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Governing Equations for Axial Velocity

The first step in developing the numerical method is to find a formal solution to Equation 8.40. Observe that Equation 8.40 is variable separable. [Pg.302]

This equation can be integrated twice. Note that dP/dz is a constant when integrating with respect to r. The constants of integration are found using the boundary conditions. [Pg.302]

Equation 8.41 allows the shape of the velocity profile to be calculated (e.g., substitute fi = constant and see what happens), but the magnitude of the velocity depends on the yet unknown value for dP/dz. As is often the case in hydrodynamic calculations, pressure drops are determined through the use of a continuity equation. Here, the continuity equation takes the form of a constant mass flow rate down the tube  [Pg.303]

This is the local pressure gradient. It is assumed to vary slowly in the z direction. The pressure at position z is [Pg.303]


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