We know that the force acting on the area element dS of a conductor is,


It follows from symmetry considerations that the resultant force vector F directed along the z-axis, and hence it can be represented as the sum (integral) of the projection of elementary forces (1) onto the z-axis :

For simplicity let us consider an element area

Integrating this expression over the half sphere (i.e. with respect to cosθ between 1 and 0), we obtain
