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12:20 AM
I have proven that an apple falls at 9.8 m/s² in Schwarzschild spacetime
2
 
 
3 hours later…
3:12 AM
Just one apple, or all apples? And did you eat it afterwards?
 
3:36 AM
@DawoodibnKareem Wow, are you really from .ps?
 
3:47 AM
zup
 
 
1 hour later…
user228700
5:08 AM
@JohnrR: Morning! :-)
 
user228700
 
user228700
Yay! Ze flower!
 
Aha, you got your pictures of flowers transferred! :-)
That looks as if you've had a bit of rain ...
 
user228700
Nope. I'm using my mobile to upload it. The dumbass that I am, I didn't think of that yesterday.
 
user228700
@JohnRennie Yep, we most certainly have! In fact, it's drizzling right now!
 
5:12 AM
This week is forecast to be very wet in the UK. Nothing to do with the monsoon, just regular British summer weather :-)
 
user228700
I have mushrooms and cows and goats as well!
 
user228700
@JohnRennie Ah :-)
 
@Kaumudi.H All taken in Kerala?
 
user228700
 
user228700
@JohnRennie All taken here, yep!
 
5:17 AM
How did the train work out BTW?
 
user228700
Still in Kerala, Sir! Train's at 9:50 PM this evening.
 
Just you on the train?
 
user228700
5:28 AM
@JohnRennie Yep, why?
 
user228700
(Sorry about that; was devouring mangoes for breakfast)
 
I had mango on Saturday!
The local supermarket had them on offer.
 
user228700
@JohnRennie Nice! :-) These were freshly plucked just a few days ago!
 
Sadly the mangos from the supermarket are nowhere near as nice as freshly picked ones.
We used to get fresh mangos when I lived in the Sudan.
 
user228700
Right :-(
 
user228700
5:32 AM
@JohnRennie Mangoes in Sudan?! Cool!
 
The trouble is the mangos have to be picked unripe so they don't go bad while being shipped to the UK. They do ripen in transit, but they aren't as nice as mangos picked when they have ripened on the tree.
 
user228700
Ah, I see. Well, the ones I just had weren't picked ripe: since we're leaving today/tomorrow, my grandma had them picked a bit raw so that they would half ripen before we left.
 
@Kaumudi.H I don't think mangos are native to the Sudan because it's very dry and mango trees need a lot of water. But they are farmed there - or were.
 
user228700
They weren't sickly sweet but they tasted just fine!
 
user228700
@JohnRennie Right, right, which is why I was curious about that. I see...
 
user228700
5:36 AM
I'm excited about travelling alone tonight! Never done that before!
 
I suspect it will be exciting for a few minutes, then very boring!
Take a good book :-)
 
user228700
I agree :-P I might not be able to read; all the lights will be off :-/
 
user228700
I'll climb in and try to go to sleep!
 
I need to manually update the software on some servers. I've just run a query to check how many servers are affected, and there are 127 of them!!! That will keep me busy for a while.
 
user228700
Oh, sheesh, wow.
 
user228700
5:46 AM
OK, have fun!
 
Probably not that much fun :-) Oh well.
 
user228700
Ah :-/ I just got a shitton of money, BTW! Now would be a good time to order a harmonica and books!
 
6:16 AM
@Kaumudi.H In the UK second hand books are available from Amazon and eBay, and they can be very cheap. Is that the case in India as well?
 
yeah
 
user228700
@JohnRennie Second hand? I'm not sure if they're second hand. The ones on Amazon anyway...
 
Sorry for answering a question directed at you, @Kaumudi : P
 
user228700
And I'm not sure if I will find the specific books that I'm looking for on eBay...
 
user228700
@Avantgarde Lol, no problemo :-)
 
SBM
6:22 AM
school's over for today; just reached home.
Hello people
 
hey SBM
 
user228700
Yello :-)
 
@Kaumudi.H it might be worth considering though. Although I prefer Amazon to eBay for buying second hand books.
 
user228700
Hmm. OK, I will look it up. Thanks :-)
 
SBM
@Kaumudi.H Yellow?
 
6:25 AM
Wow, it's just started raining cats and dogs in Wookey Hole :-(
 
I just went through the amazon website of India to check for standard physics textbooks. There doesn't seem to be a section for selling used books
 
user228700
@SBM No, um, that was "Hello", disguised as a shortened version of the word "Yellow" because yellow is a happy color and...oh, never mind :-P
 
@Avantgarde yes, I just checked a couple of books that I know K has read and I couldn't find any second hand ones either.
 
user228700
@JohnRennie Not a fan of rain?
 
@Kaumudi.H no, rain just makes everything wet, muddy and dirty
 
6:27 AM
Maybe not these particular books, but some others might be sold used (though I searched for the most standard references so it's already a bad start). Maybe there are different websites for this. Usual bookshops might have them. But it might be hard to find something elusive..
 
SBM
@Kaumudi.H Yellow reminds me of hufflepuff.
 
I guess I shouldn't complain since we need rain, but that doesn't mean I have to like it.
 
I dislike rain too
 
user228700
@JohnRennie I agree with you 100%.
 
SBM
@JohnRennie True I hate summers but I also hate rain
 
user228700
6:28 AM
@SBM All the better for I am a ravenpuff!
 
Aha! I found a used Weinberg's QFT Vol 1!
 
@Kaumudi.H Better than a Slytherclaw :-)
 
at 25% of the new book's price. (Even after that it's not cheap at all lol)
 
SBM
I thought I was the only hufflepuff in here
Certain books are so costly.
 
Weinberg's QFT? That's a seriously tough book to read :-)
 
6:30 AM
Oh yeah, I suppose.. It's definitely not the first (or second, or third..) book to pick for QFT
But it's a must-have. I presume the book is filled with nice personal insights and explanations not to be found anywhere else
kinda like the QFT analog of MTW's Gravitation. Though I've never read MTW.
 
user228700
@JohnRennie :-)
 
user228700
@SBM Nope, you have me for company! I'm a bit ambigious though, hence the "ravenpuff". I've been sorted into all four houses over the years but my values and passions align most with Ravenclaw and Hufflepuff in that order.
 
@JohnRennie Have you read MTW? Or parts of it
 
@Avantgarde Parts of it.
 
Did you like it?
 
6:34 AM
It is quite fun to read. It is written in a witty way.
 
SBM
$\large \ddot \smile$
MTW?
 
I see. That's nice.
 
But it isn't for the beginner. The authors assume you're already pretty good at maths and it's written that way.
 
user228700
Damn, LaTeX still isn't working :-/
 
@SBM Misner, Thorne and Wheeler - Gravitation.
 
6:35 AM
@SBM MTW = Misner, Thorne, Wheeler. The standard brick of a book on General Relativity
 
SBM
Okay two different things I see
LaTeX rendering instructions
 
It's more of a treatise than a book. It'd be a feat to actually read through the full book
 
user228700
Ooh, the updated one. Thanks! :-)
 
user228700
6:52 AM
@JohnR: Please ping me back when you're free(ish)!
 
@Kaumudi.H I'm freeish now. I'm doing bits and pieces at work but I'm interruptible :-)
 
user228700
Wokay! I was wondering about a book. Hang on, I'll message you on gchat.
 
7:13 AM
At 4:03, does that really happen?
why are particles even going near the object
nvm
he acknowledges (at 4:44) that there are problems with that explanation
 
7:52 AM
Any mods around?
 
SBM
I'm afraid I don't know.
 
8:12 AM
I am doing some refreshing on Analytical mechanics,
almost all results in my book is based on an approxmation:
1st order approxmation
I wonder whether there is something interesting going on in higher order (say, strange result)
or the author just too lazy to give a complete proof.
 
which book?
 
@Avantgarde David Morin's Introduction to Classical Mechanics
 
Okay.. I've never heard of that one
 
@Avantgarde it has the best problem-set; however, the reading is a bit average.
and it has very good physics jokes
 
haha
I did my learning from Goldstein
which was a hard book
but quite nice
 
8:32 AM
I am thinking my next step
should be Goldstein, or Landau?
(classical mechanics)
 
I haven't read Landau
Goldstein is a good book but it is tough to read. The problems are hard too
Fortunately, my lectures were pretty good. I only read parts of Goldstein
 
 
1 hour later…
9:42 AM
@peterh No, I'm just a wee bit political.
 
@EmilioPisanty What's up?
 
@ACuriousMind reckon this one's ready to be reopened
-2
Q: Why does this paper report potential energy in kHz, and what does it mean?

SamI am interested in studying theoretically the double well system shown in the figure below, which shows an experimental demonstration of an atomtronic battery. Caption: Figure 1. (a) Schematic of the double-well atomtronic battery system. The top panel shows the longitudinal potential e...

I've got an answer ready and would like to close the tab
 
what's the superspace in superstring theory
Is it the 2D space or the target space
 
@EmilioPisanty I concur; done.
 
@ACuriousMind excellent
thanks
 
9:47 AM
@Slereah The target space, the worldsheet has no fermionic components. You can view the action as a "modified supervolume" for the embedding $\Sigma^{2\vert 0}\to \mathbb{R}^{10\vert \mathbf{N}}$, where the $\mathbf{N}$ controls which of the string theories you get, this view of string theory is called the Green-Schwartz action
 
Alright
Is it fair to call a string a timelike 2D submanifold?
 
I don't think there's any requirement it be timelike.
 
whaaat
Well i guess it could be null
Oh wait is that why some people say there are tachyons in string theory
are there strings that span a spacelike submanifold
 
@Slereah No; bosonic string theory has tachyons simply because the ground state has negative mass.
 
oh, that kind of tachyon
Boring
 
9:55 AM
@Slereah I am not sure that is a well-defined question.
Given that the metric on the world-sheet has signature +-, I guess the classical answer is "no"
 
Is the signature inherited from the target manifold?
or is it independant
 
That depends on your philosophical idea of how the string action works :P
I mean, you can view the action just as a 2d SCFT with a bunch of scalar and fermion field, you don't need to talk about the target spacetime at all if you're careful.
 
well you have to at some point if you want to talk about the real world
 
If you take the traditional "worldsheet" stance, then you start with a worldsheet, i.e. some abstract thing that represents what a string traces out over time, and of course that already has a notion of time/space, so it starts with that signature, so it's not "inherited"
 
Isn't the worldsheet embedded in Minkowski space?
Or at least some manifold with fixed geometry
 
10:00 AM
@Slereah Some people like to say "spacetime is not fundamental in string theory", and what they mean is that while you may assign one (or several!) target spacetimes to a particular string theory, there's no unique or "real" one.
 
How do you perform measurements in string theory then?
 
@Slereah In the GS view with the modified supervolume you look at embeddings of an abstract worldsheet $\Sigma^{2\vert 0}$ into super-Minkowski space, so the abstract object obviously has to exist prior to embedding
 
Abstractly, at least
 
@Slereah I do not understand the question :P
 
@ACuriousMind Does it have to "match", though
 
10:02 AM
Match what?
Oh, I guess the embedding is "isometric"
 
Does the restriction of the metric on the target superspace to the worldsheet have to be the sheet metric
 
Ah yes
thanks
So I guess it is timelike
 
10:45 AM
o/ @ACuriousMind @Slereah
 
SBM
@Danu Hello
 
hi
 
Wait
If you don't need the target space for string theory how do you differentiate superstring theory from string theory
 
@Slereah Fermionic fields on the worldsheet :p
 
A superworldsheet?
the big problem with string theory is that there's a really big gap between GR + QFT and string theory
A lot of necessary things in between that are rarely done
 
11:02 AM
@Danu moin moin
@Slereah No, just a worldsheet with fermionic fields on it
 
If strings are submanifolds of the target space with a conformal field defined on them, and that a Lorentz cobordism implies the formation of closed timelike curves, wouldn't the process of a closed string splitting in two closed string involve something weird?
 
Bosonic string theory is a 2d CFT, superstring theory a 2d SCFT (or rather, their actions are that; string theory is not the same as just CFT)
 
The worldsheet would basically be CFT on the pair of pants spacetime
Which is singular and has CTCs
 
@Slereah No one claims that these processes "happen", I think
 
yes, but still
 
11:04 AM
These diagrams where a string splits or whatever are exactly analogous to Feynman diagrams
 
It's part of the "perturbative expansion" i guess
So it means that there's some possible causality violation in the perturbation
 
You should not take them as a literal representation of what happens/can happen
 
which relates to my old question of the links between quantum gravity and CTCs
 
@Slereah Would you claim there's "causality violation" in Feynman diagrams?
 
Well there are off-shell particles, certainly
 
SBM
11:05 AM
@ACuriousMind feynman diagrams?
 
The perturbation series is not claiming that these stringy Feynman diagrams are also embedded in the target spacetime, by the way
 
Hm
but still
Asymptotically
 
It's just...abstractly summing over them, there's not really a trace of the embedding if you don't insist on it (yet another point where the target spacetime is rather inessential)
 
You could have one closed string becoming two closed string
which means that the scattering matrix would be some Lorentz cobordism in between
I probably should read more string theory first tho
I'm still not up to string interactions
Even if the causality violation is "off shell" that would be interesting, if true
 
I'm stuck doing GR-style tensor computations :(
 
11:10 AM
I mean you don't even need the target space to infer causality violations
 
SBM
@Danu GR?
 
Any lorentz cobordism like that has causal weirdness
 
general relativity
 
SBM
oh
 
I'm gonna take a guess and say that there's probably no exactly solvable string process
especially interacting ones
no string Sine Gordon
Is there a standard notation for the worldsheet space and target space?
Like if I want to write that $X : \Sigma \to \mathcal M$
With the worldsheet $\Sigma$ and target space $\mathcal M$
What's the usual notation
 
11:27 AM
@Slereah Define "exactly solvable"
 
Yeah I guess that is also the issue
 
I have a feeling you're thinking far too "classical" about strings.
 
Well gotta start somewhere
I am not quite ready to drop the target space quite yet :p
Also CFT on a curved spacetime is an odd definition of "classical"
 
I mean not the target space thingy, but thinking that the classical strings and their motion are in any way what string theory is about :P
 
@ACuriousMind Still on the beginning of learning!
And the first chapters of string theory are always relativistic strings
 
11:30 AM
Sure, that's where one starts, but you seem to be trying to extrapolate all sorts of things about string theory from that description when no one really proposes that that classical part has much, if any, significance, I think
 
Could be
 
You're gonna quantize that theory of the relativistic string and what comes out has very little to do with what you had as a classical picture, much like understanding a classical field theory doesn't really tell you much about its QFT
 
Yeah but the fact that you have possible topology change on the 2D space seems very weird
Since independantly of any matter on it, that is causally very badly behaved
 
You don't, really. The string perturbation series that introduces these is purely quantum - no one claims the classical strings behave in that way.
 
Sure, but you still have to perform calculations on it
How do you perform the "integral" on terms where the CFT might not even be well defined?
 
11:33 AM
Yes, but no one claims that is an "actual" worldsheet, so what does causality matter? It's just a computational tool.
@Slereah The CFT does not care one whit about GR or causality.
 
Doesn't it?
 
Nope
 
Weird
I should look up what the string "propagator" looks like, i suppose
But doesn't it depend on the worldsheet metric $\gamma$?
in the same way that CFT does on a 2D spacetime?
The CFT of a scalar field in 2D is gonna be like... $$G(\tau, \sigma) = \int \mathscr D\phi \exp{(i \int d\tau d\sigma \sqrt{-\gamma} \gamma^{\mu\nu} \partial_\mu \phi \partial_\nu \phi )}$$
Or something of the form
I'm not sure it's well defined on the trouser spacetime
Hence my confusion
 
11:53 AM
Let vector A and Vector B be the two vectors of magnitude 10 unit each. If they are inclined to the X axis at 30 deg and 60 deg respectively, find the resultant.
The answer is 20 cos 15 deg
How do I solve this one?
 
Inner product
$A \cdot B = |A| |B| \cos \theta$
 
We want sum
Right?
We have to ad the vectors right? @Slereah
brb
 
Jim
Hear ye! Hear ye! Direct from the mouth of Jim, I am announcing officially that June 7 shall henceforth be Physics Pun Day here in the hbar. That's right, save up your best puns, research great ones, create new ones. On June 7 (this Wednesday), we shall unleash pun-ishment on all around. The creators of the best puns shall be immortalized, the worst puns will be mocked until I can't type any more. It's sure to be fun on the pun, so come out and bring a sense of humour
 
12:11 PM
@Slereah I don't know what you mean by "string propagator"
 
Isn't there a propagator for string theory
Also that string book says that in 2D $R_{\mu\nu} = \frac 12 g_{\mu\nu} R$
 
SBM
String theory
 
Isn't it $R_{\mu\nu} = g_{\mu\nu} R$?
cf
4
Q: the Ricci curvature in two dimension

Sepideh BakhodaIn two dimensions, we know that the Ricci curvature can be written in terms of the Gauss curvature K as $Ric(g) = Kg$. Can anyone prove this? Sorry if the question is too trivial :).

 
@Slereah I'm gonna bet on "different normalizations" there :P
@Slereah See, I don't understand what you mean by that
 
For a starting state of $|\mathfrak{string}_i \rangle$ and a finishing state of $|\mathfrak{string}_o \rangle$, how does one compute the transition amplitude between those states
I'm not sure this is related to different normalizations
I think it's part of the whole "2D GR isn't dynamic" rigamarole
Of which i have never seen a rigorous proof
 
12:21 PM
@Slereah Yeah, you should just read up on string interactions
 
Will do!
I roughly understand conformal symmetry and supersymmetry so things should be easier now
I have a proof somewhere of the Gauss Bonnet theorem for 2D Lorentz surfaces
I should try to actually prove the whole 2D isn't dynamic thing
Not as easy as it sounds
because of the whole York Hawking Gibbon term
 
@Slereah This isn't so bad, is it? It's just that the Einstein tensor vanishes identically.
 
But DOES IT?
I'm not 100% convinced that that is true
 
I think I have a proof written out.
It might not be rigorous.
Let me check.
 
Since in 2D we have $R_{\mu\nu} = R g_{\mu\nu}$, that means the Einstein tensor is $\frac12 R g_{\mu\nu}$
Not quite identically vanishing
 
12:27 PM
 
And the proof with the Gauss Bonnet theorem doesn't hold water because 1) the Gauss Bonnet theorem for Lorentz spacetimes is slightly different 2) it's valid only for compact sets so you have to work with the York term
 
You see if you think it's fine or not, I'm too lazy to check.
 
I'll give it a look, thanks
I mean I'm sure it's true, but an actual proof would be nice
 
This purports to be an actual proof
I remember it not being so easy to see why those last expressions vanish, except in locally inertial coordinates
I may have overlooked some kind of subtlety, who knows.
 
How does that mesh with $Ric = R g$ though
Can't be $Ric = Rg = Rg/2$, I don't think $R$ generically vanishes
Hm
I'll have to compare the two proofs
 
12:36 PM
Guys, shouldn’t $\vec p$ point in the opposite direction? For we know that
$$
p=\sum_i q_ir_i=qr_+-qr_-=q(r_+-r_-)=qd,
$$
where $\vec d$ points from the positive charge to the negative charge. Since the electrons in the water molecules are attracted by the oxygen nucleus, it seems to me that $O$ is $\delta-$, and $H$ is $\delta +$, so the dipole moment should be pointing in the direction of $O$.
 
@Slereah My document also shows that it generically doesn't
 
Ah wait
Apparently it's not $R$
It's $K$
And $K = R/2$
So it's all good
Phew
Damn Gaussian curvature
 
oh never mind
apparently I made some error. what my book does is correct
I'll just have to reread it
 
@Slereah Dont we have to add the vectors? Why are you finding the cross product?
 
oh, my mistake was that i thought that $\vec r$ was the distance vector (between the charge and the observer), but it's just the position vector of the charges.
 
1:18 PM
Guys, I’m confused by the minus sign that appears in $V$. We know that $\mathbf E$ points radially outward. We also know that $V=V_a-V_b$ (since $V_a$ is the potential on the positive shell with radius $a$, and $V_b$ on the negative shell), so I would think that we have
$$
V=-\int_b^a E\hat r\cdot d\vec l=-\int_b^a -Edr=\int_b^a Edr.
$$
Apparently I'm making some error with directions, but I wouldn't know where.
 
@ShaVuklia Where does the second minus sign come from?
 
@ACurious Since $E$ points radially outward, and we integrate from $b$ to $a$, our infinitesimal vector $d\vec l$ points radially inward
 
@ShaVuklia How do you know $b$ is the outer sphere?
nothing in that solution you posted really declares it to be one or the other, so sign issues can be fixed by just adjusting what is $b$ and $a$
 
It has to be, since $-\int_b^a Edl=V_a-V_b$, and we always subtract the potential on the positive shell (the inner sphere) from the potential on the negative shell
I see that since $a<b$, their potential $V$ is in the end positive
so they must be doing the right thing, since $V$ has to be positive @ACurious
though, if you think about it, $\int_b^a Edr$ seems like a positive quantity to me too
 
@ShaVuklia Not if $b > a$.
 
1:30 PM
oh right
okay, well that's "good news", because then I'm doing something wrong.
 
So, I guess the issue here is the notation $\int_b^a$ for the line integral $E\cdot\mathrm{d}l$
Because that, actually, includes the orientation of the path "twice" as you're reading it: It has it once in the order of the boundaries, and once in your infinitesimal vector pointing radially inward
Which is clearly counting the orientation once too often, which is where your error with directions lies.
 
oh
you mean $dl<0$
right?
 
The text you're reading cheats by including the orientation in the order of the boundaries, so it doesn't have to care about the orientation of the line element.
 
like, within the integration, the $dl$ "adjusts" appropriately
 
@ShaVuklia I don't know what that is supposed to mean
My point is that writing a line integral as $\int_b^a E\cdot\mathrm{d}l$ is, strictly speaking, non-sensical
Line integrals are not over intervals $[b,a]$, but over oriented paths.
 
1:33 PM
oh right
 
So that there is code for "integrate along the straight path from a point on the sphere at $b$ to the sphere at $a$".
 
yea I know that. we could have taken any (continuous, I guess) path from $b$ to $a$
and in our case it made sense to choose a straight path
I'm guessing I should revise a bit on line integrals then
 
By the prescription for line integrals, one would then evaluate that as $\int_a^b E\hat{r}\cdot\mathrm{d}l$ (note the order of the integration boundary; the evaluation prescription for line integrals always has them in the order where the smaller bound is also really the lower bound), which is equal to $\int_b^a E\mathrm{d}r$ because $\hat{r}\cdot\mathrm{d}l = -1$, because it's pointing radially inward as you said.
 
ohh, so you're saying they already switched $a$ and $b$, because they knew that $\hat r\cdot dl=-1$ in the case we went from $b$ to $a$?
 
1:38 PM
that really is a dick move
 
SBM
Gauss theorem?
 
(I still love Griffiths tho)
@SBM nah
 
It's pretty much cheating, but that's what physicists do :P
 
SBM
oh
I was also doing contour integrals coincidentally
 
no but honestly! if you're going to play around like that, then you should at least include a picture where you denote what $a$ and $b$ are
but alright, I'm happy it's solved!
thanks a lot @ACurious :)
 
SBM
1:42 PM
oh playing with $$\mathbf E = \dfrac{-\mathrm dV}{\mathrm d x} $$ I see
 
Hey John
 
@Slereah afternoon :-)
 
hello
 
rob
Greetings all
 
SBM
hello
good evening people
 
1:57 PM
would anyone be willing to help with some school/acceleration advice?
 
SBM
@heather oh what happened?
 
rob
@heather Those two words don't often go together in my experience; you could mean many things.
 
@rob, fair enough =)
basically, my situation is that i want to take this calculus class offered at a university near me this summer.
 
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