“…We consider no-flux boundary conditions at the edges, i.e., ∂ x c(l ± ) = 0. Following earlier work along these lines [13,16], we non-dimensionalize length by L 0 , time by L 2 0 /D, stress by k, and concentration by c 0 = c dx/L 0 . We then map the problem on the interval [0, 1] using u = (x − l − )/L and get three dimensionless model parameters: the hydrodynamic damping length L = η/(ξL 2 0 ) arising from the competition between viscous and frictional dissipation; the Péclet number Pe = k/ξD describing the importance of advection versus diffusion; and myosin contractility P = χc 0 /k.…”