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Report - Oregon State Library: State Employee Information Center ...

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6.0 NUMERICAL MODELING<br />

The database of well characterized and instrumented case studies on the seismic performance of<br />

bridge abutments on sloping embankments is very limited. Such cases require pre- and postearthquake<br />

geotechnical and survey data, recorded earthquake motions in vicinity of the site (or a<br />

reasonable estimate of the ground motions from a site response investigation), structural “asbuilt”<br />

drawings of the bridge and abutments affected by the ground motions, and the extraction<br />

of piles to inspect for possible subsurface damage. To supplement the case study data, a<br />

numerical modeling study was conducted. A numerical model is advantageous because<br />

numerous scenarios can be analyzed, and various design parameters can easily be adjusted to<br />

determine their influence on an embankment’s seismic performance. The major concern with<br />

applying a model to soil-structure interaction problems is the numerical uncertainty. This<br />

concern is limited in this study because a series of validation studies were performed using the<br />

available case study data on the seismic performance of various earth and retaining structures at<br />

sites where liquefaction was observed.<br />

The numerical modeling was accomplished utilizing a commercial finite difference computer<br />

program entitled Fast Lagrangian Analysis of Continua (FLAC) version 3.34 (Itasca Consulting<br />

Group 1997). The FLAC model is a non-linear, two-dimensional finite difference program<br />

capable of modeling both static and dynamic situations. Elements or zones represent the<br />

materials (soil and structural), with all the elements and zones constituting the grid (mesh). The<br />

FLAC model utilizes a time-marching scheme, where during each timestep, the following<br />

procedures take place (Figure 6.1): (1) nodal velocities and displacements are calculated from<br />

stresses and forces using the equations of motion, then (2) the basic explicit calculation sequence<br />

uses the velocities to computes strain rates, which are derived from the nodal velocities, which<br />

are used to update the stresses used in the following time step are computed from the strain rates.<br />

.These two procedures are then repeated until the computed unbalanced forces within the mesh<br />

are within a user-specified limit.<br />

Equilibrium Equation<br />

(Equation of Motion)<br />

new velocities<br />

and<br />

displacements<br />

new<br />

stresses or<br />

forces<br />

Stress/Strain Relationship<br />

(Constitutive Model)<br />

Figure 6.1: Basic Explicit Calculation Cycle<br />

109

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