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首页> 外文期刊>The Journal of Chemical Thermodynamics >PHASE DIAGRAMS OF MOLAR VOLUME AGAINST MOLE FRACTIONS AT GIVEN TEMPERATURES AND PRESSURES FOR (X(A)AR+X(B)XE+(1-X(A)-X(B))NH3)(A)
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PHASE DIAGRAMS OF MOLAR VOLUME AGAINST MOLE FRACTIONS AT GIVEN TEMPERATURES AND PRESSURES FOR (X(A)AR+X(B)XE+(1-X(A)-X(B))NH3)(A)

机译:给定温度和压力下(X(A)AR + X(B)XE +(1-X(A)-X(B))NH3)(A)的摩尔体积相对于摩尔分数的相图

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The phase behaviour of (argon + xenon + ammonia) was investigated at the temperatures T = 273.15 K, 298.15 K, 323.15 K, 348.15 K, and 373.15 K and pressures p from 5.0 MPa up to 200.0 MPa. The results are given in a table and are shown as molar volume against mole fraction (V-m,chi(A),chi(B)) diagrams. The measurements were carried out in a cylindrical autoclave with a moveable piston and a window allowing adjustment and observation of phase equilibria at given p and T. Samples were taken from the coexisting phases and were analysed to obtain their molar volumes and compositions. For given p and T the ends of the corresponding tie lines lie on isobaric and isothermal curves. Isothermal surfaces were drawn containing several isobars. Also isobaric surfaces with different isothermal curves were drawn. It is shown how isothermal surfaces can be combined with isobaric ones. The resulting intersection curves represent again the geometrical locus of all tie lines for given pressures and temperatures. In the (V-m,chi(A),chi(B)) diagram the isothermal surfaces at T = 373.15 K and 348.15 K stretch between the gas and liquid molar volumes of pure NH3. The corresponding binary isotherms, which are not interrupted, are their boundary curves. At lower temperatures one or two of the binary isotherms are interrupted. Due to this behaviour the isothermal surfaces at those temperatures are more complex. The five investigated isothermal surfaces are, however, closely related to one another and the shape of an isothermal surface is strongly dependent on the shape of the corresponding binary isotherm. The isobaric surfaces at higher pressures behave similarly. However, at lower pressures their shapes become very complex. In comparison the critical surface shows no great variation in shape or molar volume at the investigated temperatures and pressures, but consists of two separate parts. (C) 1995 Academic Press Limited. [References: 11]
机译:在温度T = 273.15 K,298.15 K,323.15 K,348.15 K和373.15 K以及压力p从5.0 MPa到200.0 MPa的条件下研究了(氩气+氙气+氨气)的相态行为。结果列于表中,并以摩尔体积相对于摩尔分数(V-m,chi(A),chi(B))的图表表示。在具有可移动活塞和窗口的圆柱形高压釜中进行测量,该窗口允许调节和观察在给定的p和T下的相平衡。从共存的相中取样并进行分析以获得其摩尔体积和组成。对于给定的p和T,相应的连接线的末端位于等压曲线和等温曲线上。绘制等温面,其中包含几个等压线。还绘制了具有不同等温曲线的等压面。它显示了等温面如何与等压面组合。对于给定的压力和温度,所得的相交曲线再次表示所有连接线的几何轨迹。在(V-m,chi(A),chi(B))图中,T = 373.15 K和348.15 K处的等温面在纯NH3的气体和液体摩尔体积之间伸展。相应的二进制等温线(不间断)是它们的边界曲线。在较低的温度下,一个或两个二元等温线会中断。由于这种行为,在那些温度下的等温表面更加复杂。但是,研究的五个等温面彼此密切相关,并且等温面的形状在很大程度上取决于相应的二元等温线的形状。在较高压力下的等压表面的行为类似。然而,在较低压力下,它们的形状变得非常复杂。相比之下,在研究的温度和压力下,临界表面的形状或摩尔体积没有很大变化,但由两个独立的部分组成。 (C)1995 Academic Press Limited。 [参考:11]

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