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05:26
Recently I came to know that classical trajectory of a particle given initial conditions is not unique..Initial conditions fix the arbitrary constants of integration which we get by integration the equation of motion...What extra things fixes.i.e. determines uniquely the trajectory in reality?
I mean if we get a set of trajectories as solution even after setting the initial conditions then what determines which trajectory the particle will follow in reality.
Am I missing any?
05:52
@ManasDogra Initial position and momentum is enough to fix it in classical mechanics
Since it's just a second order ODE
Or alternatively, initial and final position, if you're feeling fancy and can see the future
Then it's
\begin{equation}
\vec{x}(t) = \frac{\vec{x}_b - \vec{x}_a}{t_b - t_a} t + \frac{1}{2} \left[ \vec{x}_a + \vec{x}_b - \frac{\vec{x}_b - \vec{x}_a}{t_b - t_a} (t_a + t_b)\right]
\end{equation}
So I thought until I read a paper by Dhar
https://aapt.scitation.org/doi/10.1119/1.17411
But $\vec{x}(t) = \vec{v}_0 t + \vec{x}_0$ will fix it for $\ddot{\vec{x}}(t) = 0$
yeah but he's talking about weird systems
Probably more Norton's Dome stuff
In those cases it's possible that there are no unique solutions given initial conditions
@Slereah Yes that's what I was talking about...If we can make such a potential in reality what will determine which trajectory the particle would follow?
Although it's not practical to make a singular potential
Well in reality we can't make systems with arbitrary forces
And also quantum mechanics makes it not an issue in the end
IIRC the QM version of Norton's dome isn't a problem
What about $F=\frac{1}{x^3}$? with $x=0=\dot{x}$ at $t=0$ It has three solutions even after putting the boundary conditions..
05:59
I mean if you have discontinuous and divergent forces in the first place
It's gonna be weird anyway
there's plenty of known solutions like that
sorry $F=x^{1/3}$
ie the Painlevé non-singular collisions for instance
Which just uses gravity
Although it's harder to prove
So we can ignore those kind of things for all practical purposes...
@ManasDogra "In the case of singular forces, for which some of the higher derivatives do not exist at a given point"
I mean if you use weird equations you get weird results
 
1 hour later…
07:32
@ManasDogra Note that scenarios like Norton's dome are only pathological for certain points in the space of initial conditions (in the dome's case, for something sitting motionless at the exact top)
but in reality things are not points without extent - no "real" thing can be like that,real things have extent and hence will never hit only that single point with their state
Norton's dome is a philosophical problem (i.e. what does causation mean?), not a practical problem (i.e. how do we solve equations of motion in practice?)
Well you can construct problems like that for most physical laws if you're loose enough with it
sure - whenever you have a differential equation with some function as input, choosing that function to be pathological will likely mess up the uniqueness properties of the solutions at some points
08:08
@ACuriousMind can you pretty please take a look at my question?
08:40
@Korra I have no idea what the question is. (I saw your message, I just don't know what the image depicts or what "am I missing any?" is supposed to mean)
09:04
@ACuriousMind it's the Feynman diagrams
And I am trying to work out the symmetry factors
So far I concluded that the factor is 4
 
3 hours later…
12:02
Does a generic dome not have the Norton's dome property?
Only if its derivatives diverge at some point I guess
or whatever the full condition is for Lipschitz continuous functions
@RyanUnger depends on what you mean by "generic"
I clearly mean whatever so that the statement is true
the usual meaning
you get Norton's dome-like phenomena exactly when the force resulting from the shape of the dome is not Lipschitz continuous
Are you sure that every non-Lipschitz function has this property though
Norton's dome is C^\alpha right
12:14
I dunno if it's a sufficient condition for that no
I would believe that lots of C^\alpha vector fields have unique integral curves. I also believe that lots of them don't
would be hard to have a dome shaped like a Dirichlet function
@RyanUnger probably not every
in any case, I think the "generic" dome many people would write down would be some sort of polynomial, and you don't get issues with that :P
The usual one is basically $F = \sqrt{r}$
@ACuriousMind I clearly mean Baire generic in some Holder space
12:20
it's my favorite shape of domes
Love it when the church has a Baire generic shape
its modern art
Can't even find an easy example online of what's a good function to talk about Baire generic
5
Q: What is a $0\times0$ or $0\times3$ matrix?

HookedIn the comments to another question, the following exchange was noted: ... wait until you see a 0×0 matrix. and ... or worse, a 0×3 matrix! What are these things? Do they have a name or any special proprieties? Where are they used?

2
what
@Slereah what
do you know what baire generic means
I don't rly
It's one of those words you rarely see
12:27
the baire category theorem is easy you should know about it
Maybe but it's not one of those things that come up often?
uh, ok
if you say so
3 PSE results for "Baire"
Different tribe
I know it is a math term, it's just not common in physics
12:41
@EmilioPisanty I learn something new everyday
physicists not using baire is not surprising
well, it is actually
arent they supposed to read reed and simon
They are not
Someone repost that xkcd comic about specialists
@RyanUnger no, they're supposed to say "it's somewhere in Reed and Simon" when someone asks for proofs
the QFT works in mysterious ways
12:53
thanks
@VincentThacker I just added my take there
13:33
Greg Egan published a new book and he's too ashamed to say it's about wormholes
14:18
Here is a circuit with two battery $V_1$ and $V_2$, you can clearly see the direction of the electric current $I_1$ and $I_2$. Can anyone please tell me, what will be the direction of $I_1$ if I reverse the terminal of the $V_1$ battery?
And, will the direction of $I_2$ change for it?, here $V_1$, $V_2$ has no fixed voltage.
14:38
@NazmulHasanShipon Hi Nazmul. Whenever you have a circuit with two batteries I suggest using the principle of superposition to calculate the currents. This is by far the easiest way to do it.
@NazmulHasanShipon It depends on the values of V1 and V2.
14:55
@JohnRennie I don't know about principle of superposition. Can you give me a source where I can learn about it? I am high school student, about to complete.
@NazmulHasanShipon Have a look at this Khan Academy article.
And this is also a good article. Possibly better than the Khan Academy one.
@VincentThacker But I have to show diagrammatically what would the direction of currents after reversing the terminals of the voltage source $V_1$. Can @JohnRennie help me about it? Note that V_1 and V_2 isn't given.
@NazmulHasanShipon suppose we flip V₁ then the circuit looks like this:
OK so far?
yes
@JohnRennie
Suppose we ignore battery 2 and just draw in the currents we will get from battery 1. Then the circuit looks like this:
@NazmulHasanShipon OK so far?
Now ignore battery 1 and draw the currents we expect for battery 2:
@NazmulHasanShipon Yes?
Yes, @JohnRennie
What superposition says is that to get the current when both batteries are present we just add the currents from the two diagrams, so we get this:
Now, if you look at the left part and the centre part the currents are in the same direction, so when we add them the total current will be in that direction i.e. down on the left and up in the middle. Yes?
Yes, @JohnRennie
Hi, @JohnRennie if two charges are present one inside a closed surface and one outside. Then we say net flux is due to inside charge only. Charge outside contribute to zero flux. The reason stated is field enters from one side and pass through other side.
my question is
These charges field will get superposed. So after superpose
tion
15:15
@NazmulHasanShipon But on the right side the red and blue currents are in opposite directions. Which way the total current flows will depend on which is bigger, the red or the blue current, and we can't tell that without knowing the values of the voltages and resistances.
@cOnnectOrTR12 I'm starting my lunch now. I'll be back in about an hour.
@JohnRennie okay @JohnRennie but
Ok! can we differentiate between the two fields and say it’s field just passes through the surface so it’s flux is zero.
@JohnRennie will the original direction of $I_2$ change for it?
This is the question. Answer it after your healthy lunch
16:05
@NazmulHasanShipon If we take the original diagram, before the battery was reversed, and draw in the directions of the currents we get (red is battery 1 and blue is battery 2 as before):
John's "lunch" being healthy would be a new occurence ;P
Now if I₁ is upwards then on the left branch the red current from V₁ must be larger than the blue current from V₂.
Now reversing V₁ swaps the direction of the red currents but it does not change their magnitude. If we look at the diagram with V₁ swapped:
It suggests that on the right most branch the red current will be larger and the net current will be upwards.
So swapping V₁ reverses the direction of both I₁ and I₂.
But I'm not absolutely sure about this as it may still depend on the resistances present. I'd have to do the calculation to be sure.
> Hi, @JohnRennie if two charges are present one inside a closed surface and one outside. Then we say net flux is due to inside charge only. Charge outside contribute to zero flux. The reason stated is field enters from one side and pass through other side.

My question is these charges field will get superposed. So after superposition can we differentiate between the two fields and say its field just passes through the surface so its flux is zero.
@cOnnectOrTR12 There is only one electric field, and it can be described as the sum of the fields from the two charges.
If we write the field as the sum of the two fields then:
- the field of the inside charge has a non-zero total flux through the surface
- the field of the outside charge has a zero total flux through the surface
@ACuriousMind my thousand words on the matter :-)
Traditional English sausage butties!
mhhh...the sausages look a bit strange, did you bread them or something?
I sliced them lengthways before frying them - it makes them flatter so they work better in rolls.
2
@JohnRennie @JohnRennie, does that mean V_1 > V_2 ?
16:23
5
Q: Unpinning the accepted answer from the top of the list of answers

Nicolas ChabanovskyToday we changed the way we sort answers on Stack Overflow. We no longer pin the accepted answer (with the green checkmark) to the top of the list of answers. By default, we now sort strictly by votes (descending order by highest score), and the accepted answer's order in the list is based on its...

I don't know if we need this on Physics.SE, but I guess we should consider it.
@ACuriousMind The rough appearance is because they were made from coarsely ground meat and where the inside surface has browned it looks very granular. They were exceedingly good though.
@NazmulHasanShipon I think it probably means V₁ > V₂ but I would have to sit down and do the calculation to be sure.
@JohnRennie I see, sounds indeed good!
@JohnRennie can you do it for me please, I can wait?
@PM2Ring at least worth thinking about
@ACuriousMind For the rolls I used a trick I picked up from a YouTube video. You sprinkle grated cheese onto a hot frying pan, wait for it to melt and brown then put the roll down on it. Then when you lift the roll up the cheese sticks to it and you get an instant toasted cheese layer on the roll.
16:29
@JohnRennie and here I was thinking you had just browned the bun
I was almost concerned - just bread and sausages didn't sound like a Rennie lunch ;)
I spread barbeque sauce on the rolls before adding the toasted cheese layer just to make it extra healthy.
@JohnRennie make sure to have a diet coke too
@NazmulHasanShipon It's a messy calculation, but I had a quick look and I don't think we can definitely say V₁ > V₂.
@JohnRennie Okay @JohnRennie , thank you so much for doing it for me.
16:37
For example if R₃ is very large then the current through it will be very small even if V₂ is also very large so I₁ could still be upwards even though V₁ < V₂
@JohnRennie but this means we can tell and differentiate between the fields even after superposition. In other words there is one field after superposition. So how can you tell whose contributing to the flux because that can be done only by determining and distinguishing between the field lines of the two charges.
@JohnRennie I get it, thank you :) .
@cOnnectOrTR12 The flux is ∫E.dA where E is the total field and E = E₁ + E₂ where E₁ and E₂ are the fields due to the charges Q₁ inside and Q₂ outside. OK so far?
@NazmulHasanShipon you're welcome :-)
Seem right. Yeah
And if E = E₁ + E₂ we can write the integral as:

∫E.dA = ∫(E₁ + E₂).dA = ∫E₁.dA + ∫E₂.dA = Φ₁ + Φ₂
where Φ₁ and Φ₂ are the fluxes from the charges Q₁ inside and Q₂ outside.
16:42
Yes
So while there is only one field we can still calculate the fluxes separately and add them to get the total.
In this case we'd get Φ₁ ≠ 0 and Φ₂ = 0
How is phi2 zero
@JohnRennie but if R_3 is very large, how does it affect the current of V_2 ?
@cOnnectOrTR12 Φ₂ is the flux through the surface due to the charge outside the surface.
So it has to be zero.
@NazmulHasanShipon All the current that V₂ produces has to flow through R₃ before it splits to flow through the left and right branches. Yes?
yes
@JohnRennie
16:52
So charge outside will have + and - flux?
@NazmulHasanShipon And if R₃ is much larger than all the other resistors the current from V₂ is approximately given by I = V₂/R₃. Yes?
@cOnnectOrTR12 Every field line from the charge outside has to enter the surface then leave it again, so the number of field lines from the outside charge entering the surface has to be the same as the number of field lines from the outside charge leaving the surface. Yes?
Ok!
So?
Here is the confusion
So the total flux through the surface from the outside charge is zero.
@JohnRennie yes
9 mins ago, by Nazmul Hasan Shipon
@JohnRennie but if R_3 is very large, how does it affect the current of V_2 ?
16:56
How can you talk about field lines from individual charges if it has been superposed?
That's why R₃ affects the current from V₂
@cOnnectOrTR12 Because electric fields superpose.
You can take the field lines from the two charges separately, calculate the fluxes separately, then just add them to get the total.
@JohnRennie but I was wondering if that would affect the current of V_1 too.
No, because the current from V₁ splits. Some flows through the middle branch where R₃ is, but some can flow through the right branch where R₄ and R₅ are.
You mean take one charge find it’s flux1 then take another flux2. Add them and you will get net flux from charge inside.
So even if R₃ was infinite there would still be a current from V₁ because it could flow through the right most branch of the circuit.
@cOnnectOrTR12 the sum will give you the total flux from both charges, but the charge outside has a net flux of zero so in fact this is equal to the flux from the charge inside.
17:01
@JohnRennie so if V_2 > V_1, I_2 direction would be unchanged.
i.e. Φtotal = F₁ + F₂ but F₂ = 0 so we end up with Φtotal = F₁
@JohnRennie according to this picture
@NazmulHasanShipon Yes
56 mins ago, by John Rennie
user image
Yes we can do that. And I was confused how could you talk about field lines passing through when it’s superposed. How can you map out individual lines when it’s already superposed
@NazmulHasanShipon I₂ is always downwards regardless of what the two voltages are.
17:04
@JohnRennie why is that?
Thanks I was grinding on this for days
@NazmulHasanShipon the red and blue arrows show the contributions to the current from V₁ and V₂. Yes?
@cOnnectOrTR12 OK :-)
And if both arrows point in the same direction the total current must also be in that direction. Yes?
@JohnRennie but why should it point in the same direction?
@JohnRennie here it point upwards
@JohnRennie here downwards
17:08
@NazmulHasanShipon That's with V₁ reversed.
I'm talking about the diagram with V₁ in its original direction
@JohnRennie oh yes, I was talking about the reversed case.
In the reversed case I'm not sure what will happen.
so in the reversed case if V_2 > V_1, I_2 direction would be unchanged or we are not sure?
okay.
2 hours ago, by John Rennie
user image
I'm not sure.
@JohnRennie okay :) .
17:11
When we find the E due to a charged conductor (eg a thick plate)it comes as E=sigma/e0. It has been derived by taking a Gaussian surface one end inside the conductor and other outside. We take charges on one side and not on other side. But when we talk about field due to thin sheet we draw Gaussian surface cylinder with both ends on both sides. Why have we ignored the charges on other side of the thick conductor. Does it not spread on both surfaces in case of thick conductor?
I need to go now.
 
1 hour later…
18:34
Why don’t we find flux of the system of two charges, one of them inside the closed surface ?
why do we calculate flux separately?
@cOnnectOrTR12 you've been asking more or less the same question for days now here. What different answers than those you've already gotten do you expect?
If you are not satisfied with the explanations you've received so far, you really need to be more specific what you're dissatisfied with
At this point I don't see why I should try to answer your question when you'll just come back tomorrow and ask the same question again with no indication that you retained anything from the previous conversations
But no one answered this. Only recently I was told you have to find flux separately. And I am asking just why? Because now after superposition we should be finding the flux of resultant field from the system of charges
you don't have to find the flux separately, it's just easier
18:49
So even if we find the flux of resultant we will get the same net flux from inner charge?
And it’s the same thing
@ACuriousMind can you tell me how do you do that? Is it complicated?
didn't John explain that already here:
2 hours ago, by John Rennie
And if E = E₁ + E₂ we can write the integral as:

∫E.dA = ∫(E₁ + E₂).dA = ∫E₁.dA + ∫E₂.dA = Φ₁ + Φ₂
Total flux due to resultant field= flux1+flux2=flux1
Can you answer my charged conductor question ?

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