“…Here P in , P out are some given pressures and 0 < x 2 < R 0 (x 1 ) + η(x 1 , t) with x 1 = 0, L. On the bottom boundary Γ c the flow symmetry is considered, v 2 (x 1 , 0, t) = 0 , µ ∂v 1 ∂x 2 (x 1 , 0, t) = 0, 0 < x 1 < L, 0 < t < T. (6) We equip equation (2) with the following clamped boundary conditions, η(0, t) = η(L, t) = 0, η x 1 (0, t) = η x 1 (L, t) = 0.…”