This data was submitted by Nancy Saltzman ( saltzman@ncsc.org ) The data is in AVS UCD format. Enjoy - Terry --- Terry Myerson International AVS Center North Carolina Supercomputing Center avs@ncsc.org This ucd data contains the finite element model of a sedimentary basin. Three dimensional displacements are given at the nodes. Each file contains the normalized displacements describing motion of one mode of oscillation, whose frequency is indicated in the file name (eg. 27886as.inp has frequency .27866). The basin model is half-ellipsoidal in shape. The bottom curved surface models a subterranean rock interface and is required to have no displacement, while the top flat surface of the model is a free surface corresponding to the ground surface. Only one quarter of the basin is modelled since it is sufficient to obtain solution for the full basin due to symmetries in the basin shape. Accordingly, modes are classified as 'sa', 'ss', 'as', and 'aa', where the first letter refers to motion of the vertical plane containing the long horizontal axis of the ellipsoid and the second refers to motion of the vertical plane containing the short horizontal axis. In this notation 'a' indicates 'antisymmetric' motion constrained to be strictly perpendicular to the plane and 's' indicates 'symmetric' motion constrained to be entirely in the plane. This type of data is of interest to seismologists and earthquake engineers because sedimentary basins which are filled with soft sediments and surrounded by hard rock trap earthquake waves within the basins, causing high amplitude, long duration, near mono-frequency ground motions that can be devastating to structures that may have similar natural frequencies. Thus visualization of ground motion (motion at the free surface) is a primary objective. Important characteristics affecting earthquake hazard assessment are ground locations of relatively large and very small displacement amplitudes, and the direction of motion polarization at different ground locations. Characteristics of subterranean motion, particularly locations of nodal surfaces where displacement is zero, are important for physical insight into the mechanism of resonant motion.