Abstract

In this paper we analyze the Hirano active layer model used in mixed sediment river morphodynamics concerning its ill-posedness. Ill-posedness causes the solution to be unstable to short-wave perturbations. This implies that the solution presents spurious oscillations, the amplitude of which depends on the domain discretization. Ill-posedness not only produces physically unrealistic results but may also cause failure of numerical simulations. By considering a two-fraction sediment mixture we obtain analytical expressions for the mathematical characterization of the model. Using these we show that the ill-posed domain is larger than what was found in previous analyses, not only comprising cases of bed degradation into a substrate finer than the active layer but also in aggradational cases. Furthermore, by analyzing a three-fraction model we observe ill-posedness under conditions of bed degradation into a coarse substrate. We observe that oscillations in the numerical solution of ill-posed simulations grow until the model becomes well-posed, as the spurious mixing of the active layer sediment and substrate sediment acts as a regularization mechanism. Finally we conduct an eigenstructure analysis of a simplified vertically continuous model for mixed sediment for which we show that ill-posedness occurs in a wider range of conditions than the active layer model.

Highlights

  • The mixed character of the sediment is a property necessary to explain physical phenomena such as downstream fining (Sternberg, 1875; Blom et al, 2016), the gravel sand transition zone (Yatsu, 1955; Blom et al, 2017), the formation of bedload sheets (Seminara et al, 1996), or bed surface armoring (Parker and Klingeman, 1982). Hirano (1971) was the first to develop a mass conservation model for mixed-size sediment

  • We have assessed the well-posedness of the equations used to model mixed sediment river morphodynamics

  • In particular we have studied the system formed by the flow equations (SaintVenant, 1871) together with the active layer model (Hirano, 1971) and a simplified vertically continuous model (Viparelli et al, 2017)

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Summary

Introduction

The mixed character of the sediment is a property necessary to explain physical phenomena such as downstream fining (Sternberg, 1875; Blom et al, 2016), the gravel sand transition zone (Yatsu, 1955; Blom et al, 2017), the formation of bedload sheets (Seminara et al, 1996), or bed surface armoring (Parker and Klingeman, 1982). Hirano (1971) was the first to develop a mass conservation model for mixed-size sediment. Sieben (1994) identified a region of parameters where, for a sediment mixture consisting of two grain size classes under bed degradation into a substrate finer than the active layer, the model is unconditionally ill-posed This occurs when the “sorting celerity” equals the “bed celerity”. The opposite happens for coarse sediment fractions, which experience a larger exposure to the flow than in a unisize case In their analysis Stecca et al (2014) showed that the model can become illposed under degradational conditions if and only if the substrate is finer than a reference grain size distribution which is related to the grain size distribution of the bedload, instead of the active layer (as in Ribberink’s (1987) analysis).

Model equations
Flow equations
Adapted active layer model equations
Simplified vertically continuous model equations
Closure relations
Matrix formulation
Steady active layer model consisting of two size fractions
Steady vertically continuous model consisting of two size fractions
Active layer model parameter study
Hiding
Aggradational flux to the substrate
Prefactor in a sediment transport relation and morphodynamic factor
Exponent and critical Shields stress in a sediment transport relation
Active layer thickness
Consequences of ill-posedness
Numerical examples
Sensitivity analysis
Ill-posed domain of a three-size-fractions case
Effect of an unsteady active layer thickness in the ill-posed domain
Conclusions

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