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Heat capacity, of gases

Understanding the thermodynamics of natural gas is essential for optimizing the management of its resources. Correlation and prediction of thermodynamic and transport properties of natural gas are needed at different stages during the exploration and assessment of reserves as well as for its production, transport, and storage. [Pg.145]

Ihble 1 Molar composition (mole/%) of the five gaseous mixtures and the absolute average deviations (in %) obtained using different equations of state (EOS), over the full pressure and temperature ranges investigated [Pg.146]

The previous data only provide three of four thermodynamic coefficients. [Pg.186]

We also need to determine the second diagonal coefficient which is — [Pg.186]

In practice, many tables provide the heat capacities of gases at constant pressure and atmospheric pressure in the form of a polynomial  [Pg.187]

The coefficients a, b, c anJ depend on the substance and theoretically depend on pressure. This dependence is not usually provided as it can be easily calculated (see section 1.1.13). Some coefficients of relation [7.57] can be zero and one of either coefficient cord will always be zero. [Pg.187]

The heat capacity at constant volume is deduced from the previous data at constant pressure since it involves moving from a coefficient of matrix u(P,T) to a coefficient of matrix m(F,7) (see section 2.1.5), we obtain  [Pg.187]

The heat capacity of gases is essential for some process engineering design involving gas-phase chemical reactions. Here, the heat capacities, C°, for gases are required to determine the heat necessary to bring the chemical compound increase to the reaction temperature. The heat capacity of a mixture of gases may be found from the heat capacities of the individual components contained in the mixtures. [Pg.80]

The correlation for C° of the ideal gas at low pressure is a third degree polynomial, which is a function of temperature. [Pg.80]

The Appendix at the end of this chapter gives values of heat capacity constants. [Pg.80]

From classic thermodynamics alone, it is impossible to predict numeric values for heat capacities these quantities are determined experimentally from calorimetric measurements. With the aid of statistical thermodynamics, however, it is possible to calculate heat capacities from spectroscopic data instead of from direct calorimetric measurements. Even with spectroscopic information, however, it is convenient to replace the complex statistical thermodynamic equations that describe the dependence of heat capacity on temperature with empirical equations of simple form [15]. Many expressions have been used for the molar heat capacity, and they have been discussed in detail by Frenkel et al. [4]. We will use the expression [Pg.64]


Appendix The Molar Heat Capacities of Gases in the Ideal Gas (Zero Pressure) State... [Pg.104]

Mean Molal Heat Capacities of Gases Between 25°C and T°C (Reference pressure = 0)... [Pg.357]

A MOLECULAR 1NTERI UDF. THE ORIGIN OF THE HEAT CAPACITIES OF GASES... [Pg.354]

A Molecular Interlude The Origin of the Heat Capacities of Gases... [Pg.354]

The molar heat capacities of gases composed of molecules (as distinct from atoms) are Higher than those of monatomic gases because the molecules can store energy as rotational kinetic energy as well as translational kinetic energy. We saw in Section 6.7 that the rotational motion of linear molecules contributes another RT to the molar internal energy ... [Pg.354]

Table 8.1 Number of modes and heat capacity of gases in the classical limit. Table 8.1 Number of modes and heat capacity of gases in the classical limit.
For liquid water and for aqueous solutions we wiU assume Cp = 1 cal/g K, and, since the density p of water is -1 g/cm, we have pCp = 1 cal/cm K or pCp =1000 cal/Uter K. To estimate the heat capacity of gases, we will usually assume that the molar heat capacity Cp is j R cal/mole K. There are thus three types of heat capacity, the heat capacity per unit mass Cp, the heat capacity per unit volume pCp, and the heat capacity per mole Cp. However, we will use heat capacity per unit volume for much of the next two chapters, and we use the symbol pCp for most of the equations. [Pg.210]

LabWorks and the Kundt s Tube A New Way To Determine the Heat Capacities of Gases 196... [Pg.136]

Qv the heat of expln of the mixt before adding extra amt of NaCl tsthe desired temp of expln a=.the sum of molar heat capacities of individual gases of expln at O C and b= the sum of increments of the mean molar heat capacities of gases for each I C... [Pg.231]

As shown in Chap. 6, ideal-gas heat capacities, rather than the actual heat capacities of gases, are used in the evaluation of thermodynamic properties such as internal energy and enthalpy. The reason is that thermodynamic-property evaluation is conveniently accomplished in two steps first, calculation of ideal-gas values from ideal-gas heat capacities second, calculation from PVT data of the differences between real-gas and ideal-gas values. A real gas becomes ideal in the limit as P - 0 if it were to remain ideal when compressed to a finite pressure, its state would remain that of an ideal-gas. Gases in these hypothetical ideal-gas states have properties that reflect their individuality just as do real gases. Ideal-gas heat capacities (designated by Cf and Cy) are therefore different for different gases although functions of temperature, they are independent of pressure. [Pg.61]

FIG URE 1.4 Isothermal pressure correction to the molar heat capacity of gases. Perry and Chilton—Chemical Engineers Handbook, McGraw-Hill, 1973.)... [Pg.21]

Table B3 Heat capacities of gases in the ideal-gas state3 C°yR = a + bT + cT2 + dT 2 T(K) from 298 to Tmax ... Table B3 Heat capacities of gases in the ideal-gas state3 C°yR = a + bT + cT2 + dT 2 T(K) from 298 to Tmax ...
Table 1. Constants for heat capacities of gases in ideal state and liquid water. Table 1. Constants for heat capacities of gases in ideal state and liquid water.
In considering the theoretical calculation of the heat capacities of gases, we shall be concerned only with perfect gases. Since Cp = Cy+ R for an ideal gas (where Cp and are the molar quantities C ln and CJn), our discussion can be restricted to C . [Pg.106]


See other pages where Heat capacity, of gases is mentioned: [Pg.1907]    [Pg.80]    [Pg.148]    [Pg.231]    [Pg.64]    [Pg.567]    [Pg.13]    [Pg.387]    [Pg.387]    [Pg.408]    [Pg.409]    [Pg.410]    [Pg.410]    [Pg.57]    [Pg.67]    [Pg.68]    [Pg.80]    [Pg.94]    [Pg.230]    [Pg.130]    [Pg.62]    [Pg.52]   
See also in sourсe #XX -- [ Pg.80 , Pg.91 , Pg.104 , Pg.105 , Pg.106 , Pg.107 ]

See also in sourсe #XX -- [ Pg.80 , Pg.91 , Pg.104 , Pg.105 , Pg.106 , Pg.107 ]

See also in sourсe #XX -- [ Pg.880 ]

See also in sourсe #XX -- [ Pg.145 ]

See also in sourсe #XX -- [ Pg.114 ]




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Heat Capacities of Gases in the Ideal Gas State

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Heat Capacity at Constant Pressure of Inorganic and Organic Compounds in the Ideal Gas State Fit to a Polynomial Cp

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The heat capacity of a perfect gas. Chemical constants

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