用球形谐振器测量的沼气混合物 $CH_{4}$ + $N_{2}$ + $CO_{2}$ + $CO$ 在 $T$ = (273、300 和 325) K 条件下从 $p$ = (1-12) MPa 产生的声速

Daniel Lozano-Martín, José J. Segovia, M. Carmen Martín, Teresa Fernández-Vicente, D. del Campo
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引用次数: 0

摘要

本研究旨在使用球形声学共振器,在 $p$ = (1-12) MPa 和 $T$ = (273, 300 和 325) K 条件下,测量由 $CH_{4}$ + $N_{2}$ + $CO_{2}$ + $CO$ 组成的沼气混合物中的声速 $c$。将结果拟合到病毒式声学状态方程,得到病毒式声学系数 $\beta_{a}$ 和 $\gamma_{a}$,并推断到零压,确定了完美气体的绝热系数 $\gamma^{pg}$,以及完美气体的等压和等热容,分别为 $C_{p}^{pg}$ 和 $C_{V}^{pg}$。声速是在相对不确定性为 10^{6}$ 中平均扩大 165 份(k$ = 2)的情况下获得的,并与这种混合物(类似天然气的混合物)的参考状态方程 EoS GERG-2008 预测的结果进行了比较。实验数据与该模型估算值之间的相对偏差在 $T$ = 325 K 时小于 700 份(10^{6}$),在 $T$ = 300 K 时低于 400 份(10^{6}$),在测量不确定性范围内,但在本研究的最高压力数据下,在等温线 $T$ = 273 K 时明显更高,甚至达到 3 400 份(10^{6}$)以上。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Speeds of sound for a biogas mixture $CH_{4}$ + $N_{2}$ + $CO_{2}$ + $CO$ from $p$ = (1-12) MPa at $T$ = (273, 300 and 325) K measured with a spherical resonator
The present work aims to measure speeds of sound $c$ in a biogas mixture of $CH_{4}$ + $N_{2}$ + $CO_{2}$ + $CO$, at $p$ = (1-12) MPa and $T$ = (273, 300 and 325) K, using a spherical acoustical resonator. The results are fitted to the virial acoustic equation of state, and the virial acoustic coefficients are obtained, $\beta_{a}$ and $\gamma_{a}$ and extrapolated to zero pressure, determining the adiabatic coefficient as perfect gas, $\gamma^{pg}$, and the isobaric and isochoric heat capacities as perfect gas, $C_{p}^{pg}$ and $C_{V}^{pg}$, respectively. The speeds of sound are acquired with a mean expanded relative uncertainty of 165 parts in $10^{6}$ ($k$ = 2) and are compared with the results predicted by the reference equation of state for this kind of mixture (natural gas-like mixtures), EoS GERG-2008. Relative deviations between experimental data and values estimated by this model were less than 700 parts in $10^{6}$ at $T$ = 325 K, and below 400 parts in $10^{6}$, and within measurement uncertainty of at $T$ = 300 K, although appreciably higher at isotherm $T$ = 273 K at the highest pressure data for this work, and even reaching values above 3 400 parts in $10^{6}$.
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