Bed load

Bed load moves by rolling, sliding, and/or saltating (hopping).

This is due in part to attrition and abrasion which results from the stones colliding with each other and against the river channel, thus removing the rough texture (rounding) and reducing the size of the particles.

However, selective transport of sediments also plays a role in relation to downstream fining: smaller-than average particles are more easily entrained than larger-than average particles, since the shear stress required to entrain a grain is linearly proportional to the diameter of the grain.

However, the degree of size selectivity is restricted by the hiding effect described by Parker and Klingeman (1982),[1] wherein larger particles protrude from the bed whereas small particles are shielded and hidden by larger particles, with the result that nearly all grain sizes become entrained at nearly the same shear stress.

[2][3] Experimental observations suggest that a uniform free-surface flow over a cohesion-less plane bed is unable to entrain sediments below a critical value

of the ratio between measures of hydrodynamic (destabilizing) and gravitational (stabilizing) forces acting on sediment particles, the so-called Shields stress

for unit width is proportional to the excess of shear stress with respect to a critical one

is a monotonically increasing nonlinear function of the excess Shields stress

Bed load sediment in the thalweg of Campbell Creek in Alaska .