where E denotes the electric force on a charge at rest, which is zero in the present case. Thus, according to Lorentz' theory, the charges on the faces would have only (ε - 1)/ε of the values which they would have in Hertz' theory; that is, they would be practically zero. The result of Blondlot's experiment was in favour of the theory of Lorentz.
An experiment of a similar character was performed in 1905 by H. A. Wilson.[1] In this, the space between the inner and outer coatings of a cylindrical condenser was filled with the dielectric ebonite. When the coatings of such a condenser are maintained at a definite difference of potential, charges are induced on thein; and if the condenser be rotated on its axis in a magnetic field whose lines of force are parallel to the axis, these charges will be altered, owing to the additional polarization which is produced in the dielectric molecules by their motion in the magnetic field. As before, the value of the additional charge according to the theory of Lorentz is (ε - 1)/ε times its value as calculated by the theory of Hertz. The result of Wilson's experiments was, like that of Blondlot's, in favour of Lorentz.
The reconciliation of the electromagnetic theory with Fresnel's law of the propagation of light in moving bodies was a distinct advance. But the theory of the motionless aether was hampered by one difficulty: it was, in its original form, incompetent to explain the negative result of the experiment of Michelson and Morley.[2] The adjustment of theory to observation in this particular was achieved by means of a remarkable hypothesis which must now be introduced.
In the issue of "Nature" for June 16th, 1892,[3] Lodge mentioned that Fitz Gerald had communicated to him a new suggestion for overcoming the difficulty. This was, to suppose that the dimensions of material bodies are slightly altered when they are in motion relative to the aether. Five months afterwards, this hypothesis of Fitz Gerald's was adopted by
