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18:04
@yuggib My algebra book proves the first statement.
@0celo7 the converse should not be so difficult
but I never thought about it
@yuggib Oh I misread. It proves induction given the WOP.
So really it proves the second statement.
ok
induction $\Rightarrow$ WOP I don't know if it's easy
@yuggib Yeah, remember that theorem I cited about induction? The proof is pretty much "use WOP and this other lemma."
Converse...no clue.
set theory goes definitely from WOP to induction
18:11
I wouldn't be able to come up with $\Rightarrow$ on my own, much less $\Leftarrow$.
Er.
Other way around.
Hello @0celo7
@privetDruzia Hello.
Hello @Danu, @ACuriousMind
I have a short question
which is quite easy
if u don't mind?
Just ask away---I won't guarantee that I'll help you though!
Just ask it, someone will answer if they can/want.
18:19
well my question is in this comment
Please provide a reference (link) for your graphs. I think they're about inter-nuclear energy in a molecule. — Gert 3 hours ago
wait I can't post a link, the title of the post is: "Why is the potential energy minimal when the repulsion and attraction force between molecules is 0?"
the 3 comments below the omly answer
Have you seen this formula before? $F=-\nabla V$?
never
I know what it means
never? you haven't taken a calculus based physics class?
but I can't understand that this is correct. Applying the nabla operator on a scalar field of potential energy points
@privetDruzia Any idea why it's true?
18:24
returns a vector, which appearantly in my case might be the intermolecular force
@privetDruzia oh
but yes thatts the problem, I can't see why this is true
Think physically
that's the worst way to think
If you are pushing an object and it takes you energy (don't think about friction for now)
You are essentially putting energy into it
18:26
such intuition
What kind of energy? Well, that depends on the type of thing that's causing it to cost you energy.
As an example, think about lifting an object on Earth.
It takes some force: But why?
do you even lift bro?
You're increasing its potential energy
And the amount of force it takes is exactly the rate at which you're increasing its (potential) energy
(here I'm always considering "infinitely slow processes" so that the kinetic energy plays no role)
In equations, that's just $F=\frac{\mathrm d V}{\mathrm d h}$ where $h$ is the height
In this one-dimensional problem, this is of course equal to the gradient.
18:28
OK but, so if you are lifting it very high, the potential is high and the force is high
No
so no derivative/gradient so far
Be careful
If you're lifting it here or on Mount Everest, the force should be the same (ignoring variation of the gravitational potential, for now, since mountains are small compared to the radius of Earth)
Don't you agree?
Okay, so the amount of force doesn't really depend on the height
18:31
so the faster you want to lift something the more force
doesn't seem as a derivative yet I think
Let me think for a little bit on how to put this more clearly.
@Danu $F=mg$. I don't see where it depends on "how fast"
@0celo7 I know :D I messed up because I wanted to ignore kinetic energy, but then didn't.
@Danu Let me take a shot?
18:32
plz
yes
In any case, we've established that adding an arbitrary constant to the potential does not affect the force.
while he s thinking
That's already a good start, since that's something derivatives also do.
@privetDruzia Are you willing to accept that the total energy (kinetic + potential) is constant in time?
Yeah, I guess you can do it that way ^
18:34
if its constant the derivative is 0
...hmm ok why not let s try
Of course you can just think about particular examples
Yes. Are you also willing to accept (1) $F=ma$ and (2) $E(x,v)=\frac{1}{2}mv^2+V(x)$?
e.g. a free particle which is not affected by any potnetial has constant velocity (i.e. $F=0$)
The latter being the constant energy.
@BernardMeurer Hello again.
18:35
@privetDruzia Then $dE/dt=mva+V'(x)v=0$.
This implies $V'(x)=-ma=-F$
For more than one dimension it works similarly.
If a force acting on an object is a function of position only, it is said to be a conservative force, and it can be represented by a potential energy function which for a one-dimensional case satisfies the derivative condition
?
Yes.
@privetDruzia This is basically what Ocelot just showed you
$V(x)$ is an assumption
mhm
but writing it as: $F = \grad{U}$ or $dU/dt = F$
what s the difference
Uh, $dU/dt$ is not $F$
$dU/dt=\nabla U\cdot v$
chain rule
18:39
times V?
Dot product with $v=dx/dt$.
what is v? The potential energy? Isn;'t that U?
Small v is velocity.
Potential energy is capital U.
ow ok, but does velocity in my case really matter?
i.ie intermolecular forces
Intermolecular forces are radial, right? So I think they're conservative.
18:42
ok so v doens't matter
It does matter in the derivation.
(if they are indeed radial)
Where are you concerned about them mattering?
@Danu I'm assuming it's kosher to take diagrams from a textbook to put in a PSE post (specifically Lee Smooth) if I cite them?
yes but
what s the difference between writing $-dU/dx = F(x)$
I'm back, hey @DanielSank
18:45
so in one dimension
?
It's with a minus
but the difference is non-existent in one dimension
# of dimensions
In arbitrarily many dimensions, $F(x)-\nabla U$ is correct
18:47
sO IN one dimension I can write both?
ow OK
yeah,
so conclusion: there is no difference?
The difference is basic calculus
ok I ll keep it siimple
and not write the nabla operator
Actually
18:48
just $-dU/dx = F(x)$
The difference is really the difference between abstract tensor notation and component notation
so the derivative of the position with respect to the position = a force vector(which varies dependent on x)
@DanielSank Do you have access to Wald's General Relativity (1984)?
One really last question
on the scheme you can see that in the beginning
Ep is very high/maximal, but the derivative of that curve, i.e. the one below,
isn't approaching the value 0 at all for that point
@KyleKanos Wanna play (correspondence) chess sometime on chess.com? ;)
18:54
@Danu, an idea for that last question please?
I ll leave you playing chess in peace after that
@privetDruzia $E_p$ does not reach a maximum there
It "blows up"
"blows up" = goes to infinity?
Yes
and the derivative of infinity
This reflects the fact that you cannot force these particles to occupy the same point in space
@privetDruzia A derivative if a number does not exist.
18:55
which is a max is not zero...
But the derivative of a function that steeply approaches infinity does, perhaps ;)
@privetDruzia No, $\infty$ is not a maximum
You cannot work with $\infty$ like with other numbers
@privetDruzia what does "ow" mean
Oh
18:56
ok but if you would calculate the limit... that shoudl approach zero
No
It keeps on getting steeper and steeper as it approaches $r=0$
@Danu What about the diagrams?
Probably technically not.
Probably not a big deal though.
ok so, infinity is a special case, I ll just have to live with the fact that for some reason the derivative (the lower curve) of the Ep which approaches infinity is not equal to 0
You could ask Lee personally
@privetDruzia This should not be something hard to accept for you. This should be very clear and natural
If you're not really at ease with it, you should try to work on that.
(not just "sigh, accept it")
18:59
yes I am working very hard on it
every day
actually
just learned last week what a gradient was
6 months ago I didn t even know what an integral was...
*almost every day
can we try once more, one clear answer...
Why isn t it equal to zero?
( I reread your answers above
It's a function that goes steeper and steeper as it approaches $r=0$
but it never "caps off" to a maximum
It just keeps on growing, in unbounded fashion
It never reaches a maximum
I understand that infinity might not be an easy concept to deal with at first
It always keeps on getting larger and large but you can always go an $\epsilon>0$ closer to $r=0$ and achieve even higher values
I understood, as the potential energy is extremely high, you cannot put those two particles at the same spot (meaning F=0)_
In this particular model, the potential energy keeps on growing in unbounded fashion
ok
that s clear so far
@Danu Will he know what PSE is?
19:03
how can you now relate that to the intermolecular force?
@0celo7 He's very active on Mathematics. Didn't you know?
@Danu Oh right :P
@privetDruzia This particular model just says: As you try to put the molecules closer and closer, they repulse each other stronger and stronger (in unbounded fashion, again).
It will cost you infinite force (which does not exist, so this cannot happen) to put them at exactly the same spot
Because in the limit $r\to 0$ the $E_p(r)$ function is infinitely steep
19:05
the infinity force
E_p(r) is inifinitely steep so F-curve is infinitely steep?
Due to the potential energy you have those forces which occur
@0celo7 Nah.
@DanielSank Ok, Lee Introduction to Smooth Manifolds (2013)?
Beast of Burden has to be the best Rolling Stones song
@privetDruzia No, $E_p$ is infinitely steep so $F$ is infinitely large. Remember: $F=-\nabla V$
If $E_p$ being infinitely steep would imply $F$ being infinitely steep we would have something like $\nabla F\sim -\nabla V$
but that's not true
Note that in all of this, I'm using the word "steepness" as a placeholder for "value of its derivative"
19:15
@0celo7 Nah.
That clarified what I needed!
@Danu, that clarified what I needed
@DanielSank You don't have Springer access o.o
So this statement would be true when trying to explain this: "the force is a result of Ep"?
19:18
@0celo7 Oh do I have access. Yeah. I don't have 'em in the house.
@DanielSank Ok, I wanted you to take a look at some diagrams in it. I'll just post them here.
Locally Euclidean hur dur
Transition functions hur dur
@Danu ?
@0celo7 Just looking at your pictures
@Danu "hur dur"?
I'm trying to explain this stuff in very basic terms.
19:25
@0celo7 Yeah those are great.
^ See, @Danu.
@0celo7 Just felt like saying that :)
It was not a judgement
When we discussed this topic yesterday, by criticism was mostly that I think it's better to discuss tensors in the component/coordinate free picture first.
@DanielSank I thought you were mister "I dun' need no manifolds except $\Bbb R^n$"? ;)
@DanielSank Aight, I'll shoot Dr. Lee an email...aw fuck what if it goes to spam :(
19:26
@Danu Lol wut?
@0celo7 :(
@DanielSank I bet the IT department is closed today, too.
@0celo7 Write it from your university account.
Do explain who you are and why you are writing.
@dmckee That's the one I'm talking about.
Do use complete sentence and no smileys.
Do be polite and respectful.
@DanielSank's work email sent my email straight to spam.
19:27
@dmckee Hahaha, no, see... his IT department slouched and now his emails go to spam.
Don't include anything about nigerian banks or penis enlargement.
2
@dmckee I've emailed plenty of profs before, including t' Hooft. I know how it works.
@dmckee But what if I'm just a poor lonesome Nigerian viagra salesman?
@dmckee Lee sounds Asian, he might be interested in the latter.
19:28
@0celo7 't Hooft
@0celo7 OK. Then forget I said anything. Except the bit that got stared, of course.
@0celo7 He's not Asian
@Danu Seriously?
I know I checked that when writing the email.
@Danu How do you know?
@0celo7 Er ... Could be like, I don't know, related to General Lee...
user54412
@FenderLesPaul better than Can't Always Get What You Want?
19:29
@dmckee Perhaps.
Was General Lee Asian?
^ Probably not.
Feb 15 '15 at 21:16, by Danu
I am unconvinced that it works that easily on manifolds, @DanielSank
Took me a while to dig that up
At the time he'd have had trouble getting into West Point, doncha know?
@0celo7 Yup.
It's short for Het Hooft
@Danu eh? I stand by that.
19:31
which is derived from Het Hoofd (the head)
@dmckee Can I send your professional email a test? I need to see if the thing with @DanielSank was a one-off thing.
@DanielSank Sure you do :)
@Danu I know.
@0celo7 It will work now because I responded to your mail.
@0celo7 Sure. I assume you've found it already.
19:31
I should have known that, I'm sorry @Danu
@dmckee No, but I can find it.
It might actually work elsewhere too now because of that.
It's insane that a .edu account would go to spam.
@0celo7 Universities have been infested by botnets from time to time. No one is immune.
There are Oak Ridge researchers that have utk.edu accounts.
@dmckee It's very imaginatively titled "Test"
@0celo7 I'd never have thought of that.
@0celo7 Came through. No trouble.
19:37
@dmckee Ok, thanks.
@dmckee What domain is your mail on?
mssu.edu
@DanielSank My school's .edu
Yeah. What he said.
I see.
My rather dingy ivory (or rather brick) tower is called "Reynolds Hall", which we (chemical and physical sciences) share with math and bio so it's a lot of fun.
Alas, we have no moat. Much less sharks with laser beams.
19:40
(wat)
On the other hand, after a couple of years in Lego Land (repurposed FEMA trailers) we've getting new labs.
@dmckee Shiny.
@DanielSank On the architect's drawings they are very Shiny. CSI-like even. But I'll settle for larger, better laid out and equipped.
@dmckee Having recently done a lab build-out I can offer one gem that I think will really help:
Please.
19:44
Check this out
See how all the cables are overhead? There's nothing on the floor.
Wuw
We did this in our new lab and OH MY GOODNESS it's nice.
@Danu That's not my lab, just illustrating over-head cable trays.
Still a very nice picture.
And I agree: Vacuuming between my cables is shit!
@DanielSank I've had occasion to work in both kinds of space. Overhead is so worth it.
Yeah.
If you can get the architects to install the trays it's so awesome.
19:46
But our "cluster" is four quad-core computers in one of the mathematicians offices. Our computational nano-scale person is trying to rustle up some money for a little more horsepower or at least access to a grid.
We're actually getting overhead power fixtures for the teaching lab (instead of sticking up through the tables). I've never tried that, but a colleague tells me it is good.
@dmckee That's sad :P
@dmckee We have that in our newer buildings.
@Danu I think he said he was getting two more boxes this year and that would about double the capacity of it. He's a crypto guy, so he need some horsepower and memory and disk.
Also we had them in high school.
@0celo7 The labs I've been working/teaching in date around my fifth or sixth birthday.
19:51
@dmckee Wow they had power fixtures back then?
They had electricity back then?
As long as you could keep the mastodons in the treadmill...
@Danu Lightning has been around for a while.
There were a lot of blackouts during mating season.
4
@0celo7 Says who? ;)
@dmckee Maybe they should've gone for a thrust-based machine... Seems like animals generally don't get enough of that! Except panda's.
19:54
The star wall is starting to make be look unhealthily obsessed.
@dmckee Hahaha!
@Danu How are open sets of the $n$-dim half space defined?
Subspace topology inherited from $\mathbb{R}^n$?
Of course
...unless you have a different topology, obviously
Just checking.
@Danu Hmm, what should the subject line for the email (to Lee) be?
20:15
Don't know, don't care, honestly.
20:35
@ChrisWhite yes
possibly tied with "Can't You Hear Me Knockin'"
Dr. Lee is on a sabbatical. I wonder how long I will be waiting for a response :/
You won't get a response ever
just give up now
Just discard all your hard work
:(
Without the diagrams it's all useless
Or better yet, learn how to make TikZ pictures and stop stealing pictures like a plebeian
20:44
It'll be some Bourbaki style thing that no one can read except for German functional analysts
is Lee still at U Wash?
yah
@FenderLesPaul No he's at I Wash now
[apologies for that terrible... thing]
@Danu Teach me, o wise fibration
TeX - LaTeX is your friend
I learned it too ;)
20:46
I thought you were my friend :'(
wise fibration sounds like a dope indie album name
thanks for the idea
no response yet :(
Ideal gas law,
An ideal gas is defined as one in which all collisions between atoms or molecules are perfectly eleastic and in which there are no intermolecular attractive forces.
yes
why are those conditions so important for the ideal gas law?
20:47
Do you want the derivation
Warning: it's long
euhm lets start with a pragmatic explanation
that might be easier :)
I wrote down the proof somewhere once
not sure what kind of answer you're looking for
for fun?
I wanted to show it to my Chem teacher in high school
20:48
the ideal gas law derivation is not valid if you assume intermolecular forces
She doesn't know calculus so it was a waste
There's also a derivation using special relativity
Not sure if it's a derivation or a "derivation"
An explanation about the principles/reasons will be fine enough
there's also a derivation using loop quantum gravity
20:50
Link?
@0celo7 looks like it was erased from existence
how unfortunate
www.funWithQuantumLoops.com
You basically look at the trace of the energy momentum tensor averaged over some volume
@privetDruzia your question can't be answered without talking about at least some aspect of the derivation
is it long?
Ok you know what? let's go!
(don't make it too long plz)
20:52
you need the viral theorem
i already have so many proofs to study...
or the equiparition theorem
@privetDruzia you can just google it
then you need the Maxwell distribution
google "ideal gas law kinetic theory"
20:53
is this the easiest way?
and you'll see why you need intermolecular forces to be negligible and elastic collisions
you need to calculate the variance of the velocity distribution
I think Stokes theorem comes in as well
stokes theorem always comes in
they should just rename physics to applications of stokes theorem
and taylor series
eww there are integrals on the cotangent bundle
eww eww
20:56
like ew
?
yah
like...just ew
ermagherd ew

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