#point-set-topology

1 messages · Page 164 of 1

marsh forge
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Heres a hint

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It suffices to show that if I fix some point (x,y)

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All other points have a path to (x,y)

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You can choose a nice (x,y) if you want

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That does seek

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Seem

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Like a nice choice

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That is not a bad idea

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Np

eternal anvil
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so did I miss this or can you define an n-dimensional manifold as any set that is locally isometric to a subset of Rn

marsh forge
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Locally homeomorphic

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Or diffeo

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If you wanna be fancy

little hemlock
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About the first hint: is f(y) = d(x,y) continuous? If it is, then f(A) is bounded and attains its bounds and the conclusion (for the first part) follows.

fervent citrus
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yes it is

little hemlock
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I think I just wrote a proof of continuity. one sec

fervent citrus
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it's even 1-lipschitz

little hemlock
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Proof(?) Let $y \in X$, let $\epsilon > 0$ and take the open ball $V = (d(x,y) - \epsilon, d(x,y) + \epsilon) \subset \bR$. If $U = B(y, \epsilon/2)$, then we have that $f(U) \subset V$ by definition of $U$.

gentle ospreyBOT
little hemlock
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Seems kinda trivial thonk
I have no idea what 1-lipschitz means xd

fervent citrus
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it means that for all $y$ and $z$ in $X$, you have $d(f(y), f(z))\leq d(y, z)$

gentle ospreyBOT
fervent citrus
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which implies the (uniform) continuity of f

little hemlock
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that would just follow from triangle inequality, right?

fervent citrus
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Yes

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for all y and z in X, you have
d(x, y)<=d(x, z)+d(y, z)
and
d(x, z)<=d(x, y)+d(y, z)

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from which you can obtain |d(x, y)-d(x, z)|<=d(y, z)

little hemlock
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i see. thank you!

fervent citrus
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You're welcome

fluid cloud
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Heylu

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What's the natural metric on functions in [a,b]?

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A question requires me to find d_1, d_2 and d_infty of certain functions

marsh forge
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Where are they valued

fluid cloud
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erm

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[0,1]

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Consider the function $f(t):=t$ and $g(t):=t^2$ for $t \in [0,1]$. Compute
$$ d_1 (f,g) \ d_2 (f,g) \ d_{\infty} (f,g) $$

gentle ospreyBOT
fluid cloud
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ueruoer idk how to typeset on texit, but you get me right

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i dont want the entire solution, i just wanna know what the metric is

gritty widget
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d_2 is standard

fluid cloud
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yeah idk the standard for functions

gritty widget
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I gues d_1(x,y) is |x-y|

fluid cloud
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sis-

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please read my question, x and y are not real numbers

marsh forge
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My best guess

gritty widget
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idk my guess would be calculating distances of f(t) and g(t) for all t and taking supremum idk

marsh forge
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These are the standard choices

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Putting p=1,2,infty

fervent citrus
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when working with bounded functions, d_infty is pretty natural

marsh forge
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Whats your point lol

fluid cloud
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i think godel might be right

marsh forge
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These functions are trivially bounded

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Godel told you dinfty

fluid cloud
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idk how norm might help here tho

marsh forge
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Norms induce metrics

fluid cloud
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@fervent citrus idk what the natural is

marsh forge
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The metric@induced for p=infty

gritty widget
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yeah those 1 2 and infty are from p norm

fervent citrus
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What's the natural metric on functions in [a,b]?
is pretty hard to answer when asked just like that

marsh forge
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The p-metric induced by the p-norm

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Is what you want

gritty widget
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yeah the standard one is d_sup metric

marsh forge
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He clarified later

fluid cloud
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Honestly, I have no idea what I want, this is from my teacher's problem sheet; and-

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let's just say-

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he isnt that good...

marsh forge
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Wolf pls trust me lol

fervent citrus
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Big sad

marsh forge
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I told you what you want

gritty widget
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wolf pls trust me lol

fluid cloud
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lmao

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oki i trust u

gritty widget
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yeah but those are functions, so you take p norm on all the points then take sup

marsh forge
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Weird he didnt define them tho

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Have you not read oart of the book or smth

fluid cloud
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no book :(

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he just blabbers stuff in lectures and thats it

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yeah but those are functions, so you take p norm on all the points then take sup
@gritty widget that's exactly my concern, um, x isnt a vector right

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Let p ≥ 1 be a real number. The p {\displaystyle p} p-norm (also called ℓ p {\displaystyle \ell {p}} {\displaystyle \ell {p}}-norm) of vector x = ( x 1 , … , x n ) {\displaystyle \mathbf {x} =(x{1},\ldots ,x{n})} {\displaystyle \mathbf {x} =(x_{1},\ldots ,x_{n})} is

‖ x ‖ p := ( ∑ i = 1 n | x i | p ) 1 / p . {\displaystyle \left\|\mathbf {x} \right\|_{p}:={\bigg (}\sum _{i=1}^{n}\left|x_{i}\right|^{p}{\bigg )}^{1/p}.} \left\|\mathbf {x} \right\|_{p}:={\bigg (}\sum _{i=1}^{n}\left|x_{i}\right|^{p}{\bigg )}^{1/p}.
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um, @gentle osprey plis halp

fervent citrus
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bad latex

gritty widget
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you didnt put $$

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?

fluid cloud
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lmao

gritty widget
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$ texit command $

fluid cloud
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lemme just take a screenshot

gritty widget
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texit doesnt work for free, you gotta give it the dollars you know what im sayin?

fluid cloud
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BWAHAHAHHA

marsh forge
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They specialize it to functions

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W intregrsls

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Later in the page

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Scroll down

fluid cloud
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oki hang on

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:o

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im dumb.

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why dont i read the entire thing

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lmfao

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i think that's the one

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$$ \int_{X} | f(x) -g(x) | ^p d \mu $$

gentle ospreyBOT
fluid cloud
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okay, so X is [0,1], and whats mu?

fervent citrus
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probably a measure but don't worry about it

marsh forge
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Just integrate like normal

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Ignore mu

fluid cloud
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aite, thanks for your help!

sleek thicket
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Let X be a (hausdorff, second countable?) topological space. Define an n-dimensional smooth structure on X to be a sheaf of rings F on X with local stalks such that (X, F) is locally isomorphic to (R^n, C^infty).

Let M be a smooth manifold. Let (S, ι) be a pair of a topological space S and an injective continuous map ι : S -> Μ. Let F be the sheaf of smooth functions on M and G the sheaf of continuous functions on S. Pullback gives us a sheaf map ι^* : ι^(-1) F -> G. Let H be the image of ι^*.

I want to say something like there exists a smooth structure on S making ι a smooth immersion if and only if H is a smooth structure on S (and in this case, ι is a smooth immersion). Does anybody have thoughts about this? Have I missed an obvious counterexample?

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If S has a smooth structure such that ι is a smooth immersion, it has at most one, see ISM 5.18 and 5.32 (i guess with the sheaf definition this is up to isomorphism)

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Here's why I'm thinking this: Let S be an immersed submanifold of M and suppose U is an open subset of S. If a function f : U -> R is smooth, we can cover U by {Ui} where Ui is am embedded submanifold of M. Then the restrictions fi of f to Ui are smooth functions on an embedded submanifold, so there is some Vi open in M containing Ui and a smooth function gi : Vi -> R such that fi = gi|Ui. Thus a smooth function on an immersed submanfold is locally the restriction of a smooth function on the big manifold. Conversely, such a function is obviously smooth

silver nexus
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What are barycentric coordinates?

dusty condor
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Baricentric coordinates are coordinates in a simplex in such a way that the coeficients sum 1. I mean, you have a simplex given by the vertices and you can describe the points in the simplex with affine combinations with coefficients whose sum equals 1

silver nexus
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😮 Do you know where I could read more about these?

dusty condor
pseudo crane
tough hamlet
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no it's just a real number

pseudo crane
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Hm

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It seems like this wouodn’t make sense if the members of X are not real numbers

tough hamlet
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generally if it gets used in an inequality

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it's a real number

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the metric maps into R

pseudo crane
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That’s what I would assume

tough hamlet
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it still makes perfect sense

pseudo crane
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Oh

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Ok

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Yeah for some reason in the next problem I forgot that delta represented a distance

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thanks

tough hamlet
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np

marsh forge
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@honest narwhal this doesnt belong here but i have the other channels muted

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Can you give me a sketch of the uniformization thing

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that you were talking about

honest narwhal
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So I'm not terribly aware of the proofs of uniformization, and lol that super works here

marsh forge
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this looks like some pretty heavy machinery

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is this reasonable for a project

honest narwhal
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It might be on the tough end, mostly just feels like a cool theorem. I think a lot of proofs pretty much boil down to constructing these things called "Green's functions"

marsh forge
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This actually isn't too bad

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i found a like 10 page paper

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oh lmao this was overseen by Bhargava

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maybe its an reu paper

honest narwhal
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Which are you looking at?

marsh forge
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Uh it was one of the first results but im going to dinner now

honest narwhal
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Alright, well there may be other things, I mostly suggested it since it's an S-tier theorem which involves complex analysis and links to topology

marsh forge
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Yeah im into it

hybrid echo
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Hey nerds, so my prof was saying something, and I wanted to check to make sure I understand a few things properly

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Is xsin(1/x) rectifiable using Cauchy-Crofton?

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Because at least, my intuition is that the lines that intersect an infinite number of times would have measure 0, and therefore we can assign a length over any finite interval

coarse kestrel
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@dim meadow this channel's description 👀

dim meadow
celest flare
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Suppose I have a topology on X. Then can I say that the boundary of a set A is X - int(A) - ext(A)?

west spindle
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sure

gritty widget
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🥴

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(Differential Geometry)

sleek thicket
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I haven't been able to think about my manifolds hw for the last couple hours, so I'm going to do it in here

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Let M be an embedded submanifold of R^n

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I've shown that if y is some point in R^n and x a point in M minimizing |x-y|, then x - y is orthogonal to the tangent space T_x M

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because the function f(p) = |p - y|^2 is smooth and minimized at x, and so its differential at x is the zero map, but it's differential is given by dotting with grad f(x) = 2(x - y)

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Okay so define E : NM -> R^n by E(x, v) = x + v. This has a bijective differential at each point (x, 0), and so at each point there's a neighborhood of (x, 0) on which it's a diffeomorphism

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We can assume that neighborhood is of the form V_δ(x) = { (x', v') in NM : |x - x'| < δ and |v'| < δ } by shrinking it

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I want to shrink δ so that there's a unique closest point in M to anything in the union of the V_δ

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The confusing this is that this isn't a local condition

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I'm also confused about how to show existence of a closest point at all, let alone uniqueness

glad badger
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I have a problem, I hope this is the right chan, don't know what "degree" this is on but anyway

I have n number of 3D points (x,y,z) any 3 of these form a plane

Based on A plane I want to convert all the 3D points to 2D, mainting ratios etc (I want to do 2D calculations on the 3D points). I hope this makes sense.

bitter yoke
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This should just be projection onto your plane

pliant radish
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I found the first general solution

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How can I find the next part?
for the next point?

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please help : )

gloomy plover
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Not sure if you're even asking in the right channel

ivory dragon
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[definitely not]

stable jackal
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$sphere: (x-1)^2+(y-2)^2+(z+1)^2=9 \ curve: l(t)=(1+t,2+t^2,3+3t^2), \quad t\inℝ$

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how do I find the shortest distance from the sphere surface to the curve numerically?

gentle ospreyBOT
sweet wing
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you're basically minimising distance with constraints

dire warren
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How would I find this form that pulls back to dtheta if it wasn’t given in advance?

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<@&681259184582688842>

keen cliff
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idk how to help for that 1 but also idk which channel dynamical systems goes in GWchadThonkery so I'll put it in here for now

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i can show it's dense, Q²/Z² are all periodic so they're dense

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i have no idea how to find a non recurrent point tho

wanton marsh
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can you remind us of all the definitions

keen cliff
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Ya

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$x \in R(A) \iff x$ is a limit point of the sequence $x_n = A^n(x)$

gentle ospreyBOT
wanton marsh
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is A given by a matrix in M2(Z) ?

keen cliff
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A is a 2×2 integer matrix with determinant 1, and has eigenvalues non-roots of unity

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so like, eigenvalues have |λ|≠1

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there's one |λ|>1, and the other is 1/λ

wanton marsh
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yeah

keen cliff
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NW is non-wandering but that part is easy

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i am just completely bamboozled on R(A) ≠ T²

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I've been trying to get an argument that just like

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"finds" a point that does the trick

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my friend suggested to me suppose R(A) = T²

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and I was like

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hwhat

wanton marsh
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the exercise about the circle is easier lol

keen cliff
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i haven't done that one thonkeyes

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or have i eeveeThink

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feels like there's some sort of cantor set- like thing

wanton marsh
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it's not exactly the same problem since you don't have the det=1 requirement

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though

keen cliff
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i was having very loose ideas about this thing last night tho

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some sort of 2d cantor set thingy but couldn't put anything concrete enough together

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is (T²,A) conjugate to anything that might be helpful GWchadThonkery

wanton marsh
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I would try to pick a point in one of the eigenlines but

keen cliff
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yeah like

wanton marsh
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then a small ball around it corresponds to lots of small intervals on that line

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and you have to make sure you avoid them ?

keen cliff
wanton marsh
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wait am i just dumb

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why am i not thinking about the eigenline that has a small eigenvalue

keen cliff
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it'll go to 0

wanton marsh
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every nonzero point on that line should work

keen cliff
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SHIEEEET

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well I'm dumb too

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I've been working on this problem for ages

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thanks!!!

wanton marsh
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lol I was thinking about the circle exercise

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where Em is a dilatation

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so it automatically made me pick the other line

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first

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xD

keen cliff
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fooo

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k

dire warren
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@keen cliff oh hell you r doing Brin and stuck

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We shud make a new adv channel for dynamcial systems

keen cliff
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Yeah I am @dire warren

dire warren
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I beleive chapter 2 has that beast of a theroem

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Van de waarden

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Have fun haha

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This book is wild

keen cliff
dire warren
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The difficulty level varies so much between parts

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Is this for a course or self study?

keen cliff
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course

dire warren
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Nice

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Are they gonna cover the whole book?

keen cliff
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theorem 2.8.1 van de waarden
exercise 2.8.1 prove theorem 2.8.1 using proposition 2.8.2

dire warren
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Ppft

keen cliff
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nah not the whole book but I'll probably end up continuing as self study cuz this stuff is hella cool

dire warren
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😄

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Indeed

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If u ever want more dynamical systems reading I can recommend some

keen cliff
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do u have any books that does things a little bit slower

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i am KIND OF getting destroyed right now

dire warren
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Katok hassellblatt’s first course in dynamics covers similar material at a slower pace

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NOT the “intro to modern dynamical systems”

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That one is kinda MonkaS

keen cliff
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that one is very monkaS

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i tried going thru the beginning of that during reading week

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got stuck in the 0th section

dire warren
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Hahaha

honest narwhal
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Oh I have lecture notes on the Van der Waaerden section

keen cliff
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@honest narwhal pass em

honest narwhal
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@keen cliff

wheat axle
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Someone help me with my geometry hw

sleek thicket
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Let G be a lie group. A smooth representation of G is a finite dimensional \R-vector space V and a smooth homomorphism G -> GL(V). To each of these, we can associate an \R[G]-module V. When does an \R[G]-module give rise to a smooth representation of G?

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Like you can just say that it's finite dimensional over R and the action map G -> GL(V) is smooth, but we can we characterize in a more direct way?

viscid shadow
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are there 3d uniform tilings ?

oak thistle
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Can anyone help me with cone and cylinder?

gritty widget
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what kind

oak thistle
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Uh

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Problems on it

marsh forge
gritty widget
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they might be talking about the cone of a topological space or the mapping cylinder

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I joke

oak thistle
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I don't know topology

gritty widget
oak thistle
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Oh

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But it's not pre University level

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Equation of cone and stuff

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This problem

frigid patrol
marsh forge
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this is a good take

sweet wing
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This is topology. Our space are nice. Our sequences are exact. Our groups are abelian.

midnight jewel
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This is a thread about math not set theory.

west spindle
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can someone ELI5 what the fuck Spec(Z) is

marsh forge
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Set of prime ideals

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With a topology

honest narwhal
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"This is a thread about math not set theory"
Hot damn someone got destroyed

verbal prairie
dim meadow
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Fundamental group is abelian???

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Wtf

marsh forge
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Our spaces are simply connected

dim meadow
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Maybe if you only study loop spaces and topological groups

marsh forge
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Woke

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Dont forget spheres

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And homotopy spheres

verbal prairie
small obsidian
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I agree I've never understood Spec(R)

sleek thicket
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Suppose I start with an \R-algebra A and build up a manifold M such that A = C^infty(M). I can then define TA = C^infty(TM) (where TM is the tangent bundle). Is there a more direct way to characterize/build TA in terms of A?

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A book I'm reading says you can do it but it would be too far out of the way

peak narwhal
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Can half space (like half planes) work in three-dimensional (x,y,z) space? Do they just remain two-dimensional planes?

midnight jewel
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yea, a half-space in general is just the set of all $x$ such that ${\lambda(x) \geq 0 \mid \lambda\colon \R^n \to \R \text{ linear}}$

gentle ospreyBOT
midnight jewel
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the boundary, where λ(x) = 0, will be an (n-1)-dimensional hyperplane

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note that there’s the degenerate case λ(x) = 0 ∀x, which you may wanna exclude, or not

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we didn’t exclude it in our definition because it allows you to say that a manifold with boundary has each point having a neighborhood homeomorphic to a half-space

cursive nebula
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hey guys, what is S^2?

delicate spire
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surface of a sphere

cursive nebula
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AH!

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i was suspecting that but wikipedia says "two-dimensional"

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so i thought "two-dimensional" meant it was on a plane

bitter yoke
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The surface of a sphere is two dimensional

delicate spire
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topology people are weird

cursive nebula
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now i'm not really sure i know what it means to be two-dimensional.

bitter yoke
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I mean, the surface of the earth is locally flat

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It looks flat to us, and so the surface is a two-dimensional object

cursive nebula
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okay. ahh

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i just started studying topology today, so these things are a little alien still

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thank you for being patient

bitter yoke
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You'll learn about manifolds soon where you can formalize this idea

cursive nebula
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so i was thinking...
"two-dinensional" might mean "its points can all be described with two coordinates"

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but i can't do that with the surface of a sphere

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i could cut the sphere in half though and i could do it with the two halves

floral gust
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Are you familiar with tangents?

rugged swan
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You can locally do it

cursive nebula
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yeah

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i'm a math student

floral gust
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You can define the dimension as the number of independent tangent vectors

cursive nebula
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uhh

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so, it's the surface of a sphere.
that number can't be more than 3

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how do i prove it's 2?

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well, it's at least two, of course

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because i can picture a tangent PLANE in each point in the surface of a sphere

floral gust
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Yes. For which the number of independent tangent vectors can be atmost 2.

cursive nebula
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why 2 and not 3?

midnight jewel
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because linear algebra dictates that a plane cannot have three independent vectors

cursive nebula
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yeah, intuitively i dont see how there could be more

floral gust
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number of independent tangent vectors = number of vectors in the basis of the tangent plane = 2 since a plane is spanned by two vectors namely the one in x direction and the one in y

midnight jewel
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if you see the tangent space at a point as a vector space

delicate spire
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latitude and longitude

cursive nebula
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OH YEAH i know that!!

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ahh alright

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so. the surface of a sphere is locally a two-dimensional object

midnight jewel
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ye. and a thing which is everywhere locally of the same dimension is called a manifold of that dimension (this is a very rough definition)

floral gust
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Yes you can say that. To formalize this notion of dimension, you will study more in manifold theory

midnight jewel
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(like, very rough)

cursive nebula
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do you consider the tangent space for... each point of the surface?

midnight jewel
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what you do often is consider charts, that is maps from a region in the space onto ℝⁿ for the right n

cursive nebula
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because if you consider two points that arent polar opposites you get two different planes

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ahhh regions. okay

midnight jewel
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oh, I completely misunderstood your question

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sorry

floral gust
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It is the dimension of those planes which is our concern

midnight jewel
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yes, each point has its own tangent space

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there’s a notion of the tangent bundle, which is basically the “union” of all these

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(but you also remember where you are on the surface)

cursive nebula
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AH!! ok. ok.

midnight jewel
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but yea here we just need the dimension

cursive nebula
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so i was thinking of this tangent bundle and i wanted to say that it's R^3

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but for a Single Point, it's a plane

midnight jewel
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it’s not just the union, so it’s more complicated than jsut saying it’s ℝ³

floral gust
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Dont... dive into these higher level topics like tangent bundle just now. They require a bit of prerequisite knowledge of manifold theory and this sort of abstraction so fast would leave you confused.

midnight jewel
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like you don’t just take the union of some physical planes floating in space

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yea

cursive nebula
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mhmh..

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guys, can i ask you how you learnt this stuff?
do you know books you found very useful?

midnight jewel
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these things will be defined in due time, and possibly quite soon even

cursive nebula
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i have to study on my own because we're quarantined (coronavirus)

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so, no classes for now

midnight jewel
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I’m just taking classes. didn’t use any textbooks for diffgeo, which is where we covered manifolds

floral gust
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Why do you have to study manifold theory just now? Take your patience with it. Learn what you are studying right now with patience and detail.
But if you must, start with Differential Geometry of Curves and spaces, move onto introduction to topological manifolds and then onto smooth manifolds

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the latter two are by John Lee

cursive nebula
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ahh i can think of many answers

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one is that i have to take the exam in a couple of months

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haha!

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yes, thank you, i will check that out!

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i will also probably be hanging around in this channel ;v;💞💞

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our teacher let us download some solved exercises

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so i know what kind of stuff will be on the exams, but....
i need theory

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thank you for helping me :>
my questions will get progressively less and less dumb, and then... chef kiss diffgeo mastery.

marsh forge
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Uh what

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No

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You dont need diffgeo

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To do manifolds

floral gust
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Yeah it’s not like a prerequisite but more like preparatory material to get you familiar with the ideas you’ll see much formally in manifolds. Like differential forms etc. But maybe that’s just me

cursive nebula
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i dont really know what a manifold is, yet

this is a two semester course called "geometria 2". the first semester is about topology and algebraic topology and the second semester is called "curves and surfaces"!

we also have a "geometria 3" course in year 3, i don't know in which course we're going to cover manifolds, but i'm sure we will!

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(i think differential geometry is in this course though!)

marsh forge
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Youll cover it in the first

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The second is diffgeo

cursive flume
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when defining the standard topology, we have to define the soft ball, in which we basically use the "distance" or "norm"

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however it is said that it we don't need norm to define that

#

do we need vector space structure?or we don't need anything more than a set on r^n to define the soft ball?

vocal wharf
#

what

cursive flume
#

we define soft ball as follows: they are d- duples, for which holds, that $ \sum_{i=1}^d (q_i-p_i)^2<r^2$

gentle ospreyBOT
cursive flume
#

does this not imply the definition of norm?

vocal wharf
#

this just looks like the open ball with radius r around the point p in d-dimensional euclidean space?

#

i mean, generally you can give a topology to a metric space that way, but not every topology is generated by some metric

cursive flume
#

yes, I do understand this, but I'm watching Schuller's lectures on GR, but he says something fishy...

#

As part of the world-wide celebrations of the 100th anniversary of Einstein's theory of general relativity and the International Year of Light 2015, the Scientific Organizing Committee makes available the central 24 lectures by Frederic P Schuller.

Titled "A thorough introduc...

▶ Play video
#

min 22

#

he says we don't need norm

vocal wharf
#

well, if you forget the vectorspace structure on R^d and regard elements simply as d-tuples, you can still write this down and define open balls that way

cursive flume
#

so you don't need the definition of norm? just metric?

vocal wharf
#

i'm not quite sure what he's getting it

#

in general you do not need a metric to define a topology

#

but the standard topology on R^d comes from a metric

sleek thicket
#

Can someone explain why we care about lie brackets of vector fields to me? I have no idea what they represent

cursive flume
#

@vocal wharf i've found something. we don't need a metric to define a topology, but to define the standard topology we do need a metric, however a metric does not need the structure of vector space, just a metric space. a vector space which is normed is more special, because to every norm we can associate a metric, but metric can be defined independently, without the need of vector space structure, I think this is what Schuller means, do you think this is an ok explanation?

vocal wharf
#

seems good

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also notice that only euclidean space has a standard topology though

dire warren
#

They don’t need a norm because all norms on fin dimensional vector spaces are equivalent in that they induce the same topology. So they just work with this given topology @cursive flume

gentle ospreyBOT
versed pivot
#

@rich fiber
That condition implies $\frac{f(x)}{f(y)} + \frac{f(y)}{f(x)} \leq 2|x - y|$, is that right?
Since $(a-1)^2 \geq 0$ you have a simple inequailty $a + \frac{1}{a} \geq 2$ for $a > 0$
Taking $|x - y| < 1$ would contradict this

gentle ospreyBOT
versed pivot
#

I just swapped the roles of x and y and added the two inequalities

#

oh I see, I didn't read that part carefully enough

#

you can probably fix the argument if you replace x by a nearby rational but I would have to write it down to make sure

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or maybe not, if f isn't continuous

#

yes maybe this is too simple, I missed the part that y is supposed to be rational

chrome dew
#

not sure if this is helpful or not, but pick some z in ]0,infty[ and since Q and R\Q are both dense in R we can find a limit of terms of x -> z and y->z. Then you'll end up with 1 <= 0

dim meadow
#

Something I was thinking about is maybe you can let U_n be the set of points st f(x) is < 2^-n or > 2^n. I think you can show that those sets are open and dense

#

And then the intersection is clearly empty

chrome dew
#

I assumed continuity, ignore me

dim meadow
#

Lol bad assumption

#

We do though

#

Wait maybe this is bad

#

No I can show it

#

You can show that around a rational or irrational point there is a small open neighborhood not including that point

#

I'll write something up

dim meadow
#

Okay got it

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Given an irrational point x_0, suppose y is a rational point with |x_0-y| < (2^-n)f(x_0). Then f(y) >= f(x_0)/|x_0-y| > 2^n

#

Now given a rational point y_0, suppose x is an irrational point with |x-y_0| < 2^-n/f(y_0). Then f(x) <= f(y_0)|x-y_0| < 2^-n

#

This is a little off rn but I think you can make this work

#

There's still a bit of work to be done though

#

Yeah me too

#

Sure

dim meadow
#

I messed up a bit and made a correction

#

@rich fiber

#

Good

gentle ospreyBOT
dim meadow
#

Yeah juggling seems hard

#

What do you mean and?

gentle ospreyBOT
dim meadow
#

Welp

#

That's just empty

#

👀

#

Oh lol

#

Why is that open?

#

I wouldn't think it would be

#

But if it is that means the other one is closed

#

But I don't think it is

#

Oh wait

#

There's also the case of equality

#

But that doesn't seem so important

#

I don't agree with your close enough statement

#

Cause the problem is when you go closer, the radius of the ball shrinks

#

It's the juggling problem

#

I don't think that will do it

#

Okay here's something interesting

#

So you start off with the balls of radius 2^-n/f(y) about each irrational point

#

Then you intersect that with the balls of radius 2^-n f(x) about each rational point

#

This is an open dense set with the property that each point has f(x) < 2^-n or f(x) > 2^n

#

And then you're done I think

#

Yeah wtf

#

I think that does it

#

Fuck

#

Yeah this definitely does it

#

Wow that took me way too long

#

Cause it's an intersection of open sets

#

@chrome dew

#

We got it

#

What do you mean?

#

We are intersecting 2 open sets

#

👍

#

Baire is super applicable in weird ways

chrome dew
#

cool I'll check it out

dim meadow
#

What don't you get?

#

Say the two sets are U_n and U_n'

#

They do though

#

Okay look

#

U_n cap Q has the property

#

And U_n' cap R-Q has the property

#

So (U_n cap U_n') cap Q has the property

#

And (U_n cap U_n') cap R-Q has the property

#

(the property here meaning that all the elements either are < 2^-n or > 2^n)

#

Therefore A_n = U_n cap U_n' has the property

#

What's wrong with this?

#

@rich fiber

#

Lol

#

You're just inexperienced

#

Eventually you'll be able to deal with these kinds of arguments fairly easily

#

👍

dim meadow
#

👀

#

@gritty widget what do you mean?

#

Do the problem above

#

I'm writing some hw up right now

#

Please don't give me a problem

#

Yeah that was top tier

#

Yeah that shit is gross

#

The hint is baire category theorem

dire warren
#

@gritty widget try challenge problem 152

dim meadow
#

👀

#

@gritty widget R+ is R

#

Lol

#

Do you not know this?

#

(0, \infty) is homeomorphic to R

#

Locally compact hausdorff

dire warren
#

It’s a topological invariant

dim meadow
#

Locally compact, hausdorff

dire warren
#

The locally attaches to compact

#

It’s two properties

#

Hausdorff, and locally compact

#

Yeah

wooden scarab
#

I'm looking for a classification of universal covering spaces of closed 2 manifolds. It should be in some intro topology textbook I assume?

honest narwhal
#

So we can assume orientable

#

Because take the orientable double cover

dim meadow
#

For orientable we have S^2, R^2 and H^2

honest narwhal
#

Yup, this is called the uniformization theorem

wooden scarab
#

Where H^2 is a disk?

dim meadow
#

Hyperbolic plane (or disk)

honest narwhal
#

Actually is it true that any orientable surface is a Riemann surface?

wooden scarab
#

I think so *(for manifolds)

honest narwhal
#

Like if so then yeah what you said is an immediate corollary of uniformization

dim meadow
#

Classification of surfaces says yeah

honest narwhal
#

What's the classification of non-compact surfaces?

#

Or wait

dim meadow
honest narwhal
#

He said closed

#

Lol nvm

dim meadow
#

Yeah

honest narwhal
#

Yeah lol uniformization ez

dim meadow
#

For non compact there is a classification

honest narwhal
#

Well it's not ez but yeah

dim meadow
#

Yeah

#

You need ends and shit

wooden scarab
#

how about compact with boundary?

sleek thicket
#

Is the following variant of Whitney's approximation theorem true?

Let M, N be smooth manifolds and f : M -> N a homeomorphism. Then f is homotopic to a diffeomorphism

#

I'm guessing not

edgy crescent
#

I wouldnt call this a variant of whitney but it's true

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nevermind

#

it is not

#

this is troubling

#

because continuous maps are homotopic to smooth ones

#

and homotopies may be replaced by diffeotopies when they exist

#

but thats not enough

sleek thicket
#

What are diffeotopies?

edgy crescent
#

smooth homotopies

sleek thicket
#

Oh you're saying homotopies between smooth maps, not the homotopy you get from Whitney approximation

#

Can you find a counterexample?

edgy crescent
#

yes

sleek thicket
#

Oh lol I should've googled it first

gritty widget
#

anyone here familiar with basics of differential form

#

seitani ur familiar right?

edgy crescent
#

yeah my cousin was a differential form

#

rude

#

im much cuter

gritty widget
#

lol serious tho

#

i wanna ask a q

#

and idk if it belong to multivariable or this channel

edgy crescent
#

ask

gritty widget
#

so here

#

part c, is it closed?

edgy crescent
#

just compute dw

gritty widget
#

I got dx1^dx2+...+dx_{n-1}^dx_n

#

maybe i should find a counterexample

edgy crescent
#

well that's not zero right

#

?

gritty widget
#

yea, but just wondering if some operations could make it 0

edgy crescent
#

they're always linearly independent vectors in Alt^2 R^n

gritty widget
#

if not then ok ill try to find a counterexample

edgy crescent
#

find a basis for Alt^k R^n

#

it will help you be more comfortable with this stuff

gritty widget
#

we didn't use basis to define differential forms though...

#

we just define k-forms as summation of index

edgy crescent
#

yes, but they form a vector space

#

and you want to show that this sum is not zero

#

it can't be if the vectors are linearly independent

gritty widget
#

in this case what are the vectors?

edgy crescent
#

dx1^dx2, dx2^dx3, etc

gritty widget
#

ok, ill try, thanks

edgy crescent
#

as an example so you can sanity check, a basis for Alt^3 R^4 is given by
dx1^dx2^dx3,
dx1^dx2^dx4,
dx1^dx3^dx4,
dx2^dx3^dx4

gritty widget
#

wait im not even sure if d(x1 dx2) is dx1 dx2

#

im new to this stuff sorry

edgy crescent
#

it is but go make sure

#

do carmo's differential forms book is good

gritty widget
#

ah ok

#

im using calculus and analysis in euclidean space jerry shurman

edgy crescent
#

I see

#

you can google lecture notes for these things

gritty widget
#

i heard calculus on manifolds is good

edgy crescent
#

it's good to compare several sources

#

when you're confused

gritty widget
#

ok

#

oh wait...

#

d(x1 dx2) is not dx1 dx2

#

i gotta do product rule...

#

man

#

this sucks

edgy crescent
#

it is dx1 dx2

#

d isn't derivative

#

although it kinda behaves like it

gritty widget
#

according to book its supposed to be d(w^v) = dw ^ v + (-1)^k w ^ dv

#

where in my case x1 is a 0-form

edgy crescent
#

okay that's a valid way of computing it

#

but d(dw) = 0

#

always

gritty widget
#

yea that ik

edgy crescent
#

so when you have something of the form f dx_I

#

then you have an explicit formula

#

given by the partials of f

gritty widget
#

oh

#

that i think were learning later

#

lol

#

so we wont be able to use it this hw

edgy crescent
#

you can deduce it immediately from what you said

#

you have x1 dx2

gritty widget
#

but yea, i think then d( x1 ^ dx2) is not dx1 dx2 because of product rule for d operator

edgy crescent
#

so you go dx1^dx2 + x2^ddx2

#

= dx1^dx2

gritty widget
#

oh right

edgy crescent
#

so you can always just apply d to the scalar

gritty widget
#

ohhh

#

interesting

#

so its just a corollary of product rule for 1-forms i guess?

edgy crescent
#

ye

#

that product rule is for general forms

#

not 1-forms

gritty widget
#

w/bout k-forms

#

ah ok

edgy crescent
#

it's general for d(v^w)

gritty widget
#

where v is scalar

#

0-form

edgy crescent
#

v and w are any forms

gritty widget
#

d(v^w) = (dv)^w when v is any form??

edgy crescent
#

no

#

but if you have a form w = f dx

gritty widget
#

when v is 0 form that is true though right

edgy crescent
#

not really

#

w has to be a pure form

#

with constant scalar

#

something like dx1^dx3

#

not x^2 dx^1^dx^3

#

more generally w has to be closed

#

the precise useful statement is in the wiki page i linked

gritty widget
#

oh exterior product

#

man

#

we just call it different names

#

its just product of a k-form and an l-form

#

yea i got that bit

#

im thinking though, maybe d(f ^ dx1 ^ ... ^ dxk) = df (dx1 ^ dx2 ^ ... dx^n) is a special case if you keep on applying product rule, but i dont know

#

because at least we seen that d(f^dx) = df ^ dx

edgy crescent
#

yes it is

#

that's the case in the image above

#

im going to play videogames if you need me yell bloody mary 3 times to your mom

gritty widget
#

ok lol

#

go have fun

#

so i got an answer

#

and if u can approve thats good

#

so since w= dx1dx2+...+dxn-1dxn

#

i let y(t) = (t, t, ..., t): [0,1]->R^n

#

so that integral of w over y is n-1 which is not 0

#

for n>1

edgy crescent
#

your loop should be closed

#

closed forms integrate to 0 under (contractible) closed loops

gritty widget
#

y should always be closed?

#

to be able to integrate

edgy crescent
#

you can always integrate but that doesnt give you information

#

the result is that closed forms integrate to 0 over contractible closed loops

gritty widget
#

but here the definition of closed is dw = 0

edgy crescent
#

oh then why are you integrating?

#

oh you're integrating dw aren't you?

#

not w

#

I see that confused me

#

yeah a way to show dw is not zero is to integrate it

#

but that's a bit overkill

gritty widget
#

yea

edgy crescent
#

linear algebra shows it's nonzero immediately

gritty widget
#

sorry didnt clarify

#

i guess about lin alg ill ask prof tomorrow

#

and pt d), i just say since w not closed, then w not exact

edgy crescent
#

yea

gritty widget
#

ok thanks

chrome schooner
#

yo

#

help

#

lol

#

hello ;=;

#

i just need help from smart math guy

gritty widget
#

hey i think i got what you mean by vector space now

#

so for a k-form, let all the possible indices dx_{I} be the coordinates right

#

and then the dx1 ^ dx2 + ... + dx_{n-1} ^ dx_{n} is something like a bunch of 1's and 0's on the nxn matrix

#

wild guess actually

#

or are they like vectors (1,1,0,...,0), (0,1,1,0,...,0),...,(0,...,0,1,1) that are linearly independent?

#

i think thats what i meant

#

@edgy crescent if u can confirm true/not true

sleek thicket
#

I'm taking my first course on smooth manifolds and we've just gotten to flows of vector fields. My book has an appendix with proofs of existence/uniqueness of solutions to linear ODEs, and those made sense, but the theorem about the solution smoothly depending on initial conditions seems really hard. Is it important for me to understand it right now?

edgy crescent
#

@gritty widget not exactly true

#

your formula would imply that dx1^dx2, dx1^dx3 and dx2^dx3 are linearly dependent

#

the vector space of alternating k-forms in R^n has dimension n choose k

#

where a basis is given by the dxJ where J is an increasing subset of [n]

gritty widget
#

oh

#

so the dx objects are the basis of the vector space which is the V^k(A) all k-forms

#

?

#

V as in the upside down V

#

but are they known as the standard basis just like the standard basis for a linear transformation?@edgy crescent

edgy crescent
#

yes

gritty widget
#

Ok thanks

pseudo crane
#

Smells like differential geometry in here

midnight jewel
#

fields whose name ends in y are the best since you can use the descender of the y to underline the title

prime prism
#

Can I just make sure: the intersection of two simplicial complexes need not be a simplex

#

In particular it can be a disjoint union of simplicies

#

(e.g. Two tori joined in two spots)

gritty widget
#

Are two circles with the same orientation concatenated at a point homotopic to a single circle?

#

I'm thinking no but I don't know how to prove it

#

like the loop concatenation $fg$ where $f(t)=(\cos(2\pi t), \sin(2 \pi t))$ and $g(t)=(2-\cos(2\pi t), -\sin(2 \pi t))$

gentle ospreyBOT
gritty widget
#

Assume a homotopy (by defn. continuous) exists from $fg$ to $f$, so if $C$ is an open (closed) set in $\mathbb{R}^2$, the inverse image $f^{-1}(C)$ in $[0,1] \times [0,1]$ is open (closed)... something something contradiction?

gentle ospreyBOT
midnight jewel
#

Are two circles with the same orientation concatenated at a point homotopic to a single circle?
are we talking in an ambient space? like, in ℝ² or sth?

gritty widget
#

Yeah

midnight jewel
#

if you have no requirement for the homotopy to be injective (for fixed t), then you can just contract everything to a point and then expand into a circle

#

seing as ℝ² is contractible

gritty widget
#

True, I was trying to understand/learn about fundamental groups of R^3-{some knot} so what about in that case

midnight jewel
#

or just contract one of the loops into the basepoint

#

so you can pull things apart if you don’t require the basepoint to remain fixed

#

ah wait no it even works generally

#

you can turn it into a big loop

gritty widget
#

I see what you're saying yeah

midnight jewel
#

by just moving the loop a bit away from the basepoint when it first returns to it

gritty widget
#

cause that loop you're shrinking can contract to a point

#

and u just have the big boi left

midnight jewel
#

in your case with the knot it would depend whether the loop goes around the knot or not

gritty widget
#

ye ye

#

I have a much clearer image of this now ty tho

#

Didn't understand that before

gritty widget
#

sorry I didn't connect the loops at an initial basepoint but in this case they're homotopic to that setup anyway
with the stuff on the bottom, pic 1 to 2 is concatenation of the loops, 2 to 3 is performing what I'm pretty sure is a valid homotopy right? (That's my question ;-; )

#

Space is supposed to be R^3\ {trefoil}

fading vale
#

So I'm trying to understand a proof in bredon that, given a hausdorff space X the following conditions are equivalent:
-X is locally compact
-X is a locally closed subspace of a compact hausdorff space
-X is a locally closed subspace of a locally compact hausdorff space

#

for showing (1) implies (2) he says that since X is locally compact its an open subspace of its one point compactification which ofc is a compact hausdorff space which makes sense to me

#

but i dont get why this implies X is locally closed

#

does local compactness imply locally closed?

honest narwhal
#

@fading vale Open subsets are locally closed

#

Open subset of a closed subset

#

The whole space is closed

#

boom

fading vale
#

owait

#

._.

#

i was being dum

honest narwhal
#

lmfoa

fading vale
#

ok tbf he defined locally closed literally the line above this and then went abt proving this

#

oh

#

@honest narwhal yea he didnt define it as being open in its closure

honest narwhal
#

What was his def again?

fading vale
#

every a in A, there exists a neighborhood U with a in U, A cup U is closed in U

#

this still works tho i was being dumb and not thinking

dire warren
#

I’m having trouble understanding the characteristic embedding described in Milnor’s lectures on the h cobordism theorem. Why are hyperbolic sine and cosine chosen?

#

<@&681259184582688842>

gritty widget
#

I honestly have no clue if this is relevant but maybe https://en.wikipedia.org/wiki/Integral_curve#Generalization_to_differentiable_manifolds has some insight as to the motivation of that last sentence in the section you're talking about? Again no clue lol

In mathematics, an integral curve is a parametric curve that represents a specific solution to an ordinary differential equation or system of equations. If the differential equation is represented as a vector field or slope field, then the corresponding integral curves are tan...

#

from hatcher: why is $ir \cong \mathbb{1}$? Is Hatcher using $a \cong b$ as meaning "$b$ is a restriction of $a$"?

#

also apparently I don't know how to write those symbols in latex oof off to google

#

It is clear to me that ri is the identity though, just include A, A=im(r) and r=r^2, done.

#

If an element of X\A goes through ir, it will end up in A, so clearly it's not equal to the identity, so I'm guessing that Hatcher means something about restrictions with that symbol right

#

and no it's not included in the "standard notations" section even 😂

coral pivot
#

hatcher uses $\cong$ to mean homotopy

gentle ospreyBOT
coral pivot
#

i.e maps ir and the identity are homotopic

#

its the first paragraph in that page

gritty widget
#

yeah just found it lmao

#

thanks 😂 it's a fun time

coral pivot
#

lol np

gritty widget
#

ree

gentle ospreyBOT
gritty widget
marsh forge
#

huh

gritty widget
#

I can't figure out how to get mathbb{1} to work here

chrome dew
#

there is no mathbb 1

#

$\mathds{1}$

gentle ospreyBOT
chrome dew
#

I guess this package isn't default

#

$\usepackage{ dsfont }
\mathds{1}$

gentle ospreyBOT
chrome dew
#

oh well I tried

gritty widget
#

oof

#

how 2 prove homotopy type equivalence is transitive?
Suppose spaces $X \cong Y$ and $Y \cong Z$. So homotopy equivalences $f_1$ and $g_1$ exist between $X$ and $Y$, and $f_2$ and $g_2$ between $Y$ and $Z$ likewise. Again by definition these equivalences have homotopies $F$, $G_1$, $G_2$, and $H$ such that $F$ is between $g_1f_1$ and $\text{id}_X$, $G_1$ is between $f_1g_1$ and $\text{id}_Y$, $G_2$ is between $g_2f_2$ and $\text{id}_Y$, and $H$ is between $f_2g_2$ and $\text{id}_Z$. Is this the right way to set it up? Cause it's a lot ;-;

#

My immediate thought is to try to find homotopies between $f_2f_1g_1g_2$ and $\text{id}_Z$, and $g_1g_2f_2f_1$ and $\text{id}_X$ but idk how

gentle ospreyBOT
gritty widget
#

if anyone has a hint toss it up so I could keep trying

marsh forge
#

Use the original homotopies to build a new one

#

for the composites

#

its not so bad

gritty widget
#

I was thinking I might need to find a homotopy between $g_1g_2f_2f_1$ and $g_1f_1$ since then transitivity of homotopy gives that the former is homotopic to $\text{id}_X$ as desired, but I have no clue how to construct one from the other ones

gentle ospreyBOT
gritty widget
#

If it's taking me this long to work through a trivial part of a paragraph in chapter 0 of Hatcher like this should I just give up on pursuing this at all

#

Will I just never be good enough to do things this quickly

coral pivot
#

dw im starting hatchers too

#

it takes a while, its intro to an entirely new field

gritty widget
#

Good to know I'm not alone lol

#

Do I need to show that compositions of homotopic functions are homotopic? as in going down the route of trying to show $g_2f_2f_1 \cong f_1$, and then composing both sides with $g_1$?

gentle ospreyBOT
gritty widget
#

In turn showing that composition in the other direction of homotopic functions yields two also homotopic functions would prove this completely right, cause we know $g_2f_2 \cong \text{id}_Y$, compose to get $g_2f_2f_1 \cong \text{id}_Yf_1=f_1$, again the other direction $g_1g_2f_2f_1 \cong g_1f_1 \cong \text{id}_X$, and done by those two lemmas?

gentle ospreyBOT
gritty widget
#

Proving this would also show that you can multiply equations defining homotopy equivalences together too
like $a \cong b$ and $c \cong d$ implies $ac \cong bd$, cause $ac \cong bc$ and $bc \cong bd$ by the lemma

gentle ospreyBOT
gritty widget
#

So it would be nice for it to be true, is there another way to do this proof of homotopy type equivalence being transitive without proving this too? cause Hatcher says proving homotopy type is an equivalence relation is "easy" soooo

rugged raptor
#

Isn't a torus the same thing as a knitted sweater?

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Since you can entwine it around itself to make it into an arbitrarily long string, and the just knit with that string.

cursive flume
#

Schuller in his lectures makes the definiton of "manifold philosophy", which basically means: we do physics on manifolds, represent it in charts, then associate the chart properties with the real world properties, continuity works- for example, but then he goes into "ill defined properties", which can be chart dependent, if we do the physics on the whole manifold. can someone give me such an example?- we want physics to be chart independent

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I was thinking of differentiability,if we do it on the whole manifold, without making restrictions, but we can solve it with restrctions (work on a more rigorous structure, namely a differentiable manifold), does anyone know such a "property", which can "not be fixed" by "adding more structure"?

sweet wing
#

Assuming some conditions holds, this is true
is literally how most theorems are

floral gust
#

I was thinking of differentiability,if we do it on the whole manifold, without making restrictions, but we can solve it with restrctions (work on a more rigorous structure, namely a differentiable manifold), does anyone know such a "property", which can "not be fixed" by "adding more structure"?
@cursive flume I don’t know think so because you can literally introduce the property as a fix. As in “we now consider the manifolds that will satisfy the given the property.” And the 0 dim manifold would most likely satisfy this due to some sort of vacuity. Interesting is then is to ask what properties ca;you introduce and still not run out of the base cases.

cursive flume
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@floral gust yes, this was my question, what property can be defined such

floral gust
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Take any self-contradicting property

wheat brook
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@cursive flume Consider the sphere. We cannot map it to 1 chart. If we do physics on the whole sphere, we will always run into pole somewhere. The fix is to switch locally to a different chart.

cursive nebula
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hey guus, can i ask a topology question?

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ahh i did!!

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NICE

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thabk you!!

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i need it for another longer proof

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i will still check them

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i dont know if it's the SMALLEST topology that you can generate with those sets

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wait. it is

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yeah,

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/rotate

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the exercise im trying to solve is on the base chapter

gentle ospreyBOT
cursive nebula
#

i need this result (tau3 is a topology) to prove that thing

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oh thanj you!

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see i tried using the axioms, intuitively i can see it's reasonable for tau 3 to be a topology

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but idk how to write it formally

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,rotate

gentle ospreyBOT
cursive nebula
#

this is the exercise i have to do

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i have to prove that B is a base for a topology that is more fine than the topology is

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so this is what i thought

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,rotate

gentle ospreyBOT
cursive nebula
#

if tau3 is a topology, i can easily prove that B is a base for tau3

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so thats why i asked if tau3 was a topology

gritty widget
#

Hello there, I would ask you for some recommendations about some nice Topological subject to talk about for a group of undergrad students, please?

midnight jewel
#

what level are we talking? like is the target audience people who have zero experience with topology yet or ones who have already done some (or maybe even a lot of) basic topology stuff?

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“undergrad” could mean anything from no experience to having taken two years of topology classes

cursive nebula
#

hey guys,

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i'm trying to solve problem 25, but i don't know how to go about points ii) and iii)

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(what does relative topology mean?)

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,rotate

gentle ospreyBOT
cursive nebula
#

this is the idea i had for points ii) and iii) but i don't know if i'm on the righr track (it would help if i had That Definition)

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i can hit the second line in Each Point with open sets
(and they would generate the discrete topology)
but i cant do it with the first

is that it?

midnight jewel
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relative topology is also called the subspace topology

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if you have $X \subset Y$ and you have a topology $\mathcal{T}$ on $Y$ then you can define a topology on $X$ by simply saying the open sets in $X$ are all sets of the form $X \cap O$ for $O \in \mathcal{T}$

gentle ospreyBOT
midnight jewel
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ie you intersect the open sets of Y with X to get open sets in X

cursive nebula
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ahh thank you so much!

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okay, so
those lines are subspaces of R^2

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i can easily prove ii) bc i know that topology includes every singleton so it's discrete

topaz shuttle
#

Hi there does anyone know anything about the topology of complex numbers?

midnight jewel
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I mean it’s just the standard topology on ℝ²
if you have specific questions you should JustAsk

twin aurora
#

I'm trying to work out a proof of the following theorem from basic algebraic topology, that the deck transformation group of a covering space is isomorphic to the fundamental group of the base space mod the fundamental group of the covering space. does anyone have any hints to drop/resources that i could check out to be pointed in the right direction?

bitter yoke
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<@&681259184582688842>

marsh forge
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Each subgroup correspondens to a cover

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Use thiis

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Im@so drink bj

dawn geyser
#

hi everyone! i'm working with double factorials (as in 9!! = 9 x 7 x 5 x 3 x 1, not (9!)!)) and trying to use them for a proof of n-spheres but i'm really struggling with a lot of the notation

delicate spire
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hey whatchu need help with?

dawn geyser
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im working with this right now

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<@&681259184582688842>

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im basically tryna get to here by combining the recurrences but idk know how to

delicate spire
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Sn and Vn are surface area/volume of unit sphere?

dawn geyser
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i think? i don't actually know what the S is meant to represent

delicate spire
#

ok yea like for a 3d sphere it has S2 surface area V3 volume

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I found the proof I think you want on wikipedia O_o

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looks like you need 1 more recurrence formula and it's easy to get the double factorial bits

dawn geyser
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i got it from wikipedia yeah

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im just trying to understand the steps and its not really explaining it that well to me

delicate spire
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ok, I can't really follow the integration bits, but this part makes sense to me

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what part is tripping you up?

dawn geyser
#

this is my first time doing anything involving n-spheres, so we haven't learnt a lot of the theory for it.

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so basically all of it

ivory dragon
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if $V_{n+1} = \frac{S_n}{n+1}$, then $V_{n+2} = \frac{S_{n+1}}{n+2} = \frac{2\pi V_n}{n+2}$

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surely you follow at least this much?

gentle ospreyBOT
ivory dragon
#

so one can use this to show inductively the two identities below

dawn geyser
#

yeah yeah i follow that

ivory dragon
#

i'll show the first one, the next case follows. let $k = 0$, then $V_{2k} = V_{0} = 1$ by definition, so clearly $V_{0} = \frac{\pi^0}{0!} = \frac{1}{1}$.

gentle ospreyBOT
ivory dragon
#

now we can assume that this holds for some $k$ and wish to show it for $k+1$

gentle ospreyBOT
ivory dragon
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$V_{2(k+1)} = V_{2k+2} = 2\pi \frac{V_{2k}}{2k+2}$

gentle ospreyBOT
ivory dragon
#

due to the identity shown earlier

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and we know that $V_{2k} = \frac{\pi^k}{k!}$ by the inductive hypoth

gentle ospreyBOT
ivory dragon
#

conclusion follows.

dawn geyser
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ok!! thanks so much for that

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i'm just gonna reread that all real quick

ivory dragon
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ie

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$V_{2k+2} = 2\pi \frac{V_{2k}}{2k+2} = 2\pi \frac{\pi^k / k!}{2(k+1)} = \pi \frac{\pi^k}{k!(k+1)} = \frac{\pi^{k+1}}{(k+1)!}$

gentle ospreyBOT
ivory dragon
#

in case you couldnt finish the algebra yourself

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this completes the induction

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anyway a similar process holds for V_(2k+1)

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this is very standard "first proofs class" induction, no real tricks

dawn geyser
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i'm in 12th grade, doing like four unit maths. it's an extension question and we've barely covered any thing involving n-dimensions, so i'm not really able to do these sorts of proofs yet

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thanks for helping so much though

ivory dragon
#

the gist behind induction is that

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we prove something for a "base case"

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in this case, our base case was when k = 0

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and then we show that "k holds" implies "k+1 holds"

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by a "domino effect", this shows it for all integers greater than the base case

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since we've proven that k = 0 is true

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and then k = 0 is true implies k = 1 is true

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and then k = 1 is true implies k = 2 is true

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and so on

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this is called the "inductive step"

dawn geyser
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okay yep, i get that

ivory dragon
#

and the fact that we're allowed to assume is the "inductive hypothesis"

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if you show both the base case and inductive step, you have a complete proof by induction

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thats the main "mechanics" of the above proof, everything else is just algebra

dawn geyser
#

so how could i use this an example of an application of double factorials? can i use it to find the n-dimension volume?

ivory dragon
#

well, if you want to get it into double factorial form, you have to show $\frac{\pi^k}{k!} = \frac{(2\pi)^k}{(2k)!!}$

gentle ospreyBOT
ivory dragon
#

i omitted that from my proof

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this isnt particularly hard to show, however

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in any case, yes, this is how you calculate the n-volume of an n-sphere.

dawn geyser
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where n=2k?

ivory dragon
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yes

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i.e. even n

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for odd n you use the below formula

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same gist either way

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er well i should clarify

dawn geyser
#

yeah thats right, thank you for that. i think i've got it now.

ivory dragon
#

this is the volume of an n-sphere

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of radius 1

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for radius x you have to multiply by x^n

dawn geyser
#

so R is radius 1?

ivory dragon
#

(also technically "volume of the n-ball" is a more mathematically correct term but who cares)

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the formulas you screenshotted assumed a unit n-sphere

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i.e. radius 1 (R = 1)

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if you change the radius, just multiply by R^n

dawn geyser
#

ok can you give me a practice question of volume of the n-ball with a value for k?

ivory dragon
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i mean, you can make random numbers and just plug them in essentially

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calculate the volume of the 5-dimensional ball of radius 7

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or of the 12-dimensional ball of radius 2.1

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use this to rederive the formulas for the area of a circle and the volume of a sphere

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etc

dawn geyser
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units^5 right?

ivory dragon
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yes

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(mathematicians generally don't bother to write units, so if you're looking into this and see units being disregarded, dont worry - it's just notation abuse)

dawn geyser
#

this kind of stuff is crazy, idk how you guys do this for a living honestly

ivory dragon
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i mean, these methods are fairly routine

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ignore the conceptual "woah n-dimensional sphere thats so craaazy" and just see where the definitions take you

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alternatively, stop viewing "dimension" as something that's necessarily tied to spatial dimensions

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we just use "dimension" to mean "an axis on which some data can vary"

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if theres 3 dimensions or less, its usually convenient to represent that data as a location/position

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that's the motivation for the cartesian plane, for example

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but really, computers are regularly doing 1000-dimensional statistics whenever they do machine learning stuff

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its nothing crazy, just maybe a bit hard to visualize

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they're, of course, not asking "geometric" questions about this 1000-dimensional statistics (theyre not gonna ask what the "volume" is), but the idea of an n-sphere is just generalizing a geometric connection from 2/3 dimensions to higher dimensions

dawn geyser
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yeah i think its the visualisation that i struggle with but your explanation cleared up with the axis yeah

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just functions with another axis

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its hard to think of but that makes it easier

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oh by the way, what does it mean by this?

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The dimension of n-sphere is n, and must not be confused with the dimension (n + 1) of the Euclidean space in which it is naturally embedded. An n-sphere is the surface or boundary of an (n + 1)-dimensional ball.

ivory dragon
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ok so uh

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this is a notational thing

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and the reason we choose this notation is due to some fairly sophisticated topology

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well, not particularly sophisticated but

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basically a "2-sphere" is a 3d sphere

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a "3-sphere" is a 4d sphere

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etc

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the reason for this is that a "sphere" is actually the boundary of a ball

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specifically, the 2-sphere is the boundary of the 3-ball

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and so on

dawn geyser
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ok yeah thought so

ivory dragon
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since its just the boundary, it has a lower dimension

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since for example