 
          923
        
        
          Dynamic centrifugal model test for unsaturated embankments considering seepage
        
        
          flow and the numerical analysis
        
        
          Expérimentation en centrifugeuse et modélisation numérique de la réponse aux
        
        
          séismes de remblais non saturés en prenant en compte l’écoulement
        
        
          Higo Y., Oka F., Kimoto S., Kinugawa T.
        
        
          Department of Civil and Earth Resources Engineering, Kyoto University, Japan
        
        
          Lee C.-W., Doi T.
        
        
          Former graduate student of Department of Civil and Earth Resources Engineering, Kyoto University, Japan
        
        
          ABSTRACT: Earthquake-induced failure of unsaturated road embankments has taken place during the past earthquakes. It has been
        
        
          pointed out that water flow or higher water content of road embankments was a possible reason of the damage. In this study, dynamic
        
        
          resistance of unsaturated embankments with and without the seepage flow has been studied through the centrifugal model tests of
        
        
          unsaturated embankment and their numerical simulations by a multi-phase coupled finite element method with an elasto-plastic
        
        
          constitutive model. During the tests, displacement, pore pressures, and acceleration of embankments have been fully monitored. The
        
        
          dynamic behavior of unsaturated embankments with infiltration of pore water has been discussed on the basis of comparison between
        
        
          the experimental and the numerical results. From the present study, we have found that the seepage flow and the high water content
        
        
          extensively affect the dynamic stability of unsaturated road embankments.
        
        
          RÉSUMÉ: Les remblais routiers non saturés peuvent s’écrouler lors d’un séisme, la cause de cet écroulement étant sans doute à
        
        
          rechercher dans l’écoulement d’eau ou dans des grandes valeurs de teneur en eau au sein du remblai. Dans cet article, la résistance
        
        
          dynamique d’un remblai non saturé est étudiée, avec ou sans écoulement, par des essais en centrifugeuse et par leur modélisation
        
        
          numérique aux Eléments Finis, en utilisant une approche hydromécanique couplée et un modèle constitutif élasto-plastique pour le
        
        
          sol. Les déplacements, les pressions interstitielles et les accélérations ont été mesurés tout au long des essais. Les résultats
        
        
          expérimentaux et les résultats numériques ont été comparés. Les résultats de cette étude confirment que l’écoulement et la forte teneur
        
        
          en eau ont effectivement un rôle majeur pour la stabilité dynamique des remblais routiers non saturés.
        
        
          KEYWORDS: unsaturated soil, embankment, earthquake, failure, dynamic centrifugal model test, numerical simulation.
        
        
          1 INTRODUCTION
        
        
          It is well known that the road embankment is still vulnerable
        
        
          against earthquakes. Earthquakes damaged road embankments
        
        
          during the extensive earthquakes such as the 2011 off the
        
        
          Pacific Coast of Tohoku Earthquake (M9.0). In particular, road
        
        
          embankments constructed on mountain/hill sides were severely
        
        
          damaged by the 2009 Suruga Bay Earthquake, the 2007 Noto
        
        
          Hanto Earthquake and the 2004 Niigata-ken Chuetsu
        
        
          Earthquake etc.
        
        
          In the cases of the Noto Hanto Earthquake and the Niigata-
        
        
          ken Chuetsu Earthquake, seepage water flow or higher water
        
        
          content in the embankments was a possible reason of the
        
        
          damage of the road embankments. Increase in the water
        
        
          contents causes loss of the inter-particle force caused by suction
        
        
          and decrease in the skeleton stress. This suggests that the effect
        
        
          of the seepage water flow and the high water content in the
        
        
          embankments on the dynamic failure of road embankment has
        
        
          to be studied in detail. However, to the authors’ knowledge,
        
        
          there are a limited number of physical model studies on
        
        
          unsaturated embankments considering seepage water as well as
        
        
          numerical ones (e.g., Hayashi et al. 2002, Doi et al. 2010).
        
        
          In this study, seismic resistance of unsaturated embankments
        
        
          with and without the seepage water has been studied through the
        
        
          centrifugal model tests and their numerical simulations by a
        
        
          multi-phase coupled finite element method with an elasto-
        
        
          plastic constitutive model (Oka et al. 2008, Oka et al. 2011).
        
        
          The dynamic behavior of unsaturated embankments with
        
        
          infiltration of the pore water has been discussed on the basis of
        
        
          comparison between the experimental and numerical results.
        
        
          2 DYNAMIC CENTRIFUGAL MODEL TESTS
        
        
          2.1
        
        
          
            Soil used in the test
          
        
        
          The soil used in the model tests is Yodogawa-levee sand, which
        
        
          has been used to fix the embankment of Yodo River in Kansai
        
        
          area. The physical properties of Yodogawa-levee sand are listed
        
        
          in Table 1.
        
        
          2.2
        
        
          
            Testing procedure
          
        
        
          The model configuration and the sensor locations are illustrated
        
        
          in Fig. 1. Prior to preparing the specimen, test samples were
        
        
          mixed with water to set up the initial water contents of 15%.
        
        
          Then, model embankments were prepared by compacting
        
        
          method in eight layers; the base ground and the embankment
        
        
          were separated into three layers (thickness: 30mm, 15mm,
        
        
          15mm), and five layers (as same thickness: 20mm),
        
        
          respectively. During the model construction, the accelerometers
        
        
          and the pore pressure transducers were embedded at the
        
        
          prescribed locations. The degree of compaction of all the cases
        
        
          Table 1. Physical properties of Yodogawa-levee sand
        
        
          
            
              Parameter
            
          
        
        
          
            
              Value
            
          
        
        
          Sand content (%)
        
        
          73.2
        
        
          Silt content (%)
        
        
          14.7
        
        
          Clay content (%)
        
        
          12.1
        
        
          D
        
        
          max
        
        
          (mm)
        
        
          *
        
        
          2.0
        
        
          D
        
        
          50
        
        
          (mm)
        
        
          0.29
        
        
          ρ
        
        
          s
        
        
          (g/cm
        
        
          3
        
        
          )
        
        
          2.661
        
        
          w
        
        
          opt
        
        
          (%)
        
        
          13.7
        
        
          ρ
        
        
          dmax
        
        
          (g/cm
        
        
          3
        
        
          )
        
        
          1.861
        
        
          k(m/sec)
        
        
          **
        
        
          4.79
        
        
          ×
        
        
          10
        
        
          -6
        
        
          *Maximum diameter of sieved particle
        
        
          **Permeability when degree of compaction is 90%