Thermodynamics of Reversible Cycles in Gases And Saturated Vapors
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To quickly assess the difficulty of the text, read a short excerpt:
dt Therefore dr ,, + c = .305.
dt 78 TBEBMODYNAMICS OF lu the last term of the expression for h we shall suhstitute for r the simple expression given by Clausius and obtain h = .305 607 - .7 08^ 273 H- ^ ■ The following table contains the calculated values of h for several temperatures: t 0° 50° 100° 150° 200° h - 1.916 - 1.465 -1.133 -.879 -.676 The physical meaning of this negative specific heat will be considered further ou in connection with adiabatic expansion of saturated water-vapor.
We ...pass on to the calculation of the specific volume of saturated water-vapor.
2. Calculation of the Specific Volume of Saturated Water-vapor.
The first question to consider is, whether in its saturated state water-vapor follows the law of Mariotte-Gay-Lussac, and if it does not, to what extent and in what way deviations occur.
Making use of the fundamental relation (IIP), we find, after replacing (s — a) for u.
r = T{s - a- ) dp " dt J REVERSIBLE CYCLES IN OASES AND VAPORS. 79 or 273>- _ %np(s - a) ^,ldp J(273 + p dt If the Mariotte-Gay-Lussac law were applicable to satu- rated water - vapor^ then from ^ = const, we should have ps X 373 , ^273+T) = °°'^^*' Since s differs but little from (s — a), we should have p{s - o-)273 Comparing this to the equation just obtained from the funda- mental relation (IIP), we see that if the Mariotte-Gay-Lussac law were applicable to saturated water-vapor we should have %nr _ p{s - o-) 273 _ pdt Having calculated - ;3t hy the method described above, and J- from the formula r = 607 — .708^, and substituted their 80 THERMODTNAMIGS OF values in the last equation, Clausius obtained the following table : J.U/U -•^/j/'vo "^273 + r
What to read after Thermodynamics of Reversible Cycles in Gases And Saturated Vapors?
You can find similar books in the "Read Also" column, or choose other free books by Pupin, Michael Idvorsky, 1858-1935 to read online
To quickly assess the difficulty of the text, read a short excerpt:
dt Therefore dr ,, + c = .305.
dt 78 TBEBMODYNAMICS OF lu the last term of the expression for h we shall suhstitute for r the simple expression given by Clausius and obtain h = .305 607 - .7 08^ 273 H- ^ ■ The following table contains the calculated values of h for several temperatures: t 0° 50° 100° 150° 200° h - 1.916 - 1.465 -1.133 -.879 -.676 The physical meaning of this negative specific heat will be considered further ou in connection with adiabatic expansion of saturated water-vapor.
We ...pass on to the calculation of the specific volume of saturated water-vapor.
2. Calculation of the Specific Volume of Saturated Water-vapor.
The first question to consider is, whether in its saturated state water-vapor follows the law of Mariotte-Gay-Lussac, and if it does not, to what extent and in what way deviations occur.
Making use of the fundamental relation (IIP), we find, after replacing (s — a) for u.
r = T{s - a- ) dp " dt J REVERSIBLE CYCLES IN OASES AND VAPORS. 79 or 273>- _ %np(s - a) ^,ldp J(273 + p dt If the Mariotte-Gay-Lussac law were applicable to satu- rated water - vapor^ then from ^ = const, we should have ps X 373 , ^273+T) = °°'^^*' Since s differs but little from (s — a), we should have p{s - o-)273 Comparing this to the equation just obtained from the funda- mental relation (IIP), we see that if the Mariotte-Gay-Lussac law were applicable to saturated water-vapor we should have %nr _ p{s - o-) 273 _ pdt Having calculated - ;3t hy the method described above, and J- from the formula r = 607 — .708^, and substituted their 80 THERMODTNAMIGS OF values in the last equation, Clausius obtained the following table : J.U/U -•^/j/'vo "^273 + r
What to read after Thermodynamics of Reversible Cycles in Gases And Saturated Vapors?
You can find similar books in the "Read Also" column, or choose other free books by Pupin, Michael Idvorsky, 1858-1935 to read online
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