Electric field is zero inside a conductor?

In summary, the physical explanation for the fact that the electric field is zero inside a conductor in electrostatic equilibrium is that no charges can be moving in this state. This means that the macroscopically averaged electric field is zero, as determined by the Gauss Law. This phenomenon is known as electrostatic shielding and is a result of charges resting on the surface of the conductor, leaving no charge inside the cavity. This explanation also assumes that there are no currents flowing and all charges have had time to settle down.
  • #1
Ebn_Alnafees
7
0
what is the physical explanation of the fact that the electric field is zero inside a conductor? :confused:
 
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  • #2
what is the physical explanation of the fact that the electric field is zero inside a conductor?

This is not true in general, but it is true in the realm of electrostatics. That is, if we charge a conductor, and allow it to reach equilibrium, then the electrci field is zero inside.

This is because, in equilibrium, no charges can be moving. The only way for this to be is if the (macroscopically averaged, don't think of particles think of fluid) electric field is zero.
 
  • #3
Or... Are you thinking Faraday's cage kind of thing?
 
  • #4
.. I think Crosson's explanation dealt with Faraday's cage.

?
 
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  • #5
The more simple explanation is using the Gauss Law.When a conductor is charged , after equilibrium is reached , charges rest on the surface of the conductor , and inside a cavity , that is open space no charge resides , by Gauss Law , no electric field exists inside it and hence these cavity is kept protected from outside electrical influences , phenomena called "electrostatic shielding'.

BJ
 
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  • #6
thank you all i think i got it
 
  • #7
The electric field is determined by the way in which the voltage changes from
place to place. If you are inside a metal sphere, the voltage is the same
everywhere. Since the voltage isn't changing as you move around, the electric
field measures as zero everywhere inside the sphere.
 
  • #8
As somebody else said, the electric field is only zero in an electrostatic situation, in which it is assumed that all the charges have had time to "settle down" before we look at the field. We also assume there are no currents flowing (obviously, a wire carrying current has an electric field inside, or else electrons wouldn't move along it).

If there was a field inside a conductor in electrostatic equilibrium, then the free charges in the conductor would accelerate in the direction of the field - which would mean the conductor wasn't in equilibrium - a contradiction. Hence, the conclusion follows.
 
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1. What is an electric field?

An electric field is a physical quantity that describes the influence of electric charges on each other. It is a vector quantity, meaning it has both magnitude and direction.

2. Why is the electric field zero inside a conductor?

Inside a conductor, the free electrons are able to move freely and redistribute themselves in response to an applied electric field. Due to this redistribution, the net electric field inside the conductor becomes zero.

3. What is the significance of a zero electric field inside a conductor?

A zero electric field inside a conductor means that the charges within the conductor are in a state of equilibrium, and there is no movement of charge or current. This is a fundamental property of conductors and is essential for many electrical applications.

4. Is the electric field zero at the surface of a conductor?

No, the electric field is not necessarily zero at the surface of a conductor. It depends on the shape of the conductor and the distribution of charges on its surface. However, the electric field inside the conductor will always be zero.

5. Can an electric field be zero in a non-conducting material?

Yes, an electric field can be zero in a non-conducting material if there are equal and opposite charges present that cancel out the field. This is known as electrostatic equilibrium and is a common occurrence in insulators.

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