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01:00 - 19:0019:00 - 00:00

user54412
1:11 AM
@Danu Here's my earlier statement about surface gravity, recast more in line with your notation. Consider a fixed charge Q and varying mass M. What do T and $(\partial T/\partial M)_Q$ look like?
 
user54412
 
user54412
The region between $q = 1$ and $q = \sqrt{3}/2$ has $(\partial T/\partial M)_Q > 0$.
 
user54412
This derivative passing through 0 is equivalent to C diverging, as you can write C as something over this derivative with enough chain rule.
 
user54412
@Danu Another way of looking at this (probably related to all this phase transition stuff) is that normally we expect $T \to \infty$ as $M \to 0$. But as soon as there's any charge at all, $T \to 0^+$ as $M \to Q^+$ along a constant-$Q$ line.
 
user54412
 
user54412
1:26 AM
That there is an extremum in T is in retrospect no more surprising than that $T \to 0$ as the hole becomes extremal (which is, admittedly, weird).
 
1:51 AM
@ChrisWhite I recorded a Let's Play of Morrowind
 
@0celo7 Link pls
 
it's a proof of concept
not recorded in native quality
 
You're like a psychic
Also: my data science thing that I've spent the last 2 weeks on passed their expectations, so I'll be moseying on to the 2nd test
@0celo7 Lol, <30 sec in I see you ignored the Take All button & took dude's stuff one-by-one
 
@KyleKanos I wanted to see what he had...
 
And you're using a dagger
 
1:56 AM
i have nothing else...
@ChrisWhite how the hell do i hit people
 
Well I suppose you could always buy a sword
Or steal one (before or after killing someone, ofcourse)
That was like the first thing I did
Next step was getting a bow & arrow and some armor
This really is bringing back memories
I ought to get this on my Linux box
 
look at 8:15
fucking ridiculous
 
I'm at ~3
Wait...is this right at the beginning?
 
I have like one hour of game time
I've been fooling with mods this whole time
 
Okay
 
2:01 AM
I'll buy a sword.
I have 500+ gold
 
No man, don't buy one.
Find a schmuck with a sword & kill him for it
Or use some magic & blow up some daedric weaponry
There are also swords hidden all over the place
Lol you got rekt
3
Oh that made me laugh
 
I bought a sword and killed him with two hits
 
user54412
@0celo7 Practice on mudcrabs :)
 
2:34 AM
@ACuriousMind holy shit I randomly fired up Skyrim and my armor mod works now!!!!!
 
3:13 AM
This is hard to read: wikipeetia.org/Fluid
2
 
3:26 AM
We are not amused by your "amusing parody of Wikipedia."
Try this @KyleKanos
>8(
 
 
2 hours later…
5:10 AM
@ChrisWhite One can get it from rewriting the metric and comparing to Rindler (identifying something with the Rindler acceleration $a$) or, after analytic continuation and some more substitutions, to polar coordinates and force a periodicity in one of the coordinates. Both are directly coordinate related
@ChrisWhite This is kind of difficult (to interpret) because "phenomenologically" $q$ is what one should fix, not $Q$. A plot of just $\partial T/\partial M$ will look weird because at some point you'll go $|q|>1$ and stuff
So I didn't plot $T(M)$ or its derivative
@ChrisWhite I'm not sure your derivative is taken correctly, as $\mu$ of course also depends on $M$
(or did you take this into account, and just not write it out?)
 
user54412
5:28 AM
There's a lot of scratch work not written (though something still might be wrong)
 
user54412
I stand by my claim, though, that there should be a connection between $(\partial T/\partial M)_Q$ vanishing and C diverging
 
user54412
Besides, why should $q$ be fixed rather than $Q$? Certainly I can take a charged black hole and add neutral matter to it?
 
user54412
The reverse might be more difficult. Does Hawking radiation preferentially deplete charge imbalance somehow? On the one hand it seems like it should, on the other it feels like we should be constrained by the particles that actually exist.
 
5:44 AM
Send Professor Hawking an email and ask :P
Sorry, bad joke^
 
 
3 hours later…
8:32 AM
Hi @Hippalectryon
Did you read that article?
 
 
1 hour later…
9:42 AM
@skillpatrol which one ?
afk
 
10:10 AM
This one @Hippalectryon
 
Yeah I read it
 
What did you think?
 
It doesn't say anything new afaik
 
Doesn't it give you any ideas how to help yourself during exams?
 
Not really
 
10:15 AM
Automaticity could help with learning how to be careful, no?
 
Automaticity doesn't enable one to learn to be careful. It just enables one to do things a more automatic way
 
Indeed, automatically learn to be careful at the beginning.
Step 1 Read the problem carefully and think about its meaning.
That^ should be a "knee jerk" reaction
As I mentioned earlier :-)
 
@skillpatrol Btw do you have any idea on the problem I posted yesterday ?
13 hours ago, by Hippalectryon
Hi! I'm studying a usual linear accelerator for electrons and I'm trying to get the force that corresponds to the power radiated ($P=m\tau \ddot{x}^2$). I've tried calculating the associated work which gives me $W=m\tau\int_0^T\ddot{x}^2\mathrm{d}t=\int_0^T\vec{F_r}\cdot\vec{\dot{x}}\mathrm‌​{d}t$, how do I continue ?
 
I would suggest posting it on the main site.
Just ask for a hint.
 
Sounds too homeworky for PSE. And it should be an easy question :/ I'm just somehow stuck
Which is why I'm asking in the chat
 
10:33 AM
Where have you used Work = Force * distance @Hippalectryon?
 
@skillpatrol $\int_0^T\vec{F_r}\cdot\vec{\dot{x}}\mathrm‌​{d}t=\int_0^d\vec{F_r}\cdot\vec{ \mathrm‌​{d}l}$
 
...and what about Power is the amount of Work done per unit time @Hippalectryon?
 
Isn't that what I used at the beginning ? $W=\int_0^T P(t)\mathrm{d}t$
 
That tells you what Work is equal to, right?
 
yes, in terms of an integral of $\ddot{x}^2$
 
10:43 AM
You are asked for the Force that corresponds to the power.
F = P(?)
 
ugh ? How can a force equal a power ?
I'm asked to find a force that can be associated with the radiation
Basically, when you add that force to the "radiation-less" model, you get the model with radiations
Had the acceleration being constant in the radiative mode I could indeed have used F=PT/d but it's not the case here
 
Can't you ask your teacher?
 
I don't see my teacher until next year
 
Do you have a textbook?
 
Nope, only notes
 
10:53 AM
How about a library?
 
What would I do there ?
The exercise doesn't come from a textbook or anything
 
There must be some substitution...
 
I thought integrating by parts could help but that square is troublesome
I basically want to transform that $\ddot{x(t)}^2$ into $f(t)\dot{x(t)}$
 
How about a change in variable?
 
:O $u=\dot{x}$
Wait no that doesn't work q_q (it does yield a result but no $\dot{x}$ appears)
 
10:59 AM
Maybe even F =ma is used somewhere
I gotta go :(
 
Sorry
 
Nah you tried to help me, thanks ;-)
 
Later pal
 
See you
 
11:17 AM
@KyleKanos I'll try my hand at streaming tonight so you can lol some more at my shittiness
 
11:51 AM
@xXx_based_dolan_xXx nice user name
 
 
1 hour later…
1:00 PM
@0celo7 Hmm. EVO is tonight (11a to 11p Eastern), so that might be tricky :/
 
1:12 PM
@KyleKanos you really think I can get a video and audio feed working in one sitting?
 
AFAIK, it's pretty simple on Windoze
 
Do you know if twitch streaming is free?
 
I believe it is free
Can't imagine too many people streaming if they had to pay for it
They also have a list of common broadcast software: twitch.tv/broadcast
 
Hello, are here any chat netiquette I should know, or can I just ask my question?
 
@Luke Just ask
If someone's interested, they'll respond. If not...well try again later when others are on?
 
1:21 PM
I am doing an exercise in basic quantum mechanics. I should show that Π := X - t/m P is a conserved quantity. First Idea was that it has to commute to the Hamiltonian if I recall correctly
but that led me to problems regarding the dimensions
I ended up at showing 0 = ΔX – XΔ
which does not make any sense to me in 3D
because the laplace operator maps to 1D, but X multiplies by the position vector yielding something 3D
 
Correct, commutation with Hamiltonian means conservation--the relation is dA/dt = [A, H] so [A, H]=0 means dA/dt=0
 
I forgot to mention it was about a free particle, so H = p²/2m
 
So you'll have [X - aP, H] = [X, H] - a[P, H]
(a=t/m, obviously)
 
that's how I started, yes
and since H = b P², [H,P] = 0
 
So your issue is just on the first term?
 
1:32 PM
indeed. ⇒ [X,H] = 1/2m(XP² - P²X)
which is, denying coefficients, the problem with Δ I explained.
 
Well don't forget that [A, BC] = [A, B]C + B[A, C]
Then recall that [x,p] = ihbar, no?
 
Kyle doing quantum mechanics?
 
⇒ [X,P²] = [X,P]P + P[X,P]
 
hm, that seems rather trivial @KyleKanos, I wonder how I got to my conflict there.
but thank you
 
1:35 PM
Surely
@0celo7 I also have answered a few QFT questions too ;) (sadly, one is mislabeled (purely QM, no QFT) and one was really just a math question
 
@KyleKanos I don't have a dedicated USB mic
Will the mic on my phone earbuds work well enough?
 
@0celo7 You can't use built-in one?
@0celo7 Possibly.
 
@KyleKanos maybe
Not at home, can't check
I'll use whichever has the best quality I guess
I hope streaming doesn't bring me below 30 fps
I have no problem with 30
@KyleKanos huh
@KyleKanos I'll install a female nudity mod as an incentive
 
1:54 PM
@0celo7 Meh, just mod me & I'll be content
(i.e., make me moderator, not modify me)
 
There will be maybe two people in there
 
So?
 
It's going to be the official H Bar vidya stream
@KyleKanos I don't want you banning the other person
 
I probably wouldn't do much with moderator powers in a chat
 
then why do you want them?
be warned: now that I got all of my Skyrim mods to work, I'll probably stream that
 
2:09 PM
@0celo7 S&Gs
 
@KyleKanos pls define
 
Shits & Giggles
 
my precalc teacher said shiggles
"why do we have to square 234?" "shiggles."
 
holy shit I had no idea this chat was a thing
 
no cussing
there are children in here!
 
2:13 PM
eh about time children learned colorful vocabulary ahead of time
 
2:47 PM
@0celo7 lol :-P
 
@DavidZ it's no laughing matter
 
3:18 PM
 
Yes
 
How long is it?
 
8 pages
 
Can you please see if he gives something like velocity = hyperbolic functions?
 
Yes he does
 
3:23 PM
There's something I've always been meaning to ask
 
Is there any possible way you could share how he comes up with that?
 
@0celo7 $U^\mu=(\cosh(\alpha\tau))L^\mu+(\sinh(\alpha\tau))M^\mu$
 
@FenderLesPaul "how does X troll have so much rep" cannot be answered
@KyleKanos I know that, I'm at a loss trying to derive it :/
 
It's the "obvious first integral" of $DA^\mu/d\tau=\alpha^2 U^\mu$
with $\alpha=\rm const$
@FenderLesPaul I don't think he's insane, he just holds rather non-standard positions on things
 
$\alpha^2=A^\mu A_\mu$?
 
3:25 PM
Are you going to write the Putnam? @0celo7
 
@skillpatrol no
I'm bad at math
 
@0celo7 section 6.2 of MTW
 
@FenderLesPaul is that in curved spacetime
 
@0celo7 Yes, he does say that
 
@0
oops
 
3:27 PM
Also, with his notation, $DA^\mu/d\tau\equiv {A^\mu}_{;\nu}$
 
@0celo7 ah no it's in flat space-time, sorry
 
@KyleKanos Not $U^\nu A^\mu{}_{;\nu}$?
does he say how to get that equality?
 
No, the line is $U^\mu=\frac{dx^\mu}{d\tau},\quad A^\mu=\frac{DU^\mu}{d\tau}=\frac{d^2x^\mu}{d\tau^2}+{\Gamma_{\nu\sigma}}^\mu\fra‌​c{dx^\nu}{d\tau}\frac{dx^\sigma}{d\tau}$
 
that's all standard
I need the $DA/d\tau$ line
 
I already said it: $\frac{DA^\mu}{d\tau}=\alpha^2U^\mu$
I was just pointing out that the $D/d\tau$ was the covariant derivative; wasn't sure if you knew that
 
3:33 PM
@KyleKanos yes, that's standard
@KyleKanos no clue how to get that...
 
@0celo7 TIL...
 
unless
 
Oh shit, I lied to you. $\alpha^2=-A^\mu A_\mu$.
He says,
> Thus, the analog of a plane curve of constant curvature will be characterized by the diff. eq.'s
$\beta^\mu=\frac{D}{d\tau}\left(\frac{A^\mu}{\alpha}\right)-\alpha U^\mu=0,\quad-\alpha^2=g_{\mu\nu}A^\mu A^\nu$
 
3:50 PM
hmm
how the heck do you get that
 
$\beta^\mu=i\Omega B^\mu$ where $\Omega$ is the torsion (or second curvature) and $B^\mu$ the unit binormal (or second normal)
 
Does he say anything about calculating $DA/d\tau$?
 
Nope, just that it has an obvious first integral
 
fuck him too
ugh
any idea how to derive this?
 
Given the definition of $A^\mu$, he's saying $\frac{D^2U^\mu}{d\tau^2}=\alpha^2U^\mu$
Sans the 4-vector bit, that's really an $x''=\omega^2x$ equation with known solutions of hyperbolic functions
Isn't it?
 
3:56 PM
yes
I don't know how to get that equation to begin with
 
18 mins ago, by Kyle Kanos
> Thus, the analog of a plane curve of constant curvature will be characterized by the diff. eq.'s
$\beta^\mu=\frac{D}{d\tau}\left(\frac{A^\mu}{\alpha}\right)-\alpha U^\mu=0,\quad-\alpha^2=g_{\mu\nu}A^\mu A^\nu$
 
well I don't know how to get those either :P
 
Apparently there's an analogy to the Frenet-Serret equations
 
@KyleKanos do you see any quick solution to this?
 
I'm somewhat familiar with those
 
3:58 PM
6 hours ago, by Hippalectryon
13 hours ago, by Hippalectryon
Hi! I'm studying a usual linear accelerator for electrons and I'm trying to get the force that corresponds to the power radiated ($P=m\tau \ddot{x}^2$). I've tried calculating the associated work which gives me $W=m\tau\int_0^T\ddot{x}^2\mathrm{d}t=\int_0^T\vec{F_r}\cdot\vec{\dot{x}}\mathrm‌​{d}t$, how do I continue ?
 
@KyleKanos would it fall under fair use to share the relevant pages?
 
@skillpatrol Quick, no. It's actually a kinda complicated thing
 
Thanks for replying
:-)
 
Well I guess not that complicated...this guy did it with all the units in it
 
reads like the typical PSE post
 
4:04 PM
@KyleKanos great thanks :D
 
dude streng theory is so dope
 
@0celo7 According to this site, whole pages probably would not fall under fair use. I can make whole quotes though
 
@KyleKanos I need enough to reconstruct the proof. As it stands I'm not very far.
@KyleKanos How does he define the binormal and the torsion?
and which one is zero so $\beta=0$?
and what is the random $i$ doing there?
 
@0celo7 He doesn't, he just states them
 
so how does he show $\beta=0$
 
4:12 PM
Via the claim
> The true generalization of the characteristics of straight lines and plane curves are obtained not by requiring the scalar curvature or torsion to vanish, respectively, but by requiring the curvature or torsion vector to vanish component-wise.
The torsion vector being $\Omega B^\mu$
 
and that's not defined anywhere?
 
It is: $$\Omega B^\mu=\frac{D}{d\tau}\left(\frac{A^\mu}{i\alpha}\right)+i\alpha U^\mu$$
 
wtf
how the hell does he get that??
 
By analogy to $$\mathbf{t}=d\mathbf{r}/ds,\quad\kappa\mathbf{n}=d\mathbf{t}/ds,\quad\omega\mat‌​hbf{b}=d\mathbf{n}/ds+k\mathbf{t}$$
 
He references a book publishe in 1949 by Synge called "Tensor Calculus"
published*
I have no idea where the factors of i come from in that analogy though
 
4:19 PM
Those equations, btw, are standard formulas of the differential geometry of twisted curves in Euclidean 3-space
 
@KyleKanos what is k?
 
Sorry, that's a kappa at the end there
Which is curvature
 
wish I had my curve geometry book with me...
 
@0celo7 is this related to a project or just for fun?
 
@FenderLesPaul I fucked up an answer and I have to learn about accelerated motion in curved spacetime to fix it
one more month and I could go to the university library
 
4:22 PM
@0celo7 ah ok
 
Are you excited?
 
the chat notification sounds terrifying holy shit
 
yes
I turn it off
 
Dammit...Brandon's going to beat me to gold badge on LA :(
 
@0celo7 are you from the US, if you don't my asking?
 
4:24 PM
He's got a 250 review head-start
 
@FenderLesPaul read my bio
should say there
 
Click on the speaker in the upper right hand corner.
 
Well it's lunch time...I'll bbl
 
@ACuriousMind you're on the top GR users list, ahead of me now
 
nuclear engineering; what the fuck?
 
4:25 PM
@KyleKanos k
 
sorry :p
 
the chilluns!
you ruin their minds
 
ah Tennessee
cool
 
@FenderLesPaul read: applied nuclear physcis
 
I actually did a double take when I saw it said nuclear eng given your interest in GR haha
 
4:27 PM
I'm taking courses that allow me to branch out, should the need arise
 
but that's cool dude at least you get to study GR for fun and at the end of the day secure a job
 
I'm just not interested in a career in academia
 
that's fair
so you start this fall then?
 
yes
 
4:29 PM
3
A: How long can a particle survive inside of the horizon of a black hole?

0celo7A particle cannot survive in region II indefinitely. Indeed, there does exist an upper bound on the survival time of the particle. As soon as the particle crosses the horizon into region II, its remaining proper time until it reaches $r=0$ is bounded by $$\tau_\mathrm{max}=\frac{\pi GM}{c^3}$$ W...

^^is incorrect
It is possible to strategically fire rockets and live marginally longer.
I want to write a mega answer explaining the paper John Rennie linked on the OP
@KyleKanos those are the 3-space equations, yes
however, $\vec b$ is defined using the cross product
 
Is that true? I'd look forward to reading it; the answer of $\pi M$ is one that was given to us in a HW problem at one point so I'd be curious as to when it can be circumvented
 
no clue how to define it in 4 dimensions
 
Presumably using the levi-civita symbol contracted with the 4-velocity of the comoving frame
He doesn't define it in the paper though
 
@FenderLesPaul the theorem from HE I applied (a very rigorous statement of the heuristic that geodesics are maximums of proper time) does not apply! It only applies curves connecting the same spacetime points, that means both the space and time coordinates of the points have to be the same. However, it is possible to accelerate in just the right way and land further along in coordinate time. Since you hit the singularity at a point in spacetime that cannot be reached by a geodesic, it's perfectly...
...fine that the geodesic is shorter
@FenderLesPaul Cornell?
 
I see; certainly I'd like to see your detailed answer if/when you write it :)
Indeed
 
Oh cool, thanks!
 
the paper is understandable, but it relies on Rindler's work in eqs. (10), (11)
 
ah ok
 
HE = Hawking & Ellis
 
so many distractions!
:p
 
4:45 PM
@FenderLesPaul what are you interested in?
 
Other than Zeppelin :P
 
haha
physics wise you mean?
 
@FenderLesPaul @KyleKanos Does he give an explanation of why he thinks the binormal should vanish?
@FenderLesPaul yes
 
classical GR as a whole but specifically self-force problems and black hole perturbations, although currently my professor has me working on this quais-local rigid frames calculation in relation to these "super-rotations" in the BMS group
 
@0celo7 With $\Omega B^\mu$ vanishing, then we have a plane curve (of constant curvature)
 
4:54 PM
and also aspects of QG related to entanglement entropy, black hole information, scrambling and Ryu-Takyanagi-things of that nature
quasi*
 
@KyleKanos plane curve?
stupid question
@KyleKanos why is constant curvature necessary?
 
@0celo7 Does this mean you're retracting the above question?
 
@KyleKanos no
In mathematics, a plane curve is a curve in a Euclidean plane (compare with space curve). The most frequently studied cases are smooth plane curves (including piecewise smooth plane curves), and algebraic plane curves. A smooth plane curve is a curve in a real Euclidean plane R2 and is a one-dimensional smooth manifold. Equivalently, a smooth plane curve can be given locally by an equation f(x, y) = 0, where f : R2 → R is a smooth function, and the partial derivatives ∂f/∂x and ∂f/∂y are never both 0. In other words, a smooth plane curve is a plane curve which "locally looks like a line" with respect...
"curve in the Euclidean plane" does not compute
plane curve in curved spacetime?
 
Looks like a line along a set of coordinates?
 
what does that mean?
furthermore, why do constant acceleration worldlines have this property?
 
5:01 PM
> The vanishing of the "curvature vector $A^\mu$ is the well-known characteristic of a geodesic path.
 
for a geodesic $A\equiv 0$
literally the definition...
this might make a decent PSE question
@Jimself @ChrisWhite Unless you guys know anything about accelerated observers in curved spacetime
 
@0celo7 Asking why $\beta^\mu=0$ is needed?
 
@KyleKanos yes
And asking how valid this whole analogy is
@KyleKanos I can derive these
 
You want me to ask since I have the paper? Or do you want to ask since it's your interest?
Or wait for Chris and/or Jim to chime in?
 
5:16 PM
@KyleKanos yes
 
Okay
 
You think the paper is being unclear too?
 
I think it's more beyond my current level of knowledge than anything else
 
what does he say about the torsion?
 
That it vanishing along with the curvature means a plane curve
 
5:20 PM
I assume he doesn't explain why or how?
@KyleKanos wait, but the vanishing of the curvature means a geodesic
 
> In the differential geometry of twisted curves it; is well known that the vanishing of the curvature of a curve implies that the curve is a straight line, and the vanishing of the torsion implies that it is a plane curve
 
what does a constantly accelerating curve have to do with plane curves?
constant curvature -> constant acceleration, right?
 
Well he does also say,
> It turns out that any curve so characterized will be time- like along its entirety if the initial direction is chosen timelike.
 
5:37 PM
@KyleKanos this is true
1
Q: A space curve is planar if and only if its torsion is everywhere 0

MikeCan someone please explain this proof to me. I know that a circle is planar and has nonzero constant curvature, so this must be an exception, but I am a little lost on the proof. Thanks!

 
6:21 PM
0
Q: Double-slit experiment with one electron per day

FarI am a mathematician and i am studying string theory. For this purpose i studied quantum theory. After reading Feynman's book in which he described the double-slit experiment (Young experiment) I was wondering if i send one electron per day or per month (even more), could i see the interference p...

 
6:34 PM
@FenderLesPaul @KyleKanos Related: journals.aps.org/prd/abstract/10.1103/PhysRevD.3.1035
 
6:46 PM
oh that's a cool paper, thanks!
there's a related paper by Don Page if you're interested
also this paper by vishveshwara
 
I called the Library of Congress and ordered the issue of Physical Review that article is in.
I'm hardcore.
 
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