Graetz number

In fluid dynamics, the Graetz number, \mathrm{Gz} is a dimensionless number that characterises laminar flow in a conduit. The number is defined as:[1]

\mathrm{Gz}={D_H \over L} \mathrm{Re} \mathrm{Pr}

where

D_H is the diameter in round tubes or hydraulic diameter in arbitrary cross-section ducts
L is the length
\mathrm{Re} is the Reynolds number and
\mathrm{Pr} is the Prandtl number.

This number is useful in determining the thermally developing flow entrance length in ducts. A Graetz number of approximately 1000 or less is the point at which flow would be considered thermally fully developed.[2]

When used in connection with mass transfer the Prandtl number is replaced by the Schmidt number \mathrm{Sc} which expresses the ratio of the momentum diffusivity to the mass diffusivity.

\mathrm{Gz}={D_H \over L} \mathrm{Re} \mathrm{Sc}

The quantity is named after the physicist Leo Graetz.

References

  1. ^ Nellis, G., and Klein, S. (2009) "Heat Transfer" (Cambridge), page 663.
  2. ^ Shah, R. K., and Sekulic, D. P. (2003) "Fundamentals of Heat Exchanger Design" (John Wiley and Sons), page 503.