 
          3422
        
        
          Proceedings of the 18
        
        
          th
        
        
          International Conference on Soil Mechanics and Geotechnical Engineering, Paris 2013
        
        
          when temperature rises up suddenly, and then it will decrease
        
        
          with time even though the temperature is increasing. The
        
        
          highest value of EPWP is up to 3MPa. The increase of EPWP is
        
        
          due to the fact that thermal expansion coefficient of water is
        
        
          much higher than that of rock. Owing to the low permeability of
        
        
          rock, drainage is slow and the pore water expansion is impeded,
        
        
          resulting in the EPWP increase at the beginning. At later time,
        
        
          as mentioned above, migration of water from the heat source is
        
        
          gradually accelerated due to the increase of permeability,
        
        
          allowing pore pressure to dissipate.
        
        
          heater
        
        
          heater
        
        
          heater
        
        
          Figure 9. Variation of deformation at different position
        
        
          At the same time, heat-induced deformation is also
        
        
          investigated. Figure 9 shows the calculated and test results at
        
        
          different positions. It is found that the calculation can describe
        
        
          the change of the deformation qualitatively if compared with the
        
        
          test data. The deformation of the rock near the heater is
        
        
          expansive; while the deformation of the rock far away from the
        
        
          heater is contractive. It is very easy to understand that the rock
        
        
          may behave expansive due to the significant increase of
        
        
          temperature; nevertheless, the change of temperature at the
        
        
          places far away from the heater is rather. Therefore, the dilation
        
        
          of the rock far away from the heater is very small compared
        
        
          with the rock in the vicinity of the heater. As the results,
        
        
          swelling force caused by the expansion of the rock near the
        
        
          heater will cause contraction of the rock far away from the
        
        
          heater.
        
        
          4 CONCLUSIONS
        
        
          In the paper, the following two conclusions can be made:
        
        
          a) An isotropic element heating test is simulated by the
        
        
          proposed THM analysis based on an elasto-viscoplastic
        
        
          model. The calculation can well explain the phenomenon
        
        
          observed in the test that the heat-induced volumetric strain
        
        
          measured by water discharge changes from contraction to
        
        
          dilation with the increase of OCR in isotropic heating
        
        
          process. In the calculation with THM analysis, soil
        
        
          skeleton is always dilative with the increase of temperature
        
        
          regardless of what kind of OCR may be. The discharge of
        
        
          the water is just caused by different thermal expansion
        
        
          properties of the soil and the water! In a word, this
        
        
          phenomenon is merely a boundary value problem with
        
        
          soil-water interaction, not an inherent property of the rock
        
        
          itself!
        
        
          b) A field test of heating process (Gens, 2007) is also
        
        
          simulated with the same THM analysis based on the same
        
        
          elasto-viscoplastic model. It is found that the proposed
        
        
          numerical method can well describe the THM behavior,
        
        
          such as, the temperature change, the change of EPWP and
        
        
          the heat-induced deformation.
        
        
          5 REFERENCES
        
        
          Baldi G, Hueckel T and Pelegrini R (1988): Thermal volume changes of
        
        
          the mineral-water system in low-porosity clay soils,
        
        
          
            Canadian
          
        
        
          
            Geotechnical Journal
          
        
        
          , Vol. 25, 808-825
        
        
          Cekerevac C. and Laloui L. (2004): Experimental study of thermal
        
        
          effects on the mechanical behavior of a clay,
        
        
          
            International journal
          
        
        
          
            for numerical and analytical methods in geomechanics
          
        
        
          , Vol. 28,
        
        
          209-228
        
        
          Cui Y. J., Le T. T., Tang A. M., Delage P. and Li X. L. (2009):
        
        
          Investigating the time-dependent behavior of Boom clay under
        
        
          thermomechanical loading,
        
        
          
            Getechnique
          
        
        
          , 59, No. 4, 319-329
        
        
          Gens A., Vaunat J., Garitte B. and Wileveau Y. (2007): In situ behavior
        
        
          of a stiff layered clay subject to thermal loading: observations and
        
        
          interpretation,
        
        
          
            Geotechnique
          
        
        
          , Vol.57, No.2, 207-228
        
        
          Jia Y., Wileveau Y., Su K., Duveau G. and Shao J. F. (2007): Thermo-
        
        
          hydro-mechanical modeling of a situ heating experiment,
        
        
          
            Geotechnique
          
        
        
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          Zhang S. and Zhang F. (2009): A thermo-elasto- viscoplastic model for
        
        
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