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vzn
12:39 AM
@Cows new job? congrats! :) whats that about?
 
12:58 AM
Could somebody give me a hand with a double integral
$\int_{x=-a}^{x=a} \int_{y=x^2}^{y=(1-x^2)^(1/2)} dydx$
 
1:25 AM
@JakeRose is that $\int_{x=-a}^{x=a} \int_{y=x^2}^{y = \sqrt{1-x^2}} dy dx$? Have you learned how to do double integrals over non-rectangular domains?
 
Yeah
Im just strugglong with the integral of the top limit
once its subbed in and all that jazz you have to integrate it you see
 
$\int_{x=-a}^{x=a} \int_{y=x^2}^{y = \sqrt{1-x^2}} dy dx = \int_{x=-a}^{x=a} y|^{\sqrt{1-x^2}}_{x^2}dx = \int_{x=-a}^{x=a} (\sqrt{1-x^2} - x^2)dx = \int \cos^2 (\theta) d \theta - \frac{x^3}{3}|^a_{-a} = \dots$ etc right?
 
yeah thats sort of where I got up to
 
I see, so what's wrong with doing the rest
 
Its just going wrong somewhere unfortunately
actually nevermind i think ive got it
 
1:41 AM
It's probably a mess because the limits are $a,-a$ not $1,-1$
 
If I already have an x double-dot to show it to be an acceleration, do I still need to put an arrow above it to show it's a vector or is that just too much ?
 
You need the arrow really
 
If you are talking about a vector, then you can either write $\ddot{\overline{x}}$ or in more advanced notation $\ddot{x}^i$ but if you write $\ddot{x}$ people will think it's a scalar unless the context is very clear
 
Hey bolba
Im getting a acsin that cancels
When in the answer Ive got it shouldnt
Nevermind
I havent got the right answer tbf
But I at least have some of the right terms
 
If you're comparing to some online calculator, it could easily give a bad answer tbh, best try to work the logic of it out carefully, do similar examples
e.g. $\cos^2(x) = \frac{1+\cos(2x)}{2}$ etc
and it's probably a mess because of those $a$'s
 
1:59 AM
Nah I have a answer sheet with the final (ish) answers
Im not being crazy right
but $[x^3/3] with limits a and -a is \frac{2}{3}a^3$
I forgot to go out of latex
My sheet says 1/3 instead of 2/3
Maybe its wrong
 
$\frac{x^3}{3}|^{x=a}_{x=-a} = \frac{a^3}{3} - \frac{(-a)^3}{3} = \frac{a^3}{3} - \frac{-a^3}{3} = \frac{2a^3}{3}$
 
can someone explain to me how to go from the non-relativistic to the relativistic lagrangian of a free particle?
 
@gian you don't, you go the other way
 
2:15 AM
well yes i understand that the non-relativistic is just a limit of the relativistic. i'm just confused about the -m constant and why we integrate with respect to proper time
 
@DavidZ I have improved my question which was closed by you... Can you please review it? I want it to be reopened.
 
Just as non-relativistically you find the minimum path in space, relativistically you find the minimum path in spacetime, and the arc length in spacetime is $ds^2 = c^2dt^2 - dx^2 - dy^2 - dz^2 = c^2 d \tau^2 - 0$ in certain frames
 
by certain frames you mean the rest frame?
 
In the rest frame of a particle, where we have $dx = dy = dz = 0$, then $ds^2 = c^2 d \tau^2$
 
right. what about the $-m$?
or i guess $-mc$
 
2:30 AM
When you take the non-relativistic limit you want it to reduce to the usual Lagrangian, try it with $S = \alpha \int ds$
 
thanks
 
A more physical argument is, since we can always scale actions by arbitrary constants anyway, because $S = \alpha \int ds = \alpha \int c d \tau = \alpha \int c \sqrt{1-v^2/c^2}dt$, the minimum is clearly $0$ i.e. when $v = c$ so that $S = 0$, while the maximum is clearly a straight line in spacetime, so that $S = c \tau$, however when you put in the minus, the minimum is a straight line while the max is 0, so now you do the non-rel limit on $S = - \alpha \int c \sqrt{1-v^2/c^2}dt$
 
3:16 AM
Hey everyone! I asked this noob question (https://physics.stackexchange.com/questions/390315/time-dilation-questions-ive-been-trying-to-figure-out-for-years-and-was-too-afr?noredirect=1#comment876975_390315) on SE physics and was recommended to ask around here...

I am determined to really understand special relativity before I die (and then general relativity) not just the concepts but also the math and formal physics behind it
I think I somewhat understood (or have enough material) for #1
e.g. that the mirror thought experiment's math works no matter how much the clock is rotated (due to space contraction etc...)
but I'm still struggling with the rest :(
 
Hello! Physics.SE. In, 1100/10.2 by using significant figure rules, the answer is 110. But in, 1100 m/s divided by 10.2 m/s the answer is 108. The actual answer is 107.8431373. Can anybody please explain that why 110 turned 108 just by using units? Thanks!
 
 
1 hour later…
5:39 AM
@ACuriousMind is Schottenloher very famous?
 
 
2 hours later…
7:09 AM
@EranMedan You caught the room in a pretty inactive time! If you're in PST like I am consider trying very late for us (~1AM) or around 1PM
 
7:21 AM
@0celo7 I don't know, but I've heard of him, so he's not un-famous ;)
 
7:32 AM
Happy belated bday @ACuriousMind
 
@user685252 thanks but you already wished me that from your other account ;P
 
@Mesentery what significant figure rules are you using?
 
8:08 AM
@JohnRennie Hey ! Good morning :)
 
Morning :-)
 
@JohnRennie Can we take that question from yesterday now ?
 
Yes I have a few minutes now. Over to PSS ...
 
8:24 AM
mornin
 
@Mesentery The units have nothing whatsoever to do with this. What "turned" the 110 into 108 was that you changed the significant figure rules you were using.
Just getting that on the record
@Vivek Questions are automatically put in a queue to be reviewed when you edit them after they were put on hold. So the review process should already be under way.
 
8:49 AM
@DavidZ See the last part in this image i.stack.imgur.com/TVTfQ.jpg
 
@Mesentery ah I see. The image is wrong.
At least the part where they say the answer is 108 is wrong.
Going by the same significant figure rule they were explaining in the earlier part, the (rounded) answer is 110.
My only guess as to why that image says it's 108 is that the author thinks having units after a number makes every written digit significant, kind of like how a decimal point works (e.g. "1100" has two sig figs but "1100." has four).
But that's not correct. Units (or the lack thereof) have no effect on the number of significant figures.
 
@DavidZ Ok Thanks! :)
 
No problem. I like unit questions ;-)
 
How can i know the reality of this video? Any one know the guy who performed this demonstration. I cant belive its juat complete animation.. ithink it may be some optical illusion..
 
It's a ruse
it's just a 3D animation
 
9:02 AM
Please dont just avoid by just saying it's fake.. i need it for cleat
How can it be with this much perfection..
At the starting a guy switches on the machine you can see his hands on to
On top.. pressing switch
 
Yes, it is a clever ruse of mixing real video footage with the original 3D animation
which is well known
 
And that flower pot..etcc..
 
You've been taken on a ruse cruise
 
In the link you provided . Its completly another video i have seen it
This is a different video i have checked it many times
 
My guess would be that it is likely the same trick
 
9:12 AM
But look at the video ..it's perfection ..i like to hear it's optical illusion.. because all things are.. glasses/crystal here
So some thing can occur
 
shrug
 
Everyone is avoiding... it. Can anyone make me believe it's complete animation
Shrug? What?
At least please any one show me another platform for getting coplete explanation for this.. but i really want the guy who did it/uploaded it
 
9:35 AM
I would appreciate it if someone could explain-to-OP/mediate/step-in/vote-to-reopen/vote-to-close here.
 
I'll vote to close
 
@Qmechanic I think I can contribute a comment
The question is already closed, right? Am I missing something?
 
Jesus there's a lot of questions in the close queue
 
9:57 AM
 
incredible
 
poor choice of typography
 
10:16 AM
"Can something be absolutely true and absolutely false at the same time? Parallel lines and rape are two examples of the Continuum Hypothesis in real life."
🤔
 
O_o
What
 
Fucking hell
Finally it has happened. We are using non-Euclidean geometry to backup male supremacy
Men apparently operate in a non-Euclidean space
 
the cylinder, probably
 
@DavidZ : Thanks.
 
10:30 AM
the most masculine shape
 
the cylinder is isometric to the plane though
not very non-Euclidean after all
 
It's flat but it's not euclidian
You can have more than one line between two points
There's more than one axiom of Euclid :p
 
10:44 AM
I think only $\mathbb R^n$ is Euclidian, as far as manifolds go
Any other flat manifolds won't be simply connected which I think will violate axioms already
 
@Slereah It's going to be diffeomorphic to $\Bbb R^n$, yes. I do not think the metric needs to be the Euclidean metric
Well, maybe
 
Hm
I think maybe it can be one of the Bianchi space?
I'm not sure
that's probably a question for @0celo7
he worked out the euclid axioms for manifolds at some point
 
What are the Euclid's axioms again?
 
In terms of manifolds, it's basically
1) between two points there's exactly one geodesic
 
I don't actually think the original axioms say that straightlines are uniquely determined by two points
No I don't think Euclid ever mentioned (1)
That's not an axiom
 
10:51 AM
The real axiom is "between two points there's a line"
But I am translating :p
 
So "there's exactly one" is bullshit
It just says any two points can be joined by a geodesic
 
1. A straight line segment can be drawn joining any two points.

2. Any straight line segment can be extended indefinitely in a straight line.

3. Given any straight line segment, a circle can be drawn having the segment as radius and one endpoint as center.

4. All right angles are congruent.

5. If two lines are drawn which intersect a third in such a way that the sum of the inner angles on one side is less than two right angles, then the two lines inevitably must intersect each other on that side if extended far enough. This postulate is equivalent to what is known as the parallel postul
here's a bunch
 
In fact that's exactly why hyperbolic geometry satisfies 1-4
 
Does 1 and 5 imply that there's only one, though
I think axiom 2 is basically that the manifold is complete
 
@Slereah Yes.
 
10:54 AM
I'm not quite sure what axiom 3 would be
 
Geodesic circles
 
Would that imply that the manifold is isotropic at every point
I'm not sure
 
Nah.
Geodesic circles always exist in complete Riemannian manifolds
 
Oh well
All right angle are congruent would be what
Parallel transport of two orthogonal vector is orthogonal?
 
That's a bad axiom which is not really interesting in the Riemannian context
 
10:59 AM
don't diss the Euclid
 
I'm not though, the point is angles are defined on tangent planes
Where Euclid says right angles are all the same
So it's literally automatic
for all Riemannian manifolds
 
I think I take back my previous comment. Your interpretation is likely the right one.
Parallel transport is how we identify two tangent planes on a Riemannian manifold
So under that identification, right angles go to right angles
"parallel transports are conformal isomorphisms"
 
Under Euclid it also means right angles under reflection, but that too is automatic for manifolds
 
is the typesetting brigade in? I need to rant
 
11:12 AM
@Slereah Wow. It's an open problem.
page 16, question 7.2.2
 
as seen in the wild
 
@BalarkaSen dang it
 
the template just starts \documentclass[twocolumn]{article} with no font options, and obviously the produced pdf is all in Computer Modern
 
You'd think Euclid would have hammered out those problems since then
 
@Slereah Yeah strange innit
Hm, I know that if my manifold has everywhere non-positive sectional curvature then it has no conjugate points
It's basically fiddling with the Jacobi equation
Can I have everywhere positive sectional curvature but no conjugate points? I don't think so.
Maybe something like R^n with the sectional curvature dying down towards infinity
 
11:21 AM
I know there's a few spaces that obey the Euclid axioms, but the other ones I know aren't manifolds
They're weird metric spaces
 
So the geodesics would have "conjugate points at infinity"
 
That is where parallel meet :p
 
Not really.
 
Is there any Bianchi space that seems to obey the euclid postulates?
 
I mean lines on Euclidean spaces have a linear rate of divergence
 
11:23 AM
That is where I'd look
 
idk what Binachi spaces are
 
Spaces with translation invariance of the metric
 
What does translation mean
Do you have a Lie group with a left-invariant metric
 
I don't really want to a read a full wikipedia page
Give me a definition and I'll think about it
Lie groups w/ left invariant metrics are homogeneous spaces which is not super interesting
I need to do the Taylor expansion calculation someday soon
Ugh too many things to do
 
 
1 hour later…
12:39 PM
"It would be nice to have a simple characterization of what counts as a holey spacetime. There are a number of motivations for this. One is militant: one might like to excise such dishonerable spacetimes our list of physically possible models."
"Suppose we began on a surface to the past of the handle. The data on this surface fails to determine if we are in plain old Minkowski spacetime, or whacky Deutsch-Politzer spacetime."
The whackiest of spacetimes
"Unfortunately, this definition turns out to be far too strong. As Beem (1980) showed, even Minkowski spacetime is locally extendible. So you can’t excise locally extendible spacetimes without excising good ol’ Minkowski spacetime as well!"
 
1:21 PM
@dmckee Update. My friend says thanks =).
 
"Quantum theorists silently slaughter cats in tightly closed boxes. For matters of consistency, general relativists prefer family affairs instead. They travel back in time to murder their grandfathers before they themselves were born. John Earman’s new book brings good news for the elder generation: Grandfathers do not figure so prominently in a critical account of general relativity (GTR) that any such experiment will ever pass an ethics commission."
 
2:15 PM
@Slereah proving that the straight lines are the shortest curves is actually not so trivial
 
@0celo7 For Euclidian space?
 
You pretty much have to nuke it with hopf-rinow
@Slereah yeah
 
Weird
Do you know if it's probable that Euclidian space is the only manifold that obeys the Euclidian axioms
 
I’ve thought about this. It’s not so straightforward to interpret the axioms in an analytic setting
 
yeah some are a bit tricky to adapt
especially if you look at the original set of postulates
It's like Euclid didn't even know differential geometry
Pretty sloppy for the founder of geometry
-3
Q: What is heavier - a steel or a fluff?

Arctomachine"What is heavier - 1 kilo of steel or 1 kilo of fluff?" - this question is usually asked as a joke to make a fool of somebody who chooses steel, followed by the "right" answer that both are equal. However there are 2 possible correct answers that I can think of: equal, if we compare thier mass...

good stuff
1. Let it have been postulated to draw a straight-line from any point to any point.
2. And to produce a finite straight-line continuously in a straight-line.
3. And to draw a circle with any center and radius.
4. And that all right-angles are equal to one another.
5. And that if a straight-line falling across two (other), straight-lines makes internal angles on the same side (of itself whose sum is) less than two right-angles, then the two (other) straight-lines, being produced to infinity, meet on that side (of the original straight-line) that the (sum of the internal angles) is less than
The original axioms, apparently
Or in proper greek
αʹ. ᾿Ηιτήσθω ἀπὸ παντὸς σημείου ἐπὶ πᾶν σημεῖον εὐθεῖαν γραμμὴν ἀγαγεῖν.
βʹ. Καὶ πεπερασμένην εὐθεῖαν κατὰ τὸ συνεχὲς ἐπ᾿ εὐθείας ἐκβαλεῖν.
γʹ. Καὶ παντὶ κέντρῳ καὶ διαστήματι κύκλον γράφεσθαι.
δʹ. Καὶ πάσας τὰς ὀρθὰς γωνίας ἴσας ἀλλήλαις εἶναι.
εʹ. Καὶ ἐὰν εἰς δύο εὐθείας εὐθεῖα ἐμπίπτουσα τὰς ἐντὸς καὶ ἐπὶ τὰ αὐτὰ μέρη γωνίας δύο ὀρθῶν ἐλάσσονας ποιῇ, ἐκβαλλομένας τὰς δύο εὐθείας ἐπ᾿ ἄπειρον συμπίπτειν, ἐφ᾿ ἃ μέρη εἰσὶν αἱ τῶν δύο ὀρθῶν ἐλάσσονες.
Ahah one of the footnote states "This postulate effectively specifies that we are dealing with the geometry of flat, rather than curved, space."
Very relevant for a paper from ancient greece!
Why are there footnotes for this acknowledgement
 
2:45 PM
Number 5 is impossible to read
Very hard to put into Riemannian geometry terms
 
What's the simplest statement of the parallel postulate in diff geo
 
I had this written down somewhere. It took some thought
Something like lines that are parallel at one point are parallel at very point
 
but then
what is the Secret Axiom of Euclidian geometry
The Pasch axiom
Not to be confused with Pasch's theorem regarding points on a line In geometry, Pasch's axiom is a statement in plane geometry, used implicitly by Euclid, which cannot be derived from the postulates as Euclid gave them. Its essential role was discovered by Moritz Pasch in 1882. == Statement == The axiom states that, Let A, B, C be three points that do not lie on a line and let a be a line in the plane ABC which does not meet any of the points A, B, C. If the line a passes through a point of the segment AB, it also passes through a point of the segment AC, or through a point of segment BC. The...
"Let A, B, C be three points that do not lie on a line and let a be a line in the plane ABC which does not meet any of the points A, B, C. If the line a passes through a point of the segment AB, it also passes through a point of the segment AC, or through a point of segment BC."
even worse
although I guess you can just do it by the intersection of geodesics
 
I would appreciate it if someone could explain-to-OP/mediate/step-in/vote-to-reopen/vote-to-close here.
 
9
Q: Are there simple models of Euclid's postulates that violate Pasch's theorem or Pasch's axiom?

Thomas KlimpelWhile reading a paper (pdf) about the history of modern logic, I learned that some opinions (about deductive/axiomatic mathematics) typically attributed to David Hilbert can be traced back to Moritz Pasch. After googling for Moritz Pasch, I was surprised to learn that he had found important impli...

Apparently violating Pasch's axiom is pretty hard
 
2:58 PM
@Slereah what?
that's so hard to read
this is why geometry is crap
 
It just means that if you have a triangle, a line going through one side of the triangle will also go through another side
 
ugh
I have forgotten how bad algebraic topology is
 
it has all the fun of algebra and of topology
 
double complexes yay
 
that's a lot of arrows
 
3:15 PM
man, I have forgotten all of this stuff
 
we are all but dust in the wind, dude
I should really look into trapped surfaces more
I'm p. sure I'm gonna need it
 
I'm going to cite the insane Spivak books
My bibliography is pretty heavy
Choquet-Bruhat, HE, Spivak, like 20 French people
Weyl, Weinberg
 
you can cite me
 
very physicsy for a math paper
 
I too am French
 
3:26 PM
Hello, I'm new here. With here I mean this site. What's the fucntion of the chat, and is it the only chat in the Physics S.E.?
 
Found a paper on a globally hyperbolic paper that's not hole free or Minkowski space : lps.uci.edu/~jmanchak/ishf.pdf
 
Morning
 
I'm still not 100% sure what holes imply
@Mr.Nobody the function is in the name
and there are multiple chats
 
We exchange stacks
 
yes
here is my stack
 
3:27 PM
Where? This is the only one I can find, I'm pretty lost in this site since I'm new
 
here's the physics chat rooms
 
@Mr.Nobody Nah, we're just messing around. But this is the main physics chatroom
 
Wow, I don't know if I'm comfortable with such bad jokes
 
there are other chats but most of them are for a specific purpose or pretty dead
one is just @Secret talking to himself
4
 
If you can't handle bad jokes you're in the wrong place.
 
3:30 PM
Just kidding, I live for bad jokes tbh
 
Earman's GR book seems nice enough
too bad it's expensive
 
And one more question, I don't understand how this site works, like, I've seen really complicated physics questions (for me at least) like PhD level, and they get solved like, how does it work? Do people that answer get rewards like economically I mean, because if not why do these people that know so much spend their time here instead of studying their things or whatever?
 
no, it's all based on the proven concept of "internet points"
 
@Mr.Nobody The reward is to help other people
That's it.
 
Oh no, I only do it for internet points
 
3:34 PM
Lol haha
Then you're either a very altruistic person or somebody who gets fooled by internet points
 
most people into physics just enjoy talking about physics but it's not a common conversation topic
 
@Mr.Nobody Well there are a lot of us
 
It's just fun to answer physics questions
especially if I can bring up weird papers
 
I've responded to one, and the person who asked gave me the green tick, but then I've seen a much better question so I guess that the asker will change the tick
much better answer*
 
@ACuriousMind Well I'm gonna cite him because he describes the conformal group of R^n pretty well
 
3:37 PM
you can upvote multiple answers
 
might be a strange citation for a PDE paper tho
 
Yeah, upvote, but the tick is only for one if I'm not wrong
 
this paper talks about FUTURE HOLES
"Every inextendible and causally simple spacetime is hole-free."
It's hard to follow papers on hole-freeness because there's like 6 different definitions
I assume that the hole-business is maybe related to the Cauchy problem, but they're fairly silent on any such link if it exists
 
3:58 PM
do you know about a recent paper on general relativity which talks about certain ways an object can move
 
that's a bit vague
 
it concludes that there are certain prohibited ways an object can move
 
well probably, yes, but still vague
 
it was controversial
what are your guesses then?
 
I hope this isn't about the warp drive again
 
3:59 PM
no
 
@xuBe are you thinking about the recent paper showing that under some circumstances the evolution is not Cauchy complete?
 
i have zero knowledge on gr
just heard this paper which got me interested
 
Or rather, allegedly showing the evolution is not Cauchy complete?
The jury is still out ...
 
how can i start learning general relativity
what is the math that i need to understand gr
 
@xuBe read Steenrod
 
4:03 PM
Why not Nozumi
 
i just know single variable calculus
 
@Slereah what's that
 
*Nomizu
If you just know single variable calculus I'd recommend 1) learning more first 2) Callahan
 
just read Zee and learn calculus from him
 
also maybe learn classical mechanics first
it's not as trivial as you'd think
 
4:08 PM
zee teaches you that
 
4:20 PM
For decent GR you need to at least know multivariable calculus
And for doing real GR you need multivariable calculus, algebra, group theory, differential geometry, topology, algebraic topology, Morse theory, analysis, etc etc
if you're wondering about that paper about the Cauchy problem for charged black holes it may take a while
 
4:50 PM
Though if you don't like math, you can always get this
 
Anonymous
5:08 PM
@Slereah Wow, that looks like a rare kind of book
 
5:18 PM
I think that book is meant for people doing computational work.
 
@Slereah 2,013th Edition ?
The Callahan book you mentioned looks really interesting.
 
@JohnRennie it's a nice intro book
 
it looks extremely basic
 
It is
It starts with diff geo via embedded surfaces
 
5:41 PM
I used to read it when I was an undergrad
 
guys what is this expression ? Looks like gauss law of electrostatics but involves magnetic field.
 
Anonymous
@Tanuj One of maxwell's equation iirc
 
What does it exactly show ?
 
But is CaCO3 soluble in water? Some people say that it's insoluble, others that it's soluble but it takes a lot of time
 
Like for gauss law in electrostatics , I know the term on the right denotes electric flux threading the specified area and the term on the left is the sum of all charges inside the gaussian surface divided by epsilon , but what do the terms denote here ?
 
Anonymous
5:49 PM
@Tanuj Line integral of electric field
 
Anonymous
on the left
 
Anonymous
$\phi$ is just flux
 
@Blue isn't it the surface integral ?
@Blue what is this electric flux and magnetic flux associated with ? Is there a gaussian surface here too ?
Okay got it , it is line integral in fact , but what does that even mean physically ?
@Blue where can I read more about it ?
@Blue got it on wiki , giving it a reading now.
 
@Tanuj no, it's a line integral
A line integral is when you integrate the function over a path
A closed one, in this case
hence the $\oint$
 
@Slereah yea , I figured it out .
@Slereah so this equation essentially follows that a time varying magnetic field will induce an electric field ?
 
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