Formula and Method for the Prandtl Number
The Prandtl number (Pr) is a dimensionless quantity that compares a fluid's ability to diffuse momentum (through viscosity) to its ability to diffuse heat (through thermal conduction). It is defined as Pr = cp·μ / k, where cp is specific heat capacity, μ is dynamic viscosity, and k is thermal conductivity. Equivalently, Pr = ν/α, the ratio of kinematic viscosity ν = μ/ρ to thermal diffusivity α = k/(ρ·cp). This calculator computes Pr along with ν and α from your fluid's properties.
How the calculation works
Enter the fluid's dynamic viscosity (in centipoise or pascal-seconds), specific heat capacity, thermal conductivity, and density. The calculator first converts viscosity to SI units (Pa·s) if you entered centipoise, then multiplies specific heat capacity by dynamic viscosity and divides by thermal conductivity to get Pr = cp·μ/k. It also computes kinematic viscosity (ν = μ/ρ) and thermal diffusivity (α = k/(ρ·cp)) so you can confirm Pr = ν/α independently.
Common mistakes
- Confusing dynamic and kinematic viscosity: dynamic viscosity μ (Pa·s) and kinematic viscosity ν (m²/s) differ by a factor of density — mixing them up throws Pr off by orders of magnitude.
- Using molar heat capacity: Pr requires specific (per-mass) heat capacity in J/(kg·K), not molar heat capacity in J/(mol·K).
- Ignoring temperature dependence: Pr changes significantly with temperature for most fluids, especially liquids — use property values at the actual operating temperature rather than a generic table value.
Real-world applications
- Convective heat transfer correlations, such as Nu = 0.023·Re^0.8·Pr^n for turbulent pipe flow, use Pr to relate fluid friction and heat transfer.
- In boundary layer theory, Pr indicates whether the thermal boundary layer is thicker or thinner than the velocity boundary layer — low-Pr liquid metals have thick thermal boundary layers relative to velocity, while high-Pr oils have the opposite.
- Heat exchanger and cooling system design uses Pr to choose correlations appropriate for the working fluid, whether air, water, oil, or a liquid-metal coolant.