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Phase Diagram for Ammonia-Water Mixtures at High Pressures:udImplications for Icy Satellites

机译:高压氨水混合物的相图: ud对冰冷卫星的影响

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摘要

The (NH_3)x(H_20)_(1.x) phase diagram for 0 ≤ X ≤ 0.50 has been reexamined at temperatures from 125 K to 400 K and at pressures to 6.0 GPa using diamond-anvil cells. By electroplating the gasket materials with gold, complicated reactions between sample solutions and gasket materials, which affected earlier studies, have been avoided. Sample pressures were determined using the ruby-luminescence technique, and phase assignments were made using optical characterization. Phase assignments were confirmed byudRaman spectroscopy. At room temperature the stable phases observed were fluid, high pressure ices (VI and VII), and ammonia monohydrate, NH_3·H_2O. The Ice VI and Ice VII liquidi at 295 K were extrapolated to intersect at X = 0.26 ± 0.01 and 2.1 GPa. At room temperature, the eutectic for Ice VII and NH_3·H_2O was observed at 3.3 ± 0.2 GPa, and extrapolation of the room temperature liquidus indicates that the cotectic composition is near X= 0.45. Near X= 0.33. the stable phases were high pressure ices (VI, VII, and VIII), NH_3·H_2O, and another phase tentatively identified as ammonia dihydrate, NH_3·2H_2O. At this composition, the Ice VI liquidus and the congruent melting curve of NH_3·2H_2O interesect at 1.8 ± 0.2 GPa and 252 ± 5 K, and the Ice VII liquidus is approximately linear with a slope of 0.016 ± 0.002 GPa K^(-1. To within the uncertainty of the experiment, the Ice VI liquidus continues smoothly from the Ice VII liquidus. The quadruple point among NH_3·H_2O, NH_3·H2O , Ice VI, and fluid is located at 250 ± 5 K and 1.9 ± 0.3 GPa, with the accompanying double cotectic at a composition of X= 0.36 ± O.Ql. The eutectic for NH_3·H_2O and Ice VII is approximately linear with a slope of 0.033 ± 0.003 GPa K^(-1). We have applied these data to the interior of Titan in a manner similar to theudanalysis of Lunine and Stevenson (1987). The main implication of these results is that Titan is likelyudto have a thicker NH_3·H_2O ocean than previously suspected, because the stability field of NH_3·2H_2O isudsmaller than previously supposed. Implications for methane and ammonia volcanism on Titan are briefly discussed. The experimentally observed reactivity between the liquid and iron (for example) may also have implications for planetary and satellite evolution.
机译:使用金刚石砧盒,在125 K至400 K的温度和6.0 GPa的压力下,重新检查了0≤X≤0.50的(NH_3)x(H_20)_(1.x)相图。通过用金电镀垫片材料,可以避免样品溶液和垫片材料之间的复杂反应,而这会影响早期的研究。使用红宝石发光技术确定样品压力,并使用光学表征进行相分配。相位分配通过 udRaman光谱法确认。在室温下,观察到的稳定相是流体,高压冰(VI和VII)和一水氨NH_3·H_2O。推断在295 K处的Ice VI和Ice VII液体在X = 0.26±0.01和2.1 GPa处相交。在室温下,Ice VII和NH_3·H_2O的共晶在3.3±0.2 GPa处观察到,室温液相线的外推表明,共晶组成在X = 0.45附近。 X接近0.33。稳定相为高压冰(VI,VII和VIII)NH_3·H_2O,另一相暂定为氨水合物NH_3·2H_2O。在此组成下,Ice VI液相线和NH_3·2H_2O的全融曲线在1.8±0.2 GPa和252±5 K处相交,Ice VII液相线近似呈线性,斜率为0.016±0.002 GPa K ^(-1) 。在实验的不确定性范围内,Ice VI液相线从Ice VII液相线继续平稳,NH_3·H_2O,NH_3·H2O,Ice VI和流体之间的四点位于250±5 K和1.9±0.3 GPa ,伴随的双共晶组成为X = 0.36±O.Ql. NH_3·H_2O和Ice VII的共晶近似呈线性,斜率为0.033±0.003 GPa K ^(-1),我们已经应用了这些数据这些结果的主要含义是,土卫六可能具有比以前所怀疑的更厚的NH_3·H_2O海洋,因为它的稳定场NH_3·2H_2O比以前想象的要小。甲烷和氨气对山雀的影响简要讨论。实验观察到的液体和铁之间的反应性(例如)也可能对行星和卫星的演化产生影响。

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