Tan-Trieu-Giang Nguyen , Carsten Wedler , Sven Pohl , Dan Penn , Roland Span , J.P. Martin Trusler , Monika Thol
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Due to the fundamental nature of the Helmholtz energy, the equation can be used to calculate all thermodynamic properties from one mathematical expression. In contrast to typical EOS of this kind, the boundary conditions are somewhat more restricted. The relevant temperature and pressure ranges are limited to typical pipeline and storage conditions of gaseous hydrogen, including temperatures relevant for measurements with critical nozzles (140 K to 370 K with pressures up to 100 MPa). The computational speed for the implementation of the correlation in measurement sensors plays a superior role. Therefore, the equation is kept as short as possible, and exponents are of integer-kind. 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引用次数: 0
摘要
在压力为 1 兆帕至 10 兆帕的条件下,使用圆柱形谐振器对温度范围在 273 K 至 323 K 之间的正常氢(正氢)进行了声速测量;在压力为 20 兆帕至 100 兆帕的条件下,使用双路径脉冲回波系统进行了声速测量。测量的相对扩展不确定度 (k = 2) 为 0.04 % 至 0.08 %。根据这些测量结果和文献中的数据,为计算正氢的热力学性质开发了一个基本状态方程(EOS)。该方程用亥姆霍兹能表示,自变量为温度和密度。由于亥姆霍兹能的基本性质,该方程可用于通过一个数学表达式计算所有热力学性质。与典型的此类 EOS 相比,边界条件受到了更多限制。相关的温度和压力范围仅限于气态氢的典型管道和存储条件,包括与临界喷嘴测量相关的温度(140 K 至 370 K,压力高达 100 MPa)。在测量传感器中实现相关性的计算速度起着至关重要的作用。因此,方程尽可能简短,指数为整数。大多数实验数据仍然在测量不确定范围内得到了重现。
Experimental speed-of-sound data and a fundamental equation of state for normal hydrogen optimized for flow measurements
Speed-of-sound measurements for normal hydrogen (n-hydrogen) in a temperature range between 273 K and 323 K were carried out using a cylindrical resonator at pressures from 1 MPa to 10 MPa and a dual-path pulse-echo system at pressures from 20 MPa to 100 MPa. The relative expanded uncertainties (k = 2) of the measurements range from 0.04 % to 0.08 %. Based on these measurements and data from the literature, a fundamental equation of state (EOS) was developed for the calculation of thermodynamic properties of n-hydrogen. It is expressed in terms of the Helmholtz energy with the independent variables temperature and density. Due to the fundamental nature of the Helmholtz energy, the equation can be used to calculate all thermodynamic properties from one mathematical expression. In contrast to typical EOS of this kind, the boundary conditions are somewhat more restricted. The relevant temperature and pressure ranges are limited to typical pipeline and storage conditions of gaseous hydrogen, including temperatures relevant for measurements with critical nozzles (140 K to 370 K with pressures up to 100 MPa). The computational speed for the implementation of the correlation in measurement sensors plays a superior role. Therefore, the equation is kept as short as possible, and exponents are of integer-kind. Most of the experimental data are still reproduced within their measurement uncertainties.
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