Abstract

We simulate a tug-of-war (TOW) scenario for a model double-stranded DNA threading through a double nanopore (DNP) system. The DNA, simultaneously captured at both pores is subject to two equal and opposite forces −f⃗L=f⃗R-\vec{f}_L= \vec{f}_R (TOW), where f⃗L\vec{f}_L and f⃗R\vec{f}_R are the forces applied to the left and the right pore respectively. Even though the net force on the DNA polymer Δf⃗LR=f⃗L+f⃗R=0Δ\vec{f}_{LR}=\vec{f}_L+ \vec{f}_R=0, the mean first passage time (MFPT) ⟨τ⟩\langle τ\rangle depends on the magnitude of the TOW forces ∣fL∣=∣fR∣=fLR \left | f_L \right | = \left |f_R \right | = f_{LR}. We qualitatively explain this dependence of ⟨τ⟩\langle τ\rangle on fLRf_{LR} from the known results for the single-pore translocation of a triblock copolymer. We demonstrate that the time of flight (TOF) of a monomer with index mm (⟨τLR(m)⟩\langle τ_{LR}(m) \rangle) from one pore to the other exhibits quasi-periodic structure commensurate with the distance between the pores dLRd_{LR}. Finally, we study the case Δf⃗LR=f⃗L+f⃗R≠0Δ\vec{f}_{LR}=\vec{f}_L+ \vec{f}_R \ne 0, and qualitatively reproduce the experimental result of the dependence of the MFPT on Δf⃗LRΔ\vec{f}_{LR}. For a moderate bias, the MFPT for the DNP system for a chain length NN follows the same scaling ansatz as that of for the single nanopore, ⟨τ⟩=(AN1+ν+ηporeN)(ΔfLR)−1\langle τ\rangle = \left( AN^{1+ν} + η_{pore}N \right) \left(Δf_{LR}\right)^{-1}, where ηporeη_{pore} is the pore friction, which enables us to estimate ⟨τ⟩\langle τ\rangle for a long chain. Our Brownian dynamics simulation studies provide fundamental insights and valuable information about the details of the translocation speed obtained from ⟨τLR(m)⟩\langle τ_{LR}(m) \rangle, and accuracy of the translation of the data obtained in the time-domain to units of genomic distances.

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