The same diagram enables us to see what will be the distribution of electricity on one of the oval figures, larger at one end than the other, which surround both centres. Such a body, if electrified with a charge 25 and free from external influence, will have the surface-density greatest at the small end, less at the large end, and least in a circle somewhat nearer the smaller than the larger end.
There is one equipotential surface, indicated by a dotted line, which consists of two lobes meeting at the conical point . That point is a point of equilibrium, and the surface-density on a body of the form of this surface would be zero at this point.
The lines of force in this case form two distinct systems, divided from one another by a surface of the sixth degree, indicated by a dotted line, passing through the point of equilibrium, and some what resembling one sheet of the hyperboloid of two sheets.
This diagram may also be taken to represent the lines of force and equipotential surfaces belonging to two spheres of gravitating matter whose masses are as 4 to 1.
119.] In the second figure we have again two points whose charges are as 4 to 1, but the one positive and the other negative. In this case one of the equipotential surfaces, that, namely, corresponding to potential zero, is a sphere. It is marked in the diagram by the dotted circle . The importance of this spherical surface will be seen when we come to the theory of Electrical Images.
We may see from this diagram that if two round bodies are charged with opposite kinds of electricity they will attract each other as much as two points having the same charges but placed some what nearer together than the middle points of the round bodies.
Here, again, one of the equipotential surfaces, indicated by a dotted line, has two lobes, an inner one surrounding the point whose charge is 5 and an outer one surrounding both bodies, the two lobes meeting in a conical point which is a point of equilibrium.
If the surface of a conductor is of the form of the outer lobe, a roundish body having, like an apple, a conical dimple at one end of its axis, then, if this conductor be electrified, we shall be able to determine the superficial density at any point. That at the bottom of the dimple will be zero.
Surrounding this surface we have others having a rounded dimple which flattens and finally disappears in the equipotential surface passing through the point marked .
The lines of force in this diagram form two systems divided by a surface which passes through the point of equilibrium.
