Dimensionless Numbers
- Burger Number
- Definition: , where is the nonrotational baroclinic phase speed, is the inertial frequency under the f-plane approximation, and is the radius of the basin.
- Interpretation: The ratio of stratification to rotation for a circular lake.
- Analysis: Small Burger numbers correspond to shallower water, wider lakes, or rotation dominated dynamics. Large Burger numbers correspond to deeper water, narrower lakes, or stratification dominated dynamics.
- Froude Number
- Definition: , where is the gravitational acceleration, and and are the characteristic velocity and length scales.
- Interpretation: The square root of the ratio of inertia force to gravity force.
- Analysis: The Froude number describes different regimes of open channel flow, including hydraulic jumps. describes critical flow; describes supercritical flow; describes subcritical flow. The Froude number is analogous to the Mach number in compressible flow.
- Grashof Number
- Definition: , where is the gravitational acceleration, is the volumetric thermal expansion coefficient, is the temperature differrence, is the volume, and is the kinematic viscosity.
- Interpretation: The ratio of buoyant forces to viscous forces.
- Analysis: When , the viscous force is negligible compared to the buoyancy and inertial forces, and the flow starts a transition to the turbulent regime.
- Mach Number
- Definition: , where is the characteristic velocity scale, and is the speed of sound.
- Interpretation: The ratio of inertia force to compressibility force.
- Analysis: Compressibility effects can be neglected if .
- Prandtl Number
- Definition: , where is the viscosity, and is the thermal diffusivity.
- Interpretation: The ratio of momentum diffusivity (i.e. kinematic viscosity) to heat diffusivity.
- Analysis: The typical Prandtl number for water is around 7 for water (At 20 degrees Celsius). See also Schmidt number.
- Reynolds Number
- Definition: , where and are the characteristic velocity and length scales, and is the kinematic viscosity.
- Interpretation: The ratio of inertia force to viscous force.
- Analysis: Small Reynolds numbers are often associated with viscous flows, whereas large Reynolds numbers are typically found in turbulent flows.
- Richardson Number (flux)
- Definition: , where the overlines denote the ensemble averages of variables.
- Interpretation: The ratio of the buoyant destruction of turbulent kinetic energy to the shear production.
- Analysis: The flux Richardson number is related to the gradient Richardson number by , where the ratio is the turbulent Prandtl number.
- Richardson Number (gradient)
- Definition: , where is the buoyancy frequency, and is the background horizontal velocity.
- Interpretation: The ratio between the strength of stratification and velocity shear.
- Analysis: The gradient Richardson number is used for determining the linear stability of an inviscid stratified flow. A sufficient condition for the flow to be linearly stable is that the local Richardson number exceed 0.25 throughout the flow. However, does not mean the flow is necessarily unstable (the criterion is not sufficient). When the flow is not a parallel shear flow, the meaning of is not clear.
- Rossby Number
- Definition: , where is the characteristic velocity, and is the Coriolis frequency, and is the characteristic length scale.
- Interpretation: The ratio of the advective forces to the Coriolis pseudo-forces.
- Analysis: When , Coriolis effects dominate and the system approaches geostrophic balance.
- Schmidt Number
- Definition: , where is the viscosity, and is the mass diffusivity.
- Interpretation: The ratio of momentum diffusivity (i.e. kinematic viscosity) to mass diffusivity.
- Analysis: The typical Schmidt number for water is around 500, depending on the temperature and salinity. For direct numerical simulations, is commonly used in the literature. See also Prandtl number.