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07:00 - 18:0018:00 - 20:00

07:01
Hello sir!
I have a question.
Hi :-)
What do you want to ask?
Is Newton's third law of motion universal because conservation of momentum is universal?
Thank you sir very much for help!
OK :-)
07:11
Sir does Newton's third law work in quantum and relative physics?
Yes, because momentum is conserved in quantum mechanics and special relativity.
2
In general relativity things are a little more complicated, but basically conservation of momentum still applies.
Again thank you sir!
$3\times 3=6+3^*$---How does this represent the fact that there cant be a two quark hadron---I know the reason due to confinement and the meaning of LHS of that equation(bound state of two quarks(fundamental reps of SU(3) ), and also can do the math why it is 6 and 3 dim irrep on RHS...but not why this decomposition represents the fact that there cant be a two quark hadron?
07:50
@ManasDogra Confinement means that all states we actually see are color-neutral. What does color-neutral mean in terms of SU(3) reps?
@DebanjanBiswas Newton's third law doesn't really hold in relativity. "Classical Mechanics" by John Taylor gives a good intuition:
08:10
@ACuriousMind 1. But then what? There is no 1 on RHS that's why?
But even in 3*3*3 there is a 10 which is the baryon decuplet. In that way can't the 6 on RHS give rise to a bunch of colorless states?
@ManasDogra I don't know what you mean - the decuplet has nothing to do with any "10" color representation
there's a 1 in $3\otimes 3\otimes 3$ because the $3^\ast$ from the $3\otimes 3 = 6 \oplus 3^\ast$ tensors with the third $3$ into a $1\oplus 8$
and that 1 is the colorless 3-quark state
the decuplet is a "10" flavor representation of the approximate SU(3) flavor symmetry between up, down and strange, not a 10 color representation
Is this a standard procedure solving equations with Fourier transform?
08:25
What does "standard" mean there?
there isn't a book of approved standard equation solving procedures, exactly :P
@ACuriousMind Have you never seen an engineering math book
Slereah, you kill me every time :P
@Slereah no
I live in blissful ignorance
They love to have big books of standards for math
State approved equations
like..."solve this equation according to ISO 652421"?
08:31
@ACuriousMind I mean if it's common to choose a delta function there. Up to this day I didn't know how to solve in that situation
@Feynman_00 I don't really understand why that matters. If it solves the equation, it solves the equation - why is it relevant how many other people solve it that way?
Because if it this has a name I can search more about it :P
You basically have three standards for Fourier transforms
@SirCumference I don't know what are you telling about. Shouldn't Newton's third law hold in any way?
Depending on which side you put your 2 pi factor
left, right, split down the middle
08:37
Anyhow, thanks to that I'm now able to solve heat equation transforming time too
@DebanjanBiswas There is an ambiguity about what "Newton's third law" means in a general context. If you mean "forces are opposite and equal", then it's false e.g. in the presence of EM fields. If you mean "momentum is conserved", then its generally true but you have to assign momentum to fields. See physics.stackexchange.com/q/114466/50583 and its linked questions for plenty of discussion around the validity of Newton's law.
That's why you get John saying it's true (momentum is conserved) and SirCumference saying it's false (forces are not necessarily opposite and equal in EM/relativity)
@DebanjanBiswas At speeds close to the speed of light things get a little complicated because the momentum is no longer given by p = mv. Instead we get p = mv/√(1 - v²/c²)
sometimes I wonder if it is such a good idea to drill various laws into people's heads and then tell them that actually no, they're not true :p
I approve of teaching people early that laws are made to be broken :P
@ACuriousMind Oh..sorry I confused the flavor and color representations
Thanks
08:40
Drilling into people's heads things that are true for 99% of everyday life seems reasonable :P
@Slereah It develops a physical mindset imo
sometimes
sometimes it just makes people wonder about relativistic mass for 30 years
If there's one thing I kinda wish most people were taught about Newton's laws, it's that the first is really just a special case of the second
Namely F=ma with F=0 implies a=0
It somehow never occurred to me until I read Taylor in sophomore year
08:45
Newton's laws were written in a different context
@SirCumference the first actually provides a framework for the second
When he says that objects at rest are in rectilinear motion, he means "And not standing still as in Aristotle's physics"
well, I'm not too familiar with aristotle's physics
We probably should be dropping Newton and Euclid's lists of theorems really
I did find it worthwhile when my textbook mentioned it tho. Would be useful to note in intro physics classes
08:47
There are better versions of them now
Imagine a Aristotle PSE
That's what people did in ancient greece
Go to the Agora, ask Aristotle some questions
I expected Philosophy SE in place of Greece
I wonder if there's a good way to teach an intro physics class without making it feel like everything falls out of the sky
Like give a good motivation for the definition of force and whatnot
08:50
I doubt there'd be enough time for that tho
just push the student
he'll get it
joshphysics' answer is excellent and imo everything you really need to know to understand how Newton's laws work in a modern framework
you just have to remember that basically no physics concept is intuitive
people have argued for centuries about what a line was
@ACuriousMind Interesting, I'll give it a read later tonight
So it's a bit of a tall order for a kid to be expected to pick it up in an afternoon
08:51
I wanted to repost that link but I was overwhelmed with laziness
Basically this
@Slereah It depends how you view it I guess. There's an intuition for most of math, and if you accept the applications of math to physics, you get an intuition for the physics
Usually the trouble is that second step tho
@Slereah eh, people in the past were clearly just stupid
May 3, 2021 at 16:28, by ACuriousMind
imo, "intuition" is just a word for "I have seen this so often I don't need to think about it anymore" like 90% of the time
@ACuriousMind Babies born now are as smart as babies born in the past though
@ACuriousMind That's very different from my definition :P
I'd say something's intuitive when it feels natural and obvious
08:55
Can't expect them to come up with it any more than cavemen
Knowing how to apply e.g. the fundamental theorem of calculus without thinking is different than having an intuition of it imo
I don't think anybody has an actual intuition for the FTC
The sum of all changes in a function equals the net change :P
That always holds. And it still holds when you take limits and end up with derivatives/integrals
I'm not even sure we do for the pythagorean theorem
convergence of the sum of 1/2^n otoh
Big square become little square
very easy on my caveman brain
@Slereah well are we considering the pythagorean theorem to just be the 2-norm
08:58
Just as Pythagoras himself did
I'd seen a good intuition for why the 2-norm is usually the most preferable one
imo most definitions in math are meant to formalize an intuitive concept. e.g. rings formalize the concept of multiplication, inner products formalize the notion of angles, etc.
Angles didn't exist in Japanese mathematics until the arrival of the Dutch
It's not as intuitive as you'd think
I mean inner product spaces are still motivated by the notion of angle, no?
namely giving a precise definition for them
Japanese Physics before then: $\omega=\dot{}$
I'm not saying angles are an obvious thing to come up with, but just that math begins with taking a rough idea and giving a formal definition for them
09:02
They just used lengths for everything IIRC
in fact the decision on which axioms to accept in math is a matter of what you intuitively want to accept as true
all right i oughta stop philosophizing and get back to grading
09:14
If you want to do intuitive physics like geometry you can always check the constructive relativity stuff :
Metric tensor is just a lil circle
And the curvature of space is the deformation of that circle into conics
Doing all of physics as defined by the objects themselves instead of abstractions into arrays of numbers is what people have done historically a lot, really
But once we found out about analytical geometry we just sort of never wanted to go back again
It is either very powerful or we are very dumb
There's more to intuition than just seeing things visually tho
generally being able to break down an abstract concept into something familiar shows up throughout math
The circle basically does 1) set a length 2) tell you that things are the same in every direction
if you deform the circle, you are changing those things
That is the connection between Euclid's geometry and modern Cartan geometry
@SirCumference if multiplication is so intuitive, why do we need to teach kids multiplication tables? :P
Just teach kids about dagger compact categories
multiplication is only "intuitive" to you because you've known how to do it for so long you've forgotten that it was once alien to you
09:26
I was thinking along the lines of how we define things in math
i.e. whether we interpret something as a useful notion to define
that something is useful doesn't mean its intuitive
If it formalizes an intuitive concept, I'd say it's useful
but yes, the converse doesn't necessarily hold
Stiefel Whitney classes are very useful I am told and yet I will never understand what they are
I do feel like it tends to hold for most of my experiences with math though
Are there any research going on Newton's third law now? And also on conservation of momentum?
09:28
@ACuriousMind The exact values for multiplication aren't based on intuition, but knowing when to apply multiplication is often based on intuition
I mean by modern standards we don't look at Newton's third law for that, but there are research into conservation of momentum yes
I know what I'm about to say will sound stupid but I still find stunning that basic arithmetical operations succeed in describing phenomena. No special reason, but if a kid asked me "why does it work like that?" I would get a ticket to Mars
stuff like repeated addition or more general applications. that's what we typically try to instill in elementary school
A somewhat recent topic in momentum conservation was
The Abraham–Minkowski controversy is a physics debate concerning electromagnetic momentum within dielectric media. Two equations were first suggested by Hermann Minkowski (1908) and Max Abraham (1909) for this momentum. They predict different values, from which the name of the controversy derives. Experimental support has been claimed for both.David J. Griffiths argues that, in the presence of matter, only the total stress–energy tensor carries unambiguous physical significance, and how one apportions it between an "electromagnetic" part and a "matter" part depends on context and convenience.Several...
It is connected to the EM Drive that you may have heard of recently
@Slereah that's one of these problems where many people agree that it is solved but not so many agree on the solution :P
09:31
the best kind of problem
Do we know why conservation of momentum true? Or what is underlying physics behind it?
there's probably an intuition tying it to translational symmetry
but it's like 5:30am and i gotta sleep
I mean there is no fundamental reason why it is true
It could be false and that wouldn't change mathematics, just physics
@DebanjanBiswas generally Noether's theorem, for a "simple" exposition without Lagrangian mechanics see physics.stackexchange.com/a/439249/50583
as long as your system is symmetric under translations, you'll have conserved momentum
you can look at examples where that symmetry is broken and see what happens, too
like if you are Aristotle, once again
and you think that all heavy objects move towards the center of the universe
09:34
@DebanjanBiswas basically what symmetry means is that if you translate the entire system to a new location, it won't affect how the system evolves
That is a preferred point
If you have an object initially at rest, it will drop towards the center of the universe
gaining momentum
That is an example of a theory that doesn't conserve momentum and isn't translation invariant
@ACuriousMind I do gotta say that on the topic of intuition, I find a lot of people who say it's critical to math and a lot of people who say it's irrelevant
My entire experience with math had been the former, along with other mathematicians I've talked to, so I can't really see it from the latter perspective
Or rather, I don't see it as something beyond rote memorization. But that might just be me
@SirCumference I think the problem is that it's not really clear what "intuition" is
Lots of resources like 3Blue1Brown and betterexplained.com are based around the importance of intuition
@ACuriousMind Yeah, I guess it's how you want to define it
For me I just have a gut feeling when everything seems crystal clear and beautifully makes sense
Isn't there more fundamental thing with more physical arguments better than Noether's theorem?
09:38
I don't really know a better word for it other than "intuition" tho
why worry so much about what you cannot define :p
well it's an emotion I guess
it's the sole reason I like math. and the reason I think math is so great
there's this adrenaline rush when you spend many hours on a statement and suddenly get a realization on how to view it much more simply
@SirCumference Sounds to me that you just like understanding stuff :P
i guess so lol
that's what I mean when I say "intuition" is mostly code for getting used to things - everything becomes "simple" once you understand it
but people tend to conceive of understanding as binary - either you understand something or you don't - and often want to jump over that gradual process of acquiring understanding
09:46
that's true. I guess I wasn't sure how you defined "understanding" earlier
"intuition" is what - in retrospect - is imagined to allow you to skip/shorten that dreadful period where you neither understand something nor not understand it
also trying to use intuition can backfire
because metaphores only work so far
sometimes you have an unintuitive counter example
I guess there's some built-in intuitive stuff. But a lot of what's intuitive is built on a foundation that's grown through exposure and practice.
@Slereah well, the challenge is making an ever more precise intuition ;)
which gets harder and harder, but also more rewarding
I think this is a good article on intuition vs rigor: betterexplained.com/articles/…
Best advice I can give is that typically for any physics thing you will have many different descriptions available
just go through them until you find one that clicks
09:49
I do think I've had less luck with making physics intuitive compared to math. There's no real logic basis for how our universe happens to work
well yes
It's like improvising in music. When it happens, it just flows. But you can't get to the state of being able to freely improvise without listening to a lot of music, and learning the fundamentals of how to play or sing. And then practising. A lot.
Like I found a really satisfying intuition for a general wave uncertainty principle, but if I try to apply that to physics, I kind of have to just "accept" that momentum and position are related in a wavelike manner
the universe works the way it does, but it could work differently
hence I don't really have a satisfying explanation for the heisenberg uncertainty principle
09:51
that's why you have to observe first
@Slereah Yeah. I do feel like math is more about logic whereas physics is more about observing
if there was no other alternative physics would be easy
that's not to say everything in math has a fundamental basis, but most of my experience with it is about logical connections
@SirCumference Physics is about looking at reality and devising a model of it; not about somehow "deriving" reality out of nowhere
@ACuriousMind unfortunately, yes
09:52
even though the latter idea somehow got stuck in a lot of theorist heads :P
which is still cool in its own right with how much it reveals. but it does always leave some dissatisfaction with "why"
what answer could there possibly be as to "why"?
In Kepler's & Newton's times, they didn't really talk about mathematics. They talked about geometry. Even number theory was thought of in geometric terms. Algebra was just a bunch of dubious bookkeeping tricks that could be used to solve geometry problems.
It was dubious because it wasn't intuitively obvious like geometry. ;)
@ACuriousMind well, I guess it's a matter of how satisfied you end up feeling with an explanation :P
just an emotion
I mean people used algebra but it was more for accounting
09:54
Even though Euclid's axioms have various large philosophical holes in them.
@SirCumference I find the disappointment goes away once I force myself to realize the question isn't meaningful :P
well my options are either turning to some religion/philosophy or just accepting it's a moot effort
first isn't really that appealing to me but I've been struggling to do the latter
the first step is realizing that "cause and effect" are social constructs, not physical truths
at least that's my pithy summary of Norton's Causation as Folk Science which I always recommend to people thinking that causation is a fundamental aspect of physics
that's an interesting perspective
@Slereah Fair point, although that's (mostly) just addition & subtraction. And the theoretical basis for arithmetic was still Euclid's Elements.
09:57
though i gotta wonder where the fine line between social constructs and physical truths is
welp it's 6am and I still am only halfway done with grading, I probably should call it here
Night y'all
Prequantum bundle has the hbar as a term of the curvature
and the symplectic structure does relate position to momentum, ergo relates to mass
and I guess the quantization part is the Weil integrability condition
Maybe the scale has nothing to do with the bundle, just the integrability condition
10:14
Is polarization related to mass?
10:24
Probably need to read up on symplectic geometry really
That's the problem of GR, mass is basically meaningless as far as geometry goes
Damn equivalence principle
10:51
maybe I should look at how the Polyakov action works like as a bundle
The constraint is on the mass which restricts the jet space
11:07
I feel like if I pull this thread I will either unveil the secrets of quantum mechanics or find out that someone wrote that idea in 1963
 
1 hour later…
12:29
although ironically if there is such a link that would mean nothing for quantum gravity because the volume structure is one of the least important one
12:40
@ACuriousMind Wow, that was deep and very interesting
I'm glad the author inserted the cheerful note at the end, I was going as uncanny as Mr Incredible during the reading :P
13:17
@Feynman_00 in case you didn't realize: The author is the Wigner who has a lot of stuff named after him
Hey. Is this a good place to chat about physics? I just got permabanned from the physics Discord for daring to talk to a high schooler about QFT...
13:51
@ACuriousMind Oh I recognized him, I have some inside joke with my friend about Wigner haunting us :P
@JoeBentley Sure, this chat is mainly about Physics. As long as you are respectful to all users you can talk about whatever you like. See the guidelines for more details.
Was looking for experimental data to confirm that the second clock effect indeed doesn't exist and then I find a paper claiming that it does
Ugh
I hate the real world
...or do you just hate fantasy?
...caught in a laaaandslide...
who knows
I'm gonna pretend I didn't see it for now
don't need to track down 80 years of dispute on the second clock effect
@Feynman_00 somewhat disappointingly, "Wigner's ghost" is not (yet) a thing
Although I think the paper is more "It's not impossible for the effect to exist"
more than proving it true
I will pontificate and claim that it doesn't exist
Die mad, Hermann Weyl
14:21
The bundle of densities is also involved with both conformal geometry and geometric quantization
Suspiscious
Suspecting that famous "quantomorphism group" that nlab keeps talking about
@ACuriousMind but covid is :(
uh
you're not wrong but I'm not seeing the connection :P
There's no connection as I'm whining because I'm missing some lectures
oh, that sucks - hope you (or the lecturers?) get well soon
14:38
It's me. I'm quite fine but of course I cannot attend the lectures. Luckily this week QFT has been suspended for other reasons :P
Gigachads Assemble
great evening tho
(Philips, S.G.J., Mądzik, M.T., Amitonov, S.V. et al. Universal control of a six-qubit quantum processor in silicon. Nature 609, 919–924 (2022).)[nature.com/articles/s41586-022-05117-x]
-_-
Goodbye Gigachads
14:53
@ACuriousMind Why does the quantum bundle have a curvature anyway
Isn't it U(1) and therefore flat
why would U(1) mean flat?
flat means "pure gauge"
Oh wait I guess it's not like a metric curvature
nvm
But more importantly, why is it $\hbar$ then?
is it an assumption that it is a constant?
what if you have curved quantization 🤔
15:05
@Slereah the curvature of the prequantum bundle is supposed to be the symplectic form
But in proportion to the planck constant, no?
Or its inverse
I think there are different conventions for where you introduce the constant
some write the symplectic form itself as $\frac{1}{\hbar}\mathrm{d}q\wedge\mathrm{d}p$
so that $\hbar \omega$ is the "normal" symplectic form you'd expect
Apparently the diffeomorphism group lifts to a subgroup of the symplectomorphism group
perhaps there is something of note that happens with more specific subgroups
I really need to buff up on symplectic geometry
I know basically nothing about it
Probably relates to those Hamiltonian constraints in phase space I am guessing
on the appropriate mass hyperboloid
constraints usually appear under the name "symplectic reduction", see physics.stackexchange.com/a/717776/50583
Oh nice
It is a lot of work just to build a clock
15:15
If you want to build a clock from scratch, you must first invent the universe
(with apologies to Carl Sagan)
I do hope I have found a secret of the universe because otherwise it may be quite a waste of time
Nothing to show for it but learning about quantomorphisms
Is the symplectic reduction like a base space where the bundle is the symplectic space with the gauge group as fibers?
@Slereah not necessarily (the fiber is only $G$ for points whose stabilizer in $G$ is trivial)
Hopefully it will be
i.e. in general it's not a bundle because the "fiber" over each point $x$ is $G/\mathrm{Stab}_x(G)$, where $\mathrm{Stab}_x(G)$ is the subgroup of $G$ that leaves $x$ invariant even before the quotient
I am mostly gonna consider the cotangent bundle I think here
15:25
this is more a property of the action of $G$ than of the phase space itself
With Lorentz symmetry presumably
Given the dimension of a representation, is there a general method to draw Young Tableaux for SU(N) ? I know how to do the inverse.

Actually I wish to find the symmetry nature of the states transforming acc to a particular irrep...I thought the quickest way must be to draw a Young Tableaux and see from it
@ManasDogra no, because for $N>2$ it can happen that there is more than one representation with the same dimension
i.e. there can be several tableaux producing non-isomorphic reps with the same dimension
I want it to be true that all this business involves a bundle reduction from the symplectic structure to the appropriate conformal/volume structure, and this reduction corresponds to a direction/mass or something
Gonna use my monkey paw to make it so
Not 100% sure if that will help me but it sounds like a thing
15:53
0
Q: Why is this question closed?

InanimateBeingI posted this question today which is a shortened version of the previous question I posted here so that users may get the point I'm trying to ask. It's not a "check-my-work question" and neither a "home-work question". From the given links: How should I ask a homework question on this website? ...

16:14
Thinking about it more
in the Polyakov action, the 1-frame (defining the length scale of the parametrization) couples to the mass term
Another suspiscious thing
Guess I am hoping that all of this together will shake out to give a map between the integral of that quantum connection and the volume structure
also involving a mass I guess
16:41
Oh man that's gonna be a lot of bundles
I wonder if the Ancients would be pleased that the fundamental theories of physics involved so many circles
Drawing a little circle bundle over the phase space and Aristotle nods wisely
17:04
So is there any way I can find out whether the states in say $1$ of $2\times 2=1+3$ is antisymmetric without actually finding out the wavefunctions?
Not only for SU(2) but for SU(N) reps
@ACuriousMind And if this is true, how do we make the Tableau when say we are asked to evaluate $8\times8$ for SU(3)? How do we know 8 is the L-shaped diagram without just guessing?
@ManasDogra If the given group has more than one representation for a given dimension, asking you to evaluate $8\otimes 8$ doesn't actually make sense without specifying what rep the 8s are
in general you need to employ better notation than just writing down the dimension of a representation, see e.g. this with the $D^{prq}$ notation
@ManasDogra what do you mean by the state being antisymmetric?
you mean under the exchange of the two reps on the l.h.s.?
You have very generally that $V\otimes V = \mathrm{Sym}^2(V)\oplus\Lambda^2(V)$, i.e. the tensor product splits into the sum of the symmetric and anti-symmetric parts, and for $\mathrm{SU}(N)$ you have that these are definitely subrepresentations
so since you know the dimension of the symmetric and anti-symmetric parts - such as 3 and 1 respectively for $V$ being 2-dimensional - you can usually deduce which parts are (anti-)symmetric without any explicit computation
17:16
I am looking for more general---$V\otimes W$ :)
but generally I'm not sure why you're worrying about this - determining general $\mathrm{SU}(N)$ representations beyond simple products of fundamentals and adjoints rarely comes up
@ManasDogra for that the notion of (anti-)symmetry doesn't make sense
@ACuriousMind For say $3\times3\times3$ I evaluate $3\times3$ to be $6+3^*$. Now I have a 6
...and?
I did once do the horrible business of SU(3) reps
Boy it was not fun
17:35
@ACuriousMind nothing...I was probably going to say something wrong, but the doubt got cleared
You guys are magical...Even when you don't utter the answer, you make me think and answer myself!
the physics was in you all along
17:49
@ACuriousMind can I ask you something about single states and eigenstates?
@ACuriousMind From the link you sent me in the last page there is one $4\times4=1+3+5+7$ for SU(2)...How can we obtain this with Young Tableau if we don't know how to draw a 4 uniquely in the first place? Or is the 4 dimensional representation unique for SU(2)?
I could obtain this relation from angular momentum addition rules though
@Slereah Thyenkzzz :)
for su(2) and su(3) the dimensional notation is unique if you distinguish between $\mathbf{N}$ and $\mathbf{N}^\ast$
So in that case, how to draw an M or M* for SU(N)?
where N=2 or 3
07:00 - 18:0018:00 - 20:00

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