| 1864 - 564 Seiten
...motions are all reversed, it produces as much mechanical effect as can be produced by any thermo-dynamie engine, with the same temperatures of source and refrigerator, from a given quantity of heat. In order to prove the second proposition, we must consider in what respect Carnot's proof has become... | |
| Peter Guthrie Tait - 1868 - 148 Seiten
...motions are all reversed, it produces as much mechanical effect as can be produced by any thermo-dynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat. 53. In order to prove the second proposition, (which regards the Transformation of heat, as the first... | |
| Royal Society (Great Britain) - 1874 - 644 Seiten
...could be obtained very directly and easily from a simple formula which he had given in his paper on the Dynamical Theory of Heat, Transactions of the Royal Society of Edinburgh, March 17, 1851, § 21 (3), to express the second law of thermodynamics for a body of uniform temperature throughout,... | |
| South Kensington Museum - 1876 - 386 Seiten
...motions are all reversed, it produces as much mechanical effect as can be produce' any thermodvnamic engine, with the same temperatures of source and refrigerator, from a given quantitv of heat. It is to be particularly observed here that Reversibility is the sole test of perfection... | |
| Richard Wormell - 1877 - 192 Seiten
...are . all reversed, it produces as much .mechanical effect as can be produced by any thermodynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat It may be convenient for readers of this subject to remark, that some writers call Carnot's principle... | |
| Peter Guthrie Tait - 1884 - 392 Seiten
...reversed (see § 89), it produces as much mechanical effect as can be produced by any thermodynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat. 83. It is to be particularly observed here that Reversibility (see §§ 88, 89) is the sole test of... | |
| 1886 - 542 Seiten
...motions are reversed, it produces as much mechanical effect as can be produced by any thermodynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat." On page 179 is another statement in more familiar language, as follows : " Now let there be no molecular... | |
| 1888 - 932 Seiten
...motions are all reversed, it produces as much mechanical effect as can be produced by any thermodynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat. 7. Absolute Temperature. — We have seen that the fraction of the heat supplied to it which a reversible... | |
| 1890 - 956 Seiten
...motions are all reverted, it products as much mechanical effect as can be produced by any tfiermo-dynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat. The proof of this second law differs from that of Carnot (already given as regards reversible engines)... | |
| Peter Alexander - 1892 - 226 Seiten
...motions are all reversed, it produces as much mechanical effect as can be produced by any ther mo dynamic engine, with the same temperatures of source and refrigerator, from a given quantity of heat." In 1824, Sadi Carnot, in a work entitled ' Reflexions sur la Puissance Motrice du Feu,' &c., first... | |
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