The Theory of Drying And Its Application to the New Humidity Regulated And Recir
The Theory of Drying And Its Application to the New Humidity Regulated And Recir
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For saturated conditions. Precisely the same value for the vapor occurs if saturated air at 101 F. And atmospheric pressure is used instead, in which case the additional heating capacity of the air present is also available. There would then be in a cubic foot of space vapor pressure of 1 pound (nearly) per square inch and 13. 7 pounds of dry air pressure. This amount of vapor would weigh 0. 0029 pound and the air 1/15. 2 or 0. 0658 pound (15. 2 being the volume in cubic feet of 1 pound of dry ...air at 13. 7 pounds pressure and 101 F. Temperature).
HEATING CAPACITIES OF AIR AND VAPOR IN MIXTURE.
The heating capacity of the vapor in this cubic foot of space, in falling 1 degree, from 102 F. To 101 F. , is . 0029 X-42 1 ^. 00122 B. T. U. , as before, while that of the air present is . 0658X-237=. 0156 B. T. U. , or more than ten times that of the vapor present. The total heating capacity of 1 cubic foot of the mixture, in falling 1 degree, from 102 F. To 101 F. , is then the sum of these two, viz, .
What to read after The Theory of Drying And Its Application to the New Humidity Regulated And Recir?
You can find similar books in the "Read Also" column, or choose other free books by Harry Donald Tiemann to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
For saturated conditions. Precisely the same value for the vapor occurs if saturated air at 101 F. And atmospheric pressure is used instead, in which case the additional heating capacity of the air present is also available. There would then be in a cubic foot of space vapor pressure of 1 pound (nearly) per square inch and 13. 7 pounds of dry air pressure. This amount of vapor would weigh 0. 0029 pound and the air 1/15. 2 or 0. 0658 pound (15. 2 being the volume in cubic feet of 1 pound of dry ...air at 13. 7 pounds pressure and 101 F. Temperature).
HEATING CAPACITIES OF AIR AND VAPOR IN MIXTURE.
The heating capacity of the vapor in this cubic foot of space, in falling 1 degree, from 102 F. To 101 F. , is . 0029 X-42 1 ^. 00122 B. T. U. , as before, while that of the air present is . 0658X-237=. 0156 B. T. U. , or more than ten times that of the vapor present. The total heating capacity of 1 cubic foot of the mixture, in falling 1 degree, from 102 F. To 101 F. , is then the sum of these two, viz, .
What to read after The Theory of Drying And Its Application to the New Humidity Regulated And Recir?
You can find similar books in the "Read Also" column, or choose other free books by Harry Donald Tiemann to read onlineMoreLess
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