首页> 外文期刊>Physics and chemistry of minerals >Thermodynamic behaviour of the high-temperature P(1)over-bar-I(1)over-bar phase transition along the CaAl2Si2O8-SrAl2Si2O8 join
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Thermodynamic behaviour of the high-temperature P(1)over-bar-I(1)over-bar phase transition along the CaAl2Si2O8-SrAl2Si2O8 join

机译:沿CaAl2Si2O8-SrAl2Si2O8的高温P(1)-I-(1)-over-bar相变的热力学行为

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In situ high-temperature synchrotron radiation powder diffraction patterns were taken from room temperature to T = 740 degrees C from synthetic feldspars along the join CaAl2Si2O8-SrAl2Si2O8( An - SrF). Three samples of composition An(95)SrF(5), An(90)SrF(10) and An(85)SrF(15) were investigated, and the evolution of cell parameters with T was determined by Rietveld analysis of powder X-ray diffraction patterns. The high-temperature P (1) over bar -1- I (1) over bar phase transition, previously observed with T-c = 241 degrees C in anorthite, was found in An(95)SrF(5), An(90)SrF(10) and An(85)SrF(15) feldspars at T-c = 233(5)degrees, 195(2)degrees and 174(2)degrees C respectively. The transition was revealed by the disappearance of critical reflections and variations in the rate of change of cell parameters with temperature. A significant, although small ( between 0.0025 and 0.0012 at room temperature), spontaneous strain could be measured, allowing the thermodynamic behaviour of the transition to be modelled. A second-order trend for An(90)SrF(10) and An(85)SrF(15) [beta = 0.504(7) and 0.505(7) respectively] or nearly second-order for An(95)SrF(5)[beta = 0.458(4)] was observed in contrast with tricritical behaviour of end member anorthite. An extrapolation of the T-c versus composition to room temperature indicates that the critical composition for the P (1) over bar phase is An(60)SrF(40).
机译:从室温到合成长石沿CaAl2Si2O8-SrAl2Si2O8(An-SrF)的合成长石从室温获取高温同步辐射粉末衍射图。研究了三个组成为An(95)SrF(5),An(90)SrF(10)和An(85)SrF(15)的样品,并通过粉末X-的Rietveld分析确定了细胞参数随T的变化射线衍射图。在An(95)SrF(5),An(90)SrF中发现了先前在Tc = 241摄氏度的钙锰矿中观察到的棒-1- I(1)上棒相变上方的高温P(1) (10)和An(85)SrF(15)长石的Tc分别为233(5)°C,195(2)°C和174(2)°C。通过临界反射的消失和电池参数随温度变化的速率变化来揭示这种转变。可以测量到很大的自发应变,尽管很小(在室温下为0.0025至0.0012),但可以对转变的热力学行为进行建模。 An(90)SrF(10)和An(85)SrF(15)的二阶趋势[分别为beta = 0.504(7)和0.505(7)]或An(95)SrF(5 )[β= 0.458(4)]与端部成员无烟煤的三临界行为相反。 T-c对组成的外推至室温表明,棒相上P(1)的关键组成为An(60)SrF(40)。

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