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effected in electric clocks, that rather than go to the trouble and expense required by such precautions, it appears far preferable to keep an accurate time-piece in some sheltered position and use it with a source of electricity to drive the hands of the large dial. _Electrical Clocks._--One of the first attempts to apply electricity to clocks was made by Alexander Bain in 1840-1850. About the same time Sir C. Wheatstone, R. L. Jones, C. Shepherd, Paul Garnier and Louis Breguet invented various forms of electrical time-keepers. It is not proposed here to go into the history of these abortive attempts. Those who desire to follow them may consult Bain, _An Account of Some Applications of the Electric Fluid to the Useful Arts_ (1843) and _Short History of Electric Clocks_ (1852); Sir Charles Wheatstone, _Trade Circular of the British Telegraph Manufactory_; C. Shepherd, _On the Application of Electro-magnetism as a Motor for Clocks_ (1851), and a list of references in the Appendix to Tobler's _Die electrischen Uhren_ (Leipzig, 1883), and a list of books given by F. Hope Jones, _Proc. Inst. Elec. Eng._, 1900, vol. 29. The history of electrical clocks is a long and complicated matter, for there are some 600 or 700 patents for these clocks in Europe and America, some containing the germs of valuable ideas but most pure rubbish. All that can be done is to select one or two prominent types of each class and give a brief description of their general construction. [Illustration: FIG. 27.--Turret Clock for Hidalgo, Mexico, driving four 8 ft. dials.] It is in the apparently simple matter of making and keeping the electrical contact that most of the systems of electrical time-keeping have failed, for want of attention to the essential conditions of the problem. In practice every metal is covered with a thin film of non-conducting oxide over which is another film of moisture, oil, dirt or air. Hence what is wanted is a good vigorous push of a blunted point or edge preferably obliquely upon a more or less yielding surface so as to get a rubbing action. Thus if the stiff spring a b (fig. 28) were stabbed down on the oblique surface C D a good contact would invariably result, provided that the metals employed were gold, platinum or some not easily oxidizable metal. Or again, if a mercury surface be simply touched with a pin, the slight sparking that is produced on making the current will soon form a little pile of dirty oxide at
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