Phase equilibria in aluminum-carbon system at high temperatures

N. A. Gokcen, L. L. Oden
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引用次数: 2

Abstract

The partial excess Gibbs energies of carbon and aluminum in liquid Al-C were used with the equilibrium vapor pressures of pure Al and pure C to obtain the phase diagrams (1) at 1 bar of total pressure, and (2) at pressures sufficient to suppress the gas phase. The first diagram contains [gas+graphite → liquid] tectoid-type reaction at 2900±20K with the tectoid composition of 0.681 mol fraction of aluminum. The [gas/graphite] boundary is subject to large errors due to the large errors in the vapor pressure of pure graphite, but its general form is acceptable. The second diagram consists entirely of the condensed phases with peritectic reaction [liquid+graphite → Al4C3] at 2429 K. The [liquid/graphite] phase boundary was obtained from the graphite solubility in liquid solutions at 2429-2800 K, yielding the partial excess Gibbs energy of carbon in solution.

The resulting phase boundary is as reliable as the melting point of graphite, taken to be 4130 K.

高温下铝碳体系的相平衡
用液态Al-C中碳和铝的部分过量吉布斯能与纯Al和纯C的平衡蒸气压结合,得到了总压为1bar时的(1)相图和足以抑制气相的(2)相图。第一张图为[气体+石墨→液体]tectoid型反应,反应温度为2900±20K, tectoid组成为0.681 mol分数的铝。由于纯石墨的蒸气压误差较大,[气体/石墨]边界存在较大误差,但其一般形式是可以接受的。第二张图完全由在2429 K下发生包晶反应的凝聚相组成[液体+石墨→Al4C3]。根据石墨在2429 ~ 2800 K溶液中的溶解度,得到了[液/石墨]相边界,得到了溶液中碳的部分超额吉布斯能。所得相界与石墨的熔点一样可靠,取为4130 K。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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