« first day (3652 days earlier)      last day (1574 days later) » 

01:55
0
Q: Two helium balloons meet a cocktail party. Do you think they might find each other attractive?

Roger WoodHere we are talking about the mutual force between the two balloons. This is in the context of Newton's law of gravity (so electrostatics etc. are ignored). You can assume that the cocktail party is held in a room that contains air. It is not necessary to assume that the Earth's gravitational fie...

0
Q: A system with effective negative gravitational mass but positive inertial mass

Roger WoodThis post is related to an earlier question "https://physics.stackexchange.com/questions/589812/is-it-possible-that-antimatter-has-positive-inertial-mass-but-negative-gravitati?noredirect=1#comment1328882_589812" for which I received a lot of valuable and informative feedback - thanks! I'm hopin...

The quick closing and suboptimal commenting on these illustrate the (perhaps inevitable) shortcomings of a large site like Physics SE.
 
2 hours later…
04:11
Morning
 
1 hour later…
05:39
@SirCumference morning! :-)
123
123
06:12
Morning All...
@JohnRennie do you remember our chat for avogadro's law ?
You said that if we double the number of molecules , the pressure will be different and thus it is inappropriate to use avogadro's law since it is defined for constant temperature and constant pressure ..
@JohnRennie But according to kinetic gas equation temperature also depends on the number of molecules with this formula : (1/3)mNc² = RT , where N is the number of molecules. So double the molecule will double the temperature keeping other quantities constant. Right ?
@Ankit hi :-)
I'm answering a question in another room but I shouldn't be too long.
@JohnRennie okay take your time :)
06:57
@JohnRennie are you free now ?
@Ankit hi
@JohnRennie can we start now ?
Shouldn't that be 3/2mNc² = RT ?
i.e. it's the equipartition of energy theorem that says the KE of each molecule is equal to kT.
@JohnRennie no , KE = (3/2)RT
No wait, I got that wrong. The KE = 3/2 kT
So ½ mc² = 3/2 kT
07:04
Yes
Rearranging we get 1/3 mc² = kT, and multiplying both sides by Na we get 1/3 Na mc² = RT
Which is your equation.
@JohnRennie yes now can we say that doubling the total mass doubles the temperature for same c ?
In that equation Na is Avagadro's number so it is a constant. If you want to double the total mass the only way to do this is to double the mass of each molecule m.
And that would indeed double the temperature if we keep c constant.
@JohnRennie but you defined it for one mole only . Actually it is n × Na . Right
?
If we use N to mean the number of molecules and n the number of moles then N = n x Na
07:12
So it is m×Na or m×n×Na indicates the total mass of the gas . So we can increase the total mass by only changing the number of molecules . Right ?
You can take 1/3 Na mc² = RT and substitute Na = N/n. In that case you get 1/3 N mc² = nRT
But if you change N on the left hand side it also changes n on the right hand side.
Yes thete is no problem to have unequal no. Of moles.
There *
@JohnRennie Wait for a sec . I am typing my question. It may take long :)
Right, but if you double N on the left side it also doubles n on the right side and T stays unchanged.
@JohnRennie so increasing the number of molecules doesn't affect the temperature ?
No it doesn't
The temperature is proportional to the KE per molecule
07:20
@JohnRennie so it can only change if we change the speed of the molecules or their mass ?
@JohnRennie but why is temperature defined as KE per molecule and not total KE ?
That's the equipartition of energy theorem. It says every degree of freedom gets an energy of ½kT, and since there are three degrees of translational freedom it says the translational energy is 3/2 kT i.e. the KE per molecule is 3/2 kT.
@JohnRennie sorry I didn't get that .
In classical statistical mechanics, the equipartition theorem relates the temperature of a system to its average energies. The equipartition theorem is also known as the law of equipartition, equipartition of energy, or simply equipartition. The original idea of equipartition was that, in thermal equilibrium, energy is shared equally among all of its various forms; for example, the average kinetic energy per degree of freedom in translational motion of a molecule should equal that in rotational motion. The equipartition theorem makes quantitative predictions. Like the virial theorem, it gives the...
08:08
@JohnRennie any tricks for guessing which scalars don't vanish at a singularity?
Are any scalars defined at a singularity? Isn't the whole point that the geometry is undefined there?
08:49
@JohnRennie sorry, to check whether a point is a singularity or an artifact of the coordinate system
Ah, OK. scalars are coordinate invariant so all scalars have a well defined value at a coordinate singularity. It doesn't matter whether that value is zero or non-zero, only that it exists.
Wait a sec - I think I meant to ask something else (but along those lines)
I can't for the life of me remember - isn't there something where you have to keep checking higher and higher-order scalars to see if one of them blows up as we approach the singularity?
e.g. approaching r=0 for the Schwarzschild metric
@JohnRennie ping
 
3 hours later…
11:36
Just wondering, the procedure that moves us between state vectors and wavefunctions $\langle x|\psi\rangle$ involves the use of the elements of the extended, rigged Hilbert space, does this means that the original Hilbert space $\mathcal H$ is still isomorphic to $L_2(\Bbb R)$ but also that the larger rigged Hilbert space is isomorphic to $L_2(\Bbb R)$?
the larger space is not a Hilbert space
for one, $\langle x \vert x'\rangle$ is not a real number, so it has no well-defined inner product
The larger (rigged) Hilbert space is the dual of the domain of $\hat{x}$
Which is uuuuh
The Sobolev space $H^{2,1}$?
That is the so-called Gelfand triple
You have the Hilbert space, a subset of that Hilbert space, and the dual of that subset
$$H^{2,1} \subset L^2 \subset H'^{2,1}$$
Or something to that effect
ok ty, it's time to stop being lazy and just go try learn this :P
11:43
The benefit of a Hilbert space is that you have Riesz' theorem
For a Hilbert space, the dual of a Hilbert space is isomorphic to the Hilbert space
so if $|\psi\rangle \in L^2$, you can say that $\langle \psi | \in L^2$
But this isn't true of the more general wavefunctions
That's why you have to be careful
 
1 hour later…
13:03
@ACuriousMind Why do people use the Lorenz gauge with the Proca equation
I thought it wasn't gauge invariant
@Slereah they're not gauging, the "Lorenz gauge" is an equation of motion for Proca theory
Is it?
see Wiki
it's not directly the EL equation but you can split the E-L equation into the "gauge condition" and the more "ordinary" e.o.m. like Wiki does there
ah yes
I'll look up a derivation
ok I refined my question a little - is there any better method than trial and error for checking if any curvature scalar blows up
you know, while trying to see whether a "pole" is a true singularity or just a coordinate-system gig
13:10
I'm not sure, tbh
But at the very least, there's a limited amount of scalars to consider
Are you sure about that?
Infinite, but you can check them, and as far as I know, it's rarely the case that you have to go very far to find a divergence
Why can't I contract arbitrary products of the Riemann tensor?
oh ok
Usually you only have to check $R$ or $R_{ab} R^{ab}$ or $R_{abcd} R^{abcd}$
I can't think of any example where all of these are finite but a higher term isn't
There may be but it seems unlikely
probably pathological
but I'd be pretty disappointed if I had to check something like $R_{\mu\nu\rho\sigma}R^{\rho\sigma\lambda\tau}R_{\lambda\tau}^{\mu\nu}$
Although even that's one of the "small" scalars
13:16
Also proving that every component of the Riemann tensor is finite would be enough to prove that no scalar diverges, but of course that would require finding an appropriate coordinate patch
oh yeah, I didn't think of that
There's a method that only requires the Riemann tensor, but it's kind of worse?
You only have the Riemann tensor but then you have to do it on all the curves
Which is bad because some singularities are directional
ie they're not divergent on one curve but are on another
whoa, I'll check those out
if you want an example it's uuuuh
The Israel singularities I think?
Werner Israel, right?
13:19
Yes, not the country
because right now I'm getting search results for ethics in conflict :p
The Israel-Khan spacetime
"two black holes held in equilibrium by a strut"?
13:22
But unless you're doing specifically studies on singularities, don't worry too much about it
@Slereah Good Evening! :-)
No standard example of a spacetime has really weird singularities that can't be hacked out with just quadratic Riemann polynomials
Hello
in any case I'll be using FORM for practically anything related to big tensor contractions
sup?
there may be theorems proving that such and such spacetime is non-singular given some conditions, but I can't think of anything general
13:26
Programmers often confuse between Halloween and Christmas because Oct 31 = Dec 25.
5
@Azmuth that used to be my favourite conversation starter :D
@Azmuth lmao
😎
14:19
Does anyone has some solutions to Pimple/Acne problems...
?
My skin is a bit oily and I've to clean them every 5-6 hours (I live in a very high humid region), these pimples come and sometimes some pain too...
Could somebody motivate the Chern-Simons action?
This one: $\int_M A \land dA$
14:36
something something topological invariant?
15:10
@NiharKarve that's not the Chern-Simons action, you're missing the $A\wedge A \wedge A$ term
The Chern-Simons form $\omega$ in $2n-1$ dimensions fulfills $\mathrm{d}\omega = F^n$ (insert $\mathrm{Tr}$s if appropriate), so the action $\int_M \omega$ is the boundary term of a Yang-Mills theory in $2n$ dimensions living on a bulk with boundary $M$.
15:29
@ACuriousMind yes, sorry, I meant the Abelian CS action
what does insert traces if appropriate mean?
in the non-Abelian case you have $\omega = \mathrm{Tr}(...)$ and $\mathrm{d}\omega = \mathrm{Tr}(F^n)$
why are so many of the top reps European?
seriously, in the top 11, excluding Kevin Zhou and Floris
15:53
that seems an arbitrary point for cutting off the "top"
@NiharKarve If you look at the top 12 at least 4 aren't European, possibly 5. All 5 might be from the US even. If you go to top 16, I think somewhere between 7-9 of the users aren't from Europe, and possibly from the US.
16:31
0
Q: Why is it that people send questions from here over to worldbuilding even if they dont fit there either?

Topcoderecently a user made a post on worldbuilding about making a flying saucer in real life stating that he was told to go to worldbuilding by user on physics stack exchange. Unfortunately i don't have enough rep to view the original deleted question or the comments on it, but it was decided that the ...

@JMac which four arent European?
@NiharKarve Floris (probably), Emilio Pisanty, knzhou, Selene Routley and no one knows where Qmechanic is from ;)
@NiharKarve Well Floris and DavidZ have their locations in the US clearly. knzhou is in the US, and I believe dmckee is from the US as well, or at least taught there.
ah yes, add dmckee and DZ
And that's mostly based off locations obviously, I don't know who is actually from Europe and who might just live there right now, same for US.
16:41
The devil's heating mantle
I'd have thought there's no need to heating mantles in hell
Turns out there is
And Jeulin provides them
"A Beautiful Mind" vs "The Theory of Everything" - go
I've seen neither :P
Out of those two, definitely Shrek 2.
16:46
I approve
@ACuriousMind Neither have I. I have window watched them a lot of time, but never have decided on whether to watch them completely or not.
what does "window watched" mean?
@ACuriousMind Just extend the definition of "window shopping" to watching movies. ("window watching" is not a real word, it's fake ;)
all words are made up
@ACuriousMind well, any other good biographies based on a scientific personality?
16:50
not a big biopic watcher I'm afraid
nor a reader of biographies
Feynman's?
Surely you're joking! :D
Zee takes $A \wedge d A$ as his Chern-Simons Lagrangian as part of talking about anyons in 2D and says it's a way to demonstrate fractional statistics, seems interesting idk what the higher D version means
I've actually never read much of Zee, how is he?
16:53
@ACuriousMind Do you read much fantasy? I know you've read Mistborn but that's about it lol
Zee is good, worth checking
@JMac Yeah, mostly fantasy and sci-fi, though I'm reading far fewer books these days than I used to
@bolbteppa is he as chatty as Griffiths QM? (although I'll admit the main reason I turned to other books was because I wanted to see canonical quantisation first)
There's 3 good Zee books, GR, groups, QFT, loads of good stuff in there - it's never complete but what source is, Griffiths aims to give a rounded course in what it does compared to Zee but at a more basic level
sorry, what was that last bit?
ah, I was talking specifically about the tone (kinda?)
but ok
17:01
@ACuriousMind If you're into fast paced books that are pretty straightforward but entertaining, I would recommend checking out Cradle by Will Wight. I wasn't sure if I would like them going in but I got really addicted by like the middle of book 1. It's not like a literary masterpiece or anything, but a lot of people find it super addictive.
Skimming Zee and Tong they at least vaguely sync up on this
@JMac I don't really know what I'm into these days, I just know that many of the common plots and twists have started to bore me because I've seen them so often, so I'm mostly looking for stuff that's...unusual? I'm currently reading the Murderbot diaries by Martha Wells and liking it pretty well
I've read all the Murderbot novellas and loved them all, though some of the novelty wears off in the later ones.
I just loved the character of Murderbot.
And being novellas they only require an hour or two of your time.
@ACuriousMind I've read a lot of twisty series lately, and I think I was kinda burnt out on it too. I enjoy it, but like there's only so many in a row worth reading until it gets a bit much. Cradle isn't really one of those plot twist stories either. It's basically a Western take on Chinese "cultivation" novels, so it's not really a surprise that the MC constantly getting magnitudes more powerful basically and has crazy luck and stuff.
Also I've heard Murderbot Diaries is good, I might have to check that out.
Are they the ones on her website, marthawells.com?
what is this sorcery [EDIT: oops, I switched the () and [])
@JohnRennie most relatable inhuman killer machine I've ever encountered and its disinterest in the world at large keeps reminding me of that Pratchett quote that the one true hallmark of human intelligence is that we've managed to invent boredom in a world full of wonders.
With so many books having been written about AIs turning murderous I thought it was a marvellous plot device to have an AI that thought killing humans generally wasn't worth the effort.
17:30
Do you know how complicated it would be to train an AI to kill humans
The robots would just end up shooting trees or stop signs
That's why the robots who run the internet give us captchas. They are slowly compiling information on how to tell the difference between stop signs, trees, and other non-target objects.
At least I get the first three rounds of captcha wrong (no need to thank me)
Oh snap it's starting to snow kinda hard. Time for the annual round of "whoops no one in the city has winter tires yet".
123
123
18:12
Hi All
18:27
yo whats up
 
2 hours later…
20:02
The decay of a particle of mass $m$ into two particles of the same mass $m$ is kinematically forbidden by momentum conservation. However, in QFT 3-pt scattering amplitudes of identical massive on-shell particles can be different from zero. A trivial example is the theory of a massive scalar field $\phi$ $-1/2(\partial\phi)^2 -1/2 m^2 \phi^2 + \lambda \phi^3$. Here, the 3-pt amplitude is proportional to the parameter $\lambda$. What is the physical meaning of the non-vanishing amplitude?
At least one of the states involved in the scattering is a negative-energy state
20:43
Yes $\phi^3$ is a bad bad theory
Basically you have the vacuum splitting into particles of positive and negative energy
The so called vacuum radiation
This is generic of theories with no lower bound to their Hamiltonian
mmhh....
It's fairly easy to see from the classical theory if you just plot the potential energy wrt the field value
sure, I understand this. But still don't understand the physical meaning of such non-vanishing amplitude
(if any)
It means the process can still happen?
I don't know too much about $\phi^3$, the theory may not be well-formed at all, but if it is, it means such processes can happen.
ok
thanks
 
1 hour later…
22:13
2
A: Why does the $\phi$-cubed theory have no ground state?

QmechanicIn quantum theory we usually require that the Hamiltonian $H$ is bounded from below and that the system has a ground state. This is intimately related to unitarity. The $\phi^3$ theory violates this.


« first day (3652 days earlier)      last day (1574 days later) »