Derivation of the 1D Exner equation

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Derivation of the 1D Exner equation
We begin with our original statement of mass conservation:
𝑑𝑆
π‘„π‘œπ‘’π‘‘ − 𝑄𝑖𝑛 = − ,
𝑑𝑑
where 𝑄 and 𝑆 are mass flux and storage (with dimensions of mass), respectively.
Considering a control area of soil surface with dimensions 𝛿π‘₯𝛿𝑦, the change in mass storage
there is manifested as a change in the bulk sediment volume
𝑑𝑆 𝑑(πœŒπ‘  𝑉) 𝑑
πœŒπ‘ π‘‘β„Ž
=
=
πœŒπ‘  β„Žπ›Ώπ‘₯𝛿𝑦
=
𝛿π‘₯𝛿𝑦 πœŒπ‘  1 − 𝑛 .
𝑑𝑑
𝑑𝑑
𝑑𝑑
πœŒπ‘  𝑑𝑑
In the expression on the right, storage is now expressed as a change in the thickness β„Ž of a
sediment layer with a porosity 𝑛 and particle mass density πœŒπ‘  . This sediment thickness
changes in response to changes in the mass flux across the control area, which can be
expressed in terms of the flow per unit width 𝑒π‘₯ 𝛿𝑧 and sediment concentration 𝐢 in a
volume of overland flow passing through a control volume 𝛿π‘₯𝛿𝑦𝛿𝑧:
𝑑𝑄
𝑑
𝑑(𝐢𝑒π‘₯ )
π‘„π‘œπ‘’π‘‘ − 𝑄𝑖𝑛 =
𝛿π‘₯ =
(πœŒπ‘  𝐢𝑒π‘₯ 𝛿π‘₯𝛿𝑦𝛿𝑧) =
πœŒπ‘  𝛿π‘₯𝛿𝑦𝛿𝑧.
𝑑π‘₯
𝑑π‘₯
𝑑π‘₯
Substituting the new expressions into the original mass conservation expression, the
simplified expression is a form of the Exner equation:
𝑑(𝐢𝑒π‘₯ 𝛿𝑧)
π‘‘β„Ž
= −(1 − 𝑛)
𝑑π‘₯
𝑑𝑑
Which is usually rearranged and stated by defining π‘žπ‘  as a volumetric flux per unit width:
π‘‘β„Ž
1 π‘‘π‘žπ‘ 
=−
𝑑𝑑
1 − 𝑛 𝑑π‘₯
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