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00:00 - 17:0017:00 - 23:00

00:10
@Semiclassical How's it now?
Why did you remove it and why is the SE so slow at notifying me
I recall there being a closed form for $\sum |{\rm Aut}(G)|^{-1}$ where $G$ runs over all (isomorphism classes of) finite abelian groups. Can't locate it though. Ideas?
nevermind, apparently Hall proved it equals $\sum |G|^{-1}$ (same $G$s)
00:31
hi chat
@andrewL because I misread what you wrote
thought you meant taking tan of 0.78 radians, which is nearly pi/4 radians and therefore would have tangent of about 1.
Ahh, I see.
01:25
in the evenings I have to spike my coffee with Kahlua to counteract the caffeine
see, I have a method
01:37
Playing with my Rubik's cube, it occurred to me that $(1~2)$ did not seem to be in $\langle(1~2~3~4),(3~4~5~6)\rangle$, but I couldn't prove it
(Rubik's cube interpretation: One can't switch two cubies by only turning the top and right-side faces.)
Well, one can't switch two cubies at all.
user174558
@Monad 1. You may not have expressed yourself properly to him 2. He may have misunderstood you 3. A lecturer in mathematics does not mean anything
user174558
01:50
@anon I only know one Alex, and his name is Clark.
is 20 references too many for a 10 page paper?
user174558
There is no such thing as too many or too few.
user174558
You should reference what you need to, no more no less.
@LeakyNun You can if you ignore the edge cubies. (I forgot to mention I was doing this on a 2x2.)
01:59
i love the introduction to that movie
user174558
I hate the movie Pi.
user174558
I watched one minute and switched off.
"Hate" is such a strong word.
i like everything about that movie.
user174558
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ Hate need not be a strong word. I hate ice cream.
user174558
02:01
My favourite movie is Blue Lagoon: The Awakening.
you know the intro scene with the figures moving in the background, and then you suddenly realize they have stopped moving and the music comes in
i did not understand it but there were some good scenes
user174558
There is a recent movie Midnight Special. It is so terrible.
@JasperLoy but you still have to put effort into hating ice cream, no?
02:03
oh I want to see that, dont spoil please
user174558
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ Not much effort.
The moving people are Andrei's (the main character's) family. Appears multiple times in dream sequences; I always interpreted it as representing Soviet Russia's suffering.
user174558
I just dreamt Darth Vader was inviting me to a light sabre fight.
user174558
I tried to turn on my light sabre but could not, so used it as an excuse to run away.
you know what Freud would say about that
user174558
02:05
Well, to me, dreams are just random collections of thoughts which may not mean anything.
user174558
I learnt not to take my thoughts too seriously.
user174558
Sometimes, I think of all kinds of weird things which I don't mean to do.
lots of modern scientists think dreams served an evolutionary purpose
user174558
If your child is worried about his bad thoughts, tell him that they don't mean anything. They are just thoughts, not his real intentions.
user174558
02:07
To me, physics is real science, but the social sciences suffer from bad experiments.
How are the meds working? @JasperLoy
user174558
To treat humans as subjects in experiements is different from using wooden blocks to show that F=ma.
like nightmares are meant to mentally prepare you for certain rare horrible situations
user174558
Every human is different, and statistics on how people react don't mean anything to me except meaningless numbers.
like a premonition, to keep you from being eaten by a bigger animal
user174558
02:09
I am not even sure evolution is true. I have not studied it though. I think it is just a theory.
user174558
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ Thinking of going off meds by the end of this year.
user174558
Every few days, I hear scientists publishing some study on humans. I wonder how many of these studies are pressure from publish or perish.
user174558
I no longer take these studies seriously, those on human beings that is, because human beings are not blocks of wood for F=ma.
02:11
if you cite the chief editor of a journal, will they be more likely to accept your article ?
user174558
Only they know. Every person is different.
02:22
If that makes a difference, it's a bad journal.
corruption is everywhere :p
02:39
oh nooooooooooo.
user174558
02:56
My journal is in my drawer, lol.
at least its not the garbage can
 
9 hours later…
11:46
whats the common notation for real version of $L^2(X)$? (ie equivalence classes of square integrable functions from $X$ to $\mathbb R$ rather than from $X$ to $\mathbb C$.)
11:59
After some searching I think $L^2(X;\mathbb R)$ or $L^2(X,\mathbb R)$ is normal, but I have not seen many examples
Given: $ax^{2} + bx + c$, is there an easy way to compute the $n^{th}$ terms of $(ax^{2} + bx +c)^{n}$?
Hi! Can anyone please answer this question?chemistry.stackexchange.com/q/53927/31216
$c_{n} = c^{n}$
But the rest I'm unsure.
@Matix Why would anyone here be able to answer a chemistry question?
its actually in a chemistry numerical but deals with math.
its not really chemistry.
12:02
@Owatch this is the generalized version of the binomial theorem
What's the complexity (lowest) record for bitwise multiplication algorithm in terms of number of bits?
@Owatch Trinomial coefficients.
how do we find approximate simple whole number ratio?
Yes, I seem to remember a bit of that from high school..
Something to do with a pyramid too.
of 1.098 and 0.277?
@LeakyNun As far as I know if $n$ is the greatest number of bits, then it is $nlog(n)$
12:03
@TobiasKildetoft And what is the algorithm?
@Matix Euclidean algorithm
@LeakyNun No idea. Something involving fast Fourier transforms
if i divide 0.198 and 0.277 it comes 3.963.....how do i write that as a ratio?
@LeakyNun what do you mean?
you did the division incorrectly first of all
uh i meant 1.098
please help.
What numbers are you dividing?
12:09
1.098 and 0.277
and what is wrong with the result?
i have to find a simple whole number ratio of these two numbers.
there is no such, as their ratio is not a whole number
like 2:3 or something
the approximate ratio
how approximate?
12:12
I dont know about that.
normal approximation maybe
then this is not a math question. The correct ratio is 1098/277, possibly with some cancellation
okay.I ll ask in a chemistry chat or something.
@Matix continually take reciprocal of ratio and record decimal part until it is close to an integer
@TobiasKildetoft ok, thanks
i did not understand @LeakyNun.
For example, 3.963 is close to 4
so you can approximate it in one step
for other more complicated ratio like 56:138, you would need to do more stuff
@Matix Are you interested?
12:20
he's asking in the Chem chat
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ whatever
yes sorry
@Matix Do you understand my response?
Wanna see something stupidly surprisingly hard? math.stackexchange.com/q/1831401/166353
so the ratio is 4:1?
12:22
@Matix Yes. If you're interested I can tell you more.
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ I belong to the chem chat also
oh and what about 56:132?
@Matix It was 138, but if you want I can do with 132 as well
how do we do it with 138?
@AkivaWeinberger weird
12:25
@Matix So we find 138/56, and we find that it is 2.464
this is not close to a whole number
so we remove the 2, and keep 0.464
Do you understand it until now?
okay i have understood but why take the reciprocal?
so, we still want to estimate 0.464, so we take its reciprocal
1/0.464 = 2.154
This is close enough to an integer, so we take it as 2
(If you are not satisfied, you can do more steps until it approaches an integer)
so:
  138
= 56 * 2.464
= 56 * (2 + 0.464)
= 56 * (2 + 1 / 2)
= 56 * (5 / 2)
So 138/56 ~ 5/2
@BalarkaSen I think it's equivalent to showing that the convex hull of a finite union of rays is closed (at least when all the rays have their vertex at the origin, though I doubt that's needed for it to be true)
@AkivaWeinberger Hmm, I would have been tempted to claim that linear maps are closed. Is this not the case?
i am so bad at this.
thank you
12:29
welcome
What course are you taking? @Matix
@TobiasKildetoft No, it's not true.
i am only 16.
@Matix I just went 17.
12:31
@BalarkaSen I see (I didn't really think that much about it, so there is probably an easy example)
@AkivaWeinberger That sounds good to me. Instead of thinking abstractly, I'd start by thinking about the image of each term in $Ax$, for $x_i > 0$. Boundary of those regions are rays passing through origin, and union should be the convex hull. I don't have a good idea how to do this though.
Not union, I meant *intersection.
@Tobias Project the graph of $xy = 1$ in $\Bbb R^2$ to $\Bbb R$ to the x-coordinate?
@TobiasKildetoft One is given in the question post
@AkivaWeinberger Ahh, I only read the initial question. Good to know that my intuition fails as usual :)
Closed area above graph of $y=e^x$, projected onto $y$-axis
In mathematics, a trinomial expansion is the expansion of a power of a sum of three terms into monomials. The expansion is given by ( a + b + c ) n = ∑ i + j + k = n i , j ...
$\Large\displaystyle(a+b+c)^n=\sum_{i,j,k:\ i+j+k=n}\binom{n}{i,j,k}a^ib^jc^k$
12:38
If $0\notin A(\Delta)$, where $\Delta$ is where the coordinates add to $1$, then it's closed by gerw's proof.
@AkivaWeinberger Same idea, but unnecessarily complicated.
But I suppose $e^x$ is a natural choice, as it has a more distinct asymptote along the y-axis than $1/x$. I retract my previous comment.
Some nasty issues with the connectivity here , I wouldn't even dare to start a talk.
Is any of you done with this?
$$\sum _{n=1}^{\infty } \frac{\psi (n) \psi \left(n+\frac{1}{2}\right) \psi \left(n+\frac{1}{3}\right)\cdots\psi \left(n+\frac{1}{m}\right)}{n \left(n+\frac{1}{2}\right) \left(n+\frac{1}{3}\right)\cdots \left(n+\frac{1}{m}\right)}, \ m\ge2$$
@user1618033 what is $\psi$?
@LeakyNun a polygamma function (digamma here)
In mathematics, the digamma function is defined as the logarithmic derivative of the gamma function: ψ ( x ) = d d x ln ⁡ ( Γ ( x ) ) = Γ ′ ( x ...
Well, very nasty issues with connectivity. Back later.
so $\psi(n)=\dfrac{\gamma'(n)}{\gamma(n)}$
12:57
@LeakyNun Yes that is what I wanted, thanks!
13:38
does anyone here know how to prove the non-existence of a homotopy between 2 paths with same end points when there is a hole in between those 2 paths?
I've been trying to prove it for the past few days but the proof seems really ambiguous...
That alone isn't going to be enough. Consider a sphere with a puncture at the south pole and a loop around the equator
you can't shrink the loop to a point by moving the loop south, but you can bring it up to the north pole
so the loop is contractible despite the puncture it surrounds.
now, if you treat the plane as having a puncture at infinity (or equivalently, cutting it off somewhere to make a really big disk) then it should be true.
(if that seems like nitpicking, you may be right; i'm not entirely awake right now)
13:59
When my topology sheet mentions "the surface $K^2$" without further comment, it's probably supposed to be the Klein bottle, right?
How many solutions this cauchy equation has y'=x^6+y^4 ,y(2)=-1
(ignore me) $y'-y^4=x^6$
$y''-4y^3y'=6x^5$
$y'''-12y^2y'-4y^3y''=30x^4$
Oops, I'm getting nowhere
lol
yeah, that's not the kind of ODE you should hope to solve by hand
This afternoon I will to see the video in YouTube from the official channel of the CIMAT by Cédric Villani, Cédric Villani en Guanajuato, conferencia "El arte vivo de las matemáticas" is in english from the minute 5' (with optional subtittles in spanish). I say it if any user want to see it. Good afternoon.
14:05
@Semiclassical yep, found that the hard way
@user243301 "I will to" is a direction translation of "voy a"? "Voy a" is "I am going to", "I will" have no "to" afterwards :)
ohh, Cedric Villani? neat
(sorry for picking grammar)
14:21
@Semiclassical like I was just imagining a plane like $\mathbb{R^2}$ with a hole at the origin of radius $1$. Now, consider the points $(0,2)$ and $(0,-2)$ and imagine a path, the right half of the circle $x^2+y^2 = 4$ and another path, the left half of the circle. How do I prove that there cannot be a homotopy between these 2 paths?
can somebody help with this y'=ycos(x)+xcos(x)-1
hello folks
I have some issues with transforming equations from the s domain to the z-domain
example:
$\frac{0.5}{s+j\omega} + \frac{0.5}{s-j\omega}$
14:38
@Sadams
$\frac{dy}{dx} = (y+x)\cos x -1$
$\Rightarrow \frac{dy}{dx} +1 = (y+x)\cos x$
$\Rightarrow \frac{d(y+x)}{dx} = (y+x)\cos x$
$\Rightarrow \frac{d(y+x)}{y+x} = dx\cos x$
That should do it
@LeakyNun "I'm going to"
@Sadams This is of the form $y'+P(x)y=Q(x)$, which can be solved by integrating factor (although SoumyoB's method is better)
@AkivaWeinberger Well, "I'm going to" is the same as "I am going to" isn't it?
$y'-\cos(x)y=x\cos(x)-1$
$y' e^{-\sin(x)}-\cos(x) y e^{-\sin(x)} = -x\cos(x)\sin(x)+\sin(x)$
$(y e^{-\sin(x)})'=-x\cos(x)\sin(x) + \sin(x)$
$(y e^{-\sin(x)})'=-0.5x\sin(2x) + \sin(x)$
$y e^{-\sin(x)}=-0.125(\sin(2x) - 2x\cos(2x)) - \cos(x) + C$
$y = (-0.125(\sin(2x) - 2x\cos(2x)) - \cos(x) + C) e^{\sin(x)}$
@LeakyNun Oh, I misread, I thought you thought it was "I will to"
@Danu Sort of lame notation, but it's the only thing it could be.
user174558
15:49
@leakynun What are you leaking?
@JasperLoy guess :p
Hello
Given the joint density function of the variables $ X,Y$ both variables are given values interval $ [0,1]$.

$$f_{x,y}\begin{cases}
& \frac{2}{3}\text{ if } 0\leq x\leq 1,0\leq y\leq 1,0\leq x+y\leq 1 \\
& \frac{4}{3}\text{ if } 0\leq x\leq 1,0\leq y\leq 1,1\leq x+y\leq 2 \\ \\
& 0\text{ else }
\end{cases}$$

I need to find the joint density function of $f_{x}$.

Someone can help me with this?
What I need to do here?
16:13
Someone here and can help with this question? Thank you
@LifeOfPai Do you happen to know how the density function $f_X$ and the joint density function $f_{X,Y}$ are related?
morning chat
What's the relation, then?
$$f_{x}(a)=\int_{- \infty}^{ \infty} f_{x,y}(a,y)dy$$
By definition
16:20
Well, then integrate and you will get $f_X$.
But I have 3 part, did not know how to calculate this...
Here I am stuck and can not continue.
@LifeOfPai then split the integral into 3 parts
This is the question, what will be the domain and what function each part?
Thank you
Well, first plot a graph
My name is here!
Well, my real name.
16:29
@MikeMiller It's even more confusing because the full quote is: "Show that the surfaces $\sum_{g\geq 1}\Bbb R P^2$ and $K^2$ [...]"
@LifeOfPai Which part is $2/3$, which part is $4/3$, and which part is $0$?
Uh, are the reals called $\Bbb B$-something in German?
Oh, ok.
Describe in terms of the colour of the region
I messed up :P
That sucks
16:30
Did my TA forget the latter is part of the former?!
The bottom (red) is 2/3 and the other 4/3
@LifeOfPai not really
the part where the red, orange, and green overlap is 2/3
What's the full question?
where the blue orange green overlap is 4/3
Yes that what i mean, sorry
16:31
@LifeOfPai Then, imagine the z-direction as coming out of your screen
you would see two triangular prisms
@MikeMiller In the previous question I (hopefully) showed that a union of two (relatively open) acyclic subsets has trivial cup product in positive degrees. The full question is then: "Show that the surfaces $\sum_{g\geq 1}\Bbb RP^2$ and $K^2$ cannot be written as the union of two open acyclic subsets"
The assertion follows from nontriviality of $\smile$ on $H^1\times H^1$ in $\Bbb Z_2$ coefficients
Oh, imagine the density as the z-direction
sure. I still find the first thing baffling
My name is also here!
(Well, my real name, of course)
@MikeMiller ... me too :(
16:34
@LeakyNun $$\int_{0}^{1}\int_{0}^{x} \frac{2}{3} dydx + \int_{0}^{1}\int_{x}^{1} \frac{4}{3} dydx $$
I guess it was meant to say the connected sum of $g$ copies of $\Bbb{RP}^2$, where $g$ is fixed and at least 1
@LifeOfPai You don't even need integration for this
but it's correct
@LeakyNun did you happen to look at that paper I linked re: the conducting wire?
just name that $N_g$ or something lol
@MikeMiller yeah... but $K^2$ is the case $g=2$... Superfluous at best
16:34
@Semiclassical I opened it in my browser and haven't read it, lol
@LeakyNun Okay and why not?
what`s your idea?
@MikeMiller Half of the time we do, but I think our TA copy-pastes exercises from some other source sometimes.
one basic implication is that both of us were wrong
@LifeOfPai You could just treat them as solids and find their volume, that's what integration is
16:35
@LifeOfPai Plot the regions and split up your integral.
@Semiclassical Well, it'd be great if you could summarize it
on the one hand, the conducting wire is neutral in the lab frame.
It is a piecewise defined integral, if you may.
i.e. $n_{eL}=n_{nL}$
16:36
the $-$ is not needed
You right. Thank you !
I suspect this because he sometimes forgets to change certain German words, notably "und" (which should be "and")
eh, depends on whether you're talking about the number density or the charge density.
but fair enough.
...either that, or he actually typos like that.
on the other hand, while you can measure the number density of the nuclei in the lab frame (they're at rest), the number density of the electrons is properly measured in the electron frame.
16:38
@Semiclassical Where did the extra protons come from?
hence accounting for Lorentz transformations we conclude $n_{eL}=\gamma n_{eE}$ and $n_{nE}=\gamma n_{nL}$
@MikeMiller What's funny?
@Semiclassical of accord.
I mean, "agreed"
and therefore the net charge density in the electron frame is $n_{nE}-n_{eE} = \gamma n_{nL}-\frac{1}{\gamma}n_{eL}=(\gamma -\frac{1}{\gamma})n_{nL}>0$
so yeah, there's a net positive charge in the electron frame.
which is weird to me
@LeakyNun that`s my answer:
16:42
@Semiclassical why?
Why is it weird to me?
@Semiclassical Yes
Wrong intuition, I guess.
I mean, it's charge conservation not charge invariance
Wait, I thought $\gamma-\frac1\gamma<0$
i'm in bed crippled by indecision about what to do today
16:43
$\gamma=1/\sqrt{1-v^2/c^2}$
Then isn't $n_{eL}=\frac1\gamma n_{eE}$?
@LeakyNun $$f_X(x)=\begin{cases}
& 1/3 \text{ if } 0\leq x\leq X \\
& 2/3 \text{ if } X\leq x\leq 1 \\
& 0 \text{ else}
\end{cases}$$
It`s looks okay ?
@LifeOfPai Not really.
well, $\gamma>1$ for $c>v>0$
@Semiclassical well, the electrons are moving, so $n_{eL}<n_{eE}$, right?
16:45
@LeakyNun :( So I didnt understend something...
@LifeOfPai So it's in terms of $x$, right
eh, you're right. so i wrote the above relations for the densities backwards
so it's actually $\int_{-\infty}^\infty f(x,y) \ \mathrm dy$ right?
so yeah, should be $(\frac1{\gamma}-\gamma)n_{nL}$ for the net charge density
16:47
which is negative, so there's a net negative charge density
main point is just that the wire is charged in the electron's reference frame but not the lab frame.
So why it`s dont looks good ? @LeakyNun
@LifeOfPai Because it should not be a constant
@LifeOfPai Try writing the dividing point in terms of $x$
But $f_{x,y}$ a constant
So we are finding the total mass in terms of $x$
which means we look vertically
@Semiclassical guess where the charge went
Charge is conserved
@LeakyNun$$\int_{0}^{1}\frac{2}{3} dy, \int_{0}^{1}\frac{4}{3} dy$$
16:51
but only under a closed system
welllll
conservation applies to a given reference frame
to say it's the same in different reference frames would be to say it's invariant
@LifeOfPai $f_{\chi}(x)=\int_0^{1-y}\frac23\mathrm dy+\int_{1-y}^1\frac43\mathrm dy$
and that's a different matter.
Alright
charge is still invariant
The positive charge went to itself.
if you mean charge density---no, it's not. what's invariant is the 4-current.
In special and general relativity, the four-current is the four-dimensional analogue of the electric current density, which is used in the geometric context of four-dimensional spacetime, rather than three-dimensional space and time separately. Mathematically it is a four-vector, and is Lorentz covariant. Analogously, it is possible to have any form of "current density", meaning the flow of a quantity per unit time per unit area, see current density for more on this quantity. This article uses the summation convention for indices, see covariance and contravariance of vectors for background on raised...
16:53
@Semiclassical I do not understand.
It's like saying that energy is conserved, so the energy of a system is invariant under Lorentz transformations.
But it's not. What's invariant is $E^2-p^2 c^2$.
What is four-current?
@LifeOfPai Do you get it?
I shouldn't have said the four-current was invariant, btw. Covariant, rather.
Yes, Thank you. try to understend
The $y$ is a dummy variable.
It represents trying to sum every point on the vertical line we are looking at (a bit inaccurate)
16:57
anyways, the four-current is defined as $(c\rho,\mathbf{j})$
It's like a line transect, if you have studied biology
@Semiclassical More symbols please
mmkay.
where $\rho$ is the charge density and $\mathbf{j}$ is the current density
And what does invariant mean? Its magnitude?
@Semiclassical Sorry, I'll continue tomorrow.
its magnitude in the sense of $\sqrt{(\rho c)^2-\mathbf{j}^2}$, yeah
@LeakyNun I think your domain need to be $$\int_{0}^{1-x}\frac{2}{3} dy + \int_{1-x}^{1}\frac{4}{3} dy$$
16:59
bye
@LifeOfPai Yes
sorry
so you understand it now
and you can even correct my mistake
bye
Yes Thank u!
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