Page 238 - Handbook of Gold Exploration and Evaluation
P. 238

Sedimentation and detrital gold  209

                   P W ˆ 
hA=A ˆ 
h                                       4.8

            The weight of the water column is 
hA, where 
 is the weight density of the
            water. At sea level with air as the fluid, P becomes P A the atmospheric pressure
            of an element of matter at sea level. The total pressure at the plane is then:

                   P ˆ P W ‡ P A ˆ 
h ‡ P A                               4.9
            Pressure is one component of potential energy and as already noted a gradient of
            gravitational potential energy is needed between two points for flow to take
            place. The direction of the movement is in the direction of the lowest pressure.
            The rate of motion is proportional to the spatial rate of change (gradient) of
            potential energy between the two points.


            Mechanical potential energy
            As applied to natural flow conditions, an element of water moving from rest in
            the headwaters of a stream contains mostly potential energy, i.e., the product of
            its density  , acceleration due to gravity g and its elevation above sea level z. At
            any point downstream, losses of potential energy with decreasing z are
            compensated for by gains in kinetic energy. Some of this energy is expended in
            eddying, turbulence and changes in momentum, particularly at the foot of rapids
            and waterfalls. A further interchange of energy takes place when the stream
            changes direction. Flowing around a bend, the velocity increases on the outside
            and is retarded along the inside of the bend. Elements of water in a horizontal
            line across the bend thus have equal quantities of potential energy and total
            energy but different quantities of kinetic energy and pressure energy. At sea
            level, any remaining energy is dissipated in turbulence and intermolecular
            friction.



            4.2.4 Forces acting on fluids

            Forces acting on fluids and on solids and fluids in relative motion react differ-
            ently according to differences in the physical characteristics of the solids and the
            relative magnitude and direction of hydraulic forces, which act both to induce
            and resist movement thereby determining the nature of the flow. The net rate of
            entrainment, transport and deposition of bed-load materials depend upon the
            degree of balance between the individual phases of such exchange. The forces
            involved in the reactions are termed either `body' forces or `surface' forces.


            Body forces
            Body forces act from a distance upon the whole bulk of a fluid element or solid
            immersed in a fluid. Typical body forces comprise:
   233   234   235   236   237   238   239   240   241   242   243