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Theory of mechanical unfolding of homopolymer globule: All-or-none transition in force-clamp mode vs phase coexistence in position-clamp mode

机译:均聚物球的机械展开理论:力钳模式下的全或无跃迁与位置钳模式下的相共存

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Equilibrium mechanical unfolding of a globule formed by long flexible homopolymer chain collapsed in a poor solvent and subjected to an extensional force f (force-clamp mode) or extensional deformation D (position-clamp mode) is studied theoretically. Our analysis, like all previous analysis of this problem, shows that the globule behaves essentially differently in two modes of extension. In the force-clamp mode, mechanical unfolding of the globule with increasing applied force occurs without intramolecular microphase segregation, and at certain threshold value of the pulling force the globule unfolds as a whole ("all-or-none" transition). The value of the threshold force and the corresponding jump in the distance between the chain ends increase with a deterioration of the solvent quality and/or with an increase in the degree of polymerization. In the position-clamp mode, the globule unfolding occurs via intramolecular microphase coexistence of globular and extended microphases followed by an abrupt unraveling transition. Reaction force in the microphase segregation regime demonstrates an "anomalous" decrease with increasing extension. Comparison of deformation curves in force and position-clamp modes demonstrates that at weak and strong extensions the curves for two modes coincide, differences are observed in the intermediate extension range. Another unfolding scenario is typical for short globules: in both modes of extension they unfold continuously, without jumps or intramolecular microphase coexistence, by passing a sequence of uniformly elongated configurations. The values of the critical chain length, N_(cr), separating long and short chain behavior are slightly different for two extension modes: N_(cr,f) < N_(cr,D).
机译:理论上研究了由在不良溶剂中塌陷并受到拉伸力f(力钳模)或拉伸变形D(位置钳模)的长的柔性均聚物链形成的小球的平衡机械展开。与以前对该问题的所有分析一样,我们的分析表明,球在两种扩展模式下的行为本质上不同。在力钳模式中,在没有分子内微相偏析的情况下,随着施加的力的增加,小球发生机械展开,并且在拉力的特定阈值下,小球整体上展开(“全有或全无”过渡)。随着溶剂质量的降低和/或聚合度的提高,阈值力的值和链端之间的距离的相应跳变增大。在位置钳位模式下,球状展开是通过球状微相和延伸微相的分子内微相共存,然后突然解开过渡而发生的。在微相分离状态下的反作用力显示出随着延伸的增加“异常”降低。在力和位置夹紧模式下变形曲线的比较表明,在弱延伸和强延伸下,两种模式的曲线重合,在中间延伸范围内观察到差异。对于短小球,另一种展开情况是典型的:在两种扩展模式下,它们通过连续一致地延伸的构型连续展开,而没有跳跃或分子内微相共存。对于两个扩展模式,分隔长链和短链行为的临界链长度N_(cr)的值略有不同:N_(cr,f)

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