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12:00 AM
Now sythesizing the circuit, time to make some tea
@dmckee IT WORKS
MY PROCESSOR WORKS
MY BABY
MUAHAHAHAHA
TREMBLE IN FEAR MORTALS
 
@BernardoMeurer can it solve this simple problem?
tan(x)=137
 
Not yet
I have about 20 more operations to implement
it also has no floating point
Writing a float ALU is too much work for me right now
 
meanwhile I can't solve an AC circuit ;_;
 
@BernardoMeurer ::chuckles::
 
oh come on why is the resistor phase shifted!?
 
12:12 AM
@dmckee I still have to write in machine code though, lol
but the decoding works, so I just need to write an assembler
::points gun at head::
 
@EmilioPisanty In case you really do like measure theory: Let $(\Omega,\Sigma,\mu)$ be a measure space, and $P:\Sigma\to\Sigma$ an "equimeasure transformation," that is, $\mu(PB)=\mu(B)$ for each $B\in\Sigma$. Consider the linear operator $T:L^2(\Omega)\to L^2(\Omega)$ given by $(Tf)(x)=f(Px)$, $f\in L^2(\Omega)$. Then, using some measure theory + functional analysis, we may apply the "mean ergodic theorem" which says, among other things, that $L^2(\Omega)=\overline{R(I-T)}\oplus N(I-T)$.
It also says that for any $f\in L^2(\Omega)$, $$\lim_{n\to\infty}\frac{1}{n}\sum_{m=1}^n T^mf=f_0\in L^2(\Omega)$$ exists and $Tf_0=f_0$.
That is, we can average out $T$ and obtain a fixed point.
 
12:28 AM
::imagines @BernardoMeurer programming in octal just with the front switches of a PDP-8::
 
@JaimeGallego Have more respect, I would use a PDP-11 :P
 
where did @BenNiehoff go, anyway
 
Why @BernardoMeurer
We could stick with Holleritz tabulators and not these newfangled programmable gizmos anyway
Back in the good ol' days, computers were still people!
 
12:53 AM
@BernardoMeurer halp
 
@JaimeGallego Because I like them better :P
@0celouvsky What's up?
 
@BernardoMeurer I have a capacitor and inductor hooked up in series to an AC source
I needs to find out the frequency I need so that it's like an open circuit
for a short circuit I set the combined impedance to zero
what do I do for an open circuit?
$Z=\infty$?
it won't get to $Z=\infty$
 
I have no clue :/
I only take circuits next semester
 
ayy
 
Anonymous
@YashasSamaga LOL :-P So many people made the same mistake :-D...Anyhow, the chemistry paper was bogus, physics was good and maths was lengthy...I was so bored while solving the chem paper that I almost slept
 
Anonymous
1:01 AM
@YashasSamaga What? You gave the B Arch paper too? Going to be an architect now? :-P
 
Anonymous
I am getting around 250, how much are you getting?
 
@0celouvsky If it's series, then the frequency can go either to zero or to infinity. f=0 means the capacitor won't let current pass. Conversely, the inductor does not like f->infinity and "chokes" it.
 
@JaimeGallego but what impedance corresponds to an "open circuit" here
Clearly zero impedance is the short circuit, it acts just like a wire
So I solve Z(omega)=0
But what is Z supposed to be for the open circuit?
infinity? my only option is omega = infinity in that case
and that doesn't make much sense
or zero, but thats not very good either
 
Why doesn't it make much sense?
 
what the hell is omega = infinity supposed to be
that's definitely not physical
and the whole AC analysis fails in the omega -> 0 limit
I mean, I should be able to run DC current through the setup
So shouldn't act like an open circuit
 
1:10 AM
No, capacitors block DC
 
@JaimeGallego ah. because i = Cv'
thanks
 
1:50 AM
@Secret So I've been thinking about that proof (which I took from a functional analysis book) and I'm not happy with it. I read another one and I don't like it either. I'm considering writing my own, from scratch.
The difficulty is due to there being two topologies floating about.
It's very difficult to keep track what is compact/continuous in which topology.
 
2:11 AM
So anyway
Are manifolds really locally euclidian
 
@Secret My approach is as follows: 1. If two metric topologies on a set have the same convergent sequences, they are equal. 2. Any norm topology on $\Bbb R^n$ has the same convergent sequences as the usual topology. 3. If two norms generate the same topology, they are equivalent.
1. Is more or less clear, and we already talked about it I believe.
2. Is just the statement that weak convergence and strong convergence are equivalent in finite dimensions, and I can prove that pretty easily.
3. Is well known in arbitrary normed vector spaces, so it should not be a problem to prove.
@Slereah what does that mean?
are you having trouble sleeping again?
 
for a small enough neighbourhood, do we have $$\int_\gamma d^nx \sqrt{\langle \gamma'(\lambda), \gamma'(\lambda)\rangle} = |\gamma(\lambda_1) - \gamma(\lambda_0)|$$
For a geodesic $\gamma$
$|\gamma(\lambda_1) - \gamma(\lambda_0)| + \mathcal{O}(\mathfrak{something})$
I'm guessing depending on the size of the neighbourghood
it sounds reasonable enough but who knows
 
jesus christ I got 90A
that's probably wrong, crap
 
very good grade
 
90 amperes
@Slereah oh, uh
there's an MSE post on this
 
2:19 AM
That was why I was wondering about analytic manifolds 'cause that would make it easier to prove
possibly
 
let's see if i favorited it
0
A: Asymptotic behaviour of the length of a curve .

John MaLet $\delta >0$ be small so that $\gamma$ lies completely in the normal coordinate centered at $y$. In this normal coordinate, we write $$\gamma(0) = 0, \ \ \ g_{ij}(x) = \delta_{ij} + O(|x|^2).$$ Write $v = \dot\gamma(0)$. Then we have $$ \gamma (t) = tv + O(t^2), \ \ \ \dot\gamma = v+ O(t)$...

 
The $g_{ij} = \delta_{ij} + \mathcal O(|x|^2)$ is quite mysterious
is that a generic feature of normal neighs?
(I am a horse now)
 
Yeah it is
Because $\partial g(0)=0$
 
ic
 
Note the common confusion here
$g=\delta+\mathcal O(x^2)$ is not saying $g$ is analytic
Taylor's formula holds because $g$ is $C^\infty$
But $g$ doesn't have to equal the full power series
 
2:26 AM
Yeah that I remember
 
it's clean
no fuss
straight to the point
has a cute horse
 
that seems like a book for insane people
 
great design for the cover, though
just making wormholes at the beach
 
that's a woman, right?
or is it a giraffe
 
2:38 AM
the book does not specify, but I assume, yes
 
2:53 AM
yo what's $\int_0^L \sin^2(n\pi x/L)\,dx$
 
What's going on in here?
@0celouvsky Oh come on.
Use your noggin.
 
@DanielSank it's $L/2$
I must have made a mistake elsewhere
 
3:13 AM
@0celouvsky Convert $\sin$ to $e$
should be easy enough
 
@Secret Theorem. Let $||\cdot||_1,||\cdot||_2$ be two norms on $\Bbb R$. There exist constants $c,C>0$ such that $$c||v||_1\le ||v||_2\le C||v||_1$$ for all $v\in\Bbb R^n$.
*Proof.* Clearly it is enough to prove this with $||\cdot||_1=||\cdot||_e$, the Euclidean norm, since this relation is transitive. Let $e_1,\dotsc, e_n$ be a basis of $\Bbb R^n$, and write $\Bbb R^n\ni v=\sum_{i=1}^nx^ie_i$ so that $||v||_e=(\sum_{i=1}^n |x^i|^2)^{1/2}$. Our first estimate is
$$\sum_{i=1}^n|x^i|\le \sqrt{n}||v||_e. $$
To see this, note that the LHS is an $\ell^1$ norm, and $||\cdot||_e$ is an $\ell^2$ norm, so by H\"older's inequality,
$$\sum_{i=1}^n|x^i|=\sum_{i=1}^n 1\cdot |x^i|\le \left(\sum_{i=1}^n1\right)^{1/2}\left(\sum_{i=1}^n|x^i|^2\right)^{1/2}=\sqrt n||v||_e.$$
Next,
$$||v||_2=||x^1e_1+\cdots +x^ne_n||_2\le\left(\max_{1\le i\le n}||e_i||_2\right)\left(\sum_{i=1}^n|x^i|\right).$$
Letting $C=\sqrt n\cdot \max_{1\le i\le n}||e_i||_2$, we find that
$$||v||_2\le C||v||_e.$$
This inequality shows that $f:v\mapsto ||v||_2$ is Lipschitz continuous in $\Bbb R^n$ with the standard topology. Let $S$ be the usual unit sphere in $\Bbb R^n$. It is compact in the Euclidean topology, hence $f$ attains its infimum $c$ in $S$: there exists a $v\in S$ with $f(v)=m$. Since $v\ne 0$, $c>0$. Let $w\in\Bbb R^n$ be nonzero, and set $v=w/||w||_e\in S$. Hence $||v||_2=f(v)\ge c$, or
$$||\frac{w}{||w||_e}||_2\ge c\implies ||w||_2\ge c||w||_e.$$
And the proof is complete.
That's the best version I know of.
 
So anyway
what kind of fiber are continuous spin fields
I still don't know
 
what?
 
Continuous spin representation fields have this weird type of field with a continuous range of index
I am wondering if they can be described by a fiber bundle
 
oh christ no
what is a continuous index anyway
it's just a function dude
 
3:27 AM
The field transforms as
$$U(\Lambda)\hat \varphi_{\theta_n}(x) U^{-1}(\Lambda)\rightarrow \hat \varphi_{\Gamma_{mn}(\Lambda)\theta_n}(\Lambda x)$$
With $\Gamma$ a spinor Lorentz transformation
The index itself is a spinor
 
@Slereah lol
 
yeah it's fairly shit
Also does the complete atlas of a manifold have the same open sets as the projections of the local trivialisations?
fairly sure it does but I couldn't say why
 
well that's what we mean by a smooth vector bundle
 
3:43 AM
hey @DanielSank, are you available?
 
4:02 AM
@TanMath I'm cleaning my room. Availability is relative.
 
reading about vertical lifts on manifolds makes me think of this
 
(Uh... this question turned out to be more lengthy than expected, I guess I will post on the main instead)

I want something more illustrative:

Let's take classical correlations vs entanglement as examples. For classical correlations, the observables are already determined even before a measurement, and thus knowing information of one subsystem will immediately let you know the corresponding information in another subsystem.

For correlations in entanglement, suppose I take the singlet bell state. Then upon preparing the bell state, the correlations of the 2 subsystems are already establis
 
The "Frechet-Kolmogorov" theorem
who even knows this much functional analysis
Ah, this isn't even a crazy theorem
 
What's a crazy theorem
 
@Slereah idk, pick some horrible estimate from PDE theory
something like that
or that
 
4:14 AM
I'm not reading that
 
exactly.
ah, the nuclear space of A. Grothendieck
finally something engineering related
 
I should read this paper
It seems relevant to my interests
 
haha wtf
what are those ones without arrows?
wormholes?
what on Earth is a virtuous spacetime
 
A spacetime without sin
 
@Slereah what paper?
I might enjoy it too
 
4:19 AM
"Causal structure in spacetim"
By Brandon Carter
He defines spacetimes to be $C^1$
The madman
 
do you have the paper?
where did you find it
 
I don't remember
It's just in my files
 
ah, got it
it's a long paper, wow
 
yeah
 
@Slereah Oh, here's a crazy theorem
A Banach space is reflexive if and only if it is locally weakly sequentially compact.
 
4:24 AM
that paper has a lot of random causal theorems
 
page 380 and 381 seems like what you're looking for
@Slereah How's progress on the book?
@NeuroFuzzy long time no see
 
It's alright
60 pages so far
 
@0celouvsky Yee! What's up!
 
though the tough part is actually knowing what I'm talking about
Many things to learn
 
I haven't been on the website so much. A bit burnt out answering questions about special relativity haha
 
4:27 AM
Virtuous is just that there's no CTC
Well, no CCCs
No CTCs is almost virtuous
though then I'm not sure why in the diagram acausal implies virtuous
 
Accepted an offer for a university far off from my alma mater of UCSD, which goes by the strange name of UCSD. (My only acceptance letter and a really good offer at that!)
 
@NeuroFuzzy trying to figure out if there's an easy way to see that $L^2$ is locally weakly sequentially compact
I know Jost does it for Hilbert spaces in general
wondering if Yosida has the proof
@NeuroFuzzy congrats
@Slereah link?
 
No link right now
Just a smattering of things
 
@0celouvsky Ahhh more analysis!
 
who doesn't like a good bit of functional analysis at 0:36 am
 
4:39 AM
What's the difference between $$$$ and \begin{equation}\end{equation} in latex, anyway
 
can't see shit
 
The double dollar sign-double dollar sign versus begin equation end equation
 
usually the latter puts an equation number
 
@Slereah or rather {equation*}?
 
who even knows how to prove the Fourier expansion for $\Bbb R^n$ :o
I guess you'd prove it for the smooth functions as usual, then use density of bump functions in $L^2$
terrible
@Slereah oooo boi
 
4:53 AM
I've been using greek indexes and $g
$g$ for the group structure of the bundle
Bad idea
Everything looks like the metric tensor now
 
The group should be G, not g...
 
Well the group is $G$
but $g_{\alpha\beta}(p) \in G$
For $p \in V_\alpha \cap V_\beta$
 
You should be using abstract index notation for tensors anyway
 
Also Steenrod is a bit confusing because I think his definitions are a bit dated
Like he calls fiber bundles for just $\{E, X, \pi\}$
And with local trivializations, he calls them coordinate bundles
Is that a terminology still used?
 
Anyone want to try to get the PSE logo in this?
 
4:59 AM
@Slereah no
We always assume there's a local trivialization compatible with the manifold structure
 
Well his fiber bundles aren't even necessarily over manifolds
Just topological spaces
Although he does mention the other definition of fiber bundles that includes the trivialization
He calls it the EHRESMANN-FELDBAU definition
 
Hmm ok
 
then again when he wrote that bundles were like
ten years old or so
Probbly not too much standard terminology
 
Jesus. I'm off, cheers.
 
I wonder what's the original bundle paper
Let's see
later
that's the one
 
5:20 AM
Some problem solving musings:
Imagine you know the answers to a problem, and your task is to work out what is the problem that is being asked
This happens to me sometimes when I knew what is the solution I am seeking, but less clear on what is the problem I am trying to solve. As a result, the ultimate "work backwards" occurs to figure out the problem that is being asked
 
1
Q: How to find more information about Chang'e-2's actual 3D orbit in space, since it's not in JPL Horizons?

uhohedit: A simple web search in Chinese may turn up something, but I don't know anyone personally who is both both fluent and interested in space exploration. This is a pretty cool orbit - there must be something somewhere! I tried to find Chang'e-2 in the JPL Horizons database but coulnd't find it...

+100 Bounty expiring in one day. Anything??
 
5:38 AM
Cool, the proof looks fine (and you have used compactness) except this part is not very clear to me:

$$||v||_2=||x^1e_1+\cdots +x^ne_n||_2\le\left(\max_{1\le i\le n}||e_i||_2\right)\left(\sum_{i=1}^n|x^i|\right).$$
Remind me which inequality we use here to split up the eucledian norm to the product of the longest basis vector and the 1-norm of the components?
 
user228700
5:53 AM
@JohnR: Morning :-)
 
@Kaumudi.H How was the test?
 
@Kaumudi.H Morning. Sorry for the slow response, I was on the supermarket web site ordering groceries - an absolutely vital task!!
 
user228700
@SirCumference Hi. Wasn't as great as I'd hoped. I'm preparing for the next one now :-)
 
@Kaumudi.H In a year?
 
user228700
Huh? Noo. In a few weeks.
 
user228700
6:05 AM
@JohnRennie Ah, OK :-)
 
Oh, I heard that the test is only given every year o_O
 
user228700
@SirCumference There are other tests as well, you know :-P
 
@Kaumudi.H Oye facepalm
 
user228700
:-)
 
Welp, good luck :)
I gotta head to sleep
'Night
 
user228700
6:07 AM
Thanks. Night! :-)
 
Anonymous
6:34 AM
@Kaumudi.H How much are you scoring? My maths went bad....phy and chem were good
 
Anonymous
I'm getting around 250...
 
Anonymous
One guy from my center is getting 325
 
Anonymous
:-P
 
My kettle has just gone bang and appears to be dead. Oh no. This could be a critical failure!
Fortunately, like the good experimental scientist I am, I have established that it's possible to boil water in a pan :-)
 
Hm
How to note the Lorentz group
$O$ or $\mathrm{O}$
 
user228700
6:47 AM
@blue I haven't checked properly yet. I didn't do great so I'm trying not to think about it.
 
user228700
@JohnRennie :-) Hehe.
 
@Kaumudi.H it's no laughing matter. Caffeine withdrawal symptoms can be fatal!
 
user228700
:-) Yes, of course!
 
Actually I feel quite sad because I've had that kettle for over 20 years. It's older than you are :-) And now it has passed on.
I wonder where the best place to buy a new kettle is. Amazon probably ...
 
user228700
@JohnRennie Wow, that's crazy...
 
6:50 AM
That's the thing about getting old middle aged. All the stuff you own is old middle aged as well :-)
 
user228700
Hehe, yeah :-)
 
Wow, £5.49 for a new kettle. That's cheap.
 
@Slereah $O(1,3)$, you need to notate the signatures to distinguish it from other types of orthogonal groups $O(m,n)$
 
user228700
@JohnRennie eBay or Amazon?
 
I am aware, yes
I'm just talking typography
 
6:59 AM
@Kaumudi.H Argos
It's kind of a general retailer in the UK and sells all sorts of stuff - including kettles.
www.argos.co.uk
 
user228700
Ohh, OK...
 
Whether the kettle is any good I'll find out when I collect it, but ... well ... it's a kettle. All it has to do is boil water :-)
Anyway I need to go. I have to take my car to the garage for it's annual check-up. Back in a bit.
 
user228700
OK bye :-)
 
Older papers use $O$, more modern papers tend to use the upright $\mathrm{O}$
personally, upright O looks better
 
Anonymous
7:22 AM
@Kaumudi.H Oh :-P That feeling :-)
 
Anonymous
Even I was scared to check the answer key
 
Anonymous
But it is good to analyze your mistakes so that you can avoid them in future exams. :-)
 
Anonymous
Anyhow, all the best for advanced
 
9:04 AM
@JohnRennie "Annual?" You should get the oil changed at-least twice a year.
 
9:19 AM
Yo @Qmechanic what's with migrating this one?
0
Q: Two waves interference animation

BowParkI would like to plot (or to find) an animation where two waves at different frequencies, propagating with different velocities, sum together $$w_1 (x,t) = \cos(\omega_1 t - k_1 x)\\w_2 (x,t) = \cos(\omega_2 t - k_2 x)$$ and generate the resulting signal $$w(x,t) = \cos(\omega_1 t - k_1 x) + \c...

OP specifically asks for
> 2. Is there a free tool / software / site to generate such an animation?
Mathematica is nowhere near free
 
9:38 AM
I think therefore jam? :-)
 
@JohnRennie Good morning :)
 
Morning. Sorry I wasn't around last night.
Sunday evening I'm comatose after eating a massive lunch :-)
 
Nah, come on, it's weekend :)
I branched the code
made some changes already but miniscule
just created a Game struct pretty much
and then I wanted to discuss with you a bit the linked list deal
 
OK ...
 
Should the linked list be a struct inside the Board struct?
 
9:51 AM
I would put it in the game struct.
 
After all, the undo history is part of the way the game is designed not the board.
 
Yeah
Then gameInit would receive a board and initialize the linked list with that
after this every move we add a node to the list and perform the move there
no more buffers
 
Yes, that's the way I would do it.
Are you going to create a separate struct/class for the list?
 
@E
 
9:55 AM
I wanted the linked list struct to be inside the game struct
There's no reason to expose something no one else uses
 
@EmilioPisanty I am beginning to think that there exists a critical internuclear distance where the there are no bound states. This looks to happen around $a_0$, continuing along my variational path, i have it at $<0.8 a_0$
 
@JohnRennie Sounds reasonable?
 
Yes.
 

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