One Hundred Years of Electrons.

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ONE HUNDRED YEARS OF ELECTRONS.

On April 30, 1897, at a meeting of the Royal Institution in London, physicist Joseph John (J.J.) Thomson declared that cathode rays lighting up a fluorescent screen were made of negatively charged particles. Thomson boldly proclaimed that these particles--which we now know as electrons--could be found in all atoms. The term "electron" as it applied to electricity actually came about in 1891 to describe the unit of electric charge in a chemical reaction. The electron was the first known subatomic corpsucle and its discovery marks the advent of particle physics. Michael Riordan (editor of SLAC Beamline, whose Spring 1997 issue is devoted to the electron centennial) refers to the electron as a truly "industrial strength" particle, since it is the workhorse of electronics, including television, telephones, and personal computers. (Many of these devices organize electrons inside transistors which were themselves developed exactly half a century ago.) Labor saving devices aside, electrons are of course the outer constitutents of all atoms and the principal currency of exchange in all chemical reactions.

Faraday's Laws of Electrolysis

When an electric current is made to pass through a cell, the current may cause chemical reactions to occur at its electrodes. This process is called electrolysis and the cell in which it occurs is called an electrolytic cell. In the 1830s, the English scientist Michael Faraday studied the reactions which take place at the electrodes of electrolytic cells. Faraday showed that electrochemical reactions follow all normal chemical stoichiometric relations, but in addition follow certain stoichiometric rules related to charge. These are known as Faraday's laws of electrolysis. In his experimental form, but using modern terms, they are as follows:

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The mass of an element discharged at an electrode m is directly proportional to the amount of electrical charge Q passed through the electrode.

If the same amount of electrical charge Q is passed through several electrodes, the mass m of an element discharged at each electrode will be directly proportional to both (a) the atomic mass of the element, and (b) the number of moles of electrons required to discharge one mole of the element from whatever material is being discharged at the electrode (the charge number z).

HISTORY

During the 19th century, chemists ...

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