\(\tau\) = \(\gamma\)RS (1)
\(\omega\) = \(\gamma\)QS/w (2)
Fr =
\(V_{mean}\)/ (gR)0.5 (3)
Re =
\(V_{mean}\)R / n (4)
where, \(\tau\) is boundary shear stress expressed in Newton per square meter (N/m2), \(\gamma\) is specific weight of clear water (9800 N/m2), R is hydraulic radius or mean depth of water in m, S is channel slope, \(\omega\) is unit stream power expressed in watts per square meter (W/m2), Q is discharge in m3/s, w is the water surface width in m, Fr is Froude number,
\(V_{mean}\) is mean flow velocity in m/s, g is acceleration due to gravity (9.8 m/s2), Re is Reynolds number, n is kinematic viscosity (1 x 10-7 m2/s for water temperature of 20o C) (Leopold et al., 1964; Petts and Foster, 1985).
Another related measure of erosional power of flows is critical velocity for inception of cavitation (Vc) (equation 5). The critical velocity for inception of cavitation in m/s is given by Baker (1973) and Baker and Costa (1987).
Vc = 2.6 (10+D) 0.5 (5)
where, Vc is the critical velocity for the inception of cavitation in m/s and D is flow depth.
The channel bed of the Par River is dominated by boulders at various locations. Therefore, in order to evaluate the mobility of these coarse sediment theoretically, the sediment-transport equations developed by Williams (1983) were used, and the approximate minimum critical values of bed shear stress (\(\tau\)) (equation 6), unit stream power (\(\omega\)) (equation 7), and mean velocity ( \(V_{mean}\)
) (equation 8) that could initiate cobble and boulder movement were estimated. The equations used in the boulder transport calculations are as follows:
\(\tau\) = 0.17 dg (6)
\(\omega\) = 0.079 dg1.27 (7)
\(V_{mean}\) = 0.065 dg0.5 (8)
where, dg is the intermediate diameter of the grain in mm.