Electric Flux: The flux Φ of an electric field E through a surface
S is given by the integral
Φ = ∫E.ds where the integral is over the
surface S.
Gauss's Law for the Electric Field: The net flus through a closed surface S is proportional to the total charge Q enclosed by the surface.
∫ E.ds = Q
ε0
The Electric field inside a closed spherical shell of charge is exactly 0.
The electric field outside a spherically symmetric ball of charge is the same as if all the charge were concentrated in a point at the centre of the sphere.
NOTE: The charge does NOT have to be uniformly distributed; it must simply depend only on r and not on the angles.
The electric field in a region entirely surrounded by a conductor is exactly zero unless there are other charges in that region.
The electrostatic potential V a distance r>>d from a dipole made from
charges Q separated by d is given by

The field from an infinite straight line of charge with density λ
Coulombs/metre depends only on the perpendicular distance ρ from the line
has magnitude
E = __λ____
2πε0 |ρ|
and points perpendicularly outwards (or inwards) from the line.
The field from an infinite flat sheet of charge of density σ points
away from the sheet and has magnitude
E = σ independent of the distance from the sheet.
2ε0
The electric field E very near the surface of a conductor is perpendicular
to the surface and causes (or is caused by) a local charge density σ where
E = σ .
ε0