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12:05
does "particles in the same state" mean that the particles are having the same position and velocity?
In a system consisting of independent molecules (PE = 0), if two molecules are having different position but same velocity(hence, the same energy), they are still in different states, right?
and the degeneracy of that energy state is 2 (in case only those two states were allowed)?
same state usually means same energy
degeneracy would be two because there are 2 particles in with the same energy (in the same state)
what if an energy level has a degeneracy of n? The different states which belong to the same energy level are truly different, right?
if they were perfectly identical, then we could have grouped them into single state and claim that the degeneracy is 1
degeneracy is a count of the number of particles in the same state.
@Yashas If they're degenerate, yes; if the states are coalescing (which is a niche bit of a niche bit of physics), no
Why does my textbook use this to represent different energy levels:
(3,3)
(2, 1) (2, 1) <--- same energy
(2, 2)
(2, 1) and (1, 2) are different states, right?
Anonymous
12:12
Well, the context is very important here. From what I can see, they mean (1,2) and (2,1) are equivalent macrostates
I think so because in the context where I am reading it from, the numbers are numbers representing different translational states in one dimension. So 2, 1 is like 2 units in X, and 1 unit in Y and 1, 2 is 1 unit in X and 2 units in Y. That would mean velocity of the two states of the particle are different.
@Phase you said something about SR 3 and 4
Oh right
Saints Row
Anonymous
@Yashas I'm totally confused what you're talking about now. Upload a picture of your textbook's page :P
Anonymous
Where does translation even come from...
12:13
I am deal with a particle in a plane
In a 3 dimensional box?
If so then you have degeneracy
2D plane
Yeah but is there a third dimension for potential
they are independent particles
so V is taken as 0
So they're free particles...?
12:15
yea
Anonymous
Doesn't make any sense even then. I don't know how you jumped from stat mech to translation of particles in a plane all of a sudden
I need to write down the partition function for it :/
so I had to first make a list of states and ....
and then I got a doubt about the definition of state
Anonymous
Write down the full question. Only then can someone help you...
Anonymous
If you're talking about the canonical partition function you need to sum over all the energy states and take into account all degeneracy.
Anonymous
$Z=\sum_{\text{states i}} e^{-\beta E_i}$
12:20
I have N free particles in a plane of size LxL. I need to find the partition function for it.
I took N as 2 (even though it is a bad thing to do as it breaks approximations but idc)
I just realized that taking N as 2 doesn't affect my answer.
nvm screw it
Anonymous
@Yashas Sure, that's a property of the partition function being an exponential function
Say I am dealing with a particle in a box
I can compute the wavefunction and get a list of energy levels
the expression for energy turns out to be E = (n^2 + m^2 + l^2) * (some constant)
where n, m, l are quantum numbers for each direction
Anonymous
Dude. You're doing statistical mechanics. Not quantum mechanics.
Anonymous
No need of wavefunctions here
but I need the QM stuff to write partition function --,-
Anonymous
12:25
No.
some basics was taught in one class
how do I even figure out the energy levels without some QM stuff?
Anonymous
In physics, a partition function describes the statistical properties of a system in thermodynamic equilibrium. Partition functions are functions of the thermodynamic state variables, such as the temperature and volume. Most of the aggregate thermodynamic variables of the system, such as the total energy, free energy, entropy, and pressure, can be expressed in terms of the partition function or its derivatives. Each partition function is constructed to represent a particular statistical ensemble (which, in turn, corresponds to a particular free energy). The most common statistical ensembles have...
anyway if I have two states (2, 2, 1) and (2, 1, 2), they are different right?
Anonymous
You don't need any QM stuff here
Anonymous
I really recommend learning SM properly first
Anonymous
12:27
You are confusing lot of stuff now
Don't I need the energies of the states to write the partition function?
If I was given the energies, it would be easy work.
Anonymous
@Yashas They are the same macrostate
Anonymous
Different microstates
ok
so two different velocities = two different microstates?
if the velocity differs only in direction, even then they are two different microstates? but the same macrostate?
Anonymous
$v_x=1$ and $v_y=2$, and $v_x=2$ and $v_y=1$ are equivalent microstates
Anonymous
12:30
Same macrostate
what if the particles are free particles and their positions are different but their velocities are the same, even then in my context, they are taken to be the same microstate, right?
if the particles were interacting, then different positions with same velocity would be different microstates, right?
Anonymous
@Yashas Right. Here, position doesn't matter
Anonymous
Only momenta matters
Anonymous
Use $E=p^2/2m$
Anonymous
12:32
and integrate over all the states
Anonymous
@Yashas No. You haven't understood statistical mechanics
Anonymous
Please watch Balakrishnan's lectures (first 6-7)
Anonymous
For stat mech
Anonymous
You are saying strange things. It's impossible to address so many misconceptions over chat
12:35
if the particle's position matters for its energy (becaz it is interacting), then different positions can give different potential energy and say if they had the same velocity, the energy of that whatever state would be different (becaz T is same but V changed and hence E changed)?
Anonymous
Suppose in a system consisting of a gas, it doesn't matter where individual gas molecules are for finding the partition function
Anonymous
@Yashas Noooooo.....potential interations are ignored in stat mech!!!!
@Blue I was just asking in general
Anonymous
....
Anonymous
The problem is a stat mech problem
12:36
if the energies are different, then they have to be in different microstates?
@Blue but I'm too curious :(
well, I know what to write on paper to get full marks for that question but I need to understand what actually is happening :/
Anonymous
It's impossible to take into account potential interactions for so many particle systems. N-body problems are still research problems.
Anonymous
@Yashas If you want to learn about N-particle systems, first you need to learn QM properly
Anonymous
We can learn it together after your exams are over :)
Anonymous
In fact my next year's summer project will probably be based on that
13:12
My textbook says "there is a configuration with so great a weight that it overwhelms all the rest in importance to such an extent that the system will almost always be found in it"
is the most probable configuration really has way more arrangements than the 2nd most probable configuration?
to such an extent that the 2nd probable configuration is extremely rare
Anonymous
Yes, greater the number number of particles, lesser will be the standard deviation (variance) from the most probable distribution of energy.
do u have a nice pictorial representation of that fact?
Anonymous
@Yashas Yuck. "there is a configuration with so great a weight"!!!
I am too curious to see how much the two configurations differ for different values of N
Anonymous
What book are you using...
Anonymous
13:15
@Yashas It's given in any BSc physics book. You can check Reif
Oxford: Atkins' Physical Chemistry, Peter Atkins | Julio de Paula
Anonymous
Duh. You're reading from a Chemistry book. :'D
Anonymous
It's given here: books.google.co.in/…
Anonymous
But you need to search for it
It's a much more general statistical property that the standard deviation from the expected value decreases if the data is sufficiently large.
Also known as "law of large numbers"
There are also statements about how well the standard deviation estimates the general fluctuations of the data from the expected value - if you're normally distributed, with probability close to 70% a random data point will lie inside $[\mu - \sigma, \mu + \sigma]$
Anonymous
13:32
@BalarkaSen Nice! I didn't know that exact value
Anonymous
I need to learn some statistics...
Anonymous
Never had a formal statistics course in school
In fact if you look at a slightly larger interval $[\mu - 3\sigma, \mu + 3\sigma]$ the probability jumps to 0.997
That's pretty damn close to 1
Anonymous
Cool
Anonymous
I heard something similar about the birthday problem too
13:34
Oh yeah that's a different phenomenon, but surprising nonetheless
Anonymous
It was something like even if you have a 200 students in a class, the probability that two of them have the same birthday is like >90% or something (don't remember the exact value)
Anonymous
@BalarkaSen Yup
The experiment of determining whether 23 persons in a room have at least 2 persons with equal birthdays is probabilistically the same experiment as tossing a coin
i.e., the answer "yes" to the first question has probability 1/2
@Blue 200 is not a surprising number, because there are already 365 days in a year
If you have 365 students the probability is... 1
Anonymous
@BalarkaSen I think it was less...I don't remember
That it's already 1/2 when you have 23 students is damn surprising
Anonymous
13:37
@BalarkaSen Uh, really? 365 students could have 365 different birthdays. It's not exactly 1 for sure
Sid
Sid
@Blue make that 366. Happy? :P
Anonymous
(Assuming 365 days in a year)
I meant 366
Anonymous
@Sid Yup :D
Thanks @Sid
13:38
@BalarkaSen Pigeon hole principle :D
stop fighting over the leap year :P
Anonymous
We didn't even start...
@user685252 We are not fighting over the leap year... Your joke is moot bro
@Blue But yeah you should definitely learn some statistics at some point. I really like it.
It's quite surprising to see how small-scale randomness collectively cancel out to show large-scale regularity
Anonymous
13:42
@BalarkaSen Keep it in your teaching bucket list then. :) Lots of cool things up in the planner. How are your PDE/ODE reading sessions going with the ISI prof?
I'd hardly be qualified to teach you; what's in my school syllabus is relatively basic things. I myself want to learn it thoroughly at one point.
@blue can you give the definitions for microstate, macrostate, arrangement, distribution of energy?
We meet next month
@BalarkaSen one on one?
Anonymous
Sure. I wish these damned exams get over fast. I need to learn the random variables transformations and the Gaussian, Poisson stuff. Also measure theory (slowed down with it a bit)
Anonymous
13:45
Oh, btw I got the Shakarchi Stein books today morning
I should learn measure theory someday
Nice!
Anonymous
They seem to be really nice small books (and have good typography)
Anonymous
:)
Oh you bought all three?
Anonymous
@BalarkaSen Yeah, except the functional analysis one. I'm using Kreysig for that
Anonymous
13:46
It was on sale
Got it
The Fourier analysis book looks real nice
Anonymous
And I got a few bucks as gift from one of my uncles, sooo...that was the best way to spend it
Anonymous
:D
Anonymous
@BalarkaSen Strangely it comes before real analysis
Anonymous
In that series
13:47
Indeed.
Anonymous
And the real analysis book has measure theory and hilbert spaces stuff
S-S's approach to analysis is interesting
I think complex analysis also comes before real analysis
Anonymous
Yup
Anonymous
that too
Anonymous
hehe
13:48
They approach analysis through a Fourier analytic point of view
Anonymous
I think that's the author's area of research: harmonic functions and Fourier analysis...that's why
Anonymous
(From what I read somewhere)
I think it's a refreshing POV
Anonymous
mhm
Anonymous
@Yashas It will get too long, man. I'm a bit busy today
13:50
Real analysis is way harder than complex analysis
Anonymous
@BalarkaSen Most people say the opposite :P
Really? I have never seen anyone disagree.
Complex analysis is super rigid.
I guess what you could say is that multivariable complex analysis is harder, because it is.
But 1 variable complex analysis is really really nice and easy
Anonymous
Yeah, I guess they meant multivariable complex analysis
There are not many complex analytic functions. Everything's either a polynomial, or grows exponentially or more
Anonymous
I actually don't know much of either. So I shouldn't comment based on hearsay :P
Anonymous
13:54
@BalarkaSen I see
Sid
Sid
Today is a sad day...
good evening to you all
14:12
toppata morning
14:28
@BalarkaSen oh hey there jack spedicy
14:51
0
Q: Quantum Field Theory - Representation Theory (of the Lorentz Group)

user176549I am now in the middle of a one-year-course in QFT. I have one major problem, which somebody else also had and already asked in the forums (Lorentz group representations for QFT with mathematical language), but sadly it was left unanswered. I am also familiar with Representation theory for finite...

Close as duplicate?
@BalarkaSen I disagree.
Understanding the logarithm involves more conceptual hurdles than anything in real analysis.
15:12
@0celo7 ? The logarithm is very easy to understand.
One only needs to realize $e^z$ is a periodic function in the complex land
I am going to try to understand two quantum mechanics topics on here at about 1:30 pm pacific time. I encourage most of you to be here then so I can bounce thoughts back and forth. For the level of rigor please look thought the chat conversations I had with @Secret on the math chat last night. I am hoping to continue the conversation in that room.
15:39
Damn Squarepusher is pretty good
some trippy shit
16:14
Hey
I've been thinking about entropy being about energy/mass/disorder/complexity/density/heat.
Anonymous
@JohnRennie Excuses to drink more coffee ;)
Anonymous
Actually that looks like an interesting read
@Blue I'll live to be 200 years old with the amount of coffee I drink :-)
Anonymous
16:20
Nice. The world really needs you (for javascript advice, dirty jokes and physics). Keep drinking! :P
@JohnRennie do Mocha's count or does that tip the scale towards diabeetus
And that many lifelike and generations cellular automata, for example "Conways Life" or even more apparently in the "Star Wars" rule, starting in a bound universe with a random distribution of cells, have an entropy like behaviour where they tend towards cyclic behaviour, or in the infinite case any region tends towards purely cyclic behaviour, and complexity has to come in from outside but gradually dies away.
Also, yes coffee rocks :)
@Phase no idea - drink them anyway! :-)
@JohnRennie tryna get me killed smh
@JohnRennie What about tea?
16:31
That causes premature death and genital stunting in males.
@JohnRennie No, no, I'm not talking about your eating and drinking habits - I mean a good cup of hot water infused with tea leaves :)
genital stunting
Is that when your wedding tackle does a sick wheelie over a ramp
also to the above, blobs of matter preserve "entropy" better than disperse stuff, again like real entropy
uhhhh
16:40
@Phase please don't post the video on YouTube :-)
it has already been done before
@JohnRennie what else am I supposed to do with these hot wheels?
16:55
ohai
what's poppin

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