The Richardson number, a dimensionless parameter in the theory of turbulence is named after him.

Furthermore, and most importantly, it provides a method for computing these dimensionless parameters from the given variables.

Any number of new dimensionless parameters can be calculated through exponents and multiplication.

Alternatively, the dimensionless parameters via direct manipulation of the underlying differential equations.

The values of the dimensionless parameters are held to be the same for both the scale model and application.

In situations where either dimensionless parameter is large, then general relativity must be used to describe the system.

Here the c are dimensionless adjustable parameters of the theory.

In addition to the Reynolds number, there are at least two other relevant dimensionless parameters.

It is a very important dimensionless parameter in analyzing natural or free convection.

It is a dimensionless parameter that is useful in analyzing a Stefan problem.