Convection coefficients for twenty common situations in air, water, oil and steam — natural convection, forced convection, boiling and condensation, in both unit systems.
Data verified 2026-09-29 · based on compilations as published 2024–2026
| Situation[2] | Fluid[2] | h min W/m²·K[2] | h max W/m²·K[2] | h min BTU/h·ft²·°F[1] | h max BTU/h·ft²·°F[1] |
|---|---|---|---|---|---|
| Natural convection — vertical plate # | Air | 3 | 25 | 0.5283 | 4.403 |
| Natural convection — horizontal plate, facing up # | Air | 5 | 25 | 0.8805 | 4.403 |
| Natural convection — horizontal plate, facing down # | Air | 2 | 10 | 0.3522 | 1.761 |
| Natural convection — cylinder # | Air | 3 | 25 | 0.5283 | 4.403 |
| Natural convection — enclosed cavity # | Air | 2 | 8 | 0.3522 | 1.409 |
| Natural convection # | Water | 20 | 100 | 3.522 | 17.61 |
| Natural convection # | Oil | 10 | 50 | 1.761 | 8.805 |
| Forced convection — low-speed duct flow # | Air | 10 | 100 | 1.761 | 17.61 |
| Forced convection — across a cylinder # | Air | 20 | 300 | 3.522 | 52.83 |
| Forced convection — high-speed flow # | Air | 100 | 500 | 17.61 | 88.05 |
| Forced convection — tube bank # | Air | 30 | 300 | 5.283 | 52.83 |
| Forced convection — turbulent tube flow # | Water | 1500 | 15000 | 264.2 | 2642 |
| Forced convection — cross flow # | Water | 500 | 10000 | 88.05 | 1761 |
| Forced convection — laminar tube flow # | Oil | 50 | 500 | 8.805 | 88.05 |
| Forced convection — turbulent tube flow # | Oil | 500 | 1500 | 88.05 | 264.2 |
| Forced convection # | Liquid metal | 5000 | 50000 | 880.5 | 8806 |
| Boiling — pool boiling # | Water | 3000 | 100000 | 528.3 | 1.761e+04 |
| Boiling — forced convection boiling # | Water | 10000 | 100000 | 1761 | 1.761e+04 |
| Condensation — film condensation # | Steam | 5000 | 100000 | 880.5 | 1.761e+04 |
| Condensation — dropwise # | Steam | 30000 | 100000 | 5283 | 1.761e+04 |
Ranges are order-of-magnitude engineering guidance, not a substitute for a correlation. A convection coefficient is not a material property — it is a function of the flow field, and the same fluid can span the whole range depending on whether the flow is laminar or turbulent, the characteristic length, and the geometry. Forced convection up to about 500 W/m²·K in air and 15 000 in water is where most air and water heat exchangers operate. Boiling and condensation are not convection in the usual sense — they transfer latent heat and reach coefficients one to two orders of magnitude above single-phase flow, which is why heat pipes and steam systems move so much heat in a small area.
Unlike thermal conductivity, which belongs to the material and can be looked up once, a convection coefficient belongs to the flow situation. The same water in the same pipe can have an h of 200 or 15 000 depending only on whether the flow is laminar or turbulent.
The physical reason is that convection is conduction across a thin stagnant film at the surface, and the only thing that varies is how thin that film is. In laminar flow the film is thick and h is low; turbulence scours the film down to almost nothing and h rises by an order of magnitude. This is why a pump or fan buys far more heat transfer than a bigger surface does: doubling the velocity may double or triple h, while doubling the surface only doubles the area.
The coefficient is usually obtained from a correlation of the form Nu = C·Re^m·Pr^n, where the Nusselt number contains h, the Reynolds number contains velocity and geometry, and the Prandtl number contains the fluid's properties. That is why the entry you need is not "water" but "water in turbulent tube flow" — the geometry matters as much as the fluid.
The reason to look up a convection coefficient is almost always to find out which thermal resistance in a chain is the limiting one, because that is the only one worth improving.
R = 1/h for a convective surface, and t/k for a conduction path. Take a forced-air heat sink: h = 50 W/m²·K on the air side gives R = 0.02 m²·K/W. A 5 mm aluminium fin base at k = 200 gives R = 0.000025 — three orders of magnitude smaller. Essentially all the resistance is on the air side, which is why heat sink design is entirely about getting air across more surface, and why adding metal does nothing.
Now take the same sink with water at h = 5000: R = 0.0002, which is still the dominant resistance but now only eight times the conduction term. This is the crossover that makes liquid cooling so much more effective — a twentyfold drop in the air-side resistance means either a hundredfold smaller sink for the same performance, or a much cooler device.
The same reasoning drives the design of boilers and condensers. Because boiling and condensing coefficients reach 100 000, the phase-change side contributes almost no resistance — which is why the tube wall and the other fluid set the size of the equipment, and why boiling surfaces are designed for bubble nucleation rather than for extra area.
Each data column on this page is tied to the source it came from. The numbers in square brackets correspond to the table headers above.
| # | Source | Type | Revision / method |
|---|---|---|---|
| [1] | Value computed from the standard's defining relationship | derived | Computed at build time from the defining formula stated on the page, then verified against every row and anchored by known standard values. Nothing in these columns was transcribed from a printed table. |
| [2] | Published heat-transfer correlations for convection coefficients | standard | compilations as published 2024–2026 |
| Standard | Revision | What it covers on this page |
|---|---|---|
| Published convection correlations and handbook ranges | compilations as published 2024–2026 | the coefficient ranges for each situation |
| NIST Chemistry WebBook — fluid transport properties | NIST Standard Reference Database 69, 2023 release | the fluid property basis behind the correlations |
| ASHRAE Handbook — Fundamentals, heat transfer chapter | ASHRAE Handbook, 2021 Fundamentals volume | the building-services convection values |
Cross-checked against:
Derived values — the following values on this page are calculated, not taken directly from the standard:
| Value | How it is derived |
|---|---|
| Coefficients in BTU/h·ft²·°F | W/m²·K × 0.176110, the exact conversion. Recomputed at build time for every row, with one value held as a known-value check. |
Ranges are engineering guidance for order-of-magnitude work. A convection coefficient is a property of the flow situation, not of the fluid, and the same fluid spans the entire range depending on velocity, geometry and whether the flow is laminar or turbulent. For design work, use a correlation for the specific geometry or a measured value from similar equipment.
Every value on this page is traceable to the sources listed above. If you use the data in a document, paper or report, cite it as:
Each row in the tables above also has a permanent link — hover a row and use the # link to cite a single value rather than the whole page.
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