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3:00 AM
All points of that form
In any case, a geodesic on this.
The helix is a limiting case in the same way a line is the limiting case of a circle
 
you mean infinite radie
 
Yeah. Leave the last two coordinates alone, shift and grow the circle defined by the first two coordinates
in words
 
but a circle is not the same kind of limiting case of a helix
What I meant by not a regular torus is that it has the same topology but not the same geometry
 
Ah.
Right, the usual torus in R^3 does not have constant zero Gaussian curvature
 
only cylinder
ok need to go...
 
3:05 AM
Me too. Bye!
 
hi @TedShifrin
hi everybody
 
3:22 AM
Doesn't Euclidean Geometry work upon the surface of a torus? It's just a thought...
 
1
Q: Fourier Transform: If $H(\alpha)=e^{-t\alpha^{2}}F(\alpha)$, what is $h(x)$?

Jessy CatI am trying to solve the following problem from my textbook: If $f(x) \in L^{2}(-\infty, \infty)$ has Fourier transform $F(\alpha)$, then what is the function of $x$ whose transform is the function $H(\alpha)=e^{-t\alpha ^{2}}F(\alpha)$? ($t$ is a positive real constant). The answer giv...

I'm having a horrible time with Fourier transforms. I hate that I have to teach myself pretty much everything in this class...
 
@JessyCat I'm using a book by Vretblad and it's very accessible
 
Unfortunately, I doubt I'll get a chance to get my hands on a copy before my final exam.
 
it's for free online as a pdf
 
oo.
 
3:32 AM
Also, are you actually a cat
 
How many cats usually come in here and strike up a conversation?
 
at least 2 others
 
You might be able to help with that question I posted a link to up there. If it makes you more amenable to do it, I'll be a cat. meows
Well, there goes the neighborhood.
 
@GFauxPas he is obviously not a cat. hes a human.
 
I'm still working on Laplace transforms
 
3:37 AM
for what class?
 
@TheGreatDuck and you are obviously not a duck. Although if you look like a duck and quack like a duck...
 
self study
 
@GFauxPas what subject
 
<-- taking a PDE course with the flakiest professor ever.
 
@JessyCat Are you implying I am a quack, cause to some degree I am.
 
3:38 AM
@TheGreatDuck to be honest, the thought never crossed my mind.
 
@TheGreatDuck Laplace transforms! I found them interesting when studying ODEs but my ODE class only covered them in passing]
 
But you know, cats eat birds...just sayin'.
 
so im going further
 
Also, not a he.
As for how human I am, that's a matter for debate.
 
@GFauxPas know any obscure transforms?
 
3:40 AM
Obscure Laplace transforms, or obscure transforms other than Laplace?
The $\mathcal Z$-transform is the equivalent of the $\mathcal L$-transform for sequences
 
obscure laplace transforms
any regarding floor?
 
The Laplace of $\ln$ is fun to figure out
 
or any interesting/exotic functions that someone in a regular ODE diff eq class would be aware of?
hmm
 
you'll need proofwiki.org/wiki/… if you want to figure it out yourself
 
now that I think about it, we never did cover it.
 
3:43 AM
Because it's a weird one
 
oooh
I remember seeing that one
 
doesn't give you a rational function or a power function
 
it gives you gamma
which is the real value extension of factorial
(might also be a product integral)
 
$\mathcal L \{ t^q \}$ gives you gamma of something over something, where $\operatorname{Re} q > -1$.
 
which would make sense
int(ln(x)) = ln(prod(x))
where int and prod are the integral and product integral
 
3:45 AM
Oh I don't know anything about product integrals
 
do you know of product integral?
ooh
 
but $\int \ln x \, \mathrm dx = x \ln x - x + C$
 
you've seen it believe it or not. they just do not tell you.
 
Which is a fun thing to prove
write it as $1 \cdot \ln x$ and integrate by parts
 
remember diff eq of the form: y' + f(x)y = g(x)
 
3:46 AM
I don't remember how to do any ODE's except for linear ones
 
and how you do that weird exponential logarithm integral of f to find the factor to divide by?
O.O
well it is linear
 
like $\dddot{y} - 5 \dot{y} + y - \cos t + \sqrt{t} = 0$
those kinds
 
hi chat
 
I mean, I could reteach myself the others, I'd just need to invest time
hi @Semiclassical
 
3:49 AM
The joy of integrating factors
 
@GFauxPas the right hand side is the product integral of p(t)
 
Why would you need to use product integrals for that
oh yeah but I mean
 
shrugs
 
I don't feel like dealing with "Riemann products"
or however youd define it
 
I tend to prefer doing a general solution + a particular solution
when doing inhomogenous ODEs
 
3:50 AM
someone probably has a good reasoning why the product integral is the integration factor, but I cannot say.
 
@TheGreatDuck You can derive it without -too- much trouble
 
That's the semi-classical way to do it @Semiclassical
 
@Semiclassical I mean just a really simple one-sentence reasoning why the product integral yields it. Atm, it's only good as a memory-tool for me.
 
Oh you mean, you're asking the motivation behind it?
 
3:52 AM
I'm not asking anything.
 
well, you've got the ODE $y'+f(x)y=g(x)$
 
Oh
then I'm not answering anything.
 
you asked why. I just said, Idk.
 
well if ydk idk either
 
product integral? Is that the same as integration by parts?
 
3:52 AM
and said it's probably obvious, but idk.
@Sophie addition is to integral as multiplication is to product integral.
 
No @sophie it's a generalization of the idea of a definite integral to a limit of a "Riemann product" or something like that
 
I think
 
except it's to the power of dx rather than multiplied by dx
 
except that you have to figure out what that means
 
3:53 AM
@GFauxPas what do you mean by that?
I didn't make it up. I read it on wikipedia for two seconds once and remember it cause I got a good memory.
 
"mutliplying by $\mathrm d x$ can't be defined the same way as the multiplication of numbers
you need to figure out how to define it
 
@Null, not, uh, nicotine if that's what you're referring to
 
well, you want to arrange things so that the above ODE is equivalent to $d(W(x)y(x))=g(x)W(x)\,dx$
 
I'm not saying its wrong
I'm just saying it's not obvious what it means
 
@GFauxPas dx comes from delta_x. I'd imagine it's just a restructuring of the riemann sum....
 
3:55 AM
Typically, multiplying by $dx$ is just a notational shorthand
 
raise it to the power in the limit calculation rather than multiplying.
@Semiclassical WRONG. it implies each element is scaled into an infinitely tiny contribution to the sum. Like an additive accumulation.
 
so if $\lim_{\Vert \Delta \Vert}\sum f(x_i) \Delta_i = \int f(x) \, \mathrm dx$,
 
e.g. $f'(x)=\frac{df}{dx}\implies df=f'(x)\,dx$ really means $\int f'(x)\,dx=\int df.$
 
and even that actually needs additional details for it to make sense
 
If you have a specific meaning you want to attach to $dx$, go right ahead.
 
3:57 AM
@Semiclassical that is the meaning of dx.
 
right, what S.C. said. You have to figure out a meaning, and if it makes sense, prove it makes sense.
 
why do I need to prove anything? It's the definition.
XD
 
@KajHansen Are you a bit into fundamental groups and algebraic topology?
 
Not if you're talking differential 1-forms, it's not. @TheGreatDuck
 
Because you want the definition to be consistent with the results you expect
 
3:58 AM
@Semiclassical We're talking about regular integrals on real numbers. Not abstract math on dogs and cats. :p
 
If I say "I define the derivative of a product of functions to be the product of their derivatives", that definition wont be consistent with results that make sense
 
Don't know anything about that @mikeonly; wish I did
 
integrals arent on numbers, they're on functions, or on intervals
 
I really, really wish Ted was here right now. :/
 
hey @KajHansen just want to verify here we consider the $e_i$ as coloumn vector and think of the permutation as coloumns ?
 
3:59 AM
I know a tiny bit of homological algebra. Things like the five lemma. I think that comes up some in that
 
 
@KajHansen Interesting stuff. Thank you anyway. :)
 
@GFauxPas I never said that though. I just said the product integral uses the riemann product where the individual term is raised to the power of delta_x...
 
What's happening? Someone mentioned product integrals?
 
how is that confusing to you?
 
4:00 AM
@TheGreatDuck the riemann sum definition of the integral is hardly trivial
 
@GFauxPas yeah, functions of real numbers.
 
They have them as rows there @Adeek, but columns works fine too
 
for example, if the value of the integral depended on the partition of the interval used in the riemann sum, that would be very bad
 
yeah I see.
 
4:00 AM
@GFauxPas um... it's a simple equation. do you mean to say evaluating it is hard?
 
Because riemann sums are equivalence classes of sums
 
facepalm
 
I'm saying the hard work has been done for you
but don't take it for granted
 
that's an issue of integration theory
 
every time you use the fundamental theorem of calculus you're using the combined efforts of thousands of man hours of mathematicians making sure that you're allowed to do what you're doing
 
4:01 AM
"I'm saying the hard work has been done for you
but don't take it for granted" what work? All I did was tell you the product integral was used to extend factorial and that you use in diff. eq. without realizing it. um... what is the point of this?
@GFauxPas and you're telling me this... why?
 
Because you called the idea simple
 
Well, for one, because I've never heard of the product integral and I've been able to do ODEs via integrating factors just fine.
 
and I didnt like that
 
Last night, I noticed that a post of mine was 1 upvote away from winning me 2 medals. I found an excuse to edit the post (I did legitimately improve it though) knowing that this would bump my post in the "active threads" tab and likely get me the upvote I wanted. Is this abusing the system / frowned upon around here do you (guys) think?
 
The riemann sum equation itself is simple, I mean.
 
4:02 AM
and btw the factorial has an infinite number of extensions, the gamma function is not unique
 
@KajHansen meh
 
and it's simple to see that the riemann sum gives area (or is intended to give area).
at least, in hindsight.
not saying it was not hard to create
 
@arctictern, I figured that might be the response. But I felt really dirty doing it
 
just that it's not hard to understand or learn
 
I've done it a bunch in previous incarnations
 
4:04 AM
heck, multiplication giving area is a miracle
 
it's "not hard to understand or learn" if you're willing to take certain results for granted
 
whoever figured that out deserves a medal.
 
It's a heck of a lot easier to learn calculus than to invent it.
2
 
@GFauxPas um... are you implying that you have to learn the entire derivation of calculus to learn it, lol?
 
no, what I'm saying is
 
4:04 AM
haha, yeah
 
I find this conversation confusing, though.
 
that if your professor says something like the value of the integral doesn't depend on which riemann sum you use among the infinite number of possible rieman sums you can choose
you should think about it rather than accept it at face value
 
The product integral seems like something which is interesting but not really necessary.
 
4:06 AM
when they draw a picture of you cutting up the area into rectangles
 
@Semiclassical Here's an interesting question. Suppose you have a differentiable path on a sphere. Between two sufficiently close points on the sphere, there is a "most efficient" rotation of the sphere that sends the first to the second. If we partition the path into n points and multiply the small rotations together, then take the limit, what is the result? The result is actually the product integral of elements of the rotation group's lie algebra (so, infinitessimal rotations).
 
if they draw the rectangles with equal with
know that they don't have to be
 
my point was merely to make a comment about it existing and this somehow turned into a massive debate about riemann sums
 
@arctictern Hmm, fair.
 
I'm not debating
I'm philosophising
 
4:06 AM
yeah, you are.
facepalm
 
Yeah, that's kinda claptrap.
Philosophizing is argument by its very nature.
 
That's arguable
see what I did there
 
Yes, you demonstrated my point.
 
yes
 
@GFauxPas "that if your professor says something like the value of the integral doesn't depend on which riemann sum you use among the infinite number of possible rieman sums you can choose" if you're professor says that raising e to the power of a sum of natural logarithms is the same as a product are you going to argue with them day in and day out or accept it as something trivial to understand if you just pull the logarithms out?
 
4:08 AM
Duck I thought your avi was the yeti from that skiing game on old windows
 
is there a way to obtain a tight upper bound on $\sum_{h=l+1}^\infty h!^{-n}$? I tried Stirling's approximation but got a very weird sum
 
@GFauxPas lol
 
@GFauxPas umm.... ooook.
i dont even know what yer talking about.
 
not something I ever thought I'd remember again
@Sophie like, how tight?
 
Of course, all of this amounts to just the old standard that $\displaystyle e^x=\lim_{n\to\infty}(1+x/n)^n$
 
4:10 AM
right
 
SkiFree is a computer game created by Chris Pirih and released with the Microsoft Entertainment Pack in 1991. It is a simple game in which the player controls a skier avoiding obstacles on a mountain slope. It is often remembered for its Abominable Snow Monster, which pursues the player after they finish a full run. == Gameplay == The player controls a skier across a white background representing snow on a mountainside. The object of the game is to ski down an endless slope and avoid the obstacles. The game includes three modes: slalom, free style, and tree slalom. In slalom, players ski between...
 
Including the thing arctictern was saying (since the exponential map is what relates Lie algebras to Lie groups)
 
.https://youtu.be/yYDmaexVHic
Pretty dope track right here
 
@arctictern well considering I don't have almost anything, anything asymptotic should do
 
@Sophie That is one painful looking sum.
 
4:11 AM
I've managed to confuse myself on the non-simply connectedness of the rotation of the sphere
 
What's the source?
 
Maybe I'm too tired, since this is something I've already understood in the past
 
@AkivaWeinberger, is the topology on the set of matrices that correspond to rotations?
 
Eugh, that reminds me of Euler angles. Don't remind me of Euler angles.
 
4:12 AM
How do we define matrix topology again?
 
@KajHansen The interesting thing is that one full rotation can't be contracted but two full rotations can be
 
@KajHansen Mn(R) is R^(n^2)
yes, the plate trick
 
Defined by what?
 
@Semiclassical for the sum? I got it from a MSE question. I'm trying to prove $\sum_{h=0}^\infty h!^{-n}$ is transcendental
 
That seems difficult.
 
4:13 AM
I'm going to bury it
 
@KajHansen well, R^(n^2) is a coordinate vector space, so use the dot product. (same as the frobenius norm on Mn(R))
 
(well, except for $n=1$.)
 
or $n=0$
 
@Semiclassical if I give you a coordinate basis can you find a set of euler angles that produce it?
 
if you want the sum to stop making sense
 
4:13 AM
@GFauxPas Eh, not transcendental in that case
 
in general?
 
@Semiclassical who are you talking to? exp(-1) is transcendental
 
infinity is transcendental?
 
infinity isn't a number
 
sorry but it's for something I've been stuck on for a while.
 
4:14 AM
well
 
Ohh I see my mistake
 
depends
 
Couldn't help you @TheGreatDuck
 
(Regarding the plate trick thing)
 
and I must use a coordinate basis and I must use angular rotations
 
4:14 AM
Well, goodnight
 
darn
 
laila tov
 
And wouldn't, frankly. I haven't used euler angles in years and don't want to do them again.
 
@GFauxPas Laila tov ^_^
 
4:15 AM
computing and visualizing homotopy groups of rotation groups don't really involve euler angles
 
that's harsh.
 
Harsh on Euler angles. Nothing to do with you.
 
@arctictern here's the problem really. I have a coordinate basis that represents where I'm moving in space. And I can only rotate some degrees about an axis of rotation. I need to rotate the player to match the coordinate basis
hence I need the euler angles
 
Speaking of exponentials.
The lack of response to this bounty I gave is disappointing: math.stackexchange.com/q/2036252/137524
...and now I notice the comment to the main answer. Welp
 
heh
 
4:18 AM
do people usually browse the "featured" tab? I think it's too discouraging to not even understand most questions
 
sometimes
usually understand a few
 
I do occasionally.
 
i think they are over-hyped
:p
 
lol, I never click on it @Sophie. But I would if I were more knowledgeable. I just know that basically everything I know, lots of other people on here do too.
 
@KajHansen what do you know?
 
4:21 AM
hello everyone
 
answer mine please
 
@Sophie not right now I'm busy.
 
The sum one?
I don't have anything clever to say on that one. Stirling still seems sensible.
 
A broad smattering of undergrad topics @TheGreatDuck, but none in any great depth. Real/complex analysis, combinatorics, linear algebra, abstract algebra (groups/rings/fields/galois), differential geometry, general topology, Ramsey theory, elementary number theory, cryptography, dynamical systems
 
4:25 AM
I'd be more interested if I knew a clever way to represent $\frac{1}{h!^n}$. When $n=1$ that amounts to the reciprocal gamma function, and I know fun stuff for that.
But otherwise I dunno.
 
@Semiclassical I I mean another one. I want solutions to $1+2^2+3^2\dotsb n^2=a^b$ where $a,b,n$ are integers. I have reduced that to solving equations like $x^n-2y^n=1$
 
How do I make the Latex generate in the chat?
 
Oh, Pell's equation stuff? No clue on that.
I haven't done any of that.
@whatwhatwhat See the LaTeX in chat link in the room description.
 
well that's a Pell equation when $n=2$
 
If it's worse than Pell's equation, then I'm definitely not the person to ask
 
4:27 AM
@Semiclassical thanks
 
@AkivaWeinberger Oh. I still have that hydra game running from earlier.
It's up to 28500 heads cut off :)
 
@KajHansen you know way more than I know.
 
Don't worry GreatDuck. I've forgotten most of it ;)
 
by Stirling's I get $\displaystyle\sum_{h=l+1}^\infty \exp\left(nh\ln(h)-nh-\frac{n}{2}\ln(h)\right)$ so if I could get an upper bound for that I'm done. To prove transcendentality I need that to be like $O(l^{-2})$ or somthing
 
I have a question: somewhere, my understanding of chain rule/partial derivatives off. I have a function $f(y(x)+\eta (x) \alpha,y(x)'+\eta (x)',x)$ and I need to take the derivative w.r.t $\alpha$. How do I do this?
 
4:30 AM
@KajHansen um... it was a compliment. You still know way more than me.
 
haha, I know it was....I was trying to be modest. Although I truly have forgotten a lot
 
@whatwhatwhat Is there something you don't understand about my answer and the comment? For example, if $f(u,v,w)=u^2-vw$ would you be able to compute the derivative of $f(p+q\alpha,r+s\alpha^2,t)$ with respect to $\alpha$?
 
Kaj, you're a mathematician?
 
If you count someone who's completed undergrad a "mathematician" @Sophie
I don't have any original work to speak of though
 
@KajHansen that's surprising.
 
4:32 AM
@arctictern yes, but in the past I've been told (by the site and by people) that further comments should go in the chat. So voila, her eI am.
 
@whatwhatwhat We're not to the point of "further comments" but whatevs
 
I pretty much always ignore the "go to chat" warning on MSE posts
 
Usually the convo is almost done anyways
 
usually I'm trying to get the person to stop replying to me and being a jerk.
i gotta go
cya
 
4:35 AM
Have a good one
 
@arctictern Ok so the derivative would be $\frac{\partial f}{\partial \alpha}=2(p+q \alpha )(q) - (2s\alpha)$, right?
 
forgot t at the end of -2sa but yeah
 
Is this equivalent to (using your notation): $\frac{\partial f}{\partial \alpha}=f^{(1,0,0)}q-f^{(0,1,0)}$ ?
Oh right
 
@sophie Found this question on the quartic case: math.stackexchange.com/q/1981082/137524
 
It's equivalent to $$\frac{\partial u}{\partial \alpha}\frac{\partial f}{\partial u}+\frac{\partial v}{\partial \alpha}\frac{\partial f}{\partial v}+\frac{\partial w}{\partial \alpha}\frac{\partial f}{\partial w} $$ or with tuples, $$ u'f^{(1,0,0)}+v'f^{(0,1,0)}+w'f^{(0,0,1)}$$
 
4:39 AM
The answer references a theorem of Thue and a Wikipedia page
 
So do you understand the formula $$\frac{df}{d\alpha}=\frac{\partial (y+\eta(x)\alpha)}{\partial \alpha}f^{(1,0,0)}+\frac{\partial(y'+\eta'(x)\alpha)}{\partial \alpha}f^{(0,1,0)}+\frac{\partial x}{\partial\alpha}f^{(0,0,1)}$$ I wrote in my comment on main?
 
@Semiclassical I proved there are finitely many for any fixed $n>2$
 
Ah. That matches the theorem they mention.
But finitely many doesn't say how many, of course :/
 
and it doesn't help that we don't know anything about the continued fraction of $2^{1/n}$ for any $n>2$
 
Huh. That's kinda weird.
 
4:43 AM
we know literally nothing. I read some posts at MO saying even at research level we know nothing
 
Not entirely surprising, though. Continued fractions are nice for representing solutions to quadratics. No reason they should be nice for solutions to $x^n=2$.
 
there's no a priori reason why continued fractions should be nice for quadratic irrationals
 
uh
real quadratic irrationals have periodic continued fractions.
that's pretty nice.
 
that's very nice. It allows you to find solutions to Pell equations quite easily for example $838721786045180184649^2-397\times42094239791738433660^2=1$ would be very hard to find if you didn't know that
 
hey kaj you know manifold theory ?
@KajHansen
 
4:46 AM
Do you have a reference to those MO posts? Now I'm curious.
 
18
Q: Is there any pattern to the continued fraction of $\sqrt[3]{2}$?

john mangualIs there any pattern to the continued fraction of $\sqrt[3]{2}$ ? Wolfram Alpha returns for cube root of 2: $\sqrt[3]{2}=$ [1; 3, 1, 5, 1, 1, 4, 1, 1, 8, 1, 14, 1, 10, 2, 1, 4, 12, 2, 3, 2, 1, 3, 4, 1, 1, 2, 14, 3, 12, 1, 15, 3, 1, 4, 534, 1, 1, 5, 1, 1, 121, 1, 2, 2, 4, 10, 3, 2, 2, 41, 1...

 
The lack of response to your problem, then, might just be that it's very very hard.
 
that heuristic I wrote in the post has convinced me that a solution is very, very unlikely
 
hmm, Wikipedia has the following in their page on Hermite's problem (which is about continued fractions of cubic irrationals)
>In 2015, for the first time, a periodic representation for any cubic irrational has been provided by means of ternary continued fractions, i.e., the problem of writing cubic irrationals as a periodic sequence of rational or integer numbers has been solved. However, the periodic representation does not derive from an algorithm defined over all real numbers and it is derived only starting from the knowledge of the minimal polynomial of the cubic irrational.
 
wait what. $x^{-n\left(x+\frac{1}{2}\right)}e^{nx}$ has a fixed point under variation of $n$
 
4:55 AM
That'll diverge to infinity or go to zero depending on whether $x^{x+1/2}$ is bigger than $e^x$
 
I'm thinking of that as a function of x and n is a parameter
 
The crossover seems to be $x\approx 2.26924$.
 
@arctictern ok this makes sense. Yes, I think I understand your answer now. Sorry for being so dense.
 
is the point of the solution of $\ln(h)(h+1/2)=h$
 
right.
 
4:58 AM
can we prove that $x^{-n\left(x+\frac{1}{2}\right)}e^{nx}x^{\alpha}$ goes to 0 as $x\to\infty$ for any $\alpha>0$?
 
With $n$ fixed?
 
yes and positive
 
I think so, yes?
x^x grows faster than e^x, seems the essential point.
Equivalently, you want to show that $nx+\alpha\log x-n(x+1/2)\log x\to-\infty$ as $x\to\infty$ when $\alpha>0$
 
I got it with a transformation like $x\to ex$
 
Ah.
The expression I just gave seems to be dominated by $-n x \log x$, so presumably one can show that $x^{-n(x+1/2)}e^{nx}x^\alpha$ is asymptotic to $x^{-n x}$ as $x\to\infty$.
...maybe
 
5:16 AM
For real inner product spaces $V$, we can identify $\Lambda^2(V)\cong\mathfrak{so}(V)$, and if $V$ is oriented with $\dim V=4$ there are canonical subspaces of $\Lambda^2(V)$ of left and right isoclinic rotations (up to scaling). Essentially, $a\wedge b+c\wedge d$ is left isoclinic if the orientation from the ordered basis $\{a,b,c,d\}$ is correct. Apparently if $P$ is tracefree self-adjoint and $x\in \Lambda^2V$ is isoclinic then $Px$ is also isoclinic but opposite-handed.
$P(u\wedge v)$ being $(Pu)\wedge v+u\wedge (Pv)$
Dunno a good way to see this. Maybe use fact self-adjoint implies linear combination of orthogonal projections onto orthogonal subspaces.
 
5:39 AM
best to think of those as the eigenspaces of the Hodge star operator, at which point you're asking to prove the identity $*P+P*=0$, which seems like it should follow straightforwardly from def'ns
 
Random question: Does anyone know if the Pacific Tech Graphing Calculator is actively developed?
I have it—it's *excellent*—but the copy I have hasn't been updated for a retina display. Makes me wonder.
 
Is there a time when one should kinda just reconsider a math-heavy field as a career? I'm 24 and still working on a bachelor's degree (in physics; reasons for the delay involve family, legal, and financial troubles). I now see what they say about how a person's mathematical ability must be well-developed around the age of 23. If not, there's not much hope for developing it going forward. How true is this statement?
I'm might be unlucky in asking this question here because it's highly likely that most people here developed their math skills early on and have built careers out of these abilities.
 
5:58 AM
hey @arctictern
I was wondering why here is $dz_i(\partial/ (\partial z_j) = \delta_{ij}$?
 
Hey I'm back
 
hey kaj
I need your help understanding this
I don't understand how do we get this last two lines
@KajHansen
 
I'm trying to take the expectation of a squared standard normal distribution. Can I narrate my progress and someone'll let me know if I'm going wrong?
 
I'm afraid I can't really help
 
oh ok @KajHansen
 
6:26 AM
@Hatshepsut go ahead
 
6:42 AM
@DHMO Ok here goes
$X ~ N(0,1). EX^2 = \int_-\infty^\infty f_X(x)dx$
f_X(x) = 1/\sqrt(2\pi) e^(-x^2 / 2)
 
well, E(x^2) should be int x^2 f(x) dx
 
right
E X^2 = 1/\sqrt(2\pi) \int x^2 e^(-x^2 / 2)
proceed with integration by parts
u = x^2 , du = 2xdx , dv = e^(-x^2 / 2)
i dont know how to take that antiderivative, but its the main part of the standard normal pdf, so it's gonna end up having an integral from -inf to +inf of $\sqrt{2\pi}$
I mean the antiderivative of dv
I'm not sure if it's legit to use at this point because i'm just supposed to be taking an antiderivative not evaluating it at limits
@DHMO How should I be thinking about that
 
7:39 AM
@Hatshepsut try v = e^(-x^2/2)
 
7:53 AM
@DHMO So if I say dv = x e^(-x^2/2)dx, v = -e^(-x^2/2)
Then uv goes to 0 in the limit
so we just have 1/\sqrt 2pi \int e^(-x^2/2) evaluated from -inf to inf
which is the integral of the standard normal pdf
X
so its 1
which is the answer
 

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