Page:A history of the theories of aether and electricity. Whittacker E.T. (1910).pdf/220

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Faraday.

established the accuracy of this law,[1] he found by a comparison of different electrolytes that the mass of any ion liberated by a given quantity of electricity is proportional to its chemical equivalent, i.e. to the amount of it required to combine with some standard mass of some standard element. If an element is n-valent, so that one of its atoms can hold in combination n atoms of hydrogen, the chemical equivalent of this element may be taken to be 1/n of its atomic weight; and therefore Faraday's result may be expressed by saying that an electric current will liberate exactly one atom of the element in question in the time which it would take to liberate n atoms of hydrogen.[2]

The quantitative law seemed to Faraday[3] to indicate that "the atoms of matter are in some way endowed or associated with electrical powers, to which they owe their most striking qualities, and amongst them their mutual chemical affinity."

Looking at the facts of electrolytic decomposition from this point of view, he showed how natural it is to suppose that the electricity which passes through the electrolyte is the exact equivalent of that which is possessed by the atoms separated at the electrodes; which implies that there is a certain absolute quantity of the electric power associated with each atom of matter.

The claims of this splendid speculation he advocated with conviction. "The harmony," he wrote,[4] "which it introduces into the associated theories of definite proportions and electro-chemical affinity is very great. According to it, the equivalent weights of bodies are simply those quantities of them which contain equal quantities of electricity, or have naturally equal electric powers; it being the electricity which determines tho equivalent number, because it determines the combining force. Or, if we adopt the atomic theory or phraseology, then the

  1. Exp. Res., §§ 713-821.
  2. In the modern units, 96580 coulombs of electricity must pass round the circuit in order to liberate of each ion a number of grams equal to the quotient of the atomic weight by the valenoy.
  3. Exp. Res., § 852.
  4. Ibid., § 869.