Math 2.0

Fluid mechanics Definition

Grashof number

Builds on Dimensionless numbers in fluid mechanicsThermal expansion coefficientViscosityBoussinesq approximation for buoyancy

Definition

Let a surface at temperature TsT_s be in a fluid at temperature T∞T_\infty under gravity of acceleration g>0g > 0. Let the fluid have thermal expansion coefficient β\beta and kinematic viscosity ν>0\nu > 0. Let L>0L > 0 be a characteristic length, such as the height of a vertical plate. The Grashof number is the dimensionless number Gr=g β (Ts−T∞) L3ν2.\mathrm{Gr} = \frac{g \, \beta \, (T_s - T_\infty) \, L^3}{\nu^2}.

Remarks

It arises when the momentum equation with the Boussinesq approximation is made dimensionless. Some authors use ∣Ts−T∞∣\abs{T_s - T_\infty} so that Gr≥0\mathrm{Gr} \ge 0.

Example: air with β≈1/300\beta \approx 1/300 per kelvin and ν≈1.5⋅10−5\nu \approx 1.5 \cdot 10^{-5} square metres per second, at a plate L=0.5L = 0.5 metres high and 3030 kelvin warmer. Then Gr≈9.81⋅0.1⋅0.125/(2.25⋅10−10)≈5.4⋅108\mathrm{Gr} \approx 9.81 \cdot 0.1 \cdot 0.125 / (2.25 \cdot 10^{-10}) \approx 5.4 \cdot 10^8.

Non-example: gβΔTL3/(να)g \beta \Delta T L^3 / (\nu \alpha), with thermal diffusivity α\alpha, is not the Grashof number. It is the Rayleigh number, equal to Gr⋅Pr\mathrm{Gr} \cdot \mathrm{Pr}.

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  1. Boussinesq approximation for buoyancy concept
  2. Dimensionless numbers in fluid mechanics concept
  3. Thermal expansion coefficient concept
  4. Viscosity concept
  5. Grashof number definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Grashof_number
About this page
Tag7YGN4K82VT
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WritingW0 stub
MSC76R10, 80A19
DefinesGrashof number
UsesDimensionless numbers in fluid mechanics, Thermal expansion coefficient, Viscosity, Boussinesq approximation for buoyancy
Changed3 November 2026

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