Centrifugal Force

When a fluid film flows across a curved surface, the inertial pressure causes a spreading or gathering of the liquid. The liquid spreads due to the inertial force that is exerted by a concave wall surface. The opposite effect, a gathering of the liquid towards the center, occurs on a convex surface.



Given the surface normals n (as shown in the example above), the normal curvature of the surface S (convex notion in this example) can be expressed as a tensor quantity:

Figure 1. EQUATION_DISPLAY
K=Sn
(2733)

If vf is the velocity of the fluid film phase and v^f its unit vector, the normal curvature of the surface in direction of vf can be denoted:

Figure 2. EQUATION_DISPLAY
Kv^f=v^fTKv^f
(2734)

Therefore, the centrifugal acceleration due to the surface normal curvature in the flow direction is:

Figure 3. EQUATION_DISPLAY
ac=vfTvfKV^fn
(2735)

The resulting force that is added as a source term to the fluid film momentum conservation equation (Eqn. (2722)) becomes:

Figure 4. EQUATION_DISPLAY
fc=mac
(2736)