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5:51 AM
@JohnRennie Hello.
 
@Abcd Morning :-)
 
@JohnRennie Aren't 1 and 2 in series?
 
Nope!!!
 
Start at the battery cathode. Is there a route that takes you round the circuit and back to the anode that passes through C1 without going through C2? If so then they are not in series.
 
Okay, got it.
 
6:30 AM
@JohnRennie Today can you answer that dielectric question?
 
Abcd
Abcd I am sorry not to arrived here before but I am not really conversant with chat.
 
@Farcher Okay, are you free right now to discuss about it?
 
For about 20 minutes.
 
Okay
@Farcher I have marked the imaginary metal plate with red. How can we say that the lower plate of the capacitor has the same magnitude of charge as the red plate?
 
The red metal plate has a net zero charge on it.
 
6:43 AM
yes
 
If the top plate of the capacitor is has positive charge on it the top of the red plate has an equal amount of negative charge on it.
 
why?
 
That charge is
 
What about the induced charges of the dielectrics? Don't they affect it?
 
Those induced charges on the dielectric induce the charges on the metal plate.
 
6:46 AM
but that magnitude is less
magintude of induced charges is given by $Q(1- 1/k)$ if I am not wrong
 
If there were no induced charges on the red plate then there would be an electric field inside the red plate.
 
my point is that the magnitude of the induced charges is less than the magnitude of charge on the capacitor plate
@Sid Do you have any idea
 
Forget about your arrangement and consider a capacitor with dielectric inside it. One plate of the capacitor is earthed. To the other plate I add a charge +Q. How much charge is there on the bottom plate of the capacitor?
 
@Farcher -Q/2 ?
 
So when you charge a capacitor the magnitude of the charges on each of the plates is different?
 
6:56 AM
inner surfaces of the plates would have same magnitude
 
So that is what happens to the top of the red plate of your capacitor.
I wiill have to go in a minute or so as I have a dental appointment.
 
 
1 hour later…
8:07 AM
@Abcd I think I've come up with a way of showing this ...
 
Can anybody tell me where do I read stuff to understand how electricity flows in some object ? I was reading chapter 29 in HRK, but it mentioned stuff like "lattice crystals" and "valence electrons" and "polarisation" which I didn't understand a bit.
Or alternatively, you can also tell where I can read to have an understanding of "lattice crystals" and "valence electrons" and "polarisation" (I have these in my chemsitry book too but my book is very very very very bad).
Thanks
 
 
2 hours later…
9:56 AM
Any wbjeeian here?
 
 
3 hours later…
12:33 PM
Which is more preferable among IIEST and JU if I want to go for higher studies? Any ideas? @Blue
 
Sid
12:45 PM
@MadhuchhandaMandal Not of WB, but JU trumps IIEST in all respects, I think. NIRF rankings say so too
 
@Sid Triumphs you mean?
 
Sid
@MadhuchhandaMandal See the verb form
 
@Sid okay :-)
 
 
3 hours later…
4:21 PM
@JohnRennie when will you be telling it?
 
@Abcd now if you want ...
 
@JohnRennie Okay.
 
OK. Let's start with this diagram:
 
@JohnRennie by $\epsilon $ you mean dielectric constant $k$ ?
 
I'm not going to insert any imaginary metal plates. What I'm going to do is calculate the voltage $V$ by minimising the electrostatic energy.
No, I mean $\epsilon$ where $\epsilon = k\epsilon_0$
 
4:23 PM
@JohnRennie how and why will you minimise it
@Sid can you please see this problem^
 
To start with you have to take on trust the equation for the energy density of an electric field i.e. the energy of the field in joules per cubic metre. The equation is $$ \rho = \tfrac{1}{2} \epsilon E^2 $$
 
@JohnRennie yes, I have derived it too
 
where $E$ is the field strength in volts per metre
 
yes
 
OK, for the upper part of my diagram the potential difference is $V_0 - V$ and the distance is $d_1$ so the field strength is $$ E_1 = (V_0 - V)/d_1 $$
 
4:26 PM
yes'
 
And likewise for the lower part the field strength is $$ E_2 = V/d_2 $$
 
yes''
 
If $A$ is the area of the plates then the volume of the upper part is $Ad_1$
 
yes
 
And the total energy is the energy density times the volume so: $$ U_1 = \tfrac{1}{2} \epsilon_1 \left(\frac{V_0 - V}{d_1}\right)^2 A d_1 $$
 
4:29 PM
yes'
 
And likewise the total energy of the bottom part is: $$ U_2 = \tfrac{1}{2} \epsilon_2 \left(\frac{V}{d_2}\right)^2 A d_2 $$
 
@Abcd ... Is it $C= \frac{4}{3}$ ... ? I might be wrong ...
 
@NehalSamee no
 
And we add the two to get the energy of both parts:
 
@JohnRennie yes''
 
4:31 PM
$$ U = \tfrac{1}{2} \epsilon_1 \left(\frac{V_0 - V}{d_1}\right)^2 A d_1 + \tfrac{1}{2} \epsilon_2 \left(\frac{V}{d_2}\right)^2 A d_2 $$
 
yes'''
 
Which I'll rewrite to simplify it:
$$ U = \frac{\epsilon A}{2d_1} (V_0^2 - 2V_0V + V^2) + \frac{\epsilon_2 A}{2d_2} V^2 $$
 
yes
 
Sid
C is just 4, I think.
 
@Sid why?
 
4:34 PM
Now I want to find out the value of $V$ that minimises the total energy $U$, so I just differentiate to get $dU/dV$ then set that expression equal to zero. OK so far?
 
@JohnRennie why do you want to minimise it?
 
Sid
Let JR finish. Then, we can proceed with this...
 
Any system will settle into the lowest energy possible for it. That means the value of the voltage $V$ will be the one that minimises the total electrostatic energy.
3
 
K
 
OK, so if we take my equation for $U$ and differentiate it then set it equal to zero we get:
$$ 0 = \frac{\epsilon A}{d_1} (V - V_0) + \frac{\epsilon_2 A}{d_2} V $$
Or:
$$ \frac{\epsilon_1 A}{d_1} (V_0 - V) = \frac{\epsilon_2 A}{d_2} V $$
 
4:40 PM
then?
 
Now this should be starting to look familar ...
 
its C
C1V0 - C1V = C2V
 
Because $\epsilon_1 A/d_1$ is the capacitance of the upper part if you treat it as a separate capacitor. And likewise for the bottom part.
And CV = Q, so this is just the condition for two capacitors in series: $$ Q_1 = Q_2 $$
And that's why the upper and lower parts behave just as if they were two separate capacitors in series.
 
Oh wow Thanks @JohnRennie, got it.
 
@Abcd sorry it took a while, but I was trying to think of a simple way to explain it.
 
4:44 PM
Okay.
@JohnRennie Do you have any idea about the previous problem?
 
@Abcd tomorrow ...
 
My teacher did it in 2 seconds saying that "it's hit and trial and obvious."
@JohnRennie Okay. @Sid will explain then I guess.
@Sid Are you there
 
Sid
Yes. First tell me, what is your first idea on seeing that problem.?
 
@Sid my first idea isnt good... And I now know its wrong ...so leave it.
 
Sid
Being wrong isn't the point. I want to know where to start. So, Your first idea will be helpful.
 
4:49 PM
I thought that maybe inifnite capacitors would maximise it
so we need C to be greater than that
which is obviously wrong
And we know how to calculate the equivalent capacitance of infinite ladder
but not of finite ladder having n sections.
 
Sid
Good. Your idea isn't far off. And, this is actually an infinite ladder..
We know, the value of capacitance is independent of "n". So, even if there's one ladder or infinite ladder, the capacitance will remain same.
Do you agree?
 
@Sid ... Can we say that the equivalent capacitance of C , 4 and 2 will again give C ...?
 
Sid
@NehalSamee Exactly!
@Abcd Is it clear or should I draw you a diagram?
 
@Sid Why are you considering it to be infinite
 
Sid
@Abcd Okay. Let it be finite. For the value of C, I can make the value of "n" as large as I want, but the equivalent capacitance won't change. Yes?
 
5:01 PM
@Sid yes
 
Sid
@Abcd Okay. So, as large as I want, means I can keep adding the ladder and the equivalent capacitance won't change => This is an infinite ladder.
 
@Sid he has clearly mentioned its a finite ladder
 
Sid
@Abcd No. He mentions that the ladder ends at C. What if, C is also a network of many capacitance?
I agree this might not be very intuitive though..
 
@Sid Please read the first three words of the question
 
Sid
@Abcd So? If you read the whole question, it only says that the ladder terminates at C. It doesn't say what C could be.
Anyway, let's assume it's not infinite.
At least, we know that the equivalent capacitance doesn't depend on "n".
 
5:07 PM
He has also mentioned that the equivalent capicitance is independent of sections in between so it doesn't matter if it is 1,2,3 or infinity
 
Sid
(Be back in 15 minutes. I have to go take supper)
 
@JohnRennie awesome explanation sir. This was taught to us in a way I didn't get but the way you explain it's perfect.
 
Sid
@Abcd Okay back. Let's look at it this way.
 
ok
 
Sid
Let the equivalent capacitance be $C_eq$
if I remove the elements to the left of the Yellow line, Then, still the equivalent capacitance will remain same because I just removed one ladder and equivalent capacitance is independent of "n".
So, basically everything right to the Yellow line has equivalent Capacitance same as the original. Do you agree? @Abcd
 
5:25 PM
yes
 
Sid
So, we can replace the entire thing in the right as $C_e$
Meaning, we have only a simple Ckt. to solve now. @Abcd
Do you see why this is similar to the infinite network problem?
 
yes
 
Sid
There's another small thing that you need to take care of. That is, the equivalent capacitance between A and B is actually C!
To prove that, since equivalent Capacitance is independent of "n" where "n" is the number of ladders of 2 and 4, let's put n=0. What do you get? @Abcd
 
C
 
Sid
And since, equivalent capacitance is independent of "n", C is actually the equivalent Capacitance between A and B!
 
5:29 PM
yes
then @Sid
How to calculate the value of C
 
Two hemispherical shells of radius 2R and R with charges Q2 & Q1 respectively are placed coaxially
Calculate the force of interaction
 
@AvnishKabaj Calculate the PE of the system
And F = -dU/dx
 
I got (Q1•Q2)/(144e•R^2)
@Abcd I don't think it's that easy
 
@AvnishKabaj whats the answer
 
@Abcd don't know
 
5:34 PM
@AvnishKabaj then how will you verify your answer
 
Sid
 
@Abcd our phy sir will give is the answer tomorrow
 
@AvnishKabaj No, its that easy. Tell me the flaw in my reasoning
@AvnishKabaj Which chapter are you on
 
Try to solve it
Get an answer
Then tell me
 
Sid
@Abcd We see, 4 and $C_e$ in series. Then, that is in parallel with 2. The entire network is equal to $C_e$
 
5:35 PM
I'll let you know if it was correct tomorrow
 
@AvnishKabaj Alternatively, find the capacitance of the system
 
Sid
You can solve after that.
 
And use U = 1/2 CV^2
 
Man if it's that easy then just give an answer
 
@Sid ok
 
5:36 PM
@Abcd that makes no sense
Force
Not potential
 
@AvnishKabaj F= dU/ dx!!!!
Thats how we calculated the force of interaction for parallel plate capacitor too!
 

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