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5:26 AM
@JohnRennie hi
 
@AshishAhuja hi :-)
 
I was studying electric flux, and for a sphere
we can easily show that the flux is $\frac{Q}{\epsilon}$
We can extend this to all closed surfaces
and an intuitive way to think about this would be to think of electric flux sort of like air, and since this is a closed surface, the amount of total air exiting would be constant. However, would it possible for you to prove it a bit more formally, or give me a hint?
 
@AshishAhuja Formally this is the divergence theorem:
In vector calculus, the divergence theorem, also known as Gauss's theorem or Ostrogradsky's theorem, is a theorem which relates the flux of a vector field through a closed surface to the divergence of the field in the volume enclosed. More precisely, the divergence theorem states that the surface integral of a vector field over a closed surface, which is called the flux through the surface, is equal to the volume integral of the divergence over the region inside the surface. Intuitively, it states that the sum of all sources of the field in a region (with sinks regarded as negative sources) gives...
But there is a simpler way of looking at it.
 
yeah that theorem looks extremely complex
 
In electrostatics every field line has to begin and end on a charge
 
5:37 AM
yes
 
So if there are no charges inside a surface every field line that enters the surface has to exit the surface again because it cannot end inside the surface.
 
So loosely speaking the amount of field entering the surface has to equal the amount of field exiting the surface and the integral over the whole surface must be zero.
 
hmm but the electric flux is not zero for a closed surface is it? I'm talking about the situation where a charge $Q$ is placed inside the surface, sorry if I wasn't clear before
 
Conversely, if there is a charge inside the surface then field lines begin at the charge, but since they cannot end on the same charge they must exit the surface. Hence there must be a net outwards (or inwards) flow through the surface.
 
5:40 AM
Ohhh neat
 
Field lines are a bit vaguely defined, but you can consider each field line associated with a constant amount of field i.e. we have N field lines per coulomb of charge.
 
Aren't there an infinite amount of field lines?
 
Then the amount of field lines exiting (or entering) the surface will be proportional to te charge inside the surface.
@AshishAhuja A field line isn't actually a physical object. It's actually just a direction. It's the direction of the force the field produces on an infinitesimally small test charge.
 
@JohnRennie for a sphere we can prove that flux is $\frac{Q}{\epsilon}$ and here you essentially proved that it has to be constant for all closed surfaces, so doesn't that complete the proof?
 
But we tend to think of it as representing some small part of the field.
 
5:44 AM
@JohnRennie hmm, I know that but considering a finite amount of field lines has got me confused..
 
@AshishAhuja I'm not sure this counts as a "proof" :-)
It's more a argument about plasusibility.
The proof is the divergence theorem.
 
yeah true :D But it seems logically sound, so for general purposes I guess that's enough. The divergence theorem looked scary.
 
:-)
 
6:03 AM
@AshishAhuja once you understand what divergence means physically, youll realise that the theorem is actually pretty intuitive
 
interestingly, a heuristic "intuition" for the divergence theorem is similar to your earlier argument. its tough to prove the theorem rigorously though
 
i.e treating electric flux similar to air flowing out?
 
just outflow of any quantity
like water for eg.
 
got it.
 
6:08 AM
@AshishAhuja how I understood it was
consider a charge inside any arbitrary surface
draw a small sphere of radius delta with delta--->0
 
then the flux through the sphere= q/epsilon
now if you interpret the flux as the measure of the no. of field lines, then
 
ohh got it
 
the flux through the sphere=flux through the surface obviously, since the all the field lines piercing the sphere pierce the surface too
 
6:11 AM
and voila
 
this is pretty neat too
thanks
 
very similar to what you did
 
Yeah but mine lacked any formality at all. It isn't intuitively obvious why air = electric flux, so I like explanations such as yours and JR's.
 
without vector calc, this is as far as you can go I suppose. A "proof" with all the rigour would require the understanding of the divergence , etc
 
6:43 AM
Hi guys. I am back.
 
7:10 AM
If we have two point charges $Q_1$ and $Q_2$ with fields $\vec{E_1}$ and $\vec{E_2}$ inside a closed surface we have $$\phi = \oint{(\vec{E_1} + \vec{E_2}) \cdot \vec{dS}} = \oint{\vec{E_1} \cdot \vec{dS}} + \oint{\vec{E_2} \cdot \vec{dS}} = \frac{Q_1 + Q_2}{\epsilon}$$ Now we can extend this to as many charges as we want. Is this a valid proof of Gauss's Law?
@JohnRennie
 
I wouldn't say it was a proof of Gauss's law.
 
Why not? Assuming that we know that flux for a point charge is $\frac{Q}{\epsilon}$
 
@AshishAhuja right, but you need Gauss's law to tell you that the flux for a point charge is Q/ε
 
wait what
 
So all you're saying is that if Gauss's law applies for a single charge then it applies for any collection of charges, which is true.
 
7:14 AM
Ohh wait does divergence theorem require gauss's law?
 
The divergence theorem is Gauss's law.
 
But wiki has two separate pages for them?
 
The Wikipedia article for the divergence theorem starts: "In vector calculus, the divergence theorem, also known as Gauss's theorem or Ostrogradsky's theorem ..."
 
hmm okay, thanks.
 
Oh, OK, Gauss's law is a special case of Gauss's theorem/divergence theorem.
Though whether it really deserves its own page is debatable.
 
 
3 hours later…
10:04 AM
Greetings, could I get some help on this problem:
I have seen the solutions of this on the internet but I do not understand them
once we do FBD on the block we get are supposed to get , mg-N=ma, then set N=0 and say a=w^2 A where A is amplitude
I don't get the logic here
 
@Buraian Do you agree that the most probable point of losing contact is when the piston is at it's highest position?
 
well I considered that but how would you proof that?
but I think there is an arguement for it
so the least frequency such that it loses contact msut be when it is shot at top
if it is more frequency than that, it loses contact before hitting the top
 
yeah that's correct
 
right, now how do you do the force balance
 
Ok let's just talk about the highest position now
 
10:11 AM
right
 
normal force = zero as you said
so acceleration of the washer = g
 
Hmm right so here is where my doubt begins
what exactly does normal force mean here?
teh spring is supporting it, so it should be spring force, no ?
 
The washer rests on the piston, the normal force I'm talking about is between the washer and the piston
 
but the piston is acting like a spring here, no?
 
@Buraian you've probably done problems with a man on some scales in a lift. Yes?
If the lift accelerates downwards the man's weight decreases
 
10:13 AM
yea
 
Well the acceleration of the piston in this problem is given by a = -kx or some constant k. Yes?
 
hmmm I'm not sure there, that'd assume you treat the lift as a spring
 
Sorry I meant piston not lift.
 
yes yea
 
So the downward acceleration (i.e. most negative acceleration) occurs at the greatest value of x i.e. at the top of the motion.
So that's when the weight of the man washer is least.
i.e. that's when the the normal force between the bottom of the washer and the top of the piston is least.
 
10:18 AM
normal force = spring acceleration?
Ping back when replyin
 
@Buraian Go back to the lift problem.
 
yes
 
The man's weight is mg.
 
yyes
 
If the acceleration of the lift downwards is a, then the weight of the man decreases to m(g - a). Yes?
 
10:22 AM
yes due to the pseudo force
 
And that "weight" m(g-a) is the normal force between the bottom of the man's shoes and the lift. Yes?
 
hmm yes
 
If the lift accelerated faster than g the man would actually take off and lose contact with the floor of the lift.
Well in this problem the piston is the lift and the washer is the man.
 
Ohkay I think I get it now, we can think of the man in elevator as the washer and piston
 
@Buraian Yes. The washer will lose contact with the top of the piston if and only if the piston accelerates downwards faster than g.
 
10:26 AM
so the difference between case is that, here the acceleration of the 'lift' is time varying, correct?
 
Yes.
 
like a time varying pseudo force
 
Yes
 
I have one question about pseudo force and normal, for accelerating frames, to find normal is it neccesary to use pseudo force?
 
If the lift position is x(t) = A sin(ωt) then a(t) = -Aω² sin(ωt)
 
10:28 AM
for example, in this case unelss you put in pseudo force it's impossible to get correct acceleration. So, is it impossible to get the correct normal by some inertial frame outside?
 
No, that's wrong.
Consider the situation as seen from outside the lift.
 
yes
 
We have a man with a gravitation force of Fg = -mg (let's take upwards to be the positive direction).
 
yep
 
We observe the man to have the same acceleration a as the lift, so we know the net force on the man must be given by Fnet = ma. Yes?
 
10:32 AM
If I were not to observe physically would it be possible to conclude that?
 
I'm not sure what that means. The man's acceleration is a regardless of whether anyone is watching him or not.
That is, if he holds an accelerometer it will have a reading of a.
 
precisely what reason do you give for justifying that both lift and him must have some same acceleration? It is intuitive for me but I'm trying to think of a justification for it
but then he'd have to use some external experiment to know that (if he uses accelerometer)
 
Because the man and the lift are in contact so their positions are the same i.e. x_lift(t) = x_man(t)
If we differentiate twice we get a_lift(t) = a_man(t)
 
0
Q: Please explain me the last term in the given statement

user586228 Having doubt in understanding the last term in the expression.Please givea detailed explanation to the calculation methodology.

 
Previously you had described case where the lift moves in such a way that man floats
 
10:35 AM
@JohnRennie Sir please help me with this
 
then we no longer have a contact between man and lift
 
Yes, if the man loses contact with the lift then the only force acing on him is the constant Fg = mg.
 
like if lift was moving downwards with greater acceleration than g
 
So now he accelerates at a constant g.
 
@JohnRennie so if man loses contact with lift, we can not say that net force sum on man= ma? where a is acceleration of lift itself
@JohnRennie based on this and the current point
 
10:38 AM
correct. The acceleration of the man is:
1. a if a <= g
2. g if a > g
 
oh damn
that is actually a very interesting point
 
@Buraian You may also try the uestion I posted..
question*
 
@user586228 if you have n electrons then they all repel each other. Yes?
 
ok
Yes
 
Thank you sir for the help, it's a bit difficult for me to fully understand the implications but I have understood the idea required for the question @JohnRennie
 
10:42 AM
So if the distance between electron number i and electron number j is r_ij, then the potential energy due to that repulsion is U_ij = +ke²/r_ij. Yes?
That's just the usual equation for potential energy of two charges.
@Buraian OK :-)
 
Correct..
 
So to get the total potential energy due to the electron repulsion you sum U_ij i.e. you do Σ_i Σ_j ke²/r_ij
Only you need to be careful not to double count i.e. don't sum both U_ij and U_ji
So the sum is only over j from zero to i.
 
I couldn't get the last explanation..
Please help me out
 
Suppose we have two charges, so both i and j can be 1 or 2
 
10:47 AM
So Σ_i Σ_j ke²/r_ij would give us:
ke²/r_00 + ke²/r_01 + ke²/r_10 + ke²/r_11
We obviously exclude i = j because a charge doesn't have potential energy due to itself, so we are left with:
ke²/r_01 + ke²/r_10
OK so far?
 
ok then..
 
But the PE between two charges is just ke²/r
And in our sum we double counted it.
Because we counted both i=1 and j=0 as well as i=0 and j=1.
So we eliminate the duplication by making the second sum only over j < i
 
Could not get this
now I got it
 
Sir if you have some time, could you tell me what you think the answer for this question I posted is?
 
11:03 AM
Ok then how is the second term different from the first term please explain this one
 
The second term is the same as the first term because r_01 = r_10. Both are just the distance between the two electrons.
 
Not that one ..the second term in my expression...That is what I am asking..
 
There are two sources of potential energy:
1. the electrons are attracted to the nucleus and this gives a negative PE
2. the electrons are repelled by each other and that gives a positive PE
The first term is the electron-nucleus PE and the second term is the electron-electron PE.
 
Thanks a lot for helping..
 
:-)
 
11:09 AM
And what about the first term in the expression?
 
The first term is the kinetic energy of the electrons.
 
Ok can you justify slightly..
What the terms signify....???
 
You mean what $\nabla^2$ means?
 
Laplacian operato but nothing more than that
operator*
I really want to know physically what it means..
 
I don't think there is a simple physical interpretation ...
 
11:20 AM
Just a Q , is quantum realm or time travel in real life possible ?.
 
Quantum mechanics is real but time travel is impossible.
 
Ohk.
 
What is the origin of kinetic energy of electrons with reference to the laplacian operator.
 
@JohnRennie while deriving the electric field at a point a distance $d$ away from an infinitely large thin uniformly charged electric plate, I used a closed cylindrical surface with one end on the plate and the other at a distance $d$ from the plate. I was able to do it, but first I had to show that the electric flux for the curved surface is zero, and I used an informal (yet logically sound) argument to do that. Could you hint me towards a formal way to show that electric flux for the...
curved surface = zero?
 
@AshishAhuja use symmetry.
The plate is infinite, so is move parallel to the plate in any direction the field cannot change.
 
11:27 AM
Is that really a formal way? I was looking for something rigorous if possible.
 
@JohnRennie Sir please justify the kinetic energy for electrons..
 
@AshishAhuja that is rigorous.
 
@JohnRennie hmm okay then, thank you.
 
Guys . I am going to start making notes for physics and chemistry on IPAD using Apple pen. It saves a lot of time. But it will hurt eyes more. Do you think I should do it ?
My only fear is that people say kids who wrote on notebooks are better in remembrance than kids on digital media.
Sorry to disturb . Please answer whenever anyone’s free and can help me.
I can arrange things better and write things that I may have left on the same using iPad.
 
Maybe just try it out and see if it works for you? I personally don't even make extensive notes, maybe I will have to for chem in 12th, and I seem to remember stuff just fine, so I don't think a general one-fits-all approach exists.
 
11:36 AM
Ohk.
Thanks @AshishAhuja
 
@Sarabsrimt I would personally make notes on tablet because 1) Saves time , 2) Save Trees and 3) I will save it in cloud so I never-ever lost them.
 
@JohnRennie Sir please explain how the kinetic energy term is derived..
I really do not understand this in quantum
 
@user586228 there isn't a simple explanation. I'm afraid you just have to accept it.
 
ok got you and what about the psi and E function?
Where on earth do I consider this in general...give me the practical analogy...
 
@Bhavay Do you but
 
11:44 AM
@Sarabsrimt but...?
 
I meant do you use it
Or just giving advice ?
@Bhavay
 
@Sarabsrimt No , I don't as I don't have a tablet/iPad . But I would definitely use it if I had one.
 
Ohk.
 

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