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2:34 AM
Don't you hate it when there is a question on the site that, though basic and homeworky, is fun to solve?
I've got a cute and compact answer to
0
Q: How to solve this problem without using energy conservation

hdhzeroI believe most of you probably solved the following problem using energy conservation as shown here. It states a block of mass m sliding on a sphere of radius R. I've be trying to solve this problem using only Newton's laws without energy conservation. I would like to know if it is possible and,...

but it's too much like homework for me to feel comfrotable answering.
Only I want to show off how clever I've gotten at solving undergraduate stuff now that I've been out of school for more than a decade and teaching for roughly four years.
 
you can always show off here ;-P
or in a dedicated chat room
 
2:48 AM
The clever bit is using $\alpha = \dfrac{\mathrm{d}\omega}{\mathrm{d}t} = \dfrac{\mathrm{d}\omega}{\mathrm{d}\theta} \dfrac{\mathrm{d}\theta}{\mathrm{d}t} = \omega \dfrac{\mathrm{d}\omega}{\mathrm{d}\theta}$ to integrate $\alpha = (g/R) \sin\theta$.
 
@dmckee wrt. what?
 
@0celo7 We're working in angular coordinates so $\alpha = \dot{\omega} = \ddot{\theta}$. So $\alpha = (g/R) \sin \theta$ is a differential equation. By applying the above identity you can find $\omega = \omega(\theta)$ and the rest is clear sailing.
 
@dmckee Hmm, you pulled an ACM on me
 
Clearly I can't type latex with any proficiency.
 
@yuggib what would be the title of such a room?
"I can prove that in one less line" ;-D
 
3:01 AM
I like it.
 
user116211
WTH is that.... 50 people died ;\
 
Orlando. But I don't want to talk about it.
 
user116211
3:08 AM
@dmckee: Actually one of the user's wife at Agents of Nothing was present at the Pulse that night; he was the first to report that at the chatroom; we were reluctant about that first; but how we knew such thing would culminate....
 
user116211
Lately I've been thinking about heat engines a while.... what about reversible engines that operate between more then two temperatures? What would be their efficiency? Would that still be less than Carnot's? Actually Carnot operates between two temperatures....
 
user116211
I have not got any literature dealing with that ;(
 
Well, it is easy to show that the overall efficiency of (hot)--engine 1--(warm)--engine 2--(cold) is at most the same as a Carnot engine between the hot and cold reservoirs. Beyond that I don't know.
 
user116211
@dmckee Ah! yeh; it's an usual homework where we have to show that the efficiency is equal to that of an reversible engine which operates between hot and cold....
 
user116211
@yuggib: morning.
 
3:16 AM
morning
 
That's a straight ahead calculate and reduce problem.
 
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ why not :D
 
user116211
But the point is there may be a reversible engine which operates between different temperature and not like that above @dmckee showed; suppose instead of adiabatic transformations, we could have a transformation between another heat reservoir i.e., the engine works between more than two temperature.
 
user116211
I searched some old books in the library and also read Fermi; but of no avail. They only consider engines which operate between two temperatures and if more then those sort of that dmckee showed; not the type I'm conjuring up in my mind.
 
user116211
I one saw WetSavanna talking on that a bit; but then of course it was minuscule and too superficial T__T
 
user116211
3:25 AM
> However, there are many other possibilities for the interface to the outside World. The engine could make contact with many more than two different temperature reservoirs during a cycle, or heat could be added at constant volume (e.g. from detonation of a chemical reaction inside a rigid vessel, as approximately happens during a Diesel cycle).
 
user116211
Let me leave a comment in his post; let's see whether he responds......
 
@dmckee What???
I need to see this proof
 
user116211
@0celo7 whhhat?
 
user116211
wait......
 
I've never seen the Carnot proof
 
In my intro class they just said "you can find it in books"
 
@0celo7 The proof that the Carnot efficiency represents the limiting maximum? In the usual form it is more tedious than enlightening, and it relies on either the Kelvin or the Clausius version of the 2nd law which are at their heart statements of observational fact until you get statistical mechanics to motivate them.
But you can find a version of it in Zemansky & Dittman if you insist.
 
user116211
Also, the classic Fermi lectures.
 
@dmckee I don't insist
I'm not a physicist
 
@0celo7 You keep saying that, but you are being seduced by the dark side.
 
user116211
3:36 AM
He ends many of his discussion saying that ;/
 
@DavidZ it can be awfully hard to resist the urge to be helpful, but note that my comment does include the phrase learn the chain rule - the key word being learn.
 
user116211
I really don't want to help who doesn't show a minuscule of effort ;(
 
5:20 AM
@dmckee I would post the answer. Although, yes, it's a homework like question the OP is clearly just having fun with physics and I see no harm in encouraging that.
The key reason we don't answer homework questions is so we don't encourage homework questions. However I see no problem in encouraging recreational physics.
 
user54412
@JohnRennie what's confusing me is that you wrote that answer after marking the Q as a dupe
 
@ChrisWhite I VTC'd the question as a duplicate, but the OP responded by editing it in a way that I thought made a plausible argument for it not being a duplicate. I then posted an answer but forgot to withdraw my VTC. Oh well :-)
 
user116211
0
Q: Some questions about the Kitaev Chain Model

Arnab Barman RayIn the paper,'Unpaired Majorana Fermions in Quantum Wires', Kitaev shows that unpaired Majorana Modes can be found at the end of a Quantum Wire for certain conditions. In the special case(b), the two ground states $\psi _0$ and $\psi _1$ can be shown to be of even and odd parity indicating non-...

 
user116211
Too many questions in a single post - too broad?
 
user54412
yes I think so
 
5:36 AM
Although given my close votes generally run out two thirds of the way through the day I'd be inclined to save them for the truly awful questions. That one is at least a genuine question about physics.
 
user116211
-1
A: 3 Stage Resolution to Fermi's Paradox?

Wolphram jonnyI just want to add my two cents, too large for a comment. Based on Ray kurzweil idea, there is another explanation for the lack of communication from far advanced civilizations. The cosmic orgasm hypothesis (you will not find it on wikipedia). The idea is that as civilizations approach the techno...

 
user116211
The comments below the post are reallllly odd ;(
 
user54412
@MAFIA36790 You seem to notice CO's comments a lot. Then again, I guess they are everywhere
 
user54412
also, wat is that answer saying
 
user116211
I really don't know what to say about CuriousOne.... he is .... well, he was suspended for his odd comments once; and then DS gave a valuable lecture on how to add constructive comments; but yeh....
 
user54412
5:39 AM
too bad people didn't like the question -- there actually is an objective, but subtle, problem with the OP's reasoning
 
user54412
it's a case of false dichotomy (trichotomy?)
 
user54412
his three cases don't include the far more likely scenarios of there being a spread in the distribution of technological progress
 
user54412
also, it is definitely not philosophy
 
user54412
my heart breaks for philosophy sometimes -- physicists and mathematicians keep claiming it's all junk, and then they throw unwanted junk at it, and then they point to the new junk as reaffirming their suspicions
 
It's the sort of thing we've all discussed in the bar late at night, but that doesn't make it the sort of thing well suited for discussion here. That was my reasoning for my VTC.
 
user54412
5:44 AM
the background perhaps, but his problem is with a well-defined logical fallacy
 
user54412
not that I'm inclined to vote to reopen on my own
 
My general rule is that if I can't, at least in principle, answer a question with a mathematical model then it isn't physics.
 
user54412
a model? like the Drake equation? :p
 
user54412
honestly, I don't know why everyone thinks the life and intelligent life terms are so common -- it's clear that no interesting chemistry happens in most exoplanet environments, and it's clear that intelligent life developed once in a third the age of the universe here, given perfect conditions for life
 
user116211
@ChrisWhite Drake? The SETI dude?
 
user54412
5:50 AM
was he?
 
user54412
I just know his "equation"
 
user116211
An astronomer from Cornell, aha!
 
user116211
What does SETI actually do? Did they so far discover something?
 
user54412
alas, back in the day writing down a general high-school-level stoichiometry ansatz made you famous
 
user54412
@MAFIA36790 you probably would hear about it if they had ;)
 
user54412
5:53 AM
most astronomers think SETI is a waste of resources (Contact captured this pretty well)
 
user116211
To me, Anti-Life equation (which I doubt ACM knows) is more valuable than the Drake Equation ;P
 
user54412
(I'm not really against it myself, since they ask important questions and hardly cost anything, though they do tend to attract some more fringe people)
 
@ChrisWhite yes, the Drake equation is a perfectly respectable mathematical model, though it doesn't address the Fermi paradox. If you have an answer that uses some similar plausibly rigorous reasoning then I'm happy to vote to reopen the question so you can post it.
 
user116211
nods
 
user54412
@JohnRennie well, I'd argue there is no paradox if you put our best guesses rather than wishful thinking into the Drake equation, but again I'm not committed to the question
 
user54412
5:57 AM
I'm just taking the opportunity to have some virtual beer and discuss these sorts of things :p
 
philosophy with donuts
 
> supporters of SETI and other programs note that the amount of taxpayer money that goes into these programs is less than one military helicopter per year
That puts it in perspective :-)
 
it's amazing how many people thinks that $\aleph_1$ is the cardinality of the real numbers
@_@
 
$\aleph_1$ is cardinality of $2^{\mathbb{N}}$, right? which is bigger than the reals (assuming continuum hypothesis)
 
T__T a lot of confusion
Continuum Hypothesis (CH): $\aleph_1=2^{\aleph_0}$
where $\aleph_0=\#\mathbb{N}$
however, the continuum hypothesis is non-provable and non-disprovable in ZFC
but in ZFC, $\#\mathbb{R}=2^{\aleph_0}$
 
6:45 AM
do the power set of the naturals actually well defined, or only $2^{\aleph_0}$ is?
 
7:07 AM
5 hours ago, by Sᴋᴜʟʟ ᴘᴇᴛʀᴏʟ
7 hours ago, by Secret
user image
 
@Secret why do you keep mentioning this? It's not a new book, so why the sudden interest in it?
 
(Ack, cover blown!) The reason is obvious
It's a sacarsm
The EERIE Silence
 
user116211
 
What comic is that?
 
user116211
The MASK!
 
user116211
7:22 AM
Dark Horse Comics
 
Did not know that The MASK has a comic version
 
user116211
@Secret o.O
 
I am aware of the flim version, not so much of the comics
I rememebr I first watched that when I was around 6, and got scared by the scene that looks like a fire ring
 
Ha, out of 714 servers there were no, repeat no, backup errors last night!
Mind you, the Sunday night backups are not especially stressful :-)
 
@Secret Ok my memory is all muddled up again. There's no fire ring in the movie. I must have mixed up with something else
 
7:35 AM
Hey, remember that one time that nobody believed me that you can write $f\circ f^{-1}=\operatorname{id}$ and $f^{-1}\circ f=\operatorname{id}$ for injective/surjective but not necessarily bijective functions (looking at you, @0celo7 and @ACuriousMind). I happened to be looking at Spivak's textbook on calculus, and guess what I found...
(to be fair, he adds a caveat about the domain of the r.h.s. possibly being larger)
 
8:18 AM
@Secret This question has already been answered by friend, we can mark it off the list
 
8:48 AM
@Secret the power set of naturals is $2^{\aleph_0}$
 
8:59 AM
Meanwhile I was almost planning to ask about the following question, but end up searcing MSE instead.

currently, it is still beyond my level thus I will leave this for later
6
Q: What is known about the power set of the real number line?

Dan M. KatzCantor's theorem states that the cardinality of a set's powerset is strictly greater than that of the set itself. This clearly applies to the reals also; if I'm not mistaken, the cardinality of the power set of the reals would be $\beth_{2}$. Is there any literature on the powerset of the reals?...

I do, however have a quantum conceptual question that I can ask you, but phrased in undergrad wavefunction collapse language as I still have not finsih reading von neumman yet
@yuggib
Suppose I have a set up containing one electron. 8 light minutes away I placed a detector B that can read the spin of the electron (and can flash red if spin up, green in spin down).

Suppose I have a friend Ann standing next to detector B.

Now I use another detector A next to the electron unit to measure my electron spin. Suppose my measurement collapse it to spin up. will I expect 8 minutes later, Ann will inform me her detector flashes red?


My guess is that when the electron state get projected to e.g. spin up eigenstate, that information will need to travel with an upper boun
 
@Danu this looks very close to an abuse of notation in my opinion
 
9:20 AM
@Secret it depends on how your experimental setup is done
 
the most effective way to think about it in my opinion is as two non-interacting apparati, that in addition have a localized in space interaction with the particle. Of course to give a precise mathematical meaning to all that could be rather hard, nevertheless it should in principle be possible
instead you may think of a time-dependence that models the switching "on/off" of the apparati
so you would have a dynamics that consists of five parts:
the three time-independent parts are the free (non interacting with the apparati) particle dynamics, the A free (switched off) dynamics, and the B free (switched off) dynamics
the two time-dependent parts are the interaction of the particle with A, taking e.g. place from $t=0$ to $t=t_A$, and the interaction of the particle with B, taking place from $t=t_A+8\text{min}$ to $t=t_B+t_A+8\text{min}$
this would give the dynamics of the whole system A+B+particle
and of course if the measurement apparati behave as they should, you would get that for $t_A \leq t< t_A+8\text{min}$, the reduced state of the particle alone would be that of spin up. Then, your apparatus B would measure spin up, and essentially leave the reduced state of the particle unchanged (but of course the reduced state of B changes, as the whole state of the system, according to the full dynamics)
 
@secret what is "Chat interview featuring guest speaker Slereah
tomorrow" who is slereah ? please can you tell me?
 
@ yuggib, I see
@2physics the link contains all the details you need to know. But in short, he is good at CTCs
 
9:48 AM
@yuggib@Secret I got it. Thanks.
 
So
I've been thinking about minkowski surgery
I'm wondering
Is Fourier transform even applicable here
 
user116211
who is Slereah? do you know @Slereah??
 
He's the AMA guest for tomorrow
 
17
Q: Questions for the June 14th Ask Me Anything

SlereahHey I'm the scheduled guest for the june 14th Physics AMA and I was told to maybe make a little presentation and asks for any questions for the AMA people might have, so here it is. About me So I am Samuel Lereah, got a Master degree in particle physics from the university of Nantes. My master ...

 
user116211
Ah!
 
user116211
9:55 AM
@2physics Thanks; i didn't know that!
 
user116211
Hello World!!
 
stop botting
;-P
 
@MAFIA36790 :|
 
While I still have not (re)beefed myself up enough to investigate this rigorously, what Slereah recently doing about the Lereah Ghost in a wormhole and minkowski surgery in general is highly relevant to my time travel model
 
Is it
tbh I'm pretty sure time travel can't work by this point
 
user116211
9:58 AM
The 'Lereah ghost' - I like that!
 
Although there is a counterexample to the chronology protection I'd like to check
Proving a singularity structure in it is difficult, though
It's usually done by pointing at closed causal geodesics, but it has none
 
This is because over the past years I have been investigating, wondering about time travel that involve identification of two different points in minkowski space, although it is embarassing to say that right now the analysis is still scifi level because my maths have not caught up yet to make it rigorous
 
@Slereah hi are you supposed to present your speech?
 
To be fair surgery spacetimes aren't that complicated mathematically, at least when we're not doing analysis
Tomorrow yes
 
tommorow*
tomorrowww*
 
10:04 AM
Adverb: tomorrow ‎(not comparable)
  1. On the day after the present day.
Noun: tomorrow ‎(plural tomorrows)
  1. The day after the present day.
It's from to-morrow
to the (next) morning
 
user116211
2-morow
 
(mistake ,retype needed)
 
@Slereah thanks, I hope your physics teaching and your patience is as good as your skill in explaining obvious issues.
 
Probably not
 
@yuggib That's what I told him too, but he won't listen :P
 
10:18 AM
@ACuriousMind he's still a pure physicist...inside ;-P
0
A: If an isolated quantum system consists of only one particle,is it possible for it to be in a mixed state?

yuggibA mixed state represents a lack of knowledge on the system (maybe caused by the observer, maybe more fundamental). It is a notion in my opinion closely related to the Bayesian interpretation of quantum theories (seen as non-commutative probability theories). Quantum states are (non-commutative) ...

I mentioned Bayesianism related to quantum physics...I can't imagine how many annoying comments this would yield to me if e.g. c1 and lumo get to read it
T__T
I am not a fan of discussions about interpretations (since they're not so scientific), being that in probability or quantum theories; but I don't see any other explanation on why we distinguish between pure and mixed states
 
but transactional is best interpretation, obviously
 
:-D
 
@yuggib I still think it's morally correct.
 
@Slereah I really don't mind at all
@Danu morality is undefined, and surely unknown to mathematicians
 
But @yuggib
 
10:29 AM
@yuggib You're a cold sonuva... ;)
 
Modal logic has been used for morality axiomatization
 
^lol
 
@yuggib You could have just avoided dropping the name ;) I'm sure I've used the "lack of knowledge" explanation for mixed states without alerting anyone to the fact that this might need a Bayesian interpretation...
 
@Slereah T__T also to prove the existence of "god"
that does not make that interesting...
 
I have the Godel "proof" of god somewhere
 
10:30 AM
Oh mt f*cking god, the differential topology concepts of immersions and submersions are just generalizations of the baby calculus notions of the parametric, & implicit, equation representation of a surface!!!
 
@ACuriousMind ;-D that's cheating
 
user116211
CuriousOne - c1 ;D
 
@Slereah who doesn't...I have it in both pdf and paper versions
@Slereah yep
 
I'm sure the proof is okay but I question the axioms :p
 
10:31 AM
but you are not stating notation
of course
also, it is the proof of existence of a "being with all positive qualities", whatever that means
 
Well yes
That's me
All perfect baby
 
11:02 AM
Be prepared for the most insane (possible) nonsense you ever heard in my history of this chat room:
4
i would be crying to tears if it turns out some of the following is not nonsense and can actually be worked on and made rigorous
(My WIP time travel model)
Heavily inspired by Looper, Primer, The Librarian season 2 final episode, and Back to the Future (and numerous other famous time travel stories and classics such as the time machine, and the time traveler’s wife)

It rests on a couple of postulates:
1. Any identification of events in the spacetime manifold that is not in relative motion of each other (and subjected to the same gravitational potential) must have their clocks in sync. Light signals that propagate from or into one of these pairs must simultaneously took place at the other event of the pair. Thus the notion of the apex of the light cone becomes a multiply connected structure, i.e. roughly speaking the notion of 'present' can be simultaneous at multiple locations in the spacetime manifold as long they are being identified due to time travel.
(This is why Slereah's recent research on spacetime surgery is highly relevant, because it will provide me some insights on testing this)
2. The spacetime manifold is no longer a static structure, but dynamic as a whole. Time is treated like a field in the spacetime manifold, being dilated in the way as described by general relativity (e.g. by relative motion and by the stress energy tensor). Every observer, depending on where they are located, and whether they are in relative motion with each other, will not only disagree with simultaneity and size of objects, they will also in general disagree with the geometry of the spacetime manifold.
3. Because the spacetime manifold is no longer static, it has dynamics. The notion of proper time extend beyond the worldline of the observer, to the entire spacetime manifold. The evolution of every event in the spacetime manifold can be parametrised with the proper time of the observers. In particular, events evolve in the direction of the future pointing tangent vector for each tick of the proper time of the observers, thus different observers will disagree when and where time travel events happened, except for causality (see 6.)
4. If a time travel event changes history, its dynamics can be simplified into a discontinuity in the worldline of said event. These causal discontinuities are analogous conceptually to quasiparticles in condensed matter and their dynamics give the quantitative notion of the ripple effect heard in back to the future (e.g. the delay of the ripple effect is given by its 4-velocity from the source event to the spacetime position of the observer). Causal discontinuities also interact with other matter just like usual things such as the tendency to be dampened out like the 1/r^2 or exponential d
5. The dynamics and the stress energy tensor is not only determined by the curvature at an event. It is also determined by the energy momentum and dynamics of all causal discontinuities to the past of the event of interest
6. While a global notion of past and future is lost, causality can still be explained as all observers will agree with the chronological sequence of the sources and destinations of any causal discontnuities produced by time travel. However since each observer may lie before or after the source of a given causal discontinuity (and hence seeing disimilar versions of the spacetime manifold (and its evolution) before and after the source events), it would take more than one observer to reconstruct the full history of the spacetime manifold and the chronological sequence of history changes that
7. In the absence of time travel that changes history, this model reduces to general relativity, with the notion of a global past and future recovered

.
Consequence:
1. Past and future become local for every observer, due to the presence of causal discontinuties produced by time travel that changes histories, thus five minutes in the future in A's spacetime diagram (which might be 8 minutes in B's) is actually the past future of the dynamics of the spacetime manifold
2. Grandfather paradox will produce an oscillation in the spacetime manifold with a frequency characterised by the 4 velocity of the causal discontinuity and the spacetime interval of the two event that defines the region where the paradox took place. This can theoretically be
END WALL OF TEXT
and some extremely rough attempt to formulate the above wall of text
Please wait when I type up the desscription of this diagram...
First line: We have the einstein field equation and the geodesic equation
We then modified it as follows:
The stress energy tensor is no longer a local quantity. In the region of spacetime with more than one time like separated events beign idetified, it is now determined by the riemannian curvature tensor and cosmological constant throughout the entire worldine of interest within the region (i.e. the worldline from $\mu (0)$ to $\mu(r)$)
The geodesic equation describe something simialr
The model then states that this complicated dyanmics can be simplified as follows
The stress energy tensor in one position in spacetime is determined by the riemann curvature tensor in that position due to ordinary matter, plus the riemann curvature tensor caused by all the causal discontinuities (CD)
(A casual discontinuty is a change in history which is localised like a quasiparticle and propagates towards the future direction)
The geodesic equation is then completely determined by the causal discontinuities
(I don't quite remember what I wrote about the "regression operator". Give me a sec...)
ok let's see...
Mathematically the set of causal discontinuities $\mathcal{CD}$ is defined to be events that don't commute under the regression operator
and
n is a function that checks whether a given ith event is in $\mathcal{CD}$
The regression operator $\mathcal{T}$ is then described as follows:
$\mathcal{T}\mathcal{T}^{-1}$ commutes and returns the ith event in spacetime $x_i$ unaltered if $x_i \in \mathcal{CD}$
 
11:37 AM
You know, writing "END WALL OF TEXT" and then continuing to post another wall of text is not what "end" means.
 
@Secret you have now fulfilled one of the first comments made by a founding member of this room
Dec 8 '10 at 20:50, by David Zaslavsky
I think this room needs some content :-)
 
Otherwise, it regress to $x_j$, where $x_j$ is not the same as $x_i$ despite sharing the same spacetime coordinate (?) (to be worked out...)
@@@@ So guys, is this a complete nonsense and I have been misguided for 3.5 years or is there something that is actually workable?
 
5 hours ago, by Secret
5 hours ago, by Sᴋᴜʟʟ ᴘᴇᴛʀᴏʟ
7 hours ago, by Secret
user image
 
@Secret Why would you make a time travel model based on science fiction?
@Secret Sounds like nonsense to me, sorry.
 
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ the joke is wearing thin
 
11:46 AM
:30A20920 Because I am SO FED UP with different time travel stories having inconsistent way to explain their time travel, and more importantly, that all the models they have used (except for type 1 (you cannot change the past,CTCs) stories) always left behind unanswered questions and loopholes
 
@Secret I have no words
 
@Danu We've tried to explain that science fiction isn't about science before...apparently it didn't stick :P
 
@Danu I'd like to see where I said that
 
Apr 5 at 21:37, by 0celo7
@Danu admit it, you goofed
 
That sounds exactly like the kind of thing I would say and ACM produces some weird counterexample from the 4th dimension
 
11:49 AM
@ACuriousMind I know, you mentioned that it is how the authors build the plot that is important in whether there are plotholes.
(this phrase is being deleted because there is no point saying it)
 
@Danu I think his "caveat" is very important
And that's what ACM and I were getting at.
 
Hm
Should I ask MSE or MO for analysis on surgery manifolds
 
Although that was too long ago, I could have been trolling you
 
@0celo7 "admit it, you goofed"
:)
 
@0celo7 I don't even know what a "counterexample from the 4th dimension" is
 
11:52 AM
@ACuriousMind the TV show
The Twilight Zone
 
What?
 
8
 
@BernardMeurer Oh god Bob sent this to the fam group this morning
> In case anyone is interested, today (Monday, 13 June 2016) we have the earliest sunrise of 2016...which is not to be confused with the longest day of the year which occurs around summer solstice in another week. The exact calculated sunrise time here at the FoxMill Weather Station will be 5:46:10 a.m. EDT. Of course, you can easily see outside without a flashlight from Morning Civil Twilight onward which is roughly 30 minutes prior to official sunrise.
@ACuriousMind I'm just saying you often produce weird unsatisfying counterexamples
 
11:55 AM
Well, it's not my fault that you're unreasonably hard to satisfy!
 
@Secret All I want is a systematic and quantitative way to analyse all possible time travel stories so I can stop hearing people saying that these stories are mindscrewy
This is my major motivation
 
@ACuriousMind It's not you, it's me
@ACuriousMind I've been seeing someone else
@Slereah What is that a counterexample for
 
I forget
 
so...
The consensus of you guys is that I have wasted 3.5 years for nothing, and I not even knowing what misconception I have made?
 
11:59 AM
Hard to say, I tend to zone out when you post a wall of text
 
@Danu wait wait
going back and reading...
I don't think I was trolling
I was agreeing with ACM because he's smarter and correct more often
BUT
He wasn't saying that was wrong, just that he'd never seen it in a math text.
And Spivak's calculus is for engineers and biologists, it's not a math text.
 
@Secret is your analysis supposed to applied to flat spacetime?
You say Because the spacetime manifold is no longer static, it has dynamics but that's the case in GR anyway.
Well, the metric is dynamic
 
Yes, because it is a generalisation of general relativity to history altering type time travel events (by modelling them as quasiparticles that move in the future direction)
 
I'm not sure it makes sense to say the manifold is dynamic
 
12:03 PM
@JohnRennie There's theorems against that
 
The idea is that since there are timelike separated points that are being identified, clocks there must be synced. Thus to an observer located at those points, the present is simultaneously at two different positions in spacetime at once, and events in the past and future can then influence each other (because they are located within the lightcones of another)
 
@Secret hang on, you appear to have said yes to is your analysis supposed to applied to flat spacetime, then said it is a generalisation of general relativity
 
It should apply to flat and non flat spacetime
ideally..., which is why I begin my investigation with minkowski surgery spacetimes
 
OK, so you're suggesting that the topology of the spacetime is dynamic? Yes?
 
@Slereah here's where you quote Visser
Oh, @JohnRennie
Is 2D noncompact gravity dynamic or not
Compact is obviously not
 
12:07 PM
2D gravity can be dynamic
 
@JohnRennie (I am not sure if fully understood your question) yes, given that to the observers, causal discontinuities can pop up, propagate and vanish with proper time and causal discontinuties are kinda liek singularities
 
Depending on what the action is
 
EH
 
$$\int \sqrt{-g} R d^2x$$
is not
(I THINK at least)
I still haven't seen a proof of it
Well at least from the action
Well
I guess a simple proof of that would be...
All metrics in 2D are conformal to flat space, sooo
I guess that works out if $R$ is conformally invariant or something
Or if the conformal transformation is a constant
Well for $R^2$ anyway
I don't know about any other topology
I want to say that we can probably apply the uniformization theorem to Lorentzian manifolds, but that sounds like a risky gambit
 
@Slereah no?
flat space or the hyperboloid
if we're talking noncompact
 
12:12 PM
Yeah probably
Compact ones are only like
The torus
Klein bottle
Maybe projective plane
 
I think the torus is flat
 
Torus I assume is flat, yeah
same with the rest
 
@ JohnRennie
Given causal discontinuities A B and C
To different observers, causal discontinuities can in general pop up at different position in spacetime, but e.g. they all agree that when the history and their dynamics are considered, A must proceed B and then C
 
I have to confess that I struggle to see any coherent argument in your wall of text posts.
 
...I am not sure how I can do better...
I have refrained from using diagrams so far because Acuriousmind et. al. cannot comprehend my diagrams, so that leaves only text
But I think you seemed to have got the basic idea of that model, that the topology of spacetime is dynamic
I wish I am meeting face to face with you guys, I might have explained better...
 
12:18 PM
What does "the topology of spacetime is dynamic" mean
It's not dynamic in GR
The topology of spacetime is fixed
The topology of a spacelike hypersurface might change
But not spacetime as a whole
 
@Slereah I dunno, is it?
 
Well with what would it change?
 
Can the metric not evolve into something impossible for the current topology?
 
What is "current"
Spacetime means the whole thing
It includes all times
 
I know
I guess a hypersurface, yeah
 
12:22 PM
If I identified two timelike separated points in spacetime, and an observer is located at one of these point, then to this observer, both points are equally valid to be his present, right?
 
That's because they are the same point
 
lel
 
So if a light signal propagate from there future point into the past, then to that observer, he should see that the moment when that light signal entered that future point, at the same time he should have memory of some light emitted from the past point, which he previously in his frame does not have?
a discontinuity in memory due to time travel, so to speak
 
If you assume basic physical laws, then no
The light ray will have always been ther
Otherwise it would not obey Maxwell's equation
 
good old maxwell
 
12:27 PM
See what I was talking about regarding spacetime surgery
If two points are identified, then the field requires the continuity $\phi(x_1) = \phi(x_2)$
 
@0celo7 admit it, you goofed.
 
@Danu Nah.
 
:)
 
@Slereah I wonder... if the field can be dependent to how you parametrize it, in order to obey Maxwell's equation for all observers

We knew that the field at identified points must obey $\phi (x_1)=\phi (x_2)$

Now suppose we have observer A where events can be parametrised according to his proper time $\tau_A$

So perhaps the scenario can be modelled this way

Before the passing of the light pulse at the future point, at $\tau_A = 0$ the field in the spacetime manifold at the identified point is described by
 
The continuity is done with spacetime points
It's independant of coordinates
 
12:42 PM
hmm... so I guess that means the field must have the same value for all observers, thus the proper time argument above will not work
*hmm... it seems we have (at least) one possible no-go condition for my model*, and possibly a scientific explanation on why type 3 (i.e history changing) time travel models cannot be a physically plausible model:
1. Continuity of maxwell equation will be violated
so if any models cannot get around this no-go condition, then time travel will mean that everything is predetermined inside
Therefore, physically plausible time travel can ONLY occur in two types, if found:
Type 1: CTCs
Type 4: Branching timelines

(Type 4 is so resistant to being ruled out and too flexible to the point of being useless in prediction as a model)
 

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