Derivation of the 1D Exner equation We begin with our original statement of mass conservation: ππ πππ’π‘ − πππ = − , ππ‘ where π and π are mass flux and storage (with dimensions of mass), respectively. Considering a control area of soil surface with dimensions πΏπ₯πΏπ¦, the change in mass storage there is manifested as a change in the bulk sediment volume ππ π(ππ π) π ππ πβ = = ππ βπΏπ₯πΏπ¦ = πΏπ₯πΏπ¦ ππ 1 − π . ππ‘ ππ‘ ππ‘ ππ ππ‘ In the expression on the right, storage is now expressed as a change in the thickness β of a sediment layer with a porosity π and particle mass density ππ . 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 π’π₯ πΏπ§ and sediment concentration πΆ in a volume of overland flow passing through a control volume πΏπ₯πΏπ¦πΏπ§: ππ π π(πΆπ’π₯ ) πππ’π‘ − πππ = πΏπ₯ = (ππ πΆπ’π₯ πΏπ₯πΏπ¦πΏπ§) = ππ πΏπ₯πΏπ¦πΏπ§. ππ₯ ππ₯ ππ₯ Substituting the new expressions into the original mass conservation expression, the simplified expression is a form of the Exner equation: π(πΆπ’π₯ πΏπ§) πβ = −(1 − π) ππ₯ ππ‘ Which is usually rearranged and stated by defining ππ as a volumetric flux per unit width: πβ 1 πππ =− ππ‘ 1 − π ππ₯