 | Sir Dugald Clerk - Internal combustion engines - 1882 - 194 pages
...greater degree of compression before heating even better results are possible. In an engine of type 3 expanding to the same volume after ignition as before...temperature after compression T; it is T— T' D=— _— whatever may be the maximum temperature after ignition. Increasing the temperature of ignition... | |
 | Engineering - 1882 - 536 pages
...igniting at constant volume and expanding to the same volume as before ignition, the possible duty D was determined by the atmospheric absolute temperature T', and the absolute temperature after compresssion, T ; and it was D = T — T' | T, whatever might be the maximum temperature after ignition.... | |
 | William MacGregor - Gas-turbines - 1885 - 280 pages
...greater degree of compression before heating even better results are possible. In an engine of type 3 expanding to the same volume after ignition as before...temperature T', and the absolute temperature after T — T' compression T ; it is D = — ~ — whatever may be the maximum temperature after ignition.... | |
 | William Macgregor (C.E.) - 1885 - 364 pages
...atmospheric absolute temperature T', and the absolute temperature after T — T' compression T ; it is D = — „ — whatever may be the maximum temperature...ignition increases the power of the •engine, but does not^cause the conversion of a greater portion of heat into work. With any given maximum temperature... | |
 | North East Coast Institution of Engineers and Shipbuilders - Marine engineering - 1919 - 636 pages
...absolute atmospheric temperature T1, and the absolute temperature after compression T — T1 T; it is D= — ,= — Whatever may be the maximum temperature...of the engine, but does not cause the conversion of heat into work. With any given maximum temperature the smaller the difference between that temperature... | |
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... of heat into work. With any given maximum temperature the smaller the difference between that temperature and the temperature of compression, the greater is the proportion of added heat converted into work with any given amount of expansion. 