Comparison of ab initio and group additive ideal gas heat capacities

AIChE Journal ◽  
2004 ◽  
Vol 51 (1) ◽  
pp. 292-297 ◽  
Author(s):  
Robert A. Marriott ◽  
Mary Anne White
Keyword(s):  
2007 ◽  
Vol 257 (1) ◽  
pp. 102-113 ◽  
Author(s):  
N.R. Nannan ◽  
P. Colonna ◽  
C.M. Tracy ◽  
R.L. Rowley ◽  
J.J. Hurly

1990 ◽  
Vol 60 (1-2) ◽  
pp. 191-203 ◽  
Author(s):  
Sam.O. Colgate ◽  
Alwarappa Sivaraman ◽  
Kyle Reed
Keyword(s):  

2017 ◽  
Vol 494 ◽  
pp. 172-181 ◽  
Author(s):  
Yaqi Ji ◽  
George Beridze ◽  
Dirk Bosbach ◽  
Piotr M. Kowalski

Author(s):  
Dennis Sherwood ◽  
Paul Dalby

This chapter brings together, and builds on, the results from previous chapters to provide a succinct, and comprehensive, summary of all key relationships relating to ideal gases, including the heat and work associated with isothermal, adiabatic, isochoric and isobaric changes, and the properties of an ideal gas’s heat capacities at constant volume and constant pressure. The chapter also has two ‘case studies’ which use the ideal gas equations in broader, and more real, contexts, so showing how the equations can be used to tackle, successfully, more extensive systems. The first ‘case study’ is the Carnot cycle, and so covers all the fundamentals required for the proof of the existence of entropy as a state function; the second ‘case study’ is the ‘thermodynamic pendulum’ – a system in which a piston in an enclosed cylinder oscillates to and fro like a pendulum under gravity, in both the absence, and presence, of friction.


1981 ◽  
Vol 36 (3) ◽  
pp. 529-537 ◽  
Author(s):  
Michal Bureš ◽  
Vladimír Majer ◽  
Milan Zábranský
Keyword(s):  

2003 ◽  
Vol 31 (3) ◽  
pp. 189-200 ◽  
Author(s):  
Jeffery D. Lewins

Many of the conventional results obtained when optimising the performance of an intercooler during compression using a perfect gas model can be obtained when the restrictions of the model are relaxed to an ideal gas. That is, we now have temperature-dependent specific heat capacities but retain the equation of state pV = RT. This note illustrates the theme.


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