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A thermodynamic approach to alamethicm pore formation

机译:一种热力学方法来形成阿拉法西姆孔

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摘要

The structure and energetics of alamethicin Rf30 monomer to nonamer in cylindrical pores of 5 to 11 A radius are investigated using molecular dynamics simulations in an implicit membrane model that includes the free energy cost of acyl chain hydrophobic area exposure. Stable, low energy pores are obtained for certain combinations of radius and oligomeric number. The trimer and the tetramer formed 6 A pores that appear closed while the larger oligomers formed open pores at their optimal radius. The hexamer in an 8 A pore and the octamer in an 11 A pore give the lowest effective energy per monomer. However, all oligomers beyond the pentamer have comparable energies, consistent with the observation of multiple conductance levels. The results are consistent with the widely accepted "barrel-stave" model. The N terminal portion of the molecule exhibits smaller tilt with respect to the membrane normal than the C terminal portion, resulting in a pore shape that is a hybrid between a funnel and an hourglass. Transmembrane voltage has little effect on the structure of the oligomers but enhances or decreases their stability depending on its orientation. Antiparallel bundles are lower in energy than the commonly accepted parallel ones and could be present under certain experimental conditions. Dry aggregates (without an aqueous pore) have lower average effective energy than the corresponding aggregates in a pore, suggesting that alamethicin pores may be excited states that are stabilized in part by voltage and in part by the ion flow itself.
机译:使用隐含膜模型中的分子动力学模拟,研究了芳香化霉素Rf30单体在9至11 A半径的圆柱孔中生成九聚体的结构和能量,其中包括暴露于酰基链疏水区域的自由能成本。对于半径和低聚物数的某些组合,可获得稳定的低能孔。三聚体和四聚体形成看起来是封闭的6 A孔,而较大的低聚物在其最佳半径下形成开放孔。 8 A孔中的六聚体和11 A孔中的八聚体使每个单体的最低有效能量降低。但是,五聚体以外的所有低聚物具有可比的能量,这与观察到的多个电导水平一致。结果与广泛接受的“桶壁”模型一致。分子的N末端部分相对于膜法向倾斜的倾斜度小于C末端部分,从而形成了漏斗和沙漏之间混合的孔形状。跨膜电压对低聚物的结构影响很小,但是取决于其取向而提高或降低其稳定性。反平行束的能量低于普遍接受的平行束,并且可能在某些实验条件下出现。干聚集体(无水孔)比孔中的相应聚集体具有更低的平均有效能量,这表明阿来霉素孔可能是激发态,其部分通过电压稳定,部分通过离子流本身稳定。

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