This page is hosted on AFS file server space, which is being shut down on November 13, 2018. If you are seeing this message, your service provider needs to take steps now. Visit for more information.

Special Features

Wetting and Drying

Overflow and Throughflow Barriers

Bridge Piers

Wave Radiation Stress




Bridge Piers

Given the typical resolution of coastal circulation models, (e.g., in nearshore applications resolved scales are usually 10s to 100s of meters and larger), it is rarely practical to solve explicitly for the small scale flow around obstructions such as bridge pilings (diameters of meters). However, in some situations it may be desirable to include the effects of these subgrid scale obstructions on the resolved scale flow. To accomplish this, a subgrid scale obstruction parameterization has been developed and implemented in ADCIRC. Since the cross-sectional area of these obstructions is usually quite small compared to the cross-sectional area of the flow field (and thus the effect on flow continuity is quite small), their primary effect is to impart additional drag on the resolved scale flow. This section describes the theory behind the obstruction parameterization implemented in ADCIRC. The bridge pier option is turned on by setting the parameter NWP = 2 in the Model Parameter and Periodic Boundary Condition File. Required input coefficients are read in at specified nodes from the Spatially Varying Friction Coefficient File. Additional information can be found in Luettich and Westerink (1999).

The two-dimensional, vertically integrated momentum equations used in ADCIRC (e.g., Eqs. 2 -3 in the formulation section) contain bottom friction (drag) terms, as shown below:

To represent the extra drag caused by subgrid scale obstructions such as bridge piers, a second contribution has been added to , i.e.,

= bottom friction x + obstruction drag x and = bottom friction y + obstruction drag y

Options in ADCIRC exist to express the bottom friction terms as linear, quadratic or hybrid quadratic/manningís n functions of flow velocity (see the formulation section). The obstruction drag is assumed to be due primarily to form drag and therefore is represented as quadratic in velocity:

obstruction drag x = and obstruction drag y =

where is an obstruction (piling) drag coefficient.

To determine for a series of bridge pilings, we have utilized the extensive body of research conducted in the early to mid 1900s on flow around pilings. Yarnell (1934a,b), as summarized by Henderson (1966), fit the change in water level for steady, unidirectional flow past a piling to the following relation:

where, H is the total water depth, K is a pier shape factor (Table 1), is the square of the Froud number, is the fraction of the cross section obstructed by the piling, is the velocity in the along stream (s) direction and g is the acceleration of gravity. This equation is considered to be valid so long as < 0.5.

Table 1. recommended pier shape factors

Pier Shape


Semicircular nose and tail


Lens-shaped nose and tail


Twin-cylinder piers with connecting diaphragm


Twin-cylinder piers without diaphragm


90 deg triangular nose and tail


Square nose and tail



For this same case of steady, unidirectional flow in the vicinity of pilings, the corresponding ADCIRC momentum equations simplify to:

where is the free surface gradient in the along stream direction. Approximating this gradient as , Yarnellís equation and the simplified momentum equation can be combined to obtain an expression for :

This equation is used at each time step in ADCIRC, to compute at all nodes associated with bridge pilings. This allows the obstruction drag to be computed and added to the bottom friction terms as discussed above.

We note that Yarnellís equation is based on H and values measured at a point downstream of the pilings. ADCIRC uses H and at the effective piling location to minimize complications due to changing flow direction, e.g., due to reversal of the tide. Typical elevation and velocity changes that result are small enough that the overall results are not compromised by this approximation.




Henderson, F.M., 1966, Open Channel Flow, MacMillan Publishing Co., New York, pp 265-267.

Luettich, R.A., Jr. and J.J. Westerink, 1999, Implementation of Bridge Pilings in the ADCIRC Hydrodynamic Model: Upgrade and Documentation for ADCIRC Version 34.19, Contractors Report, department of the Army, US Army Corps of Engineers, Waterways Experiment Station, Vicksburg, MS, November 19, 1999, 8 p.

Yarnell, D.L., 1934a, Pile trestles as channel obstructions, U.S. Dept of Agriculture, Tech. Bull. 429.

Yarnell, D.L., 1934b, Bridge piers as channel obstructions, U.S. Dept of Agriculture, Tech. Bull. 442.

  Contact:   About Webpage    ADCIRC Listserv   Join ADCIRC Listserv   Request ADCIRC code Updated February 13, 2008