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02:49
@ChrisWhite It's almost midnight and GMP decided everything is a pointer
Halp
03:05
<3
@DanielSank Hey!
The probability line worked btw, she didn't double check my calculations :)
Nice.
Actually, I'm disappointed. This woman clearly isn't taking the calculation seriously enough.
Exactly what I was about to say! I'm still deliberating whether or not she not double checking is a good or a bad thing
Did you hear the news about Brazil?
No, what happened?
Well apparently our congress thinks impeachment is a recursive function
because earlier today we impeached the impeachment
03:10
heheh
and a few hours ago we seem to have impeached the impeachment's impeachment
So I don't even know what's happening anymore :p
I see.
Well, you could all just eat peaches...
Peaches are delicious.
Oh god
impeachment ~> peaches, what an amazing mind :p
What? The word is literally written in the middle. Impeachment.
Now that you mentioned impeachment kind of sounds like what you'd call stuffing someone with peaches
03:13
@BernardMeurer Yep.
I was going to say you could purchase some peaches and impeach yourself.
"Yeah he got totally impeached at the eating contest"
Do they grow peaches down there?
Good question, I think a few down south
but mostly it's imported for sure
@BernardMeurer Oh then don't bother.
@DanielSank hello!
03:15
@TanMath Hello.
@DanielSank Recently I've been stuffing myself with lemons
Did you get my email from like a month ago?
and oranges
Oh god
@TanMath Uhhh, not sure.
nvm, 2 months ago..
@DanielSank which email do you use? the gmail one or the google one?
03:17
@TanMath I got a note from you but it didn't actually ask any particular question so I figured I'd just wait until you asked something specific.
@DanielSank ok... I was awaiting your reply...
@DanielSank I did ask about Prof. Mohseni's email...
@DanielSank I want to buy a plant as my new pet. It has to be small to fit in my window, any ideas?
Anyway, I recently got an answer to my question on stack overflow (maybe 2 weeks old...)
@TanMath I'm going to ignore anything you email me or say to me here unless you ask a specific, well posed question. I am not interested in further general discussions.
We've been through that, over and over. I'm surprised you're still approaching things in the same way.
@BernardMeurer Get a cactus or a wandering jew.
@TanMath I will not give you anyone's email. Stop asking for it.
@DanielSank Cactus is a good one! Low maintenance, I like that
03:21
@BernardMeurer Yep. They're very easy.
If I could I'd grow edelweiss
but I don't think that's doable
Never heard of it.
It's my favorite flower
@DanielSank I was going to say that it seems that somebody else agrees with me that the programming is not the problem so I kinda wanted to go over whether I am using the right values since the natural units are confusing me...
I will send it as an email...
@TanMath Did you adhere to PEP-8?
03:28
@TanMath Listen to me please. Post your question here on the site.
@DanielSank Think I got my cactus of choice de.wikipedia.org/wiki/Echinopsis_chamaecereus
@BernardMeurer Nice.
@DanielSank Well I'm off to bed now Dan. Goodnight (and I might pass by SB again this year :))
PS. (When's your birthday?)
 
1 hour later…
04:47
I know the formulas but I am really stuck in the calculus part.
\o
do you know what a derivative is
user116211
@manshu okay, this question!
yup
@user507974 I know the high school calculus
so when its asking as some function varies as a function of another what that is code for in calculus
user116211
This came in AIPMT? I came before it numerous times.... show me your efforts, first ;P
04:51
@user507974 differentiation
do you know what v is?
@user507974 velocity
its functional form?
maybe (mv^2)/2
due to work done
v as a function of x
04:54
ohh...in that way? I don't really know.
hint: what type of force is this
electric force.
so what is the force between two charged spheres
kq^2/r^2
replace r with x in this case
now that gives you force
how can you get velocity from that
04:56
differentiating it.
-2kq^2/x
you sure thats differentiating it (you did the right thing though)
-(2kq^2/x)v
maybe
well almost the right thing, you are proportionally off
thats not differentiating though
differentiating decreases the order your polynomials right
what increases it
integration
yea, what did you integrate to get what
05:00
integrate dx to get get velocity i guess
no no no
let me think
take your time (getting you to think is my goal)
oh damn...I get it now...it was a silly mistake.
-2kq^2/x^3
colder
integrating is the right call
thats differentiating
but think physically, WHAT are you integrating
and WHAT is the result
and WHAT are you integrating with respect to
type out the equation
We are integrating force...so we should get change in momentum...So we should get the change in velocity
well force is the change in momentum (the derivative of it)
05:03
we are integrating w.r.t the distance between the balls.
force is the change in momentum per unit time.
not just change in momentum
(i guess)
yea, so you integrate with respect to tine first
time*
-(kq^2/x)v
ok, maybe lets take a bit of a different approach
ohk..
what is potential energy for coloumb interaction
05:07
-kq^2/x
yea
now from conservation of energy what can you say about the kinetic energy
(mv^2)/2 = kq^2/x
and potential
well more accurately it equals a constant E;
or $E = KE + PE $
that's it.
we got it.
(hint, you have a sign error)
05:09
v is proportional to x^{0.5}
(mv^2)/2 = -kq^2/x
but yea
thats v dependence
what about as v varies
what do you need to do
if v increases then x decreases.
well, with calculus
describe it to me in calculus
OH WAIT
youre good
you have the answer
I was looking at the wording but not the multiple choice
your teacher kinda sucks a bit
05:12
It was in a national level entrance exam...:p
well their wording could be better
when you ask how something varies as a function of something else that implies a derivative, but they were asking for the functional form of v
which you have found yourself
now i want to ask you something
yeah
calculate what happense when you take the derivative of v with respect to x
dv/dx=-1/(2(x^{1.5}))
so when x changes then v decreases even more.
ok, now multiply it by velocity
what is the x dependence
05:17
I get a = 1/(2x^2)
where a is accelaration
yea, the factor of two would actually disappear if you carried out all the terms instead of just looking at proportionality
now in general this relationship between velocity, its derivative, and acceleration is true
So we should get kq^2/x^2 again
right
yea
your hw assignment is to abstractily show why thats the case
you definitely know how to do it
one weird question i want to ask.
what does abstractily mean?
you have $a =$$ v dv\over dx$, show why that works using some simple calculus
so like show without using this specific equation
or show in a way that is more general than just the coloumb problem, a lot of times its easier in a way as long as the ydont demand an explicit answer
so like abstractly speaking $a = dv/dt$
05:22
a=dv/dt
so now show me why abstractly this equation works
multiplying and dividing by dx
we get a= (dv/dx)(dx/dt)
so a=v(dv/dt)
and a little extra credit, what is this property called?
user116211
@manshu ??
idk...I am not even sure if we can multiply and divide in this way.
05:25
@manshu Oh, how did you get that
was that a typo?
by using dx/dt=v
it's change in position w.r.t. time.
@manshu but this does doesnt equal
eh?
ohhh.
yeahhh
this $a=v$$dv \over dx$
a=v(dv/dx)
another silly mistake..
05:27
and its not really multiplication, theres a name for this property you probably learned in your class
you use it all the time when you take the derivative of something like sin(x^2)
user116211
It's a simple trick of operator... and nothing else.
I know it but I forgot the name a minute ago.
@MAFIA36790 well kind of, but its not exactly multiplication and getting that distinction down is important
user116211
@manshu: You can derive it by multiplication.... then you would say you are working with infinitesimals so that in the limit it remains the same.
user116211
@user507974 yeh... know that.
05:29
@manshu chain rule
@user507974 yeahhh..
substitution was stuck in my mind.
But how are we using chain rule in it?
care to take over mafia, gotta get back to research
Thanks a lot.
yw, good luck on your physics journey friend
user116211
$$a= \frac{\mathrm dv}{\mathrm dt}$$
user116211
05:31
Using chain rule:
user116211
$$a= \frac{\mathrm dv}{\mathrm dx}\cdot \frac{\mathrm dx}{\mathrm dt}\;.$$
@MAFIA36790 that's clearly multiply and divide by dx
ohhh
I get it..
user116211
@manshu it's not strictly multiplication... you are working with infinitsimals.
we first find the derivative of v w.r.t x and then using the chain rule we do that dx/dt
right?
user116211
yup.
user116211
05:35
Okay, you can check HC Verma's derivation of SHM..... here he used that. @manshu
checking
I see it.
But it's nowhere given anything like "I, H.C. Verma, is now gonna use chain rule."
user116211
@manshu hahaha...
user116211
It's implied that the physics author would take it for granted that the readers are well versed in calculus.
@MAFIA36790 Yeah...it's given in the preface of the book. "The book presents a calculus-based physics course..."
and later it's given that "Almost no knoledge of physics is prerequisite."
user116211
@manshu hahahaha....
user116211
05:42
Sounds funny but well-written.
True...
ttyl...gotta take bath :p
 
2 hours later…
07:38
Hello
I wonder
what are some quantities that you could calculate for any quantum theory
No matter the formalism and interpretation
I guess cross sections
expectation of observables
and then indirectly probability distributions
Yeah
(at least if you could measure all observables and obtain their expectation value)
07:49
Well, they would be rather poor observables if you couldn't :p
the fact that you could in principle it does not mean you can in practice
But in practice practice
Can you think of an observable you can't measure
$(x^2+(-i\nabla)^{18})^{1/5}$
Wouldn't it, though
or any of its self-adjoint extensions
07:52
18th derivative would just be the 18th moment
Tricky to compute I suppose but not terribly hard in principle
it is not a problem of computing, but of measuring it
Well yes, but then again
with an experimental procedure
You could say the same thing of like
Charge
You don't directly measure charge
maybe; but even if you avoid "dynamical" constants
or quantities
it is already unlikely to measure all "static" observables
07:54
But like
What is "measurement", for you
What would you say a direct measurement of a quantity is
it is a quantum measuring process
of a given observable
yes but in practice
in practice it is the realization of a quantum measuring process
what's a variable you can measure directly and with what procedure
in principle, you can measure every observable with a quantum measuring process
what has been practically done is something you should ask a bloody physicist
07:56
Well my point is
Aren't most methods used for measuring variables somewhat indirect
In the end you mostly measure positions and times
and even then smeared positions
if "indirect" means that you need an interaction between an instrument and the system, and then you read the outcome on the instrument scale, then I agree measurements are indirect
for that is how measurements are performed
in both practice and theory
for all the gory practical details on the apparati I'm not the person to ask
Or Stack Exchange in general, I think :p
Not a lot of experimentalists around
yeah, that's definitely true
think about those poor dudes that have to look at theoretical papers and then they have to imagine an experiment for it
in all likelihood, seen all the theoretical bullshit around, they can pretty much imagine a random experiment
and then find an observable in some theory the experiment is perfect for
I remind you some "brilliant mind" formulated adelic and $p$-adic quantum mechanics
and they were not mathematicians
08:05
I am not surprised
It sounds like some shit I'd try
Just look for a random math framework and try to milk it for some physics
I try that a lot but then I find out that some dude always beat me to it
A lot of physicists are on the prowl for math stuff
physicists should learn some math before trying to use it randomly
Man if I had to learn something before trying to use it
I wouldn't get a lot done!
I wouldn't have a job, certainly
I have no idea what I'm doing at my job
and historically, it has almost always worked the other way around: physicists devise some pseudomathematical tool that mathematicians then turn into something rigorous
Also knowing math that's like 3 years of studies I'd say
Oh yeah it works both ways
Also sometimes in parallel
Like gauge theory
I am getting better at math but it ain't easy
it's never easy
and once you go math you can never go bath
08:15
Never go bath?
Are all mathematicians dirty
maybe not, but rhymed only that way...
and rhyme is thyme
(supposing that it rhymes...)
Any thoughts on why we care about Nilpotent lie algebras and prove Engel's theorem for them?
08:38
@yuggib wth is that thing
like 18th order momentum op or something? what does the 5th root have to do with anything?
It's just an example of a weird observable
^
I think it has no physical meaning whatsoever
I don't think I ever saw any moment over 6th order
and even then that was just the name, not being used
Usually at best you get 4th moment for the jerk
Or the kurtosis, for a statistical distribution
 
1 hour later…
user116211
10:55
Okay, isn't Hamiltonian self-adjoint operator?
user116211
At-least I know so... it has to follow unitarity... isn't it?
user116211
But while googling, I stumbled across this paper cited by over 250:
It is.
user116211
Okay, did I learn wrong?
10:58
Otherwise you will have non-real energies
11:10
@MAFIA36790 self-adjoint and symmetric(hermitian) are not the same
for an operator to have real numerical range it is sufficient that it is symmetric
for it to be the generator of a unitary group of evolution (dynamics) it has to be self-adjoint
user116211
sorry, got offline... @yuggib o/
user116211
@yuggib ooh.
@MAFIA36790 and you should take things said by people that do not know the difference between symmetric and self-adjoint with a grain of salt
and very carefully
user116211
I have @yuggib ;D
11:17
quantum mechanics is not a theory of matrices
with accidentally an infinite number of entries
user116211
@yuggib o.O
it is a wonderful and rich theory with plenty of counterintuitive stuff
that is nevertheless very important
user116211
Thanks @yuggib for the insight o/
user116211
Ah!
user116211
15
Q: Distinguishing between symmetric, Hermitian and self-adjoint operators

Josef K.I am permanently confused about the distinction between Hermitian and self-adjoint operators in an infinite-dimensional space. The preceding statement may even be ill-defined. My confusion is due to consulting Wikipedia, upon which action I have the following notion. Let $H$ be a pre-Hilbert spa...

11:20
it is just that I find the sloppiness of physicists really stupid in this context
user116211
is hermitian different from symmetruc ;(
user116211
investigating
because they often end up overlooking some very relevant features of the theory
user116211
@yuggib ohh.
that distinction between hermitian and symmetric is not used in mathematical physics/analysis
at least as far as I know
simply the word "hermitian" does not appear
ever
11:23
"T is Hermitian if it is symmetric and bounded."
HINT THOUGH
Most operators are bounded in QM
Although I guess momentum wouldn't be hermitian then
@Slereah never read such a definition
that's what the math dude said
apart from the urreferenced math.se answer
What are the definitions you heard
I know the definitions of books like Kato, Yosida, Reed Simon, etc.
11:25
I do recall working with operators that were self-adjoints but not hermitians, though
and they never use the word hermitian
Like the momentum operator in a curved space
$p + \Gamma$ or something
that's the one
$-i\hbar(\partial_a- \frac{1}{2} \Gamma_a)$
12:08
Hm
When we say that $SO(3) \approx RP^3$
Can we decompose $RP^3$ as like
The set of axis in $R^3$ + an angle
Set of axis would be $RP^2$
I dunno
12:55
@Slereah Sort of. You have the relation $\mathbb{R}P^n = \mathbb{R}P^{n-1}\cup_f D^n$ where the gluing map is the projection $f : S^{n-1}\to\mathbb{R}P^{n-1}$.
$D$ a disk?
what does the radius on the disk corresponds to?
Uh, this is a topological statement, it doesn't have a radius.
Well what's the difference between a rotation that corresponds to the center or the edge of the disk?
12:58
Oh, I have no idea how that relation translates to interpreting $\mathbb{R}P^3$ as $\mathrm{SO}(3)$
Hm
I thought it might be more like $RP^2 \times S$

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