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8:05 AM
Possibly VPython
Well, it is similar at least
 
Anonymous
8:18 AM
@NickolasAlves Thanks
 
Anonymous
BTW welcome to this chat @NickolasAlves
 
8:49 AM
U r welcome
And thanks =D
 
 
3 hours later…
11:25 AM
Hi all, i have a potentially really easy question but I'm kinda stumped
I mean stuck
I mean, whatever here is the question
Doing some calculations on the Lie bracket between two vectors, here's what I have
Oh wait, maybe that commutator thing doesn't even make sense...
(I wanted to ask how I'm going to extract the nu'th component of the commutator)
Can I exchange $\mu \leftrightarrow \nu$ from the first line to the second?
And/or how do I get the \nu'th component of the commutator [e_mu , e_nu]
 
11:55 AM
@1010011010 : The number of the beast :)
 
12:06 PM
Morning
 
@Qmechanic But it's binary, so it's k
 
12:47 PM
in Mathematics, 28 secs ago, by s.harp
I am having some trouble with understanding the sentence, because $C_0^\infty$ is not contained in any Hilbert space that I know, and self-adjoint is a qualifier that only makes sense for operators on hilbert spaces
 
1:04 PM
Not contained in any Hilbert space? Except for like all of them
@Semiclassical Yeah so when I split up the square root then my CAS calculator gives a sensible limit at infinity. There's something very strange going on here!
 
1:23 PM
@0ßelö7 it does all seem to come down to the difference between $\sqrt{z-1}\sqrt{z+1}$ and $\sqrt{z^2-1}$.
 
Hello citizens
 
For $z>1$, Mathematica concludes both are positive. But for $z<-1$, it gives negative values for the first and positive values for the second.
actually, I don't even need the $\pm 1$. Mathematica gives $(\sqrt{z})^2=z,\sqrt{z^2}=|z|$ for all real $z$.
in the case, though, I guess it makes sense. If $z<0$, then $\sqrt{z}=i |z|^{1/2}$, so squaring that gives $-|z|=z$. By contrast, $\sqrt{z^2}=\sqrt{|z|^2}=|z|$.
I dunno. I guess the point is that if $y=\sqrt{z^2-1}$ then $y^2=z^2-1\sim z^2$ for large $z$, so for large $z$ we can take $y\sim z$ in a single-valued way.
or, to put it another way: we usually would think of the $\sqrt{}$ in $\sqrt{z^2-1}>0$ as being the principal root i.e. positive both $z>1$ and $z<1$.
But while it's certainly positive for $z>1$, if we analytically continue $\sqrt{z^2-1}$ around the branch cut then it ends up being negative for $z<-1$.
 
1:41 PM
@Semiclassical amazing
 
It does suggest that writing it as $\sqrt{z^2-c^2}$ is misleading, though
 
@Semiclassical this is making my brain hurt. How am I supposed to evaluate the far-stream velocity?
 
I'd say you evaluate it like this. For large $z$, you're away from the branch points and $\sqrt{z^2-c^2}$ should be an analytic function of $z$. Hence $\sqrt{z^2-c^2}\sim z$ for large $z$
 
What are we doing
 
conformal mappings
 
1:44 PM
@BalarkaSen g******* branch cuts
 
but I think it could be boiled down to "how does $\sqrt{z^2-1}$ behave for large complex $z$?"
Naively, you'd have $\sqrt{z^2-1}\sim |z|$ for large $z$. But then it's not analytic at infinity.
 
@Semiclassical yeah, and the answer depends on how one interprets it...wonderful
 
0
Q: "Purpose" of torque in projectile motion

AbcdTorque, $\tau$ is defined as: $$\tau = \vec{r}\times\vec{F}$$ Intuitively, it's the rotational effect of force. However, using the above definition of torque we can calculate the torque due to a force acting on any particle about a reference point. Consider projectile motion for instance...

 
My ruling is that it should be $\sqrt{z^2-1}\sim z$ for large $z$ if you insist that it's analytic at infinity.
 
Thanks so much for the help :) I'll talk to a guy in my elliptic PDE class who's also in fluids and see what he got
 
1:45 PM
@0ßelö7 How does the far-field velocity come out if you assume that?
 
@Semiclassical I'm in class right now
 
It's a function of a+b and U, however, where U is the velocity for the disk flow
@Semiclassical now physically I'd hope that as a-->b the far-stream velocity goes to U, right?
That seems like a good sanity check.
 
looks like it comes out as $w(z)\sim Uz+U\left(\dfrac{a+b}{2z}\right)^2$ for large $z$
which is to say, at infinity it behaves like the flow around a disk of radius $\frac{a+b}{2}$?
The dominant term in there is $Uz$, which corresponds to a far-field velocity of $U\hat{x}$.
 
@Semiclassical oh also there's a complex conjugate in here somewhere ::eye twitch::
 
1:51 PM
yeah, that's a pain
but I think the above asymptotic for $w(z)$ is a good sanity check.
I want to say there's a further sanity check as well. If one thinks of this $w(z)$ as the complex potential of an electrostatics problem, then the problem is one of an elliptic cylinder with finite charge per unit length in an electric field.
 
@Semiclassical yeah because it's just a complicated Laplace equation
 
The $Uz$ term confirms the presence of an electric field. The second term should then correspond to the electric field generated by the cylinder itself at large distances.
But why $\frac{a+b}{2}$? If anything I'd have expected $\sqrt{ab}$, since a cylinder of radius $\sqrt{ab}$ has the same cross-sectional area as an ellipse with semi-major/minor axes $a,b$.
oops. should've been $w(z)\sim Uz+U\dfrac{a+b}{2}\dfrac{b}{z}$
which is still pretty weird.
Hmm, maybe I get it. The surface of the elliptic cyilnder is curved, so the surface charge density would vary across the surface. So I'd need to be more careful about the relation between $U,a,b$ and the charge on the cyilnder.
 
Hm
I need to put a symbol for adjacency via mathjax
But mathjax doesn't have $\Ydown$
What to use
$Y$?
$\operatorname{Y}$ maybe
 
2:16 PM
@Slereah what is that?
 
Two points are adjacent if every of their neighbourhoods contain both points
cf this extremely great site
Subscribe and I'll send you a pizza roll
 
@Slereah what kind of non-Hausdorff BS is that
@Slereah how do I sub?
 
just kidding
no subscription yet
 
2:44 PM
in Mathematics, 57 secs ago, by Secret
ugh, f*** distributivity
lollololol
 
The page where to put thems pdfs
 
how many chapters have you written
so far
 
Define "written"
All of them have things in it
Not necessarily a lot of things
 
latexed
appropriately formatted
 
All of them are latexed
 
2:54 PM
@ACuriousMind is the burping in Rick and Morty supposed to be funny or cringey?
 
If you mean completed then 0 right now
A few are pretty close to being completed
 
@Slereah well i'm DISAPPOINTED
 
Rome wasn't built in a day!
 
@BalarkaSen do you want to write a book?
Differential topology without analysis
 
@Slereah This is my reaction to you
I give your work a light 0 out of 10
you hear me
 
2:59 PM
Nooooooo
 
@0ßelö7 no
or at least i wouldn't publicly accept that offer
Hi @Avantgarde. How do you like my new gravatar?
 
It's worse than Corey Feldmans album
@BalarkaSen what?
Why do people act so strangely about stuff like that
 
You should listen to Fantano's review of the new brainless brain album
"I am brain" or some shit like that
it was beautiful
 
3:16 PM
@BalarkaSen Ingenious, but disappointing
 
come on why does everyone keep saying that
i put a lot of work in making this you know
 
Meh
 
and I appreciate that, sure
 
We expect better from the legendary Balarka
 
actual 6 minutes of my life were spent
England is my city, MS Paint is my Photoshop
2
 
3:25 PM
@Semiclassical so when I add the swirly term I get the 1/square root thing which doesn't give a pole...
There's still no lift
Or maybe I'm wrong and just need to do the integral
 
@BalarkaSen very catchy :P
the huge content created by that one phrase is unimaginable
and awesome
 
in Mathematics, 1 min ago, by Secret
Actually what happens when we have a set theory where we are unable to have a choice function on finite sets?
in Mathematics, 1 min ago, by Secret
e.g. imagine a universe where we can only count to 3
 
Set theory with finite sets already exists
It's basically equivalent to Peano's axioms
Of course this has finite choice
Finite choice derives from just a handful of axioms, though I'm not sure which
 
3:42 PM
@0ßelö7 well, you're putting an elliptic airfoil in a stream and then adding vorticity
 
If you don't have finite choice and you still have a coherent theory I'm not sure it would be a very rich system
 
By symmetry, I think you still won't have any net force in that case. (You'll have a net torque but not a net force.)
On the other hand, if you displace the center of vorticity a bit then I think you would get a net force
 
7
Q: Which axioms of ZF are used for finite choice?

Doly GarciaApologies if this is a silly question, not an expert in set theory but just wondering about it. ZF implies finite choice. But let's suppose one wanted to work without it. The thinking here is being uncomfortable about sets where none of the elements are computable/definable, therefore one couldn...

Seems that would need induction to be nuked, something that is not very useful for most of the common maths we do
 
@Semiclassical no, the vorticity will produce a force (in the circular case) because there's a torque, and then the far-stream velocity causes it to move
You get a 1/z term in the complex velocity of you put in a vortex
But now I have that awful reciprocal square root which is actually impossible to integrate
 
Hmm, fair
 
3:50 PM
Just out of curiosity, what is the integral of 1/sqrt z around the unit disk?
I'm assuming zero but I can't into calculus apparently
 
No, it's not zero
You'd need to go through an argument of 4pi to get a zero integral
 
Huh! Maybe I should break up the integral into two square roots and use the residue theorem
Yeah I got -4 for the integral
Did it by hand, not sure how right it is
 
(If you think of your function living on a branched cover of C, then going once around the origin in C actually puts you on the second sheet
So in that sense it's not really a closed contour
 
Right so to do that integral you have to go through a branch cut
 
Right
 
3:55 PM
I'm going to office hours. This is ridiculous for a class that doesn't have the grad complex analysis as a prereq
The guy in my PDE class dropped the fluids class :(
 
most elementary way to do the square root integral is to parametrize by $z=re^{i \theta}$
 
Yeah i did that by hand
 
Check out this baby
 
But I don't want to use Residue theorem around a branch cut
I'm not sure what I'm doing here is legitimate
@Slereah geez, how much did you pay for a hard cover?
 
4:00 PM
Nothing
Birthday gift baby
 
You can't use the residue theorem on a branch cut as such, no
 
@Semiclassical but to evaluate the integral of 1/sqrt(z^2-c^2) around the ellipse id have to use the residue theorem
I can't do that integral by hand...but residue theorem probably doesn't apply
 
Use the physicist way @0ßelö7
Use the residues
 
nor directly. But if the function is analytic in the complex plane away from the cut, then you can view the integral as winding around the point at infinity
 
Where exactly is the branch cut here
From -c to c?
 
4:03 PM
And you can use the residue theorem there
Yeah
More formally, try subbing w=1/z
 
Then do a w integral around the unit circle?
 
Then f(z)dz = f(1/w)(-dw/w^2), the minus sign reflecting that z and w wind in opposite directions
Yep
 
0
Q: i have a differet answer from what is written (always)

Bol Bol Osama Amirin my book of general relativity it says that T=ict ,$ {x^\prime}$ = x $cos\theta$ + T${sin\theta}$ and x=vt ,${x^\prime}$ =0 and he conclude that ${tan\theta}$=iv/c and the problem is i always get ${tan\theta}$=-v/ic so how did he get there

 
It's still a nasty square root...
 
Key point is that f(1/w)/w^2 should have a pole at w=0
Well, the pole at w=0 should be the leading term for small w
So it may be simpler than it looks
 
4:12 PM
Is a branch cut just fancy complex analysis talk for a specific type of discontinuity btw
 
@Slereah we know
It's still an issue when trying to do integrals
 
That was a question
 
It's a discontinuity in how you represent a multi-valued function
 
Ah k
Is it general to all multivalued functions?
 
The multivslued function itself changes smoothly across the cutt
It's pretty generic, yeah
Though the structure you get as a result of the branch points is weirder for some cases than others
 
4:23 PM
@Semiclassical he delayed the homework and said he'll do most of it in class tomorrow
 
@0ßelö7 is the last paper in the book by Geroch the one with the awful GR from gauge theory
 
Yeah I tried reading it
Very philosophical
 
@0ßelö7 lol
 
@Semiclassical he looked at his notes on the problem and didn't understand what he did
😪
What a waste of time
 
So @Semiclassical
what semiclassical theory are you
Are you semiclassical gravity
Or semiclassical electromagnetism
 
4:33 PM
Quantum
 
@JohnRennie so what's the formula.... ?
 
What does "semiclassical quantum theory" mean
 
WKB approximation usually
 
And it must include the velocity of individual particles.
 
o
 
4:34 PM
@Abcd Suppose you have a ball of gas. The gas molecules/atoms are all whizzing around at high speed so each molecule/atom has a kinetic energy.
 
1
Q: Why is translational kinetic energy defined only for the centre of mass' velocity?

Abcd$$K_{\mathrm {translational}}= \frac{1}{2} Mv_{\mathrm {com}}^2$$ Why does the term for translational kinetic energy include only the velocity of the centre of mass of a rigid body? How can we ignore the velocity of the different particles constituting the system? Can someone prove this to me...

@JohnRennie Yes,I know.
 
If we add up the kinetic energies of all the molecules we get the internal energy.
 
What about the potential energy
 
@JohnRennie Consider a rolling wheel instead of gases.
 
The internal energy is just the sum of all the kinetic energies, but we don't call it that.
 
4:35 PM
I thought that was part of the internal energy too!
 
@JohnRennie I hope you didn't assume that my question referred to gases.
 
@Slereah ideal gas! :-)
 
I just said that google showed results only for gases.
 
@Abcd With a rotating object the kinetic energy of all the bits is called the rotational kinetic energy and given by $\tfrac{1}{2}I\omega^2$.
 
I guess I should remove that comment lest everyone should think that I am confused about the translational KE of ideal gases.
@JohnRennie what about their linear velocities? the formula you stated doesn't account for that, does it?
Oh!, $v=r\omega$
 
4:39 PM
That works if you've got an object rolling without slipping
 
So @JohnRennie I have inferred this: The T.KE of a rolling body is due to the velocity of centre of mass while the RKE is due to the linear velocity+angular velocity (not in the addition sense)of the constituents. Am I correct?
"+" used above in the "and" sense.
 
But suppose you toss a frisbee. Then there's no obvious relation between the rotational velocity and the linear velocity
 
The proper sign for and is $\wedge$
 
@Slereah Both are acceptable.
 
@Abcd I wouldn't say it's due to linear velocity and angular velocity, because as you say they are related by $v = r\omega$.
 
4:40 PM
&& works too
 
@JohnRennie Accepted. So can I at least conclude that all the particles are contributing to the kinetic energy during rolling?
@Semiclassical yes.
 
Anonymous
@Abcd Rolling motion is a superposition of translation and rotation. So, your first statement is wrong. For T.K.E all the particles have same translational velocity.
 
Anonymous
 
Oho! How confusing!
@Blue Picture isn't clear.
 
Anonymous
$(1/2)\sum m_i v_i^2$
 
Anonymous
4:43 PM
$v_i=v$ for all particles $i$
 
Anonymous
And you know $\sum m_i = M$
 
Anonymous
So, you get $T.K.E=(1/2)Mv^2$
 
Anonymous
Where $v$ is translational velocity of COM
 
@Blue @JohnRennie My book derives: $$K = 0.5 I_{com}\omega^2 + 0.5 Mv_{com}^2$$
 
Anonymous
@Abcd That's right.
 
Anonymous
4:45 PM
 
@Abcd yes, that's just the sum of the rotational and translational energy
 
@Blue translational velocity of com = translational velocity of each particle?
Please verify this^
 
Anonymous
@Abcd Yes. See the picture ^
 
pretty simple. Understood @JohnRennie and @Blue. Easy.
Thanks.
 
Anonymous
@0ßelö7 My gravatar is dedicated to you. :D
 
4:49 PM
That's nice I guess?
 
Anonymous
Depends on how you take it. I was looking for something more weird.
 
Anonymous
But for now this one looks nice. :P
 
Anonymous
Woah. Huge question. I think I can answer it. :P Thanks to ACM
 
Anonymous
In statistical mechanics, a semi-classical derivation of the entropy that does not take into account the indistinguishability of particles, yields an expression for the entropy which is not extensive (is not proportional to the amount of substance in question). This leads to a paradox known as the Gibbs paradox, after Josiah Willard Gibbs. The paradox allows for the entropy of closed systems to decrease, violating the second law of thermodynamics. A related paradox is the "mixing paradox". If one takes the perspective that the definition of entropy must be changed so as to ignore particle permutation...
 
Anonymous
4:53 PM
Oh, he's talking about Gibbs paradox.
 
Anonymous
Thanks a lot, I am truly reassured by your statement about the microcanonical ensemble being observer-independent. Let me ponder about the matter a bit. It seems that, as @By Simmetry was maybe hinting at, the fact that Gibbs noted that the definition of entropy works only if we include indistinguishability was an ante litteram evidence of the need for QM. — Smerdjakov 10 mins ago
 
@ACuriousMind should I skip algebra for an AdS/CFT talk?
 
@JohnRennie We defined velocity only linearly (this doesn't have relation with the previous conv.) right?
$\vec{v}$ is always linear?
Therefore we try to condense everything into $\vec{v}$'s form?
if anyone knows the answer please let me know.
Though I feel that the answer is obviously "yes".
even displacement is always linear
 
Anonymous
5:11 PM
@Abcd Yes
 
Anonymous
It's displacement per unit time
 
5:25 PM
@Blue you're name no longer matches youre avatar, change it to S.Cat,
pretty classy name i think :P
 
Anonymous
My shirt is still blue as you can see from the picture. There's always a tinge of blue associated with me. ;)
 
your shirt????
what shirt?
 
Anonymous
Zoom into the profile picture
 
oh what the hell
thats too small :P
 
Anonymous
It still exists :D
 
Anonymous
5:29 PM
I selected the picture very carefully
 
apparently...
hows you're project going?
 
Anonymous
@PrathyushPoduval I'm learning the theory portion at the moment. First chapter of the book by Naoki Shinohara is over. Also, I've progressed a bit with Arduino. I can write code for LEDs, Switches, etc now
 
nice, you bought that arduino pack?
 
Anonymous
I'm getting slow due to academic load
 
Anonymous
@PrathyushPoduval Yup
 
5:32 PM
how's it?
@Blue Dump the academic load :P
 
Anonymous
It's good. Has everything to get started
 
which book is it you're using?
 
Anonymous
I'm using Wikipedia and the book by Naoki Shinohara. For Ardunio I'm using the book named "Getting Started with Arduino"
 
Anonymous
Search on Google
 
Anonymous
Massimo Banzi
 
5:35 PM
@BalarkaSen what's a circle group?
 
@Blue I meant the one by Naoki Shinohara
 
@Blue somewhat unhelpfully, there's a user called @green who currently has a blue profile pic...
 
is it semiconductors?
 
Ah okay :P
 
5:43 PM
@Abcd It is worth your time to work through the completely general factorization of the kinetic energy of a system of particles into the CoM part and the relative part. (Of course it must be this way to satisfy the principle of relativity (which was present in classical physics from Galileo on)).
But to your specific question, the mass element at the point of contact in a rolling-without-slipping situation is momentarily at rest and so contributed nothing individually.
Which doesn't change the fact that you can write the energy in terms of Com and relative parts.
 
5:59 PM
@0ßelö7 the circle itself. R/Z
 

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