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Title: Linear Algebra - Orthogonal Bases (Part 1)
Description: These notes cover the first part of Orthogonal Bases

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Orthogonality for Subspaces and Bases
Recall that x ⊥ y if and only if x · y = 0, so it’s just a dot product based definition
...

Definition: The sets P ∈ Rn and Q ∈ Rn are orthogonal if
p · q for all p ∈ P and all q ∈ Q,
so all of P is orthogonal to all of Q (vice-versa, etc)
...
The subspaces U and W of V are U ⊥ W if all
u ∈ U and all w ∈ W have u · w = 0
...
The spans of




−1
0
1
those sets will also be orthogonal to each other
...

Property: The orthogonal complement of a subspace is also a subspace
...

• 0 ∈ V has 0 · u for all u ∈ U , so it’s in U ⊥
...


(x + y) · u = x · u + y · u = 0 + 0 = 0

for any u ∈ U
...

• Take x ∈ U ⊥ and a ∈ R
...

all three conditions hold, it’s a subspace
...

Property: The intersection between U and U ⊥ , U



U ⊥ is just the zero vector
...

Example: In R3 , here we have two subspaces:
 

 x

U =  y  | x − 2y − 3z = 0


z
1

  

1


V = a 1  , a ∈ R ,


2

What are their complements?
For  , it’ll the set of all vectors in R3 orthogonal to the plane itself, so the subspace
be
U
1 

Span  −2 
...

In R3 , the orthogonal complement of a line is a plane, the complement of a plane is a line
...
If you want an orthogonal complement of the span of two vectors,
you’d want the span of a set of vectors orthogonal to those two
...
I
...

Property: If U = Span {u1 , u2 ,
...

Corollary: If U = Span {u1 , u2 ,
...

then
U ⊥ = {x ∈ Rn such that Ax = 0}
...


...


1



−1
Example: If U = Span 
 −2


3

Row(A)⊥ = Null(A), and (using a bunch of transposes)



−1
−1
 3  2


 0  1
−2
−2


1 

  0 



  −3  then find a basis for U
...
Doing so makes the
orthogonal complement equal to the null space of the matrix
...


2

How To Solve for All At Once,

OPTIONAL

The annoyance of the previous section is that our usual reduction of A yields a basis of
the row space, column space (taking the original vectors in the pivot columns) and, with
some effort, the null space
...
We’re missing the complement of the
column space
...
Take your matrix A and put it into an augmented matrix of the form [A|I] with I the
identity matrix with the same height
...
Row reduce the A side until in RREF
...

3
...

(b) The basis of Col(A) will be the original A columns corresponding to the pivot
columns
...

(d) The basis of Null(AT ), of Col(A)⊥ , will be the row vectors on the right corresponding to zero rows on the left
...

1 −1/2 0 0 0 1
0 0 0
1 −1 1
There are several ways to analyze this algorithm
...
The justification for the right hand side is that we are actually solving it for an arbitrary
right hand side, with each column on the RHS representing a different coefficient of the b
vector
...

1
−1/2
0
0
0
1
b3
Once row reduced on the left, each zero row represents a row that COULD cause a contradiction
...
So,
the column space of A is the orthogonal complement to that one vector, so


⊥

1 
1 


Col(A) = Span  −1 
=⇒ Col(A)⊥ = Span  −1 




1
1
using the (U ⊥ )⊥ = U equality
...

  
 1
Example: The set  0  

0

is orthogonal if every pair of different vectors in the set is
     
  
0
0 
0
0 
 1
  0  is orthogonal but  0   1   1  is not
...

Proof: This is surprisingly easy
...
, vn }
...

What do we do? We inner product v1 on each side for
a1 v1 · v1 + a2 v2 · v1 + · · · + an vn · v1 = 0 · v1
which works out to be
a 1 v1 · v1 = 0
which makes a1 = 0 since v1 ̸= 0 which makes v1 · v1 ̸= 0
...
A set of n non-zero orthogonal vectors is automatically a basis of Rn , of course
...
Note too that the basic unit vectors of Rn form an orthogonal basis
...
Recall that when x ∈ Span of the
basis {v1 , v2 ,
...

Having the v form an orthogonal basis makes this even easier
...
We start with the above equation and use v1 (as before) for
x · v1 = a1 v1 · v1 + a2 v2 · v1 + · · · + an vn · v1
= a1 v1 · v1
x·v
so a1 = v1 ·v11
...
We can get
this for ANY of the vectors and coefficients:
x · vi
i ∈ 1
...

ai =
vi · vi

which works out to
x = Projv1 (x) + Projv2 (x) + · · · + Projvn (x)
...

1
0
2
1
4

They’re orthogonal, and so linearly independent, so they span R2
...

0
−1
2
1
The helpful thing here is that we can actually expand this into projections, projections
on to subspaces (U ) and orthogonal complements (U ⊥ )
...


with x1 · x2 = 0, and so on
...
, vm } then
ProjV (x) = Projv1 (x) + Projv2 (x) + · · · + Projvm (x)
...
Recall the section about projections
...
We use the same
principle
...

Recall that V is spanned by the v vectors
...
So:
(
)
Projv1 (x) + Projv2 (x) + · · · + Projvm (x) − x · vi
= Projvi (x) · vi − x · vi
(
)
vi · x
vi · vi − x · vi
=
vi · vi
vi · x
vi · vi − x · vi
=
vi · vi
= x · vi − x · vi = 0
and done
...
5: 2
...
b), 6
...

Section 4
...
df),2, 9
Title: Linear Algebra - Orthogonal Bases (Part 1)
Description: These notes cover the first part of Orthogonal Bases