This historic book may have numerous typos and missing text. Purchasers can download a free scanned copy of the original book (without typos) from the publisher. Not indexed. Not illustrated. 1907 Excerpt: ...when saturate1 steam expands adiabatically, as it is assumed to expand when it flows through a turbine. But the walls of the turbine remain at so uniform a temperature that there is no opportunity for loss through reevaporation of this condensed steam, and the gain realized must therefore result from the reduced friction, as stated above. It is fallacious to suppose there is any considerable gain because superheated steam has a higher temperature than saturated steam. The theoretical or thermodynamic gain from superheating is almost nothing. It is true that the heat represented by the superheat is received at a higher mean temperature than the other portions of the heat in the steam, and there is a theoretical advantage from this fact. The amount of heat received at this high temperature, however, is so small, compared with he amount received before superheating begins, as to be almost negligible. One pound of saturated steam at 100 pounds gauge pressure contains nearly 900 latent heat units; and if this steam were then superheated 100 degrees, it would acquire only about six heat units in addition, in spite of its high temperature. Practical Considerations.--In the account published in The Iron Age, May, 1904, of Barrus' tests upon one of the Curtis turbines at Newport, R. I., the reported results with superheated steam were not entirely favorable. This station was equipped with a separately fired Schmidt superheater and unless the superheater was worked to nearly its full capacity there was a loss from its use. This is not to condemn a moderate degree of superheating, however, such as can readily be realized by the use of superheating tubes in the same setting with a steam boiler, and such, moreover, as can be maintained from day to day in actual operatio...

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