Karman Vortex Trail
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Karman Vortex Trail
• When the Reynolds number exceeds to about 30, the two vortices are formed at the points of separation.
• They rotate in opposite direction and elongate to such extent that they become unstable and are broken off form the body.
• This process of formation of the vortices and their shedding away from the cylinder continues.
• There are two rows of vortices formed moving downstream direction with very small velocity, these trails f vortices are commonly known as Karman vortex trails or street.
• The absolute velocity of the vortices is equal to (V – Vv), then the parameter (U-Uv/ L), represents the frequency of shedding ‘f’.
• The frequency ‘f’ with which vortices are shed form the cylinder is given by empirical formula.
f = 0.198 U/D [1-19.7/Re]
f D/U = 0.198 ( 1- 19.7/Re)
• The parameter fD /U is known as strouhal number which is the function of Reynol’s number
Where, U = Free stream velocity
D = Diameter of cylinder
Uv = Velocity of vortices formed
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• They rotate in opposite direction and elongate to such extent that they become unstable and are broken off form the body.
• This process of formation of the vortices and their shedding away from the cylinder continues.
• There are two rows of vortices formed moving downstream direction with very small velocity, these trails f vortices are commonly known as Karman vortex trails or street.
• The absolute velocity of the vortices is equal to (V – Vv), then the parameter (U-Uv/ L), represents the frequency of shedding ‘f’.
• The frequency ‘f’ with which vortices are shed form the cylinder is given by empirical formula.
f = 0.198 U/D [1-19.7/Re]
f D/U = 0.198 ( 1- 19.7/Re)
• The parameter fD /U is known as strouhal number which is the function of Reynol’s number
Where, U = Free stream velocity
D = Diameter of cylinder
Uv = Velocity of vortices formed
For more help in Karman Vortex Trail click the button below to submit your homework assignment