半柔性聚酰胺的结构转变

Rakesh Palariya, Sunil P. Singh
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摘要

聚阴离子(PA)是由带正电和负电的单体沿主干组成的带电聚合物。带电单体的序列和链的弯曲对 PA 的构象和动力学行为有重大影响。利用粗粒度分子动力学模拟,我们全面研究了柔性和半柔性 PA 的结构和动力学特性。模拟结果表明,柔性 PA 链在电荷序列的参数空间中显示出从线圈到球状的过渡。此外,均方位移(MSD)(表示为⟨(Δr(t))2⟩)的行为揭示了不同的动态,特别是交替序列和电荷分离序列。MSD 遵循幂律行为,其中⟨(Δr(t))2⟩∼tβ,在没有流体动力学相互作用的情况下,交替序列和电荷隔离序列分别为 β≈ 3/5 和 β≈ 1/2。然而,当加入流体动力学相互作用时,电荷隔离序列的指数 β 变为 ∼3/5,混合良好的交替序列的指数 β 变为 2/3。对于半柔性 PA 链,改变弯曲刚度和静电相互作用强度(Γe)会导致不同的迷人构象状态,包括球状、束状和环状构象。我们的研究表明,在中间弯曲机制下,PA 可获得环状和发夹状构象。根据回旋张量特征值的比率估算出的形状因子确定了各种构象之间的转变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Structural transitions of a semi-flexible polyampholyte
Polyampholytes (PAs) are charged polymers composed of positively and negatively charged monomers along their backbone. The sequence of the charged monomers and the bending of the chain significantly influence the conformation and dynamical behavior of the PA. Using coarse-grained molecular dynamics simulations, we comprehensively study the structural and dynamical properties of flexible and semi-flexible PAs. The simulation results demonstrate a flexible PA chain, displaying a transition from a coil to a globule in the parameter space of the charge sequence. In addition, the behavior of the mean-square displacement (MSD), denoted as ⟨(Δr(t))2⟩, reveals distinct dynamics, specifically for the alternating and charge-segregated sequences. The MSD follows a power-law behavior, where ⟨(Δr(t))2⟩ ∼ tβ, with β ≈ 3/5 and β ≈ 1/2 for the alternating sequence and the charge-segregated sequence in the absence of hydrodynamic interactions, respectively. However, when hydrodynamic interactions are incorporated, the exponent β shifts to ∼3/5 for the charge-segregated sequence and 2/3 for the well-mixed alternating sequence. For a semi-flexible PA chain, varying the bending rigidity and electrostatic interaction strength (Γe) leads to distinct, fascinating conformational states, including globule, bundle, and torus-like conformations. We show that PAs acquire circular and hairpin-like conformations in the intermediate bending regime. The transition between various conformations is identified in terms of the shape factor estimated from the ratios of eigenvalues of the gyration tensor.
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