Water Resources of the United States
Visualizing the SUTRA dispersion model in 3DBackgroundThe SUTRA dispersion model in three dimensions (3D) is a generalization of the original two-dimensional (2D) model. The 2D and 3D SUTRA dispersion models are described in detail in Section 2.5 of the SUTRA documentation. This page supplements the formal documentation by providing interactive visualizations of the 3D dispersion model. A VRML browser is required to view the visualizations interactively. In the 3D SUTRA dispersion model, the longitudinal and transverse dispersivities, aL, aT1, and aT2, can depend on the direction of groundwater flow, i.e., the dispersion model can be anisotropic. SUTRA computes the value of the longitudinal dispersivity, aL, from the radius of an ellipsoid measured along the flow direction. Thus, aL is greatest when flow is along the longest axis of the ellipsoid. The transverse dispersivities, aT1 and aT2, are computed from radii of a second ellipsoid. These transverse radii are measured along two directions that are perpendicular to the flow direction and to each other. The user controls the behavior of the 3D dispersion model by setting SUTRA input parameters that determine the dimensions and orientation of the two ellipsoids in space:
3D visualizationsThe visualizations below are best viewed interactively, which will allow you to rotate, zoom, and pan the image. This requires a VRML browser. The way in which SUTRA computes the longitudinal dispersivity, aL, as a function of flow direction is illustrated in the figure below, which corresponds to Figure 2.4b in the SUTRA documentation:
Figure. How SUTRA calculates the longitudinal dispersivity, aL, as a function of flow direction. Here, v is the flow (velocity) vector; xmax, xmid, and xmin are coordinates aligned with the max, mid, and min directions, respectively; and aL is the squared radius measured along the flow direction. The principal radii of the ellipsoid (not labeled) have squared lengths of aLmax, aLmid, and aLmin, and are aligned with the max, mid, and min directions, respectively. Note that aL=aLmax for flow in the max direction, aL=aLmid for flow in the mid direction, and aL=aLmin for flow in the min direction. The way in which SUTRA computes the transverse dispersivities, aT1 and aT2, as a functions of flow direction is illustrated in the figure below, which corresponds to Figure 2.4c in the SUTRA documentation:
Figure. How SUTRA computes the transverse dispersivities, aT1 and aT2, as a functions of flow direction. Here, v is the flow (velocity) vector and xmax, xmid, and xmin are coordinates aligned with the max, mid, and min directions, respectively. The principal radii of the ellipsoid (not labeled) have squared lengths of aLmax, aLmid, and aLmin, and are aligned with the max, mid, and min directions, respectively; and aT1 and aT2 are squared radii measured in two directions perpendicular to the flow direction. These two directions, which are the transverse dispersion directions, correspond to the principal axes of the ellipse (called the slicing ellipse) formed by the intersection of the ellipsoid with the plane that passes through the origin and is perpendicular to the flow direction. Note that when groundwater flow is in one of the three principal permeability directions (max, mid, or min), aT1 and aT2 take on the values associated with the other two directions. Thus, the transverse dispersivities are aTmid and aTmin for flow in the max direction; aTmax and aTmin for flow in the mid direction; aTmax and aTmid for flow in the min direction.
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