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. 1965 Sep-Oct;69A(5):423–438. doi: 10.6028/jres.069A.045

Table 7. Comparison of the thermodynamics of vapor-equilibrium reactions of table 6 calculated by various methods.

Reference T Calculations from vapor-equilibrium data Calculations from calorimetric data Difference (method II—calorimetric data)
Method I assuming ΔCp=0 Method II ΔCp from calorimetric data
ΔHT° ΔST° ΔHT° ΔST° ΔHT° ΔST° δΔHT° δTΔST° δΔGT°
°K kcal mol−1 cal deg−1 mol−1 kcal mol−1 cal deg−1mol−1 kcal mol−1 cal deg−1mol−1 kcal mol−1 kcal mol−1 kcal mol−1
Meschi and Searcy [31] 1650 345.2±27.3a 117.5±16.4a 345.6±27.3a 117.8±16.4a 351.1±2.1b,c 130.2±0.3 −5.5 −20.5 +15.0
Prescott and Hincke [36] 1850 257.4±14.9 92.6±8.0 257.2±14.9 92.5±8.0 250.3±1.7 87.3±0.3 +6.9 +9.6 −2.7
Prescott and Hincke [37] 2150 535.6±88.0 239.8±41.5 535.0±87.8 239.6±41.4 566.8±7.2 248.9±0.7 −31.8 −20.0 −11.8
Brunner [38] 2100 467.6±3.4 209.4±1.7 466.1±3.4 208.7±1.6 567.6±7.2 249.3±0.7 −101.5 −85.3 −16.2
Grjotheim et al., [41] 1400 297.2±6.5 172.4±4.7 297.2±6.5 172.3±4.7 301.3±4.7 167.5±0.3 −4.1 +6.7 −10.8
a

These figures following the ± symbols are standard deviations defined for the values of ΔH° by:

Sb={Sy2Σxi2(Σxi)2/k}1/2, andofΔS°by:Sa={Sy2Σxi2kΣxi2(Σx)2}1/2,
where Sy2=Σδi2/(k2),δi the deviation of the experimental value from the “least-squared” value, k the number of observations, and xi-=1/Ti [42].
b

These figures following the ± symbols were obtained from the relation (ϵi2)1/2, where ϵi is the estimated uncertainty of the calorimetric data used.

c

These values of ΔH° are based on the ΔHf° (298 °K) for Al4C3 reported by King and Armstrong [26].