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4:00 PM
@Astyx Let's take a function not defined at 2 $v= 2/(t-2)$ where t is time and v is instantaneous velocity
How will I find the velocity at 2nd second @Astyx?
 
This is not a physical phenomenon since it's not bounded
(it's not even defined at 2)
 
@Astyx What does "not bounded" mean?
 
Hence the velocity can't be defined
It means that it goes to $\pm \infty$
 
@Astyx Is that the case with all indeterminate functions?
But we solve those using different methods like L Hospital Rule, Rationalization, etc
 
the more general case of not defined can be something akin to having a gap in the function. No physical motion allows this and we never saw a classical object discontinously jump from one place to other or vanishing
 
4:06 PM
Could you once again give an example ? I'm not sure I understand what you mean
In physics ${x\over x} = 1$ if that's the question
(in maths too, most of the time)
 
@Astyx I would like you to give me an example in which we use calculus to determine velocity at a particular second. I can't think of one currrently
Alright see it this way:
We have a curve which shows velocity as a function of time
 
Don't we always use calculus to compute velocity ?
 
AT a particular point the curve is not defined, it has a gap.
 
What kind of gap ?
 
SO yes, velocity should be not defined
However, using L Hospital rule, rationalisation, factorisation, I can arrive at a limiting value..and I would consider that as velocity. But that's wrong because velocity should simply be not defined.
 
4:10 PM
Hi, a quick question: In this blog post about the spectral theorem by terrence tao in exercises 16 and 17 the symbol $\ll$ is used to compare eg $\|\mu_{f,g}\|_{TV}\ll \|f\|\,\|g\|$. Apprently $\ll$ is a weaker notion than $\leq$, what does $\ll$ stand for in this context?
 
@Astyx Oh. Those circular gaps in curves when it's not defined at a point. I am sure you have seen them.
 
Physical signals are always defined and continuous everywhere (theorically)
Either the function can be extended to a continuous function
Or it can't and then talking about velocity is nonsense
 
@Astyx Ok, so that implies that a limiting value is always the correct, accurate value of instantaneous value at a point?
 
hi chat
 
Probably, If I understand what you mean by that
Hi Semi
What's up ?
 
4:13 PM
Now @Astyx that works for physics. But I want to know why methods to remove indeterminacy work in Mathematics.
 
@s.harp The only use I ever saw for that notation is $a_n\ll b_n \iff a_n = o(b_n)$
 
(I mean that in physics there's no case of indeterminacy so it's alright. However in maths I am allowed to remove indeterminacy. Why/How do such methods work?)
 
@Astyx this doesn't make sense here, since on the left and on the right one has positive real numbers, the use of this symbol is really confusing me!
 
Yeah I figured it didn't, I doubt I can help though :/
@Abcd Sorry for keeping on asking, but could you give a concrete example of a situation where this isn't clear for you ?
 
Always remember to not conflate the limit of something with the function value itself. The limit can tend towards some value, but the point can remain undefined. In physics, velocity is a derivative of displacement and since we never have any experimental records of things suddenly vanishing and appearing before moving, we tend to treat velocity as continuous
 
4:20 PM
@Astyx Anyway, I framed my question differently. I hope it would be easy to answer for you > In physics, the limiting/approaching values lead us to the actual values. however, in mathematics, limiting values always lead us to approaching values only, not to the exact value at a point.
@Secret Please see ^. Am I right?
 
yes, that's what continuous means, the limit agrees with the function value
In physics, discontinuous functions related to motions are not as common compared to continuous functions. In fact, they are often assumed to be smooth
and I never heard of any case where a velocity can be discontinuous as even if you have infinite acceleration, the best you can do is making a cusp on your velocity function
 
Eh, I have a stupid question. How do you enjoy formulas? I'm finishing my degree in computer science and I really enjoy the theoretical side of it. However with formulas I'm much worse than with worded reasoning and its holding me back.
 
@Secret Thanks a ton. You understood exactly what I was trying to ask!
 
Motion can be modeled using discontinuous functions, but it's understood that such a model is only an approximation of reality.
 
Isn't velocity just a derivative ? If you take pathological functions such as $x^2\cos({1\over x})$ ?
Or even worse, $x^2\cos({1\over x^2})$
 
4:27 PM
For me, some formulae have algebraic patterns that 1) make pretty pictures, 2) form nice relations that connect many other related formula together 3) the meaning of each symbol in the formula and how they go together explains how it can describe a theory in a concise manner
 
Sometimes the approximation matters (i.e. can be measured experimentally) and sometimes it doesn't
 
@Astyx o/
 
\o
Comment se sont passés tes partiels ?
 
[Me today in chemistry: ] The orbital calculations are finally working: To accidentally celebrate this, I read 3 journal articles in 2 hours, while sending 20+ calculations to the computing cluster
(though to be fair, each article has max of 6 pages)
 
@Astyx Ca dépend :P quid des oraux ?
 
4:31 PM
Les oraux sont finis, c'est ce qui compte
On verra les résultats quand ils seront publié, pas de spéculation d'ici là
 
I forget. Are there any people who frequent chat who are serious probabilists?
 
@Secret that answers why one should find them useful and beautiful. however do you actually think about the 'meaning' of every formula you come across or do you just work with them formally?
 
I'm trying to read up on large deviations theory.
Formulas are like sentences. Some are elegant and satisfying; others are mundane and tedious.
 
@Semiclassical There is SoumyoB unless I'm mistaken
 
4:34 PM
hmm, okay
I should perhaps look up Secret's list :P
 
Hey everyone!
 
Hi Dami
What's up ?
 
@Semiclassical very good point
 
Not too much, how about you?
 
(I'm trying to read up on large deviations theory, for context.)
 
4:37 PM
Finished my exams, or most of them at least
 
Nice!
@Semi that sounds neat
 
@Hippalectryon hey! How is it going?
 
do you manipulate formulas in your head or on paper? I do all the thinking in my head and write things down after that. however that doesn't really work with complicated formulas. but looking at them on paper doesnt seem to work for me either
 
@Waiting Great :-) currently learning Japanese in my free time
 
Depends what I'm doing.
 
4:39 PM
@Hippalectryon hehe. No more math? That's sad. :-)
 
@Waiting I haven't stopped maths :D just starting new things
 
@Hippalectryon :D Okay!
 
@Semiclassical ok, a more practical question: how do I build up my skills with formulas the best? Just working through a hard book with lots of formulas in it?
 
Ehhh. I'd debate that a bit.
The task is to be able to use formulas.
 
(or to prove them)
 
4:42 PM
What do you mean by using?
 
(:P)
 
I am mostly interested in proving formulas I think
 
Well, going back to what I said about language
If you try to read a book in another language, you may eventually pick up on what's going on if you've got a good enough dictionary and patience
But you probably won't have learned how to communicate in that language
For that there's not much substitute for actually working with other people
(Math is a bit easier in that regard, to be sure, given how 'mechanical' the rules of algebra can be.)
 
But with formulas I'd think it would be enough to just think about them for a long time!
 
Depends on the formula, heh.
 
4:45 PM
I mean, what are your ends?
 
I am exaggerating somewhat, to be sure.
 
I want to do science!
I want to understand and work on Information Theory for example
 
Hmm, well to be sure, are you thinking of formulae in a given context, like math, or just in general? If, for example, you see mathematical formulae as more of a means to the end of science, knowing how they're proven is sorta one of those things which is good on general principle and can help you understand something about the nature of the things that use it
But becomes more of a, oh I guess knowing this or that is cool and maybe useful
 
Okay, this is a bit annoying: I'm looking at a problem in a certain book, and it contains the following: "Hint: Theorem VI.5.8."
 
@Fabian did you study in Heidelberg in the past?
 
4:49 PM
This is a problem from chapter IV.
 
(Unlike a mathematician, for whom the proof is the end)
 
@s.harp No! sorry
 
@Semi that's just annoying
 
yep
To be fair, the first half of the book is more physical models and the latter is mathematical techniques, I think
and chapter 6 happens to land in the second half.
 
But yeah @Fabian, in this case you'd spend less time thinking of the formula and more time thinking of the contexts in which the formula comes up (which, to be fair, can often provide some insight into the formula)
On the other hand, if you also take math as an end in itself, you definitely want to know how they're proven, so while you may additionally think about contexts in which some formula comes up, you also want to think of the formula on its own terms and why it's true
 
4:52 PM
hah, and when I look it up it's a fact that I actually understand. So that's...nice?
 
@Daminark I think you have misunderstood me a little bit, to verify the correctness of a proof is the absolute minimum I would demand from myself. Its about feeling like I could have come up with them myself. to see the intuiton that binds together a group of theorems
 
Speaking of formulae, this book is so formula-heavy that it's hard for me to read.
 
Hi what's happening
 
Entropy is irreversibly increasing @Akiva
Appart from that, not much
 
sometimes entropy decreases, indeed you have $\langle e^{- \Delta S}\rangle =1$, which is impossible if $\Delta S>0$ always.
 
4:54 PM
Yeah, but that's when you give entropy to another system
As a whole it can only increase
 
> 3) the meaning of each symbol in the formula and how they go together explains how it can describe a theory in a concise manner
 
@Fabian Do keep in mind that there is a difference between knowing that a proof is correct and being able to see how one could come up with it if you didn't already know it
 
and for the indispensible ones, how they change the world
 
Are we discussing philosophy of math learning? Or something?
 
I don't even know now.
 
4:56 PM
@Semi
1) Merp at so many formulae
2) Why didn't they give you the mathematical techniques first?
 
Good question.
 
its a discussion for me! I dont like formulas, but I think thats a stupid state of mind
 
I don't really get the organization of this book.
 
I mean, so what do you have in mind when you say "formulas"?
 
What book
 
4:57 PM
Lemme find on Google books
 
Like, if you're thinking about some very crunchy formula to compute something, I mean hell I tend not to be terribly fond of those myself
 
@FabianGerhardt Some of these have easy or graphical manipulations that once get used to them, you can mentally rotate the formula, so to speak, but generally I tend to be better at working on paper because then I see where I am going. To me, using a formula is like driving around in mathematical space and you are heading somewhere
 
one example. why does e^ix go in a circle? approach number 1: split the sum defining e in to halfs sin and cos respectively. approach number 2: take the derivative of e^ix, its ie^ix, i something turns it by 90 degrees, the slope always is the tangent of a circle!
 
(I've got access to pdf copies of the chapters because my uni has a subscription with SpringerLink)
Full disclosure, I'm looking for a very specific part of it, which it leaves to the problems
Hence I find myself staring at this page: books.google.com/…
 
I kinda like this way of thinking of it: $|e^{ix}(w-z)|=|w-z|$, which means multiplication by $e^{ix}$ is an isometry that fixes the origin - it's a rotation. (Cont'd)
(Well it could be a rotation but trying it on $1$ and $i$ rules that out)
 
5:01 PM
I guess 'formula-heavy' isn't the right descriptor, though. More just very densely written.
 
There are some occassions I don't like formulas though, such as how most integrations and their substitutions seemed to come out at nowhere. This is the reason I started the Integral Project, in order to allow me to be able to appreciate these formulae
 
@FabianGerhardt because $|e^{ix}| = |\cos(x)+i\sin(x)| = \cos^2(x)+\sin^2(x) = 1$
(Argand plane)
 
More generally, I don't like a formula if I don't understand what it is trying to say
 
Thus, if you trace the function $x\mapsto e^{ix}$, you're essentially multiplying $1$ by $e^{i\epsilon}$ many times, or slowly rotating $1$ at a constant speed.
 
@LeakyNun yes thats approach number 1 I outlined
 
5:02 PM
Sorry I'll need to cut this short, I gotta go now, but see you!
 
@FabianGerhardt right
 
This gives a circle. And it has unit speed, because $e^{ix}\approx1+ix$ when $x$ is small.
 
connecting maths to physics?
 
But compared to something else, me being annoyed by some confusing formulae is basically miniscale
 
> Well it could be a *reflection by trying it on $1$ and $i$ rules that out
 
5:04 PM
@AkivaWeinberger I don't understand what you are saying, but that seems like exactly the thing I'd like, some abstract definitions helping one to conceptually grasp the topic
 
^Correcting a typo from a few comments up
 
...oh this bastard.
 
Who what why
(when where how)
(whence, and whither)
 
in the problem, he indicates [Ellis (1981)]
suggesting that the reader can look that up if they want
But if you go to the book's bibliography:
 
It's in a foreign language?
 
5:05 PM
Worse.
R. S. ELLIS (1981). Large deviations and other limit theorems for a class of dependent random variables with applications to statistical mechanics. Univ. of Massachusetts preprint (unpublished).
 
Oh shit
Lol
 
I should also point out that this is Ellis's own book
 
O yeah, I hate these "unpublished" bibliography items. I just encountered one in one of the landmark papers of the PhD field I am working in
and it basically introduce a gap on whatever their analysis is
 
@Astyx no, it holds for closed systems see here en.wikipedia.org/wiki/Fluctuation_theorem
 
5:08 PM
It was a preprint, so presumably it was available somehow
 
Hi @Semi
 
hi @PVAL-inactive
I'm ranting about 'unpublished' entries in a bibliography.
 
As of now, I have yet to locate that paper and thus explain the fate of those methane complexes in the analysis of the first landmark paper in the series
 
Google Scholar maybe?
 
What's funny is that one of the papers which cites Ellis 1981 (indicating that another's papers results rest on a theorem in that unpublished manuscript) indicates in the bibliography that it's "apparently a preliminary version of Ellis
(1985)"
 
5:14 PM
How do you feel about a "Personal correspondence" citation?
 
...at which point I look at what Ellis 1985 is, and realize it's the book I started with.
aaaaagggghhhh
 
@s.harp equally WTF, it is even harder as you literally need to know the person (and provided he/she still remember back then what they are doing) to get that missing info
 
Mostly I find it annoying that people cite that
 
IT is less WTF if it is not a theorem though, but just some light comments
 
It's definitely necessary to point out when someone provided a proof you use through a personal correspondence.
This happens a lot.
 
5:21 PM
Sure, that's fine.
That's closer to an acknowledgement, though.
 
Hopefully you write proof out though.
 
Hmm I see...
Btw is this Ellis guy still living?
 
I've seen it written as an acknowledgement when the proof is thought to be folklore.
 
cause if an author passed away, I don't think it will be possible to get to the content of these unpublished references
something that often (insert word) me when I read papers in the 1950s
 
If the proof is essentially known to be due to John Doe and John Doe tells you the proof and you reproduce it, you better not claim it as a result (or claim it as folklore).
 
5:26 PM
No clue. @Secret
And it's not that big of a deal yet.
 
That's true
 
5:40 PM
hello everyone
 
5:51 PM
So it's an open problem then
No known proof or disproof exists
 
@Semiclassical is it Ellis from Hawking and Ellis?
 
nah.
It's a mathematical stat mech book, not particle physics.
 
@TedShifrin Do you know something about the classification of Del Pezzo manifolds (Fano manifolds of coindex 2, i.e. Fano index n-1 where n is the complex dimension)? I am interested to know how many there are in dimension 5.
 
I wonder if anyone has ever cited Fermat's margin
 
5:57 PM
@AkivaWeinberger Seems like a likely thing to cite for those cranks that claim elementary proofs
 
Well certainly the statement of the conjecture was first contained within a margin.
So really anyone citing his work for the statement of the conjecture was citing a margin.
 
> There exists no $n>2$ for which the Diophantine equation $x^n+y^n=z^n$ has positive integer solutions [Fermat (c. 1637)]
 
(non-zero integer solutions)
 
Same thing
 
some times I like to be pedantic and pretend its being fundamental
 
6:01 PM
nvm I just proved the weaker version from the stronger version in my head
nice scam
 
[Random topology] $$[0,1) \times \omega_2$$
 
Someone is trying to incite me to insult them on main.
I must resist.
 
> P. FERMAT (c. 1637). Arithmetica (personal copy)
How would you even write that citation
The above looks wrong
 
@PVAL how does that happen
 
@PVAL-inactive: Why don't you stand by what you wrote? — gary 8 mins ago
@s.harp
 
6:03 PM
Reminds me of this great bit from Who's Line Is It Anyway?, where the prompt was "things that'll start a fight"
 
[Random infinity] Unchecked claim: The smallest unit of a set of size continuum (i.e. $\mathfrak{c}$) is the interval
 
and one of them gets on stage and offers, "Wanna start a fight?"
 
lol, that sounds pretty good
 
I have a couple good things to say in my head already.
 
"Your thesis work was a triviality."
 
6:04 PM
But they are all terribly mean.
 
[Trick question] There is no map $f: [0,1) \mapsto [0,1)$ which is bijective
 
I dunno I don't think you can beat that
 
I'll beat you
 
@Secret $f:x \mapsto x$ is surely bijective
 
On a related note,
 
6:06 PM
@Secret what unit, is the interview what?
 
When talking to a kid at a park, the correct phrasing is "I will get to the top of the slide before you" rather than "I will beat you up"
 
[Answer to trick question] I have no idea how will one wrote in symbols the half open interval of cardinality $\aleph_2$
 
@Secret how is it cardinality $\aleph_2$?
 
because one of the interval is constructed by picking all surreals of birthday < (forgot number) between 0 and 1
 
@Secret That does not prove it to be of cardinality $\aleph_2$
 
6:09 PM
my typo: interview > interval
 
ah yes, that is not a sufficient argument. To be sufficient, I need to be able to map it to $\aleph_2$ bijectively
 
@TobiasKildetoft you were right
 
but anyway, how does one wrote an interval in the surreals so that the cardinality is obvious?
 
@Secret Since we cannot know how large that is, I doubt you will succeed
@Liad About what?
 
@TobiasKildetoft remember the question about $f:X\to X$
 
6:11 PM
@Liad Yeah, but I don't remember making any claims about it
 
say: I want to pick relevant subset of surreals between 0 and 1 to construct an open interval of cardinality $\aleph_2$
 
@Secret Without starting with a set of that cardinality, you have no chance
 
@TobiasKildetoft you did .. you said we should repeatedly apply $f$
 
@Liad Ahh
@Secret You can probably easily find a subset of same cardinality as the powerset of the reals though
 
@TobiasKildetoft so $K_i = f \ ^ {i} (X)$ works because it has the finite intersection property the intersection is nonempty and it is the desired set
 
6:14 PM
@Liad I forgot the finite intersection version of compactness
 
@LeakyNun Well, I am thinking about that real induction link seen in the main, whether we can do everything of size continuum by considering it as union of intervals
 
@TobiasKildetoft and yet you solved it :P nice
 
@Liad My idea was originally based on the mistaken assumption that the space would be Noetherian, which is obviously need not be
 
i have no idea what is Noetherian
 
111
Q: Induction on Real Numbers

BajuOne of my Fellows asked me whether total induction is applicable to real numbers, too ( or at least all real numbers ≥ 0) . We only used that for natural numbers so far. Of course you have to change some things in the inductive step, when you want to use it on real numbers. I guess that using i...

This link
One thing I am interested in is how to think about cardinals more than continuum. I know I can use bijective maps to compare between them (and do some cardinal arithmetic), but I am not sure if something more concrete can be said about them such as their usual topologies
 
6:17 PM
@Liad That any chain of closed subsets stabilizes
 
Could someone explain the differentiation of $1+ln^3x$ w.r.t. x to me? Research effort: Search and tried to understand from the steps displayed by derivative-calculator.net and tried to apply chain rule but I don't think it's significant here.
 
is it $(\ln x)^3$ or $\ln\ln\ln x$?
 
@Secret I don't know. I am not well acquainted with $ln$
 
@Secret It is almost never the composition
 
I think the answer should be $3ln^2x$
but answer given is: $(3ln^2x)/x$
 
6:21 PM
close, but you miss the derivative of ln x (remember chain rule) this is why you have the 1/x term
 
@Secret so it's $(lnx)^3$
 
@Abcd $\dfrac{\mathrm d}{\mathrm dx} (1 + (\ln x)^3)$
$= \dfrac{\mathrm d}{\mathrm dx} (\ln x)^3$
$= \left[\dfrac{\mathrm d}{\mathrm d\ln x} (\ln x)^3\right] \dfrac{\mathrm d \ln x}{\mathrm dx}$
$= \left[3(\ln x)^2\right] \frac1x$
 
@LeakyNun Yes, thanks, understood.
 
I've tried to read that. Didn't get far.
 
6:34 PM
I need to revise the topology of the long line in order to deal with this:
$$\omega_2\times [0,1)$$
 
Deal with what about it? make it a long line of sorts?
 
@Secret what is $\omega_2$ ?
 
The second uncountable ordinal, which has cardinality $\aleph_2$
Paul: I am interested in analysing its topology. The natural topology should also be the order topology like the long line
 
what does the long line have to do with it?
 
thus the long line might give me some ideas on how to approach the investigation
 
6:44 PM
I am not really seeing the connection, or why you would think that I guess. It seems the product would be easier topologically to study. Maybe this is part of some other conversation I missed
 
The long line is $\omega_1 \times [0,1)$, the above just make it "longer" by using $\omega_2$ instead. If something interesting happens in terms of limit points and other topological things, then it will tell me more about sets of higher cardinality that is not just about their sizes
 
I don't think that is the long line, it should be a quotient of $\omega_2 \times [0,1)$
$\omega \times [0,1)$ is not the "normal length line", it isn't even connected (the above isn't connected either)
or maybe you had some implied long line topology, instead of product topology, which would make sense in this context I guess
 
$\omega_1$ is the first uncountable ordinal, and I took the long line (actually it should be called the closed long ray) definition from wikipedia en.wikipedia.org/wiki/Long_line_(topology)
 
Hm. Suppose $X$ is any set and $f:X\to X$ is a function. Let $Y=\{x\in X:\exists n,f^n(x)=x\}$ be the set of elements of $x$ that get sent on loops by repeated applications of $f$.
Clearly, $f(Y)=Y$.
Does $Y=\bigcap_nf^n(X)$?
 
Reminds me of a question I have answered, although it might not be that... let me look
 
6:53 PM
Hm… well, $Y\subseteq\bigcap_nf^n(X)$ seems apparent enough
 
So $Y$ is the eventually-periodic subset of $X$.
 
Oh, no, it's false
 
The thing is I don't think so, you would need x to be in each applicatio
 
@AkivaWeinberger It is possible for $Y$ to be empty while that intersection is all of $X$
 
$X=\Bbb Z$, $~f:x\mapsto x+1$
 
6:54 PM
exactly
 
Hm so how do I modify that
How about
oh wait never mind
 
You could make $F^n$ the union of previous $f^k$
Yah the question isn't really the same, but it does involve a lot of intersections and finite orbits and things like that
 
@Mike Do you know how to do this?
1
Q: Homotopy type of a sphere

SigurLet $X$ be a CW-complex of finite dimension. Suppose that $\pi_k(S^n)$ is isomorphic to $\pi_k(X)$ for all $k\geq 0$ and $n>1$. Certainly, $\dim X\geq n$. It is easy to show that $X$ has homotopy type of $S^n$ provided $\dim X \leq n+1$. Question: is it true for any $X$ of finite dimension?...

 

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