1960
DOI: 10.2514/8.4997
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Thermodynamic Properties of Air in the Temperature Interval from 1000 to 12,000 K and the Pressure Intervals from 0.001 to 1000 Atm

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Cited by 10 publications
(4 citation statements)
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“…The treatment of the diatomic molecules follows the method developed by Drellishak 12,13 and by Stupochenko 14 . In this method the energy of a particular state in the molecule € E nJv is split into three contributions: the electronic excitation energy € E el n ( ) , the vibrational energy € E vib n,v ( ) and the rotational energy Assuming that (22) is valid for all vibrational states up to dissociation, we can determine the maximum permissible value € v max of the vibrational quantum number for each rotationless (J=0) molecular state from the equation…”
Section: Diatomic Moleculesmentioning
confidence: 99%
“…The treatment of the diatomic molecules follows the method developed by Drellishak 12,13 and by Stupochenko 14 . In this method the energy of a particular state in the molecule € E nJv is split into three contributions: the electronic excitation energy € E el n ( ) , the vibrational energy € E vib n,v ( ) and the rotational energy Assuming that (22) is valid for all vibrational states up to dissociation, we can determine the maximum permissible value € v max of the vibrational quantum number for each rotationless (J=0) molecular state from the equation…”
Section: Diatomic Moleculesmentioning
confidence: 99%
“…Both problems are reported in the paper of Park [26] and Lee [27] for the development of multitemperature model. In the early 1960s, several studies were conducted by Drellishak et al [18,28] and Stupochenko et al [29] to develop a calculation method for local thermodynamic equilibrium systems. Subsequently, Capitelli et al [20,[30][31][32] performed a large body of calculations for diatomic components and predicted atmospheric partition functions.…”
Section: Introductionmentioning
confidence: 99%
“…The derivations of Herzberg [41,40], build upon the work of Dunham to produce partition functions that sum the coupled vib-rotational energy levels, and he presents concise expressions for the evaluation of the thermodynamic properties from these partition functions. These have seen use by various authors since the early 1960s through the work of Stupochenko [71] and Drellishak [19]. Jaffe too uses this approach to produce specific heat curves up to a temperature of 50, 000K for O 2 , N 2 and N O in 1987 [46].…”
Section: Diatomic Speciesmentioning
confidence: 99%
“…It has been experimentally verified however, that a number of states may exist in a quasi-steady coupling of v and J, with energies above the dissociation limit [40,19,71,10]. These discrete cases must be included inside the partition function sum, through the energy matching of the potential at the peak of the barrier r m and vib-rotational energy.…”
Section: Derivation Of R M and Maximum Rotational Quantum Number J Maxmentioning
confidence: 99%