I found a simple example where the centre of charge fails - when we place a charge +q at the centre of hollow spherical shell, -q amount of charge is uniformly induced on the inner surface and +q amount of charge is uniformly induced on the outer surface.
Of course the centre of charge of the inner -q coincides with the point charge +q. But I think we can use the centre of charge analysis only beyond the boundary of both charge distributions or in other words, it can be used only at points outside the inner sphere.
The electric field and the potential inside the cavity is not zero and constant respectively as suggested by the centre of charge analysis. However, the field is due to the point charge alone and potential is due to both the variable potential due to point charge and constant potential due to the -q amount of charge on the inner surface and +q amount of charge on the outer surface.
@JohnRennie So the main point I was missing was - using the centre of charge analysis within the boundary. Or in other words when we apply this method, on converting -q amount of inner induced charge to a point charge of same value at the centre at an internal point, the charge distribution passes through the point under our attention.
@JohnRennie Are you using the same type of formula that we use to find centre of mass sir? I think here the centre of positive and negative charges don't coincide. If they coincide do you refer to the origin as the centre of the charge distribution, sir?
If you take any arbitrary distribution of charges it creates a field that can be written as a sum of a monopole, dipole, quadrupole, octopole, etc.
Your centre of charge idea is exactly the monopole component, and in many cases this is the dominant component so the centre of charge is an excellent approximation.
Where it fails is when the other components become large. A pure dipole is an extreme example of this since the monopole component is zero.
@JohnRennie Ok sir. Sounds like expressing $\sin x$ (or other functions) as Taylor expansions. So more the number of terms like octupole, 14-pole, 140000-pole, … the better the approximation. Am I right, sir?
Fine sir. I see how it's zero for a dipole. I think by "centre of charge" analysis I meant something different - analysing whether the centre of all positive charges is same as all centre of negative charges where I compute the integral only for charges of one type.
@JohnRennie: Is there anything else I need to know regarding this for now, sir?
Ok sir. I'm having a doubt in the following question:
Question:
Capacity of a spherical capacitor is $C_1$ when inner sphere is charged and outer sphere is earthed and $C_2$ when inner sphere is earthed and outer sphere is charged. Then $C_1/C_2$ is ($a=$radius of inner sphere, $b=$radius of outer sphere)
(a) $1$ (b) $a/b$ (c) $b/a$ (d) $\frac{a+b}{a-b}$
My doubt:
First of all how can capacitance depend on which of the two plates is connected to the earth? It's a property of the capacitor as a whole right? And must be $\frac{4\pi\varepsilon_0 ab}{b-a}$ right sir?
Fine. I forgot to tell. I initially chose option (a) $1$, but the key and the solution states it's $a/b$ (option b). Do you wish to see the solution provided by the book sir?
Then they divide this to give $a/b$. But I don't see how as I mentioned earlier.
@JohnRennie: And there was no explanation for the formula for $C_2$. I understood the derivation of $C_1$ which is the normal capacitance of a spherical capacitor which I learnt a long time ago but the second formula seems different. Why do they take the radius of the inner sphere to be $b$ in the numerator and to be $a$ in the denominator?
If you earth one of the plates you fix the potential of that plate to be zero. e.g. if you earth the outer plate the potential has to be zero meaning the field outside the outer plate must be everywhere zero.
If you earth the inner plate then the potential of the inner plate must be zero, so if you integrate radially outwards from the inner plate to infinity the result must be zero. That means the field outside the outer plate is no longer zero i.e. there must be a net non-zero charge on the two spheres.
@GuruVishnu if you earth the outer plate then its potential is zero, so if you integrate the field radially from the outer plate out to infinity the result must be zero. But there is no charge outside the outer plate, so the only way for the integral to be zero is if the field outside the outer plate is everywhere zero.
Ok sir. So are we going to fix the potential difference between the two plates and find the ration of charges in the capacitor system to find the required ratio of capacitances. This seems simple.
@JohnRennie: Again it comes to be $1$ sir. For both the cases, I get $$V=kq/b - kq/a$$ where $q$ is the charge on the inner surface of the outer sphere and outer surface of the inner sphere.
Consider the following cases in relation to your question:
Inner sphere is grounded.
a) grounding the outer surface of the inner sphere
If you ground the outer surface of the inner sphere, the inner sphere becomes irrelevant and you get single spherical capacitor (the other one at infinity) ...
With the outer sphere earthed the charges are equal and opposite. With the inner sphere earthed some charge flows from earth onto the inner spere and the charges become unequal.
I agree sir. I'm not worried about an intuitive understanding but that answer seems to suggest connecting the two surfaces of a shell has different effects on the capacitance.
When you find time, can you please see the answer linked above?
Consider the following cases in relation to your question:
Inner sphere is grounded.
a) grounding the outer surface of the inner sphere
If you ground the outer surface of the inner sphere, the inner sphere becomes irrelevant and you get single spherical capacitor (the other one at infinity) ...
It seems the two sub cases under the main two cases is irrelevant but the reason seems to be valid.
And that user manages to get the final expression we got.
Yes sir. But doesn't that seem different - connecting either the inner surface of the outer plate or the outer surface of the inner plate must have the same effect right?
@JohnRennie Grounding both the plates? Not that sir. I meant he managed to get two different results each for grounding the outer surface and the inner surface of the inner sphere.
In Concepts of Physics by Dr.. H.C.Verma, in the chapter on "Capacitors", in page 144, under the topic "Capacitor and Capacitance" the following statement is given:
A combination of two conductors placed close to each other is called a capacitor. One of the conductors is given a positive char...
The way I would look at this is: suppose we start with neither sphere earthed and add charges $q$ and $-q$ in the usual way. Then we earth one of the plates, find the new voltage and calculate $C = q/V$ using the charge we originally put on the spheres i.e. ignoring any change due to charge flowing to or from earth.
But this is what I can interpret from "ignoring any change due to charge flowing to or from earth"; Can you please tell which point I'm misinterpreting, sir?
Suppose we put a charge $q$ on the capacitor then earth the outer sphere. No charge flows to or from earth and the potential difference between the spheres remains unchanged.
Now we put the same charge on the capacitor then earth the inner sphere. This time the charge on the inner sphere changes because some charge flows between the inner sphere and earth. This changes the potential difference $V$ between the spheres, so it changes the value of $q/V$. Yes?
Fine sir. I think that's where I'm facing confusion. Based on the question linked above, Andrew states charge on a capacitor is the amount of charge that flows when the two plates are connected. This means the charge must be the one on the facing surfaces. I don't understand why we need to consider $q$ as the one present at the beginning.
Suppose we place a charge $q$ on the capacitor then earth the inner sphere. The charge on the outer sphere remains at $q_b=q$ while the charge on the inner sphere changes to $q_a = -\frac{a}{b}q_b$. Yes?
So the charge that flows between the plates when they are connected must be $q_b$, because the outer sphere started with a charge $q_b$ and ended with a charge $0$ and it is only connected to the inner sphere so that charge $q_b$ must have flowed between the spheres.