The Stanton number, St, is a dimensionless number that measures the ratio of heat transferred into a fluid to the thermal capacity of fluid. The Stanton number is named after Thomas Stanton (engineer) (1865–1931). It is used to characterize heat transfer in forced convection flows.
St=
h | |
Gcp |
=
h | |
\rhoucp |
where
It can also be represented in terms of the fluid's Nusselt, Reynolds, and Prandtl numbers:
St=
Nu | |
RePr |
where
The Stanton number arises in the consideration of the geometric similarity of the momentum boundary layer and the thermal boundary layer, where it can be used to express a relationship between the shear force at the wall (due to viscous drag) and the total heat transfer at the wall (due to thermal diffusivity).
Using the heat-mass transfer analogy, a mass transfer St equivalent can be found using the Sherwood number and Schmidt number in place of the Nusselt number and Prandtl number, respectively.
Stm=
| ||
|
Stm=
hm | |
\rhou |
where
Stm
ShL
ReL
Sc
hm
u
The Stanton number is a useful measure of the rate of change of the thermal energy deficit (or excess) in the boundary layer due to heat transfer from a planar surface. If the enthalpy thickness is defined as:
\Delta2=
infty | |
\int | |
0 |
\rhou | |
\rhoinftyuinfty |
T-Tinfty | |
Ts-Tinfty |
dy
Then the Stanton number is equivalent to
St=
d\Delta2 | |
dx |
for boundary layer flow over a flat plate with a constant surface temperature and properties.
Using the Reynolds-Colburn analogy for turbulent flow with a thermal log and viscous sub layer model, the following correlation for turbulent heat transfer for is applicable
St=
Cf/2 | |
1+12.8\left(Pr0.68-1\right)\sqrt{Cf/2 |
where
Cf=
0.455 | |
\left[ln\left(0.06Rex\right)\right]2 |
Strouhal number, an unrelated number that is also often denoted as
St