Orthonormal Bases, Gram-Schmidt Process, and QR-Decomposition in Linear Algebra, Assignments of Linear Algebra

This document from math 322, linear algebra i, covers the concepts of orthonormal bases, gram-schmidt process, and qr-decomposition in the context of inner product spaces. The motivation for using orthonormal bases, the definitions of orthogonal sets and orthonormal bases, and provides examples and theorems on coordinate representations, linear independence, and orthogonal projections. The document also discusses the gram-schmidt process and its application to qr-decomposition.

Typology: Assignments

Pre 2010

Uploaded on 08/16/2009

koofers-user-jp7-1
koofers-user-jp7-1 🇺🇸

10 documents

1 / 50

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Orthonormal Bases; Gram-Schmidt Process;
QR-Decomposition
MATH 322, Linear Algebra I
J. Robert Buchanan
Department of Mathematics
Spring 2007
J. Robert Buchanan Orthonormal Bases; Gram-Schmidt Pro cess; QR-Decomposition
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17
pf18
pf19
pf1a
pf1b
pf1c
pf1d
pf1e
pf1f
pf20
pf21
pf22
pf23
pf24
pf25
pf26
pf27
pf28
pf29
pf2a
pf2b
pf2c
pf2d
pf2e
pf2f
pf30
pf31
pf32

Partial preview of the text

Download Orthonormal Bases, Gram-Schmidt Process, and QR-Decomposition in Linear Algebra and more Assignments Linear Algebra in PDF only on Docsity!

Orthonormal Bases; Gram-Schmidt Process;

QR -Decomposition

MATH 322, Linear Algebra I

J. Robert Buchanan

Department of Mathematics

Spring 2007

Motivation

When working with an inner product space, the most convenient bases are those that (^1) consist of orthogonal vectors, and (^2) consist of vectors of length 1.

Orthogonal Sets

Definition A set of vectors in an inner product space is an orthogonal set if all the vectors are pairwise orthogonal. An orthogonal set in which each vector has norm (length) 1 is called an orthonormal set.

Example The standard basis { e 1 , e 2 ,... , e n } is an orthonormal set in R n.

Recall: if vV and v 6 = 0 then

u =

vv

has norm 1.

Orthogonal Sets

Definition A set of vectors in an inner product space is an orthogonal set if all the vectors are pairwise orthogonal. An orthogonal set in which each vector has norm (length) 1 is called an orthonormal set.

Example The standard basis { e 1 , e 2 ,... , e n } is an orthonormal set in R n.

Recall: if vV and v 6 = 0 then

u =

vv

has norm 1.

Orthonormal Basis

Definition A basis for an inner product space consisting of orthonormal vectors is called an orthonormal basis. A basis for an inner product space consisting of orthogonal vectors is called an orthogonal basis.

Theorem If B = { v 1 , v 2 ,... , v n } is an orthonormal basis for an inner product space V , and if uV , then

u = 〈 u , v 1 〉 v 1 + 〈 u , v 2 〉 v 2 + · · · + 〈 u , v nv n.

Remark: The coordinates of u relative to B are 〈 u , v 1 〉, 〈 u , v 2 〉,

... , 〈 u , v n 〉. Proof.

Orthonormal Basis

Definition A basis for an inner product space consisting of orthonormal vectors is called an orthonormal basis. A basis for an inner product space consisting of orthogonal vectors is called an orthogonal basis.

Theorem If B = { v 1 , v 2 ,... , v n } is an orthonormal basis for an inner product space V , and if uV , then

u = 〈 u , v 1 〉 v 1 + 〈 u , v 2 〉 v 2 + · · · + 〈 u , v nv n.

Remark: The coordinates of u relative to B are 〈 u , v 1 〉, 〈 u , v 2 〉,

... , 〈 u , v n 〉. Proof.

Coordinates Relative to Orthonormal Bases

Theorem If B is an orthonormal basis for an n-dimensional inner product space, and if

( u )B = ( u 1 , u 2 ,... , un ) and ( v )B = ( v 1 , v 2 ,... , vn )

then (^1) ‖ u ‖ =

u 12 + u 22 + · · · u n^2

(^2) d ( u , v ) =

( u 1 − v 1 )^2 + ( u 2 − v 2 )^2 + · · · + ( unvn )^2 (^3) 〈 u , v 〉 = u 1 v 1 + u 2 v 2 + · · · + unvn

Remark: computing norms, distances, and inner products with coordinates relative to orthonormal bases is equivalent to computing them in Euclidean coordinates.

Coordinates Relative to Orthonormal Bases

Theorem If B is an orthonormal basis for an n-dimensional inner product space, and if

( u )B = ( u 1 , u 2 ,... , un ) and ( v )B = ( v 1 , v 2 ,... , vn )

then (^1) ‖ u ‖ =

u 12 + u 22 + · · · u n^2

(^2) d ( u , v ) =

( u 1 − v 1 )^2 + ( u 2 − v 2 )^2 + · · · + ( unvn )^2 (^3) 〈 u , v 〉 = u 1 v 1 + u 2 v 2 + · · · + unvn

Remark: computing norms, distances, and inner products with coordinates relative to orthonormal bases is equivalent to computing them in Euclidean coordinates.

Linear Independence

Theorem If B = { v 1 , v 2 ,... , v n } is an orthogonal set of nonzero vectors in an inner product space, then B is linearly independent.

Proof.

Linear Independence

Theorem If B = { v 1 , v 2 ,... , v n } is an orthogonal set of nonzero vectors in an inner product space, then B is linearly independent.

Proof.

Orthogonal Projections

Question: how do you create an orthogonal basis for an arbitrary finite-dimensional inner product space?

Theorem (Projection Theorem) If W is a finite-dimensional subspace of an inner product space V , then every vector uV can expressed uniquely as

u = w 1 + w 2

where w 1 ∈ W and w 2 ∈ W.

Remark: w 1 is called the orthogonal projection of u on W. w 2 is called the component of u orthogonal to W.

Proof. Later

Orthogonal Projections

Question: how do you create an orthogonal basis for an arbitrary finite-dimensional inner product space?

Theorem (Projection Theorem) If W is a finite-dimensional subspace of an inner product space V , then every vector uV can expressed uniquely as

u = w 1 + w 2

where w 1 ∈ W and w 2 ∈ W.

Remark: w 1 is called the orthogonal projection of u on W. w 2 is called the component of u orthogonal to W.

Proof. Later

Illustration

u = w 1 + w 2 = proj W u + proj Wu Thus

proj Wu = u − proj W u u = proj W u + ( u − proj W u )

w 2

w 1

u u-projwu

projWu

u

Calculating Orthogonal Projections

Theorem Suppose W is an finite-dimensional subspace of an inner product space V. (^1) If B = { v 1 , v 2 ,... , v r } is an orthonormal basis for W and uV then

proj W u = 〈 u , v 1 〉 v 1 + 〈 u , v 2 〉 v 2 + · · · + 〈 u , v rv r.

(^2) If B′^ = { v 1 , v 2 ,... , v r } is an orthogonal basis for W and uV then

proj W u = 〈 u , v 1 〉 ‖ v 1 ‖^2

v 1 + 〈 u , v 2 〉 ‖ v 2 ‖^2

v 2 + · · · + 〈 u , v r 〉 ‖ v r ‖^2

v r.