#linear-algebra

2 messages · Page 309 of 1

stuck tendon
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Not sure what you mean ;o
u is in the kernel, since Pu = Iu - u(u^tu)=u-u=0, since u is a unit vector

zinc timber
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null space of T- λ I

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not null space of T

wintry steppe
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So how exactly do i show the nullity here?

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It's a previous years exam

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I have the answer, so I know it's 1

zinc timber
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show null space is span{u}

stuck tendon
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^, by showing that u is in ker(P), and knowing that ker(P) is a subspace, we have span{u} is contained in ker P. Now show the reverse containment

wintry steppe
#

It's the same as the solution lol

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I'll keep thinking :)

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Thank you for your help 🙏

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Ahhhhhhhh

zinc timber
wintry steppe
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This matrix is projecting to the Orthogonal space

zinc timber
#

yess

wintry steppe
#

So then kern p = Span u

zinc timber
#

yes

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but try to argue that

outer goblet
#

If were trying to find a equilibrium vector E for a 2x2 matrix A for a markov chain, we can solve the equation EA=E

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just set E=(a, 1-a)

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but what would E be if A was a 3x3 matrix? or higher ?

zinc timber
#

eigen vector corresponding to ev 1

outer goblet
#

yeah but wouldnt solving it as en equation be easier?

zinc timber
#

you will get an equation

outer goblet
#

finding eigenvectors for matricies with so many decimals is pain when i dont have a calculator to solve for eigenvectors

zinc timber
#

don't have any other method

outer goblet
#

:(

cursive ginkgo
#

hi, i have A a n* n matrix so that : A^2(A − I𝑛)^2 = 0 (I𝑛 the n*n matrix with 1 on the diagonal)
knowing that (A − I𝑛)^2 ≠ 0 and A(A − I𝑛) ≠ 0.

I'm looking for the specter of A, I know that spec A ⊆ {0,1} but i don't know what to say else

pliant kayak
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you mean the spectrum right?(It‘s just so that I can help you, not tryna correct)

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I think you can follow, that A^2 has to be the 0-Matrix

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But because A(a-In)!=0 is A!= 0

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So I‘d say that A is nilpotent

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Do you know what the spectrum is?

wet stratus
#

are you sure that A^2 has to be the 0 matrix?

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unless I'm making a mistake we could for example have
A=
(1,1,0;
0,1,1;
0,0,1)
edit: I think I made a mistake here

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or we can have
A =
(1,1,0;
0,1,0;
0,0,0)

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so edit: ~~both spec A = {1} and ~~ spec A = {0,1} are possible

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A={0} clearly not as then A is the 0 matrix

pliant kayak
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I said that, because this (A^2(A − I𝑛)^2 = 0) has to hold right?

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But still I'm not sure

wet stratus
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yes but this doesn't mean that A^2 has to be 0

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if 0 is not in spec A, then A is invertible and therefore from A^2(A-I_n)^2 we get (A-I_n)^2=0 which is a contradiction

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so yeah spec A = {0,1} is the only possible option

bleak elm
#

What are some good resources for learn linear algebra ?

dreamy iron
#

I am once again asking this playlist be pinned.

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On a different note, Im looking like five practice problems proving such-n-such is a inner product, ranging in difficulty from easy to medium .

wintry steppe
#

proving something is an inner product
medium

wintry steppe
#

do you know of any more advanced linear algebra playlists? which cover topics like quotient spaces, dual spaces, tensor product, annihilators

zinc timber
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I can't understand the image

ripe shale
#

For A a square invertible matrix, we have Ax ≤ b, then does x ≤ A^(-1) b?

dusky epoch
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what's your definition of ≤?

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elementwise?

ripe shale
dusky epoch
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then no

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take A = -I

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-x ≤ b is not the same as x ≤ -b

ripe shale
#

So do you flip the sign?

dusky epoch
#

well in this particular case yes but in general Ax ≤ b does not imply any relation between x and A^-1 b

ripe shale
#

What if A is a positive matrix

dusky epoch
#

hm

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not so sure

wet stratus
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I know that we looked at M-matrices in numerical analysis for PDEs which have some properties which look similar to this. so I would assume that just being positive is not enough

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some other key words were inverse monotone and inverse positive matrices

woven zephyr
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well, in general the answer is going to be no

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take any invertible A with positive entries and at least one negative entry in its inverse

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then take x to be zero

ripe shale
woven zephyr
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right, your A has all positive entries

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are you assuming the inverse also has all positive entries?

ripe shale
woven zephyr
#

anyway, from here it's simple, you can just pick b to be zero everywhere and one in a specific entry so that A^{-1}b has a negative entry, leading to a counterexample

woven zephyr
#

then you can just do the same construction but add a very very small epsilon to each entry of b

#

and you still get a counterexample, although writing the proof is more of a pain

ripe shale
#

Here's another question, is there any other positive orthogonal matrix besides the identity?

woven zephyr
#

yes

ripe shale
#

My thought is no because the determinant would be greater than 1

ripe shale
#

Wait

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Permutation Matrix

woven zephyr
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oui

ripe shale
#

how about a positive orthogonal matrix with all entries non-zero

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Now I'm pretty sure it's no

woven zephyr
#

no, and you just need to look at the definition for why

ripe shale
stoic pythonBOT
#

meitar5674

subtle gust
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Y'all

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If a set of n vectors does not form a basis for R^n

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Does that mean that those n vectors do not span R^n OR those n vectors are linearly dependent

native rampart
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Both

subtle gust
#

I understand that a set of 3 vectors forms a basis for R^n if either of the conditions is true

wet stratus
#

3 or n?

subtle gust
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N*

native rampart
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They don't span R^n because the set is linearly dependent

subtle gust
#

Ah i see

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There's just smthng that i'm failing to understand

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Evertime it's explained to me i just don't get it

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When we test a set of vectors for spanning

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Why is it enough to show that the det of the matrix whose columns are those vectors is zero

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To prove that this set does not span R^n

native rampart
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Well the det=0 implies the matrix is not invertible

subtle gust
#

True

native rampart
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Which is same as saying linear dependence of columns

subtle gust
#

Oh i see

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What if we have 4 vectors tho

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And we're checking spanning for R^3

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The set could be lin dependent and spans R^3

native rampart
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Well you remove the redundant vector first

subtle gust
#

We wouldn't know tho

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Like if the det is zero

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Then yeah sure the set is lin dep

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But it may still be spanning R^3

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So why do we conclude that it doesn't span R^3 if the det is 0?

native rampart
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Well you don't do it like that

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The test is always with n vectors in R^n

subtle gust
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Not on my final exams tho 😭

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Oh hol on 💀

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I just realised

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That a matrix with 4 vector columns

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Would have no det

native rampart
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Yes

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It's not even square

subtle gust
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What a dumbass i am

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Sorry 💀

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Yeah got it now

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So if the det is zero (assuming the matrix is square)

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The column vectors are lin dep

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And there would be absolutely no way they span R^n

wet stratus
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yes

subtle gust
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Gr8

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Tysmmmm @native rampart and @wet stratus

wet stratus
#

the problem with testing using the det is that it doesn't tell us how linearly dependent the columns are. they could still either span a space of dimension n-1 or they could span a space of dimension 1. either way the det is 0. also calculating the det for huge n takes ages

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you could instead also do something like row reducing

native rampart
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Actually

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Efficient det algorithm is literally as fast as row reduction

wet stratus
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yes sorry I worded it badly

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row reducing also takes ages but it at least tells you more than just calculating the det

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and can be done even ifthe matrix is not square

vestal magnet
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Hey, all, how is everyone? I need to prove this:

$dimImT^* = dimImT$ as well as this $dimkerT^* = dimkerT + dimW − dimV$
Can't I just say that $dim(Im(T^)) = dim(Im(T)) dim(F) = dim(Im(T))$ and then use the fact that
dimImT + dimKerT = dimV?

stoic pythonBOT
#

meitar5674

native rampart
#

Why do you think you can claim that @vestal magnet ?
T is a map from V to W while T* is a map from W* to V*

delicate crow
#

Not sure if this is the right place to ask im working on a question and i end up with this expression and I’m wondering if this simplifies into an expression or not

dusky epoch
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isnt this (1 + z/n)^n

delicate crow
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Oh right

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Idk how I didn’t see that

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Ty hahaha

robust owl
#

How do Insel/Spence, Hoffman/Kunze and Axler compare?

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I'm taking a second course in LA next semester. So, I emailed my prof asking for a book to work through over the summer, he recommended Insel/Spence or Dummit/Foote (which seemed odd), but he also said he heard Axler was good.

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I bought a copy of Insel/Spence and it looks way thicker and more detailed than Axler.

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The prereq for this course is our first semester abstract algebra course, which basically covers all of the groups chapters of Fraleigh.

wintry steppe
#

they cover basically the same material with different points of view

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axler restricts to real and complex fields, and avoids determinantal arguments

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axler's view of stuff like the characteristic polynomial is pretty strange, since he avoids determinants

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the treatment in FIS is much easier to use

robust owl
#

Are they comparable in terms of depth? Like, is one more elementary than the other or are they both roughly the same?

wintry steppe
#

pretty much the same

robust owl
#

Do you have a personal preference for any particular book at this level?

wintry steppe
#

FIS

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i don't agree with axler's treatment of determinants and related stuff

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it makes sense to try not to use them if you're going to do stuff like functional analysis (which axler does), but for introductory linear algebra it does not matter

robust owl
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I see I see. I'll probably give FIS a shot. Thanks for the advice!

past barn
#

Would you guys recommend Serge Lang's Linear Algebra book for a first timer?

zinc timber
#

I wouldn't, at least

wintry steppe
inner wave
outer goblet
#

can someone explain to me what the anwser is for b

inner wave
#

Could someone explain the jump between the first system of equations to T(\alpha, \beta, 0, \gamma, \phi - \gamma)?

outer goblet
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it says find A_0

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what does [L_A]_B mean

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is it just A multiplied by the matrix vector made of B basis

inner wave
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and L_A is just the linear transformation of A?

outer goblet
#

yeah

inner wave
#

from R3 to R3?

outer goblet
#

yeah given by that matrix

inner wave
#

Never seen that notation before

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Could you give a full translation of b

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Maybe I could figure it out then

inner wave
outer goblet
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the rest of the text says just to show that A_0 is invertible, unrelated to acutally finding it

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Let L_A: R^3 -> R^3 be given by L_A(x) = Ax

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find [L_A]_B

inner wave
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Isn't that just a do-nothing transformation?

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Since A and L_A are the same thing?

outer goblet
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yes but _B is supposed ot mean A in beta coordiante system

inner wave
#

Oh this is change of basis stuff

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Yeah not me man sorry

outer goblet
#

haha its ok

inner wave
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Good luck

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anyway you could help me with my problem?

outer goblet
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i wish i could :(

inner wave
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Check the picture, sorry for the lack of clarity. It's the transformation of the vector of size 5, right in the middle of screenshot

wintry steppe
#

i know it's a transformation, i want to know its definition

inner wave
#

Oh my bad one second

wintry steppe
#

/where

inner wave
#

That's MathJax let me convert it

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Old MathJax too, its from the website

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This is scuffed ima screenshot

inner wave
#

Very top

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Sorry I'm running on fumes today

wintry steppe
#

the line with T(\alpha, \beta, 0, \gamma, \delta - \gamma) is just them checking that the solution to the system of equations is indeed a solution

inner wave
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But this question is about proving the surjectivity of the transformation.

wintry steppe
#

ok

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that's what they're doing

inner wave
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Yes

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How did they determine that is a possible solution out of the set of infinite possible solutions

wintry steppe
#

it's impossible to know exactly how they landed on that solution

inner wave
#

Okay second question

wintry steppe
#

just looking at it, you already know what a must be, and c shows up a few times, so killing c by setting c = 0 simplifies things a bit

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i guess that was their thought process

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alternatively, you could write that system of equations in terms of matrices and do all the row reduction nonsense

inner wave
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is the transformation surjective because the coefficient matrix of the system of equations above that line with the transformation of alpha, beta, etc. has an infinite amount of solutions?

wintry steppe
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having just one solution is enough for surjectivity

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but yes

inner wave
#

This just seems unintuitive

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Thanks for your help

outer goblet
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for markov chains

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if a matrix is regular, it has an eigenvalue = 1

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but can markov chain matrix have an eigenvalue of 1, and not be regular?

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just checking if eigenvalue 1 is an eigenvalue of the matrix enough to determine if its regular

slow wind
#

Yes that is called the contrapositive

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In logic whenever one proposition P implies another thing, Q, then the falsity of Q implies the falsity of P

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Wait sorry I misread your question

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If it's missing an eigenvalue of 1 then it isn't regular

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but imagine a diagonal matrix with one 1, and the rest of the numbers on the diagonal 100

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it wouldn't be regular, but it would have an eigenvalue of 1

little crater
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"If A is an m × n matrix whose columns do not span R^m, then the equation A**x **= b is consistent for
some b in R^m"

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I know this is true but I was wondering if it is good enough to say "let b = zero vector"

fringe fjord
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It's a strange claim because the conclusion seems to be trivially true (as you notice) independently of the "columns do not span" assumption.

little crater
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I am not sure how to start this problem

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I believe it has some connection with

little crater
#

<@&286206848099549185>

late heart
#

A linear endomorphism with kernel 0 is an automorphism right?

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i.e. f : V to V, V a vector space

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I think it just follows by rank-nullity + dimension counting

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just want to make sure I'm not being stupid

robust pond
#

Ax=3au_1 +2Au_2

little crater
robust pond
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this gives x=3u1+2u2 as a solution

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yea

wintry steppe
robust pond
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so theres a solution

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thats sufficient right

wintry steppe
#

i.e. (x_1, x_2, ...) \mapsto (0, x_1, x_2, \dots). this has kernel zero, but is not surjective

little crater
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Ax = A(3u_1+2u_2) = A(3u_1) + A(2u_2) = 3(Au_1)+2(Au_2) = 3y_1 + 2y_2 = b

robust pond
#

i dont get what youre showing here

little crater
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I said

robust pond
#

okay

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so you found a solution but

little crater
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let x = 3u_1+2u_2

robust pond
#

idk i guess im saying

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it seems like youre done

little crater
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yeah

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I just didn't know if I did it right

robust pond
#

oh

little crater
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I just applied

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and seemed okay so I guess im done catThink

molten ivy
#

How do I go about finding a unitary matrix P, such that PAP^-1 is diagonal for a given complex matrix A? Simply diagonalising the matrix doesn't yield a unitary P._.

wintry steppe
#

Anyone able to explain this last step?

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I wanna replicate this, but I want to know how how this part under the square roots formulated

limber sierra
#

$(d_2 - d_3)^2 = d_2^2 + d_3^2 - 2d_2d_3 = d_2^2 + d_3^2 + (2d_2d_3 - 2d_2d_3) - 2d_2d_3$

stoic pythonBOT
#

Namington

limber sierra
#

$=(d_2^2 + d_3^2 + 2d_2d_3) - 4d_2d_3 = (d_2 + d_3)^2 - 4d_2d_3$

stoic pythonBOT
#

Namington

limber sierra
#

so $(d_2-d_3)^2 = (d_2+d_3)^2 - 4d_2d_3$

stoic pythonBOT
#

Namington

limber sierra
#

take the square root of both sides.

#

as for why they did this: they wanted to express $d_2 - d_3$ in terms of only $d_2 + d_3$ and $d_2d_3$, since those were computed earlier in the question

stoic pythonBOT
#

Namington

limber sierra
#

squaring something is a common way to make it positive, so to go from $d_2 - d_3$ to something involving $d_2 + d_3$, considering $(d_2 - d_3)^2$ is a natural first attempt

stoic pythonBOT
#

Namington

limber sierra
#

and it turns out that, with some algebra, it works out.

wintry steppe
#

Tyty

tranquil steeple
# wintry steppe

Fun fact, that matrix A is diagonalized by DST-2 and eigenvalues are given by f(t)=4+2cos(t)+4*cos(2*t) tj=jpi/3 j=1,2,3

wet stratus
molten ivy
#

Well then it is one

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The task is to find this unitary P so it has to exist

stuck tendon
subtle gust
#

just a quick question y'all

#

any linear transformation is expressible as a matrix transformation times a vector right?

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and the null space of that matrix transformation is the kernel of the transformation

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and the column space of this matrix is the range

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right?

wet stratus
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are we assuming that the vector space is finite dimensional?

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then ignoring that in general we only have isomorphic spaces etc, yes

wintry steppe
sacred palm
#

Hey anyone good with matrices here

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just a curious question

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how can one decide if the matrix is a point line, plane r3 or r4?

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looking at the rows?

quartz compass
#

a matrix on its own is just a rectangle full of numbers, so it's not really any of those unless you have some corresponding way of turning it into one

sacred palm
#

When they ask which one does it span

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Thats actually the question I think

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Does the matrix span point line plane r3 or r4

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Im trying to find a question but cannot find one

quartz compass
#

you can look at the span of the rows or columns, but I guess usually people look at the column vectors

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probably better to post a screenshot of the actual question being asked

sacred palm
#

Okay i will post it here

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?

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Or in a ticket

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And @ you?

outer hazel
#

2 -3 6 | 0
9 -5 4 | 0
0 0 0 | 0
does it mean it has infinitely many solutions. is it always the case for when all elements in a row are 0s?

halcyon spindle
#

Yes it has infinitely many solutions but it is not always the case when we have a zero row.
Consider an mxn matrix A where m > n. If the row reduced echelon matrix of A has n nonzero rows the m-n rows are zero. Therefore the homogenous system Ax = 0 will only have the trivial solution, so not infinity many solution. But if A is nxn matrix then yes a zero row corresponds to an infinitely many solutions for Ax = 0.

normal loom
#

are the eigenvectors the same
.5 1
1 2

solar drum
#

could someone remind me what this group represents? Here F is a field and p is some prime

wintry steppe
#

Everyone, thank you. Got a def b on my exam.

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Tyty for your help

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My friends are so sad rn, but I'm good!!!

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Ty!!!

fair wren
solar drum
#

thanks

fringe fjord
#

More precisely F_p is the unique field with p elements (which is indeed also the ring of integers modulo p). Note the the F is a fixed part of the notations, not the name of some different field that already exists.

rain harness
#

Hello. I think this is the right channel. I'm trying to a problem for a game called starbase which has in-game coding

I've been trying to solve a problem that masks you to imagine an aircraft flying. The aircraft (P) has the ability to pitch, yaw and roll about it's own axis. and measure it's current orientation. On the bottom of the aircraft is a laser that gives the exact distance of the laser to the ground representing the vector R. My question is asking whether it would be possible to find the vertical distance (D in the diagram) to the ground no matter the orientation to the plane assuming that Q is at (0,0,0) and is the point where the line / laser contact the ground. and P is at (x,y,z). It can also be assumed that the magnitude of R is known.
any assistance in solving the question or any pointers on how to solve and find a general solution it really be appreciated 😄

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If just the pitch and roll parts of the question are considered it's relatively easy to solve using cosin unit vectors but the Yaw aspect is what i'm completely stuck on

errant palm
#

hi, i don't get why the basis for the row space and column space are what they are.

quartz palm
#

can someone help me get this system of equations into reduced row echelon form?
5x - 3y - 6z = -4
3x - y - 5z = 5
4x - 2y - z = -13

halcyon spindle
#

You have to first row reduced the coefficient matrix.
For A be the row reduced matrix of that system,

  1. The first entry of the nonzero rows of A has to be 1.
  2. For the column that corresponds to the first zero entry for each nonzero rows has every other entry for that column equal to 0.

Now for A to be in row reduced echelon form

  1. Every zero rows is below all nonzero rows.
  2. The column index that corresponds to first nonzero entry in each row has to be increasing from top to bottom.
#

While you do this you need to apply the same operation to the matrix (-4, 5, -13)^T.

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Note if A is row reduced, you can easily get it to row-reduced echelon form by doing row exchanges.

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Heres an example of a row reduced matrix.
$$\begin{bmatrix} 0 & 1 & 0 \ 1 & 0 & 0 \ 0 & 0 & 1 \end{bmatrix}$$.

stoic pythonBOT
#

Plegasus

halcyon spindle
#

You can do a row with row 1 and 2 to get it to row reduced echelon matrix.

#

@quartz palm

quartz palm
#

ah thanks

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i am having trouble getting to that format

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can u walk me thru it

halcyon spindle
#

Ok let work through it together.

quartz palm
#

ok

halcyon spindle
#

Your system Ax = b can be matrix by augmented matrix
$$\begin{bmatrix} 5 & -3 & -6 & -4 \ 3 & -1 & -5 & 5 \ 4 & -2 & -1 & -13 \end{bmatrix}$$.

stoic pythonBOT
#

Plegasus

wintry steppe
#

Whats recommended to take first, this class or calc3, both have calc 2 as a prereq?

quartz palm
#

but i heard calc 3 is easier than linalg

halcyon spindle
quartz palm
halcyon spindle
#

yep.

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Then what?

quartz palm
#

multiply the 2nd row by 1/3

errant palm
#

😔

halcyon spindle
#

Yep, but that is going to take so long. Let try to get all the entries except for the 1 in the first column to 0.

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So we went from $$\begin{bmatrix} 5 & -3 & -6 & -4 \ 3 & -1 & -5 & 5 \ 4 & -2 & -1 & -13 \end{bmatrix}$$ to $$\begin{bmatrix} 1 & -\frac{3}{5} & -\frac{6}{5} & -\frac{4}{5} \ 3 & -1 & -5 & 5 \ 4 & -2 & -1 & -13 \end{bmatrix}$$.

stoic pythonBOT
#

Plegasus

quartz palm
#

hmm

halcyon spindle
#

Now you try to get all the entry in the first colum except for the 1 to 0 by adding to row 2 and 3 by multiplies of row 1.

#

With that done you can move on to the second row.

quartz palm
#

idk

halcyon spindle
#

Are you working this out on paper?

quartz palm
#

not rn

#

too tired

halcyon spindle
quartz palm
#

ok

#

technically in our class we haven't covered rref but i just thought this was easier

errant palm
#

hi, i don't get why the basis for the column spaces are what it says, can someone pls help?

quartz palm
#

what is theory 4.20

#

maybe knowing that can help

tribal willow
#

so basically if im understanding this right, T : V -> V and T(W) in W?

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then where does the name “invariant” come from

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can a subspace be "variant" in the sense that it varies?

wintry steppe
#

right, T(W) is a subset of W

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that's the "i.e. if..." part

tribal willow
#

ye

#

i guess a better question is like

#

the etymology of "invariant"?

wintry steppe
#

W is "invariant" under T

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well

#

i just restated the book

tribal willow
#

yea

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but in the sense that "annihilate" means to send to 0, is there a similar reason for "invariant"?

late tangle
#

hello

wintry steppe
tribal willow
#

i think im just trying to understand what it means for W to be "never changing"

wintry steppe
#

"T doesn't map W out of W" "T doesn't change W" "W is unchanged under T" "W is invariant under T"

little crater
#

Can someone comment on my solution for this question?

A. No, because if some vector y does not have solution for Ax = y, this means our column vectors of A don't span all of R^3. This also means we don't have a pivot in every row of our coefficent matrix (theorem 4). This then tells us that we must have some free variables as not all rows contain pivots. Now applying theorem 2, if we assume some z such that Ax= z is consistent, we know from theorem 2 that our z can only have infinite solutions because we have at least 1 free variable.

tribal willow
#

ohhh

#

ok that did it, thank you

wintry steppe
#

it's just a definition, you don't need to look too deep into it lol

little crater
#

(Theorems 2 and 4 I used)

wintry steppe
#

maybe another way to phrase it is "T fixes W" (note that this isn't "T fixes the elements of W"!!!!!!!)

sweet sand
wintry steppe
tribal willow
#

my calc 3 course didn't cover stuff like implicit function theorem; is that something i would find in an analysis course?

wintry steppe
#

i dunno

#

maybe such a course would be called "multivariable analysis"

#

"analysis course" means a million different things

tribal willow
#

ah i just meant analysis course as an umbrella term for all courses with the word "analysis" in it

#

interesting though

sweet sand
wintry steppe
#

i die inside a little everytime someone uses the word "analysis" and isn't referring to a course that's not just the contents of rudin

wintry steppe
#

love that one

sweet sand
halcyon spindle
little crater
#

NervousSweat First exam tomorrow and then we have a interview with our prof to discuss our solutions. cool thing is he seems very chill about how we get our solutions. He pretty much says it is open everything but whatever you put on your paper you better defend and be able to explain

#

Like these interviews are like 20% of our grade with the exam being 10%

#

Never had anything like that before but seems cool because it is sometimes hard to express what you want to say from a sheet of paper.

halcyon spindle
#

good luck!

little crater
#

We have not got into talking about linear independence and such but it would probably be easier to explain it like that.

native rampart
delicate crow
#

oh mb i didnt realise

late tangle
#

is linear algebra hard? i'm going into it in 3 years and i wanna prepare

native rampart
#

If you just want a basic understanding of linear algebra,you can do it in like 2 months

late tangle
#

wow ty so much

#

i think i might take some online courses then

#

is y=mx+b linear algebra?

native rampart
#

That's a linear equation

late tangle
#

o mb

#

i know how to do best fit y=mx+b

#

how do you do

#

that thing

wintry steppe
#

:^)

native rampart
late tangle
#

just Lagrange interpolation 🙄

uneven raptor
keen sierra
#

the word "best" isn't defined in the problem statement, but I assume a least squares fit would be intended

zinc timber
#

(T/F) A is diagonalizable then U is diagonalizable
, where U(B) := AB-BA

#

any ideas how I might approach?

fringe fjord
#

Without loss of generality, you can assume A to be diagonal.

#

But A cannot be a multiple of I, because then U(B) would be 0.

#

Pick the simplest A you can think of that satisfies these conditions, and calculate how U(B) depends on the entries of B.

#

Wait ... U rather than U(B) should be diagonalizable?

zinc timber
#

I have tried A=E¹¹ and E²²

#

that gives me digaonalizable operator

fringe fjord
#

Hmm, I mistakenly thought it was the concrete matrix U(B) that should be diagonal.

#

For U as an operator, the approach is definitely to work in a basis that diagonalizes A.

#

When you do the calculuations you will see that this basis also diagonalizes U!

zinc timber
#

that's my guess but this approach is kinda bruteforcy

fringe fjord
#

Perhaps, but it works and is pretty simple too.

zinc timber
#

it does but....

fringe fjord
#

Do you need an argument that works for infinite-dimensional spaces?

zinc timber
#

$A=c_i E_{ii}$ then $U(E_{jk}) = c_i E_{ii}E_{jk} - c_i E_{jk}E_{ii} = c_i \delta_{ij}E_{ik}-c_i \delta_{ki}E_{ji}$

stoic pythonBOT
fringe fjord
#

wdym "sure"?

zinc timber
#

$=c_jE_{jk}-c_jE_{jk}$

fringe fjord
#

One of those c_i should be c_j

zinc timber
#

oop

stoic pythonBOT
zinc timber
#

0?

fringe fjord
#

So U(E)_{jk} = (ck-cj)E_{jk}.

#

(modulo possible sign errors)

zinc timber
#

what is the finite dimensional argument?

fringe fjord
#

That's what you have just done.

zinc timber
#

oh you were talking abt this one

#

$(c_j-c_k)E_{jk}$

#

~looks diagonal to mecatThink~

stoic pythonBOT
zinc timber
#

typo

fringe fjord
#

Eyup.

zinc timber
#

nah

#

only thing left is to show it's diagonal

#

oh

fringe fjord
#

But what your calculation shows is that the E_jk's are an eigenbasis wrt U.

zinc timber
#

ye basis os Ejk so it's doagonal

#

I thought it's a matrix itself

fringe fjord
#

U would be represented by an n²×n² matrix, if we vectorize its input and output.

zinc timber
#

ye

#

cool, tks

wintry steppe
#

is a line considered hyperplane?

#

intro to linear algebra

#

but i think a line can be a hyperplane if its in like 2d space

wintry steppe
#

Hey guys I got a question, i had a markov chain question. The teacher wanted me to show that the eigenvalue is 1 and what its eigenvector is. i iterated the steady state vector, and said that because its steady the max eigenvalue is 1 and that the steady state is the eigenvector.
The teachers solution shows him getting the actual eigenvalue of one and the other eigenvalues

#

and then ends the entire solution with the steady state vector
is the steady state vector a scaled eigenvector with eigenvalue of 1?

jaunty thorn
wintry steppe
#

yes it was a markov chain question which was a stochastic matrix

jaunty thorn
#

just use the vector (1, 1, ..., 1), that multiplied by the stochastic matrix is (1, 1, ..., 1) so 1 is clearly an eigenvector

#

not a particularly satisfying proof but it works lol

#

because the rows of a stochastic matrix add up to 1

#

so you can figure it out just by inspection

wintry steppe
#

well he like went through the effort of getting the eigenvalues through the det

#

but that being said, i just figured okay, i got the steady state after 3 iterations of simple matix multplication, its got a steady state the max eigenvalue as one.

jaunty thorn
#

yeh thats a proper way of doing it

wintry steppe
#

is that steady state also the eigenvector?

#

because he scaled it in the solution from like the eigenvector from the polynomial he got

#

i made a silly mistake with svd 😦 i thought u held null of a since i knew it held row of a. sigh i feel dumb

#

def got a b

jaunty thorn
#

wait have you been given a specific stochastic matrix

#

or is he asking you to show that 1 is an eigenvalue for all stochastic matrices

wintry steppe
#

he gave me a specific one

jaunty thorn
#

ahh right if its small enough then yeah just compute it

wintry steppe
#

2x2 i just hate doing eigenvalues

#

and eigenvectors

jaunty thorn
#

lmao yeah relateable

#

good to be able to do though, the bastards come up absolutely everywhere kekw

wintry steppe
#

yeah yeah ill use python

#

i spent like 2 hours trying to solve that tbh

#

was the last problem.

#

because it was the only one i couldnt like even know where to begin at

#

it was the first thing we went over in class, and i just sat there and plugged it out and said okay this is converging like this

#

and then i had an oh yeah the steady state shit

#

okay now im gonna spend time working on programming

#

thank you mabey

jaunty thorn
#

good luck and have fun catKing

rain monolith
#

hi, im new here. I really need help with a question I have no idea how to approach, where can i post the question?

tribal willow
quartz palm
#

i dont understand how they got from the last step to the current step

wintry steppe
#

helloo! can anyone explain to me aboute the absolute value and with functions so basicallly f(x)=|x| or f(x)= -|x| or f(x) = |-x|

#

oops wait wrong chat

wintry steppe
#

so like graphing them

quartz palm
#

so say for |-x|

#

for x = 1

#

it would be |-1|

uneven raptor
quartz palm
#

how do u get 3.8 from R3 - 4R1

wintry steppe
quartz palm
uneven raptor
#

which is not shown

quartz palm
native rampart
fair wren
#

let E be a vector space with finite dimension, and f an endormorphism from E such that f² = -id

#

prove that that f has no real eigen values

dusky epoch
#

@fair wren do you still need help with this?

fair wren
#

i tried doing this

#

if i prove that f^n has no real eigen values

#

so is f right

#

so f has no real eigen values either

#

no?

dusky epoch
#

"if i prove that f has no real eigenvalues then f has no real eigenvalues either, right?" is this what you're asking?

dusky epoch
#

you're overthinking it

fair wren
#

hm really

#

please tell me

dusky epoch
#

let's start from the basics

fair wren
#

❤️ sure ann-chan

dusky epoch
#

...we are not anywhere near close enough for you to -chan me.

fair wren
#

sowy

dusky epoch
#

anyway, can you tell me what the phrase "f has an eigenvalue λ" means?

fair wren
#

f has an eigen value if the matrix representing it M(f) = A, then there exists lambda such that det(A - \lambda * I_n) = 0

dusky epoch
#

jesus christ

#

no that's way too complicated

fair wren
#

oh damn

#

idk sorry

dusky epoch
#

besides, lambda cannot be put under an existential quantifier

fair wren
#

maybe

fringe fjord
#

It's true, but not in any sane development is it a definition.

fair wren
#

f(v) = lambda v?

dusky epoch
#

that's closer

fair wren
#

and lambda is an eigen value

dusky epoch
#

there's something you missed

fair wren
#

yes

#

v != 0

dusky epoch
#

there exists a nonzero vector v such that f(v) = lambda*v

fair wren
dusky epoch
#

now assume f has a real eigenvalue λ

#

whence derive the existence of nonzero v such that f(v) = λv

#

now think about what f^2(v) might be

fair wren
#

yeah and f²(v) = lambda ² v² = - v

gray dust
#

where did v^2 come from

#

its not even a thing that makes sense

fair wren
#

just squaring f(v)?

fair wren
#

no?

fringe fjord
#

f²(v) here means f(f(v)) not f(v)·f(v))

fair wren
#

what what

dusky epoch
#

f^2 is the composition of f with itself

gray dust
#

powers of operators usually denote repeat composition

fair wren
#

im confused with this notation tbh

#

if its the second composition

#

then they should put ()

#

letting it like that is ambiguous

dusky epoch
#

no

fair wren
#

f^(n) means n-th composition of f

#

f^n is just f(x) * ... * f(x) n time ?

dusky epoch
#

this is an operator on a vector space

fair wren
#

its just confusing for me tbh

#

hm ok

dusky epoch
#

you can't multiply vectors by vectors

#

you can't

fair wren
#

there is no dot product then?

dusky epoch
#

dot product would return a number anyway

fair wren
#

hm ok

fringe fjord
#

And a function that takes a vector to a number cannot equal -id.

dusky epoch
#

so you would be unable to unambiguously interpret the "product" of three or more vectors

fair wren
#

hm

#

ok

dusky epoch
#

anyway, given that v ≠ 0 and f(v) = λv, what is f(f(v))?

fair wren
#

= lambda ² v

#

= -v

#

=> lambda² = -1

#

no real solution

#

contradiction then

dusky epoch
#

precisely

#

it is possible to generalize this a bunch

fair wren
#

so lambda ^ n = -1

#

hm?

dusky epoch
#

no, even more

fair wren
#

hm

#

tell me

dusky epoch
#

if an operator is annihilated by a polynomial then all of its eigenvalues are roots of the polynomial

#

i.e. if an operator A: V -> V satisfies p(A) = 0 where p is a polynomial then all eigenvalues of A are roots of p

dusky epoch
#

what do you mean "get"

#

it's given

fair wren
#

hm?

dusky epoch
#

it's part of the premise

#

for you the polynomial was x^2 + 1

fair wren
#

how u got that hm?

dusky epoch
#

?

#

you were literally told that f^2 + id = 0

fair wren
dusky epoch
#

what is this if not the polynomial x^2 + 1 applied to f

fair wren
#

ah so u treat f as x and id as 1

#

hm

dusky epoch
#

have you seen the notation of a polynomial evaluated at an operator before

dusky epoch
#

oh

fair wren
dusky epoch
#

part of the definition of p(A)

#

zeroth power of any operator is the identity

fair wren
#

ah ok gotcha

fair wren
#

since i've proven that the eigen values for f are complex

#

so if the power of lambda was odd then for example y^3 = -1 there is a real solution y = -1

#

so the power of lambda should be even

#

thus dimE should also be even

dusky epoch
#

this is nonsense; the power of lambda is given to be 2

dusky epoch
#

your problem says f^2 = -id, no?

fair wren
#

yes

#

wym nonsense?

#

which part i said was wrong?

dusky epoch
#

what you're talking about seems to be entirely unrelated to the problem at hand

#

if the power of lambda was odd

#

who give a shit

#

the power of lambda is 2. it isn't odd.

fair wren
#

hm

#

so how do u further proceed from that to say the dimension is even

dusky epoch
#

from what

#

what you said?

fair wren
#

we can say that dimE = sum dimE_k , E_k are eigen spaces, since we have only 1 eigen value with multiplicity = 2, then dim E = 2?

dusky epoch
#

overthinking it.

fair wren
dusky epoch
#

also we don't necessarily have only one eigenvalue and its multiplicity is not necessarily 1

#

we wish to prove dim(E) is even

dusky epoch
#

no its multiplicitly isn't necessarily 2 either

fair wren
#

Why

#

how do u know it isn't necessarily 2?

dusky epoch
#

i can give you an operator that satisfies f^2 + id = 0 with eigenvalues of multiplicity 69 if you want

#

but that's beside the point

fair wren
dusky epoch
#

no

fair wren
#

and tell me it isn't necessarily a multiplicity of 2?

#

so whats ur point?

dusky epoch
#

my point is that your attempt is going completely in the wrong direction

#

just because f^2 + id = 0 does NOT, i repeat DOES NOT tell you anything about the multiplicity of either i or -i as eigenvalues of f

fair wren
dusky epoch
#

suppose towards a contradiction that dim(E) is odd.
then the charpoly of f will have odd degree (why?) and thus something can be said about charpoly(f) that'll contradict what's been proved previously.

fair wren
#

@dusky epoch

dusky epoch
#

no

#

you're confusing dim(E) with "power of λ"

fair wren
dusky epoch
#

do you want me to repeat myself or what

subtle gust
#

how would we prove EF and FE are similar

#

assuming E and F are both invertible

#

EF=InEFIn

#

tried every single combination lol

#

don't see how i can go from EF to FE

dusky epoch
#

$FE = F(EF)F^{-1}$

stoic pythonBOT
subtle gust
#

how could i not notice

#

tysm

subtle gust
#

how would we prove that the adjoint of the inverse is the inverse of the adjoint

dusky epoch
#

show instead that adj(A)adj(A^-1) = I

subtle gust
dusky epoch
#

probably using the defn of adjugate

#

or using the fact that M adj(M) = det(M)I

subtle gust
#

are adjoint and adjugate used interchangeably?,,,,

#

anyways

subtle gust
subtle gust
#

cuz i tried inverting both sides and i didn't reach anything useful

#

what i got was adj^-1(A)=(1/det(A))*A

paper cedar
#

What's the best way to input mathematical symbols and stuff into Discord?

dusky epoch
#

use TeXit to render latex tbh

paper cedar
#

Sorry, I am super new. Is there a channel I should go to to get setup with everything?

zinc timber
winter harbor
# fair wren so how do u further proceed from that to say the dimension is even

If E is such a real vector space endowed with an endomorphism f : E -> E such that f^2 = - id, then you can define a complex vector space structure on E as:

(a+ib)*v := a*v + b*f(v)

Notice that the dimension of E as a complex vector space with the above scalar multiplication is precisely the original dimension of E as a real vector space. Now, use the fact that a complex vector space, when treated as a real vector space, always has even dimension.

dusky epoch
#

complexification moment

winter harbor
#

There's a more overkill solution

#

Using the fact that x^2 + 1 is irreducible over the reals.

#

The polynomial x^2+1 vanishes on f

#

thus dim(ker(f^2+id))= dim(E)

#

And the fact that x^2+1 is irreducible tells us that 2 = deg(x^(2)+1) divides the dimension of E.

#

So the dimension of E is even.

dusky epoch
fair wren
#

I still don't understand neither Ann's answer or the one above

dusky epoch
#

well in fairness i didn't supply all the details but for whatever reason you didn't ask me to clarify anything

#

suppose towards a contradiction that dim(E) is odd.
then the charpoly of f will have odd degree (because its degree is equal to dim(E)) and thus something can be said about charpoly(f) that'll contradict what's been proved previously (all odd-degree polynomials have at least one root, thus f will have at least one real eigenvalue, but we already proved that it doesn't.)

fair wren
fringe fjord
#

One argument is to unfold the determinant of tI-f using Leibniz expansion. There will be one term that is a product of dim(E) factors of the form (t-<diagonal element>), and no other term has anything of the same or higher degree in t.

#

So not only does the characteristic polynomial have degree dim(E); it's leading coefficient is 1.

#

Or (-1)^{dim E} if your definition of the characteristic polynomial is the determinant of f-tI instead.

little crater
#

This look right?

#

The terminology might not be correct with the word "unique" but I meant as not being able to right it as a linear combination of the other

#

although I guess w or u could have flipped with my use of "unique"

fringe fjord
#

Yeah, the "v is unique" language makes no sense.

little crater
#

yeah kinda meant relative to the other vectors :v but it doesn't make sense with regards to w and u

#

"linearly independent" maybe?

#

although normally that is used I believe with a set of vectors and saying how none of them can be express with combinations of the others

fringe fjord
#

It would be more direct to say something like "the first three spans are all { (x,y,0) | x,y in R }, but span{u,w} doesn't contain anything with nonzero y-coordinate".

#

Speaking of linear (in)dependence is definitely better than "unique".

little crater
#

yeah that would make more sense

#

I guess I could also then show via substation with regards to the spans to show how they are not equal, let u = a w (some scalar a), then say span{u,w} != span{u,v,w} because span{u,w} = span{aw,w}= span{w} but I guess I would still need to show that span(w) was not also span(v).

Maybe start off by saying let v b linearly independent from w and u and that u = aw and then talk about the above stuff.

#

but seeing it wanted 1 example and not something in general I guess I can just use the actually vectors I provided as an example

dusky epoch
#

E is the space

fringe fjord
#

whoops, fixed.

high peak
#

Solving Ax = b where A, b have complex elements would be the same as solving it normally (just w/ complex arithmetic) correct?

high peak
#

thanks!

winter harbor
#

Complexification is a thing in linear algebra tho lol

fair wren
winter harbor
#

Essentially, a finite dimensional complex vector space can be treated as the same thing as a real vector space endowed with an endomorphism J that squares to minus the identity.

#

This is a pretty simple idea that is used a lot in quite different contexts.

wintry steppe
#

👀

#

kahler moment

winter harbor
wintry steppe
zinc timber
dusky epoch
#

something something K[x]-modules

dusky epoch
#

which part of tropo's explanation did you not understand?

pliant kayak
#

Is someone in the mood to explain tensor product to me?

winter harbor
#

Yeah, I could do that.

#

But first

#

Could you explain in our own words what the tensor product of vector spaces is?

#

That should give me a rough idea of what is troubling you with the definition.

pliant kayak
#

It's in German, give me a second

#

(sending it so I can translate it)

#

It says that the tensorproduct of two Vectorspaces V1 and V2 over the field K is composed of a Vectorspaces V' and a bi linear function k:V1×V2 - > V' with the universal property that for every Vectorspaces W and every bi linear function phi: V1×V2->W exists an unique linear Funktion phi ':V' - >W, with phi' °k=phi
(I hope you can understand something)

#

I mean I get the definition, but somehow it confuses me anyway

winter harbor
#

Yeah so

#

The idea is precisely that the tensor product of two vector spaces turns bilinear maps into linear ones

#

In a canonical way

#

And that's precisely the reason why the tensor product exists.

#

This can be summarized as follows, for $V_{1}, V_{2}$ vector spaces over a field $\mathbb{K}$, the tensor product $V_{1} \otimes_{\mathbb{K}} V_{2}$ of $V_{1}$ and $V_{2}$ is the unique vector space (up to isomorphism) that satisfies for any vector space $W$
$$
\text{Bil}(V_{1} \times V_{2}, W) \cong \text{Hom}(V_{1} \otimes_{\mathbb{K}} V_{2}, W) \cong \text{Hom}(V_{1}, \text{Hom}(V_{2},W))
$$
The isomorphism:
$$
\text{Hom}(V_{1} \otimes_{\mathbb{K}} V_{2}, W) \cong \text{Hom}(V_{1}, \text{Hom}(V_{2},W))
$$
Is called the tensor-hom adjunction, and is in a sense what defines the tensor product (up to isomorphism).

stoic pythonBOT
#

MISTERSYSTEM :urs:

winter harbor
#

Of course

#

This definition only tells us the universal property that the tensor product of two vector spaces satisfies.

#

But it doesn't tell us anything about how to construct one explicitly.

#

The next step would be to show that the tensor product of two vector spaces always exists by constructing it explicitly.

#

There are lots of ways to construct it

#

But you know

#

I think the best thing to have in mind would be that the tensor product satisfies this universal property.

#

Rather than knowing how to explicitly construct it.

fringe fjord
#

One way to look at the explicit construction it is that an element of the tensor product is a recipe for "what to do with a bilinear map from VxW once someone provides us with one*. At that time we can apply the map to various pairs of vectors, add the results, perhaps scale them. But we don't yet know which bilinear map we'll be given, so we don't know what its codomain is or what we can do with the results other than things that are possible in every vector space. And additionally we don't want to distinguish between recipes that are guaranteed to yield the same result for every bilinear map.

pliant kayak
fringe fjord
#

It's literally the entire definition, so in that sense it is "most important". On the other hand, for the same reason that it eventually tells you literally everything there is to know about the tensor product, it doesn't necessarily provide much focus.

fringe fjord
#

In particular, don't become so focused on the universal property that you forget the map k and what it alone can tell you about the tensor product without the rest of the universal property:

  • Each time you have a vector v in V1 and w in V2, you get an element k(v,w) of the tensor product.
  • To an extremely coarse approximation the tensor product can be thought of as being made of these combined elements.
  • The tensor product is a vector space, but its addition and multiplication operations need to work in funky ways in order for k to be bilinear.
  • If c is a scalar, then c·k(v,w) must be both k(cv,w) and k(v,cw) -- and so these must equal each other -- but it cannot be k(cv,cw) because that is c²k(v,w), which is different unless c is 0 or 1.
  • k(v,w) + k(v',w') cannot be the same as k(v+v', w+w'), because that would mean that k(v,w)+k(v,w) is k(2v,2w) = 4k(v,w) instead of 2k(v,w) like it ought to be. In fact k(v,w)+k(v',w') is not generally even in the image of the map k!
  • However, bilinearity means that k(v,w)+k(v',w) = k(v+v',w).
uncut yarrow
#

how would you prove: $ \begin{bmatrix}
1 & 1 \
0 & 1 \

\end{bmatrix} $ is not diagonizable

stoic pythonBOT
#

! matthewzz

uncut yarrow
#

is it because you have one eigenvector for the eigenvalue of 1 (which has multiplicity of 2)

hard drum
#

Yup, there is only one eigenvector (up to scaling)

uncut yarrow
#

also a scalar matrix is just

#

c * i (nxn identity matrix)

zinc timber
#

you can geometric multiplicity is 1 where as AM is 2

outer hazel
#

I got x=0
y=0
And z=0
After using Gaussian elimination. Does this mean anything, or is that just the answer

dusky epoch
#

outside of context, this means nothing

outer hazel
#

Idk if im asking the right questions,
What does it mean when all 3 equations in a matrix equal to 0.

dusky epoch
#

not sure what kind of "meaning" you want to get from that

#

are you asking if systems of linear equations where all right-hand sides are 0 have any special properties?

outer hazel
#

Ah yes

dusky epoch
#

well, one particular property of any such system is that the solution set is a subspace of R^n (where n is the number of variables) and in particular such systems are always consistent because they always have the all-zeroes solution

#

there's even a name for these: homogeneous systems

outer hazel
#

I see
Thanks for the info

deft sable
dusky epoch
proper cradle
#

Suppose A is n*n symmetric matrix and positive definite then how i can write diagonal entries of A in terms of eigen values and eigenvectors based on jordan normal form?

proper cradle
#

help please

hushed ocean
#

Hi guys, does anybody know of a problem in computational linear algebra which frequently requires large chains of matrix multiplication?

#

Aside from computer graphics

elder monolith
#

can u me ?

hallow arch
#

What does the dash on top the A mean?

#

trying to figure out how to solve it

fleet sun
#

conjugate

hallow arch
cinder meteor
#

In the process of transferring all my linear algebra notes to obsidian for future reference, here's the graph of all the different concepts so far

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this is about 5 hours of work, definitely should've done this throughout the year instead lol

tribal willow
#

here's my obsidian of lin alg notes

zinc timber
#

looks cool ngl

#

how does it work?

tribal willow
#

each node is an individual file, when you're writing you can link to other files

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sorta like wikipedia

#

and then it draws a line between the two notes

zinc timber
#

cool

wintry steppe
#

grassman ring stare

#

based

zinc timber
#

hoffman kunge I suppose

wintry steppe
#

that's a nice balance of matrix computation stuff and theory stuff

tribal willow
#

yeah i like hoffman kunze approach

zinc timber
#

I like exercises

tribal willow
#

i hate exercises devastation

tribal willow
#

is this calling me lazy

#

i wouldnt disagree im just making sure

zinc timber
cinder meteor
tribal willow
#

oh to have a high school linear algebra class

#

what a dream

cinder meteor
#

What are the nodes that start with ! for?

tribal willow
#

indices

cinder meteor
#

Ohhh gotcha

#

That might be a good idea for my notes

tribal willow
#

surprised you guys didnt learn fields tho

#

considering that like

cinder meteor
#

We did vector spaces

tribal willow
#

vector spaces are defined over fields

cinder meteor
#

Yeah I leaned vector spaces independently from fields completely

tribal willow
#

hmm

#

i guess it makes sense

#

don't really like

#

need to know what a field is to get what a vector space is

cinder meteor
#

It was defined to me by the axioms and once i heard abt the examples I had a pretty solid grasp of it

#

Absolutely blew my mind when I first learned that you could use polynomials and functions as vectors

tribal willow
#

tEcHnIcAlLy a field of scalars is a vector space axiom

cinder meteor
#

Yeah we got a pretty circular definition ig

#

Vector: an element of a vector space
Vector space: a set of vectors

tribal willow
#

a field is just a set with certain axioms

#

pretty sure the axioms of vector space and field are pretty similar

cinder meteor
#

I’ll check out fields rq

tribal willow
keen sierra
#

every field is a vector space over any of its subfields (including over itself), this fact is used heavily in field theory

tribal willow
#

oh damn

#

i didnt think about that

#

but it makes sense

cinder meteor
# tribal willow

I’m assuming the circular plus and multiply signs are just generalized adding and multiplying for different fields?

tribal willow
#

i dont remember why i used oplus tbh

#

the only important thing is that there's operations addition and scalars

cinder meteor
#

I gotcha

tribal willow
#

it's bad notation on my part tbh

#

oplus typically represents direct sums in lin alg i think

cinder meteor
#

So does a field require you to be able to multiply two elements of a field? Because how do you multiply two vectors in R^2 for example?

tribal willow
#

dot product

#

or er

#

i guess

cinder meteor
#

But wouldn’t you want a multiplicative operation that returns another vector or does that not@matter?

tribal willow
#

you would need to define that multiplication

#

a multiplicative operation of vector * vector = vector would be cross product, i think

cinder meteor
#

I gotcha

wintry steppe
#

for R^2, you can multiply vectors like you do complex numbers

#

identifying $\bR^2 \ni (a, b) = a + bi \in \bC$, you get $$\begin{pmatrix}a\b\end{pmatrix}\begin{pmatrix}c\d\end{pmatrix} = (a+bi)(c+di) = ac-bd + (ad + bc)i = \begin{pmatrix}ac - bd \ ad + bc\end{pmatrix},$$ and that makes $\bR^2$ into a field

stoic pythonBOT
#

TTerra

wintry steppe
#

(isomorphic to C)

cinder meteor
#

I gotcha

#

So for R^3 can you just foil some more with a stand in j?

gray dust
#

@cinder meteor plenty of things can be said for vector spaces without such an operation, but plenty can be also said for spaces with such an operation, see algebras

wintry steppe
tribal willow
#

oh shit true

wintry steppe
#

you have a lie algebra, though

#

which is still nice

tribal willow
#

yes that is totally what i meant haha yes! i know what lie algebras are 100%

#

i am excited to learn lie algebra

#

it is somewhere down on my list of things i want to learn

wintry steppe
#

you should be

tribal willow
#

it's also supposedly really important for quantum mechanics?

wintry steppe
#

they're a lot of fun!

#

yes, i think so

tribal willow
#

dope

wintry steppe
#

i couldn't tell you exactly how though

cinder meteor
wintry steppe
#

no no no no no no no no no no no no no

gray dust
#

compare the defs

cinder meteor
gray dust
#

a field is a vector space with itself as the base field

#

not all vector spaces are fields

cinder meteor
#

Ohh so the field isn’t a parent of the vector space

gray dust
#

in fact one must equip a vector space with vector multiplication to even ask if its a field

#

since a vector space doesnt have vector multiplication by default

cinder meteor
# tribal willow

Ohh so the field isnt the elements of the vector space itself, but the scalars thst you do operations with vectors in the vector space?

#

Lmk if i have this wrong

gray dust
#

eg R^n is a vector space over R

#

meaning the elements of R^n are called vectors

#

elements of R are called scalars

cinder meteor
#

So what field would the set of all second degree polynomials be? Would that also be R?

gray dust
#

in general a vector space requires two things, a set of vectors and a set of scalars (the latter called a field)

#

theres still poor terminology here

#

we say a vector space is OVER a field

#

also degree 2 polynoms dont form a vector space

#

but the polynoms of degree at most 2 do

#

and its a vector space over R

keen sierra
#

the field of rational functions, for example

gray dust
#

we’re identifying vector space/field pairs

keen sierra
#

maybe he meant what vector space contains the 2nd order polynomials?

gray dust
#

yes, which is what my example does

cinder meteor
gray dust
#

but the polynoms of degree at most 2 do
to be concise the polynom coefficients are real

cinder meteor
#

So can you have two different vector spaces that share a set of vectors, but are over different fields?

#

(My bad for asking so many clarifying questions, fields are pretty new to me atm)

keen sierra
#

a vector space over some field is also a vector space over any subfield of that field

#

for example R^2 is a vector space over R, but also over Q

gray dust
#

another example is

#

C is a vector space over C

cinder meteor
gray dust
#

C is also a vector space over R

cinder meteor
#

Thus making R a subfield of C

gray dust
#

the reason is it satisfies the vector space axioms, but thats not too illuminating

#

whats more illuminating is that the key behind checking the axioms is that R is a subfield of C

cinder meteor
#

I gotcha

faint hearth
#

How would I normalize a Vector based on a different vector?

#

Probably asked that wrong

hallow vector
#

any idea on how to start this one? I tried just putting the numbers in random order but couldn't find a combination

dusky epoch
#

4 6 10 13
6 4 13 10
10 13 4 6
13 10 6 4

hallow vector
#

what lol i've been staring at it for like an hour

#

how did you understand what kind of pattern the numbers needed so that the matrix is symmetric?

dusky epoch
#

i started with the first row and kind of filled it in row by row i guess

hallow vector
#

oh i see there's a diagonal pattern in the numbers now

#

also each mini 2x2 matrix in the 4x4 matrix is symmetric it looks like

faint hearth
#

So if I normalized 400, 60 it would be 1, 0

peak lodge
#

say you have a matrix A, is there any tricks to find the determinant of A^3 ?

#

besides manually finding A^3 and then getting the determinant

gray dust
#

so det(A^3)=(detA)^3

peak lodge
#

oh damn yeah i forgot about the determinant properties

#

thank you

serene solstice
#

How to prove that f is linear?

subtle walrus
#

using the definition of linear

verbal wedge
#

do I need to consider X^TX?

dusky epoch
#

do you know the definition of the frobenius norm?

verbal wedge
#

this one?

verbal wedge
dusky epoch
#

that first one will be enough

#

do you know why $\nrm{\bd{y}+\bd{z}}^2 = \nrm{\bd{y}}^2 + \nrm{\bd{z}}^2$ when $\bd{y}, \bd{z}$ are orthogonal vectors in $\bR^m$?

stoic pythonBOT
verbal wedge
#

I presume the proof is something to do with the inner product and how that's related to y^Tz

dusky epoch
#

...yes the proof does have to do with the inner product but also it's just pythagorean theorem generalized

verbal wedge
#

ah that makes more sense

#

thank you

dusky epoch
#

in fact $\nrm{\bd{X}}F^2 = \sum{i=1}^n \nrm{\bd{x}_i}^2$ as should be relatively clear

stoic pythonBOT
verbal wedge
#

yeah, I got to that part, didnt realise the orthogonality implication though

#

I get it now tho thanks

verbal wedge
#

@dusky epoch if you don’t mind, I had another thought I didn’t quite get

dusky epoch
#

C has orthogonal columns doesnt mean C^T C = I, it just means C^T C is diagonal

verbal wedge
#

really? it says in an example that this is true

#

it's the next part to the previous question

#

I reduced it to equating the statement in the note I've written is true

dusky epoch
#

maybe they meant orthonormal instead

verbal wedge
#

yeah, it should be that shouldn't it

#

lets say it is orthonormal, does my reasoning still stand?

dusky epoch
#

it seems ok but im not 100% sure and dont have the energy to check it for sure

verbal wedge
#

no worries

verbal wedge
#

nvm I found the solution

boreal wadi
#

$x^Ty$ is a dot/inner product

stoic pythonBOT
#

melling