It is necessary because of the spherical geometry inherent in the physics. For example, if I have a point source antenna that creates spherical waves, the energy across any spherical surface centered about our source must remain constant in a lossless medium. That is, if we have a lossless medium, then the energy emitted must remain constant. If we emit spherical waves, then the entire energy spread across a given wavefront remains constat as it propagates out in space. If we were to look at the energy at a single point on the wavefront as the wave expanded/propagated, then we would see that the fields would drop off as 1/(4 \pi r^2) since the surface of the wavefront is expanding as a spherical surface.
This is where we get the 4\pi from. In terms of statics, we can look at Gauss' Law. If I place a single point charge at the center of a spherical Gaussian surface, then the total flux through the Gaussian surface of the electric field is proportional to the charge. Through the use of spherical symmetry we can actually derive the actual electric field from this relationship. The result is of course Coulomb's law and once again due to the spherical geometry we acquire the 4\pi factor. But since Coulomb's law is incorporated into Maxwell's Equations, we can move the 4\pi off of Coulomb's law to Gauss' law and not change the resulting physics.
Your explanation was good.