Kinematic Wave Overland Flow Model
A kinematic wave model is a conceptual model of watershed response that uses laws of conservation of mass and momentum to simulate overland and channelized flows. The model represents the watershed as a wide open channel, with inflow equal to the excess precipitation. Then it simulates unsteady channel flow over the surface to compute the watershed runoff hydrograph. The watershed is represented as a set of overland flow planes and collector channels.
In kinematic wave modeling, the watershed shown in Figure 4-27(a) is represented in Figure 4-27(b) as series of overland flow planes (gray areas) and a collector channel (dashed line). The collector channel conveys flow to the watershed outlet.

Figure 4-27. Kinematic wave model representation of a watershed (USACE 2000)
The equations used to define conservation of mass and momentum are the Saint Venant equations. The conservation of mass equation is:

Equation 4-57.
Where:
- A= cross sectional area of flow (ft2, m2)
- T= time (sec.)
- Q= flow rate (cfs, m3/sec.)
- x= distance along the flow path (ft, m)
- q= lateral discharge added to the flow path per unit length of the flow path (cfs/ft, mo3/sec./m)
The momentum equation energy gradient is approximated by:

Equation 4-58.
Where:
- a and b= coefficients related to the physical properties of the watershed.
Substituting Equation 4-56 into Equation 4-55 yields a single partial differential equation in Q:

Equation 4-59.
Where:
- q= lateral inflow (cfs/ft, mL3/s/m)
Equation 4-54 can be expressed in terms of Manning’s n, wetted perimeter, and bed slope by substituting the following expression for
α𝑄
into Equation 4-56:β

Equation 4-60.
Where:
- n= Manning’s roughness coefficient
- P= wetted perimeter (ft, m)
- S= flow plane slope (ft/ft, m/m)o
The solution to the resulting equation, its terms, and basic concepts are detailed in Chow (1959) and other texts.