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Lecture Notes on Vector Spaces and Linear Transformations (COMP11120)

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Master the fundamentals of vector spaces and linear transformations with these comprehensive lecture notes for COMP11120. These notes cover key topics such as vector spaces, subspaces, bases, dimension, linear transformations, matrix representations, eigenvalues, and eigenvectors. With clear explanations, illustrative examples, and essential theorems, these notes are designed to help you understand and apply complex concepts with confidence. Perfect for students enrolled in COMP11120 or anyone interested in self-study, these notes provide a structured and organized approach to learning. Benefit from expert tips, visual aids, and concise summaries to enhance your understanding and excel in your exams. Get your copy now and take your mathematical skills to the next level!

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Uploaded on
May 30, 2024
Number of pages
2
Written in
2023/2024
Type
Class notes
Professor(s)
Andrea schalk
Contains
Vector spaces and linear transformations

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Vector Spaces and Linear Transformations

Vectors
Definition A vector is
simply an ordered n-tuple of real numbers VI , Va
, ...,
Un Examples :



2
V
, Va , ...,Un are called the components or entries of .


= = R
1




ERb
-

2 4
We has dimension a c E
say X n.
O

-

1

Vi
We write : E An
Va
V
R
=
-
is the set of all n-dimensional vectors called n
: ,


Un
dimensional real space .




Vector Operations
Vector Addition Multiplication by a scalar a ER Vector Substraction

V, qV,
a
WI Vi + wi
V2 Wa & V2
( w)

Vatwa av V w =
V +
= =

t = -


+ w =
:
I
: :
in
:
Un Wn Vn + Wn XVn where -w is shorthand for 1-1) ef




Zero Vector in Ru Position Vectors in R2
A vector with n entries
equal to 0
. ↓ =
(Y) and w =
(w) as position vectors

Zero Vector
ya
O so(V , Val
8
8 =
In entries (W , Wa&
V
: q
W
8 -




E &
V X




Equality in Rh Every point (vi , va) is uniquely represented as a position vector.
Vectors are ordered tuples of numbers : (2) * (2)
Vector Let and w be victors in Rh General View of Vectors R2
Equality 1 in


Then1 =
w if
N *
y
V = Wi
, Va = Wa , ..., Un =
Wh V
-
4-




V =
Y as
free vector
3-
-vej -



2 -




------
*




i
1 - Vil =



M



= It's n

The components V, and
ve of 1 are viewed as displacements wrt .
the unit vectors i andj in the
coordinate system .




Laws for vectors in Rh

Let , V ,
we Rh L , X , we R" and a,B be any scalars (real numbers)
·
V + w =
W + V commutativity ·
x (V + w) = XV + xW distributivity
O
u + (k + w) = (u + 1) + w associativity ·
(x + B(v = xx + B

·
V + 0 =V & is the additive unit. ·
x(B1) =
(xB) mixed associativity
0 + k =
V · /k =
V multiply with 1

· + ( 1)
-
= 0 -

V is the additive inverse



(x) + V = Q Of Y · Ov =
0 multiply with scalar O

·
x0 =
0 multiply witha vector 3
·
(-Nk = (v) = x( x)
-




multiply with negatives
R136,23
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