 
          1494
        
        
          Proceedings of the 18
        
        
          th
        
        
          International Conference on Soil Mechanics and Geotechnical Engineering, Paris 2013
        
        
          Obviously, there is a rotation of the main axes of the
        
        
          response-envelopes. That means that the ratios of quasi-elastic
        
        
          moduli depend on the stress ratio η.
        
        
          This influence can be quantified. Figure 8 shows the ratio
        
        
          E
        
        
          v
        
        
          /E
        
        
          h
        
        
          of the vertical stiffness E
        
        
          v
        
        
          = Δσ
        
        
          v
        
        
          /Δε
        
        
          v
        
        
          and the horizontal
        
        
          stiffness E
        
        
          h
        
        
          = Δσ
        
        
          h
        
        
          /Δε
        
        
          h
        
        
          as a function of the stress-ratio η. For this
        
        
          purpose data were analysed for stress-paths α
        
        
          σ
        
        
          = 90° and 270°,
        
        
          (axial compression and extension) and α
        
        
          σ
        
        
          = 0° and 180° (radial
        
        
          compression and extension).
        
        
          Figure 8: Ratio E
        
        
          v
        
        
          /E
        
        
          h
        
        
          depending on the initial stress-ratio
        
        
          
        
        
          The dependence of the ratio E
        
        
          v
        
        
          /E
        
        
          h
        
        
          on the initial stress-ratio η
        
        
          can be interpreted as a
        
        
          
            stress-induced anisotropy
          
        
        
          . Similar
        
        
          observations are also made when investigating much smaller
        
        
          stress- or strain-cycles, e.g. Ezaoui and Di Benedetto (2009) or
        
        
          Hoque and Tatsuoka (1998)
        
        
          .
        
        
          The coarser the sand, the more
        
        
          distinctive is the difference between E
        
        
          v
        
        
          and E
        
        
          h
        
        
          , i.e. the ratio
        
        
          E
        
        
          v
        
        
          /E
        
        
          h
        
        
          increases Hoque and Tatsuoka (1998). A detailed analysis
        
        
          shows a stronger influence of the stress-ratio η on the vertical
        
        
          than on the horizontal stiffness, see Bellotti, et al. (1996).
        
        
          Figure 8 does not only show a stress induced anisotropy. At
        
        
          the isotropic stress state with η = 0 the ratio E
        
        
          v
        
        
          /E
        
        
          h
        
        
          is ≠ 1. This
        
        
          means, that there are no isotropic properties at an initial
        
        
          isotropic stress state, i.e. there also is an
        
        
          
            inherent anisotropy
          
        
        
          .
        
        
          Most authors come to similar conclusions. While Hoque and
        
        
          Tatsuoka (1998) find out E
        
        
          v
        
        
          /E
        
        
          h
        
        
          ≥ 1 for all tested sands at
        
        
          isotropic stress-states, Di Benedetto (2010) also finds ratios
        
        
          E
        
        
          v
        
        
          /E
        
        
          h
        
        
          < 1 for the preparation-methods pluviation and vibration
        
        
          and thus demonstrates a dependency of this ratio on the
        
        
          specimen preparation-method. These discrepancies seem to be
        
        
          due to several factors e.g. the grain-size distribution, the shape
        
        
          of the specimen and the preparation-method.
        
        
          4
        
        
          SUMMARY AND FURTHER HINTS
        
        
          Producing experimental or numerical response envelopes is a
        
        
          convenient tool to investigate a soil’s incremental stress-strain
        
        
          behaviour and to test or compare constitutive equations.
        
        
          The investigation of the incremental stress-strain behaviour
        
        
          of sand at low cycle loading procedures in triaxial testing
        
        
          shows, that for stress-increments Δσ ≤ 50 kPa quasi-elastic
        
        
          behaviour can occur after a low number of cycles. While the
        
        
          influence of the sequence of the stress-paths on the quasi-elastic
        
        
          strains seems to be negligible, a strong influence of the mean
        
        
          pressure p on the size of the strain-response-envelopes is
        
        
          observed.
        
        
          For low number of cycles, the influence of an isotropic
        
        
          prestress on the quasi-elastic strains seems to be negligible so
        
        
          far. There is a stress-induced anisotropy, which can be shown
        
        
          by the rotation of the axes of the ellipses depending on the
        
        
          initial stress-ratio η.
        
        
          Further triaxial tests are necessary in order to investigate e.g.
        
        
          the influence of the void ratio and of a K
        
        
          0
        
        
          -preloading. Because
        
        
          of the role of triaxial extension, further tests in extension region
        
        
          will also be carried out. In addition plastic strains due to low
        
        
          cycle loading will also be investigated; first results are already
        
        
          available.
        
        
          It is known, that some common constitutive models show
        
        
          deficits when predicting deformations due to high and low cycle
        
        
          loading processes, e.g. ratcheting in hypoplasticity, elastic
        
        
          behaviour after the first un- and reloading in elastoplastic
        
        
          constitutive models, missing anisotropy.
        
        
          It is intended to use the results presented in this paper
        
        
          together with future tests as a basis for calibrating and
        
        
          validating more complex constitutive equations especially
        
        
          developed for low cycle loading processes (Ehlers and Avci,
        
        
          2011, Niemunis, et al., 2011).
        
        
          5
        
        
          REFERENCES
        
        
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            1
          
        
        
          
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            Modelling of Granular Materials
          
        
        
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