Bear Brook Watershed in Maine (BBWM) consists of a pair of research watersh
eds, East Bear Brook (EBB) and West Bear Brook (WBB), Years of research and
observations have shown both watersheds have high similarity in geographic
and hydrologic characteristics; a simple comparison of hydrographs from th
ese two watersheds further substantiates this similarity.
The Object Watershed Link Simulation (OWLS) model was developed and used to
simulate the hydrological processes within the BBWM. The OWLS model is a 3
-dimensional, vector-based, visualized, physically-based distributed waters
hed hydrologic model. Simulation results not only provide a close examinati
on of hydrologic processes within a watershed, but also dynamically visuali
ze the processes of flow separations and Variable Source Areas (VSA),
Results from flow separations suggest that surface flow from riparian area
is the predominate component for the flood rising limb and that macropore f
low from riparian area dominates during the falling limb. Soil matrix flow
has little effect during flood period but is a persistent contributor to ba
se flow. Results from VSA visualization demonstrate 3-D dynamic changes in
surface flow distribution and suggest that downstream riparian areas are th
e major contributing area for peak flow.
As water chemistry is highly relevant to the flow paths within a watershed,
simulations have provided valuable information about source of stream flow
and the water migration dynamics to support the study of watershed chemist
ry in the BBWM. More specific linkages between the chemistry behavior and t
he dynamic hydrologic processes should become the next simulation effort in
the watershed study.
There are many questions that art critical to watershed chemistry studies l
ike: which flow component (surface flow, macropore flow, soil matrix flow)
predominates during peak flows? How do the flow components distribute durin
g a flood event? How do flow contributions differ between these two watersh
eds? Which portion of the watershed contributes the most to the peak flows?
These questions remain unknown from previous observations and only can be
addressed with a physically-based distributed model.