

Wave Propagation through Random Media Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene

More information

Searching All Approximate Covers and Their Distance using Finite Automata

Searching All Approximate Covers and Their Distance using Finite Automata Searhing All Approximate Covers and Their Distane using Finite Automata Ondřej Guth, Bořivoj Melihar, and Miroslav Balík České vysoké učení tehniké v Praze, Praha, CZ, {gutho1,melihar,alikm}@fel.vut.z

More information

Camera Projection Model

Camera Projection Model amera Projection Model 3D Point Projection (Pixel Space) O ( u, v ) ccd ccd f Projection plane (, Y, Z ) ( u, v ) img Z img (0,0) w img ( u, v ) img img uimg f Z p Y v img f Z p x y Zu f p Z img img x

More information

Final Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light

Final Review. A Puzzle... Special Relativity. Direction of the Force. Moving at the Speed of Light Final Review A Puzzle... Diretion of the Fore A point harge q is loated a fixed height h above an infinite horizontal onduting plane. Another point harge q is loated a height z (with z > h) above the plane.

More information

Array Design for Superresolution Direction-Finding Algorithms

Array Design for Superresolution Direction-Finding Algorithms Array Design for Superresolution Diretion-Finding Algorithms Naushad Hussein Dowlut BEng, ACGI, AMIEE Athanassios Manikas PhD, DIC, AMIEE, MIEEE Department of Eletrial Eletroni Engineering Imperial College

More information

Perturbation Analyses for the Cholesky Factorization with Backward Rounding Errors

Perturbation Analyses for the Cholesky Factorization with Backward Rounding Errors Perturbation Analyses for the holesky Fatorization with Bakward Rounding Errors Xiao-Wen hang Shool of omputer Siene, MGill University, Montreal, Quebe, anada, H3A A7 Abstrat. This paper gives perturbation

More information

arxiv:physics/ v1 [physics.class-ph] 8 Aug 2003

arxiv:physics/ v1 [physics.class-ph] 8 Aug 2003 arxiv:physis/0308036v1 [physis.lass-ph] 8 Aug 003 On the meaning of Lorentz ovariane Lszl E. Szab Theoretial Physis Researh Group of the Hungarian Aademy of Sienes Department of History and Philosophy

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

SURFACE WAVES OF NON-RAYLEIGH TYPE SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh

More information

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics International Journal of Statistis and Systems ISSN 0973-2675 Volume 12, Number 4 (2017), pp. 763-772 Researh India Publiations http://www.ripubliation.om Design and Development of Three Stages Mixed Sampling

More information

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction Version of 5/2/2003 To appear in Advanes in Applied Mathematis REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS MATTHIAS BECK AND SHELEMYAHU ZACKS Abstrat We study the Frobenius problem:

More information

Solving Constrained Lasso and Elastic Net Using

Solving Constrained Lasso and Elastic Net Using Solving Constrained Lasso and Elasti Net Using ν s Carlos M. Alaı z, Alberto Torres and Jose R. Dorronsoro Universidad Auto noma de Madrid - Departamento de Ingenierı a Informa tia Toma s y Valiente 11,

More information

Camera Calibration The purpose of camera calibration is to determine the intrinsic camera parameters (c 0,r 0 ), f, s x, s y, skew parameter (s =

Camera Calibration The purpose of camera calibration is to determine the intrinsic camera parameters (c 0,r 0 ), f, s x, s y, skew parameter (s = Camera Calibration The purpose of camera calibration is to determine the intrinsic camera parameters (c 0,r 0 ), f, s x, s y, skew parameter (s = cotα), and the lens distortion (radial distortion coefficient

More information

MUSIC GENRE CLASSIFICATION USING LOCALITY PRESERVING NON-NEGATIVE TENSOR FACTORIZATION AND SPARSE REPRESENTATIONS

MUSIC GENRE CLASSIFICATION USING LOCALITY PRESERVING NON-NEGATIVE TENSOR FACTORIZATION AND SPARSE REPRESENTATIONS 10th International Soiety for Musi Information Retrieval Conferene (ISMIR 2009) MUSIC GENRE CLASSIFICATION USING LOCALITY PRESERVING NON-NEGATIVE TENSOR FACTORIZATION AND SPARSE REPRESENTATIONS Yannis

More information

UNCERTAINTY RELATIONS AS A CONSEQUENCE OF THE LORENTZ TRANSFORMATIONS. V. N. Matveev and O. V. Matvejev

UNCERTAINTY RELATIONS AS A CONSEQUENCE OF THE LORENTZ TRANSFORMATIONS. V. N. Matveev and O. V. Matvejev UNCERTAINTY RELATIONS AS A CONSEQUENCE OF THE LORENTZ TRANSFORMATIONS V. N. Matveev and O. V. Matvejev Joint-Stok Company Sinerta Savanoriu pr., 159, Vilnius, LT-315, Lithuania E-mail: matwad@mail.ru Abstrat

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used

More information

A 4 4 diagonal matrix Schrödinger equation from relativistic total energy with a 2 2 Lorentz invariant solution.

A 4 4 diagonal matrix Schrödinger equation from relativistic total energy with a 2 2 Lorentz invariant solution. A 4 4 diagonal matrix Shrödinger equation from relativisti total energy with a 2 2 Lorentz invariant solution. Han Geurdes 1 and Koji Nagata 2 1 Geurdes datasiene, 2593 NN, 164, Den Haag, Netherlands E-mail:

More information

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1 Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random

More information

FINITE WORD LENGTH EFFECTS IN DSP

FINITE WORD LENGTH EFFECTS IN DSP FINITE WORD LENGTH EFFECTS IN DSP PREPARED BY GUIDED BY Snehal Gor Dr. Srianth T. ABSTRACT We now that omputers store numbers not with infinite preision but rather in some approximation that an be paed

More information

General Equilibrium. What happens to cause a reaction to come to equilibrium?

General Equilibrium. What happens to cause a reaction to come to equilibrium? General Equilibrium Chemial Equilibrium Most hemial reations that are enountered are reversible. In other words, they go fairly easily in either the forward or reverse diretions. The thing to remember

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Electromagnetic radiation of the travelling spin wave propagating in an antiferromagnetic plate. Exact solution.

Electromagnetic radiation of the travelling spin wave propagating in an antiferromagnetic plate. Exact solution. arxiv:physis/99536v1 [physis.lass-ph] 15 May 1999 Eletromagneti radiation of the travelling spin wave propagating in an antiferromagneti plate. Exat solution. A.A.Zhmudsky November 19, 16 Abstrat The exat

More information

ALGORITHMS FOR SAFE SPACECRAFT PROXIMITY OPERATIONS

ALGORITHMS FOR SAFE SPACECRAFT PROXIMITY OPERATIONS AAS-2007-107 ALGORITHMS FOR SAFE SPACECRAFT PROXIMITY OPERATIONS INTRODUCTION David E. Gaylor *, Brent William Barbee Emergent Spae Tehnologies, In., Greenbelt, MD, 20770 Future missions involving in-spae

More information

arxiv:gr-qc/ v2 6 Feb 2004

arxiv:gr-qc/ v2 6 Feb 2004 Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this

More information

A General and Simple Method for Camera Pose and Focal Length Determination

A General and Simple Method for Camera Pose and Focal Length Determination A General and Simple Method for Camera Pose and Foal Length Determination Yinqiang Zheng Shigeki Sugimoto Imari Sato, Masatoshi Okutomi National Institute of Informatis, JAPAN yqzheng@nii.a.jp imarik@nii.a.jp

More information

A Study of Kruppa s Equation for Camera Self-calibration

A Study of Kruppa s Equation for Camera Self-calibration Proceedings of the International Conference of Machine Vision and Machine Learning Prague, Czech Republic, August 14-15, 2014 Paper No. 57 A Study of Kruppa s Equation for Camera Self-calibration Luh Prapitasari,

More information

Lecture 15 (Nov. 1, 2017)

Lecture 15 (Nov. 1, 2017) Leture 5 8.3 Quantum Theor I, Fall 07 74 Leture 5 (Nov., 07 5. Charged Partile in a Uniform Magneti Field Last time, we disussed the quantum mehanis of a harged partile moving in a uniform magneti field

More information

Packing Plane Spanning Trees into a Point Set

Packing Plane Spanning Trees into a Point Set Paking Plane Spanning Trees into a Point Set Ahmad Biniaz Alfredo Garía Abstrat Let P be a set of n points in the plane in general position. We show that at least n/3 plane spanning trees an be paked into

More information

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013 Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it

More information

Application of the finite-element method within a two-parameter regularised inversion algorithm for electrical capacitance tomography

Application of the finite-element method within a two-parameter regularised inversion algorithm for electrical capacitance tomography Appliation of the finite-element method within a two-parameter regularised inversion algorithm for eletrial apaitane tomograph D Hinestroza, J C Gamio, M Ono Departamento de Matemátias, Universidad del

More information

Generation of EM waves

Generation of EM waves Generation of EM waves Susan Lea Spring 015 1 The Green s funtion In Lorentz gauge, we obtained the wave equation: A 4π J 1 The orresponding Green s funtion for the problem satisfies the simpler differential

More information

10.5 Unsupervised Bayesian Learning

10.5 Unsupervised Bayesian Learning The Bayes Classifier Maximum-likelihood methods: Li Yu Hongda Mao Joan Wang parameter vetor is a fixed but unknown value Bayes methods: parameter vetor is a random variable with known prior distribution

More information

LECTURE 2 Geometrical Properties of Rod Cross Sections (Part 2) 1 Moments of Inertia Transformation with Parallel Transfer of Axes.

LECTURE 2 Geometrical Properties of Rod Cross Sections (Part 2) 1 Moments of Inertia Transformation with Parallel Transfer of Axes. V. DEMENKO MECHNCS OF MTERLS 05 LECTURE Geometrial Properties of Rod Cross Setions (Part ) Moments of nertia Transformation with Parallel Transfer of xes. Parallel-xes Theorems S Given: a b = S = 0. z

More information

Review of Force, Stress, and Strain Tensors

Review of Force, Stress, and Strain Tensors Review of Fore, Stress, and Strain Tensors.1 The Fore Vetor Fores an be grouped into two broad ategories: surfae fores and body fores. Surfae fores are those that at over a surfae (as the name implies),

More information

Aharonov-Bohm effect. Dan Solomon.

Aharonov-Bohm effect. Dan Solomon. Aharonov-Bohm effet. Dan Solomon. In the figure the magneti field is onfined to a solenoid of radius r 0 and is direted in the z- diretion, out of the paper. The solenoid is surrounded by a barrier that

More information

Robust Recovery of Signals From a Structured Union of Subspaces

Robust Recovery of Signals From a Structured Union of Subspaces Robust Reovery of Signals From a Strutured Union of Subspaes 1 Yonina C. Eldar, Senior Member, IEEE and Moshe Mishali, Student Member, IEEE arxiv:87.4581v2 [nlin.cg] 3 Mar 29 Abstrat Traditional sampling

More information

A Queueing Model for Call Blending in Call Centers

A Queueing Model for Call Blending in Call Centers A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl

More information

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install

More information

Wuming Li and Fan Yang

Wuming Li and Fan Yang NEW ZEALAND JOURNAL OF MATHEMATICS Volume 33 (004), 159 164 N DIMENSIONAL MINKOWSKI SPACE AND SPACE TIME ALGEBRA Wuming Li and Fan Yang (Reeived February 003) Abstrat. By using an n Dimensional Minkowski

More information

Model-based mixture discriminant analysis an experimental study

Model-based mixture discriminant analysis an experimental study Model-based mixture disriminant analysis an experimental study Zohar Halbe and Mayer Aladjem Department of Eletrial and Computer Engineering, Ben-Gurion University of the Negev P.O.Box 653, Beer-Sheva,

More information

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u

Strauss PDEs 2e: Section Exercise 3 Page 1 of 13. u tt c 2 u xx = cos x. ( 2 t c 2 2 x)u = cos x. v = ( t c x )u Strauss PDEs e: Setion 3.4 - Exerise 3 Page 1 of 13 Exerise 3 Solve u tt = u xx + os x, u(x, ) = sin x, u t (x, ) = 1 + x. Solution Solution by Operator Fatorization Bring u xx to the other side. Write

More information

The Lorenz Transform

The Lorenz Transform The Lorenz Transform Flameno Chuk Keyser Part I The Einstein/Bergmann deriation of the Lorentz Transform I follow the deriation of the Lorentz Transform, following Peter S Bergmann in Introdution to the

More information

div v(x) = 0, n terr = 0, v terr = v t,

div v(x) = 0, n terr = 0, v terr = v t, Proeedings of the Ceh Japanese Seminar in Applied Mathematis 6 Ceh Tehnial University in Prague, September 4-7, 6 pp. 4 8 FLOW AND POLLUTION TRANSPORT IN THE STREET CANYON PETR BAUER, AND ZBYŇEK JAŇOUR

More information