The Principles of Thermodynamics With Special Applications to Hot Air Gas And
The Principles of Thermodynamics With Special Applications to Hot Air Gas And
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339 TABLE, SHOWING FINAL TEMPERATURE FOR ONE AND TWO CYLINDERS AND RATIO = 459. 4 + *.
Lc' If* p* Pi' Final temperature in degrees Fahr.
Za' P* Pi' Final temperature in degrees Fahr.
Lc' Lc ' One cylinder a .
Two cylinders V- Lc- One cylinder fc.
Two cylinders / 2 '- 2..
185. 4 265. 9 328. 95 381. 7 427. 3 467. 9 504. 5 123. 8 159. 1 185. 4 207. 5 224. 5 239. 9 253. 6 0. 95 0. 92 0. 90 0. 88 0. 87 0. 86 0. 85 9 538. 0 568. 55 598. 8 ' 624. 8 650. 2 674. 45 697. 2 265. 9 277. 0 287. 3 296. 8 305.... 6 313. 9 321. 6 0. 84 0. 83 0. 83 0. 82 0. 82 0. 81 0. 80 3 .
10 4 11 5 12 6 13 7 14 8 15 Friction of Air in Pipes. The compressed air is conveyed by means of pipes from the reservoir to the point at which it is desired to utilize it, and therefore there is a certain loss of pressure due to friction.
This loss is independent of any changes of temperature of the air. It is directly proportional to the length of the pipe and the square of the velocity, and inversely as the diameter of the pipe.
Denoting the loss of pressure due to friction by F, we have from experiments at Mont Cenis F = 0.
What to read after The Principles of Thermodynamics With Special Applications to Hot Air Gas And?
You can find similar books in the "Read Also" column, or choose other free books by Robert Rntgen to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
339 TABLE, SHOWING FINAL TEMPERATURE FOR ONE AND TWO CYLINDERS AND RATIO = 459. 4 + *.
Lc' If* p* Pi' Final temperature in degrees Fahr.
Za' P* Pi' Final temperature in degrees Fahr.
Lc' Lc ' One cylinder a .
Two cylinders V- Lc- One cylinder fc.
Two cylinders / 2 '- 2..
185. 4 265. 9 328. 95 381. 7 427. 3 467. 9 504. 5 123. 8 159. 1 185. 4 207. 5 224. 5 239. 9 253. 6 0. 95 0. 92 0. 90 0. 88 0. 87 0. 86 0. 85 9 538. 0 568. 55 598. 8 ' 624. 8 650. 2 674. 45 697. 2 265. 9 277. 0 287. 3 296. 8 305.... 6 313. 9 321. 6 0. 84 0. 83 0. 83 0. 82 0. 82 0. 81 0. 80 3 .
10 4 11 5 12 6 13 7 14 8 15 Friction of Air in Pipes. The compressed air is conveyed by means of pipes from the reservoir to the point at which it is desired to utilize it, and therefore there is a certain loss of pressure due to friction.
This loss is independent of any changes of temperature of the air. It is directly proportional to the length of the pipe and the square of the velocity, and inversely as the diameter of the pipe.
Denoting the loss of pressure due to friction by F, we have from experiments at Mont Cenis F = 0.
What to read after The Principles of Thermodynamics With Special Applications to Hot Air Gas And?
You can find similar books in the "Read Also" column, or choose other free books by Robert Rntgen to read onlineMoreLess
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