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5:00 PM
Another analogy: centrifugal forces in Newtonian physics are ‘fictitious’ insofar as they arise from working in a noninertial reference frame
You don’t have to postulate them; they’re there in the theory already
The same is true for gravity in GR. But it is not true for gravity in SR
 
@ACuriousMind you will have clarify something further:
1.You say " laws of SR hold around every observer in SR" ...
2.So every obsever includes non-inertial frames too?
3. "freely-falling" means something special in GR,
4. I think Im asking why is this non-intertial frame special in GR
 
4. presumes that non-inertial frames are a thing in GR like they are in Newtonian mech. I’m not sure that’s true?
 
@Semiclassical kinematics or dynamics in Newtonian mech? Also I am aware GR doesnt have a seperation of kinematics or dynamics
 
@MoreAnonymous Einstein presents SR and GR concisely together in his little book, may i suggest you have a look at it?
 
@MoreAnonymous (fwiw, the numbering there is more confusing than helpful :P) It's special in GR because it is the GR equivalent of "inertial frame" - as I said, gravity is a not a "real" force in GR, it's more like changing the notion of what a "straight line" (aka geodesic) is. Freely-falling observers follow geodesics, i.e they are the generalization of inertial frames travelling in straight lines.
 
5:12 PM
@skullpetrol sure but I feel concisely might work against me :P
 
yeah, it is too concise
but he warns the reader in the preface
 
Here’s a question I don’t know: In Newtonian mechanics, you can always choose to work in an inertial frame. If you now compare that with a non-inertial frame, some forces in the latter will not appear in the former
So some forces in the non-inertial frame have a kinematic origin, whereas others really do have an origin in dynamics
Can one always find such a frame in GR? My guess would be no
 
does "inertia" even belong in GR :P
 
You have Fermi frames in GR
 
@skullpetrol stress energy tensor?
 
5:18 PM
Fermi–Walker transport is a process in general relativity used to define a coordinate system or reference frame such that all curvature in the frame is due to the presence of mass/energy density and not to arbitrary spin or rotation of the frame. == Fermi–Walker differentiation == In the theory of Lorentzian manifolds, Fermi–Walker differentiation is a generalization of covariant differentiation. In general relativity, Fermi–Walker derivatives of the spacelike vector fields in a frame field, taken with respect to the timelike unit vector field in the frame field, are used to define non-inertial...
 
The metric is ~ flat around the observer
ie there's no felt acceleration
 
Too technical for my limited knowledge of GR, alas
 
@JohnRennie Yeah I suppose. I was kinda hoping mathematical physics would have some use in e.g. stellar physics though
 
That's because GR is bad
Don't do it
 
5:20 PM
@Semiclassical I think you're describing the "momentarily co-moving reference frame"
 
My intuition for “no” was based on analogy with electromagnetism in SR
 
It's special in GR because it is the GR equivalent of "inertial frame"

@ACuriousMind I feel I'm getting confused because both GR and SR can use:

$$ ds^2 = ...$$
How does when distinguish when both use this ^
 
By looking at what's on the right side
 
...
 
^that. The metric is static in SR (and usually flat), but dynamic (through the Einstein equations) and usually curved in GR.
 
5:22 PM
Namely: if you start in a reference frame with both electric and magnetic fields at some point, then you can either find a frame where E=0 or one where B=0.
But you cannot do both!
That is, if you can find a frame where E=0, then in general you can’t find one where B=0 and vice versa
 
@ACuriousMind So if someone gave me the Rindler metric then?
 
which is why it’s not correct to say that magnetic fields are ‘merely’ the result of a Lorentz transformation
In some cases, they can be constructed as such. In others, though, they can’t
So there’s no neat division of electric/magnetic fields into kinematic/dynamic, like there is for forces in Newtonian mech
 
The Rindler "metric" is just flat space as seen from an accelerating observer, it's not a different metric from flat space.
 
So Rindler metric = SR
 
@Semiclassical I feel this is just a manifestation of the distinction between "electric" and "magnetic" being unnatural from the relativistic viewpoint, where these are just components of the field strength tensor.
 
5:29 PM
@ACuriousMind I guess u can't accelerate yourself and see a Schwarzschild metric
?
 
No, certainly not
 
Hmm ... I remember it being difficult but possible to see if 2 metrics were coordinate transformable in 4D ... Is there something similar for what u can see in an accelerated frame?
@ACuriousMind ^
 
@ACuriousMind agreed
 
@ACuriousMind For example if I give you one set of coordinates and then give you another and ask you if I can accelerate one and see the other?
 
@MoreAnonymous It's difficult but not impossible: The Cartan-Karthede algorithm allows you to determine for two arbitrary metrics to determine whether they are the same in different coordinates or not.
It's often much easier to tell when they are not - only one scalar invariant (such as the Ricci scalar) needs to be different.
 
5:37 PM
Yes ... but I'm looking for an algorithm which "if I give you one set of coordinates and then give you another and ask you if I can accelerate one and see the other?"
For example if I give you the Lorentz metric and then give you the Rindler Metric is there an algorithm that will say from Lorentz u can accelerate to Rindler?
 
@acm one thing I want to pick your brains on at some point is this business of unitary vs non-unitary evolution in QM
 
@MoreAnonymous I just gave you that algorithm.
But if it's just acceleration you don't need to go through it, of course - you can just do the coordinate transformation into the accelerated frame directly on one metric and see if you get the other metric.
 
My sense was that, if you take the collapse postulate as writ, then you are thereby committed to that step being non-unitary
 
@ACuriousMind u also followed it with: allows you to determine for two arbitrary metrics to determine whether they are the same in different coordinates or not.


I was under the impression Rindler and Lorentz were not same metrics (in the sense one cannot do a coordinate transformation and get the other)???
 
@Semiclassical the first three letters have to match :P
 
5:42 PM
@MoreAnonymous Going to an accelerated frame is just a coordinate transformation.
 
Since a unitary evolution can’t turn a mixed state into a pure state
 
@ACuriousMind OMG! My brain is dead
How could I forget something so basic
Talk tomorrow?
 
@skullpetrol yes, but I’m lazy and ACM is right here :P
 
true dat pal
 
@Semiclassical ... I feel ur going in the danger zone of physics.stackexchange.com/questions/502221/…
 
5:44 PM
acm vs acu
 
@Semiclassical Yes. This problem (without involving collapse!) also shows up when you try to explain how unitary evolution can turn a pure state of some system into a mixed thermal state. (Just picking a non-unitary evolution operator doesn't cut it, either - the standard notion of applying an operator to a pure state simply cannot produce a mixed state)
 
Sounds legit
 
I wonder what @bolbteppa has to say about this^
 
For thermal systems, you can say that the unitary evolution acts on the system + heat bath, which is much akin to describing measurements as unitary evolutions of system + apparatus.
 
Ah ...
 
5:48 PM
tracing out the heat bath/apparatus, you get mixed states for the original systems if the pure state of the total system is entangled.
 
Ahah
I know why Minguzzi chose a static metric for his simultaneity bundle
Because otherwise the Riemannian space $ \Sigma = M / G$ doesn't have a metric induced!
it's a pure topological manifold!
 
@bolbteppa I wanted to know ur thoughts on "Explicit symmetry breaking" ... u know the context ;)
 
The more subtle point is whether that non-unitary evolution should bother you. If you’ve got an epistemic view of the density matrix, then it should presumably not bother you a wit
 
@Semiclassical Yes, this is a "problem" only if you are a "$\psi$-ont" ;P
 
nooooo .... Semiclassical by the time ur done with this kind of subtlety ... u will need to change ur name to classical :P
 
5:51 PM
A psi-ontologist, if you will
 
That's much better than what I said!
 
Lol. It’s a turn of phrase I’ve heard from others
A tricky point in this is how Bohr/Heisenberg would’ve replied to the question
 
I'm a psychic
 
@Slereah I'm entirely willing to believe that you spend your time communing with the ghosts of long dead general relativists
4
 
@ACuriousMind I won't leave them alone until they give me those "unpublished" papers dammit
5
 
5:57 PM
The notion of the Heisenberg cut is probably relevant here as well
 
@Slereah I see the spirits trying to give u their unpublished papers its just spirit paper they have :P
U must stop digging their graves for these papers
boooooo
u have been warned
 
Hm
I wonder if, given a topologically trivial spacetime, you can foliate it with light clocks
Well, for synchronized points, anyway
I'm worried about caustics I suppose
The word may apparently be more "cut locus"
 
@ACuriousMind what do u mean by it? (sorry re-reading our messages )

https://chat.stackexchange.com/transcript/message/51706216#51706216
 
@ACuriousMind I guess another way of putting the epistemic reply is that, during a measurement, the question “what is the quantum state” has no meaning
 
what do u mean by "it"?
 
6:10 PM
@MoreAnonymous "It" = "the freely-falling frame"
You can reply to chat messages directly if you click on the little arrow on the right when you mouse over them, by the way
It's much more convenient than reposting the link to the message.
@Semiclassical Well, the "truly epistemic" viewpoint is that that question never has an unambiguous meaning, no? Different observers have different knowledge of the same system and therefore may ascribe different states to it.
 
@ACuriousMind So I can equate an "inertial frame" to a "non-intertial frame" in GR ... But can't in do so in SR?
^I'm getting this from "free-falling frame" = "non-inertial" ??
 
@ACuriousMind point. But even just looking at the experience of one observer, you’d already run into the issue
 
@MoreAnonymous I'm saying that "a frame of an observer only under the influence of gravity" is a non-inertial frame in SR (the metric is flat and gravity is a force, hence the path of the observer is not a geodesic), but the equivalent of an "inertial frame" in GR (the metric is curved and the path of the observer follows a geodesic).
 
I think there’s a word or two missing in that sentence
 
1 hour ago, by skullpetrol
yeah, it is too concise
:P
 
6:21 PM
@Semiclassical I...don't think so?
Maybe that construction (using the same verbal phrase for two clauses connected by 'but') isn't idiomatic in English, though :P
 
“I’m saying that X is Y in SR (because...), but the equivalent of Z in GR (because...)”
 
@ACuriousMind I'm under the impression if I have 0 stress energy tensor in GR that makes me go to flat spacetime which is SR ... I'm think over there ... GR and SR interpretation of geodesic is the same? In which case if there is an accelerating obsever in this situation he can also predict the bending of light? (alone by SR) I'm thinking of this in the context of Einstien's famous elevator thought experiment
 
Something doesn’t parse in that sentence
 
@Semiclassical Your preprocessor is supposed to expand it into "I'm saying that X is Y is SR (...), but that X is the equivalent of Z in GR (...)
 
@Semiclassical my language becomes worse the more mentally fatigued I become
 
6:26 PM
Gotcha
 
@MoreAnonymous No, vanishing stress-energy does not equal flat space - the Schwarzschild metric is a vacuum solution!
 
“but the former is the equivalent of an inertial frame in GR” is how I’d render it fwiw
 
Yeah, that sentence was not a masterpiece of comprehensibility on my part, I guess
 
@ACuriousMind interestingly in Schwarzschild I was of the opinion u still need the point (the singularity) which is definitely not 0 ... but thats a digression ... can we focus on GR talking about a situation in GR where Stress energy solution subspace refers to flat space time
 
On the contrary, even with the singularity, the stress-energy is zero everywhere where it is defined at all - at the singularity the metric diverges so you don't have a value of stress-energy there at all.
 
6:35 PM
@ACuriousMind we are digressing ... So I start with a star with finite stress energy tensor and get a blackhole with none?? I was of the opinion there the derivative of the stress energy tensor is 0 ... So where did it go??? Anyhow one concept of GR at a time unless u prefer 2 simultaneously?
 
@MoreAnonymous A true Schwarzschild black hole cannot actually form in finite time, so the stress-energy doesn't go anywhere (but also energy is not, in general, conserved in GR due to a lack of time translation invariance).
You're trying to reason about things like QM and GR with intuition, which is a Bad Idea(TM) unless you have trained it not to lead you astray.
These theories are very much not intuitive - they are precise theoretical frameworks you need to carefully study before applying them to anything.
 
@ACuriousMind I think my real folly is not spending enough time with them and being cocky while I have excessive mental fatigue
 
Go to sleep then, or do something else relaxing - tomorrow is another day :)
 
Thanks ... Please be patient with me tomorrow as well :)
I'll be re-reading alot
Goodnight chat
 
cya pal
 
7:32 PM
Yoy can describe sxhwarzchild as having a streds energy tensor :p
But then it is very bad
 
It's probably some derivative of $\delta$? :P
 
It is a delta yeah
$\delta(r)$
With some factos of mass and 4-velocities
 
8:12 PM
@MoreAnonymous omg u actually sent me real spoilers lol
 
8:33 PM
@NovaliumCompany Please tell me u found out they were real as u watched the movie :P
I'm sure as a dank meme worshipper my actions are acceptable :P
 
9:11 PM
@MoreAnonymous they were real
@MoreAnonymous Let's create a new religion - Memedoism.
Worshiped only by real dank memers
 
 
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10:55 PM
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