In a sufficiently uniform flow the Stokes force is F=γv toward trap 2. Its work over separation d lowers the second effective well by Fd. Equal effective free energies require γvd=kBTlog2. Henceat 298 K. The temperature was not specified, so the numerical result scales as T/298 K. This approximation treats a weak uniform drag as a constant tilt and neglects changes in barrier shape and hydrodynamic interactions with boundaries.
v=6πηadkBTlog2≃3.0×10−7 ms−1
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