Roshko Number formula |
||
\( Ro \;=\; St \cdot Re \;=\; \dfrac{ f \cdot l_c^2 }{ \nu }\) (Roshko Number) \( f \;=\; \dfrac{ Ro \cdot \nu }{ l_c^2 }\) \( l_c \;=\; \sqrt{ \dfrac{ Ro \cdot \nu }{ f } }\) \( \nu \;=\; \dfrac{ f \cdot l_c^2 }{ Ro }\) |
||
Symbol | English | Metric |
\( Ro \) = Roshko Number | \(dimensionless\) | \(dimensionless\) |
\( St \) = Strouhal Number | \(dimensionless\) | \(dimensionless\) |
\( Re \) = Reynolds Number | \(dimensionless\) | \(dimensionless\) |
\( f \) = Vortex Shedding Frequency | \(dimensionless\) | \(dimensionless\) |
\( l_c \) = Characteristic Length | \(in\) | \(mm\) |
\( \nu \) (Greek symbol nu) = Kinematic Viscosity | \(ft^2\;/\;sec\) | \(m^2\;/\;s\) |
Roshko number, abbreviated as Ro, a dimensionless number, is used in fluid mechanics that describes oscillating flow mechanisms, particularly in the context of vortex shedding. It’s named after Anatol Roshko, an aeronautics professor who studied turbulent wakes and vortex streets. The Roshko number is essentially a way to relate the frequency of oscillations in a flow to the fluid’s properties and the geometry of the system.