32 I KINETIC ENERGY OF ELECTRICITY IN MOTION [I] The kinetic energy of the electric flow in one cubic milli- metre of a copper wire, which is traversed by a current of density equal to 1 electromagnetic unit, amounts to less than 0.008 milligramme-millimetre. As the kinetic energy is half the product of the mass by the square of the velocity, the mass of the positive electricity in 1 cubic millimetre e.g. if v = 1 mm sec m 10 sec 0.008 mg v2 the mass of positive electricity <0ยท008 mg., <00008 mg., etc. But we must bear in mind the possibility of the kinetic energy of the current exceeding the limit here marked out, without the observations necessarily being erroneous on that account. For if the conductivity of the metals is in the ratio of the densities of the electricity in them, then the electro- motive forces arising from inertia will be equal in two wires of equal resistance, whatever be the material, length, and cross- section of the wires. In this case the extra-currents from the four branches of the bridge, in so far as they were due to mass, would also be equal, and would thus neutralise each other. It is only on the assumption that the above propor- tionality does not exist, but that the density of electricity is approximately the same in different conductors, that it is allowable to neglect, as we have done, the effect of the mass moved in the short branches of German-silver and of gas- carbon. Vice versa, if by some other method we succeeded in prov- ing that the kinetic energy of the electric current exceeds the limit stated, the above experiments would show that the densities of electricity in the materials used are in the ratio of their conductivities. A decision as to the possibility mentioned could theo- retically be obtained by dynamometric experiments, or by observing the values at different times of induction and extra- currents; but in practice all the arrangements of experiment