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动力学方法实验中的熵考量

Entropy considerations in kinetic method experiments.

作者信息

Wesdemiotis Chrys

机构信息

Department of Chemistry, University of Akron, Akron, Ohio 44325-3601, USA.

出版信息

J Mass Spectrom. 2004 Sep;39(9):998-1003. doi: 10.1002/jms.681.

Abstract

In extended kinetic method experiments, relative binding enthalpies ('affinities') and relative entropies are obtained based on unimolecular dissociation kinetics. A series of ion-bound dimers A-X-B(i) is formed, in which the sample (A) and structurally similar reference molecules (B(i)) are bridged by a central cation or anion (X). The branching ratios of the A-X-B(i) set to A-X and B(i)-X are determined at different internal energies, usually by subjecting A-X-B(i) to collisionally activated dissociation at various collision energies. The dependence of the natural logarithm of the branching ratios on the corresponding B(i)-X bond enthalpies (X affinities of B(i)) is evaluated as a function of internal energy to thereby deduce the A-X bond enthalpy (X affinity of A) as well as an apparent relative entropy of the competitive dissociation channels, Delta(DeltaS(app)). Experiments with proton- and Na(+)-bound dimers show that this approach can yield accurate binding enthalpies. In contrast, the derived Delta(DeltaS(app)) values do not correlate with the corresponding thermodynamic entropy differences between the channels leading to A-X and B(i)-X, even after scaling. The observed trends are reconciled by the transition state switching model. According to this model, the kinetics of barrierless dissociations, such as those encountered in kinetic method studies, are dominated by a family of tight transition states ('entropy bottlenecks') lying lower in energy than the corresponding dissociation thresholds. In general, the relative energies of these tight transition states approximately match those of the dissociation products, but their relative entropies tend to be much smaller, as observed experimentally.

摘要

在扩展动力学方法实验中,基于单分子解离动力学获得相对结合焓(“亲和力”)和相对熵。形成了一系列离子结合的二聚体A-X-B(i),其中样品(A)和结构相似的参考分子(B(i))由中心阳离子或阴离子(X)桥连。通常通过在不同碰撞能量下使A-X-B(i)发生碰撞激活解离,来确定A-X-B(i)分解为A-X和B(i)-X的分支比。将分支比的自然对数对相应的B(i)-X键焓(B(i)的X亲和力)的依赖性作为内能的函数进行评估,从而推导出A-X键焓(A的X亲和力)以及竞争解离通道的表观相对熵Δ(ΔS(app))。质子结合和Na(+)结合二聚体的实验表明,这种方法可以产生准确的结合焓。相比之下,即使经过缩放,导出的Δ(ΔS(app))值也与导致A-X和B(i)-X的通道之间相应的热力学熵差不相关。过渡态切换模型解释了观察到的趋势。根据该模型,无势垒解离的动力学,如动力学方法研究中遇到的那些,由一族紧密的过渡态(“熵瓶颈”)主导,这些过渡态的能量低于相应的解离阈值。一般来说,这些紧密过渡态的相对能量与解离产物的相对能量大致匹配,但正如实验观察到的那样,它们的相对熵往往要小得多。

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