4.7 Article

The translocation dynamics of the polymer through a conical pore: Non-stuck, weak-stuck, and strong-stuck modes

Journal

JOURNAL OF CHEMICAL PHYSICS
Volume 154, Issue 5, Pages -

Publisher

AIP Publishing
DOI: 10.1063/5.0033689

Keywords

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Funding

  1. National Natural Science Foundation of China [11704333, 12074151]

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This paper investigates the external voltage-driven polymer translocation through a conical pore using Langevin dynamics simulation. The process is divided into an approaching stage and a threading stage. The results show that the apex angle of the pore influences the duration and behavior of the translocation process.
The external voltage-driven polymer translocation through a conical pore (with a large opening at the entry and a small tip at the exit) is studied by using the Langevin dynamics simulation in this paper. The entire translocation process is divided into an approaching stage and a threading stage. First, the approaching stage starts from the polymer entering the large opening and ends up at a terminal monomer reaching the pore tip. In this stage, the polymer will undergo the conformation adjustment to fit the narrowed cross-sectional area of the pore, leading to three approaching modes: the non-stuck mode with a terminal monomer arriving at the pore tip smoothly, the weak-stuck mode for the polymer stuck inside the pore for a short duration with minor conformational adjustments, and the strong-stuck mode with major conformational changes and a long duration. The approaching times (the duration of the approaching stage) of the three approaching modes show different behavior as a function of the pore apex angle. Second, the threading stage describes that the polymer threads through the pore tip with a linear fashion. In this stage, an increase in the apex angle causes the reduction of the threading time (the duration of the threading stage) due to the increase in the driving force with the apex angle at the tip. Moreover, we also find that with the increase in the apex angle or the polymer length, the polymer threading dynamics will change from the quasi-equilibrium state to the non-equilibrium state.

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