8. Let us now examine the relation which subsists between the values of and for the same point, that is, between the average electromotive force and the average displacement in a small sphere with its center at the point considered. We have already seen that the forces and the displacements are harmonic functions of the time having a common period.
![{\displaystyle [{\mathsf {E}}]_{\text{Ave}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/b7e67bd6ba66d7059a3b01d6bc0b15912d76bca7)
![{\displaystyle [{\mathsf {U}}]_{\text{Ave}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/01cf641733f9787e85fac4942bfd388b0811b9fb)
A little consideration will show that if the average electromotive force in the sphere is given as a function of the time, the displacements in the sphere, both average and actual, must be entirely determined. Especially will this be evident, if we consider that since we have made the radius of the sphere very small in comparison with a wave-length, the average force must have sensibly the same value throughout the sphere (that is, if we vary the position of the center of the sphere for which the average is taken by a distance not greater than the radius, the value of the average will not be sensibly affected), and that the difference of the actual and average force at any point is entirely determined by the motions in the immediate vicinily of that point. If, then, certain oscillatory motions may be kept up in the sphere under the influence of electrostatic and electrodynamic forces due to the motion in the whole field, and if we suppose the motions in and very near that sphere to be unchanged, but the motions in the remoter parts of the field to be altered, only not so as to affect the average resultant of electromotive force in the sphere, the actual resultant of electromotive force will also be unchanged throughout the sphere, and therefore the motions in the sphere will still be such as correspond to the forces.
Now the average displacement is a harmonic function of the time having a period which we suppose given. It is therefore entirely determined for the whole time the vibrations continue by the values of the six quantities
![{\displaystyle [\xi ]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/7937b3b086707a2cd76c537b79f8a84333b7cb46)
![{\displaystyle [\eta ]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/78f7f75df758408998cb86484003ab382c7e3f08)
![{\displaystyle [\zeta ]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/605184987ff9b2cdfb7b564d1f09e497a717ac02)
![{\displaystyle [{\dot {\xi }}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/7b2703f72b374b0a9e6d837163f838b68f101f87)
![{\displaystyle [{\dot {\eta }}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/6ee98c163879e4741a338d22b80dff1cee08e743)
![{\displaystyle [{\dot {\zeta }}]_{\text{Ave}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/0e55cfbe8b1e0fd7b6522153a8af4b893454a0a3)
at any one instant. For the same reason the average electromotive force is entirely determined for the whole time by the values of the six quantities
![{\displaystyle [{\text{X}}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/9288329066deb845844e2e40035627b943fb9e1d)
![{\displaystyle [{\text{Y}}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/cbd7ef0788854e6fe9862afa0c4e66f057d12331)
![{\displaystyle [{\text{Z}}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/3b4816b034adf29fefadcc576134d04250e495bf)
![{\displaystyle [{\dot {\text{X}}}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/9ffa4e9dda540ebc597b7d6082a252082838b621)
![{\displaystyle [{\dot {\text{Y}}}]_{\text{Ave}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/d198ad0b54717c39f7cd10d16e88478c6e10d23d)
![{\displaystyle [{\dot {\text{Z}}}]_{\text{Ave}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/032ed7999dfa32a7427d4b6eead2d357ca303699)
for the same instant. The first six quantities will therefore be functions of the second, and the principle of the superposition of motions requires that they shall be homogeneous functions of the first degree. And the second six quantities will be homogeneous functions of the first degree of the first six. The coefficients by which these functions are expressed will depend upon the nature of the medium in the vicinity of the point considered. They will also
