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12:01 AM
Wait if it's a normal vector you have $n(v) = 0$ on $T\Sigma$
Yeah I think it's all good
 
Mhm
 
12:15 AM
Christodoulou does mention time
Though he doesn't specify any causality condition
p. 289
but that's only for lagrangians
Really what I want these papers to say is just "This is the bundle of the field and this is the canonical momentum"
Plz hold my hand I am dumb
What does $\underset{Y}\otimes$ mean anyway
 
@Slereah what’s the context
Bundles? Then they mean the base is Y
 
That the jet bundle $\pi^1_0 : J^1 Y \to Y$ is modelled over $$T^* X \underset Y \otimes VY \to Y$$
 
Then it’s what I said, probably...
 
12:30 AM
fugg
1:30 already
I'm gonna die tomorrow
of not sleep
time for beddy byes
 
12:40 AM
@Slereah how do you know these American colloquialisms
 
Sweating on Skype with 5 seasoned developers in a foreign country trying to make a nodejs app run in azure. Haaa I'm doomed . . . . doomed doomed doomed
 
Lots of TV my man
Hardest part of getting another culture btw
Schoolyard rhymes
Not a lot of those even on TV!
What's a good way to think about the vertical space btw
I'm trying to think of a good way
Is it related to the functional derivative?
It's the tangent of the fiber after all
 
The manifold is a horizontal line, the fibers of the bundle go up, and the vertical fibers are tangent lines to the vertical dudes
 
A vector is obtained by varying the value of the field
Or am I mistaken
 
Keep reading Christo
I think you’re basically correct
Maybe
 
12:46 AM
Hurray
It does help
And since there's some mapping between the jet bundle and the vertical space I'm guessing it will be involved for lagrangian stuff
 
1:18 AM
@Slereah the vertical bundle plays a big role in this stuff
it makes it that much harder to understand though
it's another god damn bundle floating around
 
I can sort of see the notion though, I guess?
Vertical bundle for varying the field
Horizontal bundle for the space derivatives
I guess?
Something like that
 
pretty much -- to get the horizontal bundle you need a connection of course
 
Yeah
 
but ideally the connection doesn't really matter
 
I usully try to picture the tangent bundle on $S \times \Bbb R$
It helps a bit
Well, a tangent plane anyway
 
1:21 AM
that seems pretty hard already
I think of stuff on $[0,1]$
 
The $[0,1] \times \{0\}$ bundle?
 
no, like $T[0,1]$ is what I picture as "bundle" in my mind
or $[0,1]\times S^1$ if I need a principal bundle
 
Not much of a difference with R for picturing
 
yeah
so really $(0,1)$
@Slereah the spacetime on page 3 of the 50 years book is too funny
he must have freehanded it
 
It's alright
 
1:31 AM
$V$ being the manifold is French supremacy
 
Une variété
 
@Slereah have you seen anything other than $\beta$ for the shift field?
 
Pretty much always beta
 
1:48 AM
@Slereah hae you seen HBO's Rome?
 
2:12 AM
I have another interview next week. This time it's with one of the big tech companies. OMG going have to go over algorithms and data structures. hehe
 
 
2 hours later…
4:06 AM
@EmilioPisanty Oh deer
@ooolb Oh whale
I'll stop with the puns...
 
...u so punny
 
 
3 hours later…
6:55 AM
@0celo7 I did not
 
7:48 AM
I'll never understand why people vote on questions with ≥10 score in Area 51 proposals
@JohnRennie Probably a foolish question, but shouldn't it fall into Chemistry, or at least Physics?
 
@SirCumference the comment wasn't meant to be serious. Physical chemistry questions are generally on topic both here and in the Chemstry SE.
 
Oh...welp 3:00am me is dumb
 
In this case I would guess Chemistry is better since this looks more chemistry ish than physics ish
But I suspect answering the question would require specialist knowledge of the area, and I doubt anyone on either SE has that experience.
 
@heather For me, sitting in history class was the worst, but now that I'm finally done with high school I wish I had learned more history
Funny thing, once you're done groaning in the classroom, it actually becomes quite interesting
That's at least what I notice with a lot of the subjects I used to hate learning
 
8:15 AM
Euler-Lagrange on the Jet bundle is apparently $(\partial_i - d_\lambda \partial^\lambda_i)\mathcal L = 0$
 
fml
 
Oye, is there any to get an anti-spam bot for an SE site? Just look at this
 
Apparently equations on the second jet bundle
bluh
 
Every other day we get links to sites, usually involving weight loss or testosterone
 
maybe you need to be less fat and manlier
 
8:17 AM
Eheh...
This is my 11th spam flag in the last month...
 
i am not me right now
i still havent gotten over my haircut why the fuck did i do it
 
At the very least there should be a bot to block questions with titles including ".com"
 
i need looooong hair again
 
@ooolb You need @Loong here again?
 
i’ll admit that pun was impressive
 
8:20 AM
:D
 
but your other ones kinda suck no offense
 
you should do more original ones like that
 
I usually am original
I think
 
well i mean the science ones gotta go
 
8:21 AM
@ooolb perhaps he doesn't like folding paper ...
 
@ooolb But math ones are at least good. You just gotta look at them from the right angle
Eh?
Ehhhh?
 
Another failed joke. Oh well :-)
 
Attempted pun on original and origami
 
oregano?
 
8:25 AM
@JohnRennie Oh, I thought you were talking about my pun XD
 
Apparently the tangent space of the field bundle defines the exterior derivative of the ~variational bicomplex~
Of which the variation is the part that projects on the vertical bundle
neat
 
@JohnRennie dude you cant do that
those are so different like wtf
 
@ooolb I just did :-)
 
thats like doing a pun on physics vs physiotherapy
like what
 
Oh no
Also why are those guys defining the Lagrangian on the infinite jet bundle
Do they think I'm gonna do the sine Gordon equation or something
Jesus that paper has the composite bundle $J^r F \to F \to Y \to X$
How many bundles do you need
 
9:34 AM
\o @Blue
 
Anonymous
\o/
 
:-D
 
@Slereah an infinite number of infinite bundles, obviously :P
 
Anonymous
Could someone tell me what "open" and "closed" cluster mean, in a graph (w.r.t graph theory)? I can't find any relevant definition on the net
 
Anonymous
They just say it is maximal connected set of "open" edges of a graph....I don't understand what "open" edge of a graph means
 
Anonymous
9:44 AM
"closed" edge might still make sense
 
@Blue Isn't an open edge one that only connects to one vertex (and it doesn't loop back to 'touch' the vertex twice)? It's been a few years, so I may be very wrong
(I remember such an edge being used, but I've completely forgotten what it was called)
 
Hm, how do I write the set of open sets on a manifold
$\tau(M)$?
For the topology
 
Anonymous
@Mithrandir24601 Isn't an edge, by definition, one which connects two nodes/vertices/points of a graph?
 
Anonymous
Maybe they just mean that edge is absent
 
Anonymous
And are calling it open edge
 
Anonymous
9:54 AM
But then the meaning of open cluster is confusing
 
@Blue generally yes, but in the likes of QFT, you want a way to represent incoming/outgoing particles, which only connects to one vertex, so you need another term for this - I've no idea if this is an 'open edge' or not though :/
 
Good idea, bring up QFT :p
That will simplify things
 
have you seen this @Blue?
 
Anonymous
 
Anonymous
9:58 AM
Damn, how bad can typography be....
 
@lılostafa They've changed the text in parenthesis. Yesterday it said something like "completed the annual survey, and provided your stackoverflow account!"
now it says your responses are anonymous
 
you have been "anonymized" :P
 
@Blue I love old physics/math books that I find in the university library..
 
@Blue are 'r' and 's' two separate graphs that have been connected together or something?
 
Did you see this‌​? @Blue
The story of 4 Indian mountaineers trying to summit Mount Everest, that were abandoned by their guides and left to die on the mountain
and remained there for 1 year
 
10:06 AM
How sweet of them.
 
really great journalism by the NYTimes
 
The link is broken, btw.
 
Anonymous
@Mithrandir24601 I'm still trying to decipher it. They defined those waaaay back
 
Anonymous
10:09 AM
Page 221
 
Anonymous
You'll get it on libgen :P
 
@Blue Is that how to brew coffee/amphetamines
 
Anonymous
Yeah, that would be a nice application (as mathematicians would say);)
 
So apparently Weyl came up with a lot of this 'affine connection' stuff
Physicist invents abstract math shocker
 
Anonymous
@lılostafa Ah, that's awful :(
 
Anonymous
10:20 AM
I didn't know that
 
Anonymous
Last year several soldiers had died in the Ladakh region due to an avalanche. That plane near the Himalayan range is quite a dangerous place to stay long
 
Not fair to say he was just a physicist tbh
 
10:49 AM
@lılostafa I would be cautious about stories like that. We don't know what happened. There have been similar incidents where climbers insisted on continuing when the guides said it was too dangerous.
 
[Random question]
Consider a black hole that is devouring matter and thus the surface area of its event horizon is growing
From the view of the stationary observer orbiting sufficiently far form the black hole to feel no time dilation, taking account of any time dilation that can be experienced near the vicinity of the black hole, how does one calculate the rate of growth in area of the event horizon?
 
11:04 AM
Also climbing a mountain because "it is there" is to risk your life doing something you love...
 
@Secret From the perspective of the external observer no event horizon exists. The horizon takes an infinite time to form.
 
How's the weight graph looking these days?
 
I see... so the black hole can never grew large enough to reach the orbit of the stationary observer from the stationary observer's frame of reference, but is that also the case when seen in other frames of references?

I am not sure how to ask these questions, spacetime acts in very nonintuitive ways that distance in the usual sense makes no sense so perhaps the notion of how far the event horizon is to any observer simply don't make sense as a notion because to them the black hole event horizon never formed in finite time...
The only best guess I have is that they will see nothing happen until the event horizon (seen in some suitable reference frame) become so large that the observers are now suddenly inside the event horizon
 
11:20 AM
Help I can't reproduce the Michelson Morley formula
Special relativity is wrong
\begin{eqnarray}
t_1 &=& \frac{D}{c-v}
t_2 &=& \frac{D}{c+v}
\end{eqnarray}
So \begin{equation}
t_1 - t_2 = 2D \frac{c}{c^2-v^2} = 2 t \frac{1}{1-\frac{v^2}{c^2}}
\end{equation}
But Michelson gives it as $$\approx 2t \frac v c $$
The Michelson–Morley experiment was performed between April and July, 1887 by Albert A. Michelson and Edward W. Morley at what is now Case Western Reserve University in Cleveland, Ohio, and published in November of the same year. It compared the speed of light in perpendicular directions, in an attempt to detect the relative motion of matter through the stationary luminiferous aether ("aether wind"). The result was negative, in that the expected difference between the speed of light in the direction of movement through the presumed aether, and the speed at right angles, was found not to exist;...
"Michelson obtained this expression correctly in 1881, however, in transverse direction he obtained the incorrect expression

$$ T_{t}={\frac {2L}{c}}$$"
Bloody Michelson
 
@JohnRennie Yeah, in this case, it was actually the climbers' fault, but the guides were more prepared physically and could come down and survived.
@skullpatrol I was quite surprised that a lot of (actually most of) the comments on that article said the same thing! Some even said that no one should be allowed to climb Mount Everest
because, they argued, so what?
 
Yeah, I have my doubts about people who do that sorta stuff...
...as adults we should know better, in my opinion.
@Slereah have you seen this^ book?
 
11:37 AM
Why, because it has French in the name?
 
Nah, because it's a classic.
:-)
 
I learned special relativity from a book nobody ever heard of
I don't even remember where I got it from
(Book 2 is quantum mechanics)
 
French's book begins with the Michelson-Morley experiment.
 
not a bad starting point
if you're going the historical route
 
History motivates.
 
11:46 AM
It may be more confusing than anything if the historical solution was wrong
Really I'm not sure I approve of teaching wave particle duality :p
or relativistic mass
 
Yeah, relativistic mass is briefly discussed too.
In terms of E = mc^2
 
@Slereah Nice
 
@lılostafa That was 6 months ago
2
 
@Slereah Yeah
OK
 
:-)
 
11:53 AM
OK getting back to work after watching this youtube.com/watch?v=VHoT4N43jK8
 
The Michelson-Morley experiment was made to measure the effect of the "aether."
 
that it was
 
Anyway, it's a good book.
 
12:06 PM
Hey I did a refraction experiment with 2 coins and water. I put water in this container and put one of the coins in. I then moved the other coin up and down the container to estimate the height where the two coins looked the same size. If I did this at a few water heights, why would the gradient of this line be the refractive index?
refractive index of water
 
12:55 PM
@ACuriousMind @0celo7 @BalarkaSen is a horizontal curve just a curve that only intersects every fiber at most once
 
2
Q: How do Black Hole event horizons grow?

Alexander RomanI was trying to understand how matter falls into black holes, and I got confused by this thought experiment. A small mass falls into a black hole (which negligibly effects the Schwarzschild radius) A sufficiently long time later (as measured by a distant observer) a large mass falls into the bl...

hmmm... an expanding horizon in these coordinates may look like this? :
 
@Slereah no - given a horizontal subtangentbundle (I. E. A connection), a horizontal curve is one whose tangent is horizontal at all points
 
grr, intuition is completely not helping in trying to understand black holes with growing event horizons...
Diagram description: (Color coding same as that in the PSE quoted) trying to understand what a black hole with a growing horizon due to feeding look like to an external observer and whether the horizon will grow large enough to cause the external observer to be engulfed by the horizon
The trouble is that any external observer of the black hole will not even see the horizon forming, let alone growing, so I guess they will not realise anything happen until the horizon grow enough and cause them to be now inside the horizon?
 
1:14 PM
@ACuriousMind Isn't that equivalent?
 
> The case of non-constant mass is described by the Vaidya metric. Mathematically this is described on pages 133-134 of this book.
 
Basically that the curve doesn't go along the fiber
 
O whoops, looks like we need another metric to describe a growing black hole...
 
Oh wait
I guess you mean like
100% in the horizontal space
So that it's not a combination of H and V
It's a vector that "points" to the next fiber
normal vector to the fiber sort of thing
 
You need a connection to define the horizontal space
 
1:20 PM
0
Q: Do physical models of theories give a good picture of reality?

descheleschilderI'm not sure if this is the right place to ask, but nevertheless, I ask the question. Ther are various physical models to make visible how a theory works, for example: Falaco solitons, see also here, where it is said that the swimming pool model corresponds to black holes and cosmic strings W...

Primarily opinion-based? Too broad?
 
@0celo7 I know
 
@Slereah I had nightmares about ADM
 
btw if you take the tangent space of $T\Bbb R$, at every point it has several possible horizontal space (parametrized by some angle)
Are they all equivalent via a new trivialization?
Since 1-manifolds are all flat
I am guessing so
@0celo7 time for a break probably
 
0
A: Is this answer stating that an external observer can see a black hole mass grow, correct?

John RennieThe point Luboš Motl makes in the answer you link is that the infinite time to reach the event horizon is calculated using the Schwarzschild metric. However the Schwarzschild metric is a time independant solution i.e. it only describes a black hole that has existed unchanged for an infinite time ...

uh.... still open question...
grrr
Part of the reason why GR is a lot more non intuitive to me compared to quantum mechanics (besides the fact that GR maths involves more entities with a lot more degrees of freedom like tensor algebra) is because the metric is changing. Most of my comprehension of concepts rely on the notion to be able to calculate or mentally estimate some notion of metric between points in parameter space. GR takes away that intuition and thus I cannot even easily check my answers on the back of the envelope.
 
1:43 PM
"The proof of this theorem involves some results about differential equations, which
I will not state here. The words “existence” and “uniqueness” are probably involved.
Perhaps also “Picard-Lindel¨of Theorem”."
:D
 
@Slereah Depends on your definition of horizontal
 
$T_e E = H_eE \oplus V_eE$
 
That's called choice of a connection. That defines one notion of horizontal for general vector bundles.
Horizontal could mean many different things in many different contexts
But yes, in that case it's what ACM said
 
implying Balarka knows geometry
 
Just because it intersects every fiber at most once doesn't mean it's everywhere tangent to the horizontal subbundle, btw
@0celo7 I do?
 
1:49 PM
Yeah I figured
It just means that its projection on $VE$ is zero?
 
What you gave is a 0th order condition. Being horizontal is a 1st order condition :)
On each tangent space, you could say, sure
 
Also more importantly
what the hell does that have to do with a connection
Or do only principal bundles get to have a derivative from a connection
 
If $E/M$ is a vector bundle, a choice of a subbundle transverse to $VE = \ker dp$ is exactly what a connection is
You can show it's equivalent to the ten million other versions
 
I know, but can you define a covariant derivative just from that
 
Since when does one write a bundle as a fraction
 
1:52 PM
is my question
 
Hey @JohnRennie are you there?
 
I guess you can maybe do a "derivative" by doing the usual derivative definition along a horizontal lifted curve?
 
@Slereah If $E = TM$, you can indeed.
That's right
 
That’s the covariant derivative
 
Where does the frame bundle factor in
 
1:56 PM
The general point is that horizontal lifts are exactly the parallel vector fields
along the base curve
 
Is the parallel transport of a vector $v \in TM$ just the values that the horizontal curve starting at $v$ takes?
 
It’s the principal bundle associated to the tangent bundle
 
@Slereah Answered by future-sniping
 
Damn time travelers
So is the notion of parallel transport somewhat more primitive than the covariant derivative?
(at least with that definition)
 
So they say
 
2:00 PM
They’re equivalent notions so who knows
 
Do you get that thing where you google a thing and the link contains maybe one of the word you were searching for
Stop trying to second guess me google
 
Did you mean "Stop trying to guess google"?
 
Oh they don't even do that sometimes
They just say "This result doesn't have that word but we include it anyway"
 
google is not a great search engine
use bing
:dabbing in the background:
 
2:16 PM
Sorry I only use Ask Jeeves
The gentleman's search engine
 
isn't it just called Ask now
Ask is a fucking annoying search engine
 
alas yes
No more jeeves
Too silly an idea for the modern day corporate blocks that are search engines
"In more sophisticated terms, such an assignment of horizontal spaces satisfying these properties corresponds precisely to a smooth section of the jet bundle J1E → E."
wot
 
J E T S
 
@BalarkaSen why did you say that $E = TM$
I thought the point of the connection was to be defined on the principal bundle
 
2:19 PM
If you're talking about covariant derivative
you'd better be working on the tangent bundle
 
'"Suppose that E is a smooth principal G-bundle over M. Then an Ehresmann connection H on E is said to be a principal (Ehresmann) connection"
etc etc
I thought the covariant derivative was on the frame bundle
and that you could then apply it to the tensor bundle
via math wizardry
 
if you have a general vector bundle you don't really call it the covariant derivative anymore
the right notion is the exterior covariant derivative :3
 
Plus the frame bundle isn't a vector bundle :p
 
true
you can always pass between frame bundle and associated vector bundles anyway
 
"A connection on a principal bundle allows us to define a covariant derivative (a.k.a. a Koszul connection) on sections of any associated vector bundle. "
Hm
@BalarkaSen solder form thing?
 
2:22 PM
I'm future sniping you
snipe of the future past
@Slereah Connection form, rather
 
I suppose so, since you're gonna need it for associated bundles in general
Even if it's not the tangent bundle
like the spinor bundle with the gauge bundles
Hm, I guess that's why the associated bundles are actually $(P \times V) / G$?
That way the principal connection acts on it
Hence why gauge fields are $G$ valued and all that business
 
@BalarkaSen that’s something different
Namely for bundle-valued differential forms
@Slereah gauge fields are g valued
 
That's what I said
Or is uppercase verbotten
 
g means Lie algebra
 
2:29 PM
$\mathfrak{g}$-valued
 
I need to writes n o t e s on the rotation number
 
What is the geodesic for a principal bundle
Is it just the field value along that curve
Or... field lines???
I don't know
 
You’ve gone off the deep end
 
Am I the only one who's completely nonplussed by this?
 
I just want the people writing those things to offer a clear list of associations
 
2:32 PM
"Stephen Hawking releases graduate thesis, promptly breaks internet"
 
between the concepts and the gauge stuff
 
a.k.a. "Stephen Hawking finally gets round to doing something decent with his thesis copyright, the internet somehow thinks this is important"?
 
"In Chapter 1 it is shown that this expansion creates grave difficulties for the Hoyle-Narlikar theory of gravitation."
lol Hoyle theory
 
@Slereah wot
 
you could say that that theory did not go according to Hoyle
 
2:35 PM
@0celo7 What mathematican concept corresponds to what physical concept
 
Read the books by Naber on gauge theory.
 
I would read such a thing too
 
Let me check this legally
Hawking's thesis is the worst
Typewriter + handwritten equation
You'd think he was already in a wheelchair
Naber does seem to have a "physical motivation" part
 
what's a badass font that i can use in sharelatex
 
microgramma
Microgramma is a sans serif font which was designed by Aldo Novarese and Alessandro Butti for the Nebiolo Type Foundry in 1952. It became popular for use with technical illustrations in the 1960s and was a favourite of graphic designers by the early seventies, its uses ranging from publicity and publication design to packaging, largely because of its availability as a Letraset typeface. Early typesetters (like the AM Varityper) also incorporated it. Novarese himself later developed Eurostile in 1962, a typeface very similar to Microgramma. Eurostile added lower-case letters, a bold condensed variant...
 
2:44 PM
that does not look like a very professional font
 
it's the Star Trek font
the font of the future
Naber uses $\mathcal P$ for the projection
When they say $\mathfrak{g}$-valued $1$-form, does it just mean that it's a $TP$ $1$-form
One source is implying $$\Omega ^{1}(P,{\mathfrak {g}})\cong C^{\infty }(P,T^{*}P\otimes {\mathfrak {g}})$$
Which seems odd
Doesn't $T^*P$ already have algebra values
Since the tangent vector of a Lie group is an algebra element
 
@Slereah yes, that's the idea
 
2:59 PM
@ACuriousMind I guess you travel along $\tilde \gamma_H(\lambda)$ and pick the point at $\lambda + \varepsilon$ for the derivative
 

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