#linear-algebra

2 messages · Page 252 of 1

noble swan
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Pfff, bad book

zinc timber
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we actually extend the concept of basis to the 0dim space

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so in some way it is correct,

still lodge
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is this an appropriate restatement of cayley hamilton: the characteristic polynomial of a matrix A annihilates said matrix

noble swan
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Gotcha, thanks for the help!

still lodge
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i mean wikipedia has every square matrix over a commutative ring (such as the real or complex field) satisfies its own characteristic equation.

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now idk what a commutative ring is (yet) but it sounds at least close to interchangeable

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im just tryna find my own wording so it's easier to grasp

sinful valve
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right so yeah svd is calm tbf

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where has this $M=AA^T$ come from

stoic pythonBOT
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shriller44

still lodge
zinc timber
lavish jewel
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AA^T and A^TA are symmetric, and therefore diagonalizable

sinful valve
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so yeah the idea is just getting the same orthogonal matrices

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as in same sense as eigenvalue decomp before this was mentioned

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just that that eigenvalues and vectors are taken as squared to get singular values

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wait nah S^2 and U/U^T is the eigenvalues n vectors of AA^T

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but we are interested in singular values of course

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presumably theres more than this just method to do SVD but yeah its calm

still lodge
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B is a 5 × 5 matrix with minimal polynomial (x - 1)(x − 2)^2

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is it possible to determine the characteristic polynomial of B from this info

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it's over complexes btw

zinc timber
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No

still lodge
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there are a limited number of possibilities though right

zinc timber
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it could be anything of the following
\begin{align*}
(x-1)(x-2)^4 \
(x-1)^2(x-2)^3 \
(x-1)^3(x-2)^2
\end{align*}

stoic pythonBOT
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Ryuzaki

still lodge
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alright cool that's what i thought, just double checking :)

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now if a 5x5 matrix has minimal polynomial x^3, then that must mean that the characteristic is x^5 right...?

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bc the only eigen value would be 0

zinc timber
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yes

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can you also calculate rank the of matrix with this info?

still lodge
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educated guess but wouldnt it be 3...?

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actually wait

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no yeah three

zinc timber
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2

still lodge
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why

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i was looking at JCF

zinc timber
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you need JCF for this

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there are 2 missing EVs

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so 2 1's

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rest zero

still lodge
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well if it's min polynomial is x^3 can't it have two possible JCFs

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either two blocks of single 0's or a block w two 0's and a 1

zinc timber
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char = x⁵

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only one possibility

still lodge
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ok then there's something wrong in my understanding can you elaborate pls

zinc timber
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an eigen value of algebraic multiplicity m and geometric multiplicity k means there are k-1 blocks of 1x1 and one large jordan block of size m-k+1

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let's take a simple example

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say min = x² and chr = x³ then

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$A=\mqty[ 0&0&0\0&0&1\0&0&0]$

stoic pythonBOT
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Ryuzaki

zinc timber
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do you agree?

still lodge
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yes

zinc timber
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recognize the 1x1 and 2x2 blocks

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yeah there is a 3x3 jordan block as you might have deduced

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but remember that in the 3x3 block there are only 2 ones

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number of ones = size of block - 1

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so you get 3-1=2 ones, giving you rank 2

lavish jewel
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i'm gonna have to learn this stuff at some point

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but what are you calling rank here

zinc timber
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rank of the entire matrix given min poly = x³ and char poly = x⁵

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context was different here

lavish jewel
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aight

still lodge
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hmmm

still lodge
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does the min polynomial kinda tell us what the largest block can be

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^^that could be very wrong

zinc timber
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what do you think the blocks should be

still lodge
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2x2 and 1x1

zinc timber
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ig you can find the max block size but not the exact size

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@still lodge no no I was talking about the x⁵ and x³ case

still lodge
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ohhhhhh ok yeah i was gonna say

zinc timber
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u did deduce right?

still lodge
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yeah

zinc timber
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ok then number of 1's = ?

still lodge
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but if you have the 3x3 block in the 5x5 matrix, couldnt the remaining slot(s) be a 2x2 or 2 1x1s?

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and if you have a 2x2 block you have another 1

zinc timber
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yeah but min poly discards the 2x2 block

still lodge
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why

zinc timber
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no wair

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it doesn't

still lodge
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aha

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x^2 * x^3 = x^5

zinc timber
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x³ not x², my bad

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yeah

still lodge
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ok this was still helpful ty <3

zinc timber
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there will be 2x2 block giving rank 3

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you were right

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whole time I was thinking it's x²

wise oriole
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Can someone help me w this one

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Question: Determine the pairs (a, b) ∈ R × R such that the system

respectively
(a) has no solution
(b) has a unique solution,
(c) has several solutions.
Show how you arrive at these conditions.

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I found this but I don't know what to do now

zinc timber
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can you tell me what is the condition for unique solution

wise oriole
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(a,b) element R x R that?

zinc timber
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no not that

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the one involving the ranks of the augmented matrix

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ok if you don't remember it then say our unknowns were x,y,z then the last row gives us

wise oriole
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the question above that's the only thing we got

zinc timber
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(1-b²)z=-(a+2)

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when can a solution of this exist?

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what values must b take?

wise oriole
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1 and -1?

zinc timber
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say b = 1 or -1 and a=0

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what does that give you?

wise oriole
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0?

zinc timber
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0=-2

wise oriole
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oh yh

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ah

zinc timber
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so you see how you are supposed to derive the conditions?

wise oriole
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but where did you get the (1-b²)z=-(a+2) from

zinc timber
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the last column of your matrix

wise oriole
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(b) has a unique solution then a can't be -2 and 2 / b can't be -1 and 1 right

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for (c) has several solutions: b=1/-1 and a=-2

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(a) has no solution if a is not -2

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is this correct

zinc timber
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for unique solution, it doesn't matter what a is, all you need to care about is 1-b² is not 0

wise oriole
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Then a can be everything

zinc timber
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yeah

wise oriole
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How can I say that symbolic is that a element R

zinc timber
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you only need b ≠+1 or -1

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a ∈R

wise oriole
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Oké thanks a lot

zinc timber
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your other conclusions are also wrong tho

wise oriole
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Yeah?

zinc timber
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when will u get infinite solutions?

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ok tell the conditions again

wise oriole
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(1-b^2)a=-(a+b) or b is 1 and -1

zinc timber
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see

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infinite solution means that the last equation is degenerate. like 0=0. which values of a and b give you 0=0?

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that should be the condition for infinitely many solutions

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it just means you get no additional information from the 3rd equation

wise oriole
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b = 1 or -1 you get 0 and a = -2 or am I dumb

zinc timber
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yeah

wise oriole
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Yeah bcs I’m dumb or yeah that is correct

zinc timber
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correct, lol

wise oriole
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Then why is it wrong you said

zinc timber
wise oriole
zinc timber
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no solution if u get some kind of contradiction like 0= 1

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b=±1 but a≠2 gives 0 = some non zero number

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which is impossible

wise oriole
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Then a can be everything but can’t be -2

zinc timber
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ya

wise oriole
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a ∈R / {-2} ?

zinc timber
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hm

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although it's\ and not /

wise oriole
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yh but i don't have that symbol 🙂

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and it was quick but it's right

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or not

zinc timber
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doesn't matter

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ya it's right

wise oriole
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maybe i have a quetion later but i'm ok for now thank you for your time

ionic laurel
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hi i have a few questions

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The matrix A and (B^-1)(A)(B) then they have the same set of eigenvalues for every invertible matrix B <- This is true correct?

If 2 is an eigenvalue of A, then A-2I is not invertible. (I believe this is true as well)

If two matrices have the same set of eigenvalues, then they are similar (True? Not sure)

pallid rampart
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I found out that this is true if you let the vector space to be $\brc{f\in C^\infty([-\pi,\pi]):f(-\pi)=f(\pi)}$

stoic pythonBOT
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Whoever

still lodge
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what's the difference between elementary divisors and invariant factors

worldly bear
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ive found the the characteristic polynomial of a 2x2 matrix A is x^2 - tr(A)x+det(A), and that for a 3x3 matric A, we have x^3 -tr(A)x^2 -det(A)

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Is there a similar way to find the coefficient of the linear term of the characteristic equation of the cubic or is it not possible

winter harbor
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You write it in terms of the exterior powers of your matrix.

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More specifically.

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Let $A$ be an $n \times n$ matrix over a field $\mathbb{K}$ and denote $p_{A}(x) \in \mathbb{K}[x]$ its characteristic polynomial, then:
$$
p_{A}(x) = \sum\limits_{k=0}^{n} x^{n-k} (-1)^{k} \text{tr} \left(\bigwedge^{k} A \right)
$$

stoic pythonBOT
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MISTERSYSTEM

winter harbor
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This is a consequence of something called the newton identities, which relates elementary symmetric polynomials and power sum symmetric polynomials.

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This can also be derived by embeding your matrix into the splitting field of the characteristic polynomial and using something called vieta's formula.

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You can do this because the minimal and characteristic polynomials are invariant wrt field extensions.

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I found these two stack exchange threads which might give a more in depth explanation.

worldly bear
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so I just need to learn how to compute the exterior powers of a 3x3 matrix and then I will be able to write the characteristic polynomial just by looking at it nearly?

winter harbor
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You actually just need the trace of the exterior powers tho

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If the characteristic of your field is 0

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there's an explicit formula

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which relies on computing a certain determinant

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but idk if it is worth it

worldly bear
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I think it would be nice to just go straight to the characteristic polynomial without the typical steps of det(A - lambda*I) personally

winter harbor
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Axler presents this in a short ''paper'' entitled ''down with determinants''

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which motivated him to write his book ''linear algebra done right''

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but like

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Computing characteristic polynomials like that is just...

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why would you do that

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The determinant is a tool made for computation

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so like, if you really need to calculate something explicitly, go for it.

worldly bear
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i found it

winter harbor
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this is the paper I was referring to

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ah, nice.

pliant blaze
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hi does det(-A) == det(A)

worldly bear
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i like his opening two paragraphs already

winter harbor
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for instance

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take the 2x2 identity matrix

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the determinant of - I_2 is 1

pliant blaze
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ahh ic

winter harbor
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what is true tho

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is that det(A) = c^n det(A) where n is the size of the matrix, i.e A is an n x n matrix.

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so that det(-A) = (-1)^n det(A)

pliant blaze
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yeah just remember that\

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thanks

still lodge
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If 𝑞(𝐴)=0, then 𝑞 is divisible by the minimal polynomial of 𝐴

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why isnt this named lmao

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this feels really important

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@/MISTERSYSTEM ive done some problems since we last discussed this stuff and i think ive gotten better :)

wintry steppe
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it's not named because it's basically the definition of the minimal polynomial

winter harbor
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Yeah, TTerra is right lol

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Remember how I said F[x] is a PID for F a field and we define the minimal polynomial of a matrix A as the monic polynomial that generates the ideal
Ann(A) = {f \in F[x] : f(A) = 0 } ?

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That's the idea nitez

wintry steppe
winter harbor
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yeaaaaaaaaaaaaah

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thanks

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Was dumb for a sec there stare

still lodge
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yeahhh i havent taken abstract alg yet so i only have a loose idea of what a field even is

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but our original discussion prompted me to at least make note of it to look into over winter break

worldly bear
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i feel better about not knowing what a field is bc 8 year old terance tau didn’t either 🥲

still lodge
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terrence 2pi

still lodge
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sorry to nag but

steel moon
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for #1, im having trouble to find two matrices that dont satisfy closed under addition / multiplication

lavish jewel
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how about this

steel moon
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what is that tool you are using?

lavish jewel
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the scalar mult part is also easy. take an identity matrix of size 2n+1 x 2n+1 and multiply it by -1

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it's octave 😛

steel moon
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interesting, is it some sort of computational tool for math?

lavish jewel
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indeed

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a slow but free version of matlab, sort of

steel moon
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oh cool

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for the purpose of this problem, one counter example for a property would suffice right?

lavish jewel
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for the purpose of any problem in which they ask if something is true, one counter example is enough to say it isn't

steel moon
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gotcha

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and for the 2nd problem, we should show each set is a subset of the other right?

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So something like let s in Span(S). then s is a linear combination of each of the elements in S

lavish jewel
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should be enough to show that the elements in S are linearly independent

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then mention the dimension of P3(R)

steel moon
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each of the elements in S have x^3 in it

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hm i guess i should expand it out firsrt

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to show the elements in S are linearly independent, i would need to show theres a non-trivial linear combination that equals the 0 vector

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oh whoops i got the definitions mixed up

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thats for dependant

wintry steppe
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Is anyone using the latest calculator from Texas Instruments which is the Texas Instruments C version? The one with the python programming that was released in the fall? If so, does it support Linear Algebra?

forest quiver
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My teacher meant "noncolinear" instead of "nonparallel" right?

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Oh wait no he didn't if they were parallel it would become some sort of line equation

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Wait,,, don't they mean the same thing with 2 vectors?

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Ugh

marble lance
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What does noncolinear mean for 2 vectors? If you seem them as points, then any 2 points lies on the same line. If you see them as directions and you just mean colinear as they point in the same direction, then that is the same as parallel. So I think the right word here is nonparallel.

zinc timber
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yeah you can say that they are non- parallel

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$\vec{v}_1 = c \vec{v}_2$ is also another way of saying they are co linear, so, if there is no contant c satisfying this, they are non co-linear

stoic pythonBOT
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Ryuzaki

golden kindle
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Anyone know good websites to practise linear alg problems

merry imp
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can i get a hint for this? i have an expression for the inverse of A-I by factoring A^k - I, but how can i use that to find the inverse of A+I?

teal grotto
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(-A)^0 + (-A)^1 + ... = (I - (-A))^{-1}

quaint steppe
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Hi everyone currently studying linear algebra
can someone further explain to me these example on why they are not invertible?

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what does it mean 1 is not in the range?

slow scroll
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It means that there is no x such that f(x)=1

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In general a function is invertible if and only if it is bijective.

quaint steppe
limber sierra
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right

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if $f$ is a function $A \to B$, then $f^{-1}$ must be a function $B \to A$

stoic pythonBOT
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Namington

limber sierra
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but as the image notes, $1$ is not in the range of the multiply-by-$x^2$ map

stoic pythonBOT
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Namington

limber sierra
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so $f^{-1}(1)$ makes no sense

stoic pythonBOT
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Namington

limber sierra
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hence an inverse cant exist

quaint steppe
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okay i kinda understood it already for example 2, what does backward shift means?

lavish jewel
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take all of the elements in the list and shift them one of the left

quaint steppe
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does it mean like $R^3$ going to $R^2$ for example?

stoic pythonBOT
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jinichi

lavish jewel
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if you start with (0,1,1,...) the transformation yields (1,1,0,...)

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so they note that if you have a nonzero element in the first position, the transformation gives you 0, so it has a nontrivial kernel

quaint steppe
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oh so basically the linear map backward shift rotates the input to the left and make the first input goes last?

lavish jewel
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i don't believe they mean circular shift

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just shift

quaint steppe
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oh okay

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Thank you very much

quaint steppe
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I'll probably gonna ask more questions later.

wintry steppe
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Guys, I'm dealing with a rotation matrix rotating vectors by an angle 30 degrees about the z axis. I've found one of the eigenvectors which is (0, 0, 1).

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but is it the same as (0, 0, 1)^T ?

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Transpose of that vector?

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I'd just say that eigenvector and the transpose of it are the same thing.

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(0, 0, 1)^T = (0, 0, 1)

lavish jewel
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they're not the same thing, but they are both eigenvectors of the matrix

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call your matrix R and this vector v, with eigenvalue lambda

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then v^T R = v^T lambda, and R v = lambda v

wintry steppe
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I mean yeah one of them is column vector and the second is a row vector.

lavish jewel
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this is in general not true btw

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but a rotation matrix is block diagonal, with a block that has just a 1, so it holds in this case, for this eigenvector

wintry steppe
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How can I show that they are both eigenvectors of the same eigenvalue?

lavish jewel
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apply the definition of eigenvector twice

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once from each side 😛

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you can also stop for a while to consider what it means for one matrix to be the inverse of another, and then assume your rotation matrix is diagonalizable

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if AB = BA = I, and you consider the matrix product and a bunch of dot products, it might become clearer

wintry steppe
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Should I infer any meaning from that?

zinc timber
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orthogonal matrix doesn't necessarily mean rotation

sinful valve
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what does he mean exactyl

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the inverse is the same as the complex conjugate transpose

zinc timber
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is that $AVV^{-1}=\hat{U}\hat{\Sigma}V^{-1}$?

stoic pythonBOT
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Ryuzaki

sinful valve
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yes

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its just another video i was watching on svd its really good just missing this one fact

zinc timber
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looks like some kind of svd decomposition

sinful valve
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yeah it is

zinc timber
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you need to tell the context before I can answer

sinful valve
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this is the timestamp exactly

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but hes just constructing the SVD

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its just the * thing im not sure about

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its often transpose

lavish jewel
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probably that U and V are unitary matrices

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so their inverse is their complex conjugate transpose

sinful valve
zinc timber
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Oh he already derived $AV = \hat{U}\hat{\Sigma}$ and then multiplying both sides by $V^{-1}$

stoic pythonBOT
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Ryuzaki

lavish jewel
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right, and V is unitary, so V^-1 = V^H

sinful valve
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yeah basically

lavish jewel
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in some places this is written as V^*

sinful valve
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unitary matrices i have never heard of ill have to check that

zinc timber
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basically orthogonal but in the context of complex sapce

lavish jewel
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it's the complex flavor of orthogonal matrices

sinful valve
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why do other svd not talk about this version though

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like explanations of it

lavish jewel
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wdym

sinful valve
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complex number version you mentioned

lavish jewel
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they all mention that U and V are unitary. in the real case, they mention they are orthogonal

sinful valve
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uh some didnt i dont remember but

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yeah ill just see

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is there any use case for the complex numbers in svd though?

lavish jewel
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more than use case, you can't avoid it

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when all the entries in the matrix are real though, the SVD will be as well

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or at least it CAN be, since the svd is not unique

sinful valve
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not unique as is in its general to any matrix you mean

zinc timber
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means given a matrix, the u, v, s matrix will always be the same(upto permutation)

sinful valve
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so its literally just

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the same idea but a different way of inverting it

zinc timber
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yes

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sometimes written as U^* instead of U^H

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well most of the time

sinful valve
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yeah wikipedia said there is like 4 notations to use

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that dagger looks cool tbf might use that

zinc timber
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the dagger and + I use for pseudo inverse, never knew physicians use that for conj-transpose

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lol

sinful valve
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so in my guys video then

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he has used a unitary matrix to include all real/complex basically

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to make it general ig

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cause my book only cares about real so it just say orthogonal

zinc timber
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yeah

sinful valve
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ight

zinc timber
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you can get away with saying orthogonal if the space is real

sinful valve
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when would you use an svd in complex space though

lavish jewel
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whenever it's handy to use complex numbers

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so usually engineering and physics applications

sinful valve
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yeah thats fair in computer science i dont see many uses tbf

lavish jewel
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also, the svd unique up to rotations

sinful valve
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as far as i know at least

lavish jewel
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unless you have repeated singular values, permutations won't show up

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you might use it in CS as well, since stuff like rotations are easily done with complex numbers

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at least in the more applied stuff like computer graphics

sinful valve
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yeah this is for CG this content

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the only complex numbers i cant think of are in the fast fourier transform

lavish jewel
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then you'll need complex numbers

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rotations, ffts, waves, etc

sinful valve
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are you referring to quaternions

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in cg

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thats true tbf i havent done much on them but they seem like complex numbers

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more of an extension of them to more dimensions

lavish jewel
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i was talking more like rotations on a 2d plane, but sure

sinful valve
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we dont need complex numebrs for that i guess

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but it works either way of course

lavish jewel
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you don't need quaternions either, strictly speaking

sinful valve
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nah you dont

lavish jewel
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but using them makes the computations easier

sinful valve
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yeah its also gimbal lock or sumn

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but i dont knwo much bout that

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i just remember doing a non quat one you cant liek go all around without ebing cut off

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like you get locked you cant freely rotate

zinc timber
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yeah depending on the rotational system you use, it can happen

winged prairie
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hello, I was lloking at the solution for this problem but i do not understand how they can map some of the basis vectors to 0 because wouldn't that make the set of vectors that get mapped to w linearly dependent?

stable kindle
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wouldn't that make the set of vectors that get mapped to w linearly dependent?
why would it do that

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wait ok no i think i see

zinc timber
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you are looking at the finite version of the Hahn-Banach theorem

winged prairie
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but is my intuiton corect?

stable kindle
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i don't think it's quite correct

winged prairie
#

why

stable kindle
#

so why should it

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make them linearly dependent

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you can't map all the vectors that aren't in U to 0

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but you can map the basis vectors that aren't in U's basis to 0

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and then the remaining basis vectors, the basis vectors of U, determine the actual position of things

winged prairie
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my idea is that by doing the mapping shown in the picture

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u map over all the basis vectors of U + the 0 vector

zinc timber
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yr intuition is correct

winged prairie
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so why does that not make it linearly dependent

stable kindle
#

why would it make it linearly dependent

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also why is the 0 vector important

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you can get the 0 vector out of the basis vectors

winged prairie
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because any vector can be written as a linear combination of another

stable kindle
#

it's just the linear combination of all of them

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with coefficients 0

winged prairie
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oh is it by the theorem which says that if u have a set of vectors that span a vector space

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u can reduce it to a basis ?

stable kindle
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i mean

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what

winged prairie
#

if it has 0 it cannot be a basis

stable kindle
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ok so

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let v1, ..., vn be a basis

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then consider the list 0, v1, ..., vn

winged prairie
#

ye

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so..?

stable kindle
#

sorry back

winged prairie
#

dw

stable kindle
#

this list is linearly dependent because you can get a linear combination of those elements where not all the coefficients are 0, but they sum to 0

winged prairie
#

yes i agree

stable kindle
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ok

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so...

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you can just remove 0

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and then it's independent

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it's like

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why bother talking about 0

winged prairie
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and you can remove the 0

stable kindle
#

0 always goes to 0

winged prairie
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because of this

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right?

stable kindle
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and you can get it from the other elements

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sure

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so what

winged prairie
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i was just trying to understand

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that's all

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ty

stable kindle
#

??

winged prairie
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like u confirmed

stable kindle
#

ok if you got something from that that's good

winged prairie
#

ye

stable kindle
#

i don't know what's happening here lol

winged prairie
#

i was confused but now i get it

#

dw haha

#

i wanted to understand if removing the 0 was possible

zinc timber
hard drum
stable kindle
#

i don't understand

winged prairie
#

dw man

#

u helped me that is all

#

i will be back a lot these days

zinc timber
#

the heck q vegitable doing in liner algebra

#

@winged prairie also search Hahn-Banach theorem

#

for more info

winged prairie
#

ayt

#

ty

winged prairie
#

any hint on how to do this, i don't wannt look at the solution right away

hard drum
#

You can explicitly construct linearly independent vectors in L(v, w)

winged prairie
#

so i take a basis in V

#

then what

#

and map it to W

#

?

hard drum
#

I mean that's just a way to construct maps V to W so yes i guess

still lodge
#

whatd i do wrong here :(

#

probably something silly but i dont see it

dusky epoch
#

,w det {{1,-2,3,1},{0,2,4,-1},{2,0,1,2},{1,0,5,0}}

dusky epoch
#

,w det {{-2,3,1},{2,4,-1},{0,1,2}}

dusky epoch
#

,w det {{1,-2,1},{0,2,-1},{2,0,2}}

still lodge
#

🤦‍♂️

dusky epoch
#

oh i see where you went wrong

#

you forgot a minus sign

still lodge
#

i just copied a sign wrong

#

what if you wanted a 100 but your brain said (+)

zinc timber
#

u got a generous teacher ngl

still lodge
fresh canopy
#

I tried to use the Gramm Schmidt process to solve this problem, was that the correct approach?

zinc timber
#

can't read. what's the question?

keen flame
#

what would be the vector of function f(x)=cos(2x) when [-pi,pi]?

fresh canopy
#

Gimme a sec I'll just post a screen shot

fresh canopy
zinc timber
#

and u hv to use GS orthogonalization fr tht?

#

hint: ||extend the basis to a basis of R⁴ then apply GSO||

fresh canopy
#

Thats the section it's in, so that's my assumption

#

ok I know I'm showing my L.A. iq here, but what do you mean extend the basis to a basis of R^4?

zinc timber
#

extend (v1,v2) witch is a basis of W to a basis of R⁴

lavish jewel
#

take u and v and come up with 2 more vectors such that all 4 are lin indep, and therefore span R^4

zinc timber
#

there are easier methods however

#

like $ \mqty[u^T \ u^T]\mqty[a \b \c \d] = 0$

#

...

#

tf?

lavish jewel
#

you left a space after the first $

fresh canopy
zinc timber
#

apparently I wrote 2 u's

lavish jewel
zinc timber
lavish jewel
zinc timber
#

when I copied it only one \ was copied

fresh canopy
#

ahh, I didn't even think of that.

zinc timber
#

like wtf

quasi vale
#

Is it true for operators that (ST)^n = S^n T^n?

lavish jewel
#

an alternative is to build a matrix with u and v as rows, and find its null space

#

ah

#

that's what ryu was getting at

lavish jewel
#

only if they commute

quasi vale
#

what i currently have is $(T - \lambda I)^{n}$ and $(\lambda T)^{-n}$. Is it true that $(\lambda T)^{-n} (T - \lambda I)^{n} = ((\lambda T)^{-1} (T - \lambda I))^{n}$

stoic pythonBOT
quasi vale
#

You guys may answer Heathus first, I'm sorry to interrupt.

zinc timber
#

in this specific example it's true

quasi vale
#

Thanks!

fresh canopy
#

I'm going to find the null space given V and U are transposed, please feel free to help others while I work on this.

#

Then we can see what happens next! blobsweat

zinc timber
fresh canopy
#

ok good for my skill level that's the best choice 😉 Thank you

true girder
#

Hello I'm struggling a bit with homework problems involving eigenvalues and eigenvectors. I understand how to do the full problem conceptually like ik the steps but the part where u do det(A) = 0 and have to solve for 0 im really not getting anywhere.

#

the help channels appear to be only for pre-uni hw so this was my safest bet

zinc timber
#

post the question statement and your work

true girder
#

i skipped the first step of writing the question but the matrix is all 1's accept the diagonal is all 2's

zinc timber
#

so u r struggling finding the characteristic equation?

true girder
#

ye

#

my prof said to not multiply anything out but for everything after the 1st det its all single values

zinc timber
#

it's just routine calculation

true girder
#

ik but for some reason im struggling with this. like which route is best for solving it

#

is the very bottom correct?

zinc timber
#

,w char poly {{2,1,1},{1,2,1},{1,1,2}}

zinc timber
#

looks like you've messed something

true girder
#

ok the first part of line 2 is correct somewhere below it i missed something

fresh canopy
#

Looks like finding the null space of U^T and V^T was indeed the answer! Thank y'all so much.

#

My question is, how did we know that finding the null space of their transposes would be the orthogonal compliment of the those two vectors? Is that just always the case?

lavish jewel
#

the null space is by definition orthogonal to the row space of a matrix

#

this is because you can write matrix-vector multiplication as the result of taking dot products between a matrix's rows and another vector

#

say you have a matrix [u v]^T, where u and v are column vectors. this gives you a matrix that is size 2 x n

#

now multiply that by some vector x of size n x 1

#

the resulting vector is of size 2 x 1, and the elements of the vector are u^T x and v^T x

#

u^T x = u dot x

#

so if all the entries of the resulting vector are zero, the vectors that satisfy this are orthogonal to both u and v

#

furthermore, if these vectors are linearly independent from u and v (and they are, because they're orthogonal to them) you can use them to extend u and v into a basis of R^4

#

and now consider the subspace spanned by u and v, and the one spanned by the vectors you just found

#

any pair of vectors where one vector is taken from one subspace and the other, from the other subspace, are mutually orthogonal

fresh canopy
#

Thank you so much for breaking that down. That makes so much sense!

true girder
#

ok i figured out where i went wrong

#

but now i dont remember how to solve for x^3

#

ik the quadratic formula for x^2 and x^4

#

but this is where im gonna struggle

stable kindle
#

so for cubics you just want to stare at it until you find a solution

#

they won't give you a cubic with awful roots

#

in a question

#

so for example -1 should work here

true girder
#

i need a formula / system or ill be staring til im handed an F

stable kindle
#

-1

#

basically

#

you try 0, 1, -1, 2, -2, 3, -3

#

and if none of those work then you cry

lavish jewel
#

isn't it 1?

stable kindle
#

fuck

#

ok it's 1

lavish jewel
#

well idk if you meant the factor or the root tbf

#

but lambda = 1 should make the poly 0

#

you can go from there. maybe divide the poly and then use the quadratic formula if needed

true girder
#

this video looks good

#

ye my math brain died in high school so now im just praying that i pass any required math for my major

#

but thx for the help!

#

ok so i played with it and the video did not help at all.

#

but ye 1 works

#

but how do i get the rest

#

there arent any like terms and all i can really do is factor out a lambda

#

ok so the only thing i noticed from just finding the answer online is that since the answer contains a (x-4).... one of the factors is actually 4 so maybe thats a hint

quaint steppe
#

Practicing some exercise in the book. Is my proof correct? Is there a better proof?

sick sandal
# quaint steppe

can you elaborate further on your 1st proof im not sure i follow what you did,
as to how i would do it ||probably prove injectivity by assuming ST(u1)=ST(u2) and reach u1=u2 since injectivity is equivalent to invertiblility in finite dimensional spaces for some transformation(if dimemsions are equal for U and W )||

quaint steppe
#

Idk if it's the right track.

reef latch
#

doesnt invertibility require bijection

wintry steppe
wintry steppe
#

you need to elaborate

#

this proves both parts anyways, btw

steel moon
#

how would i go about creating a subspace in a?

wintry steppe
#

visualize it :^)

steel moon
#

we want to show every vector in R^4 can be written as a sum of an element in W and some subspace

#

how can you visualize R^4 thinkies

wintry steppe
#

it might help to consider a hyperplane in R^3 first, where you can argue geometrically. then, see if you can transfer your reasoning over to a hyperplane in R^4

reef latch
#

3blue1brown

steel moon
#

😹

stable kindle
reef latch
sinful valve
#

you know if i had a shape like on a graph right

#

with the original F already there

#

so i know the coordinates of start and end

#

how would i calculate transformation matrix to get there

reef latch
#

get the basis vectors?

sinful valve
#

i only have the coordinates of each vertex by the looks

#

vertices

reef latch
#

which vertices are that

#

basically you can construct basis vectors by drawing them on top of the F

sinful valve
#

[9.812, 10.1963302752294, 14.1855010660981, 13.4, 10.8298217179903, 10.6398305084746, 12.0611940298507, 11.7371879106439, 10.4931163954944, 10.2813455657492, 9.812],
[5.649, 8.39266055045871, 7.79957356076759, 6.91607142857143, 7.39059967585089, 6.74435028248588, 6.44328358208955, 5.95532194480946, 6.24530663329161, 5.5249745158002, 5.649]

#

you see the issue xd

reef latch
#

right so get the bottom left vertex, get the bottom right

sinful valve
#

can i like plug these into a linear equation though

#

these are just x, y pairing first array is x second is y

reef latch
#

subtract bottom right from bottom left, theres your horizontal basis

sinful valve
#

these 2 you mean

quaint steppe
sinful valve
#

in my book it says you can just line up the coordinates in an equation though will that not work

reef latch
sinful valve
#

so i think my x and y of the transformed shape are joined on right

reef latch
#

thats weird, whats with the big matrix

#

I guess I'm not familiar with whatever this is :)

sinful valve
reef latch
#

oh wait, it's a transformation that includes translations?

sinful valve
#

it includes anything

#

shears /rotations

reef latch
#

I see

sinful valve
#

so in that recent slide they have the column with some single vertex

#

on LHS with the trasnformed point

#

and they are solving teh matrix to get to it i think

#

where the matrix is the unknowns

#

in my example i think i would just have a fat column vector

reef latch
#

I guess the thing with the basis vectors wont work then

sinful valve
#

with [x1,y1, x2, y2...., xn, yn]

#

ill see if there is an online tool to solve this exact issue

reef latch
#

hmm, I feel like 3 points should be enough to characterize any affine transformation

still lodge
#

are there any named theorems besides cayley hamilton that i should know as an undergrad

reef latch
#

I hear Pythagoras Theorem is all the rage

sinful valve
#

3 points how though

#

it may be a homography acc my bad

reef latch
#

well just think about it

#

like, idk, put three points on a graph

sinful valve
#

yeah ofc only 3 for affine tbf true true

#

dunno why i said not

reef latch
#

2 is enough for linear transform

sinful valve
#

so i dont need to pass all my vertices in

#

i can just solve teh matrix from one

reef latch
#

but like, you need to distinguish between a translation and a series of linear transforms

#

hence the third point

sinful valve
#

yeah I get that

#

uh just need to find out how to compute these things

#

by that then are you saying from my F

#

I need to get any 3 points of x and y

reef latch
#

probably!

sinful valve
#

to solve the affine matrix

#

ight ill see

winter harbor
#

Stuff you need to know (In my opinion)

Cayley-Hamilton Theorem

Steinitz Exchange Lemma and the Dimension Theorem (Existence of a basis and Uniqueness of dimension)

Spectral Theorem for Normal Operators (and its corollaries such as Spectral Theorem for Hermitian (Self-Adjoint) and real symmetric operators).

Rank-Nullity Theorem (First Isomorphism Theorem)

Lémme de Noyaux (a.k.a primary decomposition theorem)

Jordan Canonical Form Decomposition

Jordan-Chevalley Decomposition

Schur's Theorem (Schur's Decomposition)

SVD decomposition theorem

Rational Canonical Form and Smith Normal Form (maybe?)

Cholesky decomposition theorem

Cayley-Hamilton's Theorem

Stuff you maybe need to know (I guess).

Gershgorin Circle Theorem

Sylvester's Law of Inertia

Spectral Mapping Theorem

Witt's Extension Theorem and Witt's Decomposition Theorem

Hadamard's Inequality

Cartan-Dieudonné theorem

#

Idk, these are prolly all the linear algebra theorems I know that have a name I guess.

#

The "stuff you need to know" is prolly shit people go through in most intro to linear algebra classes I guess.

quaint steppe
#

I'm sorry if I'm constantly asking if my proof is correct. I don't have anyone to ask to. And i don't have a solution manual to check. So yeah Is my proof on this exercise correct?

#

I'm an undergrad and really new to college maths

winter harbor
#

This is not right

#

I wi give you a hint

#

Since dim(V) > 1

fresh canopy
#

So for this problem, I know I can just set up "Ax=b" and multiply the right vector by the inverse to solve for "x", which would be the coordinates being requested. But is that the ideal way to solve it? Should i be using QR factorization for this problem?

winter harbor
#

Choose a basis $e_{1}, \cdots, e_{n} \in V$ of $V$ and let $T,U \in \mathcal{L}(V)$ be such that:
\begin{align*}
T(e_{1}) = 1
\
\
T(e_{i}) = 0 ; \forall i > 1
\end{align*}
and
\begin{align*}
U(e_{1}) = 0
\
\
U(e_{i}) = 1 ; \forall i > 1
\end{align*}
Then, notice that
$$
(T+U)(e_{i}) = 1 ; \forall i \geq 1
$$
And thus, $T+U = \text{Id}_{V}$ is the Identity on $V$, which is invertible.
\
\
Therefore, we have that the set of non invertible operators is not closed under addition and as such is not a subspace of $\mathcal{L}(V)$.

#

Notice that we are explicitly using the fact that dim(V) > 1 here in order to construct T and V.

#

Moreover

#

You can fill in the details yourself if you want

#

But T and U are well defined

#

Because we especified how the act on a basis of V

#

And we can use this to extend T and U to to whole of V by linearity like this.

#

And uniquely as such

#

I should be more precise on why your argument does not apply.

#

It is NOT true that every linear operator T : V -> V between finite dimensional vector spaces is invertible.

#

You could take, for example, the 0 linear operator.

#

But that are more interesting examples

#

Such as the ones I have constructed.

#

Nilpotent operators are another important class of operators which are not invertible.

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

What is true tho

winter harbor
#

That's what I was about to say

#

As a consequence of the rank-nullity theorem

#

If an operator T : V -> V is injective, then it is invertible.

#

Or if it is surjective, then it is invertible.

#

But not every linear operator between finite dimensional vector spaces satisfy these criteria.

#

For example, 0 : V -> V which takes a vector v in V and does 0(v) = 0 is not injective nor surjective.

quaint steppe
#

thank you very much

#

im taking notes

vital pagoda
#

one of the things which define a normed space is that $| x | = 0 \iff x = 0$ where $x \in X$ where $X$ is a vector space

#

but i dont understand why that's needed

#

is there an example of something which satisfies the other two norm axioms but doesn't satisfy this one?

stoic pythonBOT
winter harbor
#

Yup, there are.

vital pagoda
#

isn't it obvious from the definition of the modulus that this will be the case though?

gray dust
#

take the constant 0 map

still lodge
#

random unrelated interjection - i asked about the studying role before but what is/how do i get permastudying (i saw it on system)

gray dust
#

ask for it. want it now?

vital pagoda
#

smh

#

ok yeah the constant 0 map does indeed satisfy the other two while violating positive definiteness

#

im still not fully comfortable with the idea of a norm tbh, does it get more natural once you learn topology?

winter harbor
#

Let $(X, \mathcal{B}, \mu)$ be a measure space, where $X$ is a set, $\mathcal{B}$ is a sigma algebra on $X$ and $\mu : \mathcal{B} \rightarrow \mathbb{R}{\geq 0} \cup {+ \infty}$ is a measure on $X$.
\
\
Let $1 \leq p < + \infty$. We define the real vector space:
$$
L^{p}(\mu) = \left{f : X \rightarrow \mathbb{R} : \int\limits
{X} |f|^{p} , d \mu < + \infty \right}
$$
We can prove that for any $f \in L^{p}(\mu)$ we have that the function defined as:
$$
|f |{L^{p}} := \left(\int\limits{X} |f|^{p} , d \mu \right)^{\dfrac{1}{p}}
$$
Satisfies all the other product of a norm. I.e, the triangle inequality (here known as Minkowski inequality). It is positive homogeneous and we have that $| f |{L^{p}} \geq 0$ for every $L^{p}$ function.
\
\
But, we have function with $|f |
{L^{p}} = 0$, but $f \neq 0$. Basically, if $f$ is 0 almost everywhere (i.e 0 everywhere up to a set of null measure), then $|f|_{L^{p}} = 0$ even if $f \neq 0$.

#

Oof

vital pagoda
#

damn yeah buddy I'm still a few months away from learning about measure spaces

winter harbor
#

This example comes from functional analysis.

#

Yeah

#

I couldn't think of a good example on finite dimensional vector spaces

#

The 0 one is prolly the easiest

stoic pythonBOT
#

MISTERSYSTEM

vital pagoda
#

whats interesting is that what inspired my question is the proofwiki proof of the p norm on the p sequence space being a vector space norm

winter harbor
#

Ohhh

#

Well

#

That's actually weird

vital pagoda
#

ahahahaha

winter harbor
#

Btw

#

This is called a pseudo-norm

vital pagoda
#

bruh just when i thought the rabbit hole doesnt get any deeper

winter harbor
#

I can't think of any non zero pseudo norm which is not a norm.

#

Btw

#

The thing with L^p spaces is that we usually identity functions that agree almost everywhere.

vital pagoda
#

yeah i looked at the definition of the pseudo norm and immediately II . II_0 popped in my mind

stable kindle
#

proofwiki is kinda weird

winter harbor
#

So that we in fact have a norm.

#

And not a pseudonorm

#

This is usually a technical detail

lofty topaz
#

is this a vector subspace ?

still lodge
#

what are the requirements for something to be a subspace

lofty topaz
#

1 include zero vector
2 closure under vector addition

#

3 closure under scalar multiplicatioon

stable kindle
#

stupid q

#

aren't 2 and 3 sufficient to give 1

#

0 is a scalar

#

am i wrong?

winter harbor
#

These 3 conditions are equivalent to

1 it is a non empty subset
2 closure under vector addition
3 closure under scalar multiplication

still lodge
#

i mean youre right but no need to be condescending, it can be helpful to check if 0 vector is included as a way to eliminate the other 2 sometimes

winter harbor
#

We need the subset to be NON EMPTY in order for it to be a subspace.

stable kindle
#

no i was saying i was about to ask a stupid question

#

i wasn't saying your q was stupid

still lodge
#

oh

winter harbor
#

The empty set satisfies the axioms 2 and 3

#

But not 1

stable kindle
#

right

still lodge
#

then yeah

lofty topaz
still lodge
#

i mean you seem to have two sets there

#

so it depends on the particular instructions...?

lofty topaz
#

I need to prove for every set if it is a subspace

reef latch
#

iirc a subspace is closed under linear transformation

sinful valve
#

i dont think the method is working tbf

#

this one i solved the values

#

but somethign is off

#

im not even sure if this is even possible

nocturne jewel
#

to which similar properties are linearity

sinful valve
#

is there any other way to find the parameters of an affine trasnformation

#

given the start and end shape

#

like we have this F right and i computed the transformation for a using that method

#

but the matrix didnt move it correctly not sure why

#

what is the standard method of getting the affine matrix uesd in a transformation

glad acorn
#

I have no idea how to work on this question

reef latch
#

seems like it should be orthogonal to the other two basis vectors

stable kindle
#

this seems false

#

let a basis for V be v1, ..., vn

#

oh wait no it works

glad acorn
tribal fossil
#

-> Prove that every m × n matrix over the field F is row-equivalent to a row-reduced matrix.
-> Let e be an elementary row operation and I be the m × m identity matrix. Prove that for every m × n matrix A, e(I)A = e(A).

Hey someone help me prove these two theorems??? pls

still lodge
#

can someone help me understand why a matrix (let's say B = {1 1}{0 1}) acts as a change of basis from B to E where E is the standard basis pls

#

ive been trying to get this into my head since fucking freshman year and it still doesnt click

#

just a discussion would be v nice

zinc timber
#

@glad acorn has it been resolved?

still lodge
#

yeah i was gonna say, isnt that like... the definition of those things...?

tribal fossil
#

i mean my teacher asked for a neat proof

zinc timber
#

given a matrix, u apply row operations blah blah and u get a row reduced matrix

#

so original matrix~the row reduced matrix we have just calculated

still lodge
#

ig you could do some visual stuff?

zinc timber
#

do I need to?

still lodge
zinc timber
#

I would have but I'm on my phone now, hard to type, I'll try once I get back to my pc

still lodge
#

<3

#

any chance on an ETA? i'll be here for a while but will probably close discord for a while

zinc timber
#

ok i'll whatever I can for now

#

say in 2D you have 2 LI vectors (1, 1) and (1,0). say I want to use them as my new coordinate vector. so any (x,y) vector in 2D can be written as a•v1+b•v2

#

i.e. the vectors (1,0) and (0,1) which was our old basis can be represented in terms of the new basis v1, v2

#

so let the the new coordinates of e1, e2 be

$a v_1 + b v_2 = e_1 \
c v_1 + d v_2 =e_2$

stoic pythonBOT
#

Ryuzaki

zinc timber
#

Now this can be written in the compact form
$\mqty(v_1 & v_2 ) \mqty(a & b \ c & d) =\mqty( \imat{2})$

stoic pythonBOT
#

Ryuzaki

zinc timber
#

now you can solve for a,b,c,d with it

#

similarly given we know the coordinate wrt one basis we can transform them into another just by multiplying the inverse of the basis transformation matrix

still lodge
#

so ig it's bc of how that matrix of the new basis vectors (or rather each basis vector) acts upon our basis E...?

quaint steppe
#

Hi again, practicing another exercise in the textbook. Is my proof correct? Can it be proved better?

zinc timber
#

no

#

you are supposed to show a invertible lt exists given S is injective

#

but here u assumed the existence

quaint steppe
#

all rightt

zinc timber
#

hint: || extend to a basis ||

teal grotto
# quaint steppe

if S is injective, then take a basis {u1,…,uk} of U. then extend this to a basis {u1,…,uk,v1,…,vr} of V (where of course k = dim U and k + r = dim V). try to define a new function T determined solely by the new basis of V

quaint steppe
viscid lily
#

I have constructed the matrix with importance scores, but dont know how to solve to get the page rankings

#

Can anyone guide me?

zinc timber
cobalt tartan
#

Wanted to doubel check something: Given an arbitrary inner product, does that change how matrix mulitplication works? I.e, say that my inner product is <u, v>, then is matrix multiplication now applying <u, v>, or is it still applying the "standard" dot product?

zinc timber
#

didn't understand what your question is exactly

cobalt tartan
#

So say that you define an inner product over R3, $<x, y> = x_1y_1 + 2x_2y_2 + 4x_3y_3$

stoic pythonBOT
#

Liria ^(;,;)^

zinc timber
#

so you mean a inner product induced by a matrix?

#

like $\innerproduct{u}{v} = v^TQu$

stoic pythonBOT
#

Ryuzaki

cobalt tartan
#

Then normally, when you do matrix multiplication of $AB$, you're applying the standard dot product between the rows of $A$ and the columns of $B$

stoic pythonBOT
#

Liria ^(;,;)^

zinc timber
#

for that you must have a positive definite matrix Q

cobalt tartan
#

Then in this IPS over $R^3$, when we multiply $A$ and $B$, do we apply the standard dot product, or do we apply this inner product?

stoic pythonBOT
#

Liria ^(;,;)^

cobalt tartan
#

As this is the definition of inner product in my textbook

zinc timber
#

actually no, matrix multiplication is universal

nocturne jewel
#

IP acts on the vectors, so idk why you're worried about its effect on matrices

#

when matrices arent the vectors

cobalt tartan
#

Ok, so it just follows standard matrix multiplication

#

Ok

lavish jewel
#

probably cuz they noted the result of matrix mult is an array of dot products

cobalt tartan
#

Yea

lavish jewel
#

but when you need to interpret it as such, it'll be apparent

cobalt tartan
#

And so matrix multiplication, even though it looks like a series of dot products, isn't really so?

lavish jewel
#

it won't just be the composition of 2 linear transformations, but explicitly written as a matrix whose elements are inner products

zinc timber
#

it's a composition of LT's (in their matrix form). The basis is already taken into account in the matrix representation so you don't need to apply it again while multiplying

cobalt tartan
#

ok

lavish jewel
#

for a nice symmetric pos semi def matrix M, if you want to compose something whose elements are inner products w.r.t. that matrix, you'd get a matrix whose elements are of the form u^T M v, and then you could factor it as U^T M V or something

#

but then that no longer has the interpretation of composition of linear transformations

#

so, not a "matrix" in the usual sense

zinc timber
#

yeah but when you try to multiply with the adjoint, then it'll be different. but I'll not go into the rabbit hole for now

wintry steppe
cobalt tartan
#

Some prof at my school wrote a textbook specifically for our linear algebra courses

wintry steppe
#

I see thanks.

keen mirage
#

help

#

how do i show dim(S(V))=n+n(n-1)/2

#

<@&286206848099549185>

zinc timber
#

For a symmetric bilinear form (which is a symmetric matrix) we must have $a_{ij} = a_{ji}$ given $i\neq j$

stoic pythonBOT
#

Ryuzaki

zinc timber
#

means you are only free to choose arbitrary value for matrix where j>= i

keen mirage
#

ahhh yeah

zinc timber
#

that answers your question?

still lodge
#

is it accurate to say that the alg multiplicity of an eigenvalue is the degree of the part of the polynomial in which said lambda sits (ik this is worded weird) and the geometric multiplicity is how many vectors make up it's nullspace..?

keen mirage
#

symmetric bilinear form correspond to symmetric matrix

zinc timber
still lodge
#

i can do problems with it i just wanna make sure the wording in my head is right so merci

#

*or at least the idea behind it

#

and a matrix is defective is the alg multiplicity of any of its eigenvalues is greater than the corresponding geometric multiplicity

zinc timber
#

If
\begin{align}
p(\lambda) = (\lambda-\alpha_1)^{k_1}(\lambda-\alpha_2)^{k_2}\cdots(\lambda-\alpha_n)^{k_n}
\end{align}
then $k_i$ is the algebraic multiplicity of the eigen value $\alpha_k$ and the geometric multiplicity is $\dim \text{ null } (T-\lambda_iI)$

stoic pythonBOT
#

Ryuzaki

still lodge
#

yep that is what i meant, epic

#

is there a faster way to do this than rational root thm

#

that's easy enough to apply but tedious ofc

zinc timber
#

yes

#

,w roots x^3-10x^2+33x-36

zinc timber
stable kindle
#

yeah i was thinking 3 from the start

still lodge
#

yeah i'll just pull out WA on my exam no biggie

stable kindle
#

just stare at it until you see something that looks good

zinc timber
#

,w formula for cubic equation

stable kindle
#

god that looks like shit wtf

still lodge
#

because it is shit

zinc timber
#

lol

stable kindle
#

no like even shittier than usual

#

anyway here's how you actually solve cubics

#

basically

#

try 0, 1, -1, 2, -2, 3, -3

#

and if none of them work then you're doomed

still lodge
#

yall got any way to intuit how many roots it might have

zinc timber
#

= degree

stable kindle
#

it will always have at least one root of the form 0, 1, -1, 2, -2, 3, -3, by Kai's Conjecture

#

then just do the long division trivially

#

and you can tell pretty easily if it'll have more

still lodge
#

bleh fine

quaint steppe
#

What does this fancy R means?

zinc timber
#

range of T2

quaint steppe
#

all right thank you

still lodge
#

ive asked this before but... what's the dif between invariant factors and elementary divisors

#

ik the latter depends on our choice of minimal polynomial

#

are invariant factors just each distinct elementary divisor of every possible minimal polynomial (in cases where you dont know the minimal polynomial ofc)

granite kraken
#

I solved this question using adjunct matrices but my professor said to solve it without using adjunct matrices. Does anyone see a possible solutions start or tips to this problem?

lavish jewel
#

if A is diagonalizable, the matrix exponentiation is pretty simple, one need only exponentiate the diagonal matrix of eigenvalues

#

then you can factor out the matrices of eigenvectors to the left and right, leaving you with a sum of diagonal matrices of the form of the polynomial

ionic laurel
#

Hi I have a question

#

If you have two bases B and C

#

would the change of coordinates matrix from B to C be the inverse of C to B and vise versa?

#

B to C is the inverse of C to B
C to B is the inverse of B to C

lavish jewel
#

yes

ionic laurel
#

👍

#

My professor wrote it as

lavish jewel
#

in general, you put the basis vectors as columns of a matrix M

ionic laurel
#

the inverse of B to C is is C to B

#

but I did not know if the converse would be true

#

thank you nonetheless

lavish jewel
#

then if x are the coordinates in that basis, we have that v = Mx, so that v has coordinates x in the basis M

#

if you do it backwards, then you get that M^-1 v = x, and now v is the coordinate vector for x in the basis of the columns of M^-1

raven parrot
#

Is there an easy way to LU Factorize a nxm matrix? The method I know and use is to RREF to get U, but in the process, get values for L.

lavish jewel
#

by hand, that's about the easiest

swift minnow
#

Hi i need help

If A,B are squared matrix, and AxB is unsymmetrical so A and B are transposed

marble lance
#

To disprove it, you just need to give a counterexample

swift minnow
#

do you have any example? i have tried

#

i didn't find any

#

is it a proof or disproof

marble lance
#

@swift minnow Sure

#

Consider any symmetric matrix

#

Then take one of the entries not on the diagonal

#

And +1 to it

#

And then take the same entry and -1 to it

#

The two matrices you get won't be symmetric

#

But their sum will be

mystic dagger
#

is this conclusion right?

#

like, h(x)=-h(x) breaks the definition of function right

stable kindle
#

let h(x) = 0

mystic dagger
#

it would be the x-axis right?

#

and the only function that obeys h(x)=-h(x)

#

yes bc 0=-0

#

oh i got it

#

thank u

swift minnow
marble lance
#

I told you how to construct an example just now

swift minnow
#

so is it a disprove?

marble lance
#

Create an example the way I said

#

Then that serves as a counterexample, yes

swift minnow
#

i typed the wrong question

marble lance
#

Is the new question: If A and B are square matrices such that AB is not symmetric, then A = B^T?

#

Or what do you mean by A and B are transposed?

#

I don't get it

swift minnow
#

it means that a x b = b x a

#

that's what i mean by transposed

#

a x b = anti symmetric

marble lance
#

I don't think you are using terminology correctly

#

Can you send a screenshot of your actual question?

swift minnow
#

Ye thing is that’s in a different language 😅

wintry steppe
granite kraken
#

Anyone got any clue how to start this problem,

zinc timber
#

let p=algebraic multiplicity of the eigen value

finite plume
#

Where have I done wrong? The correct answer is sqrt(186)/2.

dusky epoch
#

your P1P2 and P1P3 are wrong

#

they should be (3, -1, 5) and (-1, 0, 4)

finite plume
#

Wouldnt it be (2, -1, 5) then? On P1P2.

dusky epoch
#

oh oops, typo on my end

#

you're right

granite kraken
dim epoch
#

ryuzaki gave you a hint

umbral void
#

If I have an $n\times n$-matrix with integers on the diagonal and 1s on the "immediate parallels" of the diagonal, can I say something about its signature?
To be more precise, I mean matrices like
[ \begin{pmatrix} a_1 & 1 & 0 \ 1 & a_2 & 1 \ 0 & 1 & a_3 \end{pmatrix} ]
and by signature, I mean $#$ positive eigenvalues $- #$ negative eigenvalues

stoic pythonBOT
#

expectTheUnexpected

umbral void
#

i.e. this

zinc timber
#

can immediately think of Gresgorion thm, other than that, I'll have to think

winter harbor
#

You mean Gershgorin Circle Theorem? stare

zinc timber
#

there's also one convoluted method usigng strum sequence

umbral void
#

Ok, I guess I'll just not write a general formula then opencry would have been nice, but I suspect that it's hard

zinc timber
#

If you wanna know I can just give a ss of the theorem

#

all yr b_i will be 1

umbral void
#

oh no, recursion

zinc timber
umbral void
#

was to be expeceted

zinc timber
#

then you can put v=0 and check for sign changes

umbral void
#

oof, gotta think

#

thank 👍

zinc timber
#

I'wd like to know anything better myself