Chapter 16
... All of the charge resides at the surface E = 0 inside the conductor The electric field just outside the conductor is perpendicular to the surface The potential is a constant everywhere on the surface of the conductor W = -q(VB – VA) = 0, no work is required to move a charge between two points that a ...
... All of the charge resides at the surface E = 0 inside the conductor The electric field just outside the conductor is perpendicular to the surface The potential is a constant everywhere on the surface of the conductor W = -q(VB – VA) = 0, no work is required to move a charge between two points that a ...
General Physics II
... From Gauss’ law, we can find the field at a distance r from some point by finding the flux through a sphere of radius r centered on that point. The flux through that sphere must simply be the net charge enclosed within the sphere (divided by 0 ). Outside of the spherical shell, what charge would be ...
... From Gauss’ law, we can find the field at a distance r from some point by finding the flux through a sphere of radius r centered on that point. The flux through that sphere must simply be the net charge enclosed within the sphere (divided by 0 ). Outside of the spherical shell, what charge would be ...
Electromagnetic Induction
... wire moves up through the field, the current moves in one direction. When the wire moves down through the field, the current moves in the opposite direction. If the wire is held stationary or is moved parallel to the field, no current flows. An electric current is generated in a wire only when the w ...
... wire moves up through the field, the current moves in one direction. When the wire moves down through the field, the current moves in the opposite direction. If the wire is held stationary or is moved parallel to the field, no current flows. An electric current is generated in a wire only when the w ...
