#serious-discussion

1 messages · Page 305 of 1

twin flicker
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i cheated on my diet slightly for the past 2 days so i have to lock back in

gusty bough
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lock in

sturdy obsidian
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hI

burnt ledge
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zased what kind

polar temple
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do u have a heatwave as well

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we have a 32° heatwave in England ecstasy

vital niche
vital niche
vital niche
burnt ledge
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most of my degree was physics

gusty bough
gusty bough
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basically newtonian mechanics but better

vital niche
gusty bough
# vital niche thats sickk thankyou

It requires to know a tiny bit of Newtonian physics and ordinary differential equations (which once you learn derivatives or integrals at school, I encourage you to do) and you always have the same equation give a better coordinate system

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So if you have a pendulum, it would be better to analyse the angle instead of (x, y) coordinate; you would go from 2 variables to a single 1! Then apply your formula and boom you got the equation of the movement as an ODE

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That’s the ultimate basics of Lagrangian mechanics

polar temple
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its good to see year 10s studying

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i didnt study until y11 started

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summer holidays too

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do u do aqa triple?

barren cairn
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Hai!

zealous garden
polar temple
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now i dont know if i was right or if "zased" means "not very new"

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probbaly tje first

gusty bough
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Oh I thought zased was based with a typo

zealous garden
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I'm saying zased is a form of based but it's not new

torpid bay
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,w zased

jade belfry
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hi

sharp mulch
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This doxes your last name

jade belfry
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how?

ancient garden
outer crag
#

unc copying my pfp

ancient garden
outer crag
latent edge
#

,av 974792201143996416

fathom swallowBOT
#
yeetsaltaccount's Avatar

Click here to view the image.

latent edge
#

Copying your profile as we speak

outer crag
#

💔

steel vessel
#

what happened to ur name

dusky locust
#

YOU'RE MULTIPLYING

jade owl
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hi fiscussy 2

dusky locust
soft wadi
#

hey guyd

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guys

rain vale
#

Huy

rain osprey
#

Hi

eternal crow
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YEAST

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huy ka rin

uncut crest
#

I have to download the new version of OneNote. Because the old version declares its end of service

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I do not like changes

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The old one is still working. I cannot find any reason to adapt a new one

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Fk Microsoft

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@microsoft

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Now I have to adapt the new version

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I'm so fking sad

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fk

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why

untold cedar
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now I don't feel bad i forgot how to do subtraction opencry opencry opencry opencry opencry opencry opencry

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my parents are laughing at me
they say you are a freaking math student and u can't count KEK

no I can't bleakcat

median knot
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ufff 😭

mighty knoll
polar temple
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😭 sorry

zealous garden
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I am weird but nothing about that interaction supports this claim

polar temple
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cuz why would you willingly say "zased" instead of "based"

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its the first time ive seen it

zealous garden
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I didn't say it homie

polar temple
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even "based" is strange according to my hypocrisy

zealous garden
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I told you what it means

polar temple
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oh

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mb

zealous garden
#

It was asked and I answered

polar temple
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you're good bro

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you probably are still weird

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youre in a maths server

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but thats the only thing making u weird afaik

zealous garden
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<@&268886789983436800>

blazing lintel
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30+37=67

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67

vivid quest
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i've seen people react so i'm curious now

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nvm

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it's explained in the first 3 second

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i be like that

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acting

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then thinking

vernal token
burnt ledge
gray dove
#

hello guys

zealous garden
gray dove
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damn this channel pretty dead

willow crystal
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rather than being dead

burnt ledge
vast wraith
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it means people have time to think

vivid quest
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I don't use that extra time

edgy tiger
#

THIS SHIT IS FIYA !!!!!

jade belfry
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The sky is not blue. It is gray—painted over to hide the cracks. The sun is not yellow. It is a projection, hung like a stage light over an empty stage. And the stars? Only the lies we plant so no one notices the dark. There are still dinosaurs—but only one remains. We killed the rest and called it a “necessity.” Someone decided they should die by asteroid, hiding the real truth. We say volcanoes finished them, only because we can’t bear the truth staring back at us. And the stars? They’re just projections—images we plant to pretend everything is fine. But every time we say it’s fine, we strip away another piece of the world.

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“The saddest thing isn’t the world is burning.
It’s that you have a cup of water, and you don’t dump it.”

tough stratus
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yeah okay

fiery stump
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you need way more water than a cup, even for a campfire

jade belfry
#

you don't understand this is about apathy.

outer crag
peak zephyr
#

Why be apathetic when you can lose your job instead

silent mauve
mighty knoll
solid yarrow
faint light
kindred otter
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Have anyone done math projects how did you start?

gritty heath
kindred otter
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I mostly love calculus

gritty heath
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can you code

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im thinking if you can code, you can try writing an automatic differentiator
you can read up on this
https://en.wikipedia.org/wiki/Dual_number
and write some program
you'd probably want a DualNumbers class, a Function class with various hard coded functions, and the hope is you could try to implement a program that reads your input and gives you a closed form expression of your derivative, or a numerically evaluated value

In algebra, the dual numbers are a hypercomplex number system first introduced in the 19th century. They are expressions of the form a + bε, where a and b are real numbers, and ε is a symbol taken to satisfy

      ε
      
        2
      
    
    =
    0
  

{\displaystyle \va...
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idk how feasible is it tho

zealous garden
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How terrible

terse comet
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hope this helps

zealous garden
compact surge
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:3c

terse comet
#

I hate how discord embeds these

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Bit of a meme high card run, made it to ante 11

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porple stake

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@faint light i think plays this right

mint canopy
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Those red holo stones do things to my brain chemistry

fresh comet
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@soft jungle welcome to the mathcord! nachoWaves

faint light
soft jungle
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@fresh comet tyy

terse comet
#

though I did get it to like lvl 20

naive tundra
#

did anyone here study in cpge or go to x/ens (pin me plz if you see this message)

junior veldt
serene heron
#

I had a nice jokerless run a while ago

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flush builds catthumbsup

left summit
#

Hey I’m new at uni
Can someone explain what CCS, MS, and SESA are ?

raven tiger
#

Hello, I’m new to the server I came here to ask a question and discuss about it and I have no idea where to post it so I joined this server to ask it and maybe have some answers or advices of where to ask it. The question is about a new "problem" to study that I am wondering wether or not I should try to study it or not, sorry it’s difficult to explain myself but basically I studied a problem during a research internship (which is more in theorical cs) and I found a generalization of this problem that I would like to study more mathematically and I don’t really know in which category it belongs to but the question would be about is it worth spending time studying the problem but my current question is where can I ask this question and add more detail and context ???

agile fiber
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ask in one of the appropriate subject channels (e.g. if you think it's still theoretical cs then #theoretical-cs )

raven tiger
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Thank you for your answer still

agile fiber
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just make your best guess at which subject fits best

mighty knoll
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Can you describe your project?

raven tiger
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I’m anxious now that the question is weird or incomprehensible or it does not belong here but it’s ok

mighty knoll
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You’ll be fine, it sounds like pretty cool research

steep nimbus
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Hello

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Is anyone else here?

#

#

Alr

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Im leaving

fresh comet
tired carbon
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Hey guys, I finished calc bc last year, and for my senior year, I'm starting Calc 3/Multivariable - any tips? Did you guys enjoy this class?

latent edge
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I did not enjoy Calc 3

spark scroll
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i didnt enjoy it either 🥀

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mostly how it was taught tho

dry steppe
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hey guys does anyone know if matricies are in calc ab?

torpid bay
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it wasn't in mine

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ab should just be like limits and derivatives, that's all (maybe some trig ig)

fresh comet
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@dry steppe welcome to the mathcord Loves

dry steppe
torpid bay
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the class I took was trig/calc, where precalc was the other option, so I can't really remember what it was sepcifcially. but in general, trig is pretty important for calc

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i would have to look over the direct content again

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gimme a sec

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trig, series, and limit+continuity

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unit 4: rational functions are something that I see barely, and probability and combinatorics you'll end up taking an entire class about later to fully flesh out. While unit3: conic sections are the simple 2D equations that you'll need to be able to visualize, usually just visuallizing them is enough to get you on the right path if you ever see a problem with the equations from those. tho generally I just end up seeing a circle 95% of the time, and 4% is hyperbolas

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vectors and matrices are great, and will be important later on, like in calc 3 or linear algebra, but It's fine to get a handle on them here

zealous garden
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matrices are great
Yuck

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Every theorem gets better when you remove the matrices sorry not sorry

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"Given a symmetric matrix B and Invertible S, and matrix D=S^*BS
D has the same number of positive, negative, and null eigenvalues as B."
vs
"Two metric vectorspaces V,W are isometric iff V_+≈W_+, V_-≈W_-, and V_0≈W_0"

torpid bay
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ah lel

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$V \cong W \iff V_+ \approx W_+ \wedge V_- \approx W_- \wedge V_0 \approx V_0$?

fathom swallowBOT
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Yeatte

zealous garden
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Yes

torpid bay
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I'm not sure whats meant by approx?

zealous garden
#

Isometric, linearly isomorphic, same thing really

torpid bay
#

ah

fiery stump
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omg i've proven two things isometric b4 in differential geometry

zealous garden
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It's easy enough to prove the general equivalence on (in)definite metric vectorspaces, V+ etc. So all that remains is showing that every metric vectorspace admits a, not necessarily unique, decomposition into these (in)definite spaces

zealous garden
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That is for manifolds yes?

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Pseudoriemannian manifolds?

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This is for the local case of that I guess?

fiery stump
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riemannian manifolds under particular charts

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and induced riemannian metrics

torpid bay
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my intro to diff geo was a lot of fun

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the formulae are pretty nice looking too

fiery stump
#

i barely understood any of mine but i had fun too

zealous garden
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Two metric vectorspaces $(V,B)$,$(W,D)$ are isometric iff there exists a linear map $S:V\to W$ s.t. $S$ is an isomorphism, and $$B(u,v)=D(Su,Sv)$$

fathom swallowBOT
#

wraithlord_kojima

zealous garden
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Very simple

zealous garden
torpid bay
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B,D being metrics?

zealous garden
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You mean more than just a smooth structure and metric tensor?

zealous garden
fiery stump
#

man i dont remember

torpid bay
#

pretty simple requirenents

zealous garden
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We make no ask of nondegeneracy for many definitions

torpid bay
#

cones ❤️

zealous garden
warm gull
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man i really really need a good geometry book

zealous garden
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So it is pretty clear how our desired statement of isometries, the classification of metric vectorspaces, is equivalent to the typical Sylvester law of inertia

torpid bay
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,w sylvester law of inertia

zealous garden
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HAHAHAHA

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Garbage wolfram as always

torpid bay
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huh..... certainly reminds me of the jacobian and metric tensor

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this is a nother form of it, right?

zealous garden
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What?

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,w jacobian

fathom swallowBOT
zealous garden
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HAHAHA

torpid bay
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jacobian is the change of basis matrix

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with partial derivatives

zealous garden
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Jacobian is too many things

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You mean the differential?

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The map between tangent spaces?

torpid bay
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i think yeah ( also a thing that refers to too many things)

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$J = \frac{\partial x_i}{\partial x_j}$ or smthn

fathom swallowBOT
#

Yeatte

torpid bay
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i cant quite remember the indices but yeah osmeting like this

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maybe they were both on top?

zealous garden
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The partial derivative in the ith coordinate direction, grab the jth component with respect to the basis. No?

torpid bay
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did you see my diff geo notes that i posted a week ago?

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yeah they're both up

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$J = \frac{\partial x^i}{\partial y^j}$

fathom swallowBOT
#

Yeatte

warm gull
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it’s fairly simple

fiery stump
#

im not clicking links to domains i dont know

swift bronze
willow crystal
quasi jettyBOT
lost quartz
#

@adham33

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@wise siren

ocean harbor
#

u can tell its an image bc of png? not really a dangerous link but rather its embed fail kekw

dreamy ore
#

we have notation like $a_n = 2\cdot 0.5^n$ and then $a_5 = 1/16$, why cant we have $f_x = x^2 + 3$ and then $f_{2.5} = 37/4$ and $f'_{2.5} = 5$

fathom swallowBOT
torpid bay
warm gull
neat lintel
#

Suppose that $TT^$ is invertible, show that $P=T^(TT^*)^{-1}T$ is a projection onto $(\ker(T))^\perp$

fathom swallowBOT
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Nicole

neat lintel
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comp of kerT = imT^*

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P^2=P

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idk

latent edge
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Is it safe to assume T is a bounded linear operator between Hilbert spaces?

neat lintel
scarlet mango
#

hi @mint canopy . I'm very very sorry to tag you but I couldn't help noticing a small error in your bio. The spoiler part would grammatically be right if it were written in one of the three ways: 1. I asked: Why are you here?
2. I asked why you are here
3. I asked "why are you here?"
If you don't blacklist me, thank youcatglasses

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Also, sorry for stalkingKEK

unborn meteor
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LOL

scarlet mango
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I'm a language nerd

scarlet mango
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welp

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what is the intuition behind it?

burnt ledge
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its like generalising the derivative

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or partial derivatives if yoire familiar with them

burnt ledge
torpid bay
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oh i took shower am bajj

torpid bay
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i'ts required for quite a lot of things

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or rather the concept of a derivative

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u know derivatives?

scarlet mango
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yep

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can you show me the simplest application this thing may have?

torpid bay
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it's probably to use it on vectors then yeah

scarlet mango
torpid bay
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it's a little different because when you have 1 dimension input, and 1 dimension output, all you need is $\frac{dy}{dx}$

fathom swallowBOT
#

Yeatte

gritty heath
torpid bay
#

but when you have 2 inputs, then representing how much the output changes requires you to ask how much each input changes.

gritty heath
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That's it

burnt ledge
#

partial derivatives go a little bit further and they tell you how a function of several variables change when you change each of its variables

gritty heath
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There are reasons why the array is shaped in some way but its fairly geometric and I dont geometry

scarlet mango
burnt ledge
#

jacobian tells you how each of the outputs of a function with several outputs and several inputs changes when you change any of its inputs

gritty heath
haughty lion
burnt ledge
torpid bay
#

$\lbracket \frac{\partial z}{\partial x} \frac{\partial z}{\partial y} \rbracket= \frac{\partial z}{\partial u^i} = J$ for an example of 2 inputs, x,y and 1 output z

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wait hold up

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does it need to be same n for R^n?

scarlet mango
scarlet mango
torpid bay
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general derivatives

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you can put in specific x,y values after

scarlet mango
torpid bay
#

to find a specific number for

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it's a matrix yeah, it can be used to also change between coordinate systems

scarlet mango
fathom swallowBOT
#

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

torpid bay
#

i dunno the [ ] latex

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but its not a product

torpid bay
#

its a mtrix

scarlet mango
torpid bay
#

i is just an index

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$u^1 = x, u^2 = y$

scarlet mango
fathom swallowBOT
#

Yeatte

torpid bay
#

in this case

scarlet mango
torpid bay
#

imagine there's actual spaces in my latex

burnt ledge
# burnt ledge yea a matrix

In fact u can think of it like a linear transformation too, so say we have a function f: R^n -> R^m and we want to do something like a taylor expansion f(v+dv) = f(v) + [some matrix] dv + [higher order terms]

scarlet mango
#

Could we really use this definition in double integrals to change coordinates?

torpid bay
#

yes

scarlet mango
# torpid bay yes

Is there a solution process you can find that uses this matrix representation?

burnt ledge
#

if we want to find the best linear transformation to do this (similar to how f(x+dx) = f(x) + f'(x) dx + ... would do it for one variable) you find it is the jacobian

torpid bay
scarlet mango
torpid bay
#

$x = r\cos(\theta), \frac{\partial x}{\partial r} = \cos(\theta), \frac{\partial x}{\partial \theta} = -r\sin(\theta)$

fathom swallowBOT
#

Yeatte

latent edge
#

What discussy?

burnt ledge
torpid bay
#

^

scarlet mango
burnt ledge
#

Yes

latent edge
#

No

burnt ledge
#

well the one that i wrote is

scarlet mango
#

lmfao

burnt ledge
#

youve slightly misquoted me there

torpid bay
scarlet mango
burnt ledge
#

f(x+dx) = f(x) + f'(x) dx + ...

scarlet mango
gritty heath
#

Actually
3 blue 1 brown has a calculus series

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I'm sure the jacobian is explained there

scarlet mango
gritty heath
#

Much better than a text medium like discord can ever explain

molten raptor
#

konnichiwa

torpid bay
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it might be in a different form than usual

burnt ledge
#

What do you call that?

scarlet mango
scarlet mango
burnt ledge
#

I keep clicking back to mathscussy when i want to come back to ts conversation and tehn i remember this is happening in discussy 2

scarlet mango
#

yeah sorry it started as a simple question

torpid bay
#

$f(x) = \sum_{n=0}^{\infty}{\frac{(x-x_0)^n f^{(n)}(x_0)}{n!}$ might be the form you know of

burnt ledge
#

Its no problem haha im just very forgetful

torpid bay
#

in this case it's just a little substitution to get to the x + dx form

fathom swallowBOT
#

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

scarlet mango
torpid bay
#

let x = y + dy, let x_0 = y or smthn

latent edge
torpid bay
#

yeah

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and then we get $f(y + dy) = \sum_{n=0}^{\infty}{\frac{(dy)^nf^{(n)}(y)}{n!}$

fathom swallowBOT
#

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

torpid bay
#

the first few terms being $f(y+dy) = f(y) + f'(y)dy + f''(y)dy^2 / 2...$

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

let x = y + dy, and let x_0 = y

scarlet mango
burnt ledge
scarlet mango
#

it would have to be that x_0= x-dy

burnt ledge
#

the taylor expansion formula tells you "how csn you find the value of a function at x when you know all its derivatives at x0" right?

torpid bay
burnt ledge
#

we are just spinning it slightly to figure out the value of the function at y+dy, when we know all the derovatives at y

burnt ledge
#

Which is effectively the same problem but with slightly different symbols

torpid bay
#

$y = x_0$ and $ dy = x-x_0$ if we want to define it in terms of the new ones being isolated

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

yep

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its juts a change of variables

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2 new ones, 2 old ones

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just like $a = x+1$ and $b = y+1$, it's guaranteed to be fine

fathom swallowBOT
#

Yeatte

torpid bay
#

for an example of changing 2 old to 2 new

scarlet mango
torpid bay
#

yeah

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y just a vairalbe

burnt ledge
#

Yep

torpid bay
#

there's a nice little way to make the taylor series more compact which is really cool but prob later

scarlet mango
#

damn this went down a big ass rabbit hole

torpid bay
#

it goes furthur

burnt ledge
#

Hahaha yea

torpid bay
scarlet mango
#

why did we use the taylor expansion in the form we just mentioned again?

burnt ledge
#

It exposes the role of the derivative as the best linear approximation to a function

torpid bay
#

^

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specifically the first derivative's role

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being te one in J

scarlet mango
#

hmm I see

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oh yeah btw

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random

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but

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how do we use taylor series to approximate a multi-variable function?

torpid bay
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it's just a lot more terms that's all

burnt ledge
#

Basically you just taylor expand with respect to each of the variables

scarlet mango
#

if we have f(x,y), can we somehow separate the x terms from the y terms and apply taylor series in f_1(x) and f_2(y) ?

scarlet mango
gritty heath
#

You can expand with respect to x first, then expand with respect to y for each term you got from expanding the first time

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Sheer brute force works

scarlet mango
#

So that would give two different sums?

gritty heath
#

Its one giant sum

scarlet mango
#

or all the terms are in one sum?

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okeoke got it

torpid bay
#

$f(x,y) = \sum_{n=0}^{\infty}{\sum_{m=0}^{\infty}{\frac{(x-x_0)^n(y-y_0)^m \frac{\partial^{n+m} f}{\partial x^n \partial y^m} (x_0,y_0)}{n!m!}}$ iirc

#

there's a few conditions, like interchangability of the order of derivatives

scarlet mango
torpid bay
#

nah, x and y are different variables, so like take z =x^2 y^2

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$\frac{\partial^2 z}{\partial x \partial y} = 4xy$

scarlet mango
fathom swallowBOT
#

Yeatte

#

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

torpid bay
#

ye

scarlet mango
torpid bay
#

yeah I forgot the reasoning

scarlet mango
#

valid reason

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yeah my mind expanded a little more from all this

torpid bay
#

i think it's because they are two seperate variables and so you just multiply the things together

burnt ledge
fathom swallowBOT
burnt ledge
#

wtf why did all my parentheses disappear

scarlet mango
burnt ledge
#

yea

torpid bay
#

$\pdv{a}{b}$

fathom swallowBOT
#

Yeatte

burnt ledge
#

ive just written four of the terms instead of all infonitely many of them

torpid bay
#

huh, i so couldnve used that eralier

scarlet mango
burnt ledge
#

I tend not to worry myself too much about the higher order terms because the whole point of the taylor expansion is to not care about them

scarlet mango
#

Thank you to everyone who contributed in this yapping sesh

#

it was really useful to learn some of those things which I'll see in like 2 years

burnt ledge
#

Gladly

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calculus is pretty cool

torpid bay
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you can losely think of d/dx and d/dy a multiplicative in a way

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and so if I first took the taylor series for x, and then took the taylor series for y, the terms would essentially be all multiplied together

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this is actually a situation where the compact taylor series makes it easier to see

scarlet mango
torpid bay
#

yeah, neither did i, I stumbled upon some approximations for f(x+h) like a few weeks back in a notebook and turns out, it wasn't just a good approximation, it was exactly the taylor series

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I made it for help with coding simulation but it ended up being really cool

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let's take $ \d {y}{x}$

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texit?

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u ded?

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$\frac{dy}{dx}$

fathom swallowBOT
#

Yeatte

torpid bay
#

and let's add the second derivative to it

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$\frac{dy}{dx} + \frac {d^2y}{dx^2}$

fathom swallowBOT
#

Yeatte

torpid bay
#

and see that both terms are derivatives acting on a function y

scarlet mango
burnt ledge
scarlet mango
torpid bay
#

$\big(\dv{}{x} + \diff[2]{}{x})y\big) = \frac{dy}{dx} + \frac {d^2y}{dx^2}$

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oop

scarlet mango
torpid bay
#

$\big( x \big)$

fathom swallowBOT
#

Yeatte

scarlet mango
#

or just left( and right)

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lol its a bit big

#

,tex
\left( meow \right)

fathom swallowBOT
#

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

#

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

scarlet mango
torpid bay
#

$\big(\dv{}{x} + \dv[2]{}{x}\big)y = \frac{dy}{dx} + \frac {d^2y}{dx^2}$

#

ill just use partials for now

#

but just imagine they're both regular dervatives rn

scarlet mango
#

that isnt multiplication tho, its closer to matrix multiplication

torpid bay
#

$\dv[1]{y}{x}$

fathom swallowBOT
#

Yeatte

torpid bay
#

ok good got it

#

yeah this is not multiplication

#

rather its operation

scarlet mango
#

does that mean that you apply the derivative operator on y?

rocky shuttle
#

composition smugsmug

scarlet mango
#

or smth like that

torpid bay
#

yep

scarlet mango
#

I see

torpid bay
#

we can apply this to the taylor series from before

scarlet mango
#

Hmm

#

can you show me the first few terms written like that? I cant see it

scarlet mango
torpid bay
#

$f(x+dx) = f(x) + dx\dv{f}{x}{(x)}+\frac{dx^2}{2!}\dv[2]{f}{x}{(x)}+\frac{dx^3}{3!}\dv[3]{f}{x} {(x)} ...$

#

where mah (x) go sadcat

scarlet mango
#

Isn't that how we wrote it earlier?

torpid bay
#

yep, just expanded out

scarlet mango
rocky shuttle
rocky shuttle
torpid bay
#

there we go

scarlet mango
fathom swallowBOT
#

Yeatte

torpid bay
#

rn its just the taylor series

scarlet mango
#

ohhh theres more

torpid bay
#

and now we can seperate the f(x) from the rest of the terms

scarlet mango
#

OHHHH

#

I seeeee

torpid bay
#

$f(x+dx) = \big(1+ dx\dv{}{x}+\frac{dx^2}{2!}\dv[2]{}{x}+\frac{dx^3}{3!}\dv[3]{}{x} ...\big) f(x)$

scarlet mango
#

yep

#

thats nice

#

is that the thing that helped you in your coding thingy?

fathom swallowBOT
#

Yeatte

scarlet mango
#

or am I tripping? I think you were talking compact t. series

rocky shuttle
#

oh, the exp(d/dx) thingy

torpid bay
#

this is

#

let's have dx be h, to reduce the clutter a bit

scarlet mango
torpid bay
#

$f(x+h) = f(x) + h\dv{f}{x}{(x)}+\frac{h^2}{2!}\dv[2]{f}{x}{(x)}+\frac{h^3}{3!}\dv[3]{f}{x} {(x)} ...$

rocky shuttle
torpid bay
#

$f(x+h) = \big(1+ h\dv{}{x}+\frac{h^2}{2!}\dv[2]{}{x}+\frac{h^3}{3!}\dv[3]{}{x} ...\big) f(x)$

fathom swallowBOT
#

Yeatte

torpid bay
#

now let's combine the h and d/dx a bit

scarlet mango
#

Oh

#

OH

#

its the taylor series for e^x

torpid bay
#

yep

#

$\big(1+ h\dv{}{x}+\frac{h^2}{2!}\dv[2]{}{x}+\frac{h^3}{3!}\dv[3]{}{x} ...\big)=\big(1+ (h\dv{}{x})+\frac{(h\dv{}{x})^2}{2!}+\frac{(h\dv{}{x})^3}{3!} ...\big)= $

#

$\big( 1+ h\dv{}{x}+\frac{h^2}{2!}\dv[2]{}{x}+\frac{h^3}{3!}\dv[3]{}{x} ...\big) = \big( 1+ (h\dv{}{x})+\frac{(h\dv{}{x})^2}{2!}+\frac{(h\dv{}{x})^3}{3!} ...\big) = $

#

rip texit

scarlet mango
#

I think you didnt leave a space

#

after \big(

#

and the other

#

$\big( 1+ h\dv{}{x}+\frac{h^2}{2!}\dv[2]{}{x} +\frac{h^3}{3!}\dv[3]{}{x} ...\big) =\big( 1+ (h\dv{}{x})+\frac{(h\dv{}{x})^2}{2!} +\frac{(h\dv{}{x})^3}{3!} ...\big) = $

#

nope its just ded

torpid bay
#

anyway

#

yes

#

$\big(1+ (h\dv{}{x})+\frac{(h\dv{}{x})^2}{2!}+\frac{(h\dv{}{x})^3}{3!} ...\big)= e^{h\dv{}{x}}$

fathom swallowBOT
#

Yeatte

torpid bay
#

putting this back into our original

#

we get

rocky shuttle
#

imagine you'd just leave h as dx, then you'd have e^d kekw

torpid bay
#

$f(x+h) = e^{h\dv{}{x}}f(x) = \big( \sum_{n=0}^{\infty}{\frac{\big(h\dv{}{x}\big)^n}{n!}})f(x)$

scarlet mango
torpid bay
#

which is y i wanted to switch to h lel

rocky shuttle
scarlet mango
fathom swallowBOT
#

Yeatte

torpid bay
#

in this case $dx(\dv{}{x}) = 1$ actually so 👀

scarlet mango
#

this is a nice way to write this thing

fathom swallowBOT
#

Yeatte

scarlet mango
#

wait really?

torpid bay
#

dx as a differential operator

#

this gets into diffetnerial geometry tho

#

where again, dx(d/dx) isnt multiplication but operation

#

anyway, the e^(h d/dx) can be generalized as well

#

$e^{h \dv{x}{g} \dv{}{x}} f(x) = f(g^{(-1)}(g(x)+h))$

fathom swallowBOT
#

Yeatte

torpid bay
#

which is something for wayyyyy later

#

I recommend not using the compact taylor series tho, and just sticking with the ituition of the regular one

scarlet mango
scarlet mango
torpid bay
#

for now you can think of dx as an increment, prob better for now

#

tho later, you will think of them as 'dual' to each other

scarlet mango
scarlet mango
scarlet mango
scarlet mango
torpid bay
#

$\dv{y}{x}$ is the coefficient of the best linear function for a function y of x

burnt ledge
#

Yea all of this is nonsense you neednt worry about

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

take $y = e^x$

#

texit hello?

#

baby steps texit smh

burnt ledge
#

try editing out the space after the $

fathom swallowBOT
#

Yeatte

torpid bay
scarlet mango
torpid bay
#

let's say I wanted to approximate y = e^x at x = 1

#

for the first term, I just take y(0)

#

so let's write the n'th taylor polunomial as $y_n$ for now

fathom swallowBOT
#

Yeatte

torpid bay
#

so $y_0 = y(0) = 1$

fathom swallowBOT
#

Yeatte

torpid bay
#

which is good enough, it's close to (and precisely equal to) the e^x near x=0, which is what we want

#

but pretty far off for other values of x

#

so we take the next taylor polynomial

scarlet mango
scarlet mango
#

omg

torpid bay
#

yeah, but I want to find it for other values near x

#

as well

rocky shuttle
torpid bay
#

let's take he next taylor polynomial

scarlet mango
torpid bay
#

$y_1 = y(0) + \dv{y}{x}{(x)}|^{x=0} x$

fathom swallowBOT
#

Yeatte

torpid bay
#

in thise case, taking the derivative of e^x at 0, is just 1

#

so the best approximation for a function of the type a + bx is 1 + 1x for e^x

lone granite
#

Calculus?

torpid bay
#

,w plot e^x and 1+1x

torpid bay
#

its exactly equal at x=0, but also much closer for values near x =0, than the first taylor polynomial was

torpid bay
#

and we can extend this intuition for all the rest of the taylor polynomials

scarlet mango
torpid bay
#

$y_2(x) = y(0) + \dv{y}{x}{(x)}|^{x=0} x + \dv[2]{y}{x}{(x)}|^{x=0} \frac{x^2}{2!}$

#

and since the second derivative of e^x at x=0 is also 1 (wow)

#

it ends up being this

#

$y_2(x) = 1 + 1x + \frac{1x^2}{2!}$

fathom swallowBOT
#

Yeatte

scarlet mango
#

is that 2 supposed to be there at the end?

lone granite
fathom swallowBOT
#

Yeatte

torpid bay
#

,w plot e^x and 1+1x+1x^2 /2!

torpid bay
#

^ even better

scarlet mango
scarlet mango
torpid bay
#

it also takes 4 hours to forget how to do it and do just bootleg maatrices like ive done before

lone granite
scarlet mango
#

I mean I can see how the taylor series is perfect for these functions, but I could never understand the reasoning behind the inner machinations of it ya know?

lone granite
#

Name the Last Number before Absolute Infinity.

torpid bay
#

oh

#

none

#

iirc

scarlet mango
rocky shuttle
scarlet mango
#

so the number before infinity is also undefined

lone granite
#

It is possible to represent infinity minus one as a mathematical expression, but it does not actually equal anything or have any real mathematical value.

scarlet mango
#

I dont think humans will be able to comprehend what it means to be infinite in our lifetimes

torpid bay
#

infinity = non finite catthumbsup

scarlet mango
lone granite
#

How does an Infinite Hotel run out of rooms?

lone granite
scarlet mango
rocky shuttle
#

when a bigger cardinality arrives

lone granite
scarlet mango
rocky shuttle
scarlet mango
#

I think infinity can only be interpreted but will nonetheless remain undefined forever

lone granite
#

Math.

scarlet mango
#

Life.

lone granite
#

Cube.

rocky shuttle
scarlet mango
#

yeeee

lone granite
#

Try defining the difference between Infinity and Absolute Infinity.

scarlet mango
#

interpretting maths is a weird isomorphism to interpretting life or some shit

scarlet mango
zealous garden
torpid bay
#

oh

#

yeah

#

you still there fijo

scarlet mango
#

yeeee

scarlet mango
torpid bay
#

remember $e^{h \dv{}{x}} f(x)$

fathom swallowBOT
#

Yeatte

scarlet mango
#

yup

torpid bay
#

and how that makes a taylor series for x?

#

well

scarlet mango
#

you mean wrt to x?

torpid bay
#

yes

scarlet mango
#

yes

lone granite
#

Must be a dimension to see infinity

torpid bay
#

let's taek $e^{j \dv{}{y}}$

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

$e^{j\dv{}{y}}e^{h\dv{}{x}} f(x,y) = e^{j\dv{}{y}} f(x+h,y) = f(x+h,y+j)$

fathom swallowBOT
#

Yeatte

torpid bay
#

$e^ae^b = e^{a+b}$ (usually)

fathom swallowBOT
#

Yeatte

torpid bay
#

so, taking that

lone granite
zealous garden
torpid bay
#

$e^{j\dv{}{y}+h\dv{}{x}}f(x,y) = f(x+h,y+j)$ would also be the taylor series of f with respect to x and y

fathom swallowBOT
#

Yeatte

torpid bay
#

in this case we'll assume f is nice enough to where partial derivative commute

rocky shuttle
#

otherwise, use the Baker-Campbell-Hausdorff formula bleak

scarlet mango
scarlet mango
torpid bay
#

ah

#

yeah

scarlet mango
#

whattttt?????

scarlet mango
torpid bay
#

so $e^{j\pdv{}{y}+h\pdv{}{x}}f(x,y) = e^{j\pdv{}{y}}\big( \sum_{n=0}^{\infty}{\frac{\big( h\pdv{}{x}\big)^n}{n!}}f(x,y) \big)= \sum_{m=0}^{\infty}\frac{1}{m!}\big(j\dv{}{x}\big)^m{\sum_{n=0}^{\infty}{\frac{1}{n!}\big(h\pdv{}{x})^n f(x,y)}}$

fathom swallowBOT
#

Yeatte

torpid bay
#

lowkey I'm never gonna use this

scarlet mango
#

its cool tho

#

btw

torpid bay
#

but just as a concept for the derivatives being seperate from each other

scarlet mango
#

shouldnt there be parentheses around the two sums? to showcase that its the operators applying to f?

torpid bay
#

yeah

#

assume they're there

light thorn
#

So, I got an offer about a co-seminar for my calculus 2 class, it says it will help with the more difficult subjects, but I'm not sure. Should I take it if it's even still available? It was supposed to start this morning

torpid bay
#

calc 2 is fun catthumbsup

rocky shuttle
#

what's the dual of a seminar?

torpid bay
#

quasinar

scarlet mango
torpid bay
#

or a pseudonar

scarlet mango
rocky shuttle
torpid bay
#

dual just means that 2 things are connected in certain way to each other that's a little strong

#

like take dx and d/dx

scarlet mango
rocky shuttle
torpid bay
#

$dx = \dv{y}{x} dv$ but $\dv{}{x}=\dv{y}{x} \dv{}{y}$

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

in the first case its dy/dx, in the second case its the exact opposite

#

so If i used a change of coordinates, these two objects would change in the exact oppsoite way of each other, relating to the coordinate systems

agile fiber
#

duals are things that are in some way opposites or mirrors of each other, usually following a rule that dual(A) = B iff dual(B) = A and dual(dual(A)) = A

scarlet mango
#

what the heck

rocky shuttle
#

emphasis on usually

zealous garden
#

Sometimes they're anti-involutions instead of involutions

#

And sometimes it's just words on a page written by a monkey

scarlet mango
torpid bay
#

this is for the dx and dy in integrals

#

$\int dx = \int \dv{x}{y} dy$

zealous garden
#

In category theory you flip the arrows, in linear algebra you flip the arrows go to linear functionals on the space, in exterior algebra you take orthogonal complements, in geometric algebra you....

scarlet mango
#

wtf

zealous garden
zealous garden
scarlet mango
rocky shuttle
#

Do the thing

torpid bay
#

oh

fathom swallowBOT
#

Yeatte

torpid bay
#

hehe

scarlet mango
#

lol

#

but thats the good ol chain rule

#

Thats the second thing you showed

torpid bay
#

reverse chain rule technically but ye

scarlet mango
#

I was talking about the first

zealous garden
scarlet mango
rocky shuttle
torpid bay
#

of the 7 vectors product its one of the inner ones

scarlet mango
torpid bay
#

not to be confused with the interior product

zealous garden
#

In GA an inner product is none of (positive definite, non degenerate, scalar valued, symmetric)

rocky shuttle
#

I don't feel comfortable explaining GA

zealous garden
scarlet mango
zealous garden
scarlet mango
zealous garden
#

The inner product between two blades is the lowest generally nonzero term of the GP

scarlet mango
zealous garden
#

Extend to multivectors through bilinearity

rocky shuttle
#

Is that why you talk about metric vector spaces rather than just inner product spaces?

zealous garden
#

But yes

rocky shuttle
#

geometric product

zealous garden
#

Because that's the minimum requirement I need to make to access Geometric Algebras, and many theorems we care about don't really care if the form is positive definite I find

scarlet mango
#

wth are blades btw lol

zealous garden
#

Unironically though, a blade is a k-vector which is the wedge of 1 vectors

#

Geometrically, think of it as an oriented parallelogram

rocky shuttle
#

Imagine introducing sabers to GA

zealous garden
#

Or higher

scarlet mango
#

is it bad to ask what a k-vector is?

scarlet mango
torpid bay
#

$\hat{x} \wedge \hat{y} $ is a 2 blade, where $\hat{x}$ and $\hat{y}$ are 1 -blades

fathom swallowBOT
#

Yeatte

zealous garden
#

Like swordfighting specifically

torpid bay
#

i forget if its wedge or gprod

zealous garden
#

The techniques you use are called forms

#

Blades and forms

#

SPECIFICALLY swordfighting

#

It's meant to be

torpid bay
#

form 3, soresu was used by obi wan kenobi, one of the best users of form 3

scarlet mango
zealous garden
torpid bay
#

think of a 1-blade as a vector

rocky shuttle
zealous garden
#

A k-blade is easy to visualize, k-vectors can get complicated

zealous garden
scarlet mango
zealous garden
#

Then we build up from these

scarlet mango
torpid bay
#

mathematicians got bored

#

its just a name

zealous garden
#

So we have G(V), which has a space isomorphic to V which we will just call V. Vectors of V are 1-vectors. Blades are wedge products of 1-vectors, k-blades have k factors, k-vectors are sums of k-blades

scarlet mango
zealous garden
zealous garden
torpid bay
#

^ kinda yeah

zealous garden
#

Things get complicated MERELY because of how vector has historically been used

scarlet mango
zealous garden
#

And linear algebra isomorphisms abused

zealous garden
#

u^v is the parallelogram made by u,v,-u,-v laid end to end

zealous garden
#

It's equivalent to any other parallelogram in the same plane, with the same area, and same orientation

#

And you just repeat to higher dimensional analogues

scarlet mango
zealous garden
#

Technically if you really wanna do GA there's a whole completely contradictory way to view things that is arguably better, but this is a historically fruitful starting point

#

Anyways I have a meeting, bye

scarlet mango
#

okeoke bye

zealous garden
scarlet mango
#

Thank you for teaching me your ways

torpid bay
#

a k blade is a special k-vector that can be represented as a wedge product of 1-blades

scarlet mango
#

how do we even add wedge products tho lmao

#

unless we define a plane where parallelograms are now single vectors

torpid bay
#

I think of it as like putting 2 different objects into a bag together

scarlet mango
#

is there a visual way to see it? or is it some weird math shit?

rocky shuttle
#

it's just a superposition of blades

torpid bay
#

$1 + \hat{x}\wedge\hat{y}$ would be something where I have a scalar and a parallelogram, they' don't really add together into a single thing. but rather you can just manitupulate both of them at the same time and they don't interfere with each other

fathom swallowBOT
#

Yeatte

torpid bay
#

so like

#

$(1+\hat{x}\wedge\hat{y})\wedge(\hat{z}) = \hat{z}+\hat{x}\wedge\hat{y}\wedge\hat{z}$

fathom swallowBOT
#

Yeatte

scarlet mango
torpid bay
#

in the same bag, but no interferring catthumbsup

scarlet mango
#

what about 2^z?

rocky shuttle
scarlet mango
rocky shuttle
#

like "3 apples and 2 oranges" is such a combination

torpid bay
#

ye

scarlet mango
scarlet mango
#

I see

#

so we just show that we have these two things

torpid bay
#

i think

scarlet mango
#

its like when we do a+bi

rocky shuttle
scarlet mango
#

interesting

torpid bay
#

as examples of 0blade, 1-blade etc

scarlet mango
#

I cannot even fathom how these could be used in actually important fields of maths but its nevertheless interesting

torpid bay
#

well

#

actually

#

do you know quaternions?

scarlet mango
#

heard of em

#

is it 4 dimensional cube or something?

torpid bay
#

they are the vectors useed in 3D for rotations

scarlet mango
#

oh damn im far out

torpid bay
#

quaternions are like this

#

$q = a+bi+cj+dk$

fathom swallowBOT
#

Yeatte

scarlet mango
#

uhm

#

what does this mean exactly?

torpid bay
#

it's a complex number, but more

scarlet mango
#

i,j,k are vectors first of all right?

#

ohhh

torpid bay
#

yeah

scarlet mango
#

oh okeoke

torpid bay
#

technically

scarlet mango
#

How is GA connected to this tho?

torpid bay
#

$\hat{i},\hat{j},\hat{k}$ are in vector form, while $i,j,k$ are in algebra form

fathom swallowBOT
#

Yeatte

torpid bay
#

i,j,k, are actually bivectors

scarlet mango
#

huhhhh

torpid bay
#

2-blades, not 1 b-blades

#

^ i had stutter here

scarlet mango
#

so they each are represented in 2d planes?

torpid bay
#

yeah

scarlet mango
#

so we are talking 6 dimensions?

#

am I crazy for that?

torpid bay
#

it depends on how you count

scarlet mango
#

I suppose they are linearly independent

torpid bay
#

1 scalar, 3 vectors, 3 bivectors, 1 trivector

scarlet mango
#

the set containing them, i mean

torpid bay
#

yes

scarlet mango
torpid bay
#

i+j+k is a bivector, i^j^k is a scalar i tihnk

#

lemme write them in k-blade form

scarlet mango
#

this is tantamount to smoking LSD

scarlet mango
zealous garden
#

Meeting canceled

scarlet mango
torpid bay
#

$1\ \hat{x} , \hat{y}, \hat{z},\ \hat{y}\wedge}\hat{z}, \hat{z}\wedge\hat{x},\hat{x}\wedge{\hat{y} \ \hat{x}\wedge\hat{y}\wedge\hat{z}$

scarlet mango
torpid bay
#

for the various k blades

#

i,j,k are the 3 different 2 blades

scarlet mango
#

what am I even seeing here?

zealous garden
#

Hats are terrible

#

Why did you do this yeatte

torpid bay
#

remember that list of 1 scalar, 3 vectors, 3 bivector, 1, trivector? this is them listed out

zealous garden
fathom swallowBOT
#

Yeatte

$1\\ \hat{x} , \hat{y}, \hat{z},\\ \hat{y}\wedge}\hat{z}, \hat{z}\wedge\hat{x},\hat{x}\wedge{\hat{y} \\ \hat{x}\wedge\hat{y}\wedge\hat{z}$
```Compilation error:```! Extra }, or forgotten $.
l.49 ...at{x} , \hat{y}, \hat{z},\\ \hat{y}\wedge}
                                                  \hat{z}, \hat{z}\wedge\hat...
I've deleted a group-closing symbol because it seems to be
spurious, as in `$x}$'. But perhaps the } is legitimate and
you forgot something else, as in `\hbox{$x}'. In such cases
the way to recover is to insert both the forgotten and the
deleted material, e.g., by typing `I$}'.```
scarlet mango
torpid bay
#

a is the scalar, bi + cj +dk are the bivectors

#

quaternions don't describe the whole k-blade space

#

you need biquaternions for that in this case

scarlet mango
#

jeez

#

this is dank

zealous garden
#

Complex Quaternions

#

Why ever say biquaternions

#

Just say complex quaternions, it leaves no questions

#

Biquaternions is like "what? Huh?"

scarlet mango
zealous garden
#

Complex quaternions gives you the recipe

#

Quaternions with complex coefficients

scarlet mango
torpid bay
#

$i = y\wedge z \ j = z\wedge x \ k = x\wedge y$

fathom swallowBOT
#

Yeatte

scarlet mango
#

hmm

#

its a lil hard to visualize

#

xyz are vectors tho right?

torpid bay
#

yes

#

and i would rotate the plane yz

#

in 3D you can think of them as rotate about the x axis

#

but it only works for 3D

scarlet mango
torpid bay
#

hm, lets go to 2D for now

#

with a simple xy plane

scarlet mango
#

i'm listening

torpid bay
#

let's take the point (1,1) which we can represent as 1x + 1y

scarlet mango
#

yup

torpid bay
#

if I rotate te plane counter clockwise, im rotating through the plany $x\wedge y$

fathom swallowBOT
#

Yeatte

torpid bay
#

or clockwise, but by convention counter lcokwise

scarlet mango
#

Hmm

#

what do you mean when you say "rotating through the plane x^y"?

torpid bay
#

if I take the point (1,1) on the plane xy and rotate it, i will always end up at nother point on the plane xy

scarlet mango
#

yes

torpid bay
#

so if we trace out it's path through the space, it will make a circle that lives entirely within that xy plane

#

and never leave it when rotating by $x\wedge y$

fathom swallowBOT
#

Yeatte

zealous garden
torpid bay
#

let's take the usual complex number for now

scarlet mango
torpid bay
#

if i take the point (1,1) it is then notated at 1 +1i

zealous garden
#

Ew

torpid bay
#

if I rotate it by 90 degs counter lcokwsie, I just multiply by i

zealous garden
#

Don't do this please

torpid bay
scarlet mango
#

-1+1i

torpid bay
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yep, so notice how when I did that, it stayed i nthe complex plane

scarlet mango
zealous garden
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Why introduce all of this just to throw it away

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You're wasting brain space yeatte

torpid bay
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wait notated

zealous garden
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I beg of you stop this

torpid bay
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it is too late

zealous garden
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Just show how to reflect through a hyperplane

torpid bay
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I shall corrupt him

zealous garden
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It's all so much simpler

scarlet mango
zealous garden
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I'm at work so I can't spend all my energy on guiding young fijo

scarlet mango
torpid bay
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we can think of this 'i' rotate thru the complex plane as being like rotating the 1x +1y through the xy plane when we apply xy to the vector 1x +1y

torpid bay
zealous garden
rocky shuttle
torpid bay
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we took a bunch of potions in mc

zealous garden
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Use that P_v(u) = B(u,v) v/B(v,v)

scarlet mango
torpid bay
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$(x + y) \wedge (x\wedge y)$

fathom swallowBOT
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Yeatte