Scientific American Supplement, No. 803, May 23, 1891 by Various
page 83 of 143 (58%)
page 83 of 143 (58%)
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Nominal 80 horse | 54.3 | 72.3 | 129 | 21 | 469 | 517
power single | 54.3 | 72.3 | 152 | 29 | 437 | 475 cylinder Farcot | 54.0 | 72.3 | 160 | 35 | 424 | 465 engine. | 40 | 65.0 | 170 | 49 | 438 | 477 _________________|______|______|_________|________|_______|________ These motors, it may be assumed, represent the best practice that has been obtained up to the present time in the construction of compressed air motors; with the smallest of them, indicating about one-tenth of a horse power, the consumption of air, when admitted cold, was 1377 cubic feet and 988 cubic feet when the air was heated before admission. The half horse power engine consumed 1148 cubic feet of cold air, and of heated air 791 cubic feet per horse power and per hour. It should be mentioned that these, the most valuable and suggestive of all the trials carried out by Professor Riedler, were conducted with the greatest care, two distinct modes of measuring the air supplied being followed on two occasions for each test; it may therefore be considered that the results given are absolutely correct. The trials were made with an old single cylinder Farcot engine, nominally of 80 horse power, but indicating over 72.3. With this engine the consumption of air varied from 465 to 517 cubic feet, the larger consumption being due to the lower temperature (129 deg. Cent.) to which the air was raised before admission; in the most economical result the temperature was 160 deg. Cent. The volumes of air referred to are, of course, in all cases taken at atmospheric pressure. Among the important losses that have to be reckoned with in every system of distributing motive power from a central station--whether by steam or by electricity, water, or compressed air--losses must occur |
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