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Free energy of charge transfer and intraprotein electric field: method of calculation depends on the charge state of protein at a given structure

机译:电荷转移和蛋白质内电场的自由能:计算方法取决于给定结构上蛋白质的电荷状态

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Free energy of charge transfer presents a basic characteristic of reactions such as protonation, oxido-reduction and similar. Evaluation of this quantity requires calculation of charging energy. Proteins are structured dielectrics, and a consistent incorporation of their structure into calculation of intraprotein electric field results in expression for charging energy of an active group in protein , which is essentially different from that for a simple dielectric. An algorithm for semi-continuum calculation of relevant free energies is described. First of the two components of charging energy in protein, energy of the medium response to charge redistribution in reactants, should be always calculated as the charging energy by the charge redistribution using the static dielectric constant of protein. The second term is interaction energy of the charge redistribution with the 'frozen' electric field of the system before reaction. Charges of protein groups, at which the protein structure has been determined, are often different from those before reaction of charge transfer, so is the corresponding intraprotein field. The field is expressed through either both the optical and static dielectric constants of protein or only optical one depending on whether the charges of protein groups before reaction and upon structural analysis are the same or not. Proper allowance for difference in charges of reacting groups before reaction and upon structural analysis of protein is thermodynamically necessary and quantitatively important. The expression for activation free energy for charge transfer in proteins is derived in the form presenting explicitly an invariant contribution of protein structure.
机译:电荷转移的自由能表现出诸如质子化,氧化还原等反应的基本特征。评估此数量需要计算充电能量。蛋白质是结构化的电介质,将其结构一致地整合到蛋白质内电场的计算中会导致表达蛋白质中活性基团的电荷能量,这与简单电介质的本质不同。描述了一种用于相关自由能的半连续计算的算法。蛋白质中电荷能量的两个组成部分中的第一个,即介质对反应物中电荷再分布的响应能量,应始终使用蛋白质的静态介电常数通过电荷再分布计算为电荷能。第二项是反应前电荷重新分布与系统的“冻结”电场的相互作用能。已确定蛋白质结构的蛋白质基团的电荷通常与电荷转移反应之前的电荷不同,相应的蛋白质内场也是如此。通过蛋白质的光学和静态介电常数来表示该场,或者仅通过光学的形式来表示,这取决于反应之前和根据结构分析的蛋白质基团的电荷是否相同。在反应之前和蛋白质结构分析时,适当考虑反应基团电荷的差异在热力学上是必要的,并且在数量上很重要。蛋白质中用于电荷转移的活化自由能的表达形式明确代表了蛋白质结构的不变贡献。

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