1. CHAPTER 8 ADDITIONAL SUBJECTS IN FUNDMENTALS OF FLOW Dr. Ercan Kahya

5. Vorticity for the z axis: When vorticity is zero, irrotational flow

6. Case (a): rotational flow Case (b): irrotational flow Although liquid makes a rotary movement, its microelements always face the same direction without performing rotation. In natural vortices such as hurricanes, tornados, eddying water currents has a basic structure with a forced vortex at the center and free vortex at the periphery. Figure shows how the wood chips float

7. Given closed curve s, the integrated vs’ along this same curve is called circulation Γ. Taking counterclockwise rotation positive,

8. Circulation dΓ of elemantary rectangle ABCD (area dA) & the circulation is equal to the product of vorticity by area. Integration gives Stokes theorem: surface integral of vorticity equal to the circulation If there is no vorticity inside a closed curve, then circulation around it is zero.

9. Flow of viscous fluid Mass flow rate at inlet & outlet sections in x- & y-directions

10. Fluid mass stored in the fluid element per unit time (x-dir.) : Fluid mass stored in the fluid element per unit time (y-dir.) : Mass change in unit time (right hand side) : or Continuity Equation Unsteady flow & compressible fluid & for real and ideal fluid

11. For steady flow and incompressible fluid: For steady flow and incompressible fluid for axially symetric flow using cylindrical coordinates:

12. For axially symetric flow using cylindrical coordinates:

13. The strict solutions obtained for N-S equations to date are only for some special flows. Two such examples are: Flow of a viscous fluid between two parallel plates

14. A flow in a long circular pipe is a parallel flow of axial symmetry. In this case, it is convenient to use the Navier-Stokes equation using cylindrical coordinates Under the same conditions as in the previous section, N-S equation simplifies to