#linear-algebra

2 messages · Page 206 of 1

heavy crown
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yes I understand the first and second but not the third

dusky epoch
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if $E$, a $2 \times 2$ matrix, is neither invertible nor 0 then it can be written in the form $E = uv^T$ where $u, v$ are column vectors of size 2

stoic pythonBOT
heavy crown
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aha I see. I think it's because in that case |E| = 0, so E has one row or column with 0 so the dim would be less than 4

dusky epoch
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"E has one row or column with 0"

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i mean, it is possible for all entries of E to be nonzero and det(E)=0 nonetheless

heavy crown
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yes like 0 0 as row ?

dusky epoch
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the matrix $\bmqty{1&2\2&4}$ is singular

stoic pythonBOT
heavy crown
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oh, right

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yea

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so why it says the dim is 2?

dusky epoch
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"it"?

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i was the one who said it sully

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twice

heavy crown
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haha, true

dusky epoch
heavy crown
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yes

dusky epoch
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okay let $E = uv^T$ and consider the defn of $U_E$

stoic pythonBOT
dusky epoch
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we will have $U_E = { (Xu)v^T \mid X \in M_2(\bR)}$

stoic pythonBOT
dusky epoch
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i claim this is equal to ${ wv^T \mid w \in \bR^2}$

stoic pythonBOT
heavy crown
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yes that's true

dusky epoch
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yeah, and that in turn has dimension 2

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it's spanned by $\bmqty{v_1 & v_2 \ 0 & 0}$ and $\bmqty{0 & 0 \ v_1 & v_2}$

stoic pythonBOT
heavy crown
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but those were vectors of size 2?

dusky epoch
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?

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oh sorry, i should've clarified, $v = \bmqty{v_1\v_2}$

stoic pythonBOT
dusky epoch
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U_E is a subspace of M_2(R), its elements are 2x2 matrices

heavy crown
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oh okay I see

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yes

dusky epoch
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okay so bringing this all back

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we now know that if E is invertible then U_E = M_2(R) and if E is singular then U_E is a proper subspace of M_2(R)

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does this make sense?

heavy crown
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yes

dusky epoch
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okay

heavy crown
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because of the span

dusky epoch
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so you had your problem say that {AE, BE, CE, DE} is linearly independent

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and AE, BE, CE, and DE are all members of U_E by construction - as i hope is obvious

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fuck. messages not sending

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there we go

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so we have that U_E contains a linearly independent set of four points, meaning that dim(U_E) = 4 [as this is all happening in a vector space of dimension 4 !]

heavy crown
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right, so because it is linerally independent it means dim = 4

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then U_E = M_2(R)

dusky epoch
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yes

heavy crown
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and then its invertible

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hmmm

dusky epoch
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yes that's it

heavy crown
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haha

heavy crown
vital arch
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Cam anyone help me with a question

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(x/y)+(y/z)+(z/x) = 1

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Does this equation have any integer solution?

dusky epoch
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wrong channel

limber sierra
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the space of real 2x2 matrices under matrix addition is isomorphic to R^4, yes

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vector spaces do not encode vector-vector multiplication

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so the fact that you can multiply matrices is irrelevant

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erm

nocturne jewel
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eigenvectors are from linear transformations, not vector spaces

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Eigenvectors are just the vectors in the domain space which just get scaled when the transformation is applied

limber sierra
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the correspondence between linear transformations and matrices does not work well in a vector space of matrices.

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Av = Iv is nonsense

nocturne jewel
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$A:\mathbb{R}^{2\times 2} \to V$ for whatever V you want

stoic pythonBOT
nocturne jewel
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if you mean A is the transformation

limber sierra
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unless A is supposed to be a function here

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rather than a matrix

nocturne jewel
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You can have the matrix representation of A

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you wouldnt happen to have a specific question would you?

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$I^2=I$, yes

stoic pythonBOT
nocturne jewel
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If A represents a linear transformation from a 2-dim space to another 2-dim space

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then yes, that's the definition of eigenvalue/vector

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what?

quartz compass
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as an example, A=[1,0;0,2] has eigenvector [1;0] with eigevalue 1, and A is not the identity

nocturne jewel
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if A is identity, then you have the identity map, in which any vector is an eigenvector with value 1

limber sierra
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Av=lv for v being a matrix just means A is identity
what if v isnt invertible?

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for example, Av = Iv is certainly true for all (linear) A if v is the 0 matrix

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okay, so pick a slightly less degenerate example then

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let v = (1, 0; 0, 0)

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note that there are multiple linear A such that Av = v

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for example, (w, x; y, z) mapsto (w, 0; 0, 0) works, but so does (w, x; y, z) mapsto (w, w; 0, 0) or (w, x; y,z) mapsto (w, x; x+y, 2x+z)

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the problem isnt the "single element" part

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its that v is noninvertible

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perhaps you should be looking at GL(R, 2)

quartz compass
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you could write it as a block matrix like [A,0;0,A] [u;v] = [Au; Av]

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a basis for the eigenvectors are then just the eigenvectors of A concatenated with 0 on top and bottom

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so the matrix v eigenvectors for a specific eigenspace are multiples of a single eigenvector of A in both columns.

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v = [3e_1, -7e_1] for instance, given e_1 is an eigenvector of A

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as matrices these clearly are never invertible since they're linearly dependent

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try vector space of functions

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like continuous functions on [0,1]

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or finite fields maybe, just any random field you can get your hands on

nocturne jewel
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Or just polynomial spaces

quartz compass
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there's a game you can play where you turn on and off lights in a pattern by pressing a square

nocturne jewel
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I hate that game

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I can never win it

quartz compass
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you can solve it by thinking of it as a vector space over F_2

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(finite field with 2 elements)

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I think it's easy to get the misconception that group theory is just mindless, abstract jerking off

nocturne jewel
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I havent done Group so I cant answer this sully

quartz compass
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but there's a purpose to the stuff it does and it's for stuff

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like just abstracting for the sake of abstraction isn't really group theory or abstract algebra

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I'm not the end all be all either lol, I don't know what you're actually doing past just trying to find more examples of vector spaces to play with to get a better understanding

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so I don't know what automorphisms and maps you're talking about

viral flint
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You need that matrix multiplication is linear of course.
And once you have shown it's an isomorphism of M_2(R), you know there is an inverse on M_2(R) but you don't a priori know that the inverse is also given by right-multiplication by a matrix. For that part you need to use the property of matrices that if a square matrix has no null space, it is invertible. Depending on how you prove that property, it could involve determinants at least.

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Oh I thought you were asking about the question about Z = {AE, BE, CE, DE}. Ignore what I just typed then.

night gazelle
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What are, in your opinion, the necessary prerequisites to start studying linear algebra by oneself?

gray dust
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@night gazelle experience in proof writing/reading & matrix computation

stable kindle
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patience

next vapor
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if i have a set of commuting operators on a complex vector space V(dim n) and one element T with n distinct eigenvalues and a basis consisting of the eigenvectors of T, how do i show that every other element of the set can represented with a diagonal matrix

gray dust
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@next vapor it's not true as is

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take operators $\m{0&1\0&0}$ and $I$ on $\bC^2$. they commute but the former isn't diagonalizable

stoic pythonBOT
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RokabeJintaro

gray dust
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but it DOES hold if we also require the operators be hermitian, in fact in that case they're simultaneously diagonalizable iff they pairwise commute

next vapor
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but they both have just 1 eigenvalue dont they?

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in the counterexample i mean

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or am i missing something

dusky epoch
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yeah i think youre missing that @gray dust

gray dust
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my bad i missed 'n distinct eigenvalues'

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@next vapor then it's actually true, try proving it for a pair of commuting operators and extend it to any set of pairwise-commuting operators

next vapor
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i think i need to show that 2 commuting operators share eigenvectors right

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so if A and B commute, and v is an eigenvector of A with eigenvalue λ, then A(Bv)=B(Av)=B(λv)=λBv

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so Bv is also an eigenvector of A

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hm not sure where to go from here

gray dust
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@next vapor since A has n distinct eigenvalues, each eigenspace of A is 1-dim

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you showed Bv is in the λ-eigenspace so it's a scalar multiple of v, thus v is an eigenvector of B

odd kite
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I believe this holds whenever there is a complete set of orthogonal eigenvectors

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even if eigenvalues aren't district or are complex

next vapor
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that should be it right, since i can do the same thing with any 2 operators in the set

next vapor
gray dust
next vapor
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yea i was just gonna take the standard hermitian

gray dust
next vapor
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alright, thanks alot

crude ridge
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Does A(Bx) = (AB)x ?

wintry steppe
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yes

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associativity of matrix multiplication

crude ridge
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Oh forgot about that. Also, if nul(A)=nul(B) then can you say nul(A-C)=nul(B-C)?

wintry steppe
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let A and B be your favorite distinct invertible operators and let C = A.

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eg Ax = x and Bx = 2x as operators R -> R. both have null space {0}. if we take C = A, then A - C has null space R, but B - C has null space {0}

crude ridge
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Oh that's interesting, thank you

next vapor
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can i get a hint on this problem

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i have a finite dimensional inner product space V with basis v1,...v_n and orthogonal basis w_1,...w_n obtained through the original basis

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how do i show that |v_1|^2+...+|v_n|^2>=|w_1|^2+....+|w_n|^2

next vapor
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any hint? <@&286206848099549185>

spare crystal
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I want to prove that if $T : \mathbb{R}^2 \to \mathbb{R}^2$ is a linear transformation that preserves the magnitude of angles, i.e.,
$$
\frac{\langle x, y \rangle}{|x||y|} = \frac{\langle Tx, Ty \rangle}{|Tx||Ty|} \quad \text{for all $x, y \in \mathbb{R}^2$},
$$
then $|Tx| = \lambda|x|$ for all $x \in \mathbb{R}^2$ and a constant $\lambda$.

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I haven't done linear algebra in a while, so I'm not super sure where to start. Any hints are appreciated 🙂

stoic pythonBOT
spare crystal
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Intuitively, T is a rotation + reflection + scaling, so it's clear, but I'm not sure how to prove that

thorn robin
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@spare crystal Still stuck on this?

spare crystal
thorn robin
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Ok

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I can guide you through what I did

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It's not the cleanest proof

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I'm just gonna work with |<x,y>|^2 |Tx|^2 |Ty|^2 = |<Tx,Ty>|^2 instead for |x| = |y| = 1

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Since this identity holds for unit vectors iff your original identity holds for all vectors

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And makes it so we don't have to worry about |Tx| = 0

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Anyway step 1: if you evaluate T at x = (1,0) and y = (0,1) you should find that ab + cd = 0

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This will help simplify the next calculation (and it also says that the columns of T are orthogonal)

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Step 2: more generally, evaluate T at x = (cos t, sin t) and y = (1, 0)

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You should find that the identity reduces to (a^2 + c^2)*((a^2+c^2)cos^2(t) + (b^2+d^2)sin^2(t))*cos^2(t) = (a^2 + c^2)^2 * cos^2(t)

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To get to this you need to use the fact that ab + cd = 0 to deal with some cross terms

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Anyway just choose a t so that cos(t) \neq 0 and divide by cos(t)

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And also divide by a^2 + c^2, which you can do as long as T \neq 0 (since you can check that a = c = 0 implies b = d = 0 by evaluating at x = (1/sqrt(2), 1/sqrt(2)) and y = (0, 1))

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This gives you (a^2+c^2) * cos^2(t) + (b^2+d^2) * sin^2(t) = a^2 + c^2

sweet vine
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why is this true? i dont see it

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helo seion

thorn robin
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Which you can manipulate to get b^2 + d^2 = a^2 + c^2 by choosing a t with sin(t) \neq 0

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So to summarize you have ab + cd = 0 and b^2 + d^2 = a^2 + c^2

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i.e. the columns of T are orthogonal and have the same length

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So you can write T = lambda * S where S is an orthogonal matrix

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This is what you wanted

spare crystal
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oh hmm, i will try to work that out, thanks so much!!

thorn robin
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No problem lol

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Like I said it's not the cleanest proof

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I would hate to do that for n > 2

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But I think it all works

spare crystal
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yeah lol

dreamy iron
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Hi #linear-algebra

SCENARIO 1:
Given a vector space V, with basis a,b,c,d; I can prove that

a+b, b+c, c+d, d is also a basis for V.

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I proved the above claim.

I have not proved the following::
SCENARIO 2:
Consider a basis,
a,b,...., z.

a+b, b, ..... , z is also a basis.

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Is the second scenario like a special case of the first scenario.

dusky epoch
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it's not

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in scenario 2 you presumably have 26 basis vectors for a 26-dimensional space

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which is not at all a special case of scenario 1, which deals only with 4-dimensional spaces

dreamy iron
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lol, just say n, not 26

dusky epoch
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if you want n then use proper notation

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like $v_1, v_2, \dots, v_n$ and $v_1+v_2, v_2, \dots, v_n$

stoic pythonBOT
dusky epoch
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those are the lists you are considering

dreamy iron
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thanks!

dusky epoch
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of which the former you are requiring to be a basis

dreamy iron
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Yup

dusky epoch
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anyway no, these are not special cases of each other

dreamy iron
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There’s a pattern here, seemingly:

$v_1, v_2 \text{ is a basis} \iff v_1 + v_2, v_2 \text{ is a basis} $

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$$v_1, v_2 \text{ is a basis} \iff v_1 + v_2, v_2 \text{ is a basis} $$

stoic pythonBOT
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ninnymonger is a Physics main.

dusky epoch
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$v_1, v_2$ is a basis iff $v_1+v_2, v_2$ is a basis

stoic pythonBOT
dusky epoch
lavish jewel
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you can use the definition of linear independence and see what happens

dreamy iron
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and....

$$v_1, v_2, v_3 \text{ is a basis} \iff v_1 + v_2, v_2+v_3, v_3 \text{ is a basis} $$

stoic pythonBOT
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ninnymonger is a Physics main.

dusky epoch
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okay so

dreamy iron
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Is there a name for this pattern?

dusky epoch
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no

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no there is no name for it

dreamy iron
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and I also think that the following is true

$$v_1, v_2, v_3, , \ldots, ,v_n \text{ is a basis} \iff v_1 + v_2, v_2 +v_3, , \ldots, v_{n-1} + v_n ,v_n\text{ is a basis} $$

stoic pythonBOT
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ninnymonger is a Physics main.

dusky epoch
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it is true

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theres just no name for that particular change of basis

marble lance
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Linearly dependent?

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Yes

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The reasoning should be clear based on the defn

crude falcon
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hmm I have two formulas for obtaining the iterative solution in Jacobi Method

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the first one is the wikpedia one, the second is the one I've been taught, they are the same except in the second one you add the L+U matrix

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are they equivalent?

lavish jewel
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no, the second one seems wrong

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the method is based on letting A = L + D + U, and then subtracting (L + U)x from both sides

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in your second image, this would mean that L and U have a different definition, i.e. they are the strictly upper and lower triangular parts of negative A, instead of A

crude falcon
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oh true, they are using -A

wintry steppe
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Assuming the system given by Ax = b is consistent, then it has a unique solution only if A has full column rank. Is that correct?

lavish jewel
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sounds ok

wintry steppe
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Thanks

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If A has full row rank we can't infer the uniqueness right?

lavish jewel
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only if you knew the dimensions of A

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A would have to be square

wintry steppe
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Yup, assuming the general (non-square) case

dreamy iron
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Hi #linear-algebra .

I need to find ALL the vector spaces with only one basis.

Step 1: I can prove that if my basis is the empty set, then my vector space is the singleton set containing the zero vector {0}.

Step 2: If can prove that if my vector space is {0}, then my basis is the empty set of vectors.

does this prove that {0} is the only vector space with one basis?

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Step 1: is by definitions of span of the empty set and linear independence of the empty set.

Also by set theory, I know that the empty set is in unique.

viral flint
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This proves that {0} is the unique vector space with the empty set as a basis

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You would still have to show that a vector space has exactly one basis iff that basis is the empty set.

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Which BTW I think is false in one case: a one-dimensional vector space over the field with two elements

dreamy iron
native rampart
dreamy iron
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Lol. I don’t know how to work with F_2. I guess I can make the multiplication table.....

native rampart
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F_2 is nice in that span{v}={v,0}

dreamy iron
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Can you be more explicit. I dont see that

native rampart
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You have v

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and v+v=2.v=0.v=0

dreamy iron
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So that’s the addition table for F_2.

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right??

dire thunder
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F_2 is just field of remainders modulo 2

native rampart
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Yes

dreamy iron
stoic pythonBOT
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ninnymonger is a Physics main.

native rampart
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Well,You will have 0.v and 1.v in span{v}

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Yes

dire thunder
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F_2 = {0,1} and +, * defined as usual operations but taken modulo 2

native rampart
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Your field has to be over F_2

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Otherwise,you can just pick {-v_1} instead of {v_1} to span the space

dreamy iron
stoic pythonBOT
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ninnymonger is a Physics main.

native rampart
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Yes

dreamy iron
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obviously -v is in V over F_2......?

dreamy iron
native rampart
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In F_2,v=-v

next vapor
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i tried it with a basis of just 2 vectors but things got really messy and led to a dead end

viral flint
# dreamy iron How would I go about doing this?
  1. If basis is empty, it's the only basis.
  2. If basis is non-empty, there's another basis.
    As has been mentioned, 2. is wrong in general, but you can show it if you assume that it's not a basis of size 1 over F_2.
viral flint
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Hint: ||w_i is defined as v_i - a for some expression. Prove that |v_i|^2 = |w|^2 + |a|^2.||

next vapor
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idk if im messing up but i get that |w_i|^2=|v_i|^2+|a|^2-2<v_i,a>

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which doesnt seem right

next vapor
short coral
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Any easy proof for Sylvester rank inequality?

broken sun
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Hello. Can you give me an example of an operator which has no adjoint?

dusky epoch
broken sun
dusky epoch
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well you can pick a particular sequence xi and construct the operator as the first answer writes

next vapor
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sorry for the ping but i cant seem to get the equality |v_i|^2=|w|^2+|a|^2@viral flint
its just computing the inner product of v_i-a with itself right?

viral flint
broken sun
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I cannot understand such a construction. Can you elaborate?

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I know basic math.

next vapor
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so <v_i-a,v_i-a> = <v_i , v_i-a>+ <-a, v_i-a>= <v_i , v_i>+ <-a , v_i>+ <v_i , -a>+ <-a,-a>

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which simplifies to |v_i|^2+|a|^2+2<v_i,-a>

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so |w_i|^2=|v_i|^2+|a|^2+2<v_i,-a>

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but how do you go from this to that equation

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or am i going wrong somewhere?

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right? @viral flint

viral flint
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Right so far

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So if you want to get from here to the desired equation, what do you need to show?

next vapor
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i would need to have |a|^2-2<v_i,a> equal to -|a|^2 right

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so |a|^2 would have to be equal to <v_i,a>

viral flint
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Yes

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You have a formula for a presumably

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Use that to calculate |a|^2 = <a, a> and <v_i, a> and check that their difference is 0.

next vapor
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so a is <v_i,w_1>/|w_1|^2w_1+...<v_1,w_i-1>/|w_i-1|^2* w_i-1

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wait cant i just say that <v_i, a> -<a,a> =<v_i, a-a>=<v_i, 0> which is just 0?

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wait no thats wrong

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hm im not seeing any cancellations its just a jumbled mess

next vapor
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im not seeing this ill come back to it later

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i just wanna double check a solution

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I have an inner product space and i want to find all vectors v and w such that proj_v(proj_w(v))=proj_w((proj_v(w)

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but when i apply the formula for projections i get that v=w

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but that seems too simple

next vapor
viral flint
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Oh sorry forgot about this

viral flint
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Anyway

viral flint
next vapor
viral flint
next vapor
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oh right i completely forgot about that

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so when i expand <w_i,a> i get inner products in terms of the orthogonal basis

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and it equals 0 so that show the equality

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and just to confirm that equality happens iff v_i=w_i for all i

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if they are equal then equality follows trivially because its already an orthogonal basis

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the other direction we have |v_i|^2=|w_i|^2 --> so |a|^2 is 0 meaning all the inner products <v_i,w_i> are 0 meaning theyre orthogonal

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so our original basis is already orthogonal

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does this look right? @viral flint

lavish zephyr
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hey guys, why do we need gram-schmidt to obtain orthonormal bases. Why can't we just take basic projections and then obtain them

viral flint
viral flint
next vapor
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a is <v_i,w_1>/|w_1|^2w_1+...<v_1,w_i-1>/|w_i-1|^2* w_i-1 and we want everything to be 0 right

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and since w_i is a non zero vector that means each <v_i,w_i> has to be 0 for the whol thing to be 0 no?

viral flint
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Yes (although you need that w_i are linearly independent, not just non-zero)
So <v_i, w_1> = <v_i, w_2> = ... = <v_i, w_(i-1)>
Doing this for all i,
<v_i, w_j> = 0 whenever i > j
which is extremely different from saying <v_i, w_i> = 0 for all i (notice the same i in both subscripts)

next vapor
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but w_i are linearly independent arent they, since theyre an orthogonal basis

viral flint
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Yes, I was just pointing out that you need to use that to conclude that the coefficients are 0.

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More importantly, did you understand the difference between
<v_i, w_j> = 0 (all i,j such that i > j)
and
<v_i, w_i> = 0 (all i)
?

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In any case, this is getting unnecessarily complicated.
If |w_i|^2 = |v_i|^2 = |w_i|^2 + |a_i|^2, then |a_i| = 0 so a_i = 0 so w_i = v_i - a_i = v_i.
Here a_i is the a you used for finding w_i from v_i, labelled with an extra i for clarity.

next vapor
#

yea i see now

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thanks alot i appreciate it

next vapor
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If A is an nxn matrix and i wanted to show that A and A+I have different characteristic polynomials

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is there an easier way than calculating the determinant explicitly

wintry steppe
#

char poly of A = det(A - tI)
char poly of A + I = det(A + I - tI) = det(A - (t - 1)I)

nocturne jewel
#

Idk, seems complicated

merry orchid
#

someone helps me in this activity

#

someone helps me in this activity

atomic badge
#

Hello chat. I would like to confirm if it's possible to exist more than one t which would make phi a linear Transformation with this given vectors? I have found it to be t != 1. thanks in advance!

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almost forgot this if this matters at all

naive skiff
#

Can someone help me with this? I saw something like this in a classical mechanics book and I'm bent

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I'm looking to understand the steps

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Is this true?

native rampart
#

How are you defining derivative wrt B?

dull rune
#

May I get assistance for this question. Thank you so much

quartz compass
#

what have you tried

dull rune
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I do not know where to start. I've scoured the textbook but no clue where the professor got it from.

quartz compass
#

well, what's a transition matrix?

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@dull rune

dull rune
#

a matrix that when multiplied with one matrix gives out the a desired output matrix... something like that

#

so if u multiply the transition matrix by B, itll become C

quartz compass
#

not quite

#

it's the matrix that lets you change basis

#

we have two bases, the set B and set C

dull rune
#

oh right

quartz compass
#

so if you have a vector represented with coefficients on the basis B, the transition matrix will take those and give you what the coefficients on C basis should be

#

fortunately this isn't too bad, let's just build it up one step at a time

dull rune
#

yay

#

ok so I have an idea how to do soemthing similar had it been simple integers

quartz compass
#

what polynomial does the column vector (1,0,0) represent in the B basis?

dull rune
#

hmm

#

erm, the first one id have to assume, though i am guessing at this point

quartz compass
#

yeah, write it out

dull rune
#

2+x+x^2

quartz compass
#

perfect

#

so now what's this polynomial look like in the C basis as a column vector?

dull rune
#

2, 1, 1?

quartz compass
#

yeah exactly

#

so we just transformed the first basis vector from B to the C basis

#

and we could write that in a matrix like:

#

$$\begin{bmatrix} 2 & - & - \ 1 & - & - \ 1 & - & - \end{bmatrix}$$

stoic pythonBOT
#

Merosity

dull rune
#

ahh

#

yes i have that great

#

ok so if i follow that pattern, ill get something like (2,1,1),(1,2,1),(2,0,1)

quartz compass
#

maybe

#

why would that work

dull rune
#

what do u mean by why?

quartz compass
#

well it's your idea

dull rune
#

uh

quartz compass
#

why would this work

dull rune
#

well following the pattern from the first polynomial

#

the other two polynomials have similar degrees

quartz compass
#

how does it work

dull rune
#

u map each coefficient from B in a column of a matrix

#

following the 'formula' given by C

quartz compass
#

why do we do columns and not rows

dull rune
#

now that... uh...

#

i am not so sure why

#

is it just a rule? i remember glossing over the definition in my textbook

quartz compass
#

well I just figured it out, it isn't like random

#

we were trying to construct a matrix that transforms from one basis to the other

dull rune
#

Right

quartz compass
#

let's see, where does the column vector (0,1,0) in the B basis get transformed to in the C basis?

#

if you take any matrix and multiply it by this vector, what's the output?

dull rune
#

(0,1,0)?

quartz compass
#

$$\begin{bmatrix} a & b & c \ d & e & f \ g & h & i \end{bmatrix}\begin{bmatrix} 0 \ 1 \ 0\end{bmatrix} = ?$$

stoic pythonBOT
#

Merosity

quartz compass
#

what do I get from this matrix multiplication

dull rune
#

uhhhhh (b+e+h)

#

wait.

#

fuck

#

god i feel so stupid

#

(b, e, h)? surely im going crazy or i cannot do matrix multiplication

#

well the result is a 3x1, so that is why it must be a column

quartz compass
#

yeah good

#

so we got the middle column

#

we know the transition matrix needs to take the column vector (0, 1, 0) and output (1, 2, 1)

dull rune
#

oh

quartz compass
#

and you just showed that the output of that is the middle column so

#

that's why that's there

dull rune
#

i see

#

🧠

quartz compass
#

knowing where the basis vectors go tells you where all vectors go

#

that's one way to think about what linearity means

dull rune
#

oh wow

quartz compass
#

ok cool, so now you have P, maybe the rest is easier now

dull rune
#

for part b) do i do the same but going in the other direction from C to B

quartz compass
#

that would be hard wouldn't it

dull rune
#

..yeah

quartz compass
#

luckily you don't have to

dull rune
#

i see matrix inversion

#

ill go and review that

quartz compass
#

yeah that's what you'll do, really quickly think of it this way:

#

let's say you have the vector v in the B basis then you transform it to the C basis by doing Pv

#

then if you want to transform from the other way, there's some matrix Q that goes from C to B so you could do QPv

#

but now you're back in the B basis, so it should be like nothing happened

#

v = QPv

#

you could write Iv = QPv

#

this has to hold for all vectors v, so you can say I = QP and so Q is the matrix inverse of P

dull rune
#

okay i think i understand

quartz compass
#

cool

dull rune
#

lastly for part C, I feel like i get the gist of it but would u be able to offer a brief outline

quartz compass
#

try to explain it to me first and I'll correct you

dull rune
#

basically i have to find 'u' relative to C, and use whatever i got for part B and apply it?

quartz compass
#

yeah what is u relative to C

dull rune
#

(3, 1,1)?

quartz compass
#

yeah easy

dull rune
#

oh

#

nice

quartz compass
#

so fairly simple steps over all, getting P is easy, writing u in C is easy, since C to B is P^-1 is also easy to get, not much more to say

dull rune
#

so (3,1,1)(P^-1)

#

ill give it a try

quartz compass
#

well, you multiply P^-1 on the left

#

and (3,1,1)^T you should probably write it that way to be clearer

dull rune
#

oh ok

quartz compass
#

I am always making sure to say 'column vector' because I don't want to write the transpose

dull rune
#

thank you so much

quartz compass
#

you're welcome 👍

dull rune
#

i got it done and turned it in

#

u are brilliant i cant thank u enough
'

quartz compass
#

thanks, glad to help, you're welcome

next vapor
#

I have an inner product space and i want to find all vectors v and w such that proj_v(proj_w(v))=proj_w((proj_v(w))

#

I believe this is only satisfied when v=w and the algebra checks out but im unsure, can anyone confirm or deny?

quartz compass
#

nope

#

they could be perpendicular

next vapor
#

ah yes

#

thats the bit i missed in my working

#

that means <v,w> is 0 and i cant cancel it, thank you

quartz compass
#

yup exactly

#

you're welcome

next vapor
#

but just to confirm those are the only 2 scenarios right

quartz compass
#

yeah that's all

next vapor
#

show that the square of an average of n numbers is less than or equal to the average of the squares

#

i know that <v,w> <= |v||w|

#

so if i take the dot product as my inner product and v=(x_n) and w=(1) this should work

#

nvm i could just square both sides

dreamy iron
#

Hi #linear-algebra.

Im once again trying to find all the vector spaces with only one basis, but considering only the fields R and C.

#

Specifically, I’m trying to prove point 1.

#

That’s what I got...

#

it doesn’t feel right

dusky epoch
#

any nonzero real vector space necessarily has more than one basis

#

just take any basis and take any vector in it and scale it by 2, now you have a different basis.

#

your proof feels empty

dreamy iron
#

I add remarks

dusky epoch
#

this feels bureaucratic

dreamy iron
#

I don’t understand.

#

Im not doing the finite field portion cuz I don’t have to (and frankly I don’t understand finite fields well enough just yet.)

dusky epoch
#

this proof feels bureaucratically bloated

#

claim: in a nonzero real vector space, there exists more than one basis.

proof: take any basis of your nonzero vector space. take any vector in the basis. replace this vector with twice itself. now you have a different basis.

#

that's it

dreamy iron
#

Okay

#

And how about ** Find all vector spaces with only one basis.**

vapid vale
dreamy iron
#

Yes.

#

My proof is only for R or C

dusky epoch
#

unless you meant to generalize my thing

dreamy iron
#

If a basis is empty, then it’s the only basis.?

dusky epoch
#

in the zero vector space, the only basis is the empty basis, because the only other set of vectors you could have is {0}, which is linearly dependent.

dreamy iron
#

Is that the proof?

wintry steppe
#

you can also think of the empty sum as being equal to 0

dreamy iron
#

That’s much simpler than what I have.

dusky epoch
#

yes

#

sometimes things really are simple, ninnymonger

#

not every proof deserves a seven-page paper

dreamy iron
dreamy iron
marble lance
dusky epoch
#

ninnymonger (derogatory)

marble lance
#

😂

lavish jewel
dreamy iron
#

Lmao

next vapor
#

is the fact that a vector space is a direct sum of a subspace and its orthogonal compliment also true in the infinite dimensional case

#

ive been told it is but all proofs im finding are for the finite dimension case

dire thunder
#

well suppose it is not direct sum

#

first of all suppose it is just sum

stoic pythonBOT
#

Commander Vimes

dire thunder
#

wait i think it is not true @next vapor

#

ye

#

here is counterexample

stoic pythonBOT
#

Commander Vimes

dire thunder
#

then fix point c in [a,b] and take U to be set of all functions in that vector space s.t f(t)=0

#

@next vapor see that U and its orthogonal complement do not span space

next vapor
#

i see

#

hmm then how would one go about finding an orthogonal compliment for the subspace of odd functions on V=C[-1,1] given the inner product integral from -1 to 1 of f(x)g(x)

#

i know that even functions are in the compliment, but how do i show there arent any others

dire thunder
#

prolly by ibp spamming

#

hmm

#

i do not remember but it sounds like antiderivative of odd is even and of even is odd

quartz compass
#

I think you can do it by showing every function can be written as the sum of an even and odd function, $$f(x)=\frac{f(x)+f(-x)}{2} +\frac{f(x)-f(-x)}{2}$$

stoic pythonBOT
#

Merosity

next vapor
#

yea i tried that, doesnt it need to be a direct sum tho?

quartz compass
#

why do you think it isn't a direct sum

next vapor
#

sorry i mean it is a direct sum yea

#

but the dimension is infinite right

#

and i can only conclude using the direct sum argument if the dimension was finite no?

#

as in the vector space is a direct sum of a subspace and its orthogonal compliment is only true in the finite dimensional case

#

or am i missing something

quartz compass
#

what's 'the direct sum argument'?

#

I'm just writing a continuous function in a way that makes it the sum of an even and odd function

next vapor
#

how would you go from that sum to the orthogonal complement being exactly the set of even functions tho?

lavish jewel
#

the even functions are the orthogonal complement of the odd ones

next vapor
#

yea thats what im trying to show

lavish jewel
#

the product of an odd and an even function is odd

#

then use the properties of odd functions?

next vapor
#

hm ig i could just say that if we inner with an odd function we get an even function so the integral is not 0 unless one of the functions is 0

lavish jewel
#

what

#

inner product of what with an odd function

next vapor
#

sorry i mean taking an element of the odd function subspace

#

and inner it with another odd function

lavish jewel
#

you wanna show that evens are orthogonal to odds, yeah?

next vapor
#

nah i know they are, now i just have to show that the orthogonal compliment is exactly the set of even functions

lavish jewel
#

then you already have everything you need

#

just check what merosity wrote above

dusky epoch
#

why tf is everything so thin

arctic stone
#

Hey uhhh isn't this example of finding out B' incorrect?

#

I was taught that the change of basis matrix from B' TO the standard basis

#

is actually easy

#

but here it's the other way around?

dire thunder
arctic stone
#

God these stupid change of basis matrices just confuse me more and more, I've been trying to fully understand them for months now and whenever I think that I get them something contradictory comes up

dusky epoch
#

youre not alone

#

i personally keep getting confused which way they go even after years of this shit

arctic stone
#

I also hate how there are so many ways of writing them in different parts of the world

golden ermine
#

I also get confused even after drawing the commutative diagram

arctic stone
#

you mean a diagram like this one? or something else?

golden ermine
#

Oh something like this

arctic stone
#

ohhh

broken sun
#

Hello. Can you give me a simple example of an operator which has no adjoint?

dusky epoch
#

take V = the space of all polynomials with real coefficients with inner product given by <f, g> = sum f_k g_k [where f_k and g_k are the coefficients on x^k in f and g respectively]

define a map T: V -> V by Tp = p(1)*x^5

then T will not have an adjoint

wintry steppe
#

When we talk about two vector spaces being isomorphic, in what category are we talking about? The category of vector spaces?

#

Furthermore, what linear algebra books talk about things like the question I just asked? Mine doesn't ever use the word 'category'

native rampart
#

Category of Vect,ig

#

Morphisms are linear transforms

wintry steppe
#

Do you know what book talks about it, Buncho Dragons?

native rampart
#

not very familiar with the category theory approach

#

But I guess it's similar to how groups or sets work

wintry steppe
#

Are you an undergraduate?

native rampart
#

Kinda but I don't study math

wintry steppe
#

I see, CS or something then

native rampart
#

Aluffi is good,ig

dusky epoch
native rampart
#

Also,Category Theory isn't necessary to do intro algebra

dusky epoch
#

what are you talking about it obviously is

#

didnt you take a year of cat theory before you saw 2+2? /j

faint lintel
wintry steppe
#

this is why people like being coordinate-free

crude ridge
#

What would be a quick way to check if two sets of vectors are basis for the same space?

wintry steppe
#

if the space is finite-dimensional and you have your vectors in coordinates you can put them together into a square matrix and compute its determinant (i.e., check linear independence)

crude ridge
#

I don't understand how you would do that

#

Say I have two sets, each having 2 vectors that are in R5

wintry steppe
#

oh

#

you're asking for subspaces

#

nvm

#

hmm

crude ridge
#

Yeah not the entire R5 space

#

But yeah I'm struggling to think of a way to see if the first set of two vectors span the same space as the other set of two vectors

wintry steppe
#

it'd be enough to check that each of your two sets is linearly independent, and to write the vectors in one set as a linear combination of the vectors in the other one, i believe

crude ridge
#

Oh that's interesting

#

Visually, that makes sense if I'm thinking of subspaces in R3

daring ravine
#

I'm reading this paper on optimising the "Normalised Cut" for a similarity graph

#

Just confused by what they've written as the "Eigenvalue problem":

stoic pythonBOT
daring ravine
#

I'm confused by the RHS

#

Is it saying that $\lambda \mathbf{D}$ are the eigenvalues of $(\mathbf{D - W})$?

stoic pythonBOT
wintry steppe
#

no

#

what's lambda D?

#

if D is a linear transformation, no. linear transformations cannot be eigenvalues

lavish jewel
#

looks more like a generalized eigenvalue problem

daring ravine
#

So D-W is a "Laplacian", i thought it would be like:
$L y = \lambda y$

stoic pythonBOT
lavish jewel
#

right, so L is another linear transformation

#

seems you have $Ly = \lambda D y$

stoic pythonBOT
daring ravine
#

yeah exactly

#

which is not an eigenvalue problem i've really seen before

lavish jewel
#

this is a generalized eigenvalue problem

#

from wikipedia

daring ravine
#

ok awesome thank you!

#

I was spooked by it and thought i'd misunderstood previous parts of the paper

#

Thank you for cleaning this up for me ^^

wintry steppe
lapis fern
#

HI ALL. is there a name for this change of basis?

#

I've seen a discussion of something similar a few days ago.

wintry steppe
#

I’ll do anyone’s homework for money dm me

wintry steppe
#

done with a, my characterstic eqation is 0 = x'' + (a+d)x' + (bc-da)x

#

my question is how do I get x(t) and y(t)

#

for part B

dusky epoch
#

well you can get x(t) as the solutions of your 2nd order DE

#

what substitution did you make to arrive at it btw?

wintry steppe
#

i differentiated the first equation and substituted the second one

#

and then i solved for y and substituted again

dusky epoch
#

so you solved for y in terms of x and x'?

wintry steppe
#

yea

#

and then plugged it into the third equation, the differentiated one

dusky epoch
#

do you have that written out somewhere

#

cause thats what youll be using to recover y

wintry steppe
#

yeah sure i could send a picture

#

@dusky epoch how would I go about solving the second order differential equation

dusky epoch
#

isnt it literally just a linear differential equation with constant coefficients...

wintry steppe
#

it's second order

dusky epoch
#

and?

#

it'll have two solutions $x = e^{\lambda_1 t}$ and $x = e^{\lambda_2 t}$

stoic pythonBOT
wintry steppe
#

right

dusky epoch
#

where $\lambda_1, \lambda_2$ are the roots of your characteristic equation, and also the eigenvalues of $\bmqty{a&b\c&d}$

stoic pythonBOT
wintry steppe
#

yes so I differentiate x twice and plug in to the characterstic equation

#

and solve for lambda

#

?

dusky epoch
#

your lambdas are facing the wrong way

#

but yes

wintry steppe
#

oops

wintry steppe
#

i couldve sworn my teacher drew them that way lol

grizzled sphinx
#

how do I do the last part goddammit, it hurty my brain

lavish jewel
#

looks like an exam

#

lol they left the server

dusky epoch
#

whomst?

lavish jewel
#

pickleman68 posted an exam, and as soon as i asked about it, they left the server

dusky epoch
#

ah

frosty vapor
#

i banned them i thought

#

yeah i did ban

lavish jewel
crude falcon
#

in the second paragraph, when they refer to lambda as dominant eigenvector, that is a typo and they refer to an eigenvalue lambda right?

#

same with the last paragraph

lavish jewel
#

yeah

dusky epoch
#

actually it's the lambda that should be changed instead

wintry steppe
#

Is there a proper infinite dimensional subspace F of a inner product space V where every vector in V has a orthogonal projection in F?

civic anchor
#

if i row reduce a matrix do i still get the same cofactors from co factor expansion

native rampart
#

Row reduction does not preserve determinant

#

So,I don't think so

civic anchor
#

oh okay ty

wintry steppe
#

<@&286206848099549185>

#

maybe i should rephrase

#

Is there a pair (V, F) where F is an infinite dimensional subspace of a vector space V such that for every v in V, the orthogonal projection of v in F exists?

#

if F was finite dim, this projection always exists. and its easy to construct a infinite dim F for which some v dont have

soft abyss
#

maybe a really basic question, but here goes: if you allow column operations from the right to left (i.e. adding a column to a more rightward column) and row operations from the top to bottom, then every matrix can be turned into a permutation matrix (well, a permutation matrix with some columns all zeroes)

#

what can we say if you only allow row operations from bottom to top, and only allow scaling of columns by some nonzero (real or complex ) number

#

?

wintry steppe
#

hi

wintry steppe
#

If A² = - I, Identity matrix

How to know that the eigenvalue is not a real number?

red prawn
# soft abyss maybe a really basic question, but here goes: if you allow column operations fro...

A row operation corresponds to multiplication on the left by the appropriate matrix. You can find out which matrix by applying the row operation to the identity matrix.

As for scaling of columns:
A column operation corresponds to multiplication on the right by the appropriate matrix. Scaling a column would be multiplying on the right by the diagonal matrix with all 1's except for the scaling column. Again, you can find out which matrix corresponds to the column operation by performing the operation on the identity matrix.

quartz compass
stoic pythonBOT
#

Merosity

soft abyss
#

For example if we allow all row and column operations then every class is represented by a partial permutation matrix

red prawn
#

Maybe find matrices representing these allowable operations, and look at the set of those

wintry steppe
soft abyss
#

Yeah, the matrices are the set of upper triangular matrices B, and the algebraic torus T

#

I was just trying to phrase is in linear algebra terms, but that’s essentially the problem I’m working on

lavish jewel
#

A^2 v = A (Av) = A lambda v = lambda A v = lambda^2 v

soft abyss
#

B^+ M B^-1 gives you the permutations a where the B’s are upper and lower triangular

#

I’m thinking about B M T, where T is like you described

wintry steppe
soft abyss
#

It might not have an obvious answer but just making sure I haven’t missed something obvious

broken sun
red prawn
#

You could think of it as orbits of left/right action

soft abyss
#

Ha, that’s exactly what I’m working on 😛

dusky epoch
broken sun
red prawn
#

So "from bottom to top" meaning upper triangular?

soft abyss
#

Right

broken sun
#

Also, "why don't you try finding out yourself" can be an answer to any question asked here.

dusky epoch
#

it's worth knowing what the question-asker has tried, if anything.

#

anyway, try considering where T* would have to send monomials (1, x, x^2, ...)

red prawn
#

And you're looking for representatives of equivalence classes given by orbit under (b,t).m = bm(t^-1)? Does this sound like appropriate phrasing?

dusky epoch
#

if i am not mistaken, you will find that T*(x^5) would have to be a non-polynomial

soft abyss
#

Yeah I think so

#

Possibly b ^ + m t but I think it’s similar

red prawn
#

Yes, something to guarantee left action even though you're multiplying on the right

soft abyss
#

I’m not massively familiar with this stuff yet

#

So most likely yeah

red prawn
#

(also I think of it as pre-composition, so you're moving the coordinates of the system rather than the body, if you're thinking of the maps acting on a vector space)

broken sun
wintry steppe
soft abyss
#

Right l think the T is doing the re scaling

dusky epoch
soft abyss
#

And the B is just a normal action of multiplication

#

I’m not 100% clear either lol

red prawn
#

pre-composition by an inverse, it's like translations in hs algebra. f(x-a) shifts to the positive direction

broken sun
quartz compass
soft abyss
quartz compass
#

you can't "cancel" the vectors that's a good point, but what we do know is that eigenvectors are nonzero and that the 0 vector is unique so we could add v to both sides to get 0 = (lambda^2 + 1) v. Since v is nonzero, we know lambda^2+1 = 0

soft abyss
#

I’ve played about with it, and I think it’s like a permutation matrix, but you can have repeated 1s in a row

#

As well as all zero columns

broken sun
#

People may not be as smart as you expect.

soft abyss
#

Does that sound believable?

red prawn
#

Well you're not allowing column additions, so you wouldn't be able to "get rid" of the repeated ones if you were doing column ops

quartz compass
#

you're welcome

dusky epoch
#

let $T^(x^5) = \sum_{k=0}^{\infty} a_k x^k$, where the right-hand side has to have finitely many terms (else it is not a polynomial). consider $\ang{x^m, T^(x^5)}$, then you have:

$$a_m = \ang{x^m, T^*(x^5)} = \ang{T(x^m), x^5} = \ang{x^5, x^5} = 1$$

for \textbf{all} $m$, which would imply $T^*(x^5) = 1 + x + x^2 + x^3 + \dots$

soft abyss
#

But we can get rid of repeated 1s in the B m B case

#

Which allows column operations

stoic pythonBOT
dusky epoch
#

@broken sun here

soft abyss
#

I’m 95% sure anyway

#

But yes they have to stay in our case

red prawn
#

I think you got a clear picture, just a matter of explicitly writing the eq classes by this point

soft abyss
#

I think I do yeah thanks for the chat anyway!

broken sun
dusky epoch
#

yes, with my choice of inner product the monomial basis is orthogonal

broken sun
dusky epoch
#

i will not indulge your self-deprecating remarks

#

i do not know how much experience you have with linear algebra (and higher math in general), though now i think it's too little

#

so it's not that you're not smart enough, if anything it must be that you're not experienced enough

broken sun
#

I usually do not solve math problems; I usually read only main texts.

wintry steppe
#

sounds inefficient

#

doing the problems is a great way to get better

quartz compass
#

reading about math is to math like going to an art museum or watching a sports game are to painting and playing the sport

dusky epoch
broken sun
#

What is "ngl"?

dusky epoch
#

math isnt a spectator sport; if all you do is passively read texts without sitting down and doing some exercises / solving problems / proving results then your retention will be almost nil

#

ngl stands for "not gonna lie"

stable kindle
#

yeah, you gotta go through the exercises

#

you really really gotta actually rederive the proved results and then apply them to the problems, it's the onyl way

wintry steppe
#

good morning guys

#

if anyone can explain this that would be nice :)

#

i dont know what trA means

#

I understand that detA means the determinant of A

stable kindle
#

trace

wintry steppe
#

what is that

#

😐

stable kindle
#

sum of the elements on the main diagonal

wintry steppe
#

mmm

#

ok

wispy thicket
#

hello can anyone explain how to find an orthogonal basis that contains a set?

#

given an inner product, I found that the set is orthogonal. Not sure if that's part of the solution

vale plover
#

well, they should be orthogonal to be part of the basis

#

what i would do is applying vectorial product to v1,v2

#

so you obtain a third vector v3, that will be orthogonal to v1 and v2 at the same time

#

that can be a solution

wispy thicket
#

I technically found said v3 in a previous subproblem

#

so those 3 vectors would form the basis, then?

vale plover
#

another solution would be proposing a generic vector v3=(v3x, v3y, v3z). Then it should be orthogonal to v1 and v2, so it has to satisfy <v1,v3>=<v2,v3>=0

vale plover
#

well more formally what you have found with those solutions is a group of 3 orthogonal vectors in R3

#

if you want to go further, you should prove that those vectors generate R3

wispy thicket
#

I see, thanks. I wasn't sure if I just had to do that since some of my notes regarding this was just Gram-Schmidt

vale plover
#

i didn't put it beacuse is easy to see that they will generate R3

vale plover
#

in this particular case you know that v1 and v2 are orthogonal

#

if they weren't you can use GS

wispy thicket
#

ah I see, thanks!

wintry steppe
#

by checking that it sends π to 0

#

It's already the feature of the set.

#

what?

#

I mean that it's already f(pi) = 0.

#

that's the condition for a function from R to R to be in the set

#

you check that to show that something is in it

wintry steppe
#

?

#

ok

#

It's the FUCKING CONDITION.

#

not the feature.

lavish jewel
#

it says V is a vector space of real functions. check if the functions for which f(pi) = 0 are a subspace of V.

wintry steppe
#

calm down lol, sorry if i offended you

lavish jewel
#

no, but i know some german

wintry steppe
#

Oh, okay.

#

edd knows everything

#

Edd is God himself.

native rampart
#

Ergo God is Engineer

lavish jewel
#

tteppa is a considerable tteppa

wintry steppe
#

considerable is tteppa a tteppa

wintry steppe
#

they're all good.

#

kinda stuck at the first point.

#

showing that zero function is an element of T.

lavish jewel
#

well, i would sure hope that z(x) = 0 is 0 if you evaluate it at z(x=pi)

wintry steppe
#

but the zero vector must map every element of the domain onto zero in the co-domain.

#

Am I right?

lavish jewel
#

that's what i wrote up there

#

let z(x) = 0, the zero function

#

this satisfies that z(pi) = 0, so it's in T

wintry steppe
#

Jeez.

wintry steppe
lavish jewel
#

oh, another foreigner studying in germany

#

i feel you

wintry steppe
#

It's cheap you know.

lavish jewel
#

hey, i'm doing the same

#

😛

wintry steppe
#

Where are you now?

lavish jewel
#

somewhere in thüringen

wintry steppe
#

from the States?

lavish jewel
#

somewhere in latinamerica

wintry steppe
#

hmm.

#

Masters?

lavish jewel
#

did masters, now doing phd

wintry steppe
lavish jewel
#

gleichfalls

wintry steppe
lavish jewel
#

oof

wintry steppe
#

have you ever encountered one of them?

#

Jeez, they're so fucking dumb.

#

one of them just said to me: verpiss dich Amerikaner. Hahaha.

#

i assume that does not mean anything good

lavish jewel
#

classic. yeah, not the nicest encounters... this is a better convo for the discussion/chill channels tho

wintry steppe
#

can you guys help me with my linear algebra final haha

dusky epoch
#

help in what sense?

#

we are not going to help you cheat on it

wintry steppe
#

i need a sense of direction

nocturne oracle
#

most cellphones nowadays should have a compass built in

#

they also usually have some type of map

wintry steppe
#

lol

nocturne oracle
#

🙂

wintry steppe
#

i think im facing lake michigan right now

#

should be facing north then

charred shell
#

could anyone please help me

I have
W1= {x(1,2,3) where x is in R} C R3
I have to find dimension of W and Wt(orthogonal complement)

I found it as W= 1 and Wt=3-1=2

I'm not sure how to find Wt

short coral
#

Please help me understand this explanation

#

I didn't get which elementary operations were applied

novel crescent
#

hey guys i need help with linear equations, who can help me? dm

wintry steppe
#

or you can just post your question here

novel crescent
#

okay

#

hold up

#

someone pls help

#

i been stuck on this problem

lapis fern
#

,rotate

stoic pythonBOT
lapis fern
#

the point of intersection needs to be a solution to both, because that point is on the red line, as well as also being on the blue line.

#

also, with those empty boxes.....plug in your value for y and x

you'll see that the equalities agree. it's like a sanity check.


.

#

from Axler page 42.

my question: an immediate corollary of this is that dim U + dim W = dim (U ⊕ W )?

#

we have a span of W, and the w_i's are all linearly independent

#

so its a basis for W, of length n. hence dim W = 5.

#

also $$v = a_1u_1 +\, \ldots \,+ a_m u_m + b_1w_1 +\, \ldots \,+ b_nw_n$$ demonstrates a basis for V, so dim V is m+n ?

stoic pythonBOT
#

Videlicet

lapis fern
#

basically i need a justification for $$dim(U \oplus W) = dim V = dim U + dim W$$

stoic pythonBOT
#

Videlicet

wintry steppe
#

uh

#

idk if you guys are busy

#

but im wondering what it means for the origin to be stable/unstable

#

just using Matrix A with a system of equations

novel crescent
#

Can someone lmk if this is corrrect?

lapis fern
#

its wrong. are you doing it by eye?

wintry steppe
wintry steppe
#

you can check stability at the origin by looking at the (real parts of the) eigenvalues of A

#

if they are nonpositive, then the origin is stable, and conversely

nocturne oracle
#

i wish i had terra 2 help me on my la final 🥺

lapis fern
#

TTerra, while youre here might i trouble you with a question, please?

sonic quartz
#

@wintry steppe help pls exam due in 10 minites

frosty vapor
#

@wintry steppe be considerable

frosty vapor
#

what are the conditions on U and W

lapis fern
#

U is a subspace of V, and so is W.

and $$U \oplus W = V$$

stoic pythonBOT
#

Videlicet

frosty vapor
#

so this forces U intersect W to be ?

#

well

#

no

lapis fern
#

zero vector?

frosty vapor
#

no it isnt necessarily

#

this is what i was getting at

#

it needs to be backwards

#

we need intersection to be zero vector first

#

then it follow

#

U sum W could be V sure

#

but that isn't enough i think

#

@wintry steppe wat u think

#

my enlgihs

#

i am brain worm

lapis fern
#

i guess what i want is : $$ U \oplus W = V \implies dim U + dim W = dim V$$

stoic pythonBOT
#

Videlicet

lapis fern
#

is that true?

frosty vapor
#

ye no that is false pretty sure

wintry steppe
#

this is the internal direct sum right

#

dim V = dim(U + W) = dim U + dim W - dim(U cap W), and this last term vanishes

lapis fern
#

internal? what's that?

wintry steppe
#

ok nvm, ignore that comment

frosty vapor
#

monkers

#

why the last term gonna vanish

#

er

#

oh this comes from U, W subspace V

wintry steppe
#

U \oplus W = V usually means U + W = V and U cap W = 0

#

like by definition

frosty vapor
#

ye i see

#

okay yeah this works

#

i was more worried about the U cap W going to zero

lapis fern
frosty vapor
#

if you want to call it that ye

wintry steppe
#

linear algebra catThonk

lapis fern
#

i do too, lol

frosty vapor
#

i never knew that the oplus had that condition tho

#

i thought it was just take linear combo of everything

#

cool

wintry steppe
#

that's how it's defined in friedberg

lapis fern
frosty vapor
#

catThink my class didn't do oplus in my linear algebra class 🐲 no wonder

#

makes sens now tho

#

excelent

#

the only thing i know from oplus was from the group theory

wintry steppe
#

same thing

#

vector space is group wrt addition

#

well

#

i guess you have to account for scalar mult

frosty vapor
#

vector space is vector space

#

😼

sonic quartz
#

oplus is just coproduct in Ab

#

obv

wintry steppe
#

die

nocturne jewel
#

math is math motel

frosty vapor
#

hsct

lapis fern
sonic quartz
#

im being sullied

#

Where Is The Lie

wintry steppe
#

you're correct, but also, bruh

frosty vapor
sonic quartz
#

wdym this is the correct pedagogical approach

wintry steppe
sonic quartz
#

lol every time I join a question channel I just turn it into #chill

wintry steppe
#

ok, quick, everyone give me a cool linear algebra fact

sonic quartz
#

🚶

wintry steppe
#

the prize is my recognition

frosty vapor
#

Fredholm alternative

wintry steppe
#

ok ultra

frosty vapor
#

what

wintry steppe
#

lol

#

"fredholm" makes me think of C* alg stuff

frosty vapor
#

ooga

wintry steppe
frosty vapor
#

i learned about fredholm alternative in my diffeq class 💀

#

its so cursed

sonic quartz
#

was that the class that blackboxed differential forms

frosty vapor
#

no that was the first diffeq class

#

this is the "intermediate" one

#

but uh

#

this is how it should always have been

#

with linear algebra

#

sully first diffeq class had none

#

anyways time to read friedberg because i never learned direct sum

sonic quartz
frosty vapor
#

in group theory class we learned about internal and external product

#

which was cool

#

but

#

now i can return to linear algebra

verbal pivot
#

i find the fact that null spaces stop growing pretty cool to be honest

wintry steppe
#

elaborate

verbal pivot
#

Consider an operator $T \in L(V)$ where $dim(V) = n$, for all $k > n$ we have that $null T^{k} = null T^{n}$

stoic pythonBOT
#

b2unit