Question 8.1: Is the following velocity field a possible incompressible fl...

Is the following velocity field a possible incompressible flow? \nu (x,y,z,t)=\frac{\rho g\sin \theta }{\mu }\left(yh-\frac{y^{2}}{2} \right)\hat{i} where ρ is the mass density of the fluid, g (=9.81 m/s^{2}) is the gravitational constant, \mu is the viscosity of the fluid, \theta is some fixed angle (number) relative to a horizontal datum, and h is some depth of a fluid film.

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\triangledown \cdot \nu =\frac{\partial}{\partial x} \left[\frac{\rho g\sin \theta }{\mu }\left(yh-\frac{y^{2}}{2} \right) \right]+\frac{\partial}{\partial y}(0)+\frac{\partial}{\partial z}(0)=0;

so yes, this is a possible incompressible flow field. This velocity field will be determined formally in Example 9.3 via the solution of the equation of motion for a particular boundary value problem.

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