Scientific American Supplement, No. 441, June 14, 1884. by Various
page 19 of 155 (12%)
page 19 of 155 (12%)
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W = H( ------- )
\ T / I will illustrate this important doctrine in the manner which Carnot himself suggested. [Illustration: THE GENERATION OF STEAM. Fig 2.] Fig. 2 represents a hillside rising from the sea. Some distance up there is a lake, L, fed by streams coming down from a still higher level. Lower down on the slope is a millpond, P, the tail race from which falls into the sea. At the millpond is established a factory, the turbine driving which is supplied with water by a pipe descending from the lake, L. Datum is the mean sea level; the level of the lake is T, and of the millpond _t_. Q is the weight of water falling through the turbine per minute. The mean sea level is the lowest level to which the water can possibly fall; hence its greatest potential energy, that of its position in the lake, = QT = H. The water is working between the absolute levels, T and _t_; hence, according to Carnot, the maximum effect, W, to be expected is-- / T - t \ W = H( ------- ) \ T / / T - t \ but H = QT [therefore] W = Q T( ------- ) \ T / W = Q (T - t), |
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