To extend the range of applicability of continuum formulations into the con
tinuum-transition regime, an extended set of fluid dynamic equations has be
en derived. These equations, termed as the Bhatnagar-Gross-Krook (BGK)-Burn
ett equations, have been derived by taking moments of the Boltzmann equatio
n by using the BGK model for the collision integral. The second-order distr
ibution function that forms the basis of this derivation is formulated by c
onsidering the first three terms of the Chapman-Enskog expansion. It Is sho
wn that the BGK-Burnett equations have been used to compute the hypersonic
shock structure and the hypersonic flow past a blunt body. The results of t
hese computations are compared with the augmented Burnett and Navier-Stokes
solutions. The second-order distribution function does not violate Boltzma
nn's H-theorem; as a consequence the BGK-Burnett equations are entropy cons
istent for the range of Knudsen numbers for which computations have been pe
rformed.