P. Hamm, A GENERALIZED FORM OF THE SAINT-VENANT EQ UATION WITH VELOCITY AND SHEAR-STRESS PROFILES, Journal of Hydraulic Research, 34(4), 1996, pp. 481-501
The Saint-Venant equations for unsteady, non uniform open-channel flow
are obtained by partial integration of the Prandtl equations for newt
onian or non newtonian fluids. The equations are integrated with self-
similar solutions near steady, uniform flow and are extended to turbul
ent mean flow. For weakly unsteady, non uniform flow, a closed-form so
lution is given for a) the Saint-Venant kinetic energy integral with a
dissipation coefficient depending only on the Reynolds number and the
roughness, b) the friction coefficient varying in space and time and
c) velocity and shear stress profiles varying in space and time.