Classical thermodynamics, heat transfer Convective heat transfer Fact
Chilton–Colburn J-factor analogy
Statement
Consider forced flow with free-stream or mean speed along a surface, with no form drag, so that the drag is skin friction only. Let be the skin friction coefficient, the Stanton number and the Prandtl number. Let be the mass transfer Stanton number, with mass transfer coefficient . Let be the Schmidt number, with kinematic viscosity and diffusivity . The Colburn factors are and . For and , the following hold approximately:
Remarks
This is an empirical correlation, not a theorem. For the laminar flat plate it agrees with the Blasius and Pohlhausen results, which give . For it reduces to the Reynolds analogy . For turbulent flow in smooth pipes it holds roughly, which makes friction data a cheap source of heat and mass transfer estimates. On bluff bodies the measured drag includes pressure drag, and the analogy with the total drag coefficient fails.
Going deeper
For a student
The exponent comes from the laminar flat-plate result , since . The analogy extends the Reynolds analogy from to common liquids and gases. Replacing by turns every heat transfer correlation of this form into a mass transfer correlation.
Reading path
To understand this page from the ground up, read these 7 pages in order. The foundations come first.
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- no evidence level
- Heat transfer coefficient concept
- Prandtl number concept
- Reynolds number concept
- Stanton number concept
- Thermal boundary layer concept
- Reynolds analogy statement
- Chilton–Colburn J-factor analogy statement
Further reading
About this page
| Tag | FHSZN0S58C |
|---|---|
| URI | m2://FHSZN0S58C |
| Kind | statement, fact |
| Writing | W0 stub |
| MSC | 80A19, 76R05, 76R50 |
| Status | This copy of the site has no build data. Run m2 status FHSZN0S58C. |
| About | Forced convection |
| Uses | Stanton number, Prandtl number, Reynolds analogy |
| Same as | |
| Changed | 3 November 2026 |
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