(1.) In the case of flow over a Disk , both friction drag and
pressure drag contribute to total drag . The drag coefficient for
flow over a smooth disk is a function of Reynolds number .
At the front portion of the disk Reynolds number is low ; hence
there is no flow separation from a disk , the wake is laminar and
the drag is predominantly friction drag . Stokes has shown
analytically , for very low Reynolds number flows where inertia
forces may be neglected , The drag coefficient Cd is defined as
;
Cd = 24/Re
As the Reynolds number is further increased due to flow convergence
on the disk , the drag coefficient DECREASES continuously up to a
Reynolds number of about 1000 .
(2.) After this a turbulent wake develops and grows at the top of the disk ; this wake is at a relatively low pressure, leading to a large pressure drag . By the time Renold number is very high approximately equal to 1000 - 10000 due to very small converging passage at the top of the disk , about 95% of total drag is due to the pressure , Due to this Drag coefficient INCREASES suddenly .
(3.) And after the transition phase , the boundary layer at the back of the disk start separating and the size of the wake decreases at the back portion of the disk . Due to this net pressure force on the disk is reduced and the drag coefficient DECREASES abruptly.
KT 2:49 g LTE 91 % a & O Expert Q&A 618 EXTERNAL FLOW DRAG AND LIFT circ Disk dra 2.0- nun 1,5- mo The c...