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17:00
@0celo7 Well, in combination with an absymal lecturer
@0celo7 Schutz isn't really a book for people who want to be rigorous about GR
@JohnRennie Also of course his treatment of "group theory" is garbage.
Is there any group theory in Schutz's GR book?
(this is about Schwartz)
About Schutz---I also dislike it. It's too elementary
Is that the one that doesn't even derive the geodesic equation?
17:02
I feel like, if you need Schutz' book to teach you GR (and are unable to understand it from e.g. Carroll), you probably shouldn't be doing GR yet.
Similar story with e.g. Zwiebach's string theory book.
@Danu tbh none of the ST books are good
As most people here know, I'm very much opposed to rushing into advanced topics without basic understanding of the prerequisites.
@Danu Honestly though, ST books are all kinda bad
@ACuriousMind :)
I haven't really read any yet: Did you try Lüst's book?
His lecture, which I am currently attending, is based on it.
It's non-rigorous, I realize that.
so ACM won't like it
but @0celo7, did you read it?
17:04
@Danu BLT?
The one I have, on my shelf?
It's very dry. Partition function after partition function.
Maybe that's what string theory is.
@0celo7 : I know. But there is other stuff out there on things like Dirac's belt and spinors.
Incoming!!!!!!!!!!!!!!!!!!!!
@JohnRennie MY BODY IS READY
wtf
@JohnDuffield What does the Dirac belt have to do with anything, again?
17:08
@Danu I think that's the one I'll try after I'm no longer furious at BBS for being garbage :P
@ACuriousMind I think it's the closest to rigorous
@0celo7 : spin ½ particles. Follow the links, do your own research: "an object must be translated around the loop twice in order to be restored to its original position and chirality. In this sense a Mobius strip is reminiscent of spin-1/2 particles in quantum mechanics..."
smh
@Danu I think I know its first half already
user54412
@Danu What then should those people do? I've always been of the opinion that GR has no prereqs beyond some linear algebra and calculus, so I can't imagine what else you could take to prepare for it.
17:11
The guy who wrote the notes my ST course was following was one of Lüst's PhD students and closely followed BLT in writing the notes
@JohnDuffield John, I think you would do really well to just read a book on Lie algebras. Especially one for physicists, where they explain how $SU(2)$ and $SO(3)$ are related. You're getting sidetracked into some crazy stuff by this, in principle, not too complicated little fact.
Can we please not fill this chat room with another iteration of a discussion with JohnDuffield that does not accomplish anything?
@ChrisWhite Some ideas about Lagrangians
Multilinear algebra
(so tensors)
@JohnDuffield how is supersymmetry due to a lack of understanding of electrons if it applies to all particles?
@ACuriousMind That was going to be my only message, I swear!
user54412
17:14
@Danu Lagrangians. So it has come to this.
Sigh. I know why my ODE test was so hard. The integral of $1/x^2$ isn't $-1/(3x^3)$. I'm pretty much mentally retarded.
@ChrisWhite Not Lagrangians per se---I mean "theoretical mechanics"
@0celo7 Reset to Calc. 1?
I did the power rule wrong on the whole test.
@Danu I guess...
17:16
@0celo7 That's a pretty serious mistake :P
@Danu No fucking shit
I even went back and changed the correct stuff.
@ChrisWhite Also what's so bad about mentioning Lagrangians
@Danu : no I'm not getting sidetracked into crazy stuff. Dirac's belt and spinors is not crazy stuff, and nor is electron diffraction and the wave nature of matter. Thinking that E8 is some theory of everything is getting sidetracked.
That's the kind of mistake that should force one to shift emphasis onto Thomas/Stewart/Piskunov calculus to master the basics, no shame in taking one's time
I've never made that mistake before.
And today, on a freaking test, I do it on the whole thing?
17:19
@JohnDuffield do you understand how supersymmetry arose?
Or any of the things people think justify it's existence?
@0celo7 It's your call whether this "means" anything or not, but I'd give it some serious thought
@Danu And do what?
I got a near perfect score in calculus.
user54412
@Danu I'm not against Lagrangians -- everyone should know them. But I've always felt GR is over-inflated in terms of requirements, being treated like only the most advanced undergrads can handle it. It may be hard, but you don't need to know field theory or E&M or thermodynamics to do the fundamentals of GR.
I only missed one question on the AP test.
My homework to this point has been flawless.
@ChrisWhite Depends what you mean by the fundamentals
17:20
I did 3 tests to prepare for this.
All perfect.
@0celo7 your call, as I said
Then this shit?
@bolbteppa : supersymmetry proposes a selectron without understanding what an electron is, or how gamma-gamma pair production actually works to convert two bosons into two fermions, or what the difference between a boson and a fermion really is.
No need to convince me
What is there to call?
17:21
@0celo7 have you tried talking to the prof, explaining? You never know unless you try...
@ChrisWhite What are "the fundamentals"? Solving geodesic equations for given metrics?
@TerryBollinger Explain what?
That I'm stupid?
That'd be about as insightful as the "electromagnetism is solving PDEs with boundary conditions"-approach most EM classes devolve into
@ChrisWhite I have this (fairly radical) point of view that it's better to wait until you're ready to really understand the general ideas. It's not about calculating, but about some kind of hard-to-define "maturity" that does, in my experience, come from really doing all the more simple stuff first.
@0celo7 You're not stupid, you made one cascade error. Flaw of grading methods in that it amplifies that one error.
17:22
Of course, one can handle GR as in pass a class in it quite simply
user54412
@ACuriousMind I'd say intuitively "getting" spacetime as a manifold.
That doesn't mean that you really know what's going on
@TerryBollinger So what is @Danu talking about?
@ChrisWhite So you'd have to know basic differential geometry, too?
What is there to think about?
I messed up the product rule for inverse powers.
17:23
@bolbteppa : of course I understand how supersymmetry arose, and why people try to justify it. But do you understand that there's no point proposing a selectron if you don't know what an electron is?
@ChrisWhite I'm not sure the coordinate-laden approach that is necessary when you only know calculus is good for understand what exactly a manifold is.
Obviously I must have some massive deficit if it warrants a serious thinking.
user54412
@Danu Sure, but I don't know what simple stuff there is. I mean, you can do QFT or thermo on a curved manifold, but that's not fundamental GR. And someone who isn't ready for Carroll won't become ready by studying them.
@0celo7 Can you stop being so dramatic?
@Danu No!
17:24
@JohnDuffield would you say the same thing to Dirac about anti-particles?
The whole confusion about "singularities" and whether they're "real" or "coordinate" singularities basically comes from people not knowing the difference between a chart and the manifold.
@0celo7 Dunno, I just don't think point errors that spread through a test should be graded as multiple errors at every point they touch.
@TerryBollinger It's the same error on multiple questions.
user54412
@ACuriousMind Maybe my opinion is colored by the fact that I learned differential geometry from GR, whereas my math department failed at teaching it.
Not one error throughout a long question.
17:25
@ChrisWhite Of course I don't think people should be able to do (without guidance, that is) QFT in curved spacetimes right after a course on GR (although Carroll DOES do it).
I mean classical field theory
user54412
@Danu And maybe I think you should be able to do magnetohydrodynamics in curved spacetimes right after a course in GR :p
@ChrisWhite and maybe I am
(jk)
Oh...
@0celo7 Ouch, yet still: Sometimes, communicating what happened to the person doing the grading might help in some unexpected way. Often not... but I've absolutely seen cases where it helped.
Hah. I forgot a "don't" in that previous message
[editing]
@bolbteppa : I not sure what you mean. But if I could talk to Dirac maybe I'd make Moebius strips with two different chiralities, then talk about Dirac's belt and spinors, and the Dirac equation and the Dirac spinor.
17:31
@JohnDuffield are you a troll or are you for real? You are pasting identical text...
Can @Danu explain what he means by "give serious thought"
Read a calc 1 book?
@TerryBollinger (DO NOT ENGAGE, DO NOT ENGAGE)
I know what I did wrong, it was a stupid mistake
So why does it require serious thought
@0celo7 Maybe reread the sentence?
17:32
@Danu Thanks, questions answered, will comply!
@0celo7 whether this "means" something
It appears you have already decided it does not
@ACuriousMind : no, the whole confusion about real or coordinate singularities basically comes from people who don't understand GR, and who have never read Einstein's material.
good for you, now carry on with your life
@Danu Ah
I was just...not stressed...excited? I was just nervous.
I think.
@yuggib back on your discussion of trace classes and von Neumann algebras, did you have any good refs or papers on any of that?
user54412
17:35
Raise your hand if you're done with college and remember any grades you got on particular tests.
user54412
::looks around::
I'm still in college and I tend to forget which grades I had on exams that were more than a few months ago
@ChrisWhite ::begrugingly raises hand::
@TerryBollinger I was planning to talk to him later about the extremal problem. I'll try to bring it up.
Also, as I've said before, here MSc. degrees still have grades, and they do matter.
17:37
@Danu ...you're done with college? oO
@ACuriousMind College = bachelor's
user54412
@Danu You don't count.
Also it's easy to remember cause they were all #perfect
(just kidding)
@ACuriousMind We've established that we're completely different.
17:37
@TerryBollinger : am I a troll? Huh? No. And what are you on about saying I'm pasting identical text? I'm giving references for people to follow up. You know, to demonstrate that I'm not making it up?
@Danu I don't think you are.
@JohnDuffield my point is, Dirac predicted anti-particles before they were discovered and your argument against supersymmetry could be levelled at Dirac, can you address that point?
@0celo7 I can prove that they weren't all perfect :P
@0celo7 thanks, I see he's gone now, but some of that was fascinating (to the degree i was following it, which was alas minimal)
@Danu I'll never understand how the American university system translates into the European one I think
17:38
I'm not sure I've gotten a 100% score on any test
maybe once
@TerryBollinger What?
@ACuriousMind It's the German one that's really weird ;)
Who's gone now?
What is fascinating?
@ACuriousMind Shorter hair is a big part.
@Danu Probably :D
@0celo7 I conflated threads, sorry!! I thought you were replying to my last question on a different topic.
17:39
Guys
@JohnDuffield has your understanding of the definition of energy changed since yesterday?
@bolbteppa could you just stop it? Do you really enjoy this discussion you're having?
Okay lets just do the energy thing then I will
If I have a PDE of the form $f_{rr}(r,t) + A(r) f_{tt} = 0$
Can I still do separation of variables
Or did I fuck up
@bolbteppa It's pointless, remember? :P
17:41
@Danu I have hope since he ignored me pointing this out twice telling me he has recognized it, fingers crossed :D
@0celo7 and I'm glad you are bringing it up, good luck.
You would think someone in search of the truth would recognize something like this anyway :)
@bolbteppa : Dirac predicted antiparticles in 1931 and they were discovered a year later by Anderson. Supersymmetry has been around for fifty years and hasn't been vindicated at all. Spot the difference. The reason is that it isn't founded on understanding.
@bolbteppa please stop
There is no point
17:43
@Slereah What happens if you try?
(Taking the physicist's approach :D)
@JohnDuffield that's not a fair assessment at all, but nevermind that I guess, has your understanding of the definition of energy changed since yesterday?
@ACuriousMind : Well I did try :p
@Slereah please, uno momento
But I didn't check manually if I could
Hm
Let's see
$f(r,t) = R(r) T(t)$
Hm
I guess I can't
Dang it
So now I actually have to solve an unseparable 3 variable PDE D:
Oh bother
All that solving for nothing
@Slereah did you reduce the PDE to canonical form in the separate domains? I think you can do separation?
17:46
@bolbteppa : no, my understanding of the definition of energy has not changed since yesterday. Why should it? Noether's theorem doesn't tell you what energy is.
@bolbteppa I will as soon as I read up on what that is!
@JohnDuffield and finally, are you going to continue to repeat that physicists define energy in a circular fashion?
As it is the separated big PDE is $\coth(r) f_{r} + f_{rr} + 2 \cosh(r) f_{\phi t} - f_{tt} - f_{\phi\phi} = k$
@ACuriousMind What is there to not understand about how the US system works
I thought I could separate $r$ and $\phi t$
17:49
@Slereah on pages 2 & 3 the Tricomi equation is given as an example math.psu.edu/wysocki/M412/Notes412_5.pdf you'll sadly probably have a similar situation with your one
But then I remembered the $\cosh$
"sadly"?
I don't like this
I don't like this one bit!
Neither do I
@Slereah Ew.
Yeah
It looked okay when I thought I could get the $r$ out
But now I'm not so sure
@bolbteppa : yes, I will repeat that physicists define energy in a circular fashion. Would you like me to give you some references for that? Why don't you say what energy is? And then when you struggle, ask Slereah and Danu to say what energy is. When they can't and instead say it's pointless you'll maybe learn something.
17:51
It's pointless :)
@Slereah But the first thing you have to do is reduce your pde to canonical form before anything else, and since you'll probably have to solve it as though it's a wave equation in one region, a hyperbolic in another, and an elliptic in another, which I've never even seen done before, and I have no idea about matching up solutions at boundaries and stuff, but my feeling it your problem is very mechanical assuming all this stuff magically doesn't cause problems
@Danu You're pointless :D
Also it's inhomogeneous, giving more fun, but still, this exercise will probably teach you everything there is to know about pde's haha
@ACuriousMind You're less than a point!
@bolbteppa : I highly suspect things will be problematic
Since this space has no achronal spacelike foliation
17:53
I would love to throw away a week on this
Dang
@Danu I'm the empty manifold?
I'm not sure I can find a topologically trivial spacetime with a simpler metric for CTCs
@JohnDuffield Okay I see I've wasted my time
@ACuriousMind You're the empty intersection...
17:54
Don't answer you fool
YOU'RE MY EVERYTHING!
Lesson learnt
Just stop
see what I did there? :D
@ACuriousMind do curves created by the exponential map which differ only by the magnitude of the initial velocity define the same geodesic?
17:55
@0celo7 : Well I'm pretty sure a curve of a different velocity will give a different geodesic :p
There is nothing more important than understanding energy. Energy is fundamental. Matter is made of it. The mass of a body is a measure of its energy content. But you will not gain any understanding from answers like these.
hi @Tycho
Same direction in the tangent space, only different magnitude
@0celo7 Yes.
@Danu You are greeting an user who can't chat yet :P
Nobody saw what I did there? :'(
17:56
Is the usual foliation of Minkowski space also a foliation for $(T^2, \eta)$?
@ACuriousMind Ha-ha-ha. But I know the guy, so it's cool
@Danu Actually, no, I don't :/
@ACuriousMind The empty intersection is the full space
do you even power set?
@Danu Just stop it
@Danu Ohhhhhhhhhh. I thought: Empty intersection: $A\cap B = \emptyset$, not $\cap_\emptyset$.
17:58
@ACuriousMind :-)
@user3183724 No u
What is cap_emptyset
The empty intersection
You intersect nothing
Note: That is not an intersection of empty sets
What
@0celo7 An intersection $\bigcap_{i\in I} A_i$ for $I=\emptyset$.
@bolbteppa : no you haven't wasted your time. You're just doing a runner because you can't define energy, and nor can you defend supersymmetric pseudoscience.
17:59
Hm
OK, time for tea. Bye for now.
Does the set of all sets include itself? If so, isn't that another set that must also include itself?... :)
I think you can totally define a foliation for $T^2$
@TerryBollinger There is no set of all sets
@ACuriousMind what??
18:00
In mathematics, and particularly in set theory and the foundations of mathematics, a universe is a class that contains (as elements) all the entities one wishes to consider in a given situation. There are several versions of this general idea, described in the following sections. == In a specific context == Perhaps the simplest version is that any set can be a universe, so long as the object of study is confined to that particular set. If the object of study is formed by the real numbers, then the real line R, which is the real number set, could be the universe under consideration. Implicitly,...
At least not in standard ZFC axiomatization of set theory
relevant
Same leaves as Minkowski space, except on the restriction $[0,1]$, and then a map $[0,1] \rightarrow \mathbb{R}$
Though now I wonder if you can foliate a topologically trivial acausal spacetime
@ACuriousMind Damn. My Maupertuis approach is deeply flawed.
@Slereah The relevant question is if you can fornicate with it.
::hides::
18:02
@Slereah I would love to see how you manage this problem, I think the Tikhonov problem book would be helpful
I wonder if there's some general calculus of variations principle hiding around.
@bolbteppa I'll give it a whirl, though I suspect it's gonna be a tad beyond me!
@Slereah all you need to do is find a problem that looks similar in the book, already in chapter 1 there are examples which will help you classify it properly, one even has a $\sin$ function in it, I'm sure later on in the book they solve similar problems too!
Question: If one were to assume that causality resolution "takes place" within a single foliation that is treated as a single, unified, dynamic state space (vs worldlines), is it mathematically possible to show that all other foliations also remain self-consistent in terms of their interpretations of causality? I think so, but that's far from a proof...
18:06
Although I think the equation will always be hyperbolic really
No worrying about it being different things in different regions
@ACuriousMind Did you ever ask @ChrisWhite your topology question?
@Slereah did you look at the Tricomi example math.psu.edu/wysocki/M412/Notes412_5.pdf your cross terms are a function of $\tan$ it will almost certainly be different in different regions
Not $\tan$, $\coth$
And it's a physical equation, so I doubt it will be not hyperbolic
(BTW, I don't seriously expect anyone to answer that, just thinking out loud again...)
@TerryBollinger : Sounds like a question for Hawking Ellis
Hm
what's the canonical form like for 3 variables
18:12
You only have two variables in the pde though?
The eq. is $f_{rr} - f_{tt} - f_{\phi\phi} + 2 \cosh(r)f_{\phi t} + \coth(r) f_{r} + k = 0$
'fraid not
$rt\phi$
@Slereah heh, I have no idea who Hawking Ellis is, Googling now...
Hmm. The velocity vector's magnitude is constant along a geodesic, right?
Hm
Seems to be the number of real roots of the principal part
What's a good document on PDEs that is not terribly slow
And general
Heh, Hawking and Ellis, I just created a new composite physicist!
18:18
I don't want to have to go through all the slog of reading the linear homogeneous wave equation 2D case every time
Every PDE book seemingly does that
I don't think Hawking ever really addressed that type of question, though.
Later all...
$L u =\sum_{i=1}^n\sum_{j=1}^n a_{i,j} \frac{\partial^2 u}{\partial x_i \partial x_j} \quad $
Thank you wikipedia
Hm, let's see
What's the determinant for cubic equations
Or I could just put the matrix in Wolfram Alpha really
-1, -1 and 1
Indeed hyperbolic
No worries
I don't think you can really get non-hyperbolic equations from Klein Gordon
Even in a weird metric
18:37
grumble grumble
What to do
maybe method of characteristics, I guess
user54412
@0celo7 It just occurred to me I'm right next to his office right now. Should I convey the review? :p
Oh wait
Method of characteristics is first order
grumble grumble
@ChrisWhite I do wonder why he chose to be so handwavey in his book
If you can somehow inconspicuously find out I'd be interested :P
Hm
I do know a paper about solving Klein Gordon in the Godel metric
Maybe that is worth a looksie
Sort of unrelated but also neat
Apparently a lot of symmetry is involved
Hm, the metric is pretty similar
"we shall employ the separation ansatz reflecting the translational symmetry in t
and x3 directions:
(2.4) $\Psi(t, x, \phi, x_3) = e^{−i\omega t} e^{ik_3x_3} \psi(x, \phi)$"
Don't mind if I steal that ansatz, Piotr Marecki
I guess I can separate out time, maybe
I dunno
I guess that's what ansatz are for
Let's try it and see what happens
The old "Whatever" method of PDE analysis
18:58
@Slereah What makes you think it can be solved?
Why not

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