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Experimental study of the isochoric heat capacity of tert-butanol in the critical and supercritical regions

机译:临界和超临界区叔丁醇等容热容的实验研究

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The one- and two-phase isochoric heat capacities (CV) of tert-butanol in the critical and supercritical regions have been measured with a high-temperature and high-pressure nearly constant-volume adiabatic calorimeter. The measurements were made in the temperature range from 296K to 524K for 21 liquid and 7 vapor isochores from 70.56kgm~(-3) to 763.98kgm~(-3). The isochoric heat capacity jump (quasi-static thermograms supplemented by the sensor of adiabatic control) technique was used to accurately measure of the phase transition parameters (ρ_S, T_S) in the critical region. The total experimental uncertainty of density (ρ_S), temperature (T_S), and isochoric heat capacity (C_V) measurements were estimated to be 0.02%, 15mK, and 2-3%, respectively. The critical temperature (T_C=506.35±0.2K) and the critical density (ρ_C=268.1±2kgm~(-3)) for tret-butanol were extracted from the measured saturated properties (C_(VS), T_S, ρ_S) near the critical point. The measured C_V and saturated density (ρ_S, T_S) data near the critical point have been analyzed and interpreted in terms of extended scaling equations for the selected thermodynamic paths (critical isochore and coexistence curve) to accurately calculate the values of the asymptotical critical amplitude (A0± and B_0). The experimentally derived value of the critical amplitude ratio A0+/A0-=0.525 is in good agreement with the value predicted by various scaling theories. The measured thermodynamic properties of tert-butanol near the critical point were also interpreted in terms of the "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. The Yang-Yang anomaly of strength parameter R_μ=-0.036 for tert-butanol was estimated using derived second temperature derivatives of pressure and chemical potential. The measured values of saturated one- (C'V1 and C"V1) and two-phase (C'V2 and C"V2) liquid and vapor isochoric heat capacities and saturated thermal properties (ρ_S, T_S) together with reported 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, (?P/?T)'V, (?V/?T)'P, (d~2PS/dT~2), and (d~2μ/dT~2) of tert-butanol at saturation near the critical point.
机译:临界和超临界区的叔丁醇的一相和两相等速热容(CV)已通过高温高压近等体积绝热热量计进行了测量。在296K到524K的温度范围内对21个液体和7个蒸气等压线进行了测量,测量范围为70.56kgm〜(-3)至763.98kgm〜(-3)。等容热容量跳跃(绝热控制传感器补充了准静态温度记录图)技术用于精确测量关键区域的相变参数(ρ_S,T_S)。密度(ρ_S),温度(T_S)和等容热容(C_V)测量的总实验不确定性分别估计为0.02%,15mK和2-3%。叔丁醇的临界温度(T_C = 506.35±0.2K)和临界密度(ρ_C= 268.1±2kgm〜(-3))是从附近的实测饱和度(C_(VS),T_S,ρ_S)中提取的。临界点。已针对选定的热力学路径(临界等时线和共存曲线)的扩展比例方程对扩展的测度方程进行了分析和解释,以精确计算渐近临界振幅的值( A0±和B_0)。临界振幅比A0 + / A0- = 0.525的实验得出的值与各种缩放理论所预测的值非常吻合。还根据临界现象的“完全定标”理论来解释在临界点附近测得的叔丁醇的热力学性质。特别是,估计了“完全”和“不完全缩放”项对共存曲线奇异直径的贡献。使用推导的压力和化学势的第二温度导数估算了叔丁醇的强度参数R_μ= -0.036的杨阳异常。饱和一相(C'V1和C“ V1)和两相(C'V2和C” V2)液体和蒸气的等容热容和饱和热特性(ρ_S,T_S)的测量值以及报告的蒸气压(P_S,T_S)数据用于计算其他导出的热力学性质,例如K_T,ΔH_(vap),C_P,C_S,W,(ΔP/ΔT)'V,(ΔV/ΔT)'P,( d〜2PS / dT〜2)和叔丁醇在临界点附近饱和时的(d〜2μ/ dT〜2)。

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