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The Planck-Benzinger thermal work function in the condensation of water vapor

机译:普朗克-本辛格热功函数在水蒸气冷凝中的作用

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Based on the Planck-Benzinger thermal work function using Chun's method, the innate temperature-invariant enthalpy at 0 K, Delta H-0(T-0), for the condensation of water vapor as well as the dimer, trimer, tetramer, and pentamer form in the vapor phase, was determined to be 0.447 kcal mol(-1) for vapor, 1.127 for the dimer, 0.555 for the trimer, 0.236 for the tetramer, and 0.079 kcal mol(-1) for the pentamer using Delta G(T) data reported by Ken et al. in 1968 and Kell and McLaurin in 1969. These results suggest that the predominant dimeric form is the most stable of these n-mers. Using Nemethy and Scheraga's 1962 data for the Helmholtz free energy of liquid water, the value of Delta H-0(T-0) was determined to be 1.21 kcal mol(-1). This is very close to the value for the energy of the hydrogen bond E-H of 1.32 kcal mol(-1) reported by Nemethy and Scheraga, using statistical thermodynamics. It seems dear that very little energy is required for interconversion between the hypothetical supercooled water vapor and glassy water at 0 K. A hypothetical supercooled water vapor at 0 K is apparently almost as highly associated as glassy water at that temperature, suggesting a dynamic equilibrium between vapor and liquid. This water vapor condensation is highly similar in its thermodynamic behavior to that of sequence-specific pairwise (dipeptide) hydrophobic interaction, except that the negative Gibbs free energy change minimum at < T-s >, the thermal setpoint for vapor condensation, where T Delta S = 0, occurs at a considerably lower temperature, 270 K (below 0 degrees C) compared with similar to 350 K. The temperature of condensation < T-cond > at which Delta G(T) = 0, where water vapor begins to condense, was found to be 383 K. In the case of a sequence-specific pairwise hydrophobic interaction, the melting temperature, < T-m >, where Delta G(T-m) = 0 was found to be 460 K. Only between two temperature limits, < T-h > = 99 K and < T-cond > = 383 K, where Delta G(T-cond) = 0, is the net chemical driving force favorable for polymorphism of glassy water and hypothetical supercooled water vapor. Analysis of the water vapor condensation process based on the Planck-Benzinger thermal work function confirms that a thermodynamic molecular switch occurs at 10 K, wherein a change of sign in [Delta C-p(T)](cond) leads to a true negative minimum in the Gibbs free energy of vapor condensation, and hence a maximum in the related equilibrium constant, K-cond. (c) 2006 Wiley Periodicals, Inc.
机译:基于使用Chun方法的普朗克-本辛格热功函数,在0 K时固有的温度不变焓Delta H-0(T-0),用于冷凝水蒸气以及二聚体,三聚体,四聚体和使用Delta G,确定气相中的五聚体形式为:蒸气的0.447 kcal mol(-1),二聚体的1.127,三聚体的0.555,四聚体的0.236和五聚体的0.079 kcal mol(-1)。 (T)数据由Ken等报道。 1968年的Kell和McLaurin的1969年。这些结果表明,主要的二聚体形式是这些n-mer中最稳定的形式。使用Nemethy和Scheraga 1962年的液态水亥姆霍兹自由能数据,测得的Delta H-0(T-0)值为1.21 kcal mol(-1)。这与Nemethy和Scheraga使用统计热力学报道的氢键E-H的能量值1.32 kcal mol(-1)非常接近。看起来亲爱的,假设的过冷水蒸气和0 K下的玻璃状水之间的相互转化所需的能量很小。假设0 K下的假设过冷水蒸气与该温度下的玻璃状水几乎一样高的缔合力,表明两者之间存在动态平衡。蒸气和液体。该水蒸气冷凝在热力学行为上与序列特定的成对(二肽)疏水相互作用高度相似,不同之处在于负Gibbs自由能在(蒸气冷凝的热设定值)处变化最小,其中T Delta S = 0发生在比350 K低得多的270 K(低于0摄氏度)的温度下。冷凝温度,在该温度下Delta G(T)= 0,水蒸气开始冷凝,发现为383K。在序列特定的成对疏水相互作用中,熔解温度,其中Delta G(Tm)= 0为460K。仅在两个温度范围之间, = 99 K且 = 383 K,其中Delta G(T-cond)= 0,是有利于玻璃水和假设的过冷水蒸气多态性的净化学驱动力。基于Planck-Benzinger热功函数的水蒸气冷凝过程分析证实,在10 K时会发生热力学分子转换,其中[Delta Cp(T)](cond)的正负号变化会导致真实的负最小值。蒸汽冷凝的吉布斯自由能,因此在相关的平衡常数K-cond中达到最大值。 (c)2006年Wiley Periodicals,Inc.

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