#linear-algebra

2 messages · Page 159 of 1

nocturne jewel
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yeah, bases are independent vectors

hollow finch
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you were given two of linearly independent columns of A. since A has rank 2 (because you were told it has a 2 dimensional column space) we know that all the other columns are just linear combinations of the ones you were given (meaning they span). since they're linearly independent and span, they form a basis.

nocturne jewel
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Ok so the answer isnt whether b is in Col(A)?

hollow finch
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you could also look at it as if we make the matrix C with the two columns you were given, the system Cx=b has only one solution since it doesnt have a null space (they are linearly independent)

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its a two part thing

nocturne jewel
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wait so is it inf or 1 solution?

hollow finch
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we know there is at least one solutions because b is on Col(A)

nocturne jewel
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You said infinite and only 1 confusion

hollow finch
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we know there are infinitely many because Null(A) is not just the zero vector

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wdym

nocturne jewel
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but with null(A) logic there are infinite

hollow finch
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yeah if we only consider the two columns you were given

nocturne jewel
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Ok so Ax=[5,7,-2]^T has inf solution?

hollow finch
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we know there is at least one solutions because b is on Col(A)
we know there are infinitely many because Null(A) is not just the zero vector

nocturne jewel
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ok so infinite

fringe matrix
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what is the name of a Matrix such that

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M^2 = M?

slow scroll
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idempotent

fringe matrix
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ty! 🙂

slow scroll
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or... maybe a projection in this context

fringe matrix
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lol that was exacly what i wanted

slow scroll
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projection or idempotent?

fringe matrix
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projection is a type of idempotent ^_^

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i was looking at projection and wanted to give it another name

slow scroll
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ah okay

native rampart
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Well,All idempotents are projections

fringe matrix
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in matrixes yea..

slow scroll
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Well,All idempotents are projections
idk if i would call an idempotent matrix a "projection" outside the context of inner product spaces tho

brittle juniper
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When I was being taught linear algebra for the first time, it went like

an endomorphism p on a vector space E is called
• a projection when E=Ker(p)⊕Im(p) and the restriction of p on Im(p) is the identity
• a projector when p²=p
(maybe it was the other way around)

and the important result was that projections are projectors and projectors are projections (and that's why I don't remember which one was which)

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the prehilbert-specific stuff was introduced a lot later

a projection p on a prehilbert space E is said to be orthogonal when the direct sum E=Ker(p)⊕Im(p) is orthogonal

thorny hemlock
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not really sure how this is done

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rangeT = {Tv1 ... Tv_n}

soft burrow
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maybe you could suppose that under some pair of bases, the matrix has exactly dim(range T)-1 non zero entries and derive a contradiction?

thorny hemlock
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hm

soft burrow
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in the best possible case you'd have some diagonal matrix with dim(range T)-1 non-zero entries and that should contradict the given value of dim(range T)

thorny hemlock
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er

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so

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each Tv1 ... Tv_n corresponds to an entry in the matrix

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so we get dimrangeT-1 = dimrangeT ?

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but er

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how does that contradiction work

neat relic
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Hey guys, not sure if this belongs here but I've been asked to do a linear algebra online certification as proof of competence before taking on certain projects at a job..was wondering if do you guys have any in depth linear algebra certification you'd recommend pls? There's like so many it's tough to choose haha..

wintry steppe
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are there any topics of linear algebra that you know you'll need in particular?

neat relic
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ahh I don't know lol..it's to do with robotics and some machine vision so probably linear algebra topics to do with that..I think he wants proof of competence that I know linear algebra basically..

I guess personally I'm looking for like if it covers subspaces, row echelon, basis, dimension, nullspace, linear independence, eigenvalues eigenvectors, and the tougher stuff like orthonormal orthogonal gram schmidt etc..

tame mural
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I never heard of a lienar algebra cert

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that sounds so specific

neat relic
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I guess kinda online course certification

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that they want to show that I know linear algebra

round coral
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@neat relic you mean a certificate course in linear algebra, am I right ?

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you can look over edx or coursera courses on linear algebra, choose what is best for you

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these give certificates of the universities they are being offered by, but are not credit eligible mostly, don't have any exams, just graded quizzes

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i guess they may be useful for you

hollow finch
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My LA class never touched on generalized eigenvectors so I'm hoping someone can help answer some questions I have about them.

  1. How unique are they? I know eigenvectors in general are not unique because you can scale them, but from just messing around with GEs it seems adding any scalar multiple of the ordinary eigenvector(s) has no effect on whether or not it's a GE.
  2. What would be the proper way to "introduce" them in a proof? Like if I have a general nondiagonalizable 2x2 matrix A with eigenvector v and generalized eigenvector w what is the formal way to state that?
    and if anyone has any good resources I could look into to understand them better that would be appreciated. The wikipedia page is a bit difficult to understand for me.
limpid fiber
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why is f(x) = x + 4 non-linear

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I've seen the proof, but intuitively it feels like a linear function

wintry steppe
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it's "highschool linear"

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that kinda function would be called affine, usually

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linear function plus a constant

round coral
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@hollow finch I think these questions will be easily resolved when you study some more about generalized eignevectors, I would recommend , you can read either Chapter 8 of Axler, he covers all about generalized eigenvectors, decomposition theorem etc. in great detail , chapter 7 of Friedberg Insel Spence also covers this in a good way , you can choose any one you like .

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hope it helps

hollow finch
wintry steppe
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your next la class is whenever you next open a linear algebra book realshit

limpid fiber
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Yeah it's highschool linear lol
thank you

limpid fiber
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@wintry steppe if it were a line through the origin, that would be enough right?

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Is that a consequence or a condition

round coral
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if your given map, maps 0 to 0 , then it is not necessary that it's linear but if it is linear then for sure by linearity 0 will be mapped to 0

limpid fiber
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I guess it's a consequence of scalar multiplication then

stoic pythonBOT
limpid fiber
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nice, thank you

nocturne jewel
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bit bold to assume 0+0=0 \j

wintry steppe
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linear functions........ hyperthonk

thorny hemlock
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if $v1,...,vm$ is a basis of V. we know there exists $T(a_1v_1 + .... + a_mv_m) = c_1v_1 + ... + c_mv_m$. Setting all scalars to zero we can get a specific vector so$ T(a_jv_j) = c_jw_j \rightarrow Tv_j = \frac{c_j}{a_j}v_j$

stoic pythonBOT
thorny hemlock
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does this answer the question?

wintry steppe
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"there exists (equation)" what do you mean by this? what are these scalars? why are you setting these scalars to zero?

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why are you writing your basis as v1, ..., vm when the space is 1-dimensional

thorny hemlock
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lmao

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idk

wintry steppe
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you should start the problem by saying "let {v} be a basis for V"

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then what can you say?

thorny hemlock
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V = span(v) -> for all u in V, u = av for some a in F

wintry steppe
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yes

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(to be nitpicky, you mean for some a in F)

thorny hemlock
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ok

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we then make use of this ?

wintry steppe
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i guess you can do it using that, yeah

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probably not the easiest way to do it

thorny hemlock
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oh

wintry steppe
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but hey it could probably work out catshrug

thorny hemlock
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how would you do it

wintry steppe
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well you have a basis {v} of V

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meaning any element of V is a scalar multiple of v

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in particular, T(v) is

thorny hemlock
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hm that works

wintry steppe
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why?

thorny hemlock
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basis' can span, T(v) is another something in V

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av = anything in V

wintry steppe
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you should write a full proof catThink

thorny hemlock
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i dont know how

wintry steppe
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think about the problem some more then

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remember you ultimately want to show that T equals scalar multiplication by some scalar (one you need to come up with!)

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starting from a basis of V is how you find that scalar

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i gave a big hint catThimc

thorny hemlock
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ok

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isnt it what i wrote tho

wintry steppe
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at the start?

thorny hemlock
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yah

wintry steppe
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i don't understand it, i think it needs to be fleshed out a bit

thorny hemlock
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jjust change the basis to just v1

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oh ok

blissful pagoda
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This matrix is singular because I found its determinant to be 0

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Homogeneous systems all have the trivial solution

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If it is singular, then it cannot have unique nontrivial solutions

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Therefore it has no solutions or infinitely many solutions. The number of equations and unknowns are the same. So I say it has no solutions.

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Turns out it has infinitely many solutions, how is that? (part b)

wintry steppe
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the set of solutions to the system is the kernel of A. since A is singular, its kernel is nontrivial, thus infinite

blissful pagoda
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Wouldn't that imply then that all singular matrices have nontrivial kernels and therefore all singular matrices have infinitely many solutions?

wintry steppe
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all singular matrices have nontrivial kernels
this is true (and conversely for square matrices)

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an nxn homogeneous linear system of equations Ax = 0 has a unique solution (zero) if and only if the matrix A is nonsingular, and on the other hand, has infinitely many solutions if and only if A is nonsingular. if the system is not homogeneous, then you can't say for certain whether or not there are solutions

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in a nonhomogeneous nxn system Ax = b, you will have infinitely many solutions if you have one (b/c ker A is nontrivial)

neat relic
blissful pagoda
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Wait... so if I have a singular matrix (by finding determinant = 0), it will always have infinitely many solutions and never no solution?

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(other than the trivial solution of course)

acoustic path
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yep

blissful pagoda
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Oh I did not know that. I was under the impression that if a matrix was nonsingular then it had one single unique solution. And if it was singular and if it had more variables than equations then it was infinite, else no solutions. So this is wrong?

acoustic path
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no it can have no solutions

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or infinite, it depends on the singular matrix

blissful pagoda
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How can you tell

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[4:06 PM] gotta go fast: Wait... so if I have a singular matrix (by finding determinant = 0), it will always have infinitely many solutions and never no solution?

acoustic path
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ye i didnt read that first my bad

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and wym how can you tell

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just how a normal matrix can have zero, one or inf solutions, a singular matrix has zero or infinite, never one

blissful pagoda
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I thought a nonsingular matrix can't have zero or infinite solutions 🤔

pure tangle
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Can someone please help me understand why using linear combinations to find variables works? The proof I'm looking at says to think of it like a weighted average which kind of makes sense, but I'm having trouble verbalizing why if we have a weighted average, the point that the two equations intersect at will always be crossed by the equation of the weighted average

smoky crystal
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@pure tangle can you elaborate on the find variable works part? maybe an example

pure tangle
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@smoky crystal thanks for the response. Is it alright if i post a link to their explanation?

smoky crystal
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im not sure but u can dm me

pure tangle
smoky crystal
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what will be the weight average at the point (x1,y1) where it intersects?

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well it will be exactly (x1,y1)

pure tangle
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thanks so much for the response. so that's the paragraph i've been reading over and over and I'm still having trouble understanding

smoky crystal
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think of it like this, let (x1,y1) , (x2,y2) be any points on the two lines respectively, if they intersect, then we must have (x1,y1)=(x2,y2) or x1=x2 y1=y2. Now if we take their weight average for the two lines, what will happen to the weighted value at the intersection?

pure tangle
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does it not change?

smoky crystal
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nope, it will not change

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lets go the easy way and talk about average instead of weighted avg

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that'll be easier to think of

pure tangle
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thanks for being patient with me. I'm still having trouble understanding why that is

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sounds good

smoky crystal
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now, if you have x1=x2, y1=y2, say pick any points ,eg let x1=x2=4 and y1=y2=6

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well the avg for x's will be (x1+x2)/2 correct?

pure tangle
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yes

smoky crystal
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and same goes with y's

pure tangle
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yes

smoky crystal
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well plug in the values we have for x's and y's,

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so we have (4+4)/2 for x and (6+6)/2 for y

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now our average x, y . wouldnt you agree that its the same as the old one?

pure tangle
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oh so if they're equal they're not going change after averaging out our line equations

smoky crystal
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yep

pure tangle
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that makes perfect sense. Thank you so much for taking the time to help me!

smoky crystal
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nope problem, and weight average is pretty much the same thing, you can try for yourself

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the whole point of using linear combinations is that we can play around with the two equations, and somehow make a 3rd equation such that one of the variables dissapear, or in the context of line, that the line corresponding to it is independent of the values of either x or y

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like the case we have here where the blue line is independent of y

pure tangle
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that's great. Thank you so much for all the help and patience!

smoky crystal
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however, just something that i personally dont like, is the way they call this the weighted avg, but yeah anyway gl

pure tangle
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how would you better describe it?

smoky crystal
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np, i just so happen to be bored after semester finished for me

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well here it describes the weight avg for a particular case of us manipulating the equation, which is multiply both side by a costant before adding

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but it doesnt have to be

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are you a HS student?

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i prob asked too much ,its okay, anyway gl lol

wintry steppe
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linear maps..........

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maps.....

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topography

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linear algebra = topology!

primal cosmos
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@wintry steppewoke

blissful pagoda
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I am so confused what eigenspace is. Can I have some clarification?

I have 1, -2, and 3 as my eigenvalues. My eigenvector corresponding to my eigenvalue of 1 is (1/3, -2/3, 1). My eigenvector corresponding to my eigenvalue of -2 is (-1/3, -1/3, 1). My eigenvector corresponding to my eigenvalue of 3 is (1, 0, 1).

Is my eigenspace {(1/3, -2/3, 1), (-1/3, -1/3, 1), (1, 0, 1)}?

limber sierra
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well those arent your only eigenvectors

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in the sense that any scalar multiple of an eigenvector is also an eigenvector, right? (unless that scalar is 0)

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since they still satisfy Av = lambda v

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your eigenspace is the space of all eigenvectors (as well as the zero vector) of a given eigenalue - so not only will it contain the three vectors you listed, but it will also consider any scalar multiples

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if you're familiar with the notion of "span", then the eigenspace is the span of a given eigenvector

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this is distinct from the set {(1/3, -2/3, 1), (-1/3, -1/3, 1), (1, 0, 1)} itself

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since the span includes all linear combinations

blissful pagoda
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Ok I see where ur coming from.

limber sierra
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sorry my phrasing was misleading

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edited

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note that eigenspace is tied to a specific eigenvalue

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we dont really talk about "the eigenspace"

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since a given matrix/transformation may have multiple eigenspaces

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we talk about "the eigenspace of the eigenvalue"

blissful pagoda
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The thing I'm mainly confused about is this in my textbook. Isn't this implying that I have one eigenspace for each eigenvalue? The eigenspace being the eigenvalue's eigenvectors + zero vector

limber sierra
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yes thats what im saying

blissful pagoda
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I see

limber sierra
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again my phrasing was poor

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so if youre familiar with span

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lets take the eigenvalue -2 as an example

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the eigenspace of -2 would be span{(-1/3, -1/3, 1)}

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or equivalently, the set {k(-1/3, -1/3, 1) | k is a scalar}

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or equivalently, the set of eigenvectors associated to the eigenvalue -2, along with the 0 vector

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theres a bunch of different ways to think of it

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but they all result in the same object

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and yes, each eigenvalue will have its own eigenspace

blissful pagoda
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that makes sense. So my original thought of the eigenspace being all of the eigenvectors combined of all eigenvalues is just plain wrong. Got it, that's what I was mainly confused about lol

limber sierra
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yeah

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each eigenvalue has its own

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(although some may be the same, if two eigenvalues have the same eigenvectors)

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(if that's the case, then your eigenspace is multidimensional and it would be the span of multiple vectors)

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(the same definition works though: the set of eigenvectors of a given eigenvalue)

blissful pagoda
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it probably depends on instructor/prof but should I write the zero vector if I ever am asked to state the eigenspace?

limber sierra
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yes.

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or i mean

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whatever set you write

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should contain 0

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so if you write something that doesnt contain 0, make sure to union it with {0}

blissful pagoda
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gotcha

limber sierra
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the definition they give - the set of eigenvectors together with {0} - is the best one

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[although if you know what a "kernel" is there's another very handy definition]

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[the eigenspace of a vector lambda is the kernel of (A - lambda I)]

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[if you dont know what that means or if its weird to think about, dont worry about it]

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[["kernel" and "null space" are the same thing]]

blissful pagoda
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The kernel is defined in my textbook "the set of all vectors v in V that satisfy T(v) = 0 is the kernel of T and is denoted by ker(T)" but I don't know how it relates to eigenvalues and stuff

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I do understand the kernel = nullspace thing though

limber sierra
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well the idea is

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if v is an eigenvector then it satisfies Av = lambda v

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we can rearrange this to Av - lambda v = 0

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and then factoring out the vector v

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(A - lambda I)v = 0

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where I is the identity matrix (of the appropriate size)

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so now if we interpret (A - lambda I) as a linear transformation, call it T

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this is the set of vectors v such that T(v) = 0

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i.e. the kernel of T

blissful pagoda
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Oh I see

limber sierra
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where T corresponds to multiplication by (A - lambda I)

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anyway, this isnt really necessary to worry about at first

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but it might come up later on

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(it's arguably a more "natural" perspective)

blissful pagoda
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(lambda I - A) and (A - lambda I) are the same right (row equivalent in the end)

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because my textbook has it as the former

limber sierra
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oh yeah you end up with the same definitions

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thats just what you get when you go from "Av = lambda v" to "lambda v - Av = 0" (instead of what i dod, going to "A - lambda v = 0")

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the manipulations are the exact same

blissful pagoda
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yeah okay gotcha

karmic bronze
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How hard is this course

thorny hemlock
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idk how to get (ST)^2 = 0

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all those vectors that S maps are actually the zeroes in T so T(Sv) = 0 for any vector in V

native rampart
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If TS is 0 ,STST is 0

thorny hemlock
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i see

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so the first T gives a vector and then S gives another vector, the third T makes it zero yes?

native rampart
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Yes

thorny hemlock
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i see

gray dust
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maps V->V associate under composition so we can simplify STST whatever way, STST=S(TS)T=S0T=0

thorny hemlock
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i was not aware

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thanks

past meteor
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For the question:
Show that any set of five points from the plane R 2 lie on a common conic section, that is, they all satisfy some equation of the form ax2 + by2 + cxy + dx + ey + f = 0 where some of a, . . . , f are nonzero.

The solution said:
*On plugging in the five pairs (x, y) we get a system with the five equations and six unknowns a, . . . , f. Because there are more unknowns than equations, if no inconsistency exists among the equations then there are infinitely many solutions (at least one variable will end up free).

But no inconsistency can exist because a = 0, . . . , f = 0 is a solution (we are only using this zero solution to show that the system is consistent— the prior paragraph shows that there are nonzero solutions).*

I'm confused about the last line, why does using the zero solution show the system is consistent? The question says "where some of a, ..., f are nonzero" but how does this translate to a = 0, ..., f =0 being solutions?

marble lance
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The a to f are the variables in your system of equations

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Now if there are fewer variables than equations, then a system of equations has either no solutions(if there is an inconsistency) or infinitely many distinct solutions

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Because there is one solution (the solution where a to f are all 0), that eliminates the possibility of there being no solutions

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So then there must be infinitely many solutions (and in other solutions, some of the variables are nonzero)

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Unknowns probably better word than variables

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@past meteor

past meteor
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I'm still a littlee confused, so if the system has either no solutions or infinitely many, I don't get how there's still the one solution when all a to f are 0

marble lance
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Do you not think making all the unknowns 0 is a solution?

past meteor
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how does that make it solution

marble lance
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Take an equation, make them all 0, and the equation is true

past meteor
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ahhhhh, that makes sensee

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right, yeah the rest makes sense, thank you so much!!

marble lance
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Np

thorny hemlock
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shouldnt dim(nullT) = 2 ?

gray dust
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@thorny hemlock how

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@round coral let him answer

round coral
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alright

thorny hemlock
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the basis of the null space is of length 2

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?

gray dust
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no. we're given info on U, not ker(T). dim(U)=2

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@marble lance not yet

marble lance
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I don't think I want to give anything away.

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You could do a proof by contradiction and assume there is a T where U = null T, but this is NOT what the solution is doing.

gray dust
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it's the multiple helpers thing

thorny hemlock
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but isnt the question saying that the kernal equals (x1 x2 x3 x4 x5) where x1=3x2 and x3=x4=x5 ?

marble lance
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Yeah, yeah, but I still owe you for last time and I thought that was worth pointing out. Go ahead.

thorny hemlock
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Vectors of that form get sent to zero

gray dust
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the exercise is showing that for any T in L(F^5,F^2), ker(T)**!=**U

thorny hemlock
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i see

gray dust
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keyword !=. reread 'does not exist' in the text

thorny hemlock
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What if we wanted to do it by assuming that there is a linear map from F5 to F2 such that the null space is that

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then we would get that dim(RangeT) would be 3

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then dimRangeT > dimF2

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which is contradiction

gray dust
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that works

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back to the book, the problem is reading too fast

thorny hemlock
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So in the solution, they did a kinda direct proof?

gray dust
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if that's what you call any proof not using contradiction

thorny hemlock
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im bad at proofs

wintry steppe
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sad

thorny hemlock
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:(

gray dust
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it 'directly' aims to show any linear map F^5->F^2 doesn't have U as its kernel

old flame
thorny hemlock
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which is more commonly used? null or kernal ?

stoic pythonBOT
gray dust
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@thorny hemlock axler uses nullspace. i use kernel bc it used in more contexts in abstract algebra

native rampart
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If a=conjugate(a) a is real

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That is a property of complex numbers

old flame
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yeah ?

native rampart
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(Take a=x+iy,x,y in R
conj(a) will be x-iy, x+iy=x-iy implies y=0
)

old flame
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ah I see what u mean there

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so since inner product gives out a scalar, the scalar is equal to its conjugate

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got it thanks

wintry steppe
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psst

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\langle \rangle

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$$\langle x, y \rangle$$

stoic pythonBOT
old flame
wintry steppe
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the definition of the adjoint

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$\langle T^* Tv, v \rangle = \langle Tv, Tv \rangle$ by the definition of $T^*$, and that's just $|Tv|^2$. similarly for the other side

stoic pythonBOT
wintry steppe
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@old flame

old flame
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ahhhh

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so the vector in the definition is instead $Tv$ and $T^{*}v$ in the other case then

stoic pythonBOT
wintry steppe
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i guess so

old flame
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I mean by definition I just know that $\langle Tv,w \rangle = \langle v, T^{}w \rangle$. So from that we would have $\langle TT^{}v,v \rangle = \langle T^{}v, T^{}v \rangle$, So I guess its because the conjugates are equal, so the last one could swap places right ?

stoic pythonBOT
wintry steppe
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i'm not sure what this has to do with conjugates

old flame
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The one im talking about is $\langle T^{*}Tv,v \rangle

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because from the definition the adjoint is in the right

wintry steppe
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ah i see where you're coming from

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right

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ya you got it

old flame
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so self adjoints have this property $\langle v, T^{}w \rangle = \langle T^{}w,v \rangle$ ?

stoic pythonBOT
wintry steppe
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nno i don't think so, try T = identity, so that that fails if <v, w> is not a real number

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maybe i misunderstood what you meant by "because the conjugates are equal, so the last one could swap places"

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let me write something out

old flame
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sure thing

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cause I just don't know why the places could be swapped

stoic pythonBOT
wintry steppe
#

sorry i forgot how to tex there

#

the second equality sign is the definition of the adjoint

#

where it's on the right argument of the inner product

#

then you can undo the conjugate because swapping the arguments in <Tv, Tv> changes nothing

#

and then you just get the norm squared of Tv

old flame
#

oh

wintry steppe
#

does that make sense?

old flame
#

yes, so instead the swapping occurs during Tv,Tv, so it doesnt matter as its the same anyways

wintry steppe
#

mmhm

old flame
#

so I guess whenever I see T^* up front, should try to think of conjugating it to use the definition

wintry steppe
#

probably a good thing to keep in mind, yeah

old flame
#

alright, thanksssss

thorny hemlock
#

i dont get the solution for the second part

#

they just chose a specific transformation so all the u's get sent to zero and say nullT = U ?

wintry steppe
#

you should write out the proof that U = null T

#

in excruciating detail

thorny hemlock
#

theres too many problems

#

If i wrote full proofs for each one

#

it will take me hours

wintry steppe
#

well then at least convince yourself that null T = U by writing it down

thorny hemlock
#

i did

wintry steppe
#

so what part of the solution is confusing you

thorny hemlock
#

i think ive understood now

#

for the second part,

#

We just need to show that there exists a Linear transformation such that nullT=U under assumptions given right

wintry steppe
#

yes

thorny hemlock
#

yeah i think ive got it

thorny hemlock
#

$Forward: \ $T is injective \Rightarrow dimV \leq dimW \ $define $T(v_j) = w_j $ (This is injective and linear)\ Define S so $Sw_i = v_i$ for $i = {1...n}$ $Sw_i = 0$ for $i = {n+1....m}$ w1...wm is basis of W then $STv_j = v_j$

stoic pythonBOT
thorny hemlock
#

does something like this work ? the solution does it a different way

wintry steppe
#

what are the v_j's? w_j's?

thorny hemlock
#

basis

#

v1..vn basis of V w1...wm basis of W, j is just a specific something 1<= j<= n

#

@wintry steppe is this ... somwhat ok?

native rampart
#

Yea, That's fine

thorny hemlock
slate fox
#

Let V be an infinite dimensional vector space over a field F. Suppose that T : V → V
is a linear transformation such that Ker(T) is finite dimensional. Prove that Im(T) is infinite dimensional.

#

I was able to do this by finding a finite basis for V

#

but i remember seeing a clever solution using the first iso theorem that i cant recall

#

anyone know?

thorny hemlock
#

:0

steady fiber
#

a finite basis for an infinite dimensional vector space?

slate fox
#

yea contradiction

native rampart
#

That's Pretty direct,ig

slate fox
#

if i assume both ker and Im are finite dim

steady fiber
#

oh I see what you mean

native rampart
#

im(phi) iso to V/(ker phi)

thorny hemlock
slate fox
#

somehow

#

i dont remember how tho

#

and i cant find it

native rampart
#

Do you know dim(A/B)=dim(A)-dim(B)?

slate fox
#

yes

native rampart
#

dim(im(phi)) would be dim(V) -dim(ker phi)

#

Since dim(V) is infinite ,dim(im(phi)) is also infinite

slate fox
native rampart
#

ker phi is a subspace of V

thorny hemlock
#

did the normal chatting channels get deleted?

native rampart
#

No,You have the studying role

#

So you can't see them

thorny hemlock
#

oh lmao

slate fox
#

hm

brisk fractal
#

apologies for the weird notation (it's just the linear maps as matrices in their respective spaces)

spice storm
#

looks like linear done right book

brisk fractal
#

I'm a bit confused in the end result, is B^T = A or is B = A?

brisk fractal
spice storm
#

what does that cover?

brisk fractal
#

it's an abstract algebra textbook for the most part but he spends like 4 chapters covering LA in an abstract setting to build motivation

spice storm
#

oh cool

brisk fractal
#

I was reviewing his sections on dual spaces and quotient vector spaces so I would have a better understanding of inner direct products of groups

spice storm
#

sounds like grad school is making you busy during winter break

brisk fractal
#

I'm putting myself through this actually, I've felt kind of bad for my woeful lack of algebra knowledge

spice storm
#

oh nice. Is it so far worth it

brisk fractal
#

Knapp is seemingly very well written

#

I haven't done any abstract algebra beyond linear algebra and although it's aimed at graduates it's a fairly pleasant read

#

I'm actually enjoying myself despite pretty much only doing analysis/topology/geometry

wintry steppe
#

contragredient

#

this notation is really confusing

#

contragredient makes me feel like i'm gonna be eating food soon, too close to "ingredient"

#

but all i'm fed is shitty indices

#

shouldn't the end result be A^T = B (matrix transpose) anyways

#

i agree with you slim

#

not in the statement of the proposition, unless i've failed to interpret that notation from the context

#

some weird way of writing the matrix that represents a linear map

#

what else?

#

lol

#

@brisk fractal typo in the statement probably, end result should be B^T = A

#

i checked against another book (friedberg) to be sure

#

bacono can utell us what the notation means

#

pls

stoic pythonBOT
wintry steppe
#

bacono depriving us rn

#

$[T]_\beta^\gamma$ means the matrix of $T \colon V \to W$ with respect to the bases $\beta, \gamma$.

stoic pythonBOT
wintry steppe
#

friedberg

#

fries burger

#

yes

#

i don't think friedberg contains much more than axler

#

😔

#

roman talks about infinite dimensional space stuff catThink

brisk fractal
#

hello I am back on my computer

#

yeah so I think it is a typo tterra

#

the reason I ask is because in the proof it claims that A, B are just the matrices given in the statement, but then it proves that A^T = B instead of A=B

wintry steppe
brisk fractal
wintry steppe
brisk fractal
#

don't worry about it hmmm

wintry steppe
#

just reinforces what you said

#

"read a linear algebra book"

steady fiber
#

there was a typo in my textbook yesterday, I spent half an hour trying to prove something impossible

#

typos do make me mald

#

if they're critical

#

I only found out in some comment of a math stackexchange post

#

that it was a typo

#

fixed in later versions

#

@wintry steppe I'm on the cringe part of the Sylow section

wintry steppe
#

have fun!

pallid rampart
#

😩

wintry steppe
#

i like how all of these require you to find the prime factorization

steady fiber
#

I just have a prime factoring website open

thorny hemlock
#

idk how to do this :/

#

any hints?

#

<@&286206848099549185>

stoic pythonBOT
thorny hemlock
#

-1 as in inverse?

stoic pythonBOT
thorny hemlock
#

i havnt learnt all of this yet :0

#

maybe theres an easier way of doing it

#

no

#

doing the axler book

stoic pythonBOT
thorny hemlock
#

oh yeah

#

lol

#

lmao

#

ok

#

T-1 takes a vectors from W to U ?

#

confusion

#

er

#

T-1(nullS) = u \in U where u is in nullS ?

#

ok

#

i see, then use rank nulitiy thing

#

yeah got it

sweet vine
limber sierra
sweet vine
#

ok 🤔

limber sierra
#

if your matrix is hermitian that means

#

all its eigenvalues are positive

sweet vine
#

alright thanks Namington

old flame
#

How does he find the diagonal matrix with respect to the eigenvectors from the orthonormal basis ? what is the calculation procedure ?

native rampart
#

Just find the eigenvalues

#

He found the diagonal matrix and used that to find the eigenbasis

old flame
#

so use the basis to find the eigenvalues ? then find the corresponding eigenvectors right ?

native rampart
#

He didn't use the basis at all

#

He probably used the char eqn

old flame
#

oh but that is taught in chapter 8

native rampart
#

Anyway,The point is that there will always be a diagonal matrix,similar to a normal matrix

old flame
#

I mean I was trying to verify and that was stated, but not sure how lol

#

yeah well I get his point, which its literally the complex spectral theorem up next

native rampart
#

Yes

#

Well,upto rearrangement of basis

old flame
#

I see, thanks

old flame
#

I am just wondering why is the decomposition in terms of null spaces ? This I still don't really fully understood, even though I have seen this a couple chapters back

slow scroll
#

well null(...) are just the eigenspaces

stoic pythonBOT
native rampart
#

null(T-xI) will be the subspace of eigenvectors with eigenvalue x

slate fox
#

Let V = W = R^3 and T : V → W be the linear transformation T(x, y, z) =
(x + 2y + 3z, y + 2z, 2y + 4z). Find a basis BV for V and a basis BW for W such that the matrix representing T with respect to the bases BV , BW is a diagonal matrix

#

so i need to find bases {v1,v2,v3} and {u1,u2,u3} such that T(v1)=au1, T(v2)=bu2 and T(v3)=cu3

#

is this just guess and check from here?

slate fox
#

it doesnt look very linear

thorny hemlock
#

Ah

slate fox
thorny hemlock
#

Any hints on how we should define S?

#

T1 and T2 are linear maps from U to W

slate fox
#

how do I show that a cyclic operator T such that T^2=T cant be invertible

native rampart
#

If T is not I,T is not invertible

#

Because det(T)=0

slate fox
#

det(T)?

#

u mean of the matrix representing T?

native rampart
#

Well,You can take it that way

slate fox
#

how do we know the det is 0 tho

native rampart
#

If T^2=T,The minimal polynomial of T is either x or x-1 or x(x-1)

#

In first case,T=0 ,in second case T=I and in the final case,T is diagonal in some basis,with zero as an eigenvalue

slate fox
#

we havent covered eigen values or vectors yet

#

not sure what a minimal polynomial is

native rampart
#

Minimal polynomial of T is a polynomial p,such that p(T)=0(i.e, p(T)v=0 for all v)

slate fox
#

yea havent met yet that

native rampart
#

T on a Tcyclic subspace?

slate fox
#

T is cyclic if there exists a v such that the set {v,T(v), T^2(v)...} spans V

native rampart
#

You can conclude,V is atmost 2 dimensional in your case

#

Because {v,Tv,T^2v...}={v,Tv}

#

Since T^2=T

#

And then consider matrix of T in basis {v,Tv}(if 2 dimensional)

#

If V is one dimensional,T=I,and T is invertible

slate fox
#

shouldnt it be at least 2 dimensional?

#

nvm its not

#

ok yea if it has dimension 2 then it cant be invertible

#

but if it has dimension 1 doesnt that mean the question is wrong?

#

cuz the identity operator is invertible right

#

right? @native rampart

crimson pelican
#

if U,V and W be subspaceses or R^n . Is U∩(V+W)=(U∩V)+(U∩W) true ? If it is true how could I proof that ?

#

<@&286206848099549185>

native rampart
slate fox
#

ok thank you

crimson pelican
#

why how can I conclude that

thorny hemlock
#

Finding an example that fails

wintry steppe
#

it is very false, not hard to come up with a counterexample in R^2

crimson pelican
#

what if I defined a element of V and b element of W then define x= a+b then if x element of U∩(V+W) then x also element of U and x element of (V+W) . But (U∩V) does not contain x and (U∩W) does not contain x.

#

@wintry steppe @wintry steppe @thorny hemlock

steady fiber
#

find a case when the intersection of U with V+W is small, but the intersection of U with one of V or W is large

crimson pelican
#

included two vectors which have two row and one column

#

this vectors must hold 3 condition

#

okay what are the types

#

lines through the origin

#

lets choose x+y=0 and x+2y=0

wintry steppe
#

This is a physics question that has to do with vectors, so I thought this may be the right channel. If not, please lmk.

My question is why can't I multiply the magnitudes of F and ∆d together to get work? Why do I have to use the dot product?

crimson pelican
#

@wintry steppe we are trying solve the quesiton and you send quuesiton bro c'mon

steady fiber
wintry steppe
#

It's a conceptual question, so I don't think the answer should matter

steady fiber
#

they could give you a better conceptual understanding of force and distance and work

wintry steppe
#

Gotcha - thanks!

crimson pelican
#

ı dont understand

stoic pythonBOT
crimson pelican
#

(0,0)

marble lance
#

And the sum?

crimson pelican
#

sum is still (0,0) but now we have not false statement

marble lance
#

No

crimson pelican
#

yes

stoic pythonBOT
crimson pelican
#

i think its cant be zero

#

no sorry it included zero

wintry steppe
crimson pelican
#

left hand side can be equal ${0}$

#

its vector addition ı dont know

#

its line through the origin nvm ı cant find it

wintry steppe
crimson pelican
#

yes

#

span{u,w}

#

yes

#

so?

#

nope ı cant figure out thx for helping

wintry steppe
#

v and w are linearly independent, so their span is 2 dimensional. what are the 2 dimensional subspaces of R^2

crimson pelican
#

lines through the origin

#

@wintry steppe

wintry steppe
crimson pelican
#

then its just (0,0)

#

ı m going to crazt

#

y

crimson pelican
#

it is empty seyt

#

@wintry steppe

hoary osprey
#

thats not a subspace

crimson pelican
#

and what is

#

this

wintry steppe
#

the only 2 dimensional subspace of R^2 is R^2 itself.

#

so the span of v and w is R^2.

crimson pelican
#

and left hand side is R^2 but right hand side is 0

wintry steppe
#

you mean of U∩(V+W)=(U∩V)+(U∩W)?

crimson pelican
#

yeap

wintry steppe
#

almost

crimson pelican
#

U are included R2

wintry steppe
#

that's an intersection

#

not a union

crimson pelican
#

yes but (V+W) included R2

wintry steppe
#

?

crimson pelican
#

so the span of v and w is R^2.

#

Let's write W= span{w} and V=span{v}

wintry steppe
#

V + W is R^2, but U is a subset of R^2, so the intersection is just U

#

one side is U, one side is empty

crimson pelican
#

ohh okey you are right

#

ım sorry

#

thanks

wintry steppe
#

it is true

fallen karma
#

if a finite dimensional vector space V with dim(V)=n has a linear map T with n distinct eigenvalues, where v_1,v_2,...,v_n are the corresponding eigenvectors, then is any invariant subspace under T just the span of some collection of those eigenvectors?

#

just yes or no will help me

fallen karma
#

nm think I figured it out

wintry steppe
#

was it yes or no catThink

#

i am interested

fallen karma
#

haha idk yet but I suspect yes. I'm trying something with quotient operators

wintry steppe
#

i'm tempted to say yes

#

cause if you diagonalize T then it's clear that the invariant subspaces (identifying V with R^n) are just the axes, and then something about changing bases and how that interacts with subspaces idk puts away crack pipe

fallen karma
#

that's an interesting take

wintry steppe
#

lmao

#

forgot how to LA there for a second LOL

fallen karma
#

it'd be nice if it was true so it is true right??😆

#

what was wrong with what you said?

wintry steppe
#

i wanna check it before i un-strikethrough it just to make sure i'm not saying complete bs

#

cause also the entire space is invariant and so is {0} so i have to be a bit more careful with that claim

fallen karma
#

ok valid

#

but it seems worth exploring

wintry steppe
#

maybe "the only non-trivial proper T-invariant subspaces are the axes" ?

#

just thinking about how like, a diagonal matrix is just scaling along each axis, it makes sense

quartz compass
#

I figure just represent anything in the eigenbasis, it will automatically be trapped in the span

fallen karma
#

pesky {0}

#

i shoulda specified when I posed the question "and {0}"

wintry steppe
#

skimming over my LA book to see if there're any nice results about invariant subspaces that could be used here

#

alright so if you restrict T to any invariant subspace, you get an operator whose characteristic polynomial must divide that of T. now, by assumption, the char poly of T splits, so the char poly of T restricted to any invariant subspace splits

#

i.e. T restricted is also diagonalizable with some subset of the original eigenvalues

#

(still doesn't really answer the original q tho)

fallen karma
wintry steppe
#

try proving it, you take a basis of the invariant subspace and extend it

quartz compass
#

what's wrong with what I said?

#

I think you're overcomplicating it

wintry steppe
#

overcomplicating is fun catThink

fallen karma
#

i tried representing in the eigenbasis earlier but it got messy. so i went looking for another way

quartz compass
#

eh?

wintry steppe
#

Let $W \subset V$ be a $T$-invariant subspace of $V$. Since $T$ is diagonalizable, $T|_W$ is also diagonalizable in $\mathrm{End}(W)$. That is, $W$ is spanned by some of the eigenvectors of $T$.

stoic pythonBOT
wintry steppe
#

(from section 5.4 of the linear algebra book by friedberg, insel, spence)

quartz compass
#

I was thinking of something a bit simpler

#

suppose you take any invariant subspace, then all its vectors can be represented by a linear combination of some set of eigenvectors. Then let's show it actually contains the entire span of these eigenvectors

limpid fiber
#

Sorry to interupt, why is it true that if $Ax = 0$ only has the trivial solution then A cannot have a free variable?

stoic pythonBOT
quartz compass
#

so take some u in the invariant subspace, it has coefficients, $$u = \sum_{i=1}^n a_i \vec e_i$$ now we can get the vectors in our invariant subspace $Au$, $A^2u$,..., $A^{n-1}u$ to get $A^k u = \sum_{i=1}^n a_i \lambda_i^k \vec e_i$ which gets us a system of linear equations

stoic pythonBOT
quartz compass
#

it's a nice vandermonde matrix that we can invert which has det !=0 since the eigenvalues are distinct, so we can solve for any eigenvector as a linear combination of the A^k u

#

and by being a subspace we have all scalar multiples

fallen karma
wintry steppe
#

you should explore mero's idea

#

i think it is good

fallen karma
#

yeah bet, I didn't think about applying the operator more than once

wintry steppe
#

just wait until you get to cyclic subspace nonsense monkaS

fallen karma
#

thanks for your help guys

#

and gals and nb pals

wintry steppe
#

How could I forget this place exists?

half ice
#

Lots of alcohol, like me

#

But I always come back

#

😫

tame mural
#

Does the set with only the 0 vector have a name?

quartz compass
#

Dunno, maybe 'the trivial vector subspace' or something like that maybe

tame mural
#

mmm

#

thx

smoky crystal
#

its just the zero space

tame mural
#

if a transformation preserves the dot product, does that also mean it always preserves angles?

blissful vault
quartz compass
#

well, do you know any formulas that relate the dot product to the angle? @tame mural

native rampart
tame mural
#

Sure, it's the dot product of two vectors divided by the product of their norms

blissful vault
#

Is there anything I can improve in my writing?

quartz compass
bold garden
#

I understand the general point of the proof, but I was confused because I thought the stuff in the blue brackets might be too informal

#

I also don't understand what the finite-ness of S has to do with anything - why couldn't this work for a potentially infinite S (besides the fact that the theorem would be false)?

marble lance
#

I mean, you could end up choosing all the vectors of S if they are all linearly independent

#

But that's it, then you can't choose any more

bold garden
#

sure, but what I'm saying is why the statement "continue, if possible, choosing vectors such that $${u_1, u_2, ..., u_k}$$ is linearly independent" is the right way to do it

stoic pythonBOT
bold garden
#

shouldn't there be some kind of induction involved?

marble lance
#

I don't know what you mean. It's basically "in a finite number of steps, you can either choose vectors so that you cannot choose another so that's its linearly independent or you have chosen them all."

#

There's nothing wrong with saying you can do something a finite number of times

bold garden
#

oh, i wasn't aware of that, in that case i guess it's fine then

#

thank you

thorny hemlock
#

Tv = a1w1 + .... + amwm where a's/in F

#

S1(v) = a1 .... Sm(v) = am

#

thats correct right?

wild fern
#

there is $$T_1, T_2 \in L(V,W)$$, prove inversible transforms $ R \in L(V,V)$ and $S \in L(W,W)$ exists such that $T_1 = ST_2R$ iff $ dim(N(T_1)) = dim(N(T_2))$

stoic pythonBOT
native rampart
round coral
#

@wild fern you know change of basis, it follows from that

#

except that what is N in dim(N(T_1)) = dim(N(T_2)) , you didn't define that

wild fern
#

N is nullspace

round coral
#

well seen that notation for first time, either use null or ker , I don't think N is the official notation for nullspce

wild fern
round coral
#

ok, I am really ignorant, but that Q follows directly from change of basis of a linear transformation

#

hope it helps

wild fern
round coral
soft burrow
#

that's the inverse process, the quadratic form of a (e.g. real) matrix $A\in \mathcal M_{n\times n}(\bR)$ is $q: \bR^n\times \bR^n \to \bR$ given by
$$
q(x,y)=x^{\mathsf T}Ay.
$$

stoic pythonBOT
soft burrow
#

all it does is associate a degree two polynomial to the matrix. It appears naturally in mathematics, e.g. inner products can be defined by quadratic forms. One proves that quadratic forms are esseentially the same as symmetric square matrices (in fact each quadratic form has a unique such matrix)

native rampart
#

That's the bilinear form

#

The corresponding quadratic form is q(x,x)

#

Yes

soft burrow
native rampart
#

Gram-Schmidt will not always give you an eigenbasis

#

Just Take a non eigenbasis(Start your construction with a non eigenvector) and apply gram schmidt,you wouldn't get a eigenbasis

#

I don't think that's true in general

stoic pythonBOT
limpid fiber
wintry steppe
#

that's not null 2 minus 3

#

that's null of the vector (2, -3)

limpid fiber
#

yes, sorry about that typo

wintry steppe
#

or better, the null space of the 1 by 2 matrix (2 -3)

#

had a brain fart for a sec but that's what it should be

limpid fiber
#

lol yes

#

but isn't this just a vector not a matrix?

wintry steppe
#

the elements of V are vectors

#

what does Nul(2 -3) mean to you

#

that may help clarify things

stoic pythonBOT
limpid fiber
#

I am confuse because $[\begin{bmatrix}
2 \
-3 \
\end{bmatrix}]$ is in $R^2$ and $[2 -3]$ is in $R^1$ but it feels like they liberally switch between them?

round coral
#

what's so confusing about it ?

stoic pythonBOT
wintry steppe
#

how is that second one in R^1

#

wat

#

the distinction between column vectors and row vectors / tuples is usually blurred

#

just something you have to get used to

round coral
#

do you know how the vectors in R^2 and R look

limpid fiber
#

yeah, I guess they'd both be lines?

#

that's good to know though I appreciate that @wintry steppe

round coral
limpid fiber
#

but the former line is in R^2 and the latter R^1?

round coral
#

see it clearly

limpid fiber
#

okay I will look now, thank you

wintry steppe
limpid fiber
#

Does the same thing hold for a 2x2 matrix, I know the row 'picture' and vector/columns 'picutre' are the same , but I'm not exactly sure why yet

#

or is that different from what y'all are talking about?

round coral
#

these are equivalent

#

actually the 3) is the one , from which 2) comes out as I studied in the beginning, but you can do from 2) to 3) as well

#

doesn't make a difference

limpid fiber
#

nice, I hope this is related to what you were saying

#

yes what you say about 2 and 3 makes sense I think

#

I still cannot connect 1 and 3 or 1 and 2 though, I know the proof that they must have the same solution set which I know is true but still feels unenlightening

#

is that something that will become clearer as I progress in Linear algebra?

round coral
#

1 -> 2 are what you first study in any book, how to write a system of linear equations in matrix form

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as 2 and 3 are equi 1 and 3 are equi , you just need to look at it

limpid fiber
#

yeah you're right I can see 1 and 3 must be the same by definition now that I look

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but in my mind 1 is the equation for two planes, wheres 3 is a linear combination of vectors

round coral
#

although I do not like it, you can read Strang's Chapter 1 , he has discussed about geometry of linear equations well

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@limpid fiber

prisma tide
#

anyone done quaternions here?

soft burrow
prisma tide
#

ok

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@soft burrow no acess

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nvm just got it

hollow finch
#

is there a special name for the matrix $\pm\begin{bmatrix}0&1\-1&0\end{bmatrix}$?

stoic pythonBOT
hollow finch
#

i know its the matrix representation of the complex number plus minus i but does it have a name?

soft burrow
#

definitely not a unique standard name

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some authors use $\mathbf{1}=\begin{pmatrix} 1&0\0&1 \end{pmatrix}$ and $\mathbf{i}=\begin{pmatrix} 0&1\-1&0 \end{pmatrix}$

stoic pythonBOT
winter harbor
#

Given a real vector space $V$ and being $\mathscr{A}{n}(V)$ the space of all alternating n-forms $\varphi : V \times \hdots \times V \rightarrow \mathbb{R}$. We can define $A^{#} : \mathscr{A}{n}(V) \rightarrow \mathscr{A}{n}(V)$ as $(A^{#}\varphi)(v_1,\hdots,v_n) = \varphi(Av{1}, \hdots, Av_{n})$
\
\
The important thing to know is that since $\dim \mathscr{A}{n} = 1$, then the LHS is just equal to $\varphi$ times a constant, which we define as the determinant of the linear operator A.
\
\
So $\det A$ satisfies by definition:
\
\
$\det A \cdot \varphi(v
{1}, \hdots, v_{n}) = \varphi(Av_{1},\hdots,Av_{n})$

stoic pythonBOT
winter harbor
#

I just wonder if this A hash operator has a name

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or is just a trick we use only once to define the determinant of a operator

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I also wonder what's the intuition behind this definition

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if it has some geometrical insight if it's R^n maybe

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oh, V is finite and has dimension n

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I forgot to say that

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But how can we prove using this definition that $\det A = \int_{ [0,1]^{n}} 1 dx$

stoic pythonBOT
winter harbor
#

(Damn I'm horrible at typesetting)

wintry steppe
wintry steppe
#

e.g. in slightly more generality, if you have a linear A : V -> W, then you can define the pullback A^* : {k-tensors on W} -> {k-tensors on V} in an entirely analogous way

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particularly useful in smooth manifold theory catThimc

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also i think you mean to write $$\det A = \int_{A([0, 1]^n)} 1$$

stoic pythonBOT
wintry steppe
#

in that case, you can use the change of variables theorem for integrals

thorny hemlock
wintry steppe
#

\begin{align*}
\int_{A([0,1]^n)} 1 , dx^1 \wedge \cdots \wedge dx^n &= \int_{[0, 1]^n} A^(dx^1 \wedge \cdots \wedge dx^n) \
&= \int_{[0,1]^n}\det(A),dx^1\wedge\cdots\wedge dx^n \
&= \det(A) \int_{[0,1]^n} 1 , dx^1 \wedge \cdots \wedge dx^n \
&= \det(A)
\end{align
}

thorny hemlock
wintry steppe
#

can you wait?

thorny hemlock
#

yep sorry

stoic pythonBOT
wintry steppe
#

@winter harbor

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eh tbh you don't need to do the pullback and differential forms nonsense to prove that, that just follows pretty easily from the classic change of variables theorem

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but i wrote it like that to try and emphasize your definition of det A, i guess

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overkill is fun

thorny hemlock
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integral :o

winter harbor
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oh yeah, you are right, I meant A([0,1]^{N})

primal cosmos
#

is that a lebsegue integral?

winter harbor
#

thanks

wintry steppe
#

np

winter harbor
#

riemman integral in R^n

wintry steppe
#

differential forms are fun

primal cosmos
#

?

thorny hemlock
primal cosmos
wintry steppe
#

no

thorny hemlock
#

no

winter harbor
#

nah

primal cosmos
#

oh

thorny hemlock
#

rein

limber sierra
wintry steppe
#

plain old riemann integrals

limber sierra
wintry steppe
winter harbor
#

this is just the riemman integral in R^n as I have said before

thorny hemlock
#

lmao

primal cosmos
#

why don't they have an upper bound?

limber sierra
#

theyre multidimensional

wintry steppe
#

because you're integrating over a region in R^n

winter harbor
#

yup

primal cosmos
#

woah

winter harbor
#

I mean

thorny hemlock
#

oke, for my question, 1/x^3 , 1/2x^2 , x , 1 for p3 and x^2 , x, 1 is correct ?

primal cosmos
#

@thorny hemlock what was your question?

thorny hemlock
primal cosmos
#

oh woah

winter harbor
#

when you have an integrable function $\varphi{phi} : [a,b] \rightarrow \mathbb{R}$, and you want integrate this function over an its domain, you could just write it as $\int_{[a,b]} \varphi(x) dx$

stoic pythonBOT
winter harbor
#

it means that you are interating from a to b

#

or more generally

#

integrating this function over the region [a,b]

thorny hemlock
#

integrals are scary

acoustic path
#

integrals 😠

winter harbor
#

it's just that we are used historically to write it as $\int\limits_{a}^{b} \varphi(x) dx$

stoic pythonBOT
winter harbor
#

but in general

wintry steppe
#

Define $F \colon Vect_k \to Vect_k$ by $F(V) = {\text{$k$-tensors on $V$}}$ for objects $V$ and $F(T) = T^* \colon F(W)\to F(V)$ for $T\in Mor(V,W)$ by $T^*\omega(v_1,\dots,v_k)=\omega(Tv_1,\dots,Tv_k)$. Then $F$, the pullback, is a contravariant functor opencry

stoic pythonBOT
wintry steppe
#

if only texit displayed emotes

primal cosmos
#

integrals are not always so bad to set up, but the scary thing is the integration

winter harbor
#

when you are dealing with integral operators over more complicated regions in a way more complicated space as R^n (say differentiable manifolds) we just write the region we are integrating on below the integral symbol

#

for example

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stokes theorem for a general Manifold M may be written like this

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$\int_{\partial \Omega} \omega = \int_{\Omega} d \omega$

wintry steppe
#

\integral isn't a thing, use \int

winter harbor
#

I forgot it lol

wintry steppe
#

you got it right on one side sully

stoic pythonBOT
steady fiber
#

why are we doing stonks theorem in lin alg catThink

wintry steppe
#

why not?

winter harbor
#

I mean

limber sierra
#

manifolds are just vector spaces on drugs

#

so

winter harbor
#

it has to do with linear algebra

wintry steppe
#

namington not wrong

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tbh

steady fiber
#

I'm convinced

wintry steppe
#

manifolds are just the union of the basepoints of their tangent spaces

#

so

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basically linalg

steady fiber
#

everything is basically lin alg

#

or actually, alg

wintry steppe
#

algebra...

steady fiber
#

algebra is the only real math dont @ me

wintry steppe
#

the term "semidirect product" came up when i was reading IRM today and it felt nice to know what it meant catThimc

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maybe algebra isn't so bad

steady fiber
#

lol, I love semidirect products

thorny hemlock
#

whats IRM

wintry steppe
#

intro to riemannian manifolds

#

textbook

thorny hemlock
#

nice

limber sierra
#

i still dont really know what a semidirect product is

wintry steppe
#

it's a weird way of writing down a group action by automorphisms

limber sierra
#

okay actual confession

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i always forget which way to write

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the fish symbol

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for semidirect product

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i get that its like "the same as" the triangle for normal subgroups

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but

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still

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it just looks wrong

winter harbor
#

Also

steady fiber
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isn't it a way of writing a "product" of groups by a homomorphism

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and it happens to have some relationships to automorphism groups at times

winter harbor
#

uhh I said before ''the manifold M'' but I wrote Omega in the latex

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and I didn't even say it's an orientable smooth manifold with boundary

steady fiber
#

if you let the homorphism be from K -> Aut(H) for H (weird x) K

winter harbor
#

what a shame

wintry steppe
#

If $\varphi\colon K \times H \to H$ is a group action of $K$ on $H$, written $\phi(k, h) = k \cdot h$, satisfying $k \cdot (h_1h_2)=(k\cdot h_1)(k\cdot h_2)$, then define $\tilde{\varphi}\colon K \to Aut(H)$ by $\tilde{\varphi}(k)(h) = k \cdot h$. Then we have a semidirect product $H \rtimes_{\tilde{\varphi}}K$, and conversely.

stoic pythonBOT
wintry steppe
#

woh gives a fuck about semidirectproduct

#

just study everything as group action

steady fiber
#

no

wintry steppe
#

dumb fish symobl

steady fiber
#

group actions are too abstract

#

let's unabstract a bit

winter harbor
#

Also TTerra

wintry steppe
#

let's abstract to the group action ur mom had last night

winter harbor
#

I have studied about Pullbacks and Pushforward in the context of manifolds

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but I just don't get the concept at all

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I guess that's why I forgot the definition

#

what's the intuition or the motivation?

wintry steppe
#

honestly off the top of my head, i don't know what the intuition or motivation is, other than "it's a really useful thing that comes up everywhere"

#

i'd have to think

winter harbor
#

it just happens that it's useful when studying 1-differential forms of a smooth manifold

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and now it happens to be important to define the notion of the determinant of a linear operator

acoustic path
#

merry christmas my linear algebra people

thorny hemlock
#

its the 26th here, :0

#

merry christmas

winter harbor
# stoic python **TTerra**

@wintry steppe why is it that when you are integrating over A([0,1]^n) it's the same as integrating the pullback of the wedge product of those differential forms over [0,1]^n ?

wintry steppe
#

change of variables theorem

winter harbor
#

for some reason i really can't see it

#

lemme read the statement again

wintry steppe
#

you don't actually need the differential forms stuff to do it, there's a simpler proof that avoids it (despite being basically the same thing)

winter harbor
#

wait aaaaah

#

i didn't know the change of variables theorem for general manifolds

wintry steppe
#

also

#

looking at this and the page i linked, i was a bit sloppy with the signs

#

you have to be careful to account for the case that det A < 0

winter harbor
#

yeah you are right

wintry steppe
#

orientations 🙄

winter harbor
#

I really meant |det A|

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but i didn't know the change of variables theorem had something to do with pullbacks

wintry steppe
#

well the scalar you get by doing pullback by A will still be det A (without absolute values out front), just when you start integrating you'll pick up a negative sign if det A < 0, whence the absolute value

winter harbor
#

that's some motivation for me to study it

#

I really didn't get the point until now

wintry steppe
#

i am pretty sure the change of variables theorem on manifolds is just the pictured one in disguise catThink

winter harbor
#

Programa de Mestrado - Análise em Variedades - Aula 11:
Orientação. 1-formas diferenciais. Pull-back. Álgebra multilinear.
Professor: Luis Adrian Florit

Página do curso:
https://impa.br/

Download dos vídeos:
http://video.impa.br/index.php?page=programa-de-mestrado-2014-analise-em-variedades

Pré-requisito: Análise no Rn

Variedades diferenciá...

▶ Play video
#

so yeah I know some of the motivations now

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but I still don't get the intuition behind the concept

#

maybe math stack has something concerning this

wintry steppe
#

maybe you can mess around with the 1-dimensional case of pullbacks, in which case it's just composition by the operator catThimc

hollow finch
#

if $A=QS$ where $S$ is symmetric and $Q$ is skew symmetric, will it always be the case that $\operatorname{tr}(A)=0$?

stoic pythonBOT
round coral
#

yes

hollow finch
#

why? how could i prove that?

round coral
#

yes

#

wait a min typing

hollow finch
#

just saying tho thats freakin awesome btw

round coral
#

tr(AB) = tr(AB)* = tr( B* A*) = tr(-BA) = -tr(BA) = -tr(AB) => tr(AB) =0 here I used * for transpose in order to keep it neat

#

tr(AB)* = tr( B* A*) this can be proved

wintry steppe
#

nice

native rampart
#

Or just writing and expanding the matrix product works

#

Not as nice, But this approach is kinda obvious

round coral
#

yeah, that is a good way too by writing the matrix product

hollow finch
#

so tr(QS)=tr(S*Q*)=tr(-SQ)=-tr(SQ)
because tr(SQ)=tr(QS), we get tr(QS)=-tr(QS) so tr(QS)=0

hollow finch
wintry steppe
#

the matrix inside is being transposed

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not the trace itself

hollow finch
#

oh so tr((AB)*)

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?

wintry steppe
#

mmmhm

hollow finch
#

got it

#

damn that sexy

native rampart
#

It's also nice,that transpose is the only functional on matrices such that f(AB)=f(BA)