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12:00 AM
why did my table show up in the totally wrong place?
wtf LaTeX
 
user218912
how does it work when like 3 or more people co-author a paper?
 
user218912
how do you know who wrote which part
 
@0celo7 You didn't answer my question still :p
 
@ACuriousMind I'm 99% sure we proved that theorem in my algebra class.
What am I thinking of if not that?
 
Does Section 3 look good?
 
12:02 AM
Yes
 
@GPhys Well, it doesn't suffice that it's constant along "a" helix, it would have to be constant along all such helices
That'd be a very weird potential indeed
@0celo7 100% sure you didn't because there are fields of order $p^k$ for arbitrary $k\in\mathbb{N}$.
@BernardMeurer Define "good"
 
wtf did we prove then
 
@ACuriousMind How can I improve it?
(Update your page, changes made)
also, what do i put where the $?$ is?
it won't be $\neg x$ right?
 
@ACuriousMind see question 3: cosmo.nyu.edu/roman/courses/dynamics_2016/homework2.pdf (note, due date passed, I'm just asking questions our TA was not sure about when we discussed it)
 
is it $(\neg x \vee 1)$?
halp
is lost
 
12:09 AM
I had thought initially the movement along where the equipotential was constant would always be a symmetry, but not I realize that is not true in general
 
@BernardMeurer I'm a bit confused by your explanation of the Boolean algebra to begin with. First you talk about a generic set, and then suddenly you talk about truth values, and say "a" and "b" are now "0" and "1". Don't you mean the universal bounds should be 0 and 1?
 
the first question wasn't straightforward either, I guess (a particle in a constant magnetic field). Translation along the axes orthogonal to the direction of the magnetic field is a symmetry even though that transformation changes the lagrangian since it only changes the lagrangian by a total time derivative
 
@ACuriousMind the truth values should be x, y I guess
for x,y in B
 
what?
 
But the thing is that Axiom 8 proves that B only has two distinct elements
 
12:12 AM
@ACuriousMind Would it kill you to say "I don't want to look at your proof"
 
@GPhys Exactly those transformations which map a given equipotential surface to itself are symmetries.
@0celo7 Yes.
 
@ACuriousMind Why?
 
@ACuriousMind Axiom 8 defines the universal bounds, and makes it clear that only 2 elements can exist
Right?
 
@BernardMeurer You didn't prove that. If you insist on showing the algebra is a field explicitly, I don't see why you just assume that
 
@ACuriousMind Good idea :)
 
12:15 AM
It's certainly not evident from anything you've written that a Boolean algebra has only two elements
 
@ACuriousMind Okay that makes sense
 
@GPhys I find that "helical" and "toroidal" are both rather vague descriptions of how exactly the equipotential surfaces look like
 
@ACuriousMind Doesn't that follow from Axiom 8?
Or am I wrong to state so?
I get that I need to prove it, but It makes sense right?
 
@BernardMeurer no
 
@ACuriousMind I had a similar thought at the time
 
12:16 AM
you write $a,b,\dotsc$ in the first line
implying there are more than two
 
@0celo7 If there exists an operator $a\rightarrow a'$ such that $a\cdot a'=\emptyset$ and $a+a'=I$
 
Our TA grading the homeworks initially claimed that x and y translation were not symmetries in the constant magnetic field problem (assuming the magnetic field is in the z direction)
but I convinced him during lecture that it is, in fact, a symmetry
 
Dang it I had the logic for this in my head a second ago
Sigh
 
@ACuriousMind if and only if?
 
@BernardMeurer I think you can't prove that. Unless your definition deviates from the standard, a Boolean algebra has $2^n$ elements
 
12:20 AM
$n$?
 
as in, if a transformation doesn't map a potential to itself, is it always not a symmetry?
 
@BernardMeurer Some integer
 
@ACuriousMind Positive, no?
 
right now my working definition of a symmetry is a transformation that doesn't change the Lagrangian by more than a total time derivative
 
sure, 1/2 elements doesn't make any sense
 
12:21 AM
@ACuriousMind You never know.
 
@ACuriousMind I'll ask on MathSE
 
I've seen papers that explicitly state, let $M$ be an $n$-dimensional manifold, $n$ positive.
 
I don't know how to prrove this
 
I want to know what these negative dimensional manifolds are
 
I had the most wonderful proof in my head a second ago
 
12:22 AM
@BernardMeurer yeah yeah
Fermat tried that shit 400 years ago and we didn't buy it then.
3
Q: All finite boolean algebras have an even number of elements?

MikeCThis seems obvious but I wanted to check, since I don't see it mentioned anywhere. If we define a boolean algebra as having at least two elements, then that algebra has a minimal element (0) and a maximal element (1). Since each element has a unique complement, 0* = 1 and 1* = 0. If I add a thir...

@BernardMeurer It seems highly nontrivial, and you don't get 2
 
@GPhys Sure, that's correct. I'm reluctant to say "if and only if" because you are allowed to transform $t$ too, after all, and so there might be strange symmetries that don't preserve the equipotentials because they compensate for it by strangely transforming $t$.
 
You get $2^n$ like Mr. grouchy grouch said
@BernardMeurer Also a quick wiki search tells me that a Boolean algebra forms a ring, not a field
 
@ACuriousMind I would be interested in an example of such a potential, but that does answer my question in the way I intended, thanks
 
so it won't be a vector space over itself
it's just a module
 
@0celo7 Well but does it forming a ring imply it not forming a field?
 
12:26 AM
If it formed a field, they would say that instead of saying it's a ring
a field is more specific
 
Well, the two-element Boolean algebra is clearly a field
 
@ACuriousMind Exaclty
 
Just the general ones might not be
 
"clearly" -- only if you have a PhD in algebra!
I still don't know what a boolean algebra is
 
wait
 
12:37 AM
0
Q: Proving that a Boolean algebra only has 2 elements

Bernard MeurerWe define a Boolean algebra as a set of $B$ elements $a,b,\dots$ which satisfies the following axioms$^{[1]}$: $B$ has two binary operators $\wedge$ or $\cdot$ (logical AND) and $\vee$ or $+$ (logical OR) Idempotence $a\wedge a = a \vee a = a$ Commutative law $a \wedge b = b \wedge a$ $a \...

 
@ACuriousMind this is only for a potential $V(q_1,q_2,\dotsc ,q_i)$, right? (as opposed to depending on, say, $\dot q$)
I was thinking with, e.g., the constant magnetic field problem (say, in the $z$ direction), translation in $x$ or $y$ does change the potential but is still a symmetry
but in that case the potential depends on $\dot x$ and $\dot y$
otherwise that's a counterexample to the if and only if, I guess
 
1:13 AM
@ACuriousMind So, to recap, I should be able to prove this: Suppose $V=V(q_1,\dotsc ,q_i)$ is a potential that depends only on the generalized coordinates. Then, suppose $\zeta[\epsilon]$ is a coordinate transformation parametrized by $\epsilon$ that does not include a time transformation. Then, $\zeta[\epsilon]$ corresponds to a symmetry if and only if it transforms the potential like $V\mapsto V$. That is, such that the entire potential maps to itself.
(I just wrote that out so I can work on it later when I have more time)
 
@GPhys I don't think that's necessarily true
 
@ACuriousMind Getting out my algebra notes
AHA!
I was wrong!
Dammit!
 
@ACuriousMind Is there a modification of the statement to what you were saying earlier to make it true (that's my translation of what I thought you were saying before)
 
The prime field of a finite field is $\Bbb F_p$
 
looking at the Lenz-Runge vector now
 
1:22 AM
@GPhys Well...that was what I was saying before, then I thought a bit more about it and tried to find an example of a symmetry that's a) highly dependent on the potential but b) not really related to a spatial symmetry of that potential, and I remembered the 1/r potential/the Lenz-Runge vector.
 
ah
@ACuriousMind Oh my
@ACuriousMind But it does work in one direction though, right? That is, if $V\mapsto V$ then it corresponds to a symmetry?
 
1:39 AM
Well, yeah, kinda tautologically. If you transform only the $q$ and keep the $p$ fixed, then the standard Hamiltonian of $p^2 + V(q)$ is invariant if $V\mapsto V$ under the transformation.
 
Sure
err
yes
@ACuriousMind I was thinking it wasn't true, but $p^2$ can be changed by at most a total time derivative I guess
 
user218912
@0celo7 this guy in my class showed me that you don't even need to lower all the indices/ use dummy indices to do the lagrangian vector field derivatives. because the metrics cancel out.
 
user218912
so you can just take the derivative normally and get the same answer.
 
@IceLord Correct, but that's not rigorous.
You first have to justify being able to do that.
 
user218912
well mine is rigorous af.
 
user218912
1:52 AM
like 7 lines of steps for each derivative.
 
Well, no one actually does the derivatives like that
 
user218912
lol
 
but now that you understand how to do them like that, you can do the shortcut
 
user218912
but in the process I learned index notation so it was good for me anyway.
 
user218912
brb
 
1:59 AM
@ACuriousMind Or, maybe it's not so clear. The transformation can still depend on the $q_i$s of each other (like in rotations). Under this it is not so clear that $p^2$ only differs by a total time derivative?
 
@IceLord Dammit I need hardcover Lee
ask more questions
wtf is "one-to-one into"
 
user218912
@0celo7 I understand everything so far.
 
user218912
problem set 2 in 1 day, I'll be asking a lot of questions then.
 
CRAP
need help
Anyone know how to import a vector from a pdf paper into microsoft word?
 
a vector?
what does that even mean
 
2:08 AM
Basically an image whose quality doesn't get worse no matter how much you zoom in
As opposed to a raster (JPEG, PNG, etc.), which gets more pixelated when you zoom in
 
does copy paste work
 
user218912
@SirCumference google is your friend.
 
@IceLord Hasn't helped
I need figure 1 from here
 
LINK TO THE ABSTRACT
 
user218912
2:09 AM
 
Why tho
 
@IceLord nice
you destroyed him once again +1
 
user218912
lol
 
No, I'm afraid you haven't
I already got the vector graph out
I need to figure out how to put it in word
 
control V
noob
 
2:11 AM
Doesn't work...
 
Sure.
 
user218912
@SirCumference is it eps or svg or emf?
 
I've never figured out how to get vectors in word before. LaTeX equations (which retain their quality when you zoom) won't import, and pdfs won't either
@IceLord Pdf
 
@IceLord I'm making a reading list for you.
 
user218912
for physics?
 
2:13 AM
No
Well, GR books will be on there
Does that make it physics?
 
user218912
@0celo7 yes
 
ok start reading Zee
 
user218912
I'm reading like 5 books right now.
 
user218912
@SirCumference does this help
 
My shelf is looking good.
I removed the second to last physics book.
HE is now no longer on my shelf of Holy books.
 
user218912
2:15 AM
what's the last?
 
Straumann GR
 
user218912
that has a lot of differential geometry in it.
 
still the best reference for formulas in basic Riemannian geometry
 
user218912
I am still developing a book shelf.
 
Well, I have three shelves + a pile
my "main" shelf is right next to my desk
by shelf I mean a single shelf, not a shelving unit.
 
user218912
2:20 AM
okay.
 
user218912
I enrolled in a grad stat mech course. that makes 3 grad courses this semester.
 
user218912
qft = okay, condensed matter = bird, stat mech = difficult af.
 
user218912
I already missed 3 weeks of lectures and I'm so lost.
 
lol
there's this dude in my analysis class
he just showed up on monday
transferred in from single variable
prof's like "who are you"
he says "oh I transferred from 341"
Prof says "ok" ::turns around:: "so we were talking about the closure of point separating function algebras on compact metric spaces, right?"
that dude is screwed
 
user218912
That's like me in stat mech.
 
2:27 AM
@MAFIA36790 hi
want to see my new books :P
 
user218912
@0celo7 how can he switch in this late?
 
I don't know. But the class is really hard
 
user116211
@0celo7 Where? Where? Show it, man!
 
user116211
@0celo7 o/
 
@IceLord Forget that
I imported the pdf into Illustrator and cropped out the graph into an svg
Now how do I put it into word?
 
2:29 AM
 
user218912
@SirCumference ...
 
Yeah. Just found that...
Thanks tho
Now I realize I can just drag and drop eps files...
 
user116211
@0celo7 AMS Chelsea is awesome!!
 
2:45 AM
@MAFIA36790 yes it is pretty good
the print quality is very nice too.
 
user116211
I'm very much liking the brown front-cover with those golden writings.
 
yeah
but they're only old books, basically
AMS Chelsea reprints classical texts that are out of print
 
user116211
@0celo7 Like Dover?
 
Yes
But these are much nicer ;)
 
user116211
Yeh, seeing that.
 
user116211
2:49 AM
Anyways, JD has pulled off his nomination. Now, it's four: Alfred, tpg, Jim-the king, ACM.
 
hmm maybe ACM won't win after all
this tpg fellow seems to have it
@IceLord I need Lee :o
 
user116211
Frankly, I don't know very much about him.
 
user116211
@0celo7 NOOO!!
 
user116211
Most of our first choice was ACM.
 
user116211
ACM and Jim - that must be it.
 
2:55 AM
I don't like this flimsy paperback
 
user116211
Well, not bad though but nothing to AMS; I have Callahan from Springer; they look pretty same.
 
user116211
Only Bourbaki: Set Theory looks better in the Springer cover.
 
oh I have some springer books
like 20
but this one is special
 
user116211
I have three.
 
from this angle it looks fine:
 
user116211
2:59 AM
The Wileys are the worst.
 
user116211
Nay; dull looking ;/
 
cat tooth marks:
 
user116211
@0celo7 ;P
 
and then the glorious binding:
 
user116211
3:01 AM
I have many dog teeth/foot marks too but not in the front cover.
 
user116211
@0celo7 Seems to be an old library book.
 
the book is basically falling apart :/
@MAFIA36790 no it's mine
my 40 year old Spivak is in better shape than this 2 yo springer book
 
user116211
@0celo7 I know; but since the front cover was coming out, that's why the old, library feeling came.
 
I didn't even abuse it
 
user116211
@0celo7 2yr? ohh!
 
3:02 AM
the front just detached
my Shankar is holding up pretty nicely though
 
user116211
@0celo7 Wasn't there a 1 or 2 months guarantee?
 
it's even older
@MAFIA36790 It lasted about 6 months until it did that
 
user116211
ohh.
 
when I get rich I'll buy a new one
 
user116211
sure ;))
 
user116211
3:04 AM
Have you anything in mind @0celo, that might make you rich faster?
 
lots of money?
 
user116211
apart from the stripper plan
 
small million dollar loan perhaps
 
user116211
Ah!
 
user116211
Anyways, I studies Numerical Analysis yesterday and learned some pretty cool things:
 
user116211
3:09 AM
Newton's Forward Formula for equal width interpolation; Lagrange's Interpolation Formula, Numerical Integration - Quadrature Formula, Trapezoid Formula and Simpson's One Third Formula.
 
I learned three of those some time ago
my calculus prof was a numerical analyst
 
user116211
@0celo7 They are pretty easy though.
 
user116211
@0celo7 ohh.
 
@BernardMeurer ^
 
user116211
Holy hell! Can't say anything about that ;P I'm now very much fond of the brown cover; so can't expect a dark dull green cover.
 
3:22 AM
hey that's my favorite mathematics text of all time...
 
user116211
@0celo7 Sure, but I'm talking about the cover; not the content inside.
 
I happen to like the cover too
 
user116211
oops.
 
user116211
AMS has created a standard now; so ....
 
the regular AMS books are not that nice
 
user116211
3:23 AM
ooh!!
 
@MAFIA36790 Gaussian Quadrature?
If not, you certainly missed the most important one!
 
although in practice you probably want some combination of trapezoid, romberg, and gaussian quadrature
 
very good print quality but the cover is meh
 
since trapezoid is probably the best for noisy integrals
and computers are fast these days anyway
 
3:26 AM
AMS GSM books stick out like a sore thumb on math shelves
 
user116211
@GPhys: $$I=h\left[ny_0 +\frac{n^2}{2}\Delta y_0 + \frac{\frac{n^3}{3}-\frac{n^2}{2}}{2}\Delta^2 y_0 + \frac{\frac{n^4}{4}-n^3 +n^2}{6}\Delta^3 y_0 +\ldots\right]$$
 
user116211
General Quadrature formula.
 
user116211
@GPhys I have not read Romberg yet.
 
@MAFIA36790 Look up Romberg integration for probably the simplest version of what you can do with normal expansions and error estimates using evenly spaced points
 
user116211
@GPhys Trapezoid is easier to compute than Simpson.
 
user116211
3:28 AM
@GPhys sure.
 
@MAFIA36790 Gaussian Quadrature is generally the best you can do but you sacrifice evenly spaced points
 
user116211
@0celo7 Not that bad.
 
also in practice you want to do things like trapezoid integration adaptively
 
user116211
Actually I have Kelley's topology which looks very much the same.
 
WHAT
 
3:30 AM
when you double the number of points in the trapezoid rule you can write it as the previous integral estimate + a function of half the points
 
I NEED THAT BOOK
GIVE ME
 
user116211
@0celo7 But I have one!
 
so like this you can adaptively calculate the error when doing trapezoid integration without adding extra point calculations
 
How did you get it
It's out of print
 
user116211
@0celo7 It is pretty cheap here at Amazon.in.
 
user116211
3:30 AM
@0celo7 Noo!!
 
@MAFIA36790 Do you know Python?
 
@MAFIA36790 how about this
 
user116211
@GPhys no; I'm just a first year learner ;P
 
oh
 
user116211
@0celo7 I have the pdf but haven't read.
 
3:31 AM
@MAFIA36790 gaussian quadrature is amazing
 
You can get Kelley topology for like $20, but it doesn't look anything like Helgason...
And it's a crappy reprinted paperback
 
user116211
@0celo7 Kelley is actually great; especially the introductory order-theory in the first chapter.
 
@MAFIA36790 using $n$ sample points, you can get an exactly correct integral value for any polynomial up to order $2n-1$
with gaussian quadrature
 
user116211
@0celo7 Yes, now published by maybe Wiley or so. Wait...
 
so, say, by sampling 5 points you can exactly integrate any 9th order polynomial
 
user116211
3:33 AM
@GPhys Holy hell!!
 
so, for any function well approximated by polynomials (so, any smooth function), gaussian quadrature works extremely well
 
@MAFIA36790 lol you like saying that
 
@MAFIA36790 it gets better: gaussian quadrature is as simple as riemann sums computationally
(provided you have pre-stored "weight" values. but there are libraries of these weights widely available)
 
user116211
@GPhys This can be done, I know that, thanks to Weierstress Theorem; we want just a function to be continuous over the concerned interval.
 
user116211
3:36 AM
Ah! Springer!!
 
well, the functions not "well approximated by polynomials" are e.g. functions with asymptotes in their derivatives like sqrt(x) integrated from 0 to 1, but actually gaussian quadrature still works better for these functions than other methods due to the way it samples
 
user116211
The original front cover was blue.
 
the other functions where you don't want to use gaussian quadrature are extremely noisy functions
 
user116211
@GPhys I would definitely read that!
 
where the polynomial-like assumption is clearly invalid and you should just be using the trapezoid rule
the correct way to deal with e.g. integrating sqrt(x) is to just do an integral transformation to get rid of the derivative asymptote
 
3:37 AM
@MAFIA36790 lies
what is this
 
but for noisy functions you should just use the trapezoid rule (the fitting of simpson's rule is bad in very noisy functions too)
 
user116211
@0celo7 Kelley Topology :(
 
user116211
@GPhys How can I use trapezoid rule if the polynomial assumption is invalid? It comes from the Quadrature formula with the assumption that the degree of the polynomial is one. I didn't get that.
 
@MAFIA36790 Another way to interpret the trapezoid rule is just connecting the dots of your function evaluatoin points and calculating the integral under the shape you just traced out
indeed, this is where "trapezoid" comes from
it's a trapezoid between any two points
 
user116211
@GPhys ahh!
 
3:45 AM
so that works pretty much just in general
 
user116211
What book did you follow @gphys?
 
I learned it long enough ago to not know where I learned it originally
and if I was curious again it's easy enough to rederive
 
user116211
I'm now following Scarborough, Freeman and a bit of Whittaker.
 
user218912
I realized the only way I can learn stuff is to do exercises.
 
user116211
@IceLord Nay ;/
 
user116211
3:48 AM
You first learn the stuff and then apply it and furnish it doing the exercises.
 
user218912
nah
 
user218912
from what I've been experimenting with, I just go straight to the exercises and look up what I need to solve it.
 
user218912
then I remember it forever.
 
user218912
if I just read it I'll forget it in 5 mins.
 
read harder
 
user116211
3:49 AM
Anyways, @gphys, I find Newton's General Divided Difference Formula easier to compute than the Lagrange's Interpolation Formula. Do you know what advantages I get using the latter?
 
user116211
@IceLord WTH!!
 
@IceLord there are books w/o exercises
I have some
 
user116211
Bourbaki
 
user116211
No exercises.
 
user116211
But still a great book!!
 
user218912
3:50 AM
well my reading memory is bad.
 
you don't need exercises if you prove all of math, dude
 
user218912
or that^
 
user116211
^^^
 
user116211
@0celo7 That's my point!!
 
exercises have two purposes:
they're exercises
and they let you state things the reader should know, but you don't have the time/space/patience to prove them
for Bourbaki option two was not an issue so they don't have exercises
 
user116211
3:52 AM
@0celo7 They prove everything.
 
Books like HE or Li or KN don't have exercises, but you'll write pages and pages trying to decipher what they're saying
 
user116211
They even taught how to write formulas.
 
user116211
Anyways, I'm leaving for the college.
 
Bourbaki taught many modern mathematicians how to write mathematics
 
user116211
@0celo @IceLord o/
 
3:53 AM
bye
 
user116211
@0celo7 nods
 
user218912
bye.
 
writing birthday cards is the worst
@IceLord what page of gourgoulhon?
 
user218912
25
 
highly nonstandard
burn the book
I'm trying to set mine on fire rn
 
user218912
3:56 AM
lol
 
user218912
how is that nonstandard?
 
user218912
ofc you would know better but
 
user218912
it seems reasonable to me
 
I do know better
let me define spacetime
getting out the standard reference for Lorentzian manifolds
 
user218912
oh boy
 
3:58 AM
A spacetime is a time-oriented Lorentzian manifold.
 
user218912
okay then what is minkowski space?
 
$\Bbb R^4$ with the Minkowski metric and a time orientation
both orientations are equivalent
well, maybe not a time orientation
 

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