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System Dy-Fe-O: thermodynamic properties of ternary oxides using Calvet calorimetry and solid-state electrochemical cell

机译:系统Dy-Fe-O:使用Calvet量热法和固态电化学池的三元氧化物的热力学性质

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摘要

The enthalpy increments and the standard molar Gibbs energies of formation of DyFeO_3(s) and Dy_3Fe_5O_(12)(s) have been measured using a Calvet micro-calorimeter and a solid oxide galvanic cell, respectively. A co-operative phase transition, related to anti-ferromagnetic to paramagnetic transformation, is apparent from the heat capacity data for DyFeO_3 at approx 648 K. A similar type of phase transition has been observed for Dy_3Fe_5O_(12) at approx 560 K which is related to ferrimagnetic to paramagnetic transformation. Enthalpy increment data for DyFeO_3(s) and Dy_3Fe_5O_(12)(s), except in the vicinity of the second-order transition, can be represented by the following polynomial expressions:{H~0_m(T) - H~0_m(298.15 K)} (J mol~(-1)) (+-1.1 percent)=-52754+142.9 X (T (K))+2.48 X 10~(-3) X (T (K))~2+2.951 X 10~6 X (T (K))~(-1); (298.15<= T (K) <= 1000) for DyFeO_3(s), and{H~0_m(T) - H~0_m(298.15 K)} (J mol~(-1)) (+-1.2 percent)=-191048+545.0 X (T (K))+2.0X10~(-5) X (T (K))~2+8.513 X 10~6 X (T (K)) ~(-1); (298.15 <= T (K) <= 1000)for Dy_3Fe_5O_(12)(s). The reversible emfs of the solid-state electrochemical cells: (-)Pt/{DyFeO_3(s) + Dy_2O_3(s) + Fe(s)}//YDT/CSZ//{Fe(s) + Fe_(0.95)O(s)}/Pt(+) and (-)Pt/{Fe(s) + Fe_(0.95)O(s)}//CSZ//{DyFeO_3(s) + Dy_3Fe_5O_(12)(s) + Fe_3O_4(s)}/Pt(+), were measured in the temperature range from 1021 to 1250 K and 1035 to 1250 K, respectively. The standard Gibbs energies of formation of solid DyFeO_3 and Dy_3Fe_5O_(12) calculated by the least squares regression analysis of the data obtained in the present study, and data for Fe_(0.95)O and Dy_2O_3 from the literature, are given by:DELTA_F G~0_m(DyFeO_3,s) (kJ mol~(-1)) (+-3.2) = -1339.9+0.2473 X (T (K)); (1021 <= T (K) <= 1548) andDELTA_F G~0_m(Dy_3Fe_5O_(12),s) (kJ mol~(-1)) (+-3.5) = -4850.4 + 0.9846 X (T (K)); (1035 <= T (K) <= 1250).The uncertainty estimates for DELTA_F G~0_m include the standard deviation in the emf and uncertainty in the data taken from the literature. Based on the thermodynamic information, oxygen potential diagram and chemical potential diagrams for the system Dy-Fe-O were developed at 1250 K.
机译:DyFeO_3(s)和Dy_3Fe_5O_(12)(s)的形成过程的焓增量和标准摩尔吉布斯能量已分别使用Calvet微热量计和固体氧化物原电池进行了测量。从DyFeO_3在约648 K时的热容数据可以明显看出与反铁磁到顺磁转变有关的合作相变。在DysO3_5O_(12)在约560 K时观察到了类似的相变。与亚铁磁到顺磁转换有关。 DyFeO_3(s)和Dy_3Fe_5O_(12)(s)的焓增量数据,除了二阶跃迁附近,可以由以下多项式表示:{H〜0_m(T)-H〜0_m(298.15) K)}(J mol〜(-1))(+ -1.1%)=-52754 + 142.9 X(T(K))+ 2.48 X 10〜(-3)X(T(K))〜2 + 2.951 X 10〜6 X(T(K))〜(-1); (DyFeO_3(s)的(298.15 <= T(K)<= 1000)),和{H〜0_m(T)-H〜0_m(298.15 K)}(J mol〜(-1))(+ -1.2%) = -191048 + 545.0 X(T(K))+ 2.0X10〜(-5)X(T(K))〜2 + 8.513 X 10〜6 X(T(K))〜(-1); (Dy_3Fe_5O_(12)(s)的(298.15 <= T(K)<= 1000)。固态电化学电池的可逆电动势:(-)Pt / {DyFeO_3(s)+ Dy_2O_3(s)+ Fe(s)} // YDT / CSZ // {Fe(s)+ Fe_(0.95)O (s)} / Pt(+)和(-)Pt / {Fe(s)+ Fe_(0.95)O(s)} // CSZ // {DyFeO_3(s)+ Dy_3Fe_5O_(12)(s)+ Fe_3O_4 (s)} / Pt(+)分别在1021至1250 K和1035至1250 K的温度范围内测量。通过本研究获得的数据的最小二乘回归分析计算得出的固体DyFeO_3和Dy_3Fe_5O_(12)的标准吉布斯能,以及文献中Fe_(0.95)O和Dy_2O_3的数据由下式给出:DELTA_F G 〜0_m(DyFeO_3,s)(kJ mol〜(-1))(+ -3.2)= -1339.9 + 0.2473 X(T(K)); (1021 <= T(K)<= 1548)和DELTA_F G〜0_m(Dy_3Fe_5O_(12),s)(kJ mol〜(-1))(+ -3.5)= -4850.4 + 0.9846 X(T(K)) ; (1035 <= T(K)<= 1250)。DELTA_F G〜0_m的不确定性估计包括电动势的标准偏差和来自文献的数据的不确定性。根据热力学信息,在1250 K下开发了Dy-Fe-O系统的氧势图和化学势图。

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