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Experimental study of the isochoric heat capacity of isobutanol in the critical and supercritical regions

机译:临界区和超临界区异丁醇等容热容的实验研究

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The one- and two-phase isochoric heat capacities (C_v) of isobutanol in the critical and supercritical regions have been measured with a high-temperature and high-pressure nearly constant-volume adia-batic calorimeter. The measurements were made in the temperature range from 324 K to 575 K for 23 isochores (16 liquid and 7 vapor) from 73.2 kgm~(-3) to 772.2 kgm~(-3). The isochoric heat capacity jump (quasi-static thermograms supplemented by the sensor of adiabatic control) technique have been used to accurately measure of the phase transition parameters (T_s, ρ_s). The total experimental uncertainty of density (ρ), temperature (T), and isochoric heat capacity (C_v) were estimated to be 0.06%, 15 mK, and 2-3%, respectively. The critical temperature (T_c = 547.65 ± 0.2 K) and the critical density (ρ_c = 272.95 ± 2 kg m~(-3)) for isobutanol were determined from the measured saturated properties (C_(VS), T_s, ρ_s) near the critical point. The measured C_v and saturated density (T_s, ρ_s) data near the critical point have been analyzed and interpreted in terms of extended scaling type equations for the selected thermodynamic paths (critical isochore and coexistence curve) to accurately calculate the values of the asymptotical critical amplitudes of heat capacity (A_0~±) and coexistence curve (B0). The experimentally derived value of the critical amplitude ratio A_0~+/A_0~- = 0.522 is in good agreement with the value predicted by various scaling theories. The measured thermodynamic properties (C_v, T_s, ρ_s) of isobutanol near the critical point were also interpreted in the terms of "complete scaling" theory of critical phenomena. In particularly, the contributions of the "complete" and "incomplete" scaling terms on the coexistence-curve singular diameter were estimated. We determined the values of the asymmetry parameters a3 and b2 of the coexistence curve singular diameter. The strength of the Yang-Yang anomaly R_μ for isobutanol was estimated using asymmetry parameters a3 and the contribution of the second temperature derivative of vapor-pressure and chemical potential in the singularity of two-phase C_(V2). The measured values of saturated one- and two-phase liquid and vapor isochoric heat capacities (C'_(V1) C"_(V1) C'_(V2), C"_(V2)) and saturated thermal (ρ_s, T_s) properties together with vapor-pressure (P_S, T_s) data were used to calculate other derived thermodynamic properties such as (K_T, ΔH_(vap), C_P, C_s, W, (partial derivP/partial derivT)'_V, (partial derivV/partial derivt)'_p, (d~2P_s/dT~2), and (d~2μ/dT~2) of isobutanol at saturation near the critical point.
机译:临界和超临界区的异丁醇的一相和两相等速热容量(C_v)已通过高温高压近等体积绝热量热仪进行了测量。在324 K至575 K的温度范围内,对73.2 kgm〜(-3)至772.2 kgm〜(-3)的等时点(16液体和7蒸气)进行了测量。等容热容跃变(绝热控制传感器补充的准静态热谱图)技术已用于精确测量相变参数(T_s,ρ_s)。密度(ρ),温度(T)和等容热容(C_v)的总实验不确定性分别估计为0.06%,15 mK和2-3%。异丁醇的临界温度(T_c = 547.65±0.2 K)和临界密度(ρ_c= 272.95±2 kg m〜(-3))由测量的饱和特性(C_(VS),T_s,ρ_s)确定。临界点。已针对所选热力学路径(临界等时线和共存曲线)的扩展比例类型方程对临界点附近的测得的C_v和饱和密度(T_s,ρ_s)数据进行了分析和解释,以准确计算渐近临界振幅的值热容量(A_0〜±)和共存曲线(B0)的关系。临界振幅比A_0〜+ / A_0〜-= 0.522的实验得出的值与各种缩放理论所预测的值非常吻合。临界点附近的异丁醇的热力学性质(C_v,T_s,ρ_s)也用临界现象的“完全定标”理论来解释。特别是,估计了“完整”和“不完整”缩放项对共存曲线奇异直径的贡献。我们确定了共存曲线奇异直径的不对称参数a3和b2的值。利用不对称参数a3估算了异丁醇的杨阳异常R_μ的强度,并利用了蒸气压和化学势的第二温度导数对两相C_(V2)的奇异性的贡献。饱和一相和两相液相和蒸气等容热容量(C'_(V1)C“ _(V1)C'_(V2),C” _(V2))和饱和热(ρ_s, T_s)特性与蒸气压(P_S,T_s)数据一起用于计算其他导出的热力学特性,例如(K_T,ΔH_(vap),C_P,C_s,W,(偏导数/偏导数)'_ V,(部分临界点附近饱和时的异丁醇的(d〜2P_s / dT〜2)和(d〜2μ/ dT〜2)。

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