This paper deals with a derivation (using a perturbation technique) of
an approximation, due to Oberbeck(8,9) and Boussinesq,(1) to describe
the thermal response of linearly viscous fluids that are mechanically
incompressible but thermally compressible. The present approach uses
a nondimensionalization suggested by Chandrasekhar(2) and utilizing th
e ratio of two characteristic velocities as a measure of smallness, sy
stematically derives the Oberbeck-Boussinesq approximation as a third-
order perturbation. In the present approach, the material is subjected
to the constraint that the volume change is determined solely by the
temperature change in the body and uses a novel approach in deriving t
he thermodynamical restrictions. Consequently, it is free from the add
itional assumptions usually added on in earlier works in order to obta
in the correct equations.