Lecture 04- Projective Geometry

Total Page:16

File Type:pdf, Size:1020Kb

Lecture 04- Projective Geometry Lecture 04- Projective Geometry EE382-Visual localization & Perception Danping Zou @Shanghai Jiao Tong University 1 Projective geometry • Key concept - Homogenous coordinates – Represent an -dimensional vector by a dimensional coordinate Homogenous coordinate Cartesian coordinate – Can represent infinite points or lines August Ferdinand Möbius Danping Zou @Shanghai Jiao Tong University 1790-1868 2 2D projective geometry • Point representation: – A point can be represented by a homogenous coordinate: Homogeneous coordinates: Inhomogeneous coordinates: Danping Zou @Shanghai Jiao Tong University 3 2D projective geometry • Line representation: – A line is represented by a line equation: Hence a line can be naturally represented by a homogeneous coordinate: It has the same scale equivalence relationship: Danping Zou @Shanghai Jiao Tong University 4 2D projective geometry • A point lie on a line is simply described as: where and . A point or a line has only two degree of freedom (DoF, 自由度). Danping Zou @Shanghai Jiao Tong University 5 2D projective geometry • Intersection of lines: – The intersection of two lines is computed by the cross production of the two homogenous coordinates of the two lines: Intersection of lines Here, ‘ ‘ represents cross production Danping Zou @Shanghai Jiao Tong University 6 2D projective geometry • Example of intersection of two lines: Let the two lines be • The intersection point is computed as : • The inhomogeneous coordinate is Danping Zou @Shanghai Jiao Tong University 7 2D projective geometry • Line across two points: • The line across the two points is obtained by the cross production of the two homogenous coordinates of the two points: Danping Zou @Shanghai Jiao Tong University 8 2D projective geometry • Idea point (point at infinity): – Intersection of parallel lines – Let two parallel lines be where . Their intersection is computed as Its inhomogeneous coordinates are meaningless: The point with the last coordinate x3 =0 is called idea points Danping Zou @Shanghai Jiao Tong University 9 2D projective geometry • Line at infinity : all idea points lies on • Points and lines in the 2D plane are represented by 3D rays and planes respectively. • The idea points lies in - plane and - plane represents A geometric interpolation Danping Zou @Shanghai Jiao Tong University 10 2D projective geometry • Projective transformation: – A projective transformation is an invertible mapping such that three points lie on the same line if and only if do. – A projective transformation is also called as • A collineation • A homography – A homography is a linear transformation on homogeneous 3-vectors represented by a non- singular 3 × 3 matrix: Danping Zou @Shanghai Jiao Tong University 11 2D projective geometry • Given a transformation of points , the transformation of lines is given by . Danping Zou @Shanghai Jiao Tong University 12 2D projective geometry • An example of projective transformation Danping Zou @Shanghai Jiao Tong University 13 2D projective geometry • A hierarchy of transformations Isometries Similarity transformation Affine transformation Projective transformation Danping Zou @Shanghai Jiao Tong University 14 2D projective geometry • Isometrics : Euclidean transformation [+ Reflection] Rotation Translation 3DoF Euclidean transformation Reflection + Euclidean transformation A isometric transformation has 3 degree of freedom, whose invariants include length, angle and area. Danping Zou @Shanghai Jiao Tong University 15 2D projective geometry • Similarity transformation A isometric transformation has 4 degree of freedom, with one more degree of freedom on the scaling. It preserves the ‘shape’, angle. Danping Zou @Shanghai Jiao Tong University 16 2D projective geometry • An Affine transformation is a non-singular linear transformation which has the following form: 6DoF Danping Zou @Shanghai Jiao Tong University 17 2D projective geometry • Projective transformation 8DoF • Can be decomposed into a chain of essential transformations: Scale Similarity Pure Affine Pure projective Danping Zou @Shanghai Jiao Tong University 18 Summary * Page 44 Multiple-view Geometry for Computer Vision Danping Zou @Shanghai Jiao Tong University 19 Summary • Homogenous/inhomogenous coordinates • 2D points vs.. 2D lines • Points / lines at infinity • Projective transformation, Homography • Hierarchy of transformations: – Isometrics (Euclidean) ->similarity->affine->projective Danping Zou @Shanghai Jiao Tong University 20 3D projective geometry • The homogeneous a 3D point is represented by • Its inhomogeneous coordinates is • The projective transformation in 3D space is a linear transformation on homogeneous 4-vectors, represented by a non-singular matrix: Danping Zou @Shanghai Jiao Tong University 21 3D projective geometry • A plane in 3D space is written as Plane normal • Let the point on the plane be , we have : Danping Zou @Shanghai Jiao Tong University 22 3D projective geometry • Transformation of planes : Danping Zou @Shanghai Jiao Tong University 23 3D projective geometry • Joint and incidence relations – A plane is defined uniquely by three distinct points – Three planes intersect in a unique point – Two distinct planes intersect in a unique line Danping Zou @Shanghai Jiao Tong University 24 3D projective geometry • Three points define a plane : • The rank of is 3, how to solve this equation? – Method #1. Compute the basis of the null space of – Method #2. Let , solve the following equation: Danping Zou @Shanghai Jiao Tong University 25 About the null space & SVD • Fundamentals – Range (column space) : range(A) is the space spanned by the columns of the matrix A. – Null space : null(A) is a space where all the vectors satisfy – Rank : The rank is the dimension of the column space Danping Zou @Shanghai Jiao Tong University 26 About the null space & SVD • Use SVD to compute the null space of a matrix. • The Singular Value Decomposition (SVD) is a basic tool to analysis a matrix. • Many problems of linear algebra can be better understood if we first ask the question:what if we take the SVD ? Danping Zou @Shanghai Jiao Tong University 27 SVD • The SVD is motivated by the following geometric fact: – The image of the unit sphere under any matrix is a hyper-ellipse (超椭球) Orthogonal bases of the Orthogonal bases of the original space target space Danping Zou @Shanghai Jiao Tong University 28 SVD • From the geometric interpretation, we have the following equations: . • By collecting all those equations together, we have or compactly, . Since has orthogonal columns, we get Danping Zou @Shanghai Jiao Tong University 29 SVD • Back to the 2D case, we have Left singular vectors Singular values Right singular vectors Danping Zou @Shanghai Jiao Tong University 30 SVD • Step by step interpretation – Step 1. map (rotation + with/without reflection) the bases to the canonical frame. Danping Zou @Shanghai Jiao Tong University 31 SVD • Step by step interpretation – Step 2. Stretch the axes Danping Zou @Shanghai Jiao Tong University 32 SVD • Step by step interpretation – Step 3. rotate the canonical axes Danping Zou @Shanghai Jiao Tong University 33 SVD • In the step 2, what if we set ? • We have : is the null space of A Danping Zou @Shanghai Jiao Tong University 34 Null space from SVD • So the null space of a matrix can be obtained by SVD decomposition. • The bases of the null space are the right singular vectors that corresponds to the zero singular values. Danping Zou @Shanghai Jiao Tong University 35 3D projective geometry • Back to the plane problem: Three points define a plane : • Its null space can be solved by SVD Danping Zou @Shanghai Jiao Tong University 36 3D projective geometry • Three planes define a point: • Its null space can be solved by SVD Danping Zou @Shanghai Jiao Tong University 37 Summary • 3D points vs. 3D Planes • Transformations of 3D points and 3D lines • Three planes define a point / Three points define a plane • How to solve a homogenous equation • Null space of a matrix • Geometric interpretation of SVD Danping Zou @Shanghai Jiao Tong University 38 3D projective geometry • Hierarchy of 3D transformation Danping Zou @Shanghai Jiao Tong University 39 3D projective geometry • Euclidean transformation (Rigid body transformation) • A mapping is a rigid body transformation if it satisfies 1) Length is preserved : 2) The cross product is preserved: Danping Zou @Shanghai Jiao Tong University 40 3D projective geometry • Homogenous form vs. inhomogenous form Homogenous: Inhomogenous: • About the rotation matrix Danping Zou @Shanghai Jiao Tong University 41 3D projective geometry • 3D Rotation matrix transforms three orthogonal axes into r1, r2, r3 in the new coordinate system. r3 r2 r1 More about 3D rotation will be discussed in the later lectures. Danping Zou @Shanghai Jiao Tong University 42 3D projective geometry • Exercise: 1. Write a small program to compute the harries corner detector. Show all the intermediate results as shown in the slides. Requirements: 1) source codes + executable (any language, but with details how to run it) 2) result analysis (world <= 2 pages) 2. Write a small program to rectify a distorted planar image to a normal one as shown (Page 13) Requirements - The same as the previous one. Deadline : Oct 27th Danping Zou @Shanghai Jiao Tong University 43 3D Lines • A line is defined by join of two points or intersection of two planes. • Lines have 4 degrees of freedom in 3D-space Danping Zou @Shanghai Jiao Tong University 44 3D Lines • Plücker matrix: A line can be defined from two points
Recommended publications
  • Projective Geometry: a Short Introduction
    Projective Geometry: A Short Introduction Lecture Notes Edmond Boyer Master MOSIG Introduction to Projective Geometry Contents 1 Introduction 2 1.1 Objective . .2 1.2 Historical Background . .3 1.3 Bibliography . .4 2 Projective Spaces 5 2.1 Definitions . .5 2.2 Properties . .8 2.3 The hyperplane at infinity . 12 3 The projective line 13 3.1 Introduction . 13 3.2 Projective transformation of P1 ................... 14 3.3 The cross-ratio . 14 4 The projective plane 17 4.1 Points and lines . 17 4.2 Line at infinity . 18 4.3 Homographies . 19 4.4 Conics . 20 4.5 Affine transformations . 22 4.6 Euclidean transformations . 22 4.7 Particular transformations . 24 4.8 Transformation hierarchy . 25 Grenoble Universities 1 Master MOSIG Introduction to Projective Geometry Chapter 1 Introduction 1.1 Objective The objective of this course is to give basic notions and intuitions on projective geometry. The interest of projective geometry arises in several visual comput- ing domains, in particular computer vision modelling and computer graphics. It provides a mathematical formalism to describe the geometry of cameras and the associated transformations, hence enabling the design of computational ap- proaches that manipulates 2D projections of 3D objects. In that respect, a fundamental aspect is the fact that objects at infinity can be represented and manipulated with projective geometry and this in contrast to the Euclidean geometry. This allows perspective deformations to be represented as projective transformations. Figure 1.1: Example of perspective deformation or 2D projective transforma- tion. Another argument is that Euclidean geometry is sometimes difficult to use in algorithms, with particular cases arising from non-generic situations (e.g.
    [Show full text]
  • Arxiv:1910.10745V1 [Cond-Mat.Str-El] 23 Oct 2019 2.2 Symmetry-Protected Time Crystals
    A Brief History of Time Crystals Vedika Khemania,b,∗, Roderich Moessnerc, S. L. Sondhid aDepartment of Physics, Harvard University, Cambridge, Massachusetts 02138, USA bDepartment of Physics, Stanford University, Stanford, California 94305, USA cMax-Planck-Institut f¨urPhysik komplexer Systeme, 01187 Dresden, Germany dDepartment of Physics, Princeton University, Princeton, New Jersey 08544, USA Abstract The idea of breaking time-translation symmetry has fascinated humanity at least since ancient proposals of the per- petuum mobile. Unlike the breaking of other symmetries, such as spatial translation in a crystal or spin rotation in a magnet, time translation symmetry breaking (TTSB) has been tantalisingly elusive. We review this history up to recent developments which have shown that discrete TTSB does takes place in periodically driven (Floquet) systems in the presence of many-body localization (MBL). Such Floquet time-crystals represent a new paradigm in quantum statistical mechanics — that of an intrinsically out-of-equilibrium many-body phase of matter with no equilibrium counterpart. We include a compendium of the necessary background on the statistical mechanics of phase structure in many- body systems, before specializing to a detailed discussion of the nature, and diagnostics, of TTSB. In particular, we provide precise definitions that formalize the notion of a time-crystal as a stable, macroscopic, conservative clock — explaining both the need for a many-body system in the infinite volume limit, and for a lack of net energy absorption or dissipation. Our discussion emphasizes that TTSB in a time-crystal is accompanied by the breaking of a spatial symmetry — so that time-crystals exhibit a novel form of spatiotemporal order.
    [Show full text]
  • The Fractal Dimension of Product Sets
    THE FRACTAL DIMENSION OF PRODUCT SETS A PREPRINT Clayton Moore Williams Brigham Young University [email protected] Machiel van Frankenhuijsen Utah Valley University [email protected] February 26, 2021 ABSTRACT Using methods from nonstandard analysis, we define a nonstandard Minkowski dimension which exists for all bounded sets and which has the property that dim(A × B) = dim(A) + dim(B). That is, our new dimension is “product-summable”. To illustrate our theorem we generalize an example of Falconer’s1 to show that the standard upper Minkowski dimension, as well as the Hausdorff di- mension, are not product-summable. We also include a method for creating sets of arbitrary rational dimension. Introduction There are several notions of dimension used in fractal geometry, which coincide for many sets but have important, distinct properties. Indeed, determining the most proper notion of dimension has been a major problem in geometric measure theory from its inception, and debate over what it means for a set to be fractal has often reduced to debate over the propernotion of dimension. A classical example is the “Devil’s Staircase” set, which is intuitively fractal but which has integer Hausdorff dimension2. As Falconer notes in The Geometry of Fractal Sets3, the Hausdorff dimension is “undoubtedly, the most widely investigated and most widely used” notion of dimension. It can, however, be difficult to compute or even bound (from below) for many sets. For this reason one might want to work with the Minkowski dimension, for which one can often obtain explicit formulas. Moreover, the Minkowski dimension is computed using finite covers and hence has a series of useful identities which can be used in analysis.
    [Show full text]
  • Fractal-Based Methods As a Technique for Estimating the Intrinsic Dimensionality of High-Dimensional Data: a Survey
    INFORMATICA, 2016, Vol. 27, No. 2, 257–281 257 2016 Vilnius University DOI: http://dx.doi.org/10.15388/Informatica.2016.84 Fractal-Based Methods as a Technique for Estimating the Intrinsic Dimensionality of High-Dimensional Data: A Survey Rasa KARBAUSKAITE˙ ∗, Gintautas DZEMYDA Institute of Mathematics and Informatics, Vilnius University Akademijos 4, LT-08663, Vilnius, Lithuania e-mail: [email protected], [email protected] Received: December 2015; accepted: April 2016 Abstract. The estimation of intrinsic dimensionality of high-dimensional data still remains a chal- lenging issue. Various approaches to interpret and estimate the intrinsic dimensionality are deve- loped. Referring to the following two classifications of estimators of the intrinsic dimensionality – local/global estimators and projection techniques/geometric approaches – we focus on the fractal- based methods that are assigned to the global estimators and geometric approaches. The compu- tational aspects of estimating the intrinsic dimensionality of high-dimensional data are the core issue in this paper. The advantages and disadvantages of the fractal-based methods are disclosed and applications of these methods are presented briefly. Key words: high-dimensional data, intrinsic dimensionality, topological dimension, fractal dimension, fractal-based methods, box-counting dimension, information dimension, correlation dimension, packing dimension. 1. Introduction In real applications, we confront with data that are of a very high dimensionality. For ex- ample, in image analysis, each image is described by a large number of pixels of different colour. The analysis of DNA microarray data (Kriukien˙e et al., 2013) deals with a high dimensionality, too. The analysis of high-dimensional data is usually challenging.
    [Show full text]
  • Euclidean Versus Projective Geometry
    Projective Geometry Projective Geometry Euclidean versus Projective Geometry n Euclidean geometry describes shapes “as they are” – Properties of objects that are unchanged by rigid motions » Lengths » Angles » Parallelism n Projective geometry describes objects “as they appear” – Lengths, angles, parallelism become “distorted” when we look at objects – Mathematical model for how images of the 3D world are formed. Projective Geometry Overview n Tools of algebraic geometry n Informal description of projective geometry in a plane n Descriptions of lines and points n Points at infinity and line at infinity n Projective transformations, projectivity matrix n Example of application n Special projectivities: affine transforms, similarities, Euclidean transforms n Cross-ratio invariance for points, lines, planes Projective Geometry Tools of Algebraic Geometry 1 n Plane passing through origin and perpendicular to vector n = (a,b,c) is locus of points x = ( x 1 , x 2 , x 3 ) such that n · x = 0 => a x1 + b x2 + c x3 = 0 n Plane through origin is completely defined by (a,b,c) x3 x = (x1, x2 , x3 ) x2 O x1 n = (a,b,c) Projective Geometry Tools of Algebraic Geometry 2 n A vector parallel to intersection of 2 planes ( a , b , c ) and (a',b',c') is obtained by cross-product (a'',b'',c'') = (a,b,c)´(a',b',c') (a'',b'',c'') O (a,b,c) (a',b',c') Projective Geometry Tools of Algebraic Geometry 3 n Plane passing through two points x and x’ is defined by (a,b,c) = x´ x' x = (x1, x2 , x3 ) x'= (x1 ', x2 ', x3 ') O (a,b,c) Projective Geometry Projective Geometry
    [Show full text]
  • Lecture 6: Definition and Construction of Finite Element Subspaces
    18 NUMERICAL SOLUTION OF PDES 2.6. Definition of finite elements. We first define triangular finite element spaces, consid- ering the case when Ω is a convex polygon. For each 0 < h < 1, we let Th be a triangulation of Ω¯ with the following properties: i: Ω¯ = ∪iTi, ii: If Ti and Tj are distinct, then exactly one of the following holds: (a) Ti ∩ Tj = ∅, (b) Ti ∩ Tj is a common vertex, (c) Ti ∩ Tj is a common side. iii: each Ti ∈ Th has diameter ≤ h. B ¢B ¢@ ¢ B PP B ¢ @ B PB¢ B¢ ¢ @ B @ ¢ @ PP B ¢ PB @P¢ PPPBB¢¢ PP PP PP Triangulation of Ω P ¢B PP ¢ B PP ¢@ ¢ B B @ ¢ @ P B @¢ ¢B ¢B PPB @ ¢ B ¢ B @¢ B¢ B @ @ Not allowed @@ @@ @ @ Given a triangulation Th of Ω, a finite element space is a space of piecewise polynomials with respect to Th that is constructed by specifying the following things for each T ∈ Th: Shape functions: a finite dimensional space V (T ) of polynomial functions on T . Degrees of freedom (DOF): a finite set of linear functionals ψi : V (T ) → R (i = 1,..., N) which are unisolvent on V (T ), i.e., if V (T ) has dimension N, then given any numbers αi, i = 1,..., N, there exists a unique function p ∈ V (T ), such that ψi(p) = αi, i = 1,..., N. Since these equations amount to a square linear system of equations, to show unisolvence, we show that the only solution of the system with all αi = 0 is p = 0. A typical example of a DOF is ψi(p) = p(xi).
    [Show full text]
  • Dimension Theory: Road to the Forth Dimension and Beyond
    Dimension Theory: Road to the Fourth Dimension and Beyond 0-dimension “Behold yon miserable creature. That Point is a Being like ourselves, but confined to the non-dimensional Gulf. He is himself his own World, his own Universe; of any other than himself he can form no conception; he knows not Length, nor Breadth, nor Height, for he has had no experience of them; he has no cognizance even of the number Two; nor has he a thought of Plurality, for he is himself his One and All, being really Nothing. Yet mark his perfect self-contentment, and hence learn this lesson, that to be self-contented is to be vile and ignorant, and that to aspire is better than to be blindly and impotently happy.” ― Edwin A. Abbott, Flatland: A Romance of Many Dimensions 0-dimension Space of zero dimensions: A space that has no length, breadth or thickness (no length, height or width). There are zero degrees of freedom. The only “thing” is a point. = ∅ 0-dimension 1-dimension Space of one dimension: A space that has length but no breadth or thickness A straight or curved line. Drag a multitude of zero dimensional points in new (perpendicular) direction Make a “line” of points 1-dimension One degree of freedom: Can only move right/left (forwards/backwards) { }, any point on the number line can be described by one number 1-dimension How to visualize living in 1-dimension Stuck on an endless one-lane one-way road Inhabitants: points and line segments (intervals) Live forever between your front and back neighbor.
    [Show full text]
  • Nonconforming Finite Element Spaces for $2 M $-Th Order Partial Differential Equations on $\Mathbb {R}^ N $ Simplicial Grids When $ M= N+ 1$
    NONCONFORMING FINITE ELEMENT SPACES FOR 2m-TH ORDER PARTIAL DIFFERENTIAL EQUATIONS ON Rn SIMPLICIAL GRIDS WHEN m = n + 1 SHUONAN WU AND JINCHAO XU Abstract. In this paper, we propose a family of nonconforming finite ele- n ments for 2m-th order partial differential equations in R on simplicial grids when m = n + 1. This family of nonconforming elements naturally extends the elements proposed by Wang and Xu [Math. Comp. 82(2013), pp. 25{43] , where m ≤ n is required. We prove the unisolvent property by induction on the dimensions using the similarity properties of both shape function spaces and degrees of freedom. The proposed elements have approximability, pass the generalized patch test and hence converge. We also establish quasi-optimal er- ror estimates in the broken H3 norm for the 2D nonconforming element. In addition, we propose an H3 nonconforming finite element that is robust for the sixth order singularly perturbed problems in 2D. These theoretical results are further validated by the numerical tests for the 2D tri-harmonic problem. 1. Introduction In [38], Wang and Xu proposed a family of nonconforming finite elements for 2m-th order elliptic partial differential equations in Rn on simplicial grids, with the requirement that m ≤ n. These elements (named Morley-Wang-Xu or MWX elements) are simple and elegant when compared to the conforming finite elements, with a combination of simplicial geometry, polynomial space, and convergence anal- ysis. For example, in 3D, the minimal polynomial degrees of the H2 and H3 con- forming finite elements are 9 and 17, respectively (cf. [2, 42]), while those of MWX elements are only 2 and 3, respectively.
    [Show full text]
  • Arxiv:2101.09203V1 [Gr-Qc] 22 Jan 2021 a Powerful Selection Principle Can Be Implemented by Mation Behavior (Sec.III)
    Coordinate conditions and field equations for pure composite gravity Hans Christian Ottinger¨ ∗ ETH Z¨urich,Department of Materials, CH-8093 Z¨urich,Switzerland (Dated: January 25, 2021) Whenever an alternative theory of gravity is formulated in a background Minkowski space, the conditions characterizing admissible coordinate systems, in which the alternative theory of gravity may be applied, play an important role. We here propose Lorentz covariant coordinate condi- tions for the composite theory of pure gravity developed from the Yang-Mills theory based on the Lorentz group, thereby completing this previously proposed higher derivative theory of gravity. The physically relevant static isotropic solutions are determined by various methods, the high-precision predictions of general relativity are reproduced, and an exact black-hole solution with mildly singular behavior is found. I. INTRODUCTION As the composite theory of gravity [9], just like the underlying Yang-Mills theory, is formulated in a back- Only two years after the discovery of Yang-Mills theo- ground Minkowski space, the question arises how to char- ries [1], it has been recognized that that there is a strik- acterize the \good" coordinate systems in which the the- ing formal relationship between the Riemann curvature ory may be applied. This characterization should be tensor of general relativity and the field tensor of the Lorentz invariant, but not invariant under more general Yang-Mills theory based on the Lorentz group [2]. How- coordinate transformations, that is, it shares the formal ever, developing this particular Yang-Mills theory into a properties of coordinate conditions in general relativity. consistent and convincing theory of gravity is not at all However, the unique solutions obtained from Einstein's straightforward.
    [Show full text]
  • Degrees of Freedom in Multiple-Antenna Channels: a Signal Space Approach Ada S
    1 Degrees of Freedom in Multiple-Antenna Channels: A Signal Space Approach Ada S. Y. Poon, Member, IEEE, Robert W. Brodersen, Fellow, IEEE, and David N. C. Tse, Member, IEEE Abstract— We consider multiple-antenna systems that are lim- time samples will also not increase the capacity indefinitely. ited by the area and geometry of antenna arrays. Given these The available degrees of freedom is fundamentally limited to physical constraints, we determine the limit to the number of 2WT. In this paper, we will demonstrate that the physical spatial degrees of freedom available and find that the commonly used statistical multi-input multi-output model is inadequate. An- constraint of antenna arrays and propagation environment put tenna theory is applied to take into account the area and geometry forth a deterministic limit to the spatial degrees of freedom constraints, and define the spatial signal space so as to interpret underlying the statistical MIMO approach. experimental channel measurements in an array-independent but Let us review the reasoning involved to derive the 2WT manageable description of the physical environment. Based on formula [3, Ch. 8]. In waveform channels, the transmit and these modeling strategies, we show that for a spherical array of effective aperture A in a physical environment of angular spread receive signals are represented either in the time domain |Ω| in solid angle, the number of spatial degrees of freedom as waveforms or in the frequency domain as spectra. The is A|Ω| for uni-polarized antennas and 2A|Ω| for tri-polarized mapping between these two representations is the Fourier antennas.
    [Show full text]
  • Projective Geometry
    Projective geometry Projective geometry is used for its simplicity in formalism. n T A point in projective n-space, P , is given by a (n+1) -vector of coordinates x= (x0, x 1 ,….., x n ) . At least one of these coordinates should differ from zero. These coordin ates are called homogeneous coordinates. Two points represented by (n+1)- vectors x and y are equal if and only if there exists a nonzero scalar k such that x = ky. This will be indicated by x ~ y . Often the points with coordinate xn = 0 are said to be at infinity. The projective plane The projective plane is the projective space . A point of is represented by a 3 -vector . A line is also represented by a 3 -vector. A point is located on a line if and only if This equation can however also be interpreted as expressing that the line passes through the point . This symmetry in the equation shows that ther e is no formal difference between points and lines in the projective plane. This is known as the principle of duality . A line passing through two points and is given by their vector product . This can also be written as The dual formulation gives the i ntersection of two lines , i.e. the intersection of two lines l and l’ can be obtained by x = l l’ . Projective 3 -space Projective 3D space is the projective space . A point of is represented by a 4 -vector . In the dual entity of a point is a plane, which is also represented by a 4 - vector.
    [Show full text]
  • A Search Algorithm for Motion Planning with Six Degrees of Freedom*
    ARTIFICIAL INTELLIGENCE 295 A Search Algorithm for Motion Planning with Six Degrees of Freedom* Bruce R. Donald Artificial Intelligence Laboratory, Massachusetts Institute of Technology, Cambridge, MA 02139, U.S.A. Recommended by H.H. Nagel and Daniel G. Bobrow ABSTRACT The motion planning problem is of central importance to the fields of robotics, spatial planning, and automated design. In robotics we are interested in the automatic synthesis of robot motions, given high-level specifications of tasks and geometric models of the robot and obstacles. The "Movers' "' problem is to find a continuous, collision-free path for a moving object through an environment containing obstacles. We present an implemented algorithm for the classical formulation of the three-dimensional Movers' problem: Given an arbitrary rigid polyhedral moving object P with three translational and three rotational degrees of freedom, find a continuous, collision-free path taking P from some initial configuration to a desired goal configuration. This paper describes an implementation of a complete algorithm (at a given resolution)for the full six degree of freedom Movers' problem. The algorithm transforms the six degree of freedom planning problem into a point navigation problem in a six-dimensional configuration space (called C-space). The C-space obstacles, which characterize the physically unachievable configurations, are directly represented by six-dimensional manifolds whose boundaries are five-dimensional C-surfaces. By characterizing these surfaces and their intersections, collision-free paths may be found by the closure of three operators which ( i) slide along five-dimensional level C-surfaces parallel to C-space obstacles; (ii) slide along one- to four-dimensional intersections of level C-surfaces; and (iii) jump between six-dimensional obstacles.
    [Show full text]