 
          1567
        
        
          Accumulated Stress Based Model for Prediction of Residual Pore Pressure
        
        
          Étude et développement du modèle pour le pronostic sur l’excès de pression hydrostatique
        
        
          interstitielle causé par les contraintes accumulées
        
        
          Park D., Ahn J.-K.
        
        
          
            Department of Civil and Environmental Engineering, Hanyang University
          
        
        
          ABSTRACT: Even though the important influence of pore pressure rise under cyclic loading on seismic wave propagation is
        
        
          recognized, effective stress analysis is rarely performed due to difficulties in selecting the parameters for the pore pressure model. In
        
        
          this paper, a new numerical model for predicting pore pressure under cyclic loading is developed. The advantages of the model are
        
        
          that it requires only the CSR – N curve in selecting its parameters and it can be can be used for any loading pattern. The accuracy of
        
        
          the model is validated through comprehensive comparisons with measurements.
        
        
          RÉSUMÉ : L’importance de l’excès de la pression interstitielle causé par les contraintes accumulées de la propagation des ondes
        
        
          sismiques est bien reconnue, mais l’analyse de contrainte effective est rarement pratiquée en raison de difficultés à évaluer les
        
        
          paramètres pour le modèle de la pression interstitielle. Le présent article concerne le développement du nouveau modèle numérique
        
        
          pour le pronostic sur l’excès de pression interstitiellecausé par les contraintesdans le sol. Les avantages de ce modèle sontque nous
        
        
          pouvons déterminer tous les paramètres avec la courbe CSR-N et qu’il peut s’appliquer aux diverses formes de contraintes. La
        
        
          précision du modèle est contrôlée par comparaison avec le résultat du test.
        
        
          KEYWORDS: pore water pressure, damage parameter, cyclic stress ratio, accumulated shear stress, time-domain analysis.
        
        
          1 INTRODUCTION
        
        
          Build-up of residual excess pore water pressure in sands and
        
        
          silts during seismic loading causes reduction in stiffness and
        
        
          strength of soils and can lead to liquefaction. It may greatly
        
        
          influence the characteristics of ground motion propagation,
        
        
          stability of embankments, and seismic performance of structures
        
        
          such as tunnels and bridges. The importance of predicting the
        
        
          pore pressure has been well recognized and the characteristics
        
        
          of pore pressure generation for sands and silts have been
        
        
          extensively studied (Booker et al. 1976, Carraro et al. 2003,
        
        
          Derakhshandi et al. 2008, Lee and Albaisa 1974, Polito et al.
        
        
          2008, Xenaki and Athanasopoulos 2003).
        
        
          Various empirical models have been developed in the past to
        
        
          predict the generation of pore pressure under cyclic loading.
        
        
          The earliest models are based on the concept of cyclic stress
        
        
          approach, where the seismic loading is presented as uniform
        
        
          cyclic shear stress and the liquefaction potential is characterized
        
        
          by the amplitude of cyclic shear stress and number of loading
        
        
          cycles (Seed and Lee 1966, Seed et al. 1975b). The laboratory
        
        
          test that best fits the cyclic stress approach is stress controlled
        
        
          cyclic test. The result of a stress-controlled cyclic test is often
        
        
          presented in the form of
        
        
          
            CSR – N
          
        
        
          curve, where the
        
        
          
            CSR
          
        
        
          represents the ratio of shear stress (shear stress normalized by
        
        
          the effective confining pressure in a cyclic triaxial test and
        
        
          effective vertical stress in a simple shear test) that triggers
        
        
          liquefaction at the given number of cycles,
        
        
          
            N
          
        
        
          . While the stress
        
        
          controlled cyclic triaxial test is still the most popular method,
        
        
          the problems of the test procedure have been identified, which
        
        
          include difficulty in defining the exact state at which the
        
        
          liquefaction initiates, specimen non-uniformity, abrupt build-up
        
        
          of pore pressure at high pore pressures, different state of
        
        
          stresses compared to the field (Kramer 1996).
        
        
          Consequent laboratory tests have shown that the controlling
        
        
          factor of the build-up of excess pore pressure is not cyclic shear
        
        
          stress, but cyclic shear strain. Strain-controlled cyclic tests,
        
        
          especially simple shear tests, have been increasingly used to
        
        
          measure the excess pore pressure under cyclic loading.
        
        
          Numerical models that predict pore pressure as a function of
        
        
          accumulated shear strain have been proposed (Dobry et al.
        
        
          1985a, Dobry et al. 1985b, Finn and Bhatia 1982, Ivsic 2006).
        
        
          While the advantages of strain-controlled test procedure and
        
        
          strain-based pore pressure model are well recognized, it should
        
        
          be noted that the stress-controlled cyclic tests are still the most
        
        
          widely used laboratory procedure for evaluating the liquefaction
        
        
          potential. In the absence of the strain-controlled test
        
        
          measurements, the input parameters for a strain-based model
        
        
          cannot be determined. The difficulty in selecting the input
        
        
          parameters for the strain-based models is one of the reasons
        
        
          responsible for the seldom use of effective stress dynamic
        
        
          analysis in practice. In the absence of strain-controlled test data,
        
        
          it seems logical that an alternative pore pressure model that only
        
        
          requires the
        
        
          
            CSR – N
          
        
        
          curve obtained from the stress-controlled
        
        
          test in selecting its parameters be used.
        
        
          This study proposes such a pore pressure model and presents
        
        
          guidelines for selecting its input parameters. A method for
        
        
          constructing the empirical
        
        
          
            CSR – N
          
        
        
          curve from in-situ
        
        
          penetration resistance in case the measured
        
        
          
            CSR – N
          
        
        
          curve is
        
        
          not available is also outlined. The applicability of the model is
        
        
          validated through comparisons with laboratory test data selected
        
        
          from literature and also non-published test data.
        
        
          2 PORE PRESSURE MODEL
        
        
          One of the earliest pore pressure model, developed by Seed
        
        
          et al. (1975b), is defined as follows:
        
        
          1/
        
        
          1
        
        
          1 1
        
        
          sin 2
        
        
          1
        
        
          2
        
        
          
            u
          
        
        
          
            L
          
        
        
          
            N
          
        
        
          
            r
          
        
        
          
            N
          
        
        
          
        
        
          
        
        
          
        
        
           
        
        
          
        
        
          
        
        
          
        
        
           
        
        
          
        
        
          
        
        
           
        
        
           
        
        
          
        
        
          
        
        
          
        
        
          
        
        
          (1)
        
        
          where,
        
        
          = residual pore pressure normalized to the initial
        
        
          effective confining stress,
        
        
          
            N
          
        
        
          = equivalent number of cycles,
        
        
          
            N
          
        
        
          
            L
          
        
        
          = number of cycles required to cause liquefaction,
        
        
          
        
        
          = empirical
        
        
          
            u
          
        
        
          
            r