#serious-discussion
1 messages · Page 305 of 1
lock in
hI
zased what kind
is this a new form of "based"
do u have a heatwave as well
we have a 32° heatwave in England 
im in year 10 so im just doin newton's first and second laws relative to terminal velocity yh
its so bad vro but rn its better
Oh nice
yh wbu??
most of my degree was physics
Yep
if you like that, i'm pretty sure you'll enjoy lagrangian mechanics
basically newtonian mechanics but better
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
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
That’s the ultimate basics of Lagrangian mechanics
u in the uk too?
its good to see year 10s studying
i didnt study until y11 started
summer holidays too
do u do aqa triple?
Hai!
not very new
now i dont know if i was right or if "zased" means "not very new"
probbaly tje first
I'm saying zased is a form of based but it's not new
,w zased
hi
This doxes your last name
how?
wjat the helly are you talking about?
its on google....
most people's pfp's are
,av 974792201143996416
Copying your profile as we speak
💔
what happened to ur name
hi fiscussy 2
....what..
Huy
Hi
I have to download the new version of OneNote. Because the old version declares its end of service
I do not like changes
The old one is still working. I cannot find any reason to adapt a new one
Fk Microsoft
@microsoft
Now I have to adapt the new version
I'm so fking sad
fk
why
The full 'New Math' song by Tom Lehrer animated by myself for a school project.
I created it in Flash CS4 and ran it through After Effects to convert it. I'm sorry it's not HD.
Thanks very much for watching, I hope you enjoy it and please do subscribe for more videos like this.
now I don't feel bad i forgot how to do subtraction

my parents are laughing at me
they say you are a freaking math student and u can't count 
no I can't 
ufff 😭
This was awesome thank you
youre weird bro
😭 sorry
?
I am weird but nothing about that interaction supports this claim
cuz why would you willingly say "zased" instead of "based"
its the first time ive seen it
I didn't say it homie
even "based" is strange according to my hypocrisy
I told you what it means
It was asked and I answered
you're good bro
you probably are still weird
youre in a maths server
but thats the only thing making u weird afaik
what is this video about
i've seen people react so i'm curious now
nvm
it's explained in the first 3 second
i be like that
acting
then thinking
Ah Tom Lehrer
Cz its funny and i like it
hello guys
Hey
damn this channel pretty dead
Hiii
it means people have time to think
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.
“The saddest thing isn’t the world is burning.
It’s that you have a cup of water, and you don’t dump it.”
yeah okay
that guy sounds dumb
bro does not know how to put out fires
you need way more water than a cup, even for a campfire
you don't understand this is about apathy.
Jeremy.
Why be apathetic when you can lose your job instead
Jeremy? Jermy? Jerma? JERMA?
Big cup of water

i thought this was about global warming and i was like how tf would wasting water help
Have anyone done math projects how did you start?
asking your profs is a good start, but also if there is anything that interests you, you could work in that direction
what kind of math do you like, or what hobbies do you have
I mostly love calculus
can you code
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...
idk how feasible is it tho
How terrible
water makes things colder therefor dumping a cup of water on the ground cools the earth
hope this helps
Gurl...
I saw we build a fridge for the solar system
naruhodo…
:3c
Global warming solved!
I hate how discord embeds these
Bit of a meme high card run, made it to ante 11
porple stake
@faint light i think plays this right
Love when stone joker works out
Those red holo stones do things to my brain chemistry
@soft jungle welcome to the mathcord! 
😭 jesus
@fresh comet tyy
the red seal holo was really helpful since high card is so low base mult
though I did get it to like lvl 20
did anyone here study in cpge or go to x/ens (pin me plz if you see this message)
Hey I’m new at uni
Can someone explain what CCS, MS, and SESA are ?
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 ???
ask in one of the appropriate subject channels (e.g. if you think it's still theoretical cs then #theoretical-cs )
That’s the thing I don’t really think it’s theorical cs anymore the question goes to mathematicians I would say it maybe relates to advanced algebra but I’m not sure also, maybe I can ask it there and people will tell me if it’s not in the right channel ?
Thank you for your answer still
just make your best guess at which subject fits best
Can you describe your project?
What do you mean exactly by "my project" ? I just posted the question in #advanced-algebra
I’m anxious now that the question is weird or incomprehensible or it does not belong here but it’s ok
You’ll be fine, it sounds like pretty cool research

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?
For resources you can check Khan Academy
I did not enjoy Calc 3
hey guys does anyone know if matricies are in calc ab?
it wasn't in mine
ab should just be like limits and derivatives, that's all (maybe some trig ig)
@dry steppe welcome to the mathcord 
so how iportant would you say pre calc is to actual calc ab
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
i would have to look over the direct content again
gimme a sec
https://www.khanacademy.org/math/precalculus basing it off of this, Unit 2, unit 9, and unit 10 are the most important for calc. but in general you'll need to learn the other ones along the way at some point
trig, series, and limit+continuity
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
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
matrices are great
Yuck
Every theorem gets better when you remove the matrices sorry not sorry
"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"
ah lel
$V \cong W \iff V_+ \approx W_+ \wedge V_- \approx W_- \wedge V_0 \approx V_0$?
Yeatte
Yes
I'm not sure whats meant by approx?
Isometric, linearly isomorphic, same thing really
ah
omg i've proven two things isometric b4 in differential geometry
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
I think very different
That is for manifolds yes?
Pseudoriemannian manifolds?
This is for the local case of that I guess?
i barely understood any of mine but i had fun too
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 $$B(u,v)=D(Su,Sv)$$
wraithlord_kojima
Very simple
Under particular charts?
B,D being metrics?
You mean more than just a smooth structure and metric tensor?
Symmetric bilinear forms yes
man i dont remember
pretty simple requirenents
We make no ask of nondegeneracy for many definitions
cones ❤️
You may notice that through linear representation of bilinear forms, we have that B(u,v)=u^TBv=D(Su,Sv)=u^TS^TDSv => B=S^TDS
man i really really need a good geometry book
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
,w sylvester law of inertia
huh..... certainly reminds me of the jacobian and metric tensor
this is a nother form of it, right?
Wolfram Alpha doesn't understand your query!
Perhaps try rephrasing your question?
Click here to refine your query online
HAHAHA
Jacobian is too many things
You mean the differential?
The map between tangent spaces?
i think yeah ( also a thing that refers to too many things)
$J = \frac{\partial x_i}{\partial x_j}$ or smthn
Yeatte
i cant quite remember the indices but yeah osmeting like this
maybe they were both on top?

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

did you see my diff geo notes that i posted a week ago?
yeah they're both up
$J = \frac{\partial x^i}{\partial y^j}$
Yeatte
can you please help me
it’s fairly simple
im not clicking links to domains i dont know
2nded
!help
To ask for mathematics help on this server, please open your own help channel or help thread. See #❓how-to-get-help for instructions.
u can tell its an image bc of png? not really a dangerous link but rather its embed fail 
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 $f'_{2.5} = 5$
shiru
rip i went to sleep and iddnt see this
lol it’s ok
Idt so
Suppose that $TT^$ is invertible, show that $P=T^(TT^*)^{-1}T$ is a projection onto $(\ker(T))^\perp$
Nicole
Is it safe to assume T is a bounded linear operator between Hilbert spaces?
finite dimensional vector space
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 you
Also, sorry for stalking
LOL
hello! Could you explain why this equation is true? I prolly won't understand but it wouldn't hurt to try
I'm a language nerd
That is a definition
its like generalising the derivative
or partial derivatives if yoire familiar with them
this tells you how much the output of a function changes when you change its input
oh i took shower am bajj
that sounds like crazy work
i'ts required for quite a lot of things
or rather the concept of a derivative
u know derivatives?
it's probably to use it on vectors then yeah
wait isnt that basically the normal derivative? Im a lil stupid
it's a little different because when you have 1 dimension input, and 1 dimension output, all you need is $\frac{dy}{dx}$
Yeatte
If your function has multiple inputs and outputs you have to track all of thrm, so the jacobian assembles all the derivatives together
but when you have 2 inputs, then representing how much the output changes requires you to ask how much each input changes.
How does it achieve that?
That sounds true enough
You take the derivative of each output with respect to each input and throw the value in an array
That's it
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
There are reasons why the array is shaped in some way but its fairly geometric and I dont geometry
when you say value, you mean it could be a function or a scalar or 0, right? And by array, what does it look like?
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
You can find derivative at one point then its just a number
yup thats true
A matrix where the (i,j)th entry is the rate of change of the ith output variable w.r.t. the jth input variable
Yea sory thats what i meant, a derivative describes a function R -> R, partial derivatives encode the effects of each of the several inputs of a function R^n -> R, jacobian tells you each of the effects of all the inputs on all the outputs of a function R^n -> R^m
$\lbracket \frac{\partial z}{\partial x} \frac{\partial z}{\partial y} \rbracket= \frac{\partial z}{\partial u^i} = J$ for an example of 2 inputs, x,y and 1 output z
wait hold up
does it need to be same n for R^n?
So, isnt it just a system of functions, each one being the derivative of our multivariable function wrt each variable?
Yeah, I was asking whether we are talking general derivatives or at certain points
so its a matrix? or is it just some kind of isomorphism?
to find a specific number for
it's a matrix yeah, it can be used to also change between coordinate systems
Yeah matrix
In the left-most side, why is that product not in normal parentheses?
Yeatte
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
yea a matrix
its a mtrix
In vector calculus, the Jacobian matrix (, ) of a vector-valued function of several variables is the matrix of all its first-order partial derivatives. If this matrix is square, that is, if the number of variables equals the number of components of function values, then its determinant is called the Jacobian determinant. Both the matrix and (if ...
yep thats what I've known jacobian to be useful for
how is u^i defined exactly?
What is it?
Yeatte
in this case
ahh I see
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]
Could we really use this definition in double integrals to change coordinates?
yes
that seems demented
Is there a solution process you can find that uses this matrix representation?
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
the only way i know how is to manually calculate it, by just takign the derivatie
I never learned that f(x+dx)= f'(x)dx lol
$x = r\cos(\theta), \frac{\partial x}{\partial r} = \cos(\theta), \frac{\partial x}{\partial \theta} = -r\sin(\theta)$
Yeatte
Thats really weird lookin
What discussy?
taylor expansions are very important I think they can help alot in understanding
^
so that equation is a taylor expansion?
Yes
No
well the one that i wrote is
lmfao
youve slightly misquoted me there

which one is that?
This yes
f(x+dx) = f(x) + f'(x) dx + ...
but you mentioned taylor exp. right after writing f(x+dx)= f'(x)dx am I crazy?
wait shit
Actually
3 blue 1 brown has a calculus series
I'm sure the jacobian is explained there
I never learnt that thats a taylor expansion
Much better than a text medium like discord can ever explain
konnichiwa
it might be in a different form than usual
What do you call that?
I never understand his vids tho, its like for actually intelligent people
I doubt that
Thats interesting
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
yeah sorry it started as a simple question
$f(x) = \sum_{n=0}^{\infty}{\frac{(x-x_0)^n f^{(n)}(x_0)}{n!}$ might be the form you know of
Its no problem haha im just very forgetful
in this case it's just a little substitution to get to the x + dx form
yupyup
Yeatte
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
And we can sub dx-x_0 to be some constant? or am I crazy for this?
let x = y + dy, let x_0 = y or smthn
The community is getting healthy
Yeatte
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
the first few terms being $f(y+dy) = f(y) + f'(y)dy + f''(y)dy^2 / 2...$
Yeatte
how did we arrive to that lmao
let x = y + dy, and let x_0 = y
but how can we know that both of these will always hold true?
we want the "x" in the formula (the input to x for the function we're expanding) to be y+dy here, and we want "x0" in the formula (the value where we know all the derivatives) to be y
it would have to be that x_0= x-dy
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?
it's just writing 2 new variables to be in terms of 2 old ones
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
yes
Which is effectively the same problem but with slightly different symbols
$y = x_0$ and $ dy = x-x_0$ if we want to define it in terms of the new ones being isolated
Yeatte
I see, and they just work things out themselves like usual?
yep
its juts a change of variables
2 new ones, 2 old ones
just like $a = x+1$ and $b = y+1$, it's guaranteed to be fine
Yeatte
for an example of changing 2 old to 2 new
when we write "y", btw, we mean an arbitrary variable, right? Cuz its usual to write y=f(x)
Yep
there's a nice little way to make the taylor series more compact which is really cool but prob later
yes that makes sense
damn this went down a big ass rabbit hole
it goes furthur
Hahaha yea

why did we use the taylor expansion in the form we just mentioned again?
It exposes the role of the derivative as the best linear approximation to a function
hmm I see
oh yeah btw
random
but
how do we use taylor series to approximate a multi-variable function?
it's just a lot more terms that's all
Basically you just taylor expand with respect to each of the variables
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) ?
oh, thats way lazier than I thought
You can expand with respect to x first, then expand with respect to y for each term you got from expanding the first time
Sheer brute force works
So that would give two different sums?
Its one giant sum
$f(x,y) = \sum_{n=0}^{\infty}{\sum_{m=0}^{\infty}{\frac{(x-x_0)^n(y-y_0)^m \frac{\partial^{n+m} f}{\partial x^n \partial y^m} (x_0,y_0)}{n!m!}}$ iirc
there's a few conditions, like interchangability of the order of derivatives
can't we just use n for both sums?
nah, x and y are different variables, so like take z =x^2 y^2
$\frac{\partial^2 z}{\partial x \partial y} = 4xy$
also, do you perhaps mean del(y^m) ?
Yeatte
Yeatte
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
ye
that doesnt explain the reason they cant both have n lol
i think it's because they are two seperate variables and so you just multiply the things together
yea we just get $$f(x+\dd x, y+\dd y)=f(x,y) + \pdv{f}{x} (x,y)\dd x + \pdv{f}{y} (x,y)\dd y + \frac12\pdv[2]{f}{x} (x,y)(\dd x)^2 + \dots $$
wtf why did all my parentheses disappear
wait is that the same as the double sum we saw earlier?
yea
$\pdv{a}{b}$
Yeatte
ive just written four of the terms instead of all infonitely many of them
huh, i so couldnve used that eralier
nono, its just that im not accustomed to double sums very well, so I thought we would have a bunch of products
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
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
you can losely think of d/dx and d/dy a multiplicative in a way
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
this is actually a situation where the compact taylor series makes it easier to see
does that have to do with the roots of the original function?
I didn't learn abt that
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
I made it for help with coding simulation but it ended up being really cool
let's take $ \d {y}{x}$
texit?
u ded?
$\frac{dy}{dx}$
Yeatte
Yeatte
and see that both terms are derivatives acting on a function y
how does that help with your coding simulation thing?
\dv{y}{x} btw
thats very true
when using powers, you should use \big( and \big)
$\big( x \big)$
Yeatte
fijokazż
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
Yeatte
Compile Error! Click the
reaction for more information.
(You may edit your message to recompile.)
is that the correct form? looks a lil wicked
$\big(\dv{}{x} + \dv[2]{}{x}\big)y = \frac{dy}{dx} + \frac {d^2y}{dx^2}$
ill just use partials for now
but just imagine they're both regular dervatives rn
that isnt multiplication tho, its closer to matrix multiplication
$\dv[1]{y}{x}$
Yeatte
does that mean that you apply the derivative operator on y?
composition 
or smth like that
yep
we can apply this to the taylor series from before
I mean, I can't imagine it
$f(x+dx) = f(x) + dx\dv{f}{x}{(x)}+\frac{dx^2}{2!}\dv[2]{f}{x}{(x)}+\frac{dx^3}{3!}\dv[3]{f}{x} {(x)} ...$
where mah (x) go 
Isn't that how we wrote it earlier?
yep, just expanded out
where?
\dv and \pdv shenanigans from the physics latex package
(mostly the reason why i don't use them)
there we go
Yea but we didn't use the equation you mentioned
Yeatte
rn its just the taylor series
ohhh theres more
and now we can seperate the f(x) from the rest of the terms
$f(x+dx) = \big(1+ dx\dv{}{x}+\frac{dx^2}{2!}\dv[2]{}{x}+\frac{dx^3}{3!}\dv[3]{}{x} ...\big) f(x)$
Yeatte
or am I tripping? I think you were talking compact t. series
oh, the exp(d/dx) thingy
the what? e^(d/dx)?
$f(x+h) = f(x) + h\dv{f}{x}{(x)}+\frac{h^2}{2!}\dv[2]{f}{x}{(x)}+\frac{h^3}{3!}\dv[3]{f}{x} {(x)} ...$
f(x+h) = exp(h d/dx) f(x)
$f(x+h) = \big(1+ h\dv{}{x}+\frac{h^2}{2!}\dv[2]{}{x}+\frac{h^3}{3!}\dv[3]{}{x} ...\big) f(x)$
Yeatte
now let's combine the h and d/dx a bit
doesn't that give a different result tho?
Oh
OH
its the taylor series for e^x
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
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
anyway
yes
$\big(1+ (h\dv{}{x})+\frac{(h\dv{}{x})^2}{2!}+\frac{(h\dv{}{x})^3}{3!} ...\big)= e^{h\dv{}{x}}$
Yeatte
imagine you'd just leave h as dx, then you'd have e^d 
$f(x+h) = e^{h\dv{}{x}}f(x) = \big( \sum_{n=0}^{\infty}{\frac{\big(h\dv{}{x}\big)^n}{n!}})f(x)$
well i think this is the case where dx cant be multiplied by 1/dx. Or am I crazy?
which is y i wanted to switch to h lel
yeah, I don't advise using dx to denote an increment here
i think you forgot to mult. e by f(x) but yeah thats true
Yeatte
in this case $dx(\dv{}{x}) = 1$ actually so 👀
this is a nice way to write this thing
Yeatte
wait really?
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
$e^{h \dv{x}{g} \dv{}{x}} f(x) = f(g^{(-1)}(g(x)+h))$
Yeatte
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
thats insane to me, that it touches this area
to me, it seems like the dx term is an increment, but d/dx is an operator, or is that crazy work?
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
wait wtf is this lmao
ohh I see lol
I didnt understand the intuition of the regular one to begin with
Doesn't duality mean action and meaning?
$\dv{y}{x}$ is the coefficient of the best linear function for a function y of x
Yea all of this is nonsense you neednt worry about
Yeatte
I speak in nonsense
try editing out the space after the $
Yeatte

that doesnt make much sense
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
Yeatte
so $y_0 = y(0) = 1$
Yeatte
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
didnt we want to find it for x=0?
the coefficient such that dy = (dy/dx) dx 
let's take he next taylor polynomial
I don't get the connection between the two statements
$y_1 = y(0) + \dv{y}{x}{(x)}|^{x=0} x$
Yeatte
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
Calculus?
,w plot e^x and 1+1x
its exactly equal at x=0, but also much closer for values near x =0, than the first taylor polynomial was
I see
Affirmative.
and we can extend this intuition for all the rest of the taylor polynomials
we can do the same thing here too?
$y_2(x) = y(0) + \dv{y}{x}{(x)}|^{x=0} x + \dv[2]{y}{x}{(x)}|^{x=0} \frac{x^2}{2!}$
and since the second derivative of e^x at x=0 is also 1 (wow)
it ends up being this
$y_2(x) = 1 + 1x + \frac{1x^2}{2!}$
Yeatte
is that 2 supposed to be there at the end?
How much time did you spend learning these commands?
Yeatte
,w plot e^x and 1+1x+1x^2 /2!
^ even better
it takes 4 hours at most if you wanna learn sums, limits, integrals and derivatives imo
very true
Noted
it also takes 4 hours to forget how to do it and do just bootleg maatrices like ive done before


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?
Name the Last Number before Absolute Infinity.
infinity is undefined i think lol
you just did
so the number before infinity is also undefined
Mission Passed.
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.
I dont think humans will be able to comprehend what it means to be infinite in our lifetimes
infinity = non finite 
yeah maths is always useful even when it doesnt really make a lot of sense
How does an Infinite Hotel run out of rooms?
In maths, you are the maker in such concepts.
yeah ive seen the vid bud
when a bigger cardinality arrives
Video? Science.
oh shit
Science? Math.
I think infinity can only be interpreted but will nonetheless remain undefined forever
Life.
Cube.
Well, it's an umbrella term for a lot of (different) concepts in math.
yeeee
Try defining the difference between Infinity and Absolute Infinity.
valid
interpretting maths is a weird isomorphism to interpretting life or some shit
idek what that means
Not undefined, doesn't exist
yeeee
I choose to believe it exists
remember $e^{h \dv{}{x}} f(x)$
Yeatte
yup
you mean wrt to x?
yes
yes
Maybe it exists, beyond space and time. We just can't comprehend it.
Must be a dimension to see infinity
let's taek $e^{j \dv{}{y}}$
Yeatte
fr. I like to piss people off by choosing to believe contradicting things, but thats another way to put it
$e^{j\dv{}{y}}e^{h\dv{}{x}} f(x,y) = e^{j\dv{}{y}} f(x+h,y) = f(x+h,y+j)$
Yeatte
$e^ae^b = e^{a+b}$ (usually)
Yeatte
so, taking that
Our mindsets are the same, it's just that you transfer it differently.
I wish
$e^{j\dv{}{y}+h\dv{}{x}}f(x,y) = f(x+h,y+j)$ would also be the taylor series of f with respect to x and y
Yeatte
in this case we'll assume f is nice enough to where partial derivative commute
otherwise, use the Baker-Campbell-Hausdorff formula 
thats true
yessss thats really beautiful
what does that mean? that we dont have to use the del symbol?
whattttt?????
Three people for one formula is insane
so $e^{j\pdv{}{y}+h\pdv{}{x}}f(x,y) = e^{j\pdv{}{y}}\big( \sum_{n=0}^{\infty}{\frac{\big( h\pdv{}{x}\big)^n}{n!}}f(x,y) \big)= \sum_{m=0}^{\infty}\frac{1}{m!}\big(j\dv{}{x}\big)^m{\sum_{n=0}^{\infty}{\frac{1}{n!}\big(h\pdv{}{x})^n f(x,y)}}$
Yeatte
lowkey I'm never gonna use this
but just as a concept for the derivatives being seperate from each other
shouldnt there be parentheses around the two sums? to showcase that its the operators applying to f?
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
calc 2 is fun 
what's the dual of a seminar?
quasinar
Im no expert in the matter, but if you have time to spare, a little extra knowledge wouldnt hurt
or a pseudonar
what does dual mean? Is it not connected to the yoneda conjecture or whats it called from cat theory?
like, for example, connected is the dual of nnected
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
that doesnt clear it up
sorry, I'll stop with the bad puns
$dx = \dv{y}{x} dv$ but $\dv{}{x}=\dv{y}{x} \dv{}{y}$
Yeatte
ohh lol I thought it was fr sorry
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
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
what the heck
emphasis on usually
Many such cases
Sometimes they're anti-involutions instead of involutions
And sometimes it's just words on a page written by a monkey
how is dx even equal to dy/dx dv? the second one is just chain rule i get that one
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....
wtf
Well, you do a thing
how are these equal wth
Do the thing
oh
Yeatte
hehe
reverse chain rule technically but ye
I was talking about the first
Never ask a Geometric Algebraist what "Inner product" means
What does it mean in these terms i wanna know now

The answer would be "which inner product?"
of the 7 vectors product its one of the inner ones
whichever you feel comfortable explaining? idk
not to be confused with the interior product
In GA an inner product is none of (positive definite, non degenerate, scalar valued, symmetric)
I don't feel comfortable explaining GA
none of?
Correct, all of those are usually meant by one saying "Inner product" in other fields
Lmao its like it gave y'all ptsd or something
No, I did
yeah but what do you mean by none of (...)? like, i dont understand the linguistic structure of the statement lol
The inner product between two blades is the lowest generally nonzero term of the GP
I see, cant wait to learn abt it
Extend to multivectors through bilinearity
Is that why you talk about metric vector spaces rather than just inner product spaces?
Somewhat, I also redefine Inner Product Space to merely mean any nondegenerate space
But yes
whats a GP?
geometric product
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
wth are blades btw lol
You have a long way to go before you can wield a blade young padawan
Unironically though, a blade is a k-vector which is the wedge of 1 vectors
Geometrically, think of it as an oriented parallelogram
Imagine introducing sabers to GA
Or higher
is it bad to ask what a k-vector is?
again, i mean
$\hat{x} \wedge \hat{y} $ is a 2 blade, where $\hat{x}$ and $\hat{y}$ are 1 -blades
Yeatte
Do you understand how awesome the double entendres are? A k-form evaluates a k-blade and gives a scalar, a form is a technique in martial arts
Like swordfighting specifically
i forget if its wedge or gprod
The techniques you use are called forms
Blades and forms
SPECIFICALLY swordfighting
It's meant to be
form 3, soresu was used by obi wan kenobi, one of the best users of form 3
okay. first of all, what is a wedge? second of all, what is a 1-blade?
So a k-vector is a sum of k-blades
think of a 1-blade as a vector
And you use a dagger to reverse
A k-blade is easy to visualize, k-vectors can get complicated
OH MY GOD
if a blade is defined by a vector, how tf is a vector defined by a blade lmao
They both stem from the definition of 1-vector as in a vector in V the vectorspace
Then we build up from these
okay, and why is it called a blade?
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
wait, 1-vector just means a vector? like, in general?
Cus it's a flat subspace
Kinda yeah
^ kinda yeah
Things get complicated MERELY because of how vector has historically been used
what is a wedge? and a wedge product?
And linear algebra isomorphisms abused
Geometrically, think of it as building parallelograms and boxes out of your vectors
u^v is the parallelogram made by u,v,-u,-v laid end to end
hmm I see
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
what does it mean that k-vectors are sums of k-blades? I think i understand the above
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
okeoke bye
X=u^v+w^z, but maybe you can't factor X into vectors at all!
Thank you for teaching me your ways
a k blade is a special k-vector that can be represented as a wedge product of 1-blades
how do we even add wedge products tho lmao
unless we define a plane where parallelograms are now single vectors
I think of it as like putting 2 different objects into a bag together
that doesnt clear it up. It in fact makes it weirder
is there a visual way to see it? or is it some weird math shit?
it's just a superposition of blades
$1 + \hat{x}\wedge\hat{y}$ 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
Yeatte
so like
$(1+\hat{x}\wedge\hat{y})\wedge(\hat{z}) = \hat{z}+\hat{x}\wedge\hat{y}\wedge\hat{z}$
Yeatte
What does that mean? Im not very familiar with that term?
in the same bag, but no interferring 
what about 2^z?
a linear combination
is it just 2z?
like "3 apples and 2 oranges" is such a combination
ye
i mean yeah but is there no way to see it in a graph somehow?
ohhhhh
I see
so we just show that we have these two things
i think
its like when we do a+bi
you can draw multiple overlapping blades / parallelograms ig
interesting
as examples of 0blade, 1-blade etc
I cannot even fathom how these could be used in actually important fields of maths but its nevertheless interesting
they are the vectors useed in 3D for rotations
oh damn im far out
Yeatte
it's a complex number, but more
yeah
oh okeoke
technically
How is GA connected to this tho?
$\hat{i},\hat{j},\hat{k}$ are in vector form, while $i,j,k$ are in algebra form
Yeatte
i,j,k, are actually bivectors
huhhhh
so they each are represented in 2d planes?
yeah
it depends on how you count
I suppose they are linearly independent
1 scalar, 3 vectors, 3 bivectors, 1 trivector
the set containing them, i mean
yes
oh wait. then i+j+k is just a trivector?
this is tantamount to smoking LSD
Good luck
how is it a scalar?
is it because the vectors lie in different planes?
$1\ \hat{x} , \hat{y}, \hat{z},\ \hat{y}\wedge}\hat{z}, \hat{z}\wedge\hat{x},\hat{x}\wedge{\hat{y} \ \hat{x}\wedge\hat{y}\wedge\hat{z}$
good for me I guess
what am I even seeing here?
remember that list of 1 scalar, 3 vectors, 3 bivector, 1, trivector? this is them listed out
Let's start here
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$}'.```
But, i dont understand. How is a+bi+cj+dk the same as the list you provided?
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
Complex Quaternions
Why ever say biquaternions
Just say complex quaternions, it leaves no questions
Biquaternions is like "what? Huh?"
yeah because idek what to ask
that makes it clearer
$i = y\wedge z \ j = z\wedge x \ k = x\wedge y$
Yeatte
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
what do you mean by that? like, why would you rotate that?
i'm listening
let's take the point (1,1) which we can represent as 1x + 1y
yup
if I rotate te plane counter clockwise, im rotating through the plany $x\wedge y$
Yeatte
or clockwise, but by convention counter lcokwise
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
yes
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 $x\wedge y$
Yeatte
no i, the imaginary unit
let's take the usual complex number for now
lmfao true, didnt think it was a unit
if i take the point (1,1) it is then notated at 1 +1i
Ew
if I rotate it by 90 degs counter lcokwsie, I just multiply by i
Don't do this please

-1+1i
yep, so notice how when I did that, it stayed i nthe complex plane
do you mean "notated as", or "rotated at"? its like a typo fork
Why introduce all of this just to throw it away
You're wasting brain space yeatte
wait notated
I beg of you stop this
it is too late
Just show how to reflect through a hyperplane
I shall corrupt him
It's all so much simpler
where else would it go?
I'm at work so I can't spend all my energy on guiding young fijo
im not even sure what the purpose of this is anymore lmao
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
i tried, I couldn't 
Wtf do you mean you couldn't lmfao
how did we get here again lmao 
we took a bunch of potions in mc
Use that P_v(u) = B(u,v) v/B(v,v)
how do we apply xy to that vector tho? what does it mean to apply xy lol
$(x + y) \wedge (x\wedge y)$
Yeatte
See yeatte

