Abstract
The paper presents a mathematical scheme able to model the evolution of deposition-erosion processes in a one-dimensional stream, also taking account of non uniform grain-size mixtures and possibly non-equilibrium of sediment transport rate.
Instead of describing the sediment transport for fractions, that is, each fraction by means of its continuity equation, the model uses mean diameter and second-order (and possibly third-) moment of grain-size distribution. As a consequence the number of equations and variables is reduced.
Uj=Tj/Cj
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Abbreviations
- A2, B2:
-
parameters of sediment transport formula
- C:
-
concentration
- c1, c2, c3:
-
coefficients
- \(\tilde c_{D_b }\) :
-
celerity of transported mean diameter
- Dj :
-
mean diameter of class j-th
- Db :
-
mean diameter in the mixing layer
- Dt :
-
mean diameter of the transported material
- h:
-
water depth
- L*:
-
adaptation length
- m:
-
number of grain-size classes
- n, n1, l:
-
exponents
- x:
-
longitudinal coordinate
- t:
-
time
- Tj :
-
transport rate of j-th grain-size class
- Tc :
-
transport capacity of the j-th grain-size class
- U:
-
depth averaged velocity
- u * :
-
friction velocity
- w:
-
particle fall velocity
- Z:
-
bed elevation
- αj :
-
percentage of the j-th class inside the transport layer
- βj :
-
percentage of the j-th class into the exchange layer
- δ:
-
exchange layer thickness
- Δ:
-
height of the dunes
- σb, γb :
-
second and third moments of grain-size distribution inside the mixing layer
- σt, γt :
-
second and third moments of grain-size distribution of transported material
- Ï„*:
-
adaptation time
- ζj :
-
hiding factor for j-th grain-size class
References
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© 1991 Springer-Verlag
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Armanini, A. (1991). Variation of bed and transport mean diameters in non-equilibrium conditions. In: Armanini, A., Di Silvio, G. (eds) Fluvial Hydraulics of Mountain Regions. Lecture Notes in Earth Sciences, vol 37. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0011208
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DOI: https://doi.org/10.1007/BFb0011208
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