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00:29
it's not really surprising that the mass distribution within the galaxy changes the rotation velocity within the galaxy, no?
compute the angular velocity for a circular orbit as a function of the radius $r$ for a point mass $M$, and for a uniform mass distribution $\rho$
 
1 hour later…
01:39
Ok will try that, it just confused me because I saw the curve resembling the positive side of sqrt(x)
which to me seems weird since i'd expect the center of the galaxy to be the fastest spinning
 
3 hours later…
04:31
0
Q: Suggestion for Review Queue

RC_23Suggestion for the site designer is when being asked to review a First Answer (say), both the question and answer should be displayed by default, instead of the answer only. Most answers don't make much sense without the context given by the question, and the reviewer has to dig for it.

 
2 hours later…
06:04
@RonaldVilliers The key point is that a lot of the dark matter is outside the visible matter i.e. the visible matter is embedded inside a much larger disk of dark matter.
 
3 hours later…
09:15
@ACuriousMind Could it also be that condensed matter groups are typically larger, and condensed matter physicists just ask questions within their group
Well a lot of people on PSE are students though
@B.Brekke I don't think most questions here get asked by people who are "in a group"
even most of the hep-th questions are the typical questions students taking a course or reading a textbook have, not the questions hep-th researchers have
if your explanation was correct, we should see proportionate amounts of hep-th and cond-mat questions at "low" levels, and then a drop-off as the cond-mat people join a group and stop asking while the hep-th people continue :P
Yes, that is a good point
 
5 hours later…
14:28
what do "Conformally flat metrics" mean?
 
1 hour later…
15:48
Why is the sum of the voltages of the capacitors in series equal to the voltage of the battery?
My background knowledge is only up to electric potential and capacitors.
I know nothing about Kirchhoff or above.
The one thing I only know is charge quantity is same on all the capacitors in series.
15:59
@MethNoob suppose you start at the minus terminal of a battery. For convenience, call that 0 volts. Then the potential at the positive terminal will be the battery voltage.
As you move around the loop, you’ll pass across each capacitor in series. For each, there willl be a voltage drop
And once you reach the end, you’ll be back at the minus terminal of the battery. But then you know what the potential is, ie, it’s just zero
So the voltage rise from the battery must equal the voltage drops from the capacitors
I will try to sketch and think about it.
So set negative terminal of battery as 0V and positive as NV where N is real number.
@ACuriousMind sanity check: suppose a phase space function is not classically conserved w/r/t the Hamiltonian. If we quantize this, then we know at least that this observable won’t commute with the Hamiltonian, regardless of the quantization?
So moving from positive to negative terminal voltage drops.
Why?
Right.
Because that’s what the battery does
Is it because potential energy changes because the charges moves?
16:09
You can look up details on how batteries work (huzzah chemistry)
Well, you can certainly say this: if you move a positive test charge from the positive terminal to the negative terminal, it’s potential energy will have decreased
Yeah I was thinking this.
The details behind why the PE is higher at one terminal than another is a matter of chemistry
For the purpose of the loop rule we just take it as a given that there exist such a thing as batteries which generate gains in electric potential energy
@ ACM or to put it differently: if an observable commutes with the Hamiltonian in QM, then it must be conserved classically
(But not necessarily vice verse b/c of Groenwald)
Potential is 0 on negative and N V on positive terminal. Potential difference is NV. "So the voltage rise from the battery must equal the voltage drops from the capacitors" is little bit confusing.
Well, think of just a single loop with a battery and a capacitor
Yes makes little sense.
16:17
Then the change in voltage from the positive terminal to the negative terminal can be found in two ways: either you go back across the battery, or you go across the capacitor
Both ways should give the same answer, b/c electric potential only cares about where you are not how you get there
This discussion only makes sense once the capacitor is in equilibrium with the battery, tho
Ie once the capacitor has stopped charging
Before that, we have to include the resistance of the wire if the story is to hang together
I think I understand it now a bit may be I need to contemplate it for a bit thanks for help I will try to reread it again and think more carefully
Kk
Tbh once you do circuits you get into the habit of just treating the loop rule as a mathematical tool rather than think about why it holds
Just write the loop rule and trust that it works…which is not really the best mindset :P
16:53
@Semiclassical No :) You could theoretically get unlucky that the exact value of $\hbar$ is such that the quantum corrections exactly cancel the classical PB
but that's vanishingly unlikely, so I'd take it as true for all practical purposes (and in particular it's true if you view $\hbar$ as some sort of formal variable instead of a mere constant)
 
4 hours later…
20:27
@Bohemianrelativist Conformally equivalent to flat space
So $g = e^{f} \eta$
 
2 hours later…
22:16
Hi
22:56
@ACuriousMind lol, true. But no non-conspiratorial way of doing it :P
I say conspiratorial, but I could see a scenario where you handle some things classically and not others, and thereby end up with hbar-dependent parameters in the classical Hamiltonian
In which case that scenario is a bit more plausible
yes
I think one scenario in which you get this is if you have an "anomaly" where some classical symmetry gets naively quantized to something with non-vanishing commutator and then you try to "correct" the symmetry so it becomes a quantum symmetry again
i.e. you might have some $f$ with vanishing Poisson bracket but non-vanishing Moyal bracket with the Hamiltonian and then you try to find a "simple" correction $g$ for $f + g(\hbar,p,q)$ such that the commutator/Moyal bracket vanishes
23:48
Sounds right

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