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Here the picture of gravitational drive [Eq. 2] is used as an example, but the present study covers any kind of driving force acting on the bulk. Due to the invariance of Eq. 2 with respect to (y-y, g-g), the sign of g only changes the direction of motion of the liquid along the channel. Therefore, one can take g0 without loss of generality.
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Here the picture of gravitational drive [Eq. 2] is used as an example, but the present study covers any kind of driving force acting on the bulk. Due to the invariance of Eq. 2 with respect to (y-y, g-g), the sign of g only changes the direction of motion of the liquid along the channel. Therefore, one can take g0 without loss of generality.
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In practice, the velocity profile is affected by the heterogeneous chemical properties of the substrate, in particular via the Navier slip length. This would lead to an explicit dependence of the mobility factor Q on the transverse coordinate x. However, in our study we assume, unless mentioned otherwise, that the no-slip condition is fulfilled on the whole substrate, leading to the simple expression Q= H 3 /3, which depends on x only via H. Some analytical results still hold for general and explicitly x -dependent expressions for Q (x; H (x)).
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In practice, the velocity profile is affected by the heterogeneous chemical properties of the substrate, in particular via the Navier slip length. This would lead to an explicit dependence of the mobility factor Q on the transverse coordinate x. However, in our study we assume, unless mentioned otherwise, that the no-slip condition is fulfilled on the whole substrate, leading to the simple expression Q= H 3 /3, which depends on x only via H. Some analytical results still hold for general and explicitly x -dependent expressions for Q (x; H (x)).
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Meandering perturbations have also been analyzed numerically and have been found to be stable in every situation considered.
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Meandering perturbations have also been analyzed numerically and have been found to be stable in every situation considered.
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