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首页> 外文期刊>Physics and chemistry of minerals >Thermodynamics and crystal chemistry of the hematite-corundum solid solution and the FeAl_2O_3 phase
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Thermodynamics and crystal chemistry of the hematite-corundum solid solution and the FeAl_2O_3 phase

机译:赤铁矿-刚玉固溶体和FeAl_2O_3相的热力学和晶体化学

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摘要

High-temperature oxide-melt calorimetry and Rietveld refinement of powder X-ray diffraction patterns were used to investigate the energetics and structure of the hematite-corundum solid solution and ternary phase FeAlO_3 (with FeGaO_3 structure). The mixing enthalpies in the solid solution can be described by a polynomial ΔH_(mix) = W X_(hem)(1-X_(hem)) with W = 116 ± 10 kJ mol~(-1). The excess mixing enthalpies are too positive to reproduce the experimental phase diagram, and excess entropies in the solid solution should be considered. The hematite-corundum solvus can be approximately reproduced by a symmetric, regular-like solution model with ΔG_(excess) = (W_H-TW_S)X_(hem)X_(cor), where W_H = 116 ± 10 kJ mol~(-1) and W_S = 32 ± 4 J mol~(-1) K~(-1). In this model, short-range order (SRO) of Fe/Al is neglected because SRO probably becomes important only at intermediate compositions close to Fe:Al = 1:1 but these comsitions cannot be synthesized. The volume of mixing is positive for Al-hematite but almost ideal for Fe-corundum. Moreover, the degree of deviation from Vegard's law for Al-hematite depends on the history of the samples. Introduction of Al into the hematite structure causes varying distortion of the hexagonal network of oxygen ions while the position of the metal ions remains intact. Distortion of the hexagonal network of oxygen ions attains a minimum at the composition (Fe_(0.95)Al_(0.05))_2O_3. The enthalpy of formation of FeAlO_3 from oxides at 298 K is 27.9 ± 1.8 kJ mol~(-1). Its estimated standard entropy (including configurational entropy due to disorder of Fe/Al) is 98.9 J mol~(-1) K~(-1), giving the standard free energy of formation at 298 K from oxides and elements as +19.1 ± 1.8 and -1144.2 ± 2.0 kJ mol~(-1), respectively. The heat capacity of FeAlO_3 is approximated as C_p(T in K) = 175.8 - 0.002472T - (1.958 * 10~6)/T~2 - 917.3/T~(0.5) + (7.546 * 10~(-6)) T~2 between 298 and 1550 K, based on differential scanning calorimetric measurements. No ferrous iron was detected in FeAlO_3 by Mossbauer spectroscopy. The ternary phase is entropy stabilized and is predicted to be stable above about 1730 ± 70 K, in good agreement with the experiment. Static lattice calculations show that the LiNbO_3-, FeGaO_3-, FeTiO_3-, and disordered corundum-like FeAlO_3 structures are less stable (in the order in which they are listed) than a mechanical mixture of corundum and hematite. Al high temperatures, the FeGaO_3-like structure is favored by its entropy, and its stability field appears on the phase diagram.
机译:利用高温氧化物熔体量热法和粉末X射线衍射图的Rietveld精制研究了赤铁矿-刚玉固溶体和三相FeAlO_3(具有FeGaO_3结构)的能级和结构。固溶体中的混合焓可以用多项式ΔH_(mix)= W X_(hem)(1-X_(hem))描述,其中W = 116±10 kJ mol〜(-1)。过量的混合焓太正以至于无法复制实验相图,因此应考虑固溶体中的过量熵。赤铁刚玉固溶体可以通过对称的,类似规则的溶液模型近似复制,其中ΔG_(excess)=(W_H-TW_S)X_(hem)X_(cor),其中W_H = 116±10 kJ mol〜(-1 ),W_S = 32±4 J mol〜(-1)K〜(-1)。在该模型中,Fe / Al的短程有序(SRO)被忽略了,因为SRO可能仅在接近Fe:Al = 1:1的中间成分时才变得重要,但这些化合物无法合成。赤铁矿的混合量为正,而铁刚玉的混合量几乎为理想。此外,赤铁矿与维加德定律的偏离程度取决于样品的历史。将Al引入赤铁矿结构会导致氧离子六边形网络发生各种变形,而金属离子的位置保持不变。氧离子六边形网络的畸变在成分(Fe_(0.95)Al_(0.05))_ 2O_3处达到最小值。在298 K下由氧化物形成FeAlO_3的焓为27.9±1.8 kJ mol〜(-1)。其估计的标准熵(包括由于Fe / Al紊乱引起的构型熵)为98.9 J mol〜(-1)K〜(-1),在298 K时由氧化物和元素形成的标准自由能为+19.1±分别为1.8和-1144.2±2.0 kJ mol〜(-1)。 FeAlO_3的热容近似为C_p(T in K)= 175.8-0.002472T-(1.958 * 10〜6)/ T〜2-917.3 / T〜(0.5)+(7.546 * 10〜(-6))基于差示扫描量热法测量,T〜2在298和1550 K之间。莫斯鲍尔光谱法在FeAlO_3中未检测到亚铁。三元相是熵稳定的,并被预测在约1730±70 K以上是稳定的,这与实验非常吻合。静态晶格计算表明,LiNbO_3-,FeGaO_3-,FeTiO_3-和无序刚玉状FeAlO_3结构(按列出的顺序)比刚玉和赤铁矿的机械混合物更不稳定(按列出的顺序)。在高温下,FeGaO_3型结构因其熵而受青睐,其稳定性场出现在相图中。

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