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

Figure 5. Comparison of vapor pressures (log10 P versus 1/T) calculated from heat of formation and thermodynamic data with published values obtained in high-temperature equilibrium measurements.

Figure 5.

(a) 4AlN(c) + 3C(c) → Al4C3(c) + 2N2(g): A and A′ calculation from thermal data,* A′′ = Prescott and Hincke [36].

(b) Al4C3(c) → 4Al(g) + 3C(c): B and B′ = calculation from thermal data,* B′′ = Meschi and Searcy [31], ○ = Chupka et al. [34], Δ = Campbell [35].

(c) 2Al2O3(c) + 9C(c) = Al4C3(c) + 6CO(g): C and C′ calculation from thermal data,*

C′′ = Prescott and Hincke [37], C′′′ = Brunner [38].

CI = Al4O4C(c) + 6C(c) → Al4C3(c) + 4CO(g): Cox and Pidgeon [40].

CII = 2Al2O3(c) + 3C(c) → Al4O4C(c) + 2CO(g): [40].

CIII = Al2O3(c) + 3C(c) → Al2OC(c) + 2CO(g): [40].

(d) 8MgO(c) + Al4C3(c) → 2MgAl2O4(c) + 3C(c) + 6Mg(g): D and D′ = calculation from thermal data, D′′ = Grjotheim et al. [41].