#linear-algebra

2 messages · Page 270 of 1

fringe fjord
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Doesn't S contain vectors for all choices of a and b here?

wintry steppe
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For example span({a, b, a+b}) = a(1, 0, 1,) + b(0, 1, 1).

a basis {(1, 0, 1), (0, 1, 1)}, dim = 2

nocturne jewel
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Oh yeah duh

fringe fjord
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In which case {(1,1,1,-1),(0,1,0,-1),(4,2,1,-2)} would be a basis.

wintry steppe
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@fringe fjord sorry im confused... what are you trying to say?

fringe fjord
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I'm suggesting a basis for your span.

dusky epoch
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hold on what

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@wintry steppe can you show the problem exactly as stated please

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as a screenshot maybe

wintry steppe
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Sorry not in English. :( But I have to find a basis if $V = span({a, b, \frac{a}{b^2}, -b}), a, b \in \bR, b \neq 0$.

stoic pythonBOT
wintry steppe
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Basically I have a set of all 2x2 matrices ({a, b}, {c, d})

and a = -d, bc = -(a/d)

dusky epoch
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can you send the screenshot no matter what language it's in? please?

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i have a strong suspicion that you are messing up the notation severely

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and span() does not mean what you think it means

vivid crypt
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hi

dusky epoch
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mate

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do you have

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a PICTURE

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i want a PICTURE not a translation not a transcription just a PICTURE or a SCREENSHOT

wintry steppe
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Sorry, Ann, I do not. And that actual problem does not exist (I just need it to solve something else).

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It just a part of my problem.

dusky epoch
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can you show the whole problem then

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im extremely suspicious of all this

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you're tasking us with finding a basis for something that either isn't a vector space at all or has a very obvious one-element basis

wintry steppe
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Lets try with this.

$X$ is a set of all 2-by-2 matrices $A$ such that $A^2 = 0$. Find a basis for span(X).

stoic pythonBOT
wintry steppe
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We defined a linear span as a set of all linear combinations of elements of that set.

dusky epoch
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okay so you start with the set of all 2x2 matrices whose square is zero and you take the span of that

tall gull
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hey guys

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im only in calc 1 in school but i got a book on linear algebra and its rlly interesting

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ok nvm this question was dumb

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sorry

wintry steppe
dusky epoch
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ok sure that describes a subset of X

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i don't think that'll help you much in finding span(X)

wintry steppe
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And I am stuck because I have never had to find a basis if I have squares or fractions.

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That is the problem...

dusky epoch
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you're confusing this desc of a subset of X with the span of X

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i think span(X) might just be all of R^(2×2) but im not 100% sure about that

wintry steppe
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We need to find a basis for a vector space, right? I am confused.

dusky epoch
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you're confusing yourself on what said vector space even is

wintry steppe
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Take all such matrices and make all linear combinations and find a basis for that vector space.

dusky epoch
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and make all linear combinations

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thats precisely what your desc doesnt capture

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(but i would STRONGLY ADVISE AGAINST trying to make it do that)

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i can say for sure [0 1; 0 0] and [0 0; 1 0] are in our space so its dimension is at least 2

fringe fjord
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If Mate does indeed have all the nilpotent matrices there, then the span does not have dimension 4 because they all have trace 0.

dusky epoch
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oh true

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so span(X) ⊆ {A ∈ R^(2×2): tr(A) = 0}

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hence its dimension is at most 3

fringe fjord
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I think trace and determinant both 0 is a necessary and sufficient condition.

wintry steppe
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That is what I am using here.

dusky epoch
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necessary and sufficient condition for what

fringe fjord
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For being nilpotent, not being in the span.

dusky epoch
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yeah my point exactly

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ok, hold on

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$\bmqty{1 & -1 \ 1 & -1}$

stoic pythonBOT
fringe fjord
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OTOH I found three lin indep members an hour ago, so we are indeed looking at just the trace-0 matrices.

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As matrices we could just take ((0,1),(0,0)) and ((0,0),(1,0)) and ((1,-1),(1,-1)).

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These are all easily nilpotent, independent, and since we agree every matrix in the span has trace 0, there can't be more than 3 matrices in a basis.

wintry steppe
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@fringe fjord and @dusky epoch , thank you very much!!

barren sandal
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What would you guys say are the prerequisites to self learning linear algebra?

nocturne jewel
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Nothing really imo

molten pilot
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What really is the cross product?

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I mean, it seems awfully limiting to create an operation that would only work in R^3

nocturne jewel
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Exterior Product

molten pilot
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What?

nocturne jewel
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but it's just a product that gives a mutually orthogonal vector to 2 other vectors

molten pilot
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Hmmm

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Ig a better way to frame the question is "why does the cross product exist?"

wintry steppe
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one way to look at it is as the vector v x w with <v x w, -> = det(v, w, -). this lets you extend it to any R^n, but then you have to put in n - 1 vectors instead of two

molten pilot
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I didn't quite get that

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What does <v × w, -> mean?

wintry steppe
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for any vector u, <v x w, u> = det(v, w, u)

molten pilot
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Ah, you mean the dot product

wintry steppe
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yes

dapper gorge
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Does the generalized binomial theorem hold for 1/n, where n is a natural number in the case (I+N)^(1/n) where N is nilpotent? Wikipedia assumes the case for n=2. How would you go about proving something like this? N is nilpotent so the formula is just a finite sum, but rather complicated

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Just curious, as I don't even feel too comfortable with power series with just ordinary real numbers

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In mathematics, the square root of a matrix extends the notion of square root from numbers to matrices. A matrix B is said to be a square root of A if the matrix product BB is equal to A.Some authors use the name square root or the notation A1/2 only for the specific case when A is positive semidefinite, to denote the unique matrix B that is po...

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4.4. Jordan decomposition

fringe fjord
# molten pilot I mean, it seems awfully limiting to create an operation that would only work in...

Another answer could be that the cross product is a prototypical example of an antisymmetric bilinear map. Now for each vector space V there's a systematic way to construct a universal antisymmetric bilinear map, meaning a vector space W and a antisymmetric bilinear map f: V×V -> W such that every other antisymmetric bilinear map V×V -> U for any U is the composition of f with a unique linear transformation W -> U.
In general, if V has dimension n, W ends up having dimension n(n-1)/2, so W is cannot be the same vector space as W -- except that n(n-1)/2=n iff n=3. So exacty for 3 dimensions we can choose W to be V itself, and the cross product then turns out to be a possible definition for a universal f: V×V -> V.

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(There are many possible f: R³×R³ -> R³ with this universal property, though, so it's not the entire story. However, the cross product (together with its negative) additionally distinguishes itself by being the only one to satisfy T(v×w) = T(v)×T(w) whenever T is an orientation-preserving rotation, which is nice enough to prefer it. The fact that this is even possible is another low-dimensional coincidence, though).

thorn nexus
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hey, can someone help me?

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with a system of equations

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10x+7y=263
4x+8y=230

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i have to solve for x and y

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bro wtf

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is no one gonna snwerr

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answer

nocturne jewel
thorn nexus
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what

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im in 8th grade

nocturne jewel
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since you're asking here and not #prealg-and-algebra , I'm assuming you're learning Linear Algebra

thorn nexus
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8th grade regents class

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so should we chat there?

nocturne jewel
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You can ask your question there, yes

still lodge
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what material should be covered in college level lin alg class

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for theoretical purposes let’s make it an honors class

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im starting to feel like my lin alg class was lacking and would like to fix that

gleaming knot
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I'm curious, what's lacking?

deft apex
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what did you cover?

still lodge
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i dont have my notebook with me to say exactly (there was no syllabus KEK) the matrix stuff youd expect, eigenstuffs, JCF

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some very light inner product stuff

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cayley hamilton (w/o proof) and some work with polynomials

nocturne jewel
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I mean, sounds typical

still lodge
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and in our last lecture he introduced RCF

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that last bit is what feels lacking

nocturne jewel
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but you can also just add the proof for Cayley-Hamilton in yourself, it's not that hard imo

still lodge
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cuz i remember it looking cool/important and opening up to other stuff

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perhaps im overthinking im just curious what other people might have done in their classes

nocturne jewel
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R^n stuff, abstract vector spaces, inner products, least-squares, transformations/matrices, eigentheory

still lodge
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wdym exactly by abstract vector spaces

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the entire class was done in R2 R3 and polynomial space for me

nocturne jewel
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polynomial space, matrix space, function space

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vectors that aren't coordinate vectors

still lodge
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ah

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ok well he gave us a question involving matrix space on the final which was very cool and good

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but thats it lol

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i’ll probably just try and fill in some gaps then

hushed hedge
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Is it possible to check whether two lines are intersecting with each other only using the affine form?

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If i have this:
x+y+3z+6=0
2x+y-2z-10=0, can i check using the affine form or do i have to make a equationsystem?

queen oxide
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anyone have any ideas for this

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i tried the usual x+yi stuff but it becomes a huge mess and idk if its the right way of doing it

dusky epoch
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consider: |z* + 2i| = |z - 2i|

queen oxide
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or is there a way of doing this without converting to cartesian lol

dusky epoch
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you'll have the equation of an ellipse.

queen oxide
dusky epoch
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no you're overthinking it

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you know the definition of an ellipse, right?

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it's the set of all points for which the sum of the distances to two foci is constant

wintry steppe
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@dusky epoch can I ask you a question

dusky epoch
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why me specifically

wintry steppe
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Cause it's related to LA and you seem knowledgeable

dusky epoch
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you can certainly try but don't expect me to answer immediately

wintry steppe
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How important are polynomials in LA? Thus far we have used them alot in class but from what I've seen in LA books they are not covered excessively

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If you have a good resource on polynomials that'd be great

dusky epoch
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i mean

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i guess they serve as good examples of vector spaces to examine that arent just R^n

wintry steppe
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I see

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Are polynomials in LA used alot in cs?

zinc timber
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(sometimes useful to find the eigen values)

vapid lake
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Let V be the free F2 vector space over {a, b} and let U = {0, a + b} ⊆ V .
What does this mean?

V = {a, b, U} ?

stable kindle
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is this just {0, a, b, a+b}?

subtle walrus
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ye, all F2-linear combinations of a and b

wintry steppe
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One quick question: i have a 2x2 matrix C, a 2x3 matrix A and a 3x2 matrix B such that AB = C, now i want to show that C is invertible, i was wondering if it suffices to show that both A and B have rank 2

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I already forgot linear algebra lol

zinc timber
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AB=C does not necessarily mean C is invertible, even if A and B have rank 2

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$A = \m{1 & 0 & 0 \ 0 & 1 & 0}, B = \m{1 & 0 \ 0 & 0 \ 0 & 1}, C = AB = \m{1 & 0 \ 0 & 0 }$

stoic pythonBOT
wintry steppe
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Ah damn you are right

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Ye i think it was rank(AB) <= min(rank(A), rank(B)), not "="

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Any advice what i could try here?

zinc timber
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you need to be more specific about your problem

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it's too vague

wintry steppe
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Its a little bit much to explain, but i think i will just brutally calculate it. Thanks!

haughty berry
wintry steppe
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why is 0 a vector and 1 a scalar ?; can't 1 be a vector too ?

broken notch
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What's the best book for numerical linear algebra?

zinc timber
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0 is taken as an element of the vector space V, whereas 1 is taken as an element of the field

wintry steppe
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why is 0 not a scalar too then ?

zinc timber
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if you take it as an element of F then yes

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if it confuses you, take $0_V \in V $ and $0_F \in F$ to distinguish them

stoic pythonBOT
wintry steppe
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So multiplying by the zero vector is the same as multiplying by the scalar 0 ?

tranquil steeple
broken notch
tranquil steeple
wintry steppe
broken notch
tranquil steeple
wintry steppe
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Yes

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You can write 0 for the 0 scalar and the 0 vector, if v is a vector and you write v + 0, its clear that its the 0 vector here. If you write 0*v then its clear that its the 0 scalar here

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now im confused

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But v + 0 makes no sense if 0 is meant to be a scalar

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Yes, vector addition and scalar multiplication

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So you can add vectors together and you can scale them, but nowhere it says that you can multiply vectors

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You know what i mean?

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yeah

wintry steppe
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why are there two Rs ?

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C(R) makes sense

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but F(R,R) doesnt

teal grotto
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F(R,R) is the space of all functions from R to R

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im not sure why they were inconsistent

wintry steppe
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yeah if so why not write C(R,R) ?

teal grotto
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typically, you will see C(X,Y) denote the space of all continuous functions from X to Y, and if X = Y, its shortened to C(X)

teal grotto
wintry steppe
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i see

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thanks

vapid lake
subtle walrus
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a + a = 1*a + 1*a = (1 + 1)*a = 0*a = 0

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so you get b

hearty rapids
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can someone eli5 what a linear transformation is to me

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all i can understand is you're changing the dimensions of a vector

wintry steppe
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do you know what a vector space over a field is?

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or do you want to keep it to R^n

hearty rapids
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ooh no idk what a vector space is

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should i learn what a vector space is first?

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the video series i was using didn't teach the vector space before they did the linear transformation

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for context this is the video

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ik what a span of vectors is

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a span is just the set of all linear combinations of v1,..., vp

silver cradle
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im not familiar with the cauchy schwartz inequality, could someone explain how i would go about using it here?

nocturne jewel
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$\abs{u\cdot v}\leq \norm{u}\norm{v}$

stoic pythonBOT
nocturne jewel
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That's cauchy schwarz this

silver cradle
nocturne jewel
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yeah, abs value CS-Ineq QED

silver cradle
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would this be trivial if we assume the first property?

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i was thinking maybe they did not want us to use it in that case then

nocturne jewel
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trivial based on what you just proved tbh

silver cradle
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gotcha

static jasper
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can someone help me putting this matrix in superior triangular?

drifting scarab
vapid lake
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On transformation,
T : V → W be the unique linear transformation such that T(a) = c + d, T(b) = c + d. where V ={a , b} and W = {c , d}. Im trying to find kernel and image of this

halcyon spindle
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The image would also be the only element in W which is 0.

halcyon spindle
wintry steppe
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norm

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it explains this below

spring oriole
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What's a good linear algebra textbook for someone that needs to relearn linear algebra

dapper gorge
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In most cases, we say that a subset S of some inner product space is orthogonal if given any two elements x,y in S, x and y are orthogonal. What if there are no two distinct elements in a set? Do we consider the set {x}, where x is non zero, to be orthogonal? Although by definition ⟨x,x⟩>0, but I'm wondering if this is a special case

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In a text I'm using I think this assumption is made

wintry steppe
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post text

dapper gorge
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ok

wintry steppe
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S should be orthogonal if that condition holds for distinct elements

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otherwise the only orthogonal set is {0}

dapper gorge
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This is Stephen Friedberg (and some other authors) text

wintry steppe
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note "distinct"

dapper gorge
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yeah

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I have pointed that

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So what about the case {x}? i.e., a set where there are no distinct elements?

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Again, if x is non zero (x,x)>0, but idk

wintry steppe
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singleton is vacuously orthogonal

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there's no other element in {x} to take the inner product with

dapper gorge
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This is a question on definitions

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I don't think the definition above adresses the singleton set

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?

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If it does I don't see it at least

wintry steppe
dapper gorge
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According to what definition of orthogonality of sets?

wintry steppe
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the one in the book

dapper gorge
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btw

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I'm not questioning singleton set is not orthogonal, just a matter of definitions

wintry steppe
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the book's definition doesn't assume there are actually two distinct vectors in S to take the inner product of. it says if there are, then their inner product is zero

dapper gorge
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which I'd like to understand rigorously

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gocha

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thank you

wintry steppe
vapid lake
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How many elements are in the free F2 vector space over S when S is a set of n elements? F2 should include the basis, im not sure how it affects the dimension

zinc timber
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free F2 vs of dim n has 2ⁿ elements

vapid lake
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why @zinc timber

zinc timber
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basic fact about vector spaces

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$F_2^n ={ (x_i, x_2, \cdots, x_n) | x_i \in F_2 }$ you have 2 choices for each $x_i$ so $2^n$

stoic pythonBOT
thorn cypress
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is the dot product iv.iv = ||v| |^2 where i is the imaginary

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and v is complex vector

zinc timber
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yes

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$\ip{iv, iv} = i\ip{v, iv} = i \bar{i} \ip{v, v} = \ip{v, v} = \norm{v} ^ 2$

stoic pythonBOT
quartz compass
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I would have said no by how I interpreted the question, since I interpret the dot product to be distinct from the inner product

zinc timber
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dot products are inner products, so component wise multiplication (that u r calling dot) is not an ip

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so can't be a valid dot (ip)

quartz compass
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I'm saying without asking the person who asked the question, it's ambiguous

wintry steppe
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What does direction ratio/number mean geometrically in 3D??

errant palm
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i cant figure out how they got this answer, can someone pls help me? ty

wintry steppe
errant palm
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oh hbooy

gentle relic
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Can u pls help me understand augmented matrix

hushed hedge
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determine all the vectors that are orthogonal to u = (2,0,4) and v = (-1,2,3), aren't you suppose to use the cross product for u x v? I get (-8,-10,4) but that's wrong

dusky epoch
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you've determined just one vector orthogonal to both u and v

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you're not trying to claim it's the only one in existence, are you?

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@hushed hedge

hushed hedge
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ah sorry

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are there more? is v x u another vector orthogonal?

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actually v x u is wrong, if u x v is one vector, how do i find the second one?

dusky epoch
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there are not just two such vectors

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theres infinitely many of them

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consider: scaling u × v by 2 would still yield a vector orthogonal to both u and v

hushed hedge
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right

dusky epoch
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scaling it by 3 would yield yet another vector

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and so on

hushed hedge
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but how does my book get t(4,5,-2)?

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i should make a equationsystem right? To figure it how they behave (?)

dusky epoch
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your book knows that the vectors orthogonal to u and v form a line going through the origin

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and u×v is just one vector on said line

hushed hedge
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aha ok

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i didn't look at it that way, thanks

halcyon spindle
gentle relic
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like jee main level if u know jee

fickle citrus
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It's just vocabulary

gentle relic
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like ... ? i did not get you

dusky epoch
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"augmented matrix" is just a name

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it's what we call the matrix A with the column b attached to it on the right

fickle citrus
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It's specifically referring to attaching the coefficients to the original matrix

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^

dusky epoch
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(where A and b come from your linear system, Ax=b)

gentle relic
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oh ok

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so like its transformation of matrix

fickle citrus
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no, it's a more compact way of writing everything

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writing everything out explicitly

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Since the x does not matter

gentle relic
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ohh like just the way a person denotes it ok

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o ok got it

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thanks

wintry steppe
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i think it's genuinely confusing when students are asked to try interpreting matrices, and then we say "oh yeah and this augmented matrix is just like, better for rote row reductions, lmao"

severe nymph
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x²+(y-3√2x)²=1 solve this equation

zinc timber
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no

haughty berry
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^ KEK

hearty rapids
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so all a linear transformation is

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is checking if T( vector u + vector v) = T(vector u) + T(vector v)

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which is the first condition

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and then

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T( c * vector u) = c (T * vector u)

gray dust
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yes

hearty rapids
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oh then that's simple

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i got tons of practice to do lmao

crystal plover
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Yo, is this legit?

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wolfram gave me x=8 as the answer

fringe fjord
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Looks good to me.

crystal plover
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thx

polar marsh
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i have a problem from my linear algebra exam that i couldn't solve

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let B is an element of M_n(R) and we now that BB=B and that B^T * B=BB^T, we now have to show that this implies B=B^T

golden ermine
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Try showing that B^T = (B^T)^2

polar marsh
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you can transpose both side

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s

nocturne jewel
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then dont ask anything

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Yeah, we don't care for stupid questions. You're not obligated to ask anything.

crystal plover
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ok another question, wolfram tells x=67 but i don't really know how to get it :/

winter harbor
# polar marsh let B is an element of M_n(R) and we now that B*B=B and that B^T * B=B*B^T, we n...

$\cdot$ (Part 1 : The Idea)

If you have a any matrix $B \in \mathcal{M}_{n}(\mathbb{C})$, then it is always the case that:
$$
\langle Bx, y \rangle = \langle x, B^{\ast} y\rangle
$$
Where $B^{\ast}$ is the adjoint of B, i.e its conjugate transpose, $x,y \in \mathbb{C}^{n}$ and $\langle \cdot, \cdot \rangle$ is the hermitian inner product on $\mathbb{C}^{n}$.

Since we are over $\mathbb{R}^{n}$, then the adjoint is just the usual transpose and the hermitian inner product is just the euclidean inner product on $\mathbb{R}^{n}$. So in any case, we have that:
$$
\langle Bx, y \rangle = \langle x, B^{t} y \rangle
$$
Still holds. Moreover, we have that, by definition:
$$
\langle x, y \rangle = x^{t} y
$$
For any two vectors in $\mathbb{R}^{n}$.
\
\
With this is mind, we can now prove your result by showing that for any two given $x,y \in \mathbb{R}^{n}$, we have that:
$$
\langle Bx, y \rangle = \langle B^{t} x, y \rangle
$$

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Is this good enough so far?

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I will write down the proof now

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I just wrote down a few definitions to see if we are on the same page

stoic pythonBOT
#

MISTERSYSTEM

wise oriole
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can someone explain this

polar marsh
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exactly what is in my textbook

winter harbor
#

Hmmm

winter harbor
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But there's a really simple proof that just got to my mind

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Since B^2 = B, then unless B = Id or B = 0, then the minimial polynomial of B is p(x) = x(x-1). In the case B = Id, then the minimal polynomial is just p(x) = x - 1 and in the case B = 0 we have that p(x) = x.

In any case, the only eigenvalues of B are either 1 or 0, which are all real.

Moreover, since BB^t = B^t B, then B is a normal matrix. Since B is a normal matrix with real eigenvalues, then B is hermitian, and as a consequence of B being a real matrix it is also symmetric; i.e B = B^t (as a consequence of the spectral theorem)

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If you still haven't seen the spectral theorem for normal matrices in your class

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You probably can't approach the problem like this tho lmao

zinc timber
#

I think I have an different approach to this problem, we already know that $B$ is diagonalizable with eigen values $0, 1$. Now If we could show that $E_0$ and $E_1$ are mutually perpendicular, then we'll be able to find an orthonormal basis that makes $B$ into a diagonal one, which would imply $B^t = B$. \

Now we see that $B^tB = BB^t$ i.e. they commute implying they preserve each others eigen spaces, which can be seen by following, let $v\in E_0$ of $B$ then $B^TBv = 0 = B B^Tv \imply B^Tv \in N(B)$.

stoic pythonBOT
#

Compile Error! Click the errors reaction for more information.
(You may edit your message to recompile.)

dusky epoch
#

k0 - 2k1 = 0
k2 +3(k3) = 0

however there seems to be no solution.

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how are you getting that there is no solution

#

you claim the system $\begin{cases} k_0 - 2k_1 = 0 \ k_2 + 3k_3 = 0 \end{cases}$ has no solutions at all?

stoic pythonBOT
dusky epoch
#

im adhering to your notation here btw, even though it is a little wonky (though not in a way that seriously affects anything)

#

does all this resolve your question

#

there are much less wonky ways of saying that but yes

polar marsh
#

i can't find really something on normal matrices in my book

#

we have just seen that if a matrix is hermitian then its eigenvalues are real

barren sentinel
#

guys i need some help

#

i have got these matrices which apply transformation to the world coordinates to convert it into image coordinates

#

(for a camera)

#

how would i do the opposite?

devout hedge
#

Are there any websites with linear algebra lessons?

zinc timber
#

yes youtube

devout hedge
#

Any specific channel?

lavish jewel
#

gilbert strang's MIT OCW

devout hedge
#

👍

barren sentinel
#

how do u invert R4 to R3?

#

do i need to transpose or something?

#

or its just not possible?

dusky epoch
#

what do you mean by "invert R4 to R3?"?

odd kite
#

yes do you mean a linear function from R4 to R3 for example

slim cedar
#

Probably a very simple question, but given a d times d matrix A, and two vectors x,y in R^d, can i say anything about <Ax, Ay> if Det(A)=1?

barren sentinel
# barren sentinel

trying to make a backwards imaging mordel but i understand that i cant invert 4x3 matrix 🤔

slim cedar
#

surely the inner product is the same as <x,y> right?

barren sentinel
#

idk if this is correct

#

but i hope it is

#

this is the diagram btw

versed rock
#

So, if i have these 2 vector [2, -4] and [-1, 2]. Can i say that [x, y] = [2, -4] + t[-1, 2] , right?

nocturne jewel
#

however they're parallel vectors

odd kite
#

@barren sentinel can you link the whole document or give some more context

versed rock
#

Exercise 18 and 19 should be trivial right?

#

I Know it's true, but i don't think the way i do it is right

odd kite
#

18 is

versed rock
#

,rotate

stoic pythonBOT
nocturne jewel
versed rock
#

How can i prove 20 and 21?

#

21 for me looks right, like, intuitively i know this

nocturne jewel
#

show that an element from span(S) is in span(T)

#

like any other subset proof

versed rock
#

Like this?

nocturne jewel
#

yeah, just make c_i = 0 for all i b/w k+1 and m

#

$v=\sum_{i=1}^k c_iu_i=\sum_{i=1}^k c_iu_i+\sum_{i=k+1}^m 0u_i$

stoic pythonBOT
hushed hedge
#

My book writes the basis for the zero vector space like this: (-1,5,3), is it equivalent to (1/3,-5/3,1) ?

nocturne jewel
#

you mean nullspace or kernel

hushed hedge
#

Yeah, i mean nullspace. Thanks!

forest wave
#

what steps do I need to do this simplification?

wintry steppe
#

factor the quadratic

forest wave
#

hmm

#

go on

wintry steppe
#

that's it

#

all you have to do is factor the quadratic

forest wave
#

well how do I do that?

wintry steppe
forest wave
#

actually I figured it out

vast bobcat
#

I don't remember how to answer these

#

can anyone help with with steps for 8. a at least

fringe fjord
#

The first step would be to reread the section in your textbook (or lecture notes or whatever) that describes diagonalization of matrices.

#

(If you're looking for a mindless step-by-step procedure, you might end up doing a lot more work than if you exploit the specific features of each example anyway).

vast bobcat
keen sierra
# vast bobcat can anyone help with with steps for 8. a at least

You know that if $A$ is diagonalizable, then the diagonal elements of $P^{-1}AP$ will be the eigenvalues of $A$. And you know the columns of $P$ will be eigenvectors associated with those eigenvalues. So if you don't see any obvious shortcuts, you may as well proceed by finding eigenvalues.

stoic pythonBOT
#

OurBelovedBungo

dull rose
#

I don't understand how these vectors becomes a line, and I am not sure how to do the vector equation.

#

This is the answer.

golden ermine
#

Well: the vector < 2, 4 > is just 2 * < 1, 2 > and similarly, < -3, -6 > = -3 * < 1, 2 >

#

So these vectors also belong in the span of < 1, 2 >

dull rose
#

but then I could make the same argument for < 2,4 > since it equals 2 * < 1,2 > and (-2/3) * < -3, -6 > ? And therefore wouldn't this make the vectors belong in the span of < 2,4 >? Or is < 2,4 > acceptable too?

golden ermine
#

That’s fine too

#

We just prefer < 1, 2 > over < 2, 4 >

dull rose
#

Oh alright, thanks!

compact tartan
#

if i have to put one more matrix in reduced row echelon form I am going to combust

exotic horizon
#

is there a faster method to calculate the inverse of this method or do I need to calculate the minor matrixes every time ? I know how to calculate the determinant here already

wintry steppe
#

pairing it with the identity, row reducing it itself to the identity, and taking the new matrix seems especially feasible as this is a triangular matrix

exotic horizon
#

I thought that this could only be used to calculate the determinant? Isn't the new matrix just the identity of this one ?

zinc timber
#

wym?

#

you calculate the inverse using row reduction

sharp shell
#

the difference between A*A^T and A^T * A is that the first one has the dot product of the the coloms on the diagonal and the second the dot products of the rows correct?

fringe fjord
#

It's the other way around. (And it's not just the diagonal).

exotic horizon
zinc timber
#

No you attach the identity matrix with it

#

$\left[\begin{array}{cc|cc} 1 & 2 & 1 & 0 \ 3 & 4 & 0 & 1 \end{array}\right]$ for example

stoic pythonBOT
exotic horizon
lavish jewel
#

the one on the right, where the identity matrix originally was

pliant kayak
#

can you do the LU decomposition with a non quadratic matrix?

tranquil steeple
pliant kayak
#

thanks

wintry steppe
pliant kayak
#

if you multiply a row with -1/3 for example by doing the LU decomposition, how do you change the matrix L? I.e. here the second line has everywhere -1, if I wanna take that away, what do I have to do in Mat L?

lavish jewel
#

you can put a -1 in the corresponding diagonal element

pliant kayak
#

but what if I multiply with -1/3, do I have to put a -3?

lavish jewel
#

right

#

idk if this makes it clearer, so that you don't mix the two up. you're really doing L (L^-1 A)

#

so if you multiplied by -1/3 and you want the matrix to still be A, you need to do the inverse transformation too

#

which is -3

pliant kayak
#

I'm asking cause I did it, but it didn't work 💔

#

so I guess I'm making a mistake

lavish jewel
#

do notice that doing this essentially does nothing

#

you have to keep the two matrices separate

wintry steppe
#

y is supossed to be 7/38 what did I do wrong?

clever karma
wintry steppe
#

ooooh

#

Now it comes out right

hearty rapids
#

is #5 just about getting it into reduced row echelon form?

#

i tried swapping row 1 with row 4 to get row 4 on top so there is a 1 on the top left corner

#

actually no it seems like swapping the third row with the first row is the better approach

#

sigh

#

ok i figured it out

#

x4 has to be a free

lucid rose
#

What does one dimensional flat mean?

#

Is it one free parameter?

lavish jewel
#

it's a line that doesn't necessarily pass through the origin

lucid rose
#

When is the set of solutions a one dimensional flat

lavish jewel
#

when the n-1-dimensional flats defined by the rows of the matrix intersect in a line

#

that would indeed be the case when you have one free parameter

#

since then the solution would have a particular term, call it x0, and then a null space component, let's say xn

#

so that the solutions are of the form x0 + c xn for some scalar c

lucid rose
#

I’m guessing for two dimensional flat it would be 2 free parameters?

lavish jewel
#

sounds about right

lucid rose
#

What about when the set of solutions is a single vector

#

What does that mean

lavish jewel
#

there's a unique solution

#

just the point described by that vector

lucid rose
#

So say if it’s like R^4

#

If the solution is a single vector

#

Then x1-x4 all have one possible solution

exotic horizon
#

do any of you know a resource where I could learn LU decomposition? It's still very confusing to me and I struggle with what I'm finding online

sleek spruce
#

replace x1 with x and x2 with y to help conceptualize it

sleek spruce
#

even if you replace it with z, you get a plane

#

but in a different axis

#

just let the grader know that x1 = x

#

and x3 = z

#

the purpose of the homework is to practice sketching in 3d, so both answers would work

#

if you really wanted to, you could do it for xy, xz, yz

soft moss
#

can someone help with this one please?

zinc timber
zinc timber
sharp shell
#

whats the cross thingy for?

#

alternative to + for psuedo inverse or somthing else

nocturne jewel
zinc timber
#

phys guys use it for adjoint

sharp shell
#

so what do I take it for if I see it in lin algebra context

zinc timber
#

idk check yr textbook what they have mentioned

odd kite
lavish jewel
#

i would really suggest to check in the book, i've just as often seen * and H for conjugate transpose

odd kite
#

but usually when that's the case, no daggers appear I think

lavish jewel
#

in those cases the dagger can mean pseudo inverse or something like that

#

if abdos showed the RHS, it would help

zinc timber
#

physicist messed things up again

dusky wadi
#

what's an orthogonal projection

#

linalg done wrong asked for it without explanation

dusky epoch
#

context?

dusky wadi
#

an orthogonal projection matrix from R² to the line x_1 = -2x_2

zinc timber
#

means you project onto a subspace along it's orthogonal complement

dusky wadi
#

context: I'm in chapter 1
they've barely introduced matrix multiplication

zinc timber
lavish jewel
#

are you sure you're supposed to be seeing how to solve this yet? 😛 have you done more abstract linear algebra before?

dusky wadi
#

I was just trying to parse what an exercise meant

lavish jewel
#

have you seen orthogonality?

dusky wadi
#

no

lavish jewel
#

just leave the problem for later

dusky wadi
#

this may be a problem with the texbook

zinc timber
lavish jewel
#

sounds like it

zinc timber
#

LA done wrong for a reason

dusky wadi
#

lol

#

I'll come back to it eventually

zinc timber
#

yeah read ahead like me then come back catThink

dusky epoch
#

can i have a pdf and page reference

dusky wadi
#

pg 33 ex 5.4

lavish jewel
#

a quick ctrl f search says that is the first occurrence of "projection" in the book

dusky wadi
#

oh oof

lavish jewel
#

this book is like, hint:

dusky wadi
#

it's just like

#

once in a while

#

treil forgets where in the texbook he is

lavish jewel
#

page 1: the end

pastel brook
dusky wadi
#

it's pretty good otherwise

halcyon spindle
#

He later asks you in the next section to find the matrix of the rotation around (2,2,3)^T after introducing invertible linear transformation.

unborn heart
#

i think you can still solve this problem by thinking projection as like an "informal everyday word" without formally knowing what projection is

halcyon spindle
#

He hint was confusing, “imagine your on the tip of the vector looking down towards the tail” or something.

unborn heart
#

very informally, if you were to project the blue point onto the red line, it would go to the green point

dusky wadi
#

ohhhhh

#

thanks

wintry steppe
#

Guys can i show that something is true by logic and not by using math? I explain: If I am consider Grassmann's theorem can i prove that it's true by logic and not by mathematical process? because to me is more easy

gleaming knot
#

Cool question. Yes, a proof by logic is a mathematical proof. To think otherwise would be a pretty weird misconception

#

After all, math is logic and logic is math

wintry steppe
#

Yes, you are right.. and sorry for my english but i come from italy and i'm try doing my best

agile plover
#

Are there any tricks of linear algebra that would allow me to compute a multivariate Gaussian likelihood without a full matrix inversion?

#

$e^{-\frac{1}{2}\sum_i(x_i - \mu)^tS^{-1}(x_i - \mu)}$

stoic pythonBOT
agile plover
#

x, mu are d x 1, S is d x d, so this becomes 1x1 at the end. there are tricks for sampling from a multivariate gaussian, where you only have to do either a cholesky or LU decomposition, but those aren't used for calculating likelihood.

waxen turret
#

how do we solve this kind of problem??

zinc timber
little frigate
#

Let A be a 3x3 matrix and consider the invariant that AD = 0

#

how could one possibly find all the matrices D that would fit that condition

zinc timber
#

AD =0 means cols of D are in null A

little frigate
#

null A being... what people often refer as null space?

zinc timber
#

ye

little frigate
#

mmhm, the course started one week ago...

#

unless the concept itself is simpler than I think it is

#

I don't think we're being expected to know that- I only personally know that because I've already heard about it outside of that class context. It will be seen later

#

Here's what the matrix A looks like, I think that helps since it's filled with essentially 1s and zeros for the most part, so perhaps some technique could be preferred

#

I think that the two following propositions could help although

#

For clarifications purposes, B_1 ... B_n corresponds to the columns of B

#

so there definitely seems to be something revolving around columns hmmm

#

Oh

little frigate
ripe birch
#

any idea how to approach this? A is just some arbitrary operator and a_n is an eigenvalue of that operator (and apparently it's multiplied into an identity matrix that isn't shown so that it can be subtracted from A).

My first thought was come up with a formula for the nth degree polynomial of (A - a_n)^n and see what kinda magic I could do but I don't really don't see anything. I do have a solution manual to this but I don't really follow a key step, and it may not make any sense to math people since it's a physics problem written in physics form

dusky epoch
#

sounds vaguely like cayley-hamilton

viral magnet
zinc timber
#

what if n doesn't have enough eigen values? what if min poly has an irred factor?

#

is your field ℂ?

viral magnet
#

I guess it's also nice to prove that every term in the product commutes. So you can just move the term to the front and get the zero vector right away

ripe birch
#

Looking into Cayley-Hamilton theorem. Seems like it could be related.

@viral magnet so the solution does say to have it act on what's essentially some arbitrary state vector. Not sure where a 0 will come from yet, but I'll keep looking.

@zinc timber I wouldn't think too much into it for that first question. If that 2nd question is asking if it can be complex (im not all that familiar with math terms yet) then yes it can

#

why do you say one of the terms will zero out?

viral magnet
#

Take just a 2x2 matrix with distinct eigenvalues

zinc timber
#

(if F=R² the you cannot write $A=\m{\cos 1 & \sin 1 \ -\sin 1 & \cos 1}$ in that form)

stoic pythonBOT
zinc timber
#

that's why I asked whether the field is ℂ of not

viral magnet
#

@ripe birch
Write an arbitrary vector as a linear combination of eigenvectors. So for 2x2 you have a sum of two vectors say lam1 * v1 + lam2 * v2 where v1 is an eigenvector corresponding to a_1 and similarly for v2.

Calculate (A-a_1 I) * (lam1 * v1) and similarly for v2

ripe birch
#

trying that real quick

#

oh that's wild

#

they do each go to zero dont they

weak needle
weak needle
ripe birch
#

seems so weird to work. Only thing im caught up on is explaining why our arbitrary vector can definitely be written as a linear combination of eigenvectors. I'm assuming not every vector can be but no basis for that??

#

@weak needle beat me to it

weak needle
#

yeah so cayley hamilton is the way to go

zinc timber
#

can be written as an LC of generalized evs

viral magnet
#

You learn the Cayley Hamilton theorem in physics class?

zinc timber
#

(given field is ALC)

ripe birch
#

bro we don't learn ANYTHING about formal math in physics class. They gave us 1 month of LA, 2 months of ODEs, 3 months of PDEs, and random other crap

#

i like me some math dont get me wrong, i just am not up to speed on the fields that we use as much as I'd like to be

ripe birch
#

like @zinc timber you speakin another language to me rn

viral magnet
#

It's a physics class, they throw words like eigenbasis around like it's given

zinc timber
#

(ignore)

#

(that's why I'm enclosing them in paren)

weak needle
#

and 1 in that entry

ripe birch
#

my favorite part was when my professor said "a Hilbert space, just so far as what you need to use it within this class, is some place where you can do calculus". Kind of a paraphrase but you get the gist. We're basically bullied

#

The internet and this discord is how I learn my math

zinc timber
#

hilbert spaces are good tho

#

most well behaved

viral magnet
zinc timber
#

like an obidient pet

zinc timber
viral magnet
#

Right, a simpler proof I believe

ripe birch
#

am I gonna need to know what a ring is to figure out this cayley-hamilton theorem?

ripe birch
#

riemann i like your showing a lot, i just don't know if i can justify the arbitrary vector consisting of eigenvectors

viral magnet
#

You don't need Caley Hamilton for a physics class

ripe birch
#

are any of you familiar with bra-ket notation from quantum mechanics? I think there's a math equivalent of some sort but I'm not sure

#

in other words. Does this look anything like something you'd be familiar with?

#

where that alpha ket is basically a vector

lavish jewel
#

sure, kets are vectors and bras are linear functionals

viral magnet
#

Yea I am

viral magnet
ripe birch
#

bless. So I follow up until the start of the 2nd line. Looks like operator A just turned into a'' from nothing i dont see it

viral magnet
#

Or vectors in the dual space

ripe birch
#

i'm almost positive that's the case. dual space sounds super familiar from my textbook

lavish jewel
ripe birch
#

@zinc timber This is wizardry

viral magnet
zinc timber
#

if the space is reflexive then they are same, ex for hilbert spaces, they are the the same

lavish jewel
#

yep it looks like they're decomposing the vector into a basis of vectors a''

viral magnet
zinc timber
#

yes but why are they assuming there is such a basis

lavish jewel
#

linear functionals map to the base field, not to kets

zinc timber
viral magnet
#

Bras return a complex number when applied to the kets

lavish jewel
#

they take kets and return elements of the field

#

linear functionals are linear forms, not just linear maps

zinc timber
#

wth is happening here stare

ripe birch
#

so back to what you said @viral magnet . I see that |a''> is the eigenvector. is the a'' that appears in (a''-a') the eigenvalue from having A apply onto our ket?

lavish jewel
#

idk, riemann saying linear functionals map vectors to vectors

zinc timber
#

lol

#

(technically the truth)

lavish jewel
#

if you treat the base field as a vector space, sure

viral magnet
#

Right, a bit messy on my part. Vectors are functions in Hilbert spaces

zinc timber
#

not always

ripe birch
#

AcHkTuAlLy

viral magnet
#

Oh shit in uncountable Hilbert spaces

zinc timber
#

(not all vs are hilbert spaces)

viral magnet
#

Or countable I forget

zinc timber
#

(nothing to do with the coutability)

ripe birch
#

so my question was that A just turns into a''. You mentioned that a'' was an eigenvector. When A turns into a'' it's still an operator and not a vector, so I'm assuming the a'' you mentioned being an eigenvector was the other a'', not the one I inquired about. Hope that clarifies it. Kinda weird to word

viral magnet
ripe birch
#

🙂

viral magnet
#

Can you rephrase it and use kets where you mean the vector and no kets when you mean eigenvalue

ripe birch
#

Sure. So we have a line which says (A - a') | a'' >

#

the following line has (a'' - a') | a'' >

#

with seemingly no other changes. so operator A just turned into the operator a'' (times identity matrix ofc) and it seems random

#

ill repost the pic to have it less buried

viral magnet
#

All uses of little a are either eigenvalues or eigenvectors

#

So A|a> = a |a>

zinc timber
lavish jewel
#

this notation is super unfriendly :x but as riemann says, the transformation A | a'' > yields the eigenvalue corresponding to the eigenvector | a'' >

ripe birch
#

So this theorem only works on kets which are eigenkets of A?

lavish jewel
#

and here they have simply removed the | > to denote an element of the field instead of a vector

#

this would honestly look so much simpler if you were to use matrix notation lol

viral magnet
#

Wtf now eigenket's a word

ripe birch
#

😂

viral magnet
#

Next thing you know they'll make up eigenSchrodinger

ripe birch
#

listen we're physicists for a reason. we live to brutalize your field

oblique prairie
#

i’m just lurking but i was about to say what the heck another eigen thing

ripe birch
#

eigenket is just an eigenvector in whatever dual space that is

lavish jewel
#

i'm not even a mathematician, this is just bad notation right now opencry overloading of the same symbol

viral magnet
ripe birch
#

I'm gonna eigenFreakTheFuckOut this semester

zinc timber
#

sometimes they look nice

lavish jewel
#

i can give you an alternative explanation using matrices and vectors

zinc timber
#

but this is not one of those moments

lavish jewel
#

if you'd like. otherwise, i'll leave you two be

ripe birch
#

yeah that works. Does this theorem only work on eigenvectors? or does it produce null kets on ANY vector?

zinc timber
#

like wtf a'', a and a' all together

viral magnet
#

Someone take eigenBruh to be the dual of eigenKet

lavish jewel
#

this works for diagonalizable operators A

ripe birch
#

and it does not matter if the vector this operator combination acts on is an eigenvector of A or not?

lavish jewel
#

it doesn't, because if the operator is diagonalizable, its eigenvectors can be used to span any vector it acts on

viral magnet
#

"All operators are diagonalizable" --physicists

zinc timber
ripe birch
#

@viral magnet you're not wrong 🤷

lavish jewel
#

then by linearity, it boils down to using A on several eigenvectors

lavish jewel
zinc timber
ripe birch
#

all operators are also linear and hermitian and have real eigenvalues

#

🙂

lavish jewel
#

also, all series converge

ripe birch
#

and if they don't

#

we approximate them to be 0

lavish jewel
#

anyway. do you want the matrix vector explanation?

ripe birch
#

oooo plz

lavish jewel
#

-1/12

#

ok

ripe birch
#

LMAO

lavish jewel
#

so let's say there is a diagonalizable matrix A, which has eigenvectors v_i with eigenvalues a_i

ripe birch
#

physics notation be like

zinc timber
#

(i actually prefer dot notation over d/dt)

lavish jewel
#

and we make a product pi_n (A - I a_i), where I is an identity matrix

#

the matrix (A - I a_i) has the eigenvector v_i corresponding to a_i as an element of its null space

dusky epoch
#

$\mathit{\imath}$

stoic pythonBOT
dusky epoch
#

charge

lavish jewel
#

one can additionally decompose any vector u into a linear combination of the eigenvectors e_i, which in the proof were also assumed to be orthogonal, apparently

ripe birch
#

oo we're gettin into slightly spooky territory with the jargon, but ill try to follow

#

i thought we said earlier that perhaps not every vector can be written as a l.c. of eigenvectors

zinc timber
#

(why not just use Cayley hamilton )catThin4K bleakkekw

lavish jewel
#

you can do a change of basis into the eigenbasis by doing a transformation V, a matrix whose columns are the eigenvectors v_i, and doing V V^T u

ripe birch
#

oooo is this the gram-schmitty process?

#

or different

lavish jewel
#

sure

ripe birch
#

let's go

zinc timber
#

no they are different

#

you may not necessarily have orthogonal eigen vectors

lavish jewel
#

the proof they showed kinda assumed they were

#

they're just orthogonally projecting on the eigenvectors lmao

ripe birch
#

i believe in quantum we always form an orthonormal basis with our eigenvectors

lavish jewel
#

now the trick is that V V^T u is a sum of eigenvectors

#

so when we consider A - I a_n, the operator can be replaced by a_j - a_n, where a_n is indexed by the big Pi in front, and j is the index of an eigenvector's corresponding eigenvalue

#

p_n (a_j - a_n) V V^T u is then 0,

#

since each eigenvector will be multiplied by some term (a_j - a_n) such that n = j

#

for completion, it seems the assumption made was that A is self adjoint

#

diagonalizable in an orthogonal basis

#

since the proof used orthogonal projections and assumed decomposition in an eigenbasis was possible without ever saying anything about it

ripe birch
#

i can nearly assure you that assumption is correct. we jump to conclusions more than a clingy ex-gf trying to win you back

lavish jewel
#

the proof you shared definitely made that assumption

#

the first step they write is "decompose the ket into the eigenbasis through orthogonal projections"

#

which is what i did with the V V^T, where V's columns are eigenvectors and therefore V is orthogonal, so that V V^T = I and doesn't affect the result

#

then in the eigenbasis, linear transformations are simply scaling factors

#

anyway, yes. orthogonally diagonalizable A

#

if not, you need something different for the proof

zinc timber
#

ye like m(x) be mini poly so some power of that poly will be divisible by m(x) which makes it nilpotent kekw starebleak

ripe birch
#

so let me see if i understand this correctly. We take some arbitrary vector, and we project it onto the eigenbasis. Doing that allows the operator A to extract those eigenvalues a_j and eventually filter for where j=n?

lavish jewel
#

almost

ripe birch
#

ill take an almost. that means im close. What isn't quite right there?

lavish jewel
#

once you have the vector in the eigenbasis, you replace A with the eigenvalue of the corresponding eigenvector

#

then if you want you can use pigeonhole principle for the product part lol

#

if you have n pigeons and drill n+1 holes into then, then at least one pigeon has 2 holes

zinc timber
#

lol

viral magnet
#

Pigeonhole? More like pigeontroll

ripe birch
#

so by simply putting our vector into the eigenbasis, A MUST be replaced with the eigenvalue of the eigenvector I projected onto?

#

oh i guess. because when A acts on it you get that eigenvalue

lavish jewel
#

right

#

you don't HAVE to

ripe birch
#

but you'll get it anyway

lavish jewel
#

but if you don't, then doing this doesn't help you prove the thing

quartz compass
#

lmao

ripe birch
#

ok talking about the projection thing really helped, i appreciate that. I could feel the answer on the tip of my tongue but something was missing I couldn't quite get. Projecting the arbitrary vector along an eigenvector makes sense tho

zinc timber
#

at least one pigeon has 2 assholes

ripe birch
#

thank you all for joining me on this adventure. This was 100x more productive than the physics server

zinc timber
#

ya phys server sucks

ripe birch
#

it really shouldn't. but it do

viral magnet
#

Physics server: how about we run a simulation with a mole of spheres

lavish jewel
#

i'm still butthurt about the linear functionals though

ripe birch
#

math people are just better to be around. I love physics as a field, but the people of math are just better.

zinc timber
#

which one?

viral magnet
#

Kolmogorov will visit you in your dreams and tell you to suck it up

ripe birch
#

I've met a lot of physicists. wouldn't party with em. Went to a party of grad-level mathematicians, that was a blast. Way more fun 😂

lavish jewel
#

well get bent, you got this explained to you by an engineer

ripe birch
#

engineers are also more fun, but also more psychotic

#

stop using i,j,k as basis vectors you psychopaths

lavish jewel
#

i don't do that :x

zinc timber
#

they said maths server not mathematicianskekw

ripe birch
#

then maybe you're a step above your bretheren

lavish jewel
#

why would i use j as a basis vector, when it obviously is sqrt(-1)

#

...

ripe birch
#

then again i can't speak, my people try to use phi as the azimuthal angle in spherical coorinates

zinc timber
#

quaternions catKing

viral magnet
#

Why use e as unit vector when that's clearly Euler's number

ripe birch
#

like we use theta in 2D, but flip to phi in 3D

zinc timber
#

R³ iso to a subspace of quaternions

ripe birch
#

@viral magnet also a thing i never understood. one of my texts did that and i almost cried

#

thankfully i haven't seen it since

viral magnet
golden ermine
#

Number theorists using pi as a function to count the number of primes less than n

ripe birch
#

EH?

quartz compass
#

ever1 stop trying to attach universal meaning to symbols

viral magnet
#

Also what a lazy name

#

"Prime counting function"

lavish jewel
#

i'm afraid this has gotten a little off topic, please move over to discussion-i or chill

ripe birch
#

ill see yall in off topic

#

wait i cant find off topic. chill it is?

lavish jewel
#

yeah

#

btw

#

as i said

viral magnet
dusky wadi
stoic pythonBOT
#

Alison40

spring pasture
#

@zinc timber

zinc timber
#

@spring pasture ?

spring pasture
zinc timber
#

the army sam? stare

spring pasture
old swift
#

I've met a lot of physicists. wouldn't party with em. Went to a party of grad-level mathematicians, that was a blast. Way more fun 😂

hearty rapids
#

i'm so confused

#

why is a arbritary?

#

because there is already a 1 in R1?

#

how is it reduced row echelon form when there is a 3 above the 1 in column 4?

sharp shell
#

u have to choose the values so it is row reduced

#

there can be a 3 above the 1 if u choose the c accordingly

hearty rapids
#

huh?

#

i thought reduced row echelon form meant if there is a 1 in any column

#

it has to be zeroes above and below

tulip basalt
#

Is there a way to like solve (A+B+C)x=0? A is a Vandermond matrix and B and C look like each other so I think this will be an easier way to solve my system but I have no idea how.

lavish jewel
#

wdym by "look like each other"

tulip basalt
#

They're both the operators applied to the exponential function with different exponent and such

#

and A contains those exponentials

#

It's like if T and S are operatos B=T(A) and C=S(A) applied component-wise

#

Does anyone how I can solve a system like this one?

#

Can I just take out an operator like (I+T+S)Ax=0 then apply the inverse on both sides to get Ax=0?

viral magnet
tulip basalt
#

Let $A=\left[\begin{matrix}
e^{ikx_1\cdot y_1} & e^{ikx_2\cdot y_1} \
e^{ikx_1\cdot y_2} & e^{ikx_2\cdot y_2}
\end{matrix}\right]\in (L^2(\Omega))^2\times(L^2(\Omega))^2$, $T,S: L^2(\Omega)\to L^2(\Omega')$ be compact operators.
Then, let $B=T(A),C=S(A)$ applied component-wise. How can I solve (A+B+C)x=0? Thanks!

stoic pythonBOT
#

emphatic_wax

viral magnet
#

Well that's beyond my linear algebra knowledge

tulip basalt
#

thanks for trying though

#

thanks for everyone. i solved it

echo night
#

Can some kind soul check my life dilemma about a Change of Basis on #help-3?

viral magnet
tulip basalt
#

Well I figured I proved some weeks ago that my operators are injective so I just pull them out and take the inverse so I'll have Ax=0

#

And I know the answer to this from a paper I read

serene solstice
#

How do I answers the next two questions?

boreal spindle
#

hey can someone explain me the solution for this excersize question?

fringe fjord
#

Please don't ping helpers after waiting just two minutes.

boreal spindle
#

Oh sorry!

fringe fjord
#

Also, when the solution you're asking about takes up half a page, please explain which parts of it your problems start at. Otherwise you're basically asking people to repeat what is already there, in the hope that they'll randomly guess the rewording you need.

boreal spindle
#

I didn't understand almost all of it unfortunately

#

it's the solution for part a) though

#

I understood the part where they explained that the matrix is supposed to be 2x3 and the rest I'm lost

#

<@&286206848099549185>

viral magnet
boreal spindle
#

In the original question?

fringe fjord
#

It would make sense if $\mathbb R_k[x]$ means the vector space of polynomials of degree at most $k$.

stoic pythonBOT
#

Troposphere

boreal spindle
#

it's 2 and 1

sand sinew
ashen bane
oblique prairie
#

sometimes people ping after exactly 15

exotic horizon
#

how can I find a matrix when given the eigenvectors associated to it ?

lavish jewel
#

do you have the eigenvalues as well?#

exotic horizon
#

yes

lavish jewel
#

are the eigenvectors orthogonal?

#

well, in general you'd take the eig vecs as columns of a matrix Q and the eigvals along the diagonal of a diagonal matrix D

#

then the matrix is QDQ^-1

quartz compass
#

the way I like to think of it is, you know the eigenvalue equation $Av=v \lambda $ instead of writing one of these for each eigenvalue/eigenvector, you can throw all the eigenvectors in a matrix at once and write this as $AV=VD$, here the matrix $V$ has its columns the eigenvectors and $D$ is a diagonal matrix of eigenvalues.

stoic pythonBOT
#

Merosity

zinc timber
#

what if I write it as Av = lambda v catThimccatThimc

lavish jewel
#

it's the same thing anyway

quartz compass
#

heh I was gonna explain why I wrote it that way but it was getting too long

lavish jewel
#

once you consider more than one vector at a time

quartz compass
#

I think of multiplying on the right as column operations and multiplying on the left as row operations

zinc timber
#

yes that interpretation is actually helpful

quartz compass
#

since D is putting a scalar on the entire column, that's why I wrote it with the scalars on the right yup

zinc timber
#

though I still need to pause for a moment

lavish jewel
#

you don't have to worry about it if you use einstein notation

zinc timber
#

$v=v^ie_i$

stoic pythonBOT
zinc timber
#

btw I ended up ordering a larger one, edd

lavish jewel
#

ah

#

did you already receive it?

zinc timber
#

no it'll take like a weeksadcat

#

they also dropped the price after I ordered it, those scammers

lavish jewel
#

haha

exotic horizon
quartz compass
#

you're welcome 👍

dusky wadi
#

would the matrix from R² to R² for the orthogonal projection onto $x_1 = -2x_2$ be $\begin{bmatrix} \frac{1}{\sqrt{5}} && 0 \ \ -\frac{2}{\sqrt{5}} && 0\end{bmatrix}$

stoic pythonBOT
#

Alison40

zinc timber
#

no check again

quartz compass
#

a nice way to project onto a space spanned by a vector v is to make the matrix $P=\frac{vv^T}{v^Tv}$

stoic pythonBOT
#

Merosity

quartz compass
#

(it follows from the usual derivation with dot products, also fun to check P^2=P)

dusky wadi
#

ok I'll actually come back to this question

#

i thought i could do it with rotation matrices but i was wrong

quartz compass
#

the only part where you "need" rotation matrices is the fact that $x+2y=0$ can be seen as $(1,2)\cdot (x,y)=0$ so you can do a 90 degree rotation or just see by inspection $(x,y)=(2,-1)$ is a basis for this 1D subspace

stoic pythonBOT
#

Merosity

dusky wadi
#

i just realised i can solve it using simultaneous equations

thorn yacht
#

Hey, could I just ask whether the following statement is true or false?:
If f is a linear operator over the finite-dimensional vector space V, then V has a basis that consists of eigenvectors for f: V->V.

(My TA said that this was true, but from what I can see, this isn't always the case, so if someone could perhaps clear this up, that would be very helpful, thanks.)

zinc timber
#

no that's not always true, (the special case when it is true, we call T diagonalizable)

lavish jewel
#

as ryu says

zinc timber
#

ex the matrix $\m{1 & 1 \ 0 & 1}$ do not have a basis consisting of evs

stoic pythonBOT
lavish jewel
#

that's a so-called "defective matrix"

#

the requirement for what you said to be true is for the operator to have n linearly independent eigenvectors, where n is the dimension of the vector space

zinc timber
#

(My TA said that this was true, but from what I can see, this isn't always the case, so if someone could perhaps clear this up, that would be very helpful, thanks.)
hmmCat

thorn yacht
#

Thanks for clearing it up 🙂 👍

zinc timber
subtle walrus
zinc timber
severe heron
#

Let A and B be 4 × 4 matrices. Suppose that A has eigenvalues
x1, x2, x3, x4 and B has eigenvalues 1/x1, 1/x2, 1/x3, 1/x4, where each xi > 1. Prove that A + B has at least one eigenvalue greater than 2. Can someone help? Any hints on how to start?

quartz compass
#

idk maybe try to look at manipulating their characteristic equations to try to make an inequality

zinc timber
#

no other information given on A or B?

severe heron
#

nope

#

here's the entire Q

zinc timber
#

maybe you can show that B and A^-1 are similar

quartz compass
#

something I have in mind is f(x) is the characteristic polynomial of A, then x^4 f(1/x) is the characteristic polynomial of B, then try to do something with cayley hamilton by plugging in the matrix A+B and break it into an inequality in terms of A and B separately

zinc timber
#

I'm not super sure on this because xi's may not be distinct

severe heron
#

okay i'll try that out

quartz compass
#

I guess now that I think of it, their characteristic polynomials are the same, just with the coefficients reversed

quartz compass
zinc timber
#

if confused on the multiplicity part, like they didn't mention distinct

quartz compass
#

oh, why does it matter

zinc timber
#

like if they are taking something like [1 1 \ 0 1] has ev 1, 1, then it might not work, idk

quartz compass
#

hmm

zinc timber
#

because say $A = \m{2 & 0 \ 0 & 2}$ and $B=\m{1/2 & 1 \ 0 & 1/2}$ fits the description

stoic pythonBOT
severe heron
#

4 by 4

zinc timber
#

(just any 2x2 block, that's not the point)

severe heron
#

okay

severe heron
#

i used the fact that sum of ev of (A+B)=sum of individual ev of A and B= x1+1/x1+x2+1/x2+x3+1/x3+x4+1/x4 > 8 using am gm

#

and now since there are 4 eigenvalues of (A+B) we can say by PHP that one of them must be greater than 2 i guess

exotic horizon
#

Hi! does anyone know how to find the dimension of an eigenspace (we are given a matrix and eigenvalue) ?

zinc timber
#

nullity (A-cI)

exotic horizon
#

c is a real number right ? What is nullity ?

zinc timber
#

c is the eigen value

#

nullity = dim of the null space

exotic horizon
#

thank you!

magic light
#

Need some reminders on what operations are allowed on determinants

#

I know you can add columns together like C1: C1 + C2 - C3

#

and that you can take a constant out of a row like
|aa ab|
|c d|

a * |a b |
|c d|

#

but what else? can I do row operations?

haughty berry
# magic light but what else? can I do row operations?

(The transpose of a matrix doesnt affect its determinant, so anything that works for rows goes for columns as well)
You can add rows by a constant without affecting the determinant. So like R1: R1 + 3R2 wont affect the determinant
Multiplying a row by a scalar multiplies the determinant by the scalar
Swapping two rows multiplies the determinant by -1

#

Determinants are also multilinear

magic light
#

also 1 is constant right?

#

R1: R1 + R2 => unchanged?

haughty berry
#

It doesnt really matter in the case that youre adding rows

#

So like

#

R1: R1 + 3R2 => unchanged as well

#

Lemme show you

magic light
#

this makes me feel like I can just do gaussian elimination on a determinant, no?

#

also a follow up - can I take a constant from a column?

haughty berry
#
\def\sline{\text{---}}
Suppose you have:
\[ \det\begin{pmatrix} \sline v_1 \sline \\\vdots\\\sline v_n \sline\end{pmatrix} \]
And say you add $\alpha v_i$ to $v_1$ ($i\neq 1$):
\[ \det\begin{pmatrix} \sline v_1 + \alpha v_i \sline \\\vdots\\\sline v_n \sline\end{pmatrix} \]
Since determinants are multilinear:
\[ = \det\begin{pmatrix} \sline v_1 \sline \\\vdots\\\sline v_n \sline\end{pmatrix} + \alpha\det\begin{pmatrix} \sline v_i \sline \\\vdots\\\sline v_n \sline\end{pmatrix} \]
The second determinant above has $v_i$ twice (once in the first row, the second in the $i$th row), so it is just $0$:
\[ = \det\begin{pmatrix} \sline v_1 \sline \\\vdots\\\sline v_n \sline\end{pmatrix} \]
Which is your original determinant
haughty berry
stoic pythonBOT
haughty berry
magic light
haughty berry
#

Yeah, but that's not related to adding rows

magic light
#

I was just curious why that thing is 0

haughty berry
#

Oh

#

You remember how the determinant of a non invertible matrix is 0?

#

So if the rows are linearly dependent, then the determinant is 0

magic light
#

I see.

#

My professor likes giving us a bunch of tricks in the determinants. If we solve it by brute forcing we get a cubed equation.

#

No calculators in the test.

haughty berry
#

that sucks

#

i cant do math without my calculator lol

magic light
haughty berry
#

Characteristic polynomials?

magic light
#

the question in this case was to find an orthonormal base for R^3 using the eigenvectors of A^TA

#

when A was given to us

#

Soo yeah.