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Hele-Shaw flow : ウィキペディア英語版
Hele-Shaw flow
Hele-Shaw flow (named after Henry Selby Hele-Shaw) is defined as Stokes flow between two parallel flat plates separated by an infinitesimally small gap. Various problems in fluid mechanics can be approximated to Hele-Shaw flows and thus the research of these flows is of importance. Approximation to Hele-Shaw flow is specifically important to micro-flows. This is due to manufacturing techniques, which creates shallow planar configurations, and the typically low Reynolds numbers of micro-flows.
The governing equation of Hele-Shaw flows is identical to that of the inviscid potential flow and to the flow of fluid through a porous medium (Darcy's law). It thus permits visualization of this kind of flow in two dimensions.
==Mathematical formulation of Hele-Shaw flows==

Let x, y be the directions parallel to the flat plates, and z the perpendicular direction, with 2H being the gap between the plates (at z=\pm H).
When the gap between plates is asymptotically small
: H \rightarrow 0, \,
the velocity profile in the z direction is parabolic (i.e. is a quadratic function of the coordinate in this direction). The equation relating the pressure gradient to the velocity is,
: = p \frac \,
where is the velocity , p(x,y,t) is the local pressure, \mu is the fluid viscosity.
This relation and the uniformity of the pressure in the narrow direction z permits us to integrate the velocity with regard to z and thus to consider an effective velocity field in only the two dimensions x and y. When substituting this equation into the continuity equation and integrating over z we obtain the governing equation of Hele-Shaw flows,
: \frac+\frac=0.
This equation is supplemented by the no-penetration boundary conditions on the side walls of the geometry,
: p \cdot \hat n= 0 \,
where \hat n is a unit vector perpendicular to the side wall.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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