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4:00 AM
Well that was an interesting touchdown
 
Who's playing?
 
Packers at Cardinals
 
the Murrica Freedoms
 
@DanielSank Do you want me to give a justification for the usefulness of linear maps in physics
 
4:03 AM
@0celo7 Uh, no.
 
*multilinear
Hmm, I thought you said something like that earlier
 
I think it's important to point out that there are lot of coordinate independent objects in physics.
It's good to start there.
Here's an example:
$\ddot{\phi}(t) + 2\beta \dot{\phi}(t) + \omega_0^2 \phi(t) = J(t)$
That's an equation of a forced damped oscillator right?
But we can rewrite it like this:
 
Seems like it
 
$\langle t | D^2 + 2 \beta D + \omega_0^2 | \phi \rangle = \langle t | J \rangle$
And then:
$(D^2 + 2 \beta D + \omega_0^2) | \phi \rangle = |J \rangle$
 
wat
 
4:06 AM
What part do you not understand?
Help me help you.
$D$ means time derivative.
 
@0celo7: Pick a decomposition into increasing, compact submanifolds with boundary. Progressively define a nonvanishing vector field on each except possibly vanishing on the boundary. At each next stage modify the previous one only near the boundary. Take a limit. Eventually zeroes are "pushed off to infinity".
 
@DanielSank I have no idea what you're trying to tell me/us
 
chat decided to turn the ping noise back on and deafen me
@DanielSank I understand that
 
@ACuriousMind I'm trying to point out that there are a lot of equations we write down which can be understood in a coordinate independent way.
 
@MikeMiller O...k.
 
4:08 AM
Once you do that, it's easy to understand that equations like the first one I wrote are special cases expressed in a particular coordinate system.
 
You asked for the idea.
 
But everything's easier with coordinates.
 
From there it's much easier to understand that what a physicist calls a tensor is really a representation in a particular basis of what a mathematician calls a tensor.
 
@DanielSank Taking a read on that README and some documentation I found for RPC
 
@DanielSank Uh. How is the first equation "coordinate dependent"?
 
4:09 AM
@ACuriousMind It's not. The third one is.
 
@MikeMiller I know
 
@DanielSank Well, in the second and the third I'm not sure what $\langle t \vert$ or $\lvert \phi\rangle$ are supposed to be
 
@ACuriousMind Really?
$|\phi\rangle$ is the state of the oscillator.
$|t\rangle$ is a time basis state.
i.e. $\langle t | \omega \rangle = \exp( i \omega t)$.
 
@DanielSank ??? There is no time operator and no time eigenstates
 
@ACuriousMind This is not quantum mechanics.
This is linear algebra.
 
4:12 AM
@DanielSank I'm not following you
 
@ACuriousMind oye
 
What is the vector space?
 
@ACuriousMind The possible trajectories of the oscillator.
$\phi(t)$ is a particular trajectory expressed in the time basis.
 
@DanielSank That's not a vector space. What is the sum of two trajectories?
 
4:13 AM
Of course it's a vector space.
 
Twojectories
 
@ACuriousMind you can add functions together can't you?
 
@FenderLesPaul well played
 
@DanielSank But that requires a choice of origin.
 
@KyleKanos takes bow
 
4:14 AM
@ACuriousMind Hence: coordinates are better
QED
 
@ACuriousMind I don't understand. The function $\phi(t)=0$ is the zero element.
What are you on about?
$D$ is obviously a linear operator on this vector space.
$\langle t | D |f + g \rangle = f'(t) + g'(t)$.
 
Hmm. Physics probably should just be taught entirely using bra-ket notation linear algebra
3
 
@KyleKanos YES!
I actually wrote a book doing this.
It's so close to being ready to release.
 
.....link pls
 
@DanielSank Hm. Okay, I meant that you cannot in general add two trajectories. I didn't realize that part is specific to the oscillator already
 
4:17 AM
@KyleKanos Not yet.
I need to spend a weekend on it.
It's soooo close.
 
Well email me when it's ready
 
@KyleKanos Ok!
 
Because I will read the shit out of that
 
@DanielSank so an RPC is like a function call where you delegate the function's processing to another machine over a network? Is it necessarily synchronous?
 
@KyleKanos I explain the following thigs:
 
4:18 AM
@DanielSank Okay, so your vector space is the space of smooth functions. I could quibble about the $\langle t \rvert$, but I'll leave that be. How is now that notation "less coordinate invariant" than the $\phi(t)$?
 
quibble away
 
1. A lot of problems can be expressed without a particular choice of basis. This is because integration and derivatives are linear operators.
2. E&M, linear mechanics problems (like the oscillator) and quantum are examples.
3. Matrices are representations of linear operators in particular bases.
4. Change of basis.
5. Greens functions are really simple if you think of things in this way.
@BernardMeurer You're right about the first part, but definitely not synchronous.
Trying to make that look synchronous is why a lot of RPC systems fail.
 
@DanielSank I was confused about what you want me to do...
I agree I should maybe start out simple...
 
@DanielSank So while the function is being run by the networked PC the client can still continue it's runtime processing and wait for the function return?
 
@ACuriousMind $(D^2 + 2 \beta D + \omega_0^2)|\phi \rangle = |J\rangle$ is more coordinate independent than $\ddot{\phi}(t) + 2 \beta \dot{\phi}(t) + \omega_0^2 \phi(t) = J(t)$.
Don't you think?
 
4:21 AM
guys help
 
@BernardMeurer Yes.
 
I can definitely see the use of this in quantum computing
 
I can't stop looking at random threads in biology SE
it's been like two hours
 
@BernardMeurer It's useful for a lot of things.
 
First, I do not know, apart from figuring out if the qutip package is messed up, how modeling a two level system helps...But I knew that you were trying to help me, so I was going to do it...
 
4:22 AM
@FenderLesPaul Sounds like you found a new interest!
 
@FenderLesPaul good!
You are entrapped in my community!
 
this is a trapped horizon I am not familiar with
:p
 
@TanMath Did you ignore the part where @dmckee specifically told you that n00bs always think they've found a problem with software packages and they're always wrong?
It's like you're not even reading the things people are telling you.
 
@DanielSank I did not...
 
Ok, then in that case erase from your mind the notion that qtip is messed up.
 
4:23 AM
I know that I couldn't have possibly found an error in the package...
@DanielSank I did not say that it isn't messed up...
 
@TanMath It's possible, it's just much less likely than there being an error in your code.
 
@DanielSank No. Because you have the space of functions in one variable. Writing them as $\lvert \phi \rangle$ or $\phi(t)$ makes me prefer $\phi(t)$ because I'm trained to think of $\lvert\phi \rangle$ for some abstract vector in a space about which I don't have information such as "functions in one variable".
 
I said that modeling a two level system could show that the qutip package is messed up, but it is not necessarily messed up...
@FenderLesPaul so far, what is your favorite thread?
 
@ACuriousMind Ok, look, suppose I have an $n$ dimensional space over $\mathbb{R}$.
 
OOMGOMGOMGOMGOMGOMGOMGOMGOMGOMG
 
4:26 AM
Actually, @ACuriousMind, here's a great example for you.
 
Rodgers just scored another Hail Mary TD
 
Consider the set of arrows in the 2D plane.
These for a vector space, right?
(say "right" and then I'll go on)
 
right
(given an origin)
 
@KyleKanos you certainly love sports...do you realize this is a physics chatroom? :p
 
Ok, now if I pick two coordinate axes, I can represent these arrows as pairs of numbers.
 
4:27 AM
@TanMath I found two I've really liked so far
 
So, you might want to say that this vector space is just $\mathbb{R}^2$.
But it's not quite.
 
@TanMath Yes, I'm just like many other normal Americans
 
I can choose a different set of axes, and when I do that the same arrow gets a different pair of real numbers.
 
And while this is a physics chat room, there is absolutely no requirement that every line actually be about physics
 
4:27 AM
@DanielSank Remote function calls sounds awesome, never touched this before; exciting!
 
@DanielSank I'm familiar with that :P
 
The number pairs are representations in a particular basis of the more abstract vector space of arrows.
@ACuriousMind Right, so the functions $\phi(t)$ are representations of something more general.
 
@FenderLesPaul I like this one too...
 
For example, I can express $|\phi\rangle$ in a different basis.
@ACuriousMind observe:
 
Don't go Fourier transform on me
 
4:29 AM
lol
 
$\langle \omega | \phi \rangle = \int dt \, \langle \omega | t \rangle \langle t | \phi \rangle = \int dt \, e^{-i \omega t} \phi(t)$.
@ACuriousMind Why not?
It's exactly the right way to think about Fourier transforms.
 
Hmm, I wonder if those should be \equiv's there
 
Of course, $\int dt \, | t \rangle \langle t |$ is the identity, as you expect.
 
What are you talking about?
 
@BernardMeurer Oh yeah, it's actually rather fascinating.
 
4:30 AM
@DanielSank reading this article on it
 
@DanielSank Did you get that from Shankar
 
I spent hours convinced I'd found a problem in GNU's implementation of atan2. Turns out I was (a) supplying the arguments in the wrong order and (b) supplying them in degrees rather than radians at the same time.
 
You have to think about how to take a sequence of bytes from the network, which is totally without type information, and turn that into a well typed object in your language of choice.
@dmckee hahahahahaha nice
 
@DanielSank how is that defined
 
@dmckee (a) is the worst
 
4:31 AM
@0celo7 No.
 
@DanielSank Because that's not a coordinate change. "Momentum" is not a coordinate on space time, while position is.
 
@FenderLesPaul I had this question in my mind so I asked a biology.SE question:
24
Q: Hot water and bacteria

TanMathI know that it is common to say, "use hot water when washing your hands" or when you've got a cut, "wash your hands with warm water," etc. I was wondering, why is this the case? Since bacteria grow in warm environments, you would think that it might be beneficial for bacteria. Is this just anothe...

 
@ACuriousMind wtf
Who said anything about relativity?
 
@dmckee lol
 
Why the hell do you guys always complicate simple stuff by going straight to relativity?
 
4:32 AM
@KyleKanos Yep. I must have looked at the prototype twenty or thrity times, but I kep seeing what I expected instead of what was there.
 
It's so frustrating.
 
I have a feeling we can't have a discussion for five minutes until someone throws in the relativity card and the other party in the conversation gets sad
 
@DanielSank relativity is complicated...
 
@DanielSank ...what has momentum being the Fourier transform of position to do with relativity?
 
@ACuriousMind You said spacetime.
 
4:32 AM
What is the discussion about? Fourier transform?
 
Why did you say space time?
 
Uh...habit?
 
@TanMath Read the chat log for heaven's sake.
 
@TanMath yeah I saw that
 
Well relativity is wrong, so we probably should just drop it from curricula
 
4:33 AM
@KyleKanos wat?
 
I liked your answer to the question about why yellow/black
 
Oh god @KyleKanos don't go there
 
is used for danger signs
 
@FenderLesPaul thanks..
 
Anyway, "spacetime" was not essential there, just replace it by "space"
 
4:33 AM
Mmmm, curly fries
 
sweet potato fries > all
 
@ACuriousMind Ok whatever. How can you possibly not think a Fourier transform is a basis change?
 
That looks like octopus
 
@DanielSank cause he's a boss ass bitch
son
 
daughter
 
4:34 AM
 
let's not be gender exclusive
 
That's fried octopus
 
Ok @ACuriousMind, what if we work with a finite discrete set of time samples, and then use a discrete Fourier transform to produce a new set of samples? I can represent that as a matrix acting on a set of numbers. Would you consider that a basis change?
 
@KyleKanos ew...
 
@FenderLesPaul I exclude whatver crappy genders I want
 
4:35 AM
@TanMath Don't knock it without trying it
 
@KyleKanos :( :( :( :(
 
@DanielSank Oh, it's a basis change alright. Just not a coordinate change, but I get now that you didn't mean with "coordinate change" what I had in mind.
 
@DanielSank I think @KyleKanos is threatning
 
I thought we were talking about shit on manifolds
 
@ACuriousMind Sheesh ok I meant basis change.
 
4:35 AM
@0celo7 you discriminator!
 
@0celo7 We're getting to that.
 
@TanMath guilty as charged
 
Abuse
 
::spanks::
 
^ for you!
 
4:36 AM
I was doing something
 
Anyway, we've established that there are coodinate independent things in very simple situations, and we've even shown a nice notation for it, and we showed an example of a basis transformation.
 
then I was interrupted by Battlefield 4
 
@DanielSank They offered octopus at the Greek restaurant I went to tonight...I'm curious about my son's will to try it
He really loves octopuses
 
@DanielSank I'm sorry I wasted some of your nice explanations :)
 
now I can't remember what I was doing
 
4:37 AM
(octopi?)
 
@KyleKanos Like, he likes them alive?
 
@DanielSank Yes
 
Well then, there is no reason for me to stay here... @DanielSank anything else you want to say? Are you busy talking to @ACuriousMind?
 
But he also loves eating
Dude, he's 6
 
@KyleKanos How old is he? I have a book about them of which I came into possession of a duplicate copy. I'll send it to you if you want it.
 
4:37 AM
Oh god @0celo7
 
@KyleKanos octopi is common (from the Latin version), but the original Greek has octopodes
 
@TanMath Try a 2 level system.
@ACuriousMind Yes, and in modern Greek it's more like octopodia.
 
heck try a 1 level system
 
@DanielSank like I just model a two level system? that is it?
 
^ LOL
 
@TanMath Yeah, try Rabi oscillations or something to convince yourself you're using qutip right.
 
@FenderLesPaul Never heard of that before! You might have inspired a new research area
 
Then add dissipation or something.
 
I just love this
 
Well, Cardinals just won in overtime, so I'm going to head to bed now
 
4:39 AM
@DanielSank I am convinced I am using it right...I will do a two level system then...then I come back to you? what is the next step?
@KyleKanos they did?
score?
 
Yes, that's why I wrote it...26-20
 
@TanMath Just do that.
 
Oh...
Ok...I will tell you when I will done... I will probably get it done late night today...
 
@KyleKanos night brewski
 
@KyleKanos gud night!
 
4:41 AM
Anyway @0celo7 @ACuriousMind my point here is that you can show some object to have meaning independent of it's representation via components. The curvature tensor, for example, has a very simple meaning which can be expressed without components.
 
@BernardMeurer What?
 
@TanMath so are you a student in the US or...?
 
You're never too young
for that kind of stuff
 
My goodness
 
One can then introduce what you guys call "algebraic tensors", again without components.
 
4:41 AM
What meaning does the curvature tensor have
 
Finally, one chooses a coordinate system and shows that the tensor can be expressed in terms of various basis tensors, i.e. with components. Then you show that these components have various transformation properties. Sets of numbers obeying those transformation properties are, sadly, what physicists call a "tensor".
This order of development makes it waaaaaaay easier to reason about tensors and do physics.
@0celo7 Ok let's go through this slowly.
How many "slots" does the curvature tensor have?
 
I probably know what you're going to say, but let's do it anyway
 
@0celo7 If you know then why ask?
 
@DanielSank How are you defining it
 
@0celo7 Like, what rank tensor is it?
 
4:44 AM
4
 
Correct.
 
woo
 
That means that if I feed it three vectors (or covectors, I won't distinguish for now) I get back what?
 
looks like multiple books on diff geo have served me well
 
@0celo7 you seem like the kind of guy that would frequent 4chan
 
4:44 AM
@FenderLesPaul Uh, I do.
 
@FenderLesPaul Yikes.
 
I don't make that a secret.
 
can't argue with that
 
@0celo7 come on I ain't got all day.
 
@DanielSank a vector
 
4:45 AM
@0celo7 Correct.
The curvature tensor takes three inputs:
 
ok that's a little condescending
 
First you give it a vector $v$.
 
I know what the curvature tensor is
 
oh, but you asked...
 
get to the point
 
4:46 AM
Don't be like that, I'm aswering your question.
 
@FenderLesPaul Although I've been significantly cutting back lately. I have to make an extra effort to remember to browse.
 
You give it a vector $v$ and then you pick an infinitesimally small parallelogram. That parallelogram is specified by two more vectors which define two of the sides if you see what I mean.
You feed these three things into the curvature tensor.
The output vector is the result of parallel transporting $v$ around that parallelogram.
 
@0celo7 can't cut back man
 
@0celo7 ok?
 
/b is good for your mental health, or so I've been told
 
4:48 AM
@DanielSank ok, I knew exactly what you were going to say
That's literally in every GR book.
 
@0celo7 ok....
Yeah...
But you asked for a geometric picture... if you knew it why ask?
 
Although the better answer is that the Riemann curvature is really the unique generalization of the Gaussian curvature to more than 2 dimensions.
 
@0celo7 Riiiight that's so much better that I have no idea what it means.
 
@DanielSank Use the Gauss theorem for an isometric immersion $M^2\to\mathbb{R}^3$
You can see that the Riemann curvature reduces to Gauss in this case
And the Riemann tensor is the unique tensor of second order in the metric derivatives
@DanielSank (sadly I don't get what the point of that was)
I would NEVER advocate for defining the Riemann tensor as $R^i{}_{jkl}=\partial_j\Gamma^i{}_{kl}\cdots$
 
user54412
I don't suppose anyone from this chat will be in the bay area next week?
 
user54412
5:00 AM
I have this bizarre goal of meeting as many internet people as possible in real life.
 
@ChrisWhite not next week sadly
I'm getting to SF on around the 12th of February
 
5:31 AM
@ChrisWhite come to Ithaca!
 
@BernardMeurer Still around?
 
@ChrisWhite I've actually made it a mission to go to all the astro lunches this coming semester
as someone interested in GR research I've realized I know next to nothing about actual theoretical astrophysics
so I'm trying to ameliorate that
damn there are so many things in science I know nothing about
le sigh
 
all they do is look at stars
 
goes back to biology SE
stars are dope
 
If you're interested in this whole RPC thingy I'd be happy to learn with you. I'd like to get something written in Scala and python (if you understand how to do it in both a statically and dynamically typed language, you understand it, eh?), and then use it in some projects.
Actually, in the end I may just write code to implement cap'nProto's RPC system (not the encoding) in Scala (it's already done in python) but learning the basics first is usually a good idea.
 
5:35 AM
@0celo7 also I've noticed that lunches for almost every physics subfield are more interesting than the ones in the department I work in
i.e. particle physics
especially since particle physics lunches are almost always pheno talks
which are sooo boring
 
@ChrisWhite Awww I thought I was your only one.
Such a player.
 
"Fraternal twin higgs model with adopted sibling particles and a dad particle who was left at an early age"
by dude from IAS
 
5:51 AM
man
people in bio SE cite waaaay more than people in physics SE
one of the advantages of a subject that is inherently mathematical I suppose
 

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