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氦氧混合气体的压缩性和电容系数。

The compressibility and the capacitance coefficient of helium-oxygen atmospheres.

作者信息

Imbert G, Dejours P, Hildwein G

出版信息

Undersea Biomed Res. 1982 Dec;9(4):305-14.

PMID:7168095
Abstract

The capacitance coefficient beta of an ideal gas mixture depends only on its temperature T, and its value is derived from the ideal gas law (i.e., beta = 1/RT, R being the ideal gas constant). But real gases behave as ideal gases only at low pressures, and this would not be the case in deep diving. High pressures of helium-oxygen are used in human and animal experimental dives (up to 7 or 12 MPa or more, respectively). At such pressures deviations from the ideal gas law cannot be neglected in hyperbaric atmospheres with respect to current accuracy of measuring instruments. As shown both theoretically and experimentally by this study, the non-ideal nature of helium-oxygen has a significant effect on the capacitance coefficient of hyperbaric atmospheres. The theoretical study is based on interaction energy in either homogeneous (He-He and O2-O2) or heterogeneous (He-O2) molecular pairs, and on the virial equation of state for gas mixtures. The experimental study is based on weight determination of samples of known volume of binary helium-oxygen mixtures, which are prepared in well-controlled pressure and temperature conditions. Our experimental results are in good agreement with theoretical predictions. 1) The helium compressibility factor ZHe increases linearly with pressure [ZHe = 1 + 0.0045 P (in MPa) at 30 degrees C]; and 2) in same temperature and pressure conditions (T = 303 K and P = 0.1 to 15 MPa), the same value for Z is valid for a helium-oxygen binary mixture and for pure helium. As derived from the equation of state of real gases, the capacitance coefficient is inversely related to Z (beta = 1/ZRT); therefore, for helium-oxygen mixtures, this coefficient would decrease with increasing pressure. A table is given for theoretical values of helium-oxygen capacitance coefficient, at pressures ranging from 0.1 to 15.0 MPa and at temperatures ranging from 25 degrees C to 37 degrees C.

摘要

理想气体混合物的电容系数β仅取决于其温度T,其值由理想气体定律推导得出(即β = 1/RT,R为理想气体常数)。但实际气体仅在低压下表现为理想气体,在深潜中并非如此。在人体和动物实验潜水中使用了高压氦氧混合气(分别高达7或12兆帕甚至更高)。在这样的压力下,就目前测量仪器的精度而言,在高压环境中理想气体定律的偏差不可忽略。本研究通过理论和实验均表明,氦氧混合气的非理想性质对高压环境的电容系数有显著影响。理论研究基于均相(He-He和O2-O2)或异相(He-O2)分子对中的相互作用能以及气体混合物的维里状态方程。实验研究基于在精确控制的压力和温度条件下制备的已知体积的二元氦氧混合气样品的重量测定。我们的实验结果与理论预测吻合良好。1)氦的压缩因子ZHe随压力呈线性增加[在30℃时,ZHe = 1 + 0.0045P(P的单位为兆帕)];2)在相同温度和压力条件下(T = 303K,P = 0.1至15兆帕),氦氧二元混合物和纯氦的Z值相同。根据实际气体状态方程推导,电容系数与Z成反比(β = 1/ZRT);因此,对于氦氧混合物,该系数会随压力增加而减小。给出了一张表格,列出了压力范围为0.1至15.0兆帕、温度范围为25℃至37℃时氦氧电容系数的理论值。

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