Is it possible to charge a conducting sphere from the inside

In summary, the conversation discusses the concept of electrostatic equilibrium and the behavior of electric fields inside a conducting sphere. It is stated that at electrostatic equilibrium, the electric field inside a conductor will be zero regardless of the shape of the cavity. The Law of Gauss is mentioned as the reason for this. The conversation also mentions that this principle applies to all conductive objects, not just spheres. There is a discussion about the effects of gravity on electric fields and how they are typically too small to be detected in a laboratory. The conversation then goes on to talk about different scenarios where the electric field may not be zero, such as in cases of external forces or inductive currents. The conversation ends with a simpler example of making current flow through a
  • #1
CinaMarcina
2
0
Hello..
i just saw this amazing Forum and wanted to contribute, so here is my first question and i hope i get an answer x.d
I was told that at electrostatic equilibrium, the electric field inside a conducting sphere will be ZERO,
How can i charge thissphere from the inside, so the Electric field in side it won't equal zero.?
 
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  • #2
Electric field inside a conductor's cavity (in the classical realm atleast) will be zero, no matter what the shape of the cavity is. You will have an electric field only if you physically place a charge in the cavity (here inside the sphere).

This directly follows from Gauss's Law.
 
  • #3
I don't really get what you are talking about ...
Why would you charge the sphere from the inside ?
Then sure, you would have an electric field in there (assuming it is a hollow sphere and you somehow got your charge in there),but if the charge somehow
gets the chance to distribute itself along the sphere,it will do so in a way that results in 0 electirc field inside.

This principle isn't just exclusive to spheres.
ANY conductive object however charged has zero electric field inside.
It is a bit like saying there is no pressure difference in a gas filled container (in the absence of gravity)
This follows from the fact that if there was a difference in pressure / (electrostatic potential for your problem) inside it, this differnce would cause the gas / (charges)
to redistribute in a way that is "stable" and therefore does not cause any current to flow.
In other words some arrangement that has no pressure gradient /(electric field) inside it.
 
  • #4
Then how about.
Actually, it is not necessary for the electric field to be zero in a conductor at electrostatic equilibrium. The true condition is not that E=0. The requirement is that the force on charges is such that they can not move in response. Therefore the condition is that the force on charges is zero in the conductor. And for the surface, the force must be perpendicular to the surface. For instance, even a perfect conductor would have a non-zero electric field inside of it if it is in a gravitational field. And I\'m sure you could come up with some other cases as well. The effects due to gravity are small, and the other cases probably perverse, so this is rarely discussed (although old papers have been published about this).
 
  • #5
That's why I was careful to mention "in the classical realm". In reality, electric forces on an electron far outweigh any other kind of forces.
Doing some rough order of magnitude calculations, gives you that the gravitational field will be at least 10^20 order of magnitude lesser than electric field strength. This is impossible to detect in a lab.

Even if you make the field strengths same (maybe around a black hole/neutron star or something),
the gravitaional force/electrical force ~ m/q ratio of the electron ~ 10^-11. which is again small but might be detectable.

Now if you can to go in that domain, let's see: Considering the continuous generation/annihilation of virtual photons (electrostatic force carriers) in free space might give some interesting results. What if we place a black hole inside conducting cavity. Considering the net charge on the black hole to zero, there will still be some detectable photons coming from the event horizon, which might interact with the electrons. This might lead to a net charge inside the cavity surface.
 
  • #6
I actually came up with an easier example.
Just fling your object really fast through a really strong magnetic field.
It will act like some kind of mechanical hall effect sensor where the electric field is not created by
the electric current but the bulk movement of the object.
However you could argue that the lorentz force is fundimentally an electric effect... :I

Actually now that i think about it every generator and transformer defies the principle of
0 E-field inside it, but those are not in a stable state...
The inductive currents slow down the relative movement.

The Law should be more like: "In any conductor on which no external forces act and which is in a stable state there is
no electric field.(If you approximate charge to be continuous)"

Because if you imagine a low number of charge carriers on the object,
it becomes apparent that it is impossible to arrange them in a way that would result in exactly 0 electric field.
But since the "charge quanta" are so tiny the approximation of a continuous charge distribution is valid
 
  • #7
Tazerfish said:
Actually now that i think about it every generator and transformer defies the principle of
0 E-field inside it, but those are not in a stable state...
The inductive currents slow down the relative movement.

The Law should be more like: "In any conductor on which no external forces act and which is in a stable state there is
no electric field.(If you approximate charge to be continuous)"

Because if you imagine a low number of charge carriers on the object,
it becomes apparent that it is impossible to arrange them in a way that would result in exactly 0 electric field.
But since the "charge quanta" are so tiny the approximation of a continuous charge distribution is valid

I agree with you but then I was going more "complicated" cause I was still trying to preserve the conditions of electrostatics. You're right in restating the law but then the OP already mentions the E field being zero in electrostatic conditions. And in electrostatics the electric force on an electron far exceeds any other kind of force.

P.s. A more 'simpler' (not electrostatic) example: just make current flow through the conductor which has the cavity!
 

Related to Is it possible to charge a conducting sphere from the inside

1. Can a conducting sphere be charged from the inside?

Yes, it is possible to charge a conducting sphere from the inside. This can be achieved by placing an electric charge inside the sphere or by connecting the sphere to an external power source.

2. Will the charge on the inside of the sphere affect the charge on the outside?

Yes, the charge on the inside of the sphere will have an impact on the charge distribution on the outside. This is because charges will repel or attract each other, causing a redistribution of charges on the surface of the sphere.

3. How does the charge distribution on the inside of the sphere affect its electric field?

The charge distribution on the inside of the sphere will determine the strength and direction of the electric field inside the sphere. This is because the electric field is influenced by the distribution of charges in a given space.

4. Can a conducting sphere be charged from the inside if it is already charged on the outside?

Yes, a conducting sphere can still be charged from the inside even if it is already charged on the outside. However, the existing charge on the outside may affect the distribution of charges on the inside and the resulting electric field.

5. Is there any limit to how much charge can be placed on the inside of a conducting sphere?

There is no specific limit to how much charge can be placed on the inside of a conducting sphere. However, the amount of charge that can be placed will depend on the size and material of the sphere, as well as the strength of the electric field that can be sustained before the sphere experiences electrical breakdown.

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