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Chapter 3 - 4 = Euclidean & General Chapter 3 - 4 = Euclidean & General

Chapter 3 - 4 = Euclidean & General - PowerPoint Presentation

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Chapter 3 - 4 = Euclidean & General - PPT Presentation

Vector Spaces MATH 264 Linear Algebra Introduction There are two types of physical quantities Scalars quantities that can be described by numerical value alone Ex temperature length speed ID: 655137

linear vector vectors space vector linear space vectors section properties theorem coordinate combination set textbook slide direction continued problems scalar matrices subspace

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Slide1

Chapter 3 - 4 =Euclidean & GeneralVector Spaces

MATH

264 Linear

AlgebraSlide2

IntroductionThere are two types of physical quantities:Scalars = quantities that can be described by numerical value alone (Ex: temperature, length, speed)Vectors = quantities that require both a numerical value and direction (Ex: velocity, force,…)Linear Algebra is concerned with 2 types of mathematical objects, matrices and vectors. In this section we will reciew the basic properties of vectors in 2D and 3D with the goal of extending these properties in

 Slide3

 

Continued on Next Slide

Slide4

Vectors in 2-space, 3-space, and n-spaceSection 3.1 in TextbookSlide5

DefinitionsVectors with the same length and direction are said to be equivalent.The vector whose initial and terminal points coincide has length zero so we call this the zero vector and denote it as 0. The zero vector has no natural direction therefore we can assign any direction that is convenient to us for the problem at hand.Slide6

The solutions to a system of linear equations in n variables are n x 1 column matrices, the entries representing values for each of the n variables. We call the set of all n x 1 column matrices n-space and denote it by Sometimes we write an element of n-space as a sequence of real numbers

called an

ordered n-tuple.

 

 Slide7

is an example of a vector space

and we often refer to its elements as

vectors

. A vector space is a non-empty set V with 2 operations (addition & scalar multiplication) which have the properties for any

u

,

v

,

w

,

in

V

and any real numbers

k

and m: Slide8
Slide9
Slide10

SubspacesSection 4.2 in TextbookSlide11

Intro to SubspacesIt is often the case that some vector space of interest is contained within a larger vector space whose properties are known. In this section we will show how to recognize when this is the case, we will explain how the properties of the larger vector space can be used to obtain properties of the smaller vector space, and we will give a variety of important examples.Slide12

Definition:A subset W of vector space V is called a subspace of V if W is itself a vector space under the addition and scalar multiplication defined on V.Slide13
Slide14

Theorem 4.2.1If W is a set of one or more vectors in a vector space V then W is a subspace of V if and only if the following conditions are true:If u and v are vectors in W then u+v is in

W

If

k is a scalar and u

is a vector in

W

then

ku

is in

W

This theorem states that

W

is a subspace of

V

if and only if it’s closed under addition and scalar multiplication.Slide15
Slide16
Slide17
Slide18

Theorem 4.2.2:Definition:Slide19

Theorem 4.2.3:Slide20
Slide21

Example:Slide22

Linear IndependenceSection 4.3 in TextbookSlide23

Intro to Linear IndependenceIn this section we will consider the question of whether the vectors in a given set are interrelated in the sense that one or more of them can be expressed as a linear combination of others. In a rectangular xy-coordinate system every vector in the plane can be expressed in exactly one way as a linear combination of the standard unit vectors.Ex: express vector (3,2) as linear combination of

and

is:

 Slide24
Slide25

Theorem:Note: span – a set of all linear combinationsFor vectors

in

the following statements are equivalent:

Any vector in the span of

can be written uniquely as a linear combination

If then

None of the vectors

is a linear combination of the others.

 Slide26
Slide27

Example:Continued on Next Slide Slide28
Slide29
Slide30

Example:Slide31

Example: Linear Independence in  

Continued on Next Slide

Slide32

Continued on Next Slide Slide33
Slide34

Example: Linear Independence in  Slide35

Coordinates & BasisSection 4.4 in TextbookSlide36

Intro to Section 4.4We usually think of a line as being one-dimensional, a plane as two-dimensional, and the space around us as three-dimensional. It is the primary goal of this section and the next to make this intuitive notion of dimension precise.

In

this section we will discuss

coordinate systems in general vector spaces and lay the groundwork for a precise definition of dimension

in the next section.Slide37
Slide38

In linear algebra coordinate systems are commonly specified using vectors rather than coordinate axes. See example below:Slide39

Units of MeasurementThey are essential ingredients of any coordinate system. In geometry problems one tries to use the same unit of measurement on all axes to avoid distorting the shapes of figures. This is less important in applicationSlide40
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Slide43
Slide44
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Slide47
Slide48

Questions to Get DoneSuggested practice problems (11th edition) Section 3.1 #1, 3, 5, 7, 9, 11, 13, 15, 17, 19, 21, 23Section 3.2 #1, 3, 5, 7, 9, 11Section 3.3 #1, 13, 15, 17, 19Section 3.4 #17, 19, 25Slide49

Questions to Get DoneSuggested practice problems (11th edition) Section 4.2 #1, 7, 11Section 4.3 #3, 9, 11Section 4.4 #1, 7, 11, 13Section 4.5 #1, 3, 5, 13, 15, 17, 19Section 4.7 #1-19 (only odd)Section 4.8 #1, 3, 5, 7, 9, 15, 19, 21Slide50

Questions to Get DoneSuggested practice problems (11th edition) Section 6.2 #1, 7, 25, 27