Introduction
Continuing in the field of the field of physics, but this time I will comment on the conductor in electrostatic equilibrium, you must know the potential difference between two points is the work overloaded by the electrostatic field, to be able to move the unit of positive charge from one point A to another B, since my reader friend must also know that the electric flux through a surface closed in any way is equal to the charge enclosed in its interior divided by the permissiveness of the vacuum. The unique thing about all this is that a full-body conductor to mention the body itself, where the electric charges can move freely, thanks to the constitution of atoms and that the body is also in our own, they have negative and positive charges, there is also the case of the negative charge goes when the so-called excess of electrons is evident.
Continuing with the computer ideas we have that a conductive material this can also be one that allows the transport of electric charge, as in the case of metallic solids they are good conductors, since their valence electrons are little bound to atomic nuclei Thanks to this, it allows them to move easily through the solid, which is why they are free electrons. In the case of the field created by two parallel planes with equal and opposite charges, it is considered when point P1 is chosen to be between both planes, the field produced by each of the faces will be made. If the point P2 is not included between the planes, the total charge enclosed by the surface will be zero, so the flow Ø = 0, where ∫ Exds = 0 and E = 0.
Now, all points of the conductor must have the same potential and the work to go from one point to another is null E = 0. All charges are distributed on the surface of the conductor: V (A) -V (B) = ∫ ABE x dr = 0. Thanks to Coulomb's law, the reader friend charges of the same sign will repel each other, evading that they are moving away and the field is zero within a null surface, All conductors tend to electrostatic equilibrium, that is, if an agglomeration of charge in a conductor is abandoned At its own strength, it disperses until the charge density at every point inside the conductor is zero.
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