The only vector in both W 0 Ii - University of Minnesotarylai/docs1/teaching/math4242/S...To find...

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Lecture 26: Quick review from previous lecture If W is a subspace of V with dimW = n and dimV = m, then every vector v 2 V can be uniquely decomposed into v = w + z where w 2 W and z 2 W ? . Moreover, dimV =dimW + dimW ? . coimg A = (ker A) ? and img A = (coker A) ? . The linear system Ax = b has a solution (it is compatible) , b ? coker A. The only vector in both W and W ? is zero element 0. ————————————————————————————————— Today we will discuss linear functions. - Lecture will be recorded - ————————————————————————————————— Midterm 2 will cover 2.5, Chapter 3, and 4.1 - 4.4. Details about Midterm 2 has been announced on Canvas. MATH 4242-Week 11-2 1 Spring 2020 - W - t w ' Ii . . na . .

Transcript of The only vector in both W 0 Ii - University of Minnesotarylai/docs1/teaching/math4242/S...To find...

Lecture 26: Quick review from previous lecture
• If W is a subspace of V with dimW = n and dimV = m, then every vector v 2 V can be uniquely decomposed into
v = w + z
?.
• coimgA = (kerA)? and imgA = (cokerA)?.
• The linear system Ax = b has a solution (it is compatible) , b ? cokerA.
• The only vector in both W and W ? is zero element 0.
————————————————————————————————— Today we will discuss linear functions.
- Lecture will be recorded -
————————————————————————————————— Midterm 2 will cover 2.5, Chapter 3, and 4.1 - 4.4. Details about Midterm 2 has been announced on Canvas.
MATH 4242-Week 11-2 1 Spring 2020
-
Ii .
.na..
Fact:
(1) Let A be any real m n matrix. Any vector b in imgA has “exactly one” vector from coimgA mapping from it.
(2) Moreover, if {v1, · · · ,vr} is a basis of coimgA, then
{Av1, · · · , Avr} is a basis of imgA.
[To see this:]
Thus, we also have
Fact: A compatible linear system Ax = b with b 2 imgA has a unique solution x 2 coimgA satisfying Ax = b.
The general solution is x = x+z, where x 2 coimgA and z 2 kerA. Then x has the smallest norm of all the solutions to Ax = b.
MATH 4242-Week 11-2 2 Spring 2020
IR " A- IRM
So we can find v e IR "
so that =
Av = b .
(wing A) ' -
= Ker A .
Av = b .
b = Ax , where × E co ing A .
( Unique ) : suppose Ax , = Axz = b, X . . xz EwingA A (X , - Xz) = O .
lx , -ta) E KerA
To × . -x. c- Kera /
:
11×11 I 11×91 . #
To find the solution of minimum Euclidean norm, that is, x:
1. Using Gaussian Elimination to find the general solution x to the system Ax = b.
2. Finding the basis v1, · · · , v` for kerA, and then using the conditions vT j x = 0.
Example. Find the solution of minimum Euclidean norm x of the linear system Ax = b, where
A =
0
1
A .
MATH 4242-Week 11-2 3 Spring 2020
I . Find general solutions for Ax = b
.
Ker A = span ( ( It) ) .
Chapter 7 Linearity
7.1 Linear Functions
Definition: [Linear operators] If L : V ! W is a mapping between vector spaces V and W , we say that L is linear if for all vectors x and y in V , and scalars c such that
L[cx] = cL[x]
L[x + y] = L[x] + L[y].
We call such a mapping L a linear operator. We call V the domain for L, and W the codomain.
We may also say L is a linear function, or a linear map (or mapping), or a linear transformation. They all refer to the same properties.
Properties:
• For any scalars c and d and any vectors x and y in V ,
L[cx + dy] = cL[x] + dL[y]
• For any scalars c1, · · · , cn and any vectors x1, · · · ,xn in V , then
L[c1x1 + · · · + cnxn] = c1L[x1] + · · · + cnL[xn].
• L[0] = 0 (the 0 on the left is the zero element in V ; the 0 on the right is the zero element in W ).
MATH 4242-Week 11-2 5 Spring 2020
an
1-To see +4,3 j L Ext y ] = LEXI + L[y ] .
x = O , y = O
"
-
V
Example.
1. Let C0([a, b]) be the vector space of continuous functions on the interval [a, b]. Define the operator L by
L[f ](x) =
f (t)dt.
In other words, we have defined L[f ] to be a function, that is, the integral of f .
2. Now define the operator L : C1([a, b]) ! C 0([a, b]) by
L[f ](x) = d
dx f (x) = f
0(x),
where f is in C 1([a, b]), the space of di↵erentiable functions on [a, b].
MATH 4242-Week 11-2 6 Spring 2020
check L is Linear :
.
Cx k Cf're) = CLAIM .Is constant
Lfftg) Cx) = (ftg) '
ex, = f-Exit gtx) = Lct) +4.97 .#
Q: What are the linear operators L : R ! R? Suppose L is any linear operator L : R ! R. Then L[cx] = cL[x] for any
numbers c and x (we think of c as a scalar and x as a vector, but since x is in R they’re both just numbers).
Warning: The function f (x) = ax+ b is not a linear function unless b = 0, even though its graph is also a line; this is because f (0) = b, so it doesn’t pass through the origin (unless b = 0)
Example. We can think of A (m n matrix) as defining a mapping L from Rn
.
The mapping L is linear (that is, a linear mapping from Rn to Rm).
MATH 4242-Week 11-2 7 Spring 2020
- F - -
LEX] = LEE ! ] = x Lal .
# 41×1 matrix ?
lines passing through the origins. (Llxtax) #
-
Lcvtw) = LENI LEW] . #
Q: Are there any other linear mappings from Rn to Rm? That is, can there be a linear mapping not of the above form, for some matrix A?
Fact 1: Every linear mapping L from Rn to Rm is given by matrix multiplica- tion, L[v] = Av, where A is an m n matrix.
[To see this:]
Let ei , . . ., en be the standard basis the IR"
et , - - - , ein 4 for RM .
For j -- I. . . ., n ,
.
= V, er t .-- -+Viren
= r , a-
= A (I:/ = Air . #