- #1
The field inside the conductor, induced by charge displacement, can be thought of as originating at the + charges on the left surface and ending at the - charges at the right surface. This field cancels the externally generated field inside the conductor, but isn't (very) present outside of the conductor. From far away, the shift of charges inside the conductor isn't significant, an observer out there just sees + and - charges in a relatively small space far away that cancel each other.Neitrino said:Dear willem2 and DaveE,
Let me ask another question...
"When you get far away from the conductor, it should look like the conductor had no effect. Like this:"
When an initial charged (with charge +Q) plate creates an electric filed it originates from the charged surface and penetrates into area A, then it penetrates into area B (inside the conductor thickness) where it is canceled by the induced filed - so if it is canceled inside the conductor how / why does it propagate onwards - into area C ?
Thank you so much for you kind explanations
If the conductor is not infinite in extent then the induced charge distributions on the surface will not be uniform. I believe you are using the approximation that the conductor is finite and that it is not in the same problem.Neitrino said:When an initial charged (with charge +Q) plate creates an electric filed it originates from the charged surface and penetrates into area A, then it penetrates into area B (inside the conductor thickness) where it is canceled by the induced filed - so if it is canceled inside the conductor how / why does it propagate onwards - into area C ?
SDL said:It actually does, don't forget you conductor sample is finite. The external electric field is always normal to a conductor's surface. If you insert a rectangular conductor into a uniform field, like it's shown on your drawing, what this field at the upper and the lower surfaces would be?
?alan123hk said:after the conductor is added, the electric field in all spaces does not change
It is good that you are happy but the diagram is incorrect. Your supposition is true only for flat sheets that have no edges (are of infinite extent). The real world is considerably more complicated.... so much for happiness.alan123hk said:BTW, the diagram below is something I came up with, I believe it has never been seen before, I am very happy with this diagram.
A conductor is a material that allows electric charges to flow through it easily. Examples of conductors include metals like copper and aluminum.
An electric field is a region in which electrically charged particles experience a force. It is created by a charged object and can be represented by lines of force.
A conductor in an electric field will experience a force due to the presence of the electric field. The charges within the conductor will redistribute themselves, resulting in an electric field inside the conductor that is equal and opposite to the external electric field. This causes the net force on the conductor to be zero, and it will remain in a state of electrostatic equilibrium.
A conductor allows electric charges to move freely, while an insulator does not. In an electric field, charges in a conductor will redistribute themselves to cancel out the external field, while charges in an insulator will remain stationary and experience a force due to the electric field.
The shape of a conductor can affect its behavior in an electric field. A conductor with sharp edges or points will experience a higher concentration of charges at these points, resulting in a stronger electric field and potential for discharge. A conductor with a smooth, rounded shape will distribute charges more evenly and have a weaker electric field.