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Title
Generalized Computer Program Fluvial-12 Mathematical Model for Erodible Channels Users Manual
Date
8/1/1986
Prepared By
Howard H. Chang, Ph.D., P.E.
Floodplain - Doc Type
Educational/Technical/Reference Information
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<br />Eq. 8 relates the direction of bed load movement to the direction of <br />near-bed velocity and transverse bed slope azjar. As transverse velocity <br />starts to move sediment away from the concave baok, it creates a trans- <br />verse bed slope that counters the transverse sediment movement. An <br />equilibrium is reached when the effects of these counteractive factors are <br />in balance. Under this situation, the angle of deviation becomes zero. <br />In this model, transverse bed profile evolution is related to the trans- <br />verse variation in bed material load. Since bed material load, excluding <br />wash load, is usually concentrated near the bed, it is assumed to follow <br />the direction given by Eq. 8, i.e. <br /> <br />q; = q, tan 8 . . . . . . . .. . . . . .. .. . .. .. .. . .. . .. . .. . .. . . .. . .. . . .. . .... (9) <br />in which q; = transverse bed material load per unit channel length; and <br />q, = longitudinal bed material load per unit channel width. <br />Unsteady sediment transport is complicated by sediment sorting. <br />Methods for estimating sediment rate by tracking variation in bed ma- <br />terial composition and stream bed profile evolution have been devel- <br />oped by Bennett and Nordin (4), Alonso et al. (1), and Borah et al. (5), <br />among others, To treat this time-dependent sediment transport, bed ma- <br />terials are divided into five size fractions, and the size for each fraction <br />is represented by its geometric mean diameter. For each size fraction, <br />sediment transport capacity is first computed using a sediment transport <br />formula. Then the actual sediment rate is obtained by considering sed- <br />iment material of all size fractions already in the flow and the exchange <br />of sediment load with the bed using the method by Borah et al. (5). If <br />the stream carries a load in excess of its capacity, it will deposit the ex- <br />cess material on the bed. In the case of erosion, any size fraction avail- <br />able for entrainment at the bed surface will be removed by the flow and <br />added to the sediment already in transport. During sediment removal, <br />the exchange between the flow and the bed is assumed to take place in <br />the active layer at the surface. Thickness of the active layer is based upon <br />the relation defined by Borah et al. (5). As a function of the material size <br />and composition, this thickness also reflects the flow condition. During <br />degradation, several of these layers may be scoured away, resulting in <br />the coarsening of the bed material and formation of a armor coat. How- <br />ever, new active layers may be deposited on the bed in the process of <br />aggradation. These procedures for computing sediment rate and sedi- <br />ment sorting are applied to the longitudinal and transverse direction. <br />They are also coupled with stream bed prome changes described in the <br />next section. <br />Prediction of Stream Bed Profile Changes.-Changes in stream bed <br />prome, at each time step, due to longitudinal and transverse variations <br />in sediment load are simulated. Changes along the longitudinal direc- <br />tion, i.e., aggradation or degradation, are computed using the continuity <br />equation for sediment movement in the longitudinal direction. This is <br />explained in Ref. 7. <br />Changes in channel bed elevation at a point due to transverse load <br />are computed using the continuity equation <br /> <br />az 1 10 <br />- +---(rq;) = 0...... ..... ....... .... ...,.... .... ... ... (to) <br />at 1-~rar <br /> <br />648 <br /> <br />26 <br />
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