LINEAR ALGEBRA a Pathway to Abstract Mathematics 3Rd Edition

Total Page:16

File Type:pdf, Size:1020Kb

LINEAR ALGEBRA a Pathway to Abstract Mathematics 3Rd Edition LINEAR ALGEBRA A Pathway to Abstract Mathematics 3rd Edition G. Viglino Ramapo College of New Jersey January 2018 Contents CONTENTS CHAPTER 1 MATRICES AND SYSTEMS OF LINEAR EQUATION 1.1 Systems of Linear Equations 1 1.2 Consistent and Inconsistent Systems of Equations 14 Chapter Summary 27 CHAPTER 2 VECTOR SPACES 2.1 Vectors in the plane, and Beyond 31 2.2 Abstract Vector Spaces 40 2.3 Properties of Vector Spaces 51 2.4 Subspaces 59 2.5 Lines and Planes 68 Chapter Summary 75 CHAPTER 3 BASES AND DIMENSION 3.1 Spanning Sets 77 3.2 Linear Independence 86 3.3 Bases 94 Chapter Summary 109 CHAPTER4 LINEARITY 4.1 Linear Transformations 111 4.2 Image and Kernel 124 4.3 Isomorphisms 135 Chapter Summary 149 CHAPTER 5 MATRICES AND LINEAR MAPS 5.1 Matrix Multiplication 151 5.2 Invertible Matrices 165 5.3 Matrix Representation of Linear Maps 178 5.4 Change of Basis 191 Chapter Summary 202 Contents CHAPTER 6 DETERMINANTS AND EIGENVECTORS 6.1 Determinants 205 6.2 Eigenspaces 218 6.3 Diagonalization 233 6.4 Applications 246 6.5 Markov Chains 259 Chapter Summary 275 CHAPTER 7 INNER PRODUCT SPACES 7.1 Dot Product 279 7.2 Inner Product 292 7.3 Orthogonality 301 7.4. The Spectral Theorem 315 Chapter Summary 307 Appendix A Principle of Mathematical Induction Appendix B Solutions to Check Your Understanding Boxes Appendix C Answers to Selected Odd-Numbered Exercises Preface PREFACE There is no mathematical ramp that will enable you to continuously inch your way higher and higher in mathematics. The climb calls for a ladder consisting of discrete steps designed to take you from one mathematical level to another. You are about to take an important step on that lad- der, one that will take you to a plateau where mathematical abstraction abounds. Linear algebra rests on a small number of axioms (accepted rules, or “laws”), upon which a beautiful and practi- cal theory emerges. Technology can be used to reduce the time needed to perform essential but routine tasks. We fea- ture the TI-84+ calculator, but any graphing utility or Computer Algebraic System will do. The real value of whatever technological tool you use is that it will free you to spend more time on the development and comprehension of the theory and its applications. In any event, if you haven’t already discovered in other courses: MATHEMATICS DOES NOT RUN ON BATTERIES Systems of linear equations are introduced and analyzed in Chapter 1. Graphing utilities can be used to solve such systems, but understanding what those solutions represent plays a dominant role throughout the text. We begin Chapter 2 by sowing the seeds for vector spaces in the fertile real number field, where they soon blossom into the concept of an abstract vector. The remainder of Chapter 2 and all of Chapter 3 are dedicated to a study of vector spaces in isolation. Functions from one vector space to another which, in a sense, respect the algebraic structure of those spaces are investigated in Chapters 4 and 5. The sixth chapter focuses on Eigenvalues and Eigenvectors, along with some of their important applications. The first six chapters may provide a full plate for most one-semester courses. If not, then Chap- ter 7 (on inner product spaces) is offered for dessert. We have made every effort to provide a leg-up for the step you are about to take. Our primary goal was to write a readable book, without compromising mathematical integrity. Along the way, you will encounter numerous Check Your Understanding boxes designed to challenge your under- standing of each newly introduced concept. Complete solutions to the problems in those boxes appear in Appendix B, but please don’t be in too much of a hurry to look at our solutions. You should TRY to solve the problems on your own, for it is only through ATTEMPTING to solve a problem that one grows mathematically. In the words of Descartes: We never understand a thing so well, and make it our own, when we learn it from another, as when we have discovered it for ourselves. 1.1 Systems of Linear Equations 1 1 CHAPTER 1 MATRICES AND SYSTEMS OF LINEAR EQUATIONS Much of the development of linear algebra calls for the solution and interpretation of systems of linear equations. While the “solution part” can be relegated to a calculator, the “interpretation part” cannot. We focus on the solution-part of the process in Section 1, and on the more important interpretation-part in Sections 2. §1. SYSTEMS OF LINEAR EQUATIONS To solve the system of equations: 2x +64y – 4z = 2x ++6y 4z = 0 xy++2z = – 2 is to determine values of the variables (or unknowns) x, y, and z for which each of the three equations is satisfied. You certainly solved such systems in earlier courses, and if you take the time to solve the above Brackets are used to denote sets. In particular, system, you will find that it has but one solution: –11– 1 x ===–11 y z –1 . We can also say that the three-tuple denotes the set containing but one element—the ele- –11– 1 is a solution of the given system of equation, and that ment –11– 1 . –11– 1 is its solution set. In general: An (ordered) n-tuple is an expression of the form c1c2 cn , where each ci is a real number (written ci ), for 1 in. We say that the n-tuple c1c2 cn is a solution of the system of m equations in n unknowns: The x s denote variables a11x1 ++a12x2 a1nxn = b1 i (or unknowns), while the a x ++a x a x = b 21 1 22 2 2n n 2 aij ’s and bi ’s are con- . ... stants (or scalars). ... ... am1x1 ++am2x2 amnxn = bm if each equation in the system is satisfied when ci is substi- tuted for xi , for 1 in. The set of all solutions of a system of equations is said to be the solution set of that system. 2 Chapter 1 Matrices and Systems of Linear Equations EQUIVALENT SYSTEMS OF EQUATIONS Consider the system of equations: – 3x +2y = x 1 ---2+ y = --- 2 2 As you know, you can perform certain operations on that system which will not alter its solution set. For example, you can: (1) Interchange the order of the equations: – 3x +2y = x 1 ---2+ y = --- x 1 2 2 ---2+ y = --- 2 2 – 3x +2y = (2) Multiply both sides of the resulting top equation by 2: x 1 ---2+ y = --- x +14y = 2 2 – 3x +2y = – 3x +2y = (3) Multiply the resulting top equation by 3 and add it to the bottom You used this third equation: maneuver a lot when eliminating a variable x +14y = x +14y = from a given system of equations For example: – 3x +2y = 13y = 5 (i) x +13yz– = multiply by 3 3x +312y = (2) 2x –35y +3z = – 3x +2y = (3) – 3x ++y 2z = 2 add: 13y = 5 multiply (1) by -2 and add it to (2) The above three operations, are said to be elementary equation –511y +1z = operations: 10yz–5= multiply (1) by 3 and add it ELEMENTARY OPERATIONS ON to (3) SYSTEMS OF LINEAR EQUATIONS Interchange the order of any two equations in the system. Multiply both sides of an equation by a nonzero number. Add a multiple of one equation to another equation. EQUIVALENT SYSTEM Two systems of equations sharing a common solution set are said to OF EQUATIONS be equivalent. As you may recall: THEOREM 1.1 Performing any sequence of elementary opera- tions on a system of linear equations will result in an equivalent system of equations. 1.1 Systems of Linear Equations 3 AUGMENTED MATRICES Matrices are arrays of numbers (or expressions representing numbers) arranged in rows and columns: 47 17 0 10 2134 10 6 36 5 12 7 4 1 –739 –38 11 2– 12 9 (i) (ii) (iii) (iv) (v) Matrix (i) contains 2 rows and 3 columns and it is said to be a 23 (two-by-three) matrix. Similarly, (ii) is a 32 matrix, and (iii) is a 33 matrix (a square matrix). In general, an mn matrix is a matrix consisting of m rows and n columns. In particular, (iv) is a 13 matrix (a row matrix), and (v) is a 31 matrix (a column matrix). It is often convenient to represent a system of equations in a more com- pact matrix form. The rows of the matrix in Figure 1.1(b), for example, concisely represents the equations in Figure 1.1(a). Note that the vari- ables x, y, and z are suppressed in the matrix form, and that the vertical line recalls the equal sign in the equations. Such a matrix is said to be the augmented matrix associated with the given system of equations. 2x +64y – 4z = 24–6 4 2x ++6y 4z = 0 26 4 0 AUGMENTED MATRIX xy++2z = – 2 11 2– 2 System of Equations Augmented Matrix (a) (b) Figure 1.1 Switching two equations in a system of equations results in the switching of the corresponding rows in the associated augmented matrix. Indeed, each of the three previously introduced elementary equation operations corresponds with one of the following elementary matrix row operations: ELEMENTARY MATRIX ROW OPERATIONS Interchange the order of any two rows in the matrix. Multiply each element in a row of the matrix by a nonzero number. Add a multiple of one row of the matrix to another row of the matrix. The following terminology is motivated by Theorem 1.1: DEFINITION 1.1 Two matrices are equivalent if one can be EQUIVALENT derived from the other by performing elemen- MATRICES tary row operations.
Recommended publications
  • 1 Euclidean Vector Space and Euclidean Affi Ne Space
    Profesora: Eugenia Rosado. E.T.S. Arquitectura. Euclidean Geometry1 1 Euclidean vector space and euclidean a¢ ne space 1.1 Scalar product. Euclidean vector space. Let V be a real vector space. De…nition. A scalar product is a map (denoted by a dot ) V V R ! (~u;~v) ~u ~v 7! satisfying the following axioms: 1. commutativity ~u ~v = ~v ~u 2. distributive ~u (~v + ~w) = ~u ~v + ~u ~w 3. ( ~u) ~v = (~u ~v) 4. ~u ~u 0, for every ~u V 2 5. ~u ~u = 0 if and only if ~u = 0 De…nition. Let V be a real vector space and let be a scalar product. The pair (V; ) is said to be an euclidean vector space. Example. The map de…ned as follows V V R ! (~u;~v) ~u ~v = x1x2 + y1y2 + z1z2 7! where ~u = (x1; y1; z1), ~v = (x2; y2; z2) is a scalar product as it satis…es the …ve properties of a scalar product. This scalar product is called standard (or canonical) scalar product. The pair (V; ) where is the standard scalar product is called the standard euclidean space. 1.1.1 Norm associated to a scalar product. Let (V; ) be a real euclidean vector space. De…nition. A norm associated to the scalar product is a map de…ned as follows V kk R ! ~u ~u = p~u ~u: 7! k k Profesora: Eugenia Rosado, E.T.S. Arquitectura. Euclidean Geometry.2 1.1.2 Unitary and orthogonal vectors. Orthonormal basis. Let (V; ) be a real euclidean vector space. De…nition.
    [Show full text]
  • Glossary of Linear Algebra Terms
    INNER PRODUCT SPACES AND THE GRAM-SCHMIDT PROCESS A. HAVENS 1. The Dot Product and Orthogonality 1.1. Review of the Dot Product. We first recall the notion of the dot product, which gives us a familiar example of an inner product structure on the real vector spaces Rn. This product is connected to the Euclidean geometry of Rn, via lengths and angles measured in Rn. Later, we will introduce inner product spaces in general, and use their structure to define general notions of length and angle on other vector spaces. Definition 1.1. The dot product of real n-vectors in the Euclidean vector space Rn is the scalar product · : Rn × Rn ! R given by the rule n n ! n X X X (u; v) = uiei; viei 7! uivi : i=1 i=1 i n Here BS := (e1;:::; en) is the standard basis of R . With respect to our conventions on basis and matrix multiplication, we may also express the dot product as the matrix-vector product 2 3 v1 6 7 t î ó 6 . 7 u v = u1 : : : un 6 . 7 : 4 5 vn It is a good exercise to verify the following proposition. Proposition 1.1. Let u; v; w 2 Rn be any real n-vectors, and s; t 2 R be any scalars. The Euclidean dot product (u; v) 7! u · v satisfies the following properties. (i:) The dot product is symmetric: u · v = v · u. (ii:) The dot product is bilinear: • (su) · v = s(u · v) = u · (sv), • (u + v) · w = u · w + v · w.
    [Show full text]
  • Vector Differential Calculus
    KAMIWAAI – INTERACTIVE 3D SKETCHING WITH JAVA BASED ON Cl(4,1) CONFORMAL MODEL OF EUCLIDEAN SPACE Submitted to (Feb. 28,2003): Advances in Applied Clifford Algebras, http://redquimica.pquim.unam.mx/clifford_algebras/ Eckhard M. S. Hitzer Dept. of Mech. Engineering, Fukui Univ. Bunkyo 3-9-, 910-8507 Fukui, Japan. Email: [email protected], homepage: http://sinai.mech.fukui-u.ac.jp/ Abstract. This paper introduces the new interactive Java sketching software KamiWaAi, recently developed at the University of Fukui. Its graphical user interface enables the user without any knowledge of both mathematics or computer science, to do full three dimensional “drawings” on the screen. The resulting constructions can be reshaped interactively by dragging its points over the screen. The programming approach is new. KamiWaAi implements geometric objects like points, lines, circles, spheres, etc. directly as software objects (Java classes) of the same name. These software objects are geometric entities mathematically defined and manipulated in a conformal geometric algebra, combining the five dimensions of origin, three space and infinity. Simple geometric products in this algebra represent geometric unions, intersections, arbitrary rotations and translations, projections, distance, etc. To ease the coordinate free and matrix free implementation of this fundamental geometric product, a new algebraic three level approach is presented. Finally details about the Java classes of the new GeometricAlgebra software package and their associated methods are given. KamiWaAi is available for free internet download. Key Words: Geometric Algebra, Conformal Geometric Algebra, Geometric Calculus Software, GeometricAlgebra Java Package, Interactive 3D Software, Geometric Objects 1. Introduction The name “KamiWaAi” of this new software is the Romanized form of the expression in verse sixteen of chapter four, as found in the Japanese translation of the first Letter of the Apostle John, which is part of the New Testament, i.e.
    [Show full text]
  • Basics of Linear Algebra
    Basics of Linear Algebra Jos and Sophia Vectors ● Linear Algebra Definition: A list of numbers with a magnitude and a direction. ○ Magnitude: a = [4,3] |a| =sqrt(4^2+3^2)= 5 ○ Direction: angle vector points ● Computer Science Definition: A list of numbers. ○ Example: Heights = [60, 68, 72, 67] Dot Product of Vectors Formula: a · b = |a| × |b| × cos(θ) ● Definition: Multiplication of two vectors which results in a scalar value ● In the diagram: ○ |a| is the magnitude (length) of vector a ○ |b| is the magnitude of vector b ○ Θ is the angle between a and b Matrix ● Definition: ● Matrix elements: ● a)Matrix is an arrangement of numbers into rows and columns. ● b) A matrix is an m × n array of scalars from a given field F. The individual values in the matrix are called entries. ● Matrix dimensions: the number of rows and columns of the matrix, in that order. Multiplication of Matrices ● The multiplication of two matrices ● Result matrix dimensions ○ Notation: (Row, Column) ○ Columns of the 1st matrix must equal the rows of the 2nd matrix ○ Result matrix is equal to the number of (1, 2, 3) • (7, 9, 11) = 1×7 +2×9 + 3×11 rows in 1st matrix and the number of = 58 columns in the 2nd matrix ○ Ex. 3 x 4 ॱ 5 x 3 ■ Dot product does not work ○ Ex. 5 x 3 ॱ 3 x 4 ■ Dot product does work ■ Result: 5 x 4 Dot Product Application ● Application: Ray tracing program ○ Quickly create an image with lower quality ○ “Refinement rendering pass” occurs ■ Removes the jagged edges ○ Dot product used to calculate ■ Intersection between a ray and a sphere ■ Measure the length to the intersection points ● Application: Forward Propagation ○ Input matrix * weighted matrix = prediction matrix http://immersivemath.com/ila/ch03_dotprodu ct/ch03.html#fig_dp_ray_tracer Projections One important use of dot products is in projections.
    [Show full text]
  • A Guided Tour to the Plane-Based Geometric Algebra PGA
    A Guided Tour to the Plane-Based Geometric Algebra PGA Leo Dorst University of Amsterdam Version 1.15{ July 6, 2020 Planes are the primitive elements for the constructions of objects and oper- ators in Euclidean geometry. Triangulated meshes are built from them, and reflections in multiple planes are a mathematically pure way to construct Euclidean motions. A geometric algebra based on planes is therefore a natural choice to unify objects and operators for Euclidean geometry. The usual claims of `com- pleteness' of the GA approach leads us to hope that it might contain, in a single framework, all representations ever designed for Euclidean geometry - including normal vectors, directions as points at infinity, Pl¨ucker coordinates for lines, quaternions as 3D rotations around the origin, and dual quaternions for rigid body motions; and even spinors. This text provides a guided tour to this algebra of planes PGA. It indeed shows how all such computationally efficient methods are incorporated and related. We will see how the PGA elements naturally group into blocks of four coordinates in an implementation, and how this more complete under- standing of the embedding suggests some handy choices to avoid extraneous computations. In the unified PGA framework, one never switches between efficient representations for subtasks, and this obviously saves any time spent on data conversions. Relative to other treatments of PGA, this text is rather light on the mathematics. Where you see careful derivations, they involve the aspects of orientation and magnitude. These features have been neglected by authors focussing on the mathematical beauty of the projective nature of the algebra.
    [Show full text]
  • Basics of Euclidean Geometry
    This is page 162 Printer: Opaque this 6 Basics of Euclidean Geometry Rien n'est beau que le vrai. |Hermann Minkowski 6.1 Inner Products, Euclidean Spaces In a±ne geometry it is possible to deal with ratios of vectors and barycen- ters of points, but there is no way to express the notion of length of a line segment or to talk about orthogonality of vectors. A Euclidean structure allows us to deal with metric notions such as orthogonality and length (or distance). This chapter and the next two cover the bare bones of Euclidean ge- ometry. One of our main goals is to give the basic properties of the transformations that preserve the Euclidean structure, rotations and re- ections, since they play an important role in practice. As a±ne geometry is the study of properties invariant under bijective a±ne maps and projec- tive geometry is the study of properties invariant under bijective projective maps, Euclidean geometry is the study of properties invariant under certain a±ne maps called rigid motions. Rigid motions are the maps that preserve the distance between points. Such maps are, in fact, a±ne and bijective (at least in the ¯nite{dimensional case; see Lemma 7.4.3). They form a group Is(n) of a±ne maps whose corresponding linear maps form the group O(n) of orthogonal transformations. The subgroup SE(n) of Is(n) corresponds to the orientation{preserving rigid motions, and there is a corresponding 6.1. Inner Products, Euclidean Spaces 163 subgroup SO(n) of O(n), the group of rotations.
    [Show full text]
  • Math 102 -- Linear Algebra I -- Study Guide
    Math 102 Linear Algebra I Stefan Martynkiw These notes are adapted from lecture notes taught by Dr.Alan Thompson and from “Elementary Linear Algebra: 10th Edition” :Howard Anton. Picture above sourced from (http://i.imgur.com/RgmnA.gif) 1/52 Table of Contents Chapter 3 – Euclidean Vector Spaces.........................................................................................................7 3.1 – Vectors in 2-space, 3-space, and n-space......................................................................................7 Theorem 3.1.1 – Algebraic Vector Operations without components...........................................7 Theorem 3.1.2 .............................................................................................................................7 3.2 – Norm, Dot Product, and Distance................................................................................................7 Definition 1 – Norm of a Vector..................................................................................................7 Definition 2 – Distance in Rn......................................................................................................7 Dot Product.......................................................................................................................................8 Definition 3 – Dot Product...........................................................................................................8 Definition 4 – Dot Product, Component by component..............................................................8
    [Show full text]
  • Clifford Algebra with Mathematica
    Clifford Algebra with Mathematica J.L. ARAGON´ G. ARAGON-CAMARASA Universidad Nacional Aut´onoma de M´exico University of Glasgow Centro de F´ısica Aplicada School of Computing Science y Tecnolog´ıa Avanzada Sir Alwyn William Building, Apartado Postal 1-1010, 76000 Quer´etaro Glasgow, G12 8QQ Scotland MEXICO UNITED KINGDOM [email protected] [email protected] G. ARAGON-GONZ´ ALEZ´ M.A. RODRIGUEZ-ANDRADE´ Universidad Aut´onoma Metropolitana Instituto Polit´ecnico Nacional Unidad Azcapotzalco Departamento de Matem´aticas, ESFM San Pablo 180, Colonia Reynosa-Tamaulipas, UP Adolfo L´opez Mateos, 02200 D.F. M´exico Edificio 9. 07300 D.F. M´exico MEXICO MEXICO [email protected] [email protected] Abstract: The Clifford algebra of a n-dimensional Euclidean vector space provides a general language comprising vectors, complex numbers, quaternions, Grassman algebra, Pauli and Dirac matrices. In this work, we present an introduction to the main ideas of Clifford algebra, with the main goal to develop a package for Clifford algebra calculations for the computer algebra program Mathematica.∗ The Clifford algebra package is thus a powerful tool since it allows the manipulation of all Clifford mathematical objects. The package also provides a visualization tool for elements of Clifford Algebra in the 3-dimensional space. clifford.m is available from https://github.com/jlaragonvera/Geometric-Algebra Key–Words: Clifford Algebras, Geometric Algebra, Mathematica Software. 1 Introduction Mathematica, resulting in a package for doing Clif- ford algebra computations. There exists some other The importance of Clifford algebra was recognized packages and specialized programs for doing Clif- for the first time in quantum field theory.
    [Show full text]
  • Inner Product and Orthogonality
    Math 240 TA: Shuyi Weng Winter 2017 March 10, 2017 Inner Product and Orthogonality Inner Product The notion of inner product is important in linear algebra in the sense that it provides a sensible notion of length and angle in a vector space. This seems very natural in the Euclidean space Rn through the concept of dot product. However, the inner product is much more general and can be extended to other non-Euclidean vector spaces. For this course, you are not required to understand the non-Euclidean examples. I just want to show you a glimpse of linear algebra in a more general setting in mathematics. Definition. Let V be a vector space. An inner product on V is a function h−; −i: V × V ! R such that for all vectors u; v; w 2 V and scalar c 2 R, it satisfies the axioms 1. hu; vi = hv; ui; 2. hu + v; wi = hu; wi + hv; wi, and hu; v + wi = hu; vi + hu; wi; 3. hcu; vi = chu; vi + hu; cvi; 4. hu; ui ≥ 0, and hu; ui = 0 if and only if u = 0. Definition. In a Euclidean space Rn, the dot product of two vectors u and v is defined to be the function u · v = uT v: In coordinates, if we write 2 3 2 3 u1 v1 6 . 7 6 . 7 u = 6 . 7 ; and v = 6 . 7 ; 4 5 4 5 un vn then 2 3 v1 T h i 6 . 7 u · v = u v = u1 ··· un 6 . 7 = u1v1 + ··· unvn: 4 5 vn The definitions in the remainder of this note will assume the Euclidean vector space Rn, and the dot product as the natural inner product.
    [Show full text]
  • 1 Euclidean Vector Spaces
    1 Euclidean Vector Spaces 1.1 Euclidean n-space In this chapter we will generalize the ¯ndings from last chapters for a space with n dimensions, called n-space. De¯nition 1 If n 2 Nnf0g, then an ordered n-tuple is a sequence of n numbers in R:(a1; a2; : : : ; an). The set of all ordered n-tuples is called n-space and is denoted by Rn. The elements in Rn can be perceived as points or vectors, similar to what we have done in 2- and 3-space. (a1; a2; a3) was used to indicate the components of a vector or the coordinates of a point. De¯nition 2 n Two vectors u = (u1; u2; : : : ; un) and v = (v1; v2; : : : ; vn) in R are called equal if u1 = v1; u2 = v2; : : : ; un = vn The sum u + v is de¯ned by u + v = (u1 + v1; u2 + v2; : : : un + vn) If k 2 R the scalar multiple of u is de¯ned by ku = (ku1; ku2; : : : ; kun) These operations are called the standard operations in Rn. De¯nition 3 The zero vector 0 in Rn is de¯ned by 0 = (0; 0;:::; 0) n For u = (u1; u2; : : : ; un) 2 R the negative of u is de¯ned by ¡u = (¡u1; ¡u2;:::; ¡un) The di®erence between two vectors u; v 2 Rn is de¯ned by u ¡ v = u + (¡v) Theorem 1 If u; v and w in Rn and k; l 2 R, then (a) u + v = v + u (b) (u + v) + w = u + (v + w) 1 (c) u + 0 = u (d) u + (¡u) = 0 (e) k(lu) = (kl)u (f) k(u + v) = ku + kv (g) (k + l)u = ku + lu (h) 1u) = u This theorem permits us to manipulate equations without writing them in component form.
    [Show full text]
  • Course Notes Geometric Algebra for Computer Graphics∗ SIGGRAPH 2019
    Course notes Geometric Algebra for Computer Graphics∗ SIGGRAPH 2019 Charles G. Gunn, Ph. D.y ∗Permission to make digital or hard copies of part or all of this work for personal or classroom use is granted without fee provided that copies are not made or distributed for profit or commercial advantage and that copies bear this notice and the full citation on the first page. Copyrights for third-party components of this work must be honored. For all other uses, contact the Owner/Author. Copyright is held by the owner/author(s). SIGGRAPH '19 Courses, July 28 - August 01, 2019, Los Angeles, CA, USA ACM 978-1-4503-6307-5/19/07. 10.1145/3305366.3328099 yAuthor's address: Raum+Gegenraum, Brieselanger Weg 1, 14612 Falkensee, Germany, Email: [email protected] 1 Contents 1 The question 4 2 Wish list for doing geometry 4 3 Structure of these notes 5 4 Immersive introduction to geometric algebra 6 4.1 Familiar components in a new setting . .6 4.2 Example 1: Working with lines and points in 3D . .7 4.3 Example 2: A 3D Kaleidoscope . .8 4.4 Example 3: A continuous 3D screw motion . .9 5 Mathematical foundations 11 5.1 Historical overview . 11 5.2 Vector spaces . 11 5.3 Normed vector spaces . 12 5.4 Sylvester signature theorem . 12 5.5 Euclidean space En ........................... 13 5.6 The tensor algebra of a vector space . 13 5.7 Exterior algebra of a vector space . 14 5.8 The dual exterior algebra . 15 5.9 Projective space of a vector space .
    [Show full text]
  • Normed Vector Spaces
    Normed vector spaces A normed vector space is a vector space where each vector is associated with a “length”. In the 2 or 3 dimensional Euclidean vector space, this notion is intuitive: the norm of a vector can simply be defined to be the length of the arrow. However, the concept of a norm generalizes this idea of the length of an arrow vector. Moreover, the norm of a vector changes when we multiply a vector by a scalar. Thus, a norm implements our intuition that scaling a vector changes its length. Definition 1 More rigorously, a normed vector space is a tuple (V; F ; k:k) where V is a vector space, F is a field, and k:k is a function called the norm that maps vectors to strictly positive lengths: k:k : V! [0; 1) . The norm function must satisfy the following conditions: 1. 8v 2 V kvk ≥ 0 2. kαxk = jαj kxk 3. kx + yk ≤ kxk + kyk Below we outline the intuitive reasoning behind each aspect of the definition of a norm: 1. says that all vectors should have a positive length. This enforces our intuition that a “length” is a positive quantity. 2. says that if we multiply a vector by a scalar, it’s length should increase by the magnitude (i.e. the absolute) value of that scalar. This axiom ties together the notion of scaling vectors (Axiom 6 in the definition of a vector space) and the norm of a vector. 3. says that the length of the sum of two vectors should not exceed the sum of the lengths of each vector.
    [Show full text]