Determination of Heat Transfer Coefficient for Internal Flow
Laminar Flow
- The heat transfer rate for laminar flow can be calculated using the following equation:
Q = A * h*ΔT
where
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- Q is the heat transfer rate, k is the thermal conductivity of the fluid
- A is the cross-sectional area of the pipe
- ΔT = (Ts – Tref) is the mean temperature difference between the fluid and the pipe wall
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- For laminar flow, the Nusselt number (Nu) can be calculated using the following equation:
Nu = 3.66
- Using the Nusselt number, the average heat transfer coefficient (h) can be calculated as:
h = (Nu * k) / h
where h is the hydraulic diameter of the pipe.
- Once the average heat transfer coefficient (h) is known, the heat transfer rate (Q) can be calculated using the first equation mentioned above.
- The assumption of laminar flow is only valid for low Reynolds numbers (less than 2300).
Turbulent Flow
- The Dittus-Boelter equation is a widely used empirical equation that relates the average heat transfer coefficient for forced convection to the fluid properties, the flow conditions, and the geometric properties of the system.
- The equation for heat transfer coefficients is given by:
h = Nu * k/d
where h is the average heat transfer coefficient, k is the thermal conductivity and D is the hydraulic diameter of the pipe or duct.
- The Reynolds number is defined as:
Re =ρ* V * D/ μ
where, ρ is the fluid density, V is the fluid velocity, D is the hydraulic diameter, and μ is the dynamic viscosity of the fluid.
- The Prandtl number is defined as:
Pr = μ*Cp / k
- where Cp is the specific heat at a constant pressure of the fluid.
The assumption for Equations Dittus -Boelter equation
- The Dittus – Boelter equation is valid for
- Fully developed for thermal and fluid flows
- Turbulent flow in a circular pipe, Reynolds numbers > 2300
- Constant Wall Temperature.
- However, it has been found to give reasonably accurate results for a wide range of geometries and flow conditions.
Calculator For Internal Heat Transfer
Validation with CFD Results
- The heat transfer from the experimntal correlations need to be comparedCFD Results for validation of any internal heat transfer problems as presented in the post.
- Difference up to 20% is acceptable depending on complexicity of case
Heat Transfer Coefficient for Different Geometries
HTC Calculator tab — 6 geometries supported:
- Flat Plate (laminar/mixed correlations)
- Cylinder (Churchill–Bernstein)
- Sphere (Whitaker)
- Pipe – internal flow (Dittus–Boelter / laminar)
- Annulus (hydraulic diameter method)
- Finned Surface (efficiency-weighted)
Both Forced Convection and Natural Convection modes, with automatic regime detection (laminar/turbulent/mixed). Fluid presets for Air, Water, Engine Oil, Ethylene Glycol, and Steam are included.
Unit Converter tab — 15 quantity categories: HTC, heat flux, power, temperature (°C/°F/K/°R), ΔT, thermal conductivity, resistance, diffusivity, length, area, velocity, pressure, viscosity, density, and specific heat — with a live conversion table.
Reference tab — dimensionless numbers with definitions and typical HTC ranges
Heat Transfer Coefficient Table for internal flow
The heat transfer coefficient (h) for internal flow in ducts and pipes depends on factors such as fluid properties, flow type (laminar or turbulent), and pipe geometry. Below is a general table summarizing approximate values for different cases.
Heat Transfer Coefficient (hh) for Internal Flow in Ducts and Pipes
| Flow Type | Fluid Type | Heat Transfer Coefficient, hh (W/m²·K) | Remarks |
|---|---|---|---|
| Laminar Flow (Re<2300Re < 2300) | Air | 5 – 25 | Low heat transfer due to no turbulence |
| Water | 100 – 1000 | Higher heat transfer due to high thermal conductivity | |
| Oil | 50 – 300 | Lower than water due to low thermal conductivity | |
| Turbulent Flow (Re>4000Re > 4000) | Air | 30 – 300 | Strong mixing enhances heat transfer |
| Water | 500 – 10,000 | High heat transfer due to turbulence | |
| Oil | 100 – 1000 | Moderate improvement over laminar flow | |
| Boiling Flow (Two-Phase) | Water (boiling) | 3000 – 100,000 | Phase change greatly enhances heat transfer |
| Condensing Flow (Two-Phase) | Steam | 5000 – 100,000 | Condensation significantly increases hh |
Common Equations for Convective Heat Transfer Coefficient
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Laminar Flow (Constant Wall Temperature)
- Circular Pipe:
- Nu=3.66
- Parallel Plates: Nu=4.86
- Circular Pipe:
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Turbulent Flow (Dittus-Boelter Equation,
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Valid for 0.7<Pr<160
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Re>10,000
- Nu=0.023*Re^0.8*Pr^0.3
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Sieder-Tate Correlation (Includes viscosity effects)