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Anonymous
17:00
@0celo7 Alright, thanks. I'm reading a bit more about this thing :)
so the change that comes in can do so in a lot of different ways, but once it goes through a coin machine one just has some number of each kind of coin
So it emits it in a different way
it's not that it emits it in a different way. it's still EM radiation
it's that, once the energy has been stored in the system, it only comes out in specific packets
(if anyone wants to chime in on me not explaining this well, please do)
And this packets are the distribution of the frequencies
eh, these packets are the photons themselves
17:02
@Blue study the differentiability of x^2 sin(1/x). Compute the derivative. Is it continuous?
What is the “tangent line” at zero?
the distribution is how often photons of one quantized energy are emitted versus photons of a different quantized energy
Do this and you’ll understand what I’m saying.
Yeah I meant them. The packets and the photons and each one has a frequency and the graph changes based on them
something like that
what gets a bit tricky here is that the blackbody distribution requires a few different parts of physics
I think I have to wash my water bottle. I feel slightly nauseous after drinking from it.
17:04
on the one hand it involves EM radiation, so photons of a given frequency carrying energy
So the black body absorbs all the energy but it emits it in packets
Which are the initial energy if I sum them
I'd say that's closer to it, yeah. (I hesitate to call it completely right, because I'm not remembering the details quite right)
@Curio in the sense that the amount of energy it emits via radiation in 1 second is the same as the amount of energy it absorbs in that same second
it's about the rates of energy absorption and energy emission being balanced
getting back to a moment to what I was saying: On one hand, blackbody radiation clearly involves EM waves and therefore the speed of light
@Blue @BalarkaSen India is on the top of r/WTF!!
but it also invokes some thermodynamics/statistical mechanics assumptions
I don't really want to get into that. But it's why Boltzmann's constant k showed up in an earlier statement.
Is the spectrum of the black body complete?
17:09
@Curio what do you mean by complete?
And finally it does involve some assumptions vis a vis quantum theory, namely that the blackbody radiator can be modeled as a set of oscillators with quantized energy levels
as in, does it emit at every real frequency?
Anonymous
@0celo7 What ?
All the visible radiations
I'm not really understanding the question either.
17:10
@Blue A bunch of Indians going 70+ in thick smog and creating a huge traffic accident
And then 15 people get out of a 7 person car
It’s amazing
Anonymous
LOL
Anonymous
That's typical
Anonymous
You should see the trains here
I mean, like the rainbow
I feel like your question is more about EM radiation than the blackbody
17:11
@Curio then yes
It’s hilarious. Visibility is 10 feet and people don’t slow down.
If you're asking "does every color we see in nature correspond to light of some frequency?" then yes
Anonymous
@0celo7 Okay, so that is differentiable at $0$ but the derivative is not continuous
I wasn't asking this, but, does a blackbody emit a continue spectrum
Yah. So the tangent line at 0 doesn’t make much sense.
17:13
That's a bit more subtle, I think
on the one hand, the individual photons emitted from a blackbody should indeed be quantized
however, when you're looking at radiation intensity
The black body absorbs all the radiations but it emits the total energy in packets. Are these ones correspond to all the frequencies?
you're not looking at just one photon
you're looking at a whole bunch of photons which are striking your detector at nearly the same time
going back to the change analogy: if someone dumps a whole bunch of change in my lap, there's a lot of possible totals for that
and when you're talking radiation intensity, you're talking about a looooot of photons
@Semiclassical photons don't have to have a well-defined frequency
you're right, and I wondered if I wasn't saying that carefully enough
x photons of a frequency, y photons of b frequency
17:20
@Curio no, that's not quite right, though
the quantization is really for the 'oscillators' inside the blackbody
@EmilioPisanty hmm, this takes us back to the what is a particle question. If we take the photon to be the limiting case of a Fock state then by definition it has a precise frequency.
lol
prooobably should avoid invoking second quantization language in this context :P
@JohnRennie that's an extremely narrow view of what single-particle states are
Oscillator?
17:21
In that view, the superposition of "one particle over here" plus "one particle over there" no longer has single-particle character
@EmilioPisanty it's one end of a spectrum, and the existence of the issue is why I think a canonical question on the topic would be very interesting.
@JohnRennie maybe
but I would argue that that view is out-and-out wrong
@EmilioPisanty but we've said that these packets contain different energy so the photons should have different frequencies.
@Curio fyi, probably should not get too distracted by the other conversation going on here. it's relevant, but higher level than what you're talking about and more likely to be confusing
Anonymous
@0celo7 Hmm. Take $f(x,y)=x^2\sin(1/x)$ and $f(0,0)=0$. Even though the derivative is not continuous the tangent plane $z=0$ is still the best linear approximation as the limit $\lim_{(h,k)\to(0,0)}\frac{f(h,k)-f(0,0)-\mathbf{A}(h,k)}{\sqrt{h^2+k^2}}$ evaluates to $0$. Also, similarly it can be shown that the line $y=0$ is the best linear approximation for $x^2\sin(1/x)$. Could you give me an example where the limit turns out to be non-zero but still the function is differentiable?
17:23
a superposition of two Fock states with single-particle character (but different frequencies) should still be a single-particle state
otherwise, there are no physically-available states with well-defined particle number
@Semiclassical we've said that these packets contain different energy so the photons should have different frequencies. Is it right?
@curio in particular, anything regarding "Fock states" should be taken as outside of what you're going to learn about any time soon
@Curio continuous spectra are just more tricky to handle
even without quantum mechanics
here's the picture I'd give, though it's probably not entirely right either
you can't just say "oh, I have five joules at 500nm"
17:25
the blackbody absorbs radiation at any frequency and stores it internally
@Semiclassical @curio I'll second this statement
however, it stores it in the following way: n1 number of photons at energy level E1, n2 number of photons at energy level E2, and so forth
And then it emits E1, E2,...
I should probably not insist on saying that it's n1 photons stored at a given energy level; that's a bit too narrow
but the blackbody has some way of storing the energy in such a way that there's only integer numbers of various energies allowed
so it contains some number of 'energy quanta'
(think of it like a bank choosing to store what it knows about its revenue electronically---it's the same info, just transcribed in a certain way)
the blackbody can then give up one unit of that stored energy as radiation
@Semiclassical that's true; the mode at frequency $f$ can only have energy $E=nhf$ equal to an integer multiple of $hf$. But it is allowed to have a probability distribution over $n$
17:29
Right. That's where the statistical mechanics comes in, and more precisely the role of temperature
buuuut that's a harder conversation
@Semiclassical I'm not quite sure how one can talk about blackbody spectra without talking about thermodynamics, but OK.
Is all the stored energy emitted?
@EmilioPisanty for the purposes of a derivation of the Planck distribution, I entirely agree.
for an elementary discussion of how the Planck distribution arises, though...eh
There's a lot of physics which converges at the same time in the blackbody problem
quantum, thermo, and EM
@Curio if it's going to remain in thermal equillibrium, the blackbody had better give up energy at the same rate as it absorbs it
talking more specifically about the 'timing' of that process is not simple to do, I think
and it's really not necessary, since the radiation intensity we observe is going to be measured over some particular range of time
So it doesn't emit all the energy it absorbs
"if it's going to remain in thermal equillibrium, it had better give up energy at the same rate as it absorbs it"
in that particular sense, it does emit all the energy it absorbs.
17:36
I meant, not all in one time
ah
that's pretty much right, then. it emits as much energy in one second as it absorbed in that same second
that's a statistical statement, though. in one second it emits and absorbs a lot of photons
(I'm not actually sure how many photons a blackbody would radiate per second.)
Can it emit all the frequencies?
As individual photons, I'd say no.
I mean, radiations with all the frequencies
It can emit photons of energy $h\nu$, $2h\nu$, etc.
however, we're again talking about a huge number of photons
17:39
@Blue what is $A(h,k)$?
So not all the frequencies because the energy is quantized
in which case it's a bit like asking whether, if we've got a trillion pennies, we can represent any amount of money between 0 and 10 billiion
@Semiclassical that's incorrect
is it? I was worried I was wrong on that.
@Curio yes, it can emit radiation at all positive frequencies
Anonymous
17:40
@0celo7 $A:\Bbb R^2\to \Bbb R$, given by $A(h,k) = [\frac{\partial f}{\partial x} \space \frac{\partial f}{\partial y}][h \space k]^T$
@Semiclassical it can emit energies $h\nu$, $2h\nu$, etc., at each frequency $\nu$.
durrrr
yes
So the spectrum is continue
Like stars' spectrum
Anonymous
For that choice of $A$ the limit can never be non-zero. It can either be $0$ or not exist at all (think so)
17:42
@Curio yes
@EmilioPisanty something doesn't sound right here, come to think of it. emit those energies as what?
is the dimension of the kernel just the amount of orthonormal basis vectors required to describe all the vectors in the preimage set that map to the zero vector?
i.e. if the Kernel is just zero, then it's zero dimensional?
@Semiclassical as electromagnetic radiation at frequency $\nu$
hmm
I guess you're not wanting me to use the word photon for that
the different outcomes $0h\nu$, $h\nu$, $2h\nu$, etc, occur with different probabilities
you're essentially looking at the counting statistics of that mode
17:44
So does it absorb radiations of all frequencies?
(once it's been monochromatized)
@Curio yes
@0celo7 OK, I will
If it didn't absorb radiation of all frequencies it wouldn't be a black body :^)
@0celo7 lmaooo
17:44
It might be a Pea-green body, maybe clementine-orange
#proudtobeanIndian
that it absorbs at all frequencies is a definition
@Phase So you figured out dual space schtick?
@Semiclassical what did you mean so?
pretty much what I said.
it can only store the radiation energy it absorbs in certain quantized energy levels
17:47
@BalarkaSen think so
I came to a conclusion about inner products
that seemed to be right
@EmilioPisanty I feel like we're using terminology differently (which means I'm probably remembering stuff wrong)
And the radiations of frequency which it can't store go away immediately
Doh
for it to be a blackbody it needs to be able to interact with all positive frequencies
there are no "frequencies which it can't store"
17:49
So it stores all
@BalarkaSen it seems to have been deleted
@BalarkaSen is the dimension of the kernel just the amount of orthonormal basis vectors required to describe all the vectors in the preimage set that map to the zero vector?
i.e. if the Kernel is just zero, then it's zero dimensional?
@Curio it absorbs, stores and emits at all positive frequencies
if it is an ideal blackbody
real black bodies are only approximations so they might have gaps
Are there negative ones?
17:51
not for these purposes
No
@Blue I don't know why you're computing that thing. If it has to do with linear approximations, I'd just recommend ignoring them. They never show up in practice.
At least that expression never shows up.
in this case frequency is just a scalar that measures the periodicity of the emitted light
rather than any direction
@0celo7 Uh, this is wrong dude.
So it's fine in the positive numbers
17:52
@BalarkaSen ??
the gradient would be zero if the derivative is continuous
at least that's what he said
too many conversation threads at once
So it continually absorbs and emits
Anonymous
@0celo7 Which thing?
there's a video of the actual crash but I can't find it
$f$ is differentiable at $a$ iff there is a linear transformation $A$ such that $\lim_{h \to 0} (f(a + h) - f(a) - Ah)/\|h\|$ is zero.
17:53
I thought he was doing a difference quotient.
Ah, no, that's not what he's doing
You can't do difference quotients for non-C^1 things
He's just writing the defn of derivative
aka what i said
Yeah but he's doing it with partial derivatives.
Which is wrong in the non-C^1 case
Do all matrices with Linearly independent columns have nullity zero, and thus are surjective?
17:55
Let's consider the graph again. If it is at 5000K it stores x energy and it emits y and it absorbs y.
@0celo7 I agree.
Anonymous
Uh. I would just use the limit definition of $\partial f_x$
Anonymous
Would that be wrong?
Have you checked if your function has continuous partial derivatives?
If it is at 10000K it stores 2x energy and it emits 2y and absorbs 2y
17:57
You need to check that before plugging in $A = [f_x, f_y]$
@Blue You can't calculate a Frechet derivative using partials unless they are continuous functions.
You're getting a strange result because you're assuming it's continuous, I think.
@0celo7 I'll have a look after I finish dinner
!?
@Phase Dimension of kernel is equal to the dimension of the null space is equal to the dimension of a basis of the null space, yes.
Anonymous
17:58
@BalarkaSen Oh, and what's the reason for that? I forgot :/
@Curio why would you think that?
for one, is that per-frequency, or integrated over the spectrum?
Doesn't need to be orthonormal (which doesn't make sense if you don't have a inner product beforehand)
@Phase Wait, no.
@Blue Because it's not true otherwise?
I'm confused by this whole notion of a basis without an inner product
You need continuity for the estimates to work.
17:59
How would you even know what basis to choose
Anonymous
@0celo7 Oh, got it

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