Chapter 3 Euclidean Vector Spaces Vectors in n-space Norm, Dot Product, and Distance in n-space Orthogonality

Slides:



Advertisements
Similar presentations
Chapter 4 Euclidean Vector Spaces
Advertisements

Chapter 6 Vocabulary.
6.3 Vectors in the Plane Many quantities in geometry and physics, such as area, time, and temperature, can be represented by a single real number. Other.
Euclidean m-Space & Linear Equations Euclidean m-space.
Section 9.3 The Dot Product
Chapter 12 – Vectors and the Geometry of Space
6 6.1 © 2012 Pearson Education, Inc. Orthogonality and Least Squares INNER PRODUCT, LENGTH, AND ORTHOGONALITY.
Chapter 5 Orthogonality
Chapter 2 Matrices Definition of a matrix.
Orthogonality and Least Squares
6 6.1 © 2012 Pearson Education, Inc. Orthogonality and Least Squares INNER PRODUCT, LENGTH, AND ORTHOGONALITY.
VECTORS AND THE GEOMETRY OF SPACE 12. VECTORS AND THE GEOMETRY OF SPACE So far, we have added two vectors and multiplied a vector by a scalar.
6.4 Vectors and Dot Products
C HAPTER 4 Inner Product & Orthogonality. C HAPTER O UTLINE Introduction Norm of the Vector, Examples of Inner Product Space - Euclidean n-space - Function.
Length and Dot Product in R n Notes: is called a unit vector. Notes: The length of a vector is also called its norm. Chapter 5 Inner Product Spaces.
6.4 Vectors and Dot Products The Definition of the Dot Product of Two Vectors The dot product of u = and v = is Ex.’s Find each dot product.
Chapter 9-Vectors Calculus, 2ed, by Blank & Krantz, Copyright 2011 by John Wiley & Sons, Inc, All Rights Reserved.
Vectors in 2-Space and 3-Space II
Elementary Linear Algebra Howard Anton Copyright © 2010 by John Wiley & Sons, Inc. All rights reserved. Chapter 3.
Inner Product Spaces Euclidean n-space: Euclidean n-space: vector lengthdot productEuclidean n-space R n was defined to be the set of all ordered.
Vectors and the Geometry of Space
Chapter 5: The Orthogonality and Least Squares
Copyright © Cengage Learning. All rights reserved. 12 Vectors and the Geometry of Space.
CHAPTER FIVE Orthogonality Why orthogonal? Least square problem Accuracy of Numerical computation.
Chapter 5 Orthogonality.
Linear Algebra Chapter 4 Vector Spaces.
1.1 – 1.2 The Geometry and Algebra of Vectors.  Quantities that have magnitude but not direction are called scalars. Ex: Area, volume, temperature, time,
Elementary Linear Algebra Anton & Rorres, 9th Edition
1 MAC 2103 Module 6 Euclidean Vector Spaces I. 2 Rev.F09 Learning Objectives Upon completing this module, you should be able to: 1. Use vector notation.
Chapter 5 General Vector Spaces.
H.Melikyan/12001 Vectors Dr.Hayk Melikyan Departmen of Mathematics and CS
Chapter 6 Additional Topics in Trigonometry
Section 10.2a VECTORS IN THE PLANE. Vectors in the Plane Some quantities only have magnitude, and are called scalars … Examples? Some quantities have.
Vectors CHAPTER 7. Ch7_2 Contents  7.1 Vectors in 2-Space 7.1 Vectors in 2-Space  7.2 Vectors in 3-Space 7.2 Vectors in 3-Space  7.3 Dot Product 7.3.
Chapter Content Real Vector Spaces Subspaces Linear Independence
Euclidean m-Space & Linear Equations Systems of Linear Equations.
Chapter 3 Vectors in n-space Norm, Dot Product, and Distance in n-space Orthogonality.
6 6.1 © 2016 Pearson Education, Inc. Orthogonality and Least Squares INNER PRODUCT, LENGTH, AND ORTHOGONALITY.
Vector Norms and the related Matrix Norms. Properties of a Vector Norm: Euclidean Vector Norm: Riemannian metric:
Elementary Linear Algebra Anton & Rorres, 9th Edition
Chapter 10 Real Inner Products and Least-Square
Chap. 5 Inner Product Spaces 5.1 Length and Dot Product in R n 5.2 Inner Product Spaces 5.3 Orthonormal Bases: Gram-Schmidt Process 5.4 Mathematical Models.
Chapter 4 Euclidean n-Space Linear Transformations from to Properties of Linear Transformations to Linear Transformations and Polynomials.
4.8 Rank Rank enables one to relate matrices to vectors, and vice versa. Definition Let A be an m  n matrix. The rows of A may be viewed as row vectors.
Lecture 9 Vector & Inner Product Space
Copyright © Cengage Learning. All rights reserved. 12 Vectors and the Geometry of Space.
Section 6.2 Angles and Orthogonality in Inner Product Spaces.
Section 3.3 Dot Product; Projections. THE DOT PRODUCT If u and v are vectors in 2- or 3-space and θ is the angle between u and v, then the dot product.
Section 9.3: The Dot Product Practice HW from Stewart Textbook (not to hand in) p. 655 # 3-8, 11, 13-15, 17,
Linear Algebra Chapter 4 n Linear Algebra with Applications –-Gareth Williams n Br. Joel Baumeyer, F.S.C.
Chapter 4 Vector Spaces Linear Algebra. Ch04_2 Definition 1: ……………………………………………………………………. The elements in R n called …………. 4.1 The vector Space R n Addition.
12.3 The Dot Product. The dot product of u and v in the plane is The dot product of u and v in space is Two vectors u and v are orthogonal  if they meet.
Chapter 5 Chapter Content 1. Real Vector Spaces 2. Subspaces 3. Linear Independence 4. Basis and Dimension 5. Row Space, Column Space, and Nullspace 6.
Section 4.1 Euclidean n-Space.
Extending a displacement A displacement defined by a pair where l is the length of the displacement and  the angle between its direction and the x-axix.
1 MAC 2103 Module 4 Vectors in 2-Space and 3-Space I.
Chapter 4 Vector Spaces Linear Algebra. Ch04_2 Definition 1. Let be a sequence of n real numbers. The set of all such sequences is called n-space (or.
Vectors and Dot Products OBJECTIVES: Find the dot product of two vectors and use the properties of the dot product. Find the angle between two vectors.
Inner Product Spaces Euclidean n-space: Euclidean n-space: vector lengthdot productEuclidean n-space R n was defined to be the set of all ordered.
Dot Product of Vectors.
Chapter 1 Linear Equations and Vectors
Elementary Linear Algebra
Lecture 03: Linear Algebra
C H A P T E R 3 Vectors in 2-Space and 3-Space
12.3 The Dot Product.
Linear Algebra Lecture 38.
Vectors and Dot Products
CHAPTER 3 VECTORS NHAA/IMK/UNIMAP.
Linear Vector Space and Matrix Mechanics
Presentation transcript:

Chapter 3 Euclidean Vector Spaces Vectors in n-space Norm, Dot Product, and Distance in n-space Orthogonality

Definition If n is a positive integer, then an ordered n-tuple is a sequence of n real numbers (a 1,a 2,…,a n ). The set of all ordered n-tuple is called n-space and is denoted by. Note that an ordered n-tuple (a 1,a 2,…,a n ) can be viewed either as a “generalized point” or as a “generalized vector” 3. 1 Vectors in n-space

Definition Two vectors u = (u 1,u 2,…,u n ) and v = (v 1,v 2,…, v n ) in are called equal if u 1 = v 1,u 2 = v 2, …, u n = v n The sum u + v is defined by u + v = (u 1 +v 1, u 1 +v 1, …, u n +v n ) and if k is any scalar, the scalar multiple ku is defined by ku = (ku 1,ku 2,…,ku n ) Remarks The operations of addition and scalar multiplication in this definition are called the standard operations on.

If u = (u 1,u 2,…,u n ) is any vector in, then the negative (or additive inverse) of u is denoted by -u and is defined by -u = (-u 1,-u 2,…,-u n ). The zero vector in is denoted by 0 and is defined to be the vector 0 = (0, 0, …, 0). The difference of vectors in is defined by v – u = v + (-u) = (v 1 – u 1,v 2 – u 2,…,v n – u n )

Theorem (Properties of Vector in ) If u = (u 1,u 2,…,u n ), v = (v 1,v 2,…, v n ), and w = (w 1,w 2,…,w n ) are vectors in and k and m are scalars, then: a) u + v = v + u b) u + (v + w) = (u + v) + w c) u + 0 = 0 + u = u d) u + (-u) = 0; that is, u – u = 0 e) k(mu) = (km)u f) k(u + v) = ku + kv g) (k+m)u = ku+mu h) 1u = u

Theorem If v is a vector in, and k is a scalar, then a) 0v = 0 b) k0 = 0 c) (-1) v = - v Definition A vector w is a linear combination of the vectors v 1, v 2,…, v r if it can be expressed in the form w = k 1 v 1 + k 2 v 2 + · · · + k r v r where k 1, k 2, …, k r are scalars. These scalars are called the coefficients of the linear combination. Note that the linear combination of a single vector is just a scalar multiple of that vector.

Definition 3.2 Norm, Dot Product, and Distance in n-space Example If u = (1,3,-2,7), then in the Euclidean space R 4, the norm of u is

Definition A vector of norm 1 is called a unit vector. That is, if v is any nonzero vector in R n, then Normalizing a Vector The process of multiplying a nonzero vector by the reciprocal of its length to obtain a unit vector is called normalizing v.

Example: Find the unit vector u that has the same direction as v = (2, 2, -1). Solution: The vector v has length Thus, Definition, The standard unit vectors in R n are: e 1 = (1, 0, …, 0), e 2 = (0, 1, …, 0), …, e n = (0, 0, …, 1) In which case every vector v = (v 1,v 2, …, v n ) in R n can be expressed as v = (v 1,v 2, …, v n ) = v 1 e 1 + v 2 e 2 +…+ v n e n

The distance between the points u = (u 1,u 2,…,u n ) and v = (v 1, v 2,…,v n ) in R n defined by Example If u = (1,3,-2,7) and v = (0,7,2,2), then d(u, v) in R 4 is Distance

Dot Product Example The dot product of the vectors u = (-1,3,5,7) and v =(5,-4,7,0) in R 4 is u · v = (-1)(5) + (3)(-4) + (5)(7) + (7)(0) = 18

It is common to refer to, with the operations of addition, scalar multiplication, and the Euclidean inner product, as Euclidean n-space. Theorem and If u, v and w are vectors in and k is any scalar, then a) u · v = v · u b) u · (v+ w) = u · v + u · w c) k (u · v) = (ku) · v d) v · v ≥ 0; Further, v · v = 0 if and only if v = 0 e) 0 · v = v · 0= 0 f)(u +v) · w = u · w + v · w g) u · (v- w) = u · v - u · w h)(u -v) · w = u · w - v · w i) k (u · v) = u · (kv) Example (3u + 2v) · (4u + v) = (3u) · (4u + v) + (2v) · (4u + v ) = (3u) · (4u) + (3u) · v + (2v) · (4u) + (2v) · v =12(u · u) + 11(u · v) + 2(v · v)

Theorem (Cauchy-Schwarz Inequality in ) If u = (u 1,u 2,…,u n ) and v = (v 1, v 2,…,v n ) are vectors in, then |u · v| ≤ || u || || v || Or in terms of components Properties of Length in If u and v are vectors in and k is any scalar, then a) || u || ≥ 0 b) || u || = 0 if and only if u = 0 c) || ku || = | k ||| u || d) || u + v || ≤ || u || + || v || (Triangle inequality for vectors)

a) d(u, v) ≥ 0 b) d(u, v) = 0 if and only if u = v c) d(u, v) = d(v, u) d) d(u, v) ≤ d(u, w ) + d(w, v) (Triangle inequality for distances) Properties of Distance in If u, v, and w are vectors in and k is any scalar, then Theorem If u, v, and w are vectors in with the Euclidean inner product, then

Dot Products as Matrix Multiplication

3.3 Orthogonality Example In the Euclidean space, determine if the vectors u = (-2, 3, 1, 4) and v = (1, 2, 0, -1) are orthogonal. Solution: since u · v = (-2)(1) + (3)(2) + (1)(0) + (4)(-1) = 0, u and v are orthogonal. Example In the Euclidean space R 3, determine if the standard unit vectors i=(1, 0, 0), j=(0, 1, 0), k=(0, 0, 1) is an orthogonal set. Solution: we must show that i · j = i ·k = j ·k = 0.

Lines and Planes Determined by Points and Normals A line in R 2 is determined uniquely by its slope and one of its points, and that a plane in R 3 is determined uniquely by its “inclination” and one of its points. One way of specifying slope and inclination is to use a nonzero vector n, called normal, that is orthogonal to the line or plane in question. The point-normal equation of the line through the point P 0 (x 0, y 0 ) that has normal n=(a, b) is: a(x-x 0 )+b(y-y 0 )=0 The point-normal equation of the plane through the point P 0 (x 0, y 0, z 0 ) that has normal n=(a, b, c) is a(x-x 0 )+b(y-y 0 )+c(z-z 0 )=0 Example Find a point-normal equation of the plane through the point P(-1, 3, -2) that has normal n=(-2, 1, -1). Solution:

Theorem (a)If a and b are constants that are not both zero, then an equation of the form ax+by+c=0 represents a line in R 2 with normal n=(a, b). (b) If a, b, and c are constant that are not all zero, then an equation of the form ax+by+cz+d=0 represents a plane in R 3 with normal n=(a, b, c). Lines and Planes Determined by Points and Normals Cont. Example: Determine whether the given planes are parallel. 4x-y+2z=5 and 7x-3y+4z=8 Solution:

Orthogonal Projections In summary, (vector component of u along a) (vector component of u orthogonal to a) Theorem Projection Theorem If u and a are vectors in R n, and if a  o, then u can be expressed in exactly one way in the form u=w 1 +w 2, where w 1 is a scalar multiple of a and w 2 is orthogonal to a. Note: 1.Here the vector w 1 is called the orthogonal projection of u on a, or sometimes the vector component of u along a, denoted by proj a u, and 2.The vector w 2 is called the vector component of u orthogonal to a. Hence w 2 =u-proj a u.

Theorem (Pythagorean Theorem in R n ) If u and v are orthogonal vectors in R n with the Euclidean inner product, then Example Let u=(2, -1, 3) and a=(4, -1, 2). Find the vector component of u along a and the vector component of u orthogonal to a. Solution: