In the immediate proximity of each of point charges, the contribution from the other charge to the total field strength is negligibly small, and hence the electric field lines emerge from (enter) the charge in a spatially homogeneous bundle, their total number being proportional to the magnitude of the charge. Only a fraction of these lines gets into a cone with an angle 2α at the vertex near the charge +q1 The ratio of the number of these lines to the total number of the lines emerging from the charge + q1 is equal to the ratio of the areas of the corresponding spherical segments:
Since the electric field lines connect the two charges of equal magnitude, the number of lines emerging from the charge +q1 within the angle 2α is equal to the number of lines entering the charge -q2 at an angle 2β. Consequently,
an electric field line will not enter the charge - q2.