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Summary - Enthalpy and Heat Capacity of Graphite

Recommended Equations

The equations recommended by the Scientific Group Thermodata Europe (SGTE)[29] for the enthalpy and heat capacity of carbon are recommended because they are in excellent agreement with recent assessments by JANAF[27] and CODATA[28] as well as data on different grades of graphite from measurements by McDonald,[24] Cezairliyan and Righini,[25-26] West and Ishihara,[11] and Buchnev et al.[4] The SGTE recommendations are also in good agreement with the recommendations for nuclear graphite given by Butland and Maddison.[6]

The SGTE equation for the graphite enthalpy increment relative to the enthalpy in the standard state at 298.15 K is:


H(T)-H(298.15) = - 17368.441 + 24.3 T + 4.723 10^-4 T^2
                 + 5.1252 10^6 T^-1 - 7.929 10^8 T^-2   (1)
                 + 4.8 10^10 T^-3

where enthalpy is in J/mol and temperature is in K. The SGTE equation for the heat capacity of graphite in J/(mol-K) is :


Cp = 24.3 + 9.446 10^-4 T - 5.1252 10^6 T^-2 +          (2)
     1.5858 10^9 T^-3 - 1.44 10^11 T^-4

where temperature is in K. Values calculated with Eqs (1-2) are given in Table 1. The SGTE equations for graphite enthalpy increments and heat capacities in kJ/kg and kJ/(kg-K) are:


H(T) - H(298.15) = - 1446.04454 + 2.023145 T +
               3.9322 10^-5 T^2 + 4.26709 10^5 T^-1     (3)
             - 6.60145 10^7 T^-2 + 3.9963 10^9 T^-3

and


Cp = 2.023145 + 7.8645 10^-5 T - 4.26709 10^5 T^-2 +    (4)
     1.3203 10^8 T^-3 - 1.199 10^10 T^-4

Figure 2
Figure 2
Figure 3
Figure 3
Table 2 gives graphite enthalpy increments and heat capacities in kJ/kg and kJ/(kg-K). Both experimental measurements by Rasor and McClelland[9] on a number of types of graphite and those of Sheindlin et al.[3] on six brands of Russian graphite gave enthalpies and heat capacities which increased at much faster rates than those from measurements on high-purity graphites (Fig 2 and Fig 3). The observations by Rasor and McClelland that (1) significant vapor was released at high temperature and (2) white deposits were formed on some graphites led analysts to conclude that the results of Rasor and McClelland and of Sheindlin et al. may be due to impurities in the samples or to the breakdown of the graphite at high temperatures (above 2500 K).

Uncertainties

The good agreement of the measurements of McDonald, Cezairliyan and Righini, West and Ishihara, and Buchnev et al. and the recent recommendations of CODATA, JANAF, and the SGTE would indicate low uncertainties (within 5%) for the recommended enthalpies and heat capacities of graphite. However, the lack of data on the grades of graphite used in Russian reactors leads to uncertainty in the high-temperature properties. Are Russian nuclear graphites closer to those used in the experiments by Sheindlin et al. or those of Buchnev et al.? Because the graphite enthalpies and heat capacitics obtained by Sheindlin et al. deviate significantly from those of Buchnev et al. and from the recommended values, large uncertainties are estimated at high temperatures.

Figure 5
Figure 5
Figure 6
Figure 6
Uncertainties in the enthalpy increments are: 8% below 500 K, 3% from 800 to 2500 K, and 10% above 3000 K. Between 500 and 800 K, enthalpy increment uncertainties decrease linearly from 8% to 3%. Between, 2500 and 3000 K, uncertainties increase linearly from 3% to 10%. Uncertainties in the graphite heat capacities are: 10% below 500 K; 5% from 800 through 2500 K. Between 500 and 800 K, the heat capacity uncertainties decrease linearly from 10% to 5%. Above 2500 K, uncertainties increase linearly from 5% at 2500 K to 11% at 3000 K. Above 3000 K, the negative uncertainty remains at -11% but the positive uncertainty increases linearly to +50% at 3600 K. So at 3600 K, the uncertainties in the heat capacity values are: +50%, -11%. Fig 5 and Fig 6 show the recommended values for the enthalpy and heat capacity of graphite with estimated uncertainties designated by dotted lines.


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