Hedstrom Number formula |
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\( He \;=\; \dfrac{ \left(\rho \cdot d^2\right) \cdot \tau }{ \mu^2 } \) | ||
Symbol | English | Metric |
\( He \) = Hedstrom Number | \(dimensionless\) | \(dimensionless\) |
\( \rho \) (Greek symbol rho) = Fluid Mass Density | \(lbm\;/\;ft^3\) | \(kg\;/\;m^3\) |
\( d \) = Pipe Inside Diameter | \(in^2\) | \(mm^2\) |
\( \tau \) (Greek symbol tau) = Pipe Yield Point | \(in\) | \(mm\) |
\( \mu \) (Greek symbol mu) = Fluid Dynamic Viscosity | \(lbf-sec\;/\;ft^2\) | \( Pa-s \) |
Hedstrom number, abbreviated as He, a dimensionless number, is used in fluid dynamics to characterize the relative importance of viscous forces to inertial forces in a fluid flow. The Hedström number helps determine whether viscous effects or inertial effects dominate in a fluid flow. Its interpretation is similar to the Reynolds number, which is another dimensionless parameter used in fluid dynamics. The key differences between the Hedström number and the Reynolds number are the choice of characteristic velocity and the absence of density in the Hedström number.
Hedstrom Number Interpretation
It’s often used alongside the Reynolds Number (which compares inertia to viscosity) to fully describe non-Newtonian flow regimes. For Bingham fluids, the Hedstrom Number helps engineers design pumps, pipelines, or mixers by predicting how much force is needed to initiate and sustain flow.