首页> 外文期刊>Geochimica et Cosmochimica Acta: Journal of the Geochemical Society and the Meteoritical Society >HEAT CAPACITY MEASUREMENTS OF SYNTHETIC PYROPE-GROSSULAR GARNETS BETWEEN 320 AND 1000 K BY DIFFERENTIAL SCANNING CALORIMETRY
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HEAT CAPACITY MEASUREMENTS OF SYNTHETIC PYROPE-GROSSULAR GARNETS BETWEEN 320 AND 1000 K BY DIFFERENTIAL SCANNING CALORIMETRY

机译:用差示扫描量热法测量320和1000 K之间的合成焦-石榴石石榴石的热容量

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The heat capacity of synthetic periclase (MgO), pyrope (Mg3Al2Si3O12), grossular (Ca3Al2-Si3O12), and four pyrope-grossular solid solutions (PY(89.8)Gr(10.2), PY(73.6)Gr(26.4), PY(48.8)Gr(51.2), PY(24.0)Gr(76.0)) has been measured between 320 and 1000 K by differential scanning calorimetry. Measurements were made in both interval-scanning and step-scanning modes; with the latter method, Cp was determined to a precision of better than +/- 1%. The results, together with previous calorimetric measurements on synthetic grossular and pyrope, now permit a complete description of the heat capacities for both phases between 10-1200 K and 10-1350 K, respectively. The following best-fit equations for the temperature range from 298 to 1200 K were obtained for pyrope and grossular, respectively (T in Kelvin and Cp in J/mol*K): Cp(pyrope) = 542.01 - 1387.07 . T--0.5-20.492 x 10(6) . T-2 + 2500.67 x 10(6) . T-3; Cp(grossular) = 607.81 - 3214.49 . T--0.5 - 12.141 x 10(6) . T-2 + 1269.92 x 10(6) . T-3. For the solid solution garnets a model assuming ideal mixing (linear combination) of molar heat capacities of the endmember phases reproduces the experimental heat capacities within errors. This indicates that the vibrational entropies of mixing and enthalpies of mixing are temperature-independent between room temperature and 1000 K. It is expected that excess heat capacities of mixing are not present in most silicate solid solutions at temperatures between 320 and 1000 K. [References: 32]
机译:合成百事可乐(MgO),发烧级(Mg3Al2Si3O12),颗粒状(Ca3Al2-Si3O12)和四种发烧型颗粒固溶体(PY(89.8)Gr(10.2),PY(73.6)Gr(26.4),PY(已通过差示扫描量热法在320至1000 K之间测量了48.8)Gr(51.2),PY(24.0)Gr(76.0))。在间隔扫描和步进扫描模式下均进行了测量;使用后一种方法,测定的Cp精度优于+/- 1%。该结果以及以前对合成粗粒和焦炉石的量热测量结果,现在可以完整地分别描述10-1200 K和10-1350 K之间两个相的热容。分别针对焦油和焦油分别获得以下针对298至1200 K的温度范围的最佳拟合方程(开尔文中的T和J / mol * K中的Cp):Cp(pyrope)= 542.01-1387.07。 T--0.5-20.492 x 10(6)。 T-2 + 2500.67 x 10(6)。 T-3; Cp(总值)= 607.81-3214.49。 T--0.5-12.141 x 10(6) T-2 + 1269.92 x 10(6)。 T-3。对于固溶石榴石,假定末端构件相的摩尔热容的理想混合(线性组合)的模型将在误差范围内再现实验热容。这表明在室温至1000 K之间,混合的振动熵和混合的焓与温度无关。预计在320至1000 K的温度下,大多数硅酸盐固溶体中不存在过量的混合热容量。 :32]

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