Page 251 - Handbook of Gold Exploration and Evaluation
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222    Handbook of gold exploration and evaluation

              Channel velocities vary throughout the water body due to the interrelationship of
              such factors as the presence of a free stream surface, sediment loadings, channel
              geometry, and friction along the channel bed and walls. The maximum velocity
              appears to occur below the free surface at a distance of about 0.05 to 0.50 of its
              depth, the closer the banks the deeper the maximum (Chow, 1959).


              Velocity distribution
              The actual velocity distribution depends in each case upon the configuration of
              the channel bed and the shape of the channel upstream of the velocity measure-
              ment site. Examples of the effects of changing sectional shape upon the
              distribution of velocity are given in Fig. 4.16. This figure shows a series of
              velocity curves constructed from measurements of velocity taken at various
              stages of flow and discharges in Behana Creek, at Aloomba, North Queensland,
              Australia.
                 An infinite variety of flow rates and sediment loadings impose constantly
              changing physical constraints on streams flowing through locally different
              geological structures. Progressive increases in discharge and decreases in the
              size of particles in transport are normal responses to downstream changes in
              width, depth and roughness. Shape differences depend largely upon the extent to
              which flow is retarded by frictional resistance along its boundaries. Roughness
              has a marked affect on energy losses due to friction. If the sediments are fine
              grained and the banks are more resistant to erosion than the bed, the cross-
              section will be narrow and deep. If the sediments are coarse, armouring of the
              bed will protect it against erosion and the stream section will tend towards
              lateral expansion and shoaling.


              Grading concept
              Theoretically, if flow conditions remain unchanged through time to a final state
              of equilibrium the longitudinal profile will achieve a smooth concave upward
              curve. In practice, grading is a complicated process and many factors intervene
              to prevent this happening and compromises are sought. In 1948, Machin defined
              a graded stream as one in which, over a period of years; channel form and slope
              are delicately adjusted to provide with available discharge, just the velocity
              required to transport the incoming load. He classified the Shoshone River,
              Wyoming with an average gradient of 10 m/km as graded, the Illinois River with
              a gradient of less than 1 m/km, ungraded. The distinction was made on the basis
              of differences in the nature of the materials in transport. The Shoshone River
              must handle material up to 25 mm to 250 mm diameter; bed-load in the Illinois
              River is mainly silt and clay.
                 Modern views of grading hold that any stream may be called graded if, by
              adjusting its geometry to achieve an average state of operation, it achieves a
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