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Use of Exact Solutions of Wave Propagation Problems to Guide Implementation of Nonlinear Seismic Ground Response Analysis Procedures
Authors:Annie O L Kwok  Jonathan P Stewart  Youssef M A Hashash  Neven Matasovic  Robert Pyke  Zhiliang Wang  Zhaohui Yang
Affiliation:1Project Engineer, Praad Geotechnical Inc., 5465 South Centinela Ave., Los Angeles, CA 90066-6942.
2Professor and Vice Chair, Dept. of Civil and Environmental Engineering, Univ. of California, Los Angeles 5731 Boelter Hall, Los Angeles, CA 90095 (corresponding author). E-mail: jstewart@seas.ucla.edu
3Associate Professor, Dept. of Civil and Environmental Engineering, RM 2230C NCEL, MC-250, Univ. of Illinois at Urbana-Champaign, 205 N. Mathews Ave., Urbana, IL 61801.
4Associate, GeoSyntec Consultants, 2100 Main St., Ste. 150, Huntington Beach, CA 92648.
5Consulting Engineer, 1076 Carol Lane, No. 136, Lafayette, CA 94549.
6Senior Engineer, Geomatrix Consultants Inc., 2101 Webster St., 12th Floor, Oakland, CA 94612.
7Engineer, URS Corporation, 1333 Broadway, Suite 800, Oakland, CA 94612.
Abstract:One-dimensional nonlinear ground response analyses provide a more accurate characterization of the true nonlinear soil behavior than equivalent-linear procedures, but the application of nonlinear codes in practice has been limited, which results in part from poorly documented and unclear parameter selection and code usage protocols. In this article, exact (linear frequency-domain) solutions for body wave propagation through an elastic medium are used to establish guidelines for two issues that have long been a source of confusion for users of nonlinear codes. The first issue concerns the specification of input motion as “outcropping” (i.e., equivalent free-surface motions) versus “within” (i.e., motions occurring at depth within a site profile). When the input motion is recorded at the ground surface (e.g., at a rock site), the full outcropping (rock) motion should be used along with an elastic base having a stiffness appropriate for the underlying rock. The second issue concerns the specification of viscous damping (used in most nonlinear codes) or small-strain hysteretic damping (used by one code considered herein), either of which is needed for a stable solution at small strains. For a viscous damping formulation, critical issues include the target value of the viscous damping ratio and the frequencies for which the viscous damping produced by the model matches the target. For codes that allow the use of “full” Rayleigh damping (which has two target frequencies), the target damping ratio should be the small-strain material damping, and the target frequencies should be established through a process by which linear time domain and frequency domain solutions are matched. As a first approximation, the first-mode site frequency and five times that frequency can be used. For codes with different damping models, alternative recommendations are developed.
Keywords:Earthquakes  Ground motion  Wave propagation  Seismic effects  Damping  
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