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05:00
@0celo7 Can you cite a source that says I would even need to do that?
[40] Private communication overheard in the mens' room at a recent conference, but we didn't see who it was because we didn't want to get up.
[34] Toilet stall conversation with unknown physicist at HEP conference
[22] All our friends (until now), "Conversation of Energy: ∂φ/∂k," private gossip.
[69] Thesis: unpublished
^ in Slovakian
05:02
@tpg2114 what
[38] (WRITE YOUR NAME HERE), My favorite paper, My Favor. J. 1 (1980) 1.
suppose you need to know about geodesics on Lorentzian manifolds
just make some shit up and cite HE
people will believe you
Hmmm...is it acceptable to write "This is a straightforward calculation:" and then do three lines of turning symbols into other symbols to show it?
I actually reviewed a paper for an English language journal where more than half of their citations were for Slovakian theses (or thesii?) that were unpublished in any form
@ACuriousMind The straightforward calculation is omitted.
This theorem is a trivial modification of the previous one.
05:03
"the reader can show"
Left as an exercise for the reader.
I sent the editor a message saying that without access to their sources, I couldn't verify anything they said. So then my inbox got blown up with copies of several different masters' theses in Slovakian
THEOREM: Blah. PROOF: Clear.
@0celo7 Well, it's not so straightforward as to be obivous, but explaining the individual steps would be really boring.
@tpg2114 Did you then request a translator?
@tpg2114 wait you're not a peer?
05:04
The worst is "The extension to 3D is trivial"
yeah
try that for Gauss-Bonnet...
@ACuriousMind No, I just ripped apart their text for crappy english that made it impossible to understand the content of the paper.
"The extension from 0 D to $\omega$ D is trivial"
"The extension to complex vector bundles is trivial"
The extension from integers to Calabi-Yau manifolds is trivial
05:06
@0celo7 I actually sent the editor an email that said "I'm happy to review this, but you do know I'm a grad student, right?" To which he replied "That probably means you are eager to not disappoint somebody who may hire you someday and so I know you'll not f**k it up."
why would a lit person hire you
oh!
not an English journal
a jouirnal in English
was wondering why a fluids grad student was reviewing a lit journal ;)
Many works of literature include the sea
Which is made of fluids
I thought you were making the really insulting leap that I must be below engineering and study literature...
At Georgia Tech no less. Where I'm fairly certain nobody, ever, has decided to go to grad school for literature
[42] No, dummy, it's an exponent, not a footnote.
probably not true
05:10
heheh
@Slereah Wait, 42 is an exponent? How big are the numbers you work with?
@tpg2114 you know what's a shitty journal
J. Math. Phys.
don't ever cite it
@0celo7 From AIP?
yah
05:13
I don't associate them with crap journals usually
@ACuriousMind can tell you all about it
poor @yuggib has a publication there...it's worthless now
@0celo7 Stop trolling.
But I only deal with Physics of Fluids from them -- and apparently the entire editorial board resigned recently to start a competing journal because of some BS that went on with AIP
They do the Gallery of Fluid Motion which has some pretty awesome pictures. I'm all about the pictures.
@0celo7 Jokes and hyperbole are not really funny when the other person has no way to tell to what extent you are joking.
@ACuriousMind $\pi \Leftrightarrow$ quantum mechanics
05:15
I think you mean $\pi + e$
You dolt
@ACuriousMind Yeah... so is it actually a bad journal? I haven't come across it before.
@tpg2114 no
I've looked through a dozen of their papers tonight
but there is the paper of doom
DERIVATION OF PI FROM QUANTUM MECHANICS
@dmckee Yes. Yes, it does.
@tpg2114 Well...the journal as such is surely not bad, but there was a recent singular instance where a paper "OMG, we found $\pi$ in quantum mechanics!" was published there after the suspiciously low review time of...one day.
@0celo7 Good, cause now I'm pulling a bunch of papers applicable to my research
05:16
was it reviewed on friday
"I want to go home, let's just approve this"
I must sleep
@ACuriousMind Eh, that happens sometimes...
good night everyone
@tpg2114 I'm just not sure how exactly that happens, especially when it's not really clear what kind of advancement in either maths or physics the result actually signifies.
Was the result even non-trivial
You can find pi with random processes
05:19
Or is there some way to have the paper reviewed prior to officially submitting it?
@ACuriousMind I've seen several papers that intentionally troll people and usually the editor is in on it
It has been known since the 17th century
Throw sticks at a circle or something
Pi!
@Slereah imo, not really - they put in some gamma functions and used that those have powers of pi as special values to get it. Or something like that.
It happens more often in the pure sciences though. But I did see a paper that was criticizing how relaxed standards for numerical papers were
05:20
@tpg2114 Hmmm...that might be the most reasonable explanation.
The authors wrote this crazy complicated numerical scheme and then just said they neglected all terms higher than O(0) and their code just output the solution they wanted exactly
And so their error was 0 always
String theory
@Slereah There's another one that I can't seem to search for where the stickman says something about including second-order effects and why does that field need its own journal...
What about...*hyper*symmetry
ACM is too quick
Dang... I couldn't find the right search terms for that one
Good job
He literally has all of them memorized
I, uh, searched "xkcd complicated simple", it was the top hit :D
I have the pictures memorized, but not the titles so I can search for them...
See -- I was searching for "xkcd secondary terms"
And... nothing
05:25
Apparently the spin bundle proof of the positive mass theorem is a simplification of the original proof
Which used calculus of variations
but wait, what if there is no spin bundle???
Then the photon can't go round and round D:
there's a few papers on non-orientable spin structures, but they are all done by math people
There's never a paper like "Here's a non-orientable spacetime, this is what happens to particles on it"
05:46
Oh my God....I just bountied the wrong question.
How do I undo it
I just lost 50 rep on a moronic question...
Please tell me there's a way to fix this
"If there is no gravity on the moon why is the american flag waving?"
ahahah
No...no...
;-;
Welp...fml
user54412
06:01
@tpg2114 Just for you, I expanded all the definitions in the ADM equations, which are the Einstein equations put in "time derivative = stuff" form.
user54412
user54412
Note all $\Gamma$, $\bar{\Gamma}$, and $\pi$ terms have first derivatives, and all $R$ terms have first derivatives and products of two first derivatives.
user54412
Then the evolution equations are:
-17
Q: If there is no gravity on the moon why is the american flag waving?

ZaneIf there is no gravity on the moon, how could this flag be flapping in the wind? (see link) http://www.stumbleupon.com/su/2wD6eg/hea-www.harvard.edu/~fine/images/desktops/Armstrong.jpg

user54412
06:02
So how do I get the bounty off this
Ask on Meta
Er...ask who?
user54412
You can check that all the terms are either 1st derivatives, products of 2 1st derivatives, or second derivatives.
The board
user54412
The mods can clear bounties. They probably can't give the rep back though.
06:06
50 points lost isn't a tragedy, either
It was 25% of my total rep
That's a tragedy
Well go earn more :V
Or ask mods
user54412
@tpg2114 I leave it as an exercise to the reader to verify that the above equations are indeed hyperbolic :p
user54412
Also, those are the vacuum equations. They are "trivially" extended to include dynamical matter (as one professor of mine actually once said).
06:15
"Trivial" is basically meaningless
Not quite sure what the whole spacetime as a fluid would accomplish, tho
"Instead of solving GR, we just have to solve Navier Stokes!"
OH WAIT
06:31
If spacetime is a fluid, then what does it mean for the velocity of a fluid. Surely, spacetime cannot actually flow, right?
I actually found this approach kinda hard to wrap my head around
 
1 hour later…
07:56
hope you all enjoy your little exclusive club
found a place where I can collaborate with real physicists
08:37
The Mixmaster Universe is a solution to Einstein's field equations of general relativity studied by Charles Misner in an effort to better understand the dynamics of the early universe. He hoped to solve the horizon problem in a natural way by showing that the early universe underwent an oscillatory, chaotic epoch. == DiscussionEdit == The model is similar to the closed Friedmann-Lemaitre-Robertson-Walker universe, in that spatial slices are positively curved and are topologically three-spheres . However, in the FRW universe, the can only expand or contract: the only dynamical parameter is overall...
This sounds like a rap album
 
4 hours later…
12:29
@Slereah lol
in Academia, Nov 27 at 23:29, by Ghost
deleted my answer - I will not tolerate being lectured and talked down to by some one who seems to think that they are better than everyone else. (@ChrisWhite)
He's just pissy. Nothing new.
But now I want to know what got deleted!
@ChrisWhite Any idea?
The time stamps fit.
in Academia, 2 days ago, by Ghost
The irony is that another colleague mentioned their interest in joining Academia.SE (and a few other sites) - I echoed the advice of my other colleagues and told them not to (and mentioned that as they are not American, they are not likely to get a warm reception).
Better not mention that I am not american ;)
12:42
This is a very cheerful post, and it no doubt gets upvotes from everyone who wants it to be true, but how does it answer the question? There are certainly fields (like mine, and more importantly the OP's) where no one in that part of the world is doing similar research. How does someone in country A convince someone in country B to actively collaborate, when the person in B can find a substitute collaborator in B with the same level of knowledge? The problem is that for people in B, finite resources really are best spent with the local collaborations, yielding more results per unit effort. — Chris White Nov 27 at 23:20
^offending comment
I don't even get how that would set him/her off so much.
Anyway I suspect we are breaking the be-nice policy
@I'mmostlyjustanidiot Probably.
13:07
@I'mmostlyjustanidiot Judging by his reaction to this site, he easily feels "persecuted." Not sure if that's the right word, but maybe you get my meaning.
13:25
@SirCumference-Pies I raised a flag for you informing the moderators. Next time something like this happens, just click the flag button on the post, and choose "needs moderator attention" in the dialogue that pops us.
13:37
@user36790: While your willingness to improve others posts is commendable, please try to exercise more care when using your edit priviledges. This is not the first case where your edits are partly superfluous - \begin{equation}...\end{equation} is fully equivalent to $$...$$in MathJaX (though not in LaTeX) - and partly just wrong - the correct English word is neither stillstand nor still-stand, but standstill.
13:51
@ACuriousMind Did you "finish" Fallout 4?
@0celo7 Not yet
@ACuriousMind : Why are you inconsistent with colons after @'ing people? This is just a general comment.
Both you and the Frenchman.
@0celo7 The colon is there when I type the address by hand - it is not there when I use the reply function or autocompletion
-1
Q: How fast would you have to shoot a fish through the air in order to cook it?

user3172913This came out of a debate in a pub - if you were to accelerate an uncooked fish through the air, how fast would you have to shoot it before the friction would cook it to an edible level?

Sometimes, the "homework" close reason is unintentionally hilarious.
I wish cooking fish by shooting them had been homework at my school :D
user116211
14:09
@ACuriousMind: Yep! Actually the word didn't flashed that time; the word was marked by the red line as usual in Windows. So, I added the hyphen between those other distinguishable words which removed the line. I didn't think beyond that.
14:19
@DanielSank : point out what? I've had things pointed out carefully and politely to me, and I've learned from it. The difficulty seems to be when I then point these things out carefully and politely to people like you. It's something like the Avatar quote: "Moat: It is hard to fill a cup that is already full. Jake Sully: My cup is empty".
14:31
Got a 100 on the last pre-final ODE test. I somehow managed to compute the convolution of two cosine functions by hand! Correctly!
@0celo7 : right. You don't travel along a worldline, you don't travel round a CTC, it would signify Mayfly Day instead of Groundhog Day. There is no way you can move such that everything else not only moved back to where it was, but never moved at all. Time travel is science fiction.
14:47
Proof?
Can you prove that there are no CTCs in physical spacetime?
"

I will reiterate: there is no reason to assume a constant curvature. Because when you posit that the universe is homogeneous and isotropic, you also posit that there is no gravitational field and no spacetime curvature. There are no observations of any curvature, and for all we know some guy 46 billion light years away sees half the sky as black."

That is a really interesting thing to think about!
@0celo7 haven't you been down this road before? It might not be a good idea to go there again
In mathematical physics, a closed timelike curve (CTC) is a world line in a Lorentzian manifold, of a material particle in spacetime that is "closed", returning to its starting point. This possibility was discovered by Kurt Gödel in 1949, who discovered a solution to the equations of general relativity (GR) allowing CTCs known as the Gödel metric; and since then other GR solutions containing CTCs have been found, such as the Tipler cylinder and traversable wormholes. If CTCs exist, their existence would seem to imply at least the theoretical possibility of time travel backwards in time, raising...
Not enough Analysis in my history apparently :D
14:54
@DavidZ Is that a friendly reminder or a moderator reminder?
Friendly for now
@DavidZ Hey I just edited my question to better fit the "homework-like" question requirement. Do you mind reopening my question?
@TheMan can you post a link?
Asking whether your work is correct isn't on topic either
15:00
So how can I make my question better?
I'm obviously just trying to make sure that I got my concepts right
I'll let you know soon (sorry, working on three things at once at the moment)
15:15
@Danu I did $\int \mathrm{d}r/r^3$ correctly on a test. I'm very proud of myself.
Stellar progress
@TheMan OK, now that my other thing is done: the thing is, you don't really have a question for us. You encountered a problem, you came up with a solution to the problem and an explanation for the solution, and that's that. I understand wanting to check with someone to make sure you understand it, but that's not what we're here for.
@Danu :)
next I'll be able to find the inverse of a 2x2 matrix!
Maybe start with a 1x1 matrix first ;)
Don't wanna go up to PhD level in one step
Now, if something seemed wrong about your solution, and you made a decent effort to figure out how to fix it but couldn't find out, then maybe you'd have a good question for this site. But that doesn't seem to be the case, from what you wrote.
15:21
I think one can safely do matrix inverses in 5th year courses.
Triple integrals, on the other hand...
And make no mistake, that's a good thing. After all, your real goal is (or should be) to solve your problem, not to come up with a question to ask here.
I appreciate you asking about it, by the way. That is the mark of a great contributor. :-)
So the universe seems consistent in temperature and such?
@DavidZ Im just beginning to learn the concept of momentum. I saw a question on it. I tried my very best to come up with an answer to that problem to satisfy the homework-lie question requirement. However, I have no idea whether or not that explanation even makes sense, and since the last time I took physics was a few semesters ago, I have no real human being to check with. So I am asking a question to the community on how they can answer the problem.
@DavidZ Can I ask a 10 part question about photons going round and round
@TheMan yep, I know, I see that's what you did. Like I said, that's not the sort of thing we're here for.
15:23
@ACuriousMind @0celo7 @DavidZ @I'mmostlyjustanidiot @TheMan @Danu A small newtonian question, that although I know how to do the prove mathematically, don't really understand how to phrase what is happening in words:

Why does the inability of a function U to obey the symmetry of mixed derivatives, which implies that dU cannot be a total differential, will mean that the force F derive from U must be non conservative?

That is, what differs between a total differential $dU$ and some non conservative "differential" $\delta U$ in a geometric sense?
@0celo7 no
@Danu What about...a 0.5x0.5 matrix?
@I'mmostlyjustanidiot huh?
@ACuriousMind how is that even defined o.o
But isn't that a question? So should I just delete all of my explanation and have the community attempt to answer my question?
@ACuriousMind CMB
15:24
@ACuriousMind I am just reading the Horizon problem, and the temperature of the CMB is roughly the same everywhere
@DavidZ :(
@Secret 1. You don't need to ping everyone in the room. 2. What?
@ACuriousMind if only @all worked...
@TheMan no, that would be going backwards. Remember, your goal is to get a solution to your problem, not to come up with a question to ask here. You already have a solution to your problem. So what do you need us for?
What is the solution to the horizon problem?
15:26
@I'mmostlyjustanidiot Wiki says "Two theories that attempt to solve the horizon problem are the theory of cosmic inflation and variable speed of light.". From that you should conclude we don't have a unique solution yet.
It said that and then went on to talk about assumptions of homogeneity and isotrophy
variable speed of light
but isn't that just GR
It's Isotropy; isotrophy would be a state of "same nourishment", literally translated
lemme find an Einstein quote...
15:28
@DavidZ Because the solution is possibly incorrect, and I am trying to understand the concept of momentum, therefore trying to seek someone to answer the question listed with an explanation, which is what questions on StackExchange are. Plus, it isn't actually a homework question for me anyways. Just a random question that I came across and wanting to know more.
@TheMan Well then, let's try this: why do you think the solution might be incorrect?
We know that a conservative force $F$ can be described by a potential $U$. Thus dU is an exact differential, that is

$$dU=U_x dx+U_y dy$$

We also know that for mixed 2nd derivatives of U, $U_{xy}=U_{yx}$

If a function $S$ of which a force $A$ can be derived does not have equal mixed derivatives, then this S will not be able to satisfy the exact differential equation and thus $A$ cannot be conservartive

But why is that , what makes a total differential differ from a non total differential, what extra things (or terms) that the non total differential that give it path dependent properties
@TheMan Questions on Physics.SE are a little different from what is par for the course on e.g. SO or math.SE. We don't want "homework-like" questions that are just about solving a specific problem or correct a user's solution to a problem.
@TheMan By the way, the fact that it's not actually homework doesn't matter. Even though the hold reason still talks about homework for historical reasons, it's more about requests for calculations these days. (We're in the process of figuring out new wording, as a long-term project)
15:30
@DavidZ Because I learned the concept on my own, and I have nobody to check with.
@TheMan you mean, as a reason you think the solution might be incorrect?
@Secret WTF is a "non-total differential"? How can the mixed second derivatives not match, is your function $S$ not twice differentiable?
If your only reason to think you might be wrong is that you don't trust yourself, that doesn't cut it for a question on the main site. It'd be fine to ask here in chat though.
Alright then.
@Danu Damn, you caught me :P
15:33
@ACuriousMind Note that the match on membership times is pretty good ;)
"Maybe I can be talking a lot of bullshits, so I'm sorry.", " can them goes through every kind o materials" - Only a Curious Mind
ok, let me rephrase it

$U$ is a potential function if it satisfy the following equation
$$dU=U_x dx+U_y dy$$

Where $(U_x,U_y)$ is the force $F$

Because by integration, it can be shown that the change in U depends on the endpoints of the integration only, and not its path

If we have a non conservative force $G$, then it cannot be described by a potential. Any attempt to find this potential $K$ one will find $K_{xy}\neq K_{yx}$ thus a potential function does not exist for $G$

Therefore if we try to compute the total change of the quantity K by integrating
@I'mmostlyjustanidiot that about sums up his GR knowledge
@Secret The quantity $K$ does not exist if the components of $G$ were continuously differentiable (because mixed derivatives are equal for twice continuously differentiable functions). It doesn't make sense to speak about its "total change" - it does not exist.
@Secret what
$\mathrm{d}U$ is defined by that equation
$U$ is a potential function if $\nabla U=-F$
or $\mathrm{d}U=-F^\flat$
or is $\nabla U$ a covector...
Wow, @ACuriousMind VTC'd on his alter ego
15:46
Because we have this quantity, work $W$, which in most textbooks infinitesimal work is denoted by $\delta W$. If one integrate this along some curve from the positions a to b we then get $\Delta W$ which is path dependent

Therefore, my question is fundamentally speaking, why is $\delta W$ integrated vs $dU$ integrated give different properties for $\Delta W$ and $\Delta U$, how does the mixed derivatives give $\Delta U$ the property of path independence, other than it allows U to satisfy the total differential equation?
how is infinitesimal work defined, @Secret
$(\sum F)\cdot \delta x$ or somthing like that?
@Secret "$\delta W$" is suggestive notation, it is not obtained from $W$. Quite the opposite! You define $\delta W$ (without having a quantity called $W$ at your disposal), and then you define $W[\gamma] = \int_\gamma \delta W$.
The notation is suggestive of the fact that if the integration of $\delta W$ is path independent, then $W$ is a path-independent function - a potential - and indeed $\delta W = \mathrm{d} W$.
is it not a functional
OH GOD CHAT SESSION
But the $\delta$ is not an operation which is executed on $W$, $\delta W$ is one object, not $\delta$ applied to $W$.
what is this chat session about?
15:50
@0celo7 Not if it is path-independent, that's the point!
@BalarkaSen Chatting and sessioning
@ACuriousMind I mean in general
@0celo7 Yes.
@ACuriousMind good
brb class
@BalarkaSen nothing in particular. Sometimes we have a topic, but I don't think there's anything particular lined up for today
@ACuriousMind riiiight.
@DavidZ Ah, I see.
15:51
Ok, so basically the question boils down to how $\delta W$ obeying mixed derivatives (hence satisfying the total differential equation) result in it to be path independent, other than the fact that all the algebra works out and the outcomes just popped out from the computation

Is there some more fundamantal reason in terms of what underlying property that obeying mixed derivative changes $\delta W$ to make it path dependent?
Mar 24 at 16:04, by ACuriousMind
C'mon session harder
@Secret "Mixed derivatives" is just an integrability condition. $\delta W$ is a one-form. If it obeys mixed derivatives, then its exterior derivative (its "curl" if you wish) is zero, i.e. $\mathrm{d}(\delta W) = 0$. On topologically trivial spaces, this directly implies there is some 0-form $f$ such that $\mathrm{d} f = \delta W$, and since we want to use the suggestive notation, we call this $f$ then $W$.
more sessioners incoming.
Ah, makes sense, thanks
@0celo7 not sure what your morphisms are
I am not convinced you can make such a category.

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