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12:03 AM
:25044167 I'm not telling you what to do, I'm not qualified for that
 
I realized that.
I don't know what to do though.
I'm supposed to have "grown out of" ADHD
And there's no way to actually test it, really
I need to talk to my doctor when I go back home
In any case, @ACuriousMind, I've been looking back at the "all Galilean spaces are isomorphic" thing
and that took so long, the proof is spread out over hours of chat :D
 
Hehe...yes, I recall that that didn't go quickly
 
12:20 AM
my mission this weekend is to piece together scraps of paper and chat to write down the proofs from Arnold so I don't forget them
@ACuriousMind Classic.
@dmckee I have a question about terminology
This problem involves a man throwing a box up at an angle
I'm supposed to calculate the "vertical reaction force" of his feet against the ground
So I can get a recoil force using impulse
is the vertical component of that what they want?
(or the negative of that) or do I also add his weight
 
12:35 AM
Does the box contain fruit for the weird people in those basic math word problems who are always buying and sharing fruits?
 
...huh?
I know how to do the problem, just don't know what they want
So I think I know how to do it :D
 
Nothing, I'm just wondering what is in the box the man is throwing
 
probably useless math books
abstract algebra, topology, etc.
@ACuriousMind you're free to interpret the problem too, but there might be a language barrier
"Assume he completes the throw in 0.25 s. What is the vertical reaction of both his skates (i.e., the sum of the two) onto the ice during the throw?"
it's normal force
so that's dumb
more work :'(
 
I would interpret that such that you should indeed calculate the vertical component of the recoil force.
 
does that include the weight?
assuming you defined it as I did, it doesn't
 
12:41 AM
No, I think it's really just the reaction force to the force the man exerts on the box
 
but that's what the profs want
recoil + weight
i.e. the force his feet are exerting on the ground during the throw
 
Well, I'd call that recoil/reaction + weight, not merely reaction. But, well, I never had mechanics in English, so I don't know about proper terms.
 
I don't either
 
@0celo7 I'm uncertain. If I was writing a question of that kind I would either want the whole normal force acting on the thrower or would ask explicitly about the change of the normal force acting on the thrower.
Unfortunately I don't know that the language there is universally understood to have a unique meaning.
 
@dmckee someone asked one of the profs on Blackboard and he clarified as normal force
@ACuriousMind are all linear transformations invertible?
mapping from n dimensions to n
 
12:55 AM
What have you tried in finding the answer to that question? :P
Because there is a completely equivalent question I'm quite sure you know the answer to
 
uh
I don't really know how to approach it
I told you, my linear algebra class is a joke
 
Do you know that there is a bijection between linear maps $\mathbb{R}^n\to\mathbb{R}^m$ and $n\times m$ matrices?
I.e. every matrix defines a linear map and every kinear map has a matrix?
 
yes, yes, of course
that we did cover
 
Are all $n\times n$ matrices invertible?
 
::smashes head against keyboard::
uh, just forget I asked that
 
12:58 AM
Told you you knew the answer :P
 
ok, so in the "all inner product spaces are isomorphic" proof
we set $\phi(e_i)$ equal to the vector in R^n with 1 in the ith slot, right?
how does one show that $\phi$ has an inverse
 
You, uh, just define it in the same manner?
 
what guarantees that the matrix of $\phi$ is invertible
 
@0celo7 Why are you worrying about that? Just define the inverse $\psi$ by $\psi(x_i) = e_i$, where I denoted by $x_i$ the vector with a one in the ith slot.
Now it's evident that $\psi\circ\phi$ and $\phi\circ\psi$ are both the identites, and thus $\phi$ is an isomorphism.
 
I just am!
 
1:09 AM
@0celo7 Well then, strictly speaking, you don't have the notion of "invertible matrix" since the map is not from a vector space to itself.
And the "matrix" of $\phi$ is rather silly: In the natural way to write it down, it looks like the identity matrix (but it isn't, because it's between different spaces).
 
alright, I get it
all inner product spaces are isomorphic, proof recorded in the holy notebook
what should I write down next?
ah, the unitary matrix thing
@ACuriousMind So I tried checking what matrix commutes with the complex structure
and I found it's just GL(n,R)
I think
I commuted a matrix with four blocks ABCD with the complex stucture and got A=B=D=-C
so that's one block dof, so unless the blocks are complex I got GL(n,R)
Oct 21 at 16:00, by ACuriousMind
As for why those are those are those who preserve the complex structure, just write the complex structure as $\left(\begin{matrix}0 & -E_n \\ E_n & 0\end{matrix}\right)$ and just examine which block matrices $\left(\begin{matrix} A & B \\ C & D\end{matrix}\right)$ with $A,B,C,D\in\mathrm{GL}(n,\mathbb{R})$ commute with it.
 
1:30 AM
@0celo7 I get $B=-C$ and $A=D$, so two $\mathrm{GL}(n,\mathbb{R})$ matrices.
 
...
how did I get D=-C?
that's not even what I have written in my matrices?
smh
see what I mean D:
@ACuriousMind other problem, why do these have to be GL(n,R)?
isn't GL(n,R) invertible? it has to be by defintion of a group
 
it is
 
but I see no reason why A,B have to be invertible
 
@0celo7 Yes. Non-invertible matrices have no chance of preserving the structure
 
@ACuriousMind ok, why?
@ACuriousMind the hermitian inner product defined under that exercise is not antilinear in one of its arguments, is that an issue?
 
1:53 AM
@0celo7 Uh. Thinking about it, we're actually only interested in the group of matrices preserving the structure. Sorry, of course non-invertible matrices can commute with the structure.
 
@ACuriousMind ok, I figured something like that
 
@0celo7 Why would it be an issue?
 
the unitary group preserves a Hermitian inner product
the one he defines isn't a hermitian inner product
it's not antilinear in an argument
 
Is it linear in that argument?
 
it's linear in both
@ACuriousMind I can't get this to work with that antilinearity in the "standard" inner product!
@ACuriousMind yeah, I'm having trouble with this proof :(
 
2:12 AM
@0celo7 Did you remember that the complex scalar multiplication is defined as $(a+b\mathrm{i})x = ax + bJx$ for $J$ the complex structure?
 
complex structure outta nowhere
uh, I did not
first I'll prove "all unitary groups are isomorphic"
then do that one
notation should be obvious: $$\langle x,y\rangle_V=\langle U_V,x,U_Vy\rangle_V=\langle\phi U_Vx,\phi U_Vy\rangle_W=\langle U_W\phi x,U_W\phi y\rangle_W$$
$\phi:V\to W$ was proven to exist earlier this evening
@ACuriousMind make sense?
so $U_V=\phi^{-1}U_W\phi$
 
in Mathematics, 8 mins ago, by Martin Sleziak
We are currently mitigating an attack. Standby for updates.
 
@ACuriousMind sorry, I don't see how that helps
my proof of "all unitary groups are isomorphic" never uses the properties of unitarity, antilinearity or hermiticity
 
@0celo7 Write the Hermitian product as $y^T x + \mathrm{i} y^T J x$. Now using $(a+b\mathrm{i})x = ax + bJx$ and $J^T = -J$, you can show it's antilinear in the first and linear in the second argument.
Also: We are under ATTACK?!
2
 
@ACuriousMind ok
 
2:23 AM
@ACuriousMind Yeah.
Happens all the time.
 
that's not clear at all from the defintion though
wait, if $Jx=\mathrm{i}x$, then $y^Tx-y^Tx=0$ o.o
 
@DanielSank First time I hear of it
 
@ACuriousMind I mean, websites are attacked all the time.
 
@0celo7 No, you are not allowed to do that. In $\mathrm{i}y^T J x$, the $y^T,J,x$ are treated as a real matrix and as real vectors. Inside that formula, complex scalar multiplication is not defined.
 
o...k, so not sure what to do now
also my unitary isomorphic proof is flawed somewhere
I think...
I never use any of the properties of the complex inner product in the proof
all I use is the general invariance group defintion
 
2:29 AM
@DanielSank Hm, I guess so. Didn't notice anything odd on the site, though
@0celo7 That's because the same proof works to show that all groups that preserve the same kind of inner product are isomorphic, e.g. it also shows all orthogonal groups are the same.
 
> it also shows all orthogonal groups are the same
yes, that's true
 
(of the same dimension)
 
@ACuriousMind that's implied
so, about this antilinear thing
 
in English Language & Usage, 4 mins ago, by cornbread ninja 麵包忍者
We are back online and monitoring all systems.
 
@ACuriousMind ok, I need a bigger hint for this problem
I'm not sure what I can and can't do now
 
2:43 AM
Just compute $\langle (ax+bJx,y) \rangle$ and $\langle x,ay+bJy\rangle$ where $\langle -,-\rangle$ is the Hermitian product.
 
NO
I WAS DOING THAT
DON'T HELP ME
;_;
I'm a confused kid
 
You, uh, told me you needed a bigger hint?
 
@ACuriousMind I know, but I had figured it out
now the victory is less good
actually I got antilinear in the second
ok, after a bit of derping I figured it out
 
As usual, then ;)
 
$\langle x,y\rangle =(x,y)+\mathrm{i}[x,y]$. $\langle \eta x,\beta y\rangle=\eta\bar\beta\langle x,y\rangle$
You agree?
 
2:55 AM
yes
 
but...
you said antilinear in the first
that was my derping
 
It, uh, doesn't matter in which it is antilinear
 
;_; I spent so long trying to reproduce your result
@ACuriousMind I'm flipping through problems in Arnold
"find 1-forms on the plane that are not differentials of any function"
I thought the plane had trivial cohomology
 
I can't read :)
thought it said closed
 
3:18 AM
@ACuriousMind how exacly is the limit on the top of page 81 chart independent?
 
@0celo7 The "prove this!" there is meant to say you should figure that out yourself :P
 
@ACuriousMind honestly, I've tried
I don't see what property of charts is needed
 
That they're diffeomorphisms.
 
ok, so the charts are diffeomorphisms between the domains
is $\phi$ the image of a curve in $M$ under a chart?
 
Yes.
 
3:27 AM
well, no
it says on the previous page near the bottom $\phi(t)\in M$
 
@0celo7 On the previous page, $M$ is embedded. Here it is not, hence the need for a chart.
 
ah
ok, notation
$\phi$ is the curve
chart is $h$, other chart is $h'$
ugh no clue what to do :/
@ACuriousMind I don't see what diffeomorphism has to do with anything
 
3:51 AM
@ACuriousMind are the charts somehow linear or something?
I'm completely lost
 
4:06 AM
@0celo7 Observe that $\lim_{t\to 0}\frac{(h\circ \phi)(t)-(h\circ \psi)(t)}{t} = (h\circ \phi)'(t)-(h\circ \psi)'(t)$ and the use the chain rule for $(h'\circ \phi)' = (h'\circ h^{-1}\circ h\circ \phi)'$
(where primes except for the one on $h'$ denote usual differentiation)
 
ok, I figured out I need to get the equation after "observe that"
but I don't see how I get it
 
$0 =t-t$
 
o.o
what
 
Add $+t-t$ to the numerator.
 
I know that's what you meant
I still don't see it
 
4:10 AM
You do realize that $(h\circ \phi)'(0)$ is defined as $\lim_{t\to 0}\frac{(h\circ \phi)(t) - t}{t}$?
 
@ACuriousMind no
 
But that is the definition of a derivative!
 
@ACuriousMind huh?
I don't see how that is of the form $[f(x)-f(0)]/x$
 
No, wait :D
Godamnit, why it Arnold define this so weirdly
 
Russian
 
4:12 AM
If he had just taken the equality of the derivatives as the definition instead of that limit, it'd be so much easier.
 
:)
I have 5 books here that do it that way lol
Arnold is the ugly duckling
 
Well, we can always throw the towel and just Taylor expand
 
D:
HERESY
this isn't physics, taylor expansions are forbidden
@ACuriousMind ok, then what?
 
No, it's rigorously allowed.
 
are chart transtitions just linear maps on vectors?
@ACuriousMind is that it? just taylor expand?
 
4:21 AM
We Taylor expand $f := h'\circ h = f(h(\phi(0))) + Df(h(\phi(0))(h(\phi(t))-h(\phi(0)) + r(h(\phi(t))(h(\phi(t))-h(\phi(0))$ where $\lim_{t\to 0} r(h(\phi(t))) = 0$ by Taylor's theorem.
 
lol screw that
 
Hm, few brackets missing. Anyway, doing that carefully yields the chart independence for Arnold's weird definition, since a bunch of terms drop out due to $\phi(0) = \psi(0)$ and the Jacobian $Df$ is linear
 
aight
thanks pal, will look at it in physics lecture tomorrow
@ACuriousMind shouldn't you be asleep?
is this a record?
 
What? No, this is quite far from a record :P
In autumn/winter the sun comes up much later to remind me to go to sleep :D
 
you're a daemon
dude, your sleep schedule is identical to mine and we live 6 hours apart :D
diff eq test on Tuesday is gonna suck
Variation of crap and Laplace transforms and reduction of order
and pursuit curves isogonal trajectories
gulp this might be pretty tough
@ACuriousMind I'm off, I still have a reflection ;P
 
4:31 AM
g'night
 
4:52 AM
@0celo7 What have you learned in college so far?
 
5:43 AM
He's learned that Mathematics is more of an obstacle than a tool at this point.
 
 
3 hours later…
8:38 AM
Soon he will learn the evils of mathematics and become a real physicist
 
8:57 AM
0
Q: Why is the main page of PSE looking so weird in my Opera browser?

user36790Pictures would say better: Then this; notice a large bar in the right part of the page; the conspicuous part is the appearance of hot questions at the bottom: What is going on? I'm using Opera 30.0.1835.88; I then checked the Chem.SE page It can be easily seen the ads are at their prop...

 
 
2 hours later…
10:52 AM
!@#$/^ Google it — Joel 14 hours ago
lol hemad
 
 
2 hours later…
12:30 PM
@DanielSank What?
 
He's asking about the big picture.
The so called view of the forest, not the trees :-)
 
12:57 PM
@user685252 Uh, I'm way too lazy to do anything with my life ;_;
 
1:13 PM
Well then, you will be pushed aside by those who are not.
aka survival of the most competitive @0celo7
 
1:51 PM
Seriously, while being smart will let you skate though (roughly) undergrad, after that brains alone won't carry you: diligence trumps them regularly in grad-school and the work place. (Honest geniuses get a little bit of a break, but the merely very smart get no such consideration.)
3
 
@dmckee I'm diligent when something challenges me
Y'all have seen, I've done a lot of work to teach myself stuff, but that stuff was interesting.
 
2:14 PM
@ACuriousMind lol
@ACuriousMind Ok, we might have to revisit the Galilean thing. I've managed to confuse myself again by reading what I wrote in the past D:
My past self confused my present self, lol
 
Is there a way to search one's favourited questions, and only those?
 
The starred ones?
 
Yep
I mean, I'm favouriting mainly questions I want to refer to later, and it is kinda annoying to scroll through the list searching for them when I want to do that
 
2:31 PM
There is a "favourites" option.
 
@ACuriousMind infavorites:mine
 
You have 57
 
He doesn't want to scroll through all 57
Talk about lazy :P
 
@Loong Thanks
@0celo7 That's already three pages - that is inefficient to scroll through when I know the exact keyword I'm looking for
Also, I figured there must be a way otherwise I would have no idea why Qmechanic favourites so many things
 
And solving quadratic equations is inefficient as well :)
 
2:37 PM
66
Q: The Role of Rigor

Gil KalaiThe purpose of this question is to ask about the role of mathematical rigor in physics. In order to formulate a question that can be answered, and not just discussed, I divided this large issue into five specific questions. 1) What are the most important and the oldest insights (notions, results...

Now that^ is worth following
:-)
 
@ACuriousMind What is $r$?
 
@0celo7 Some function that goes to zero like that. There a explicit formulae for the Taylor error term, but they're not needed here.
I also realized we can do this an easier way:
 
@ACuriousMind Oh the error! Silly me.
 
Just add $h(\phi(0))-h(\psi(0))$ to the original statement to get that it's just the difference between to derivatives. This works since $\phi(0)=\psi(0)$
Then what I originally wanted to do with $+t-t$ works.
 
Uh how is $h(\phi(0))$ defined? I thought $\phi$ was in $R^n$.
 
2:40 PM
Hm
I want to ask a question
 
I thought $\phi$ is the image of some $\gamma:I\to M$ under $h$.
 
But that would mean typing it on my phone currently
 
here or main site?
 
@0celo7 Oh, yeah, I chose to interpret $\phi$ as the curve and denote what Arnold writes $\phi$ as $h\circ \phi$ Call it whatever you want
 
@ACuriousMind great
make the shitty notation more complicated :)
 
2:42 PM
Main site
 
@Slereah What phone?
 
Wouldn't want to ask it here, it's a PHYSICS question!
Not math :p
 
lel
I'm going through the exercises in Arnold
don't worry, physics will be in there
@ACuriousMind difference between two derivatives?
in the limit or something?
 
@0celo7 Remember that the chain rule gives the chart independence once we know that Arnold's $\lim_{t\to 0}\frac{\phi(t)-\psi(t)}{t}$ is the same as $\phi'(t)-\psi'(t) = 0$?
 
6 hours ago, by Slereah
Soon he will learn the evils of mathematics and become a real physicist
 
2:45 PM
Right, oh oh you want to add $-\phi(0)+\psi(0)=0$?
 
@0celo7 Yes
@user685252 Nooooooooooooooooooooooooo
 
ahhhhhh
@user685252 I'm not even a physics student ffs
although a decent part of my department are physics people
 
and the grad students in my group are scared of engineering
 
It is your destiny
 
2:46 PM
I'd be perfectly happy doing physics one day, as long as it...
but I'm also considering some applied math stuff
but that's a long way out
@ACuriousMind Wait you want me to be a mathematician?
 
I want everyone to be more of a mathematician :P
 
@ACuriousMind stupid time: why can we separate the limits?
generally $\lim (f+g)\ne \lim f+\lim g$, right?
so why can we do it here
 
@0celo7 False.
Limits are linear.
 
AH
if each one is finite
nevermind :)
that's the condition, right?
 
The sum of two real numbers is also a real number, says the mathematician :P
 
2:55 PM
@ACuriousMind ok, but evaluated at $t=0$
now the chain rule...
 
@0celo7 Yes
 
@ACuriousMind should that be like $f(\phi)$?
 
@0celo7 Don't look at my Taylor expansion, just use the chain rule!
 
where!
what is the chain rule!
Is the chain rule real if our eyes aren't real!
I just want to write $\phi(t)=\phi(0)+v_\phi(0)t+O(t^2)$
but that's not what you want
 
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