Trying to overcome the limitation of Greenberg's model, Underwood put forward an
exponential model as shown below.
(1)
where The model can be graphically expressed as in figure 1.
is the free flow speed and is the optimum density, i.e. the density
corresponding to the maximum flow.
Figure 1:
Underwood's exponential model
In this model, speed becomes zero only when density reaches infinity which is
the drawback of this model.
Hence this cannot be used for predicting speeds at high densities.