The Exner equation is a statement of conservation of mass that applies to sediment in a fluvial system such as a river.^{[1]} It was developed by the Austrian meteorologist and sedimentologist Felix Maria Exner, from whom it derives its name.^{[2]}
Contents

The equation 1

Basic equation 1.1

Including external changes in elevation 1.2

References 2
The equation
The Exner equation describes conservation of mass between sediment in the bed of a channel and sediment that is being transported. It states that bed elevation increases (the bed aggrades) proportionally to the amount of sediment that drops out of transport, and conversely decreases (the bed degrades) proportionally to the amount of sediment that becomes entrained by the flow.
Basic equation
The equation states that the change in bed elevation, \eta, over time, t, is equal to one over the grain packing density, \varepsilon_o, times the negative divergence of sediment flux, q_s.

\frac{\partial \eta}{\partial t} = \frac{1}{\varepsilon_o}\nabla\cdot\mathbf{q_s}
Note that \varepsilon_o can also be expressed as (1\lambda_p), where \lambda_p equals the bed porosity.
Good values of \varepsilon_o for natural systems range from 0.45 to 0.75.^{[3]} A typical good value for spherical grains is 0.64, as given by random close packing. An upper bound for closepacked spherical grains is 0.74048. (See sphere packing for more details); this degree of packing is extremely improbable in natural systems, making random close packing the more realistic upper bound on grain packing density.
Often, for reasons of computational convenience and/or lack of data, the Exner equation is used in its onedimensional form. This is generally done with respect to the downstream direction x, as one is typically interested in the downstream distribution of erosion and deposition though a river reach.

\frac{\partial \eta}{\partial t} = \frac{1}{\varepsilon_o}\frac{\partial\mathbf{q_s}}{\partial x}
Including external changes in elevation
An additional form of the Exner equation adds a subsidence term, \sigma, to the massbalance. This allows the absolute elevation of the bed \eta to be tracked over time in a situation in which it is being changed by outside influences, such as tectonic or compressionrelated subsidence (isostatic compression or rebound). In the convention of the following equation, \sigma is positive with an increase in elevation over time and is negative with a decrease in elevation over time.

\frac{\partial \eta}{\partial t} = \frac{1}{\varepsilon_o}\nabla\cdot\mathbf{q_s}+\sigma
References

^ Paola, C.; Voller, V. R. (2005). "A generalized Exner equation for sediment mass balance". Journal of Geophysical Research 110: F04014.

^ Parker, G. (2006), 1D Sediment Transport Morphodynamics with applications to Rivers and Turbidity Currents, Chapter 1, http://vtchl.uiuc.edu/people/parkerg/_private/ebookPowerPoint/RTebookCh1IntroMorphodynamics.ppt.

^ Parker, G. (2006), 1D Sediment Transport Morphodynamics with applications to Rivers and Turbidity Currents, Chapter 4, http://vtchl.uiuc.edu/people/parkerg/_private/ebookPowerPoint/RTebookCh4ConservationBedSed.ppt.
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