Reynolds Analogy

The following equation (Equation 6.69) is known as the Reynolds Analogy. It allows other parameters to be found if the velocity is known and vise versa. It consists of dimensionless parameters.

This analogy is further expanded by the Modified Reynolds analogy (Eq. 6.70):

See Section 6.7.3 (page 298) and ME3304 S24 Lecture Note (3) Convection.

The following is from lecture 7A, not sure what it means or if its true