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6.8 Discussions
6.8.1 Stress path and time dependent behaviour
The stress path of the soil at P1 in test Ts5 simulated by CRISP is shown in
Figure 6.21. Comparing to Figure 6.11, the stress path at the same position for
test To1 is different. As mentioned in Section 4.2.2, the draining rate of zinc
chloride solution in To1 is 50 mm/min. which is equal to a rate of 0.72 m / day
in prototype scale. Such relatively fast excavation rate make the soil behaviour
essentially undrained. The subsequent soil expansion causes the negative excess
pore water pressure to increase significantly. In the mean time, the dissipation
of such excess pore pressure is slow due to the low permeability of clay. Hence,
the stress path goes up vertically, yielding and finally fail as shown in Figure
6.11. The undrained condition of test To1 is indicated by stress path shown by
the failure pattern in Figures 4.8 and 4.12.
In contrast, for the CRISP analysis on test Ts5, the excavation rate is about
9 mm/min which is 0.13 m/day in prototype scale. It is a typical excavation
process which is much slower than that of test To1. The corresponding magnitude
of deformation of soil is also much smaller than those of test To1. In this
case, the built-up of negative excess pore pressure is not as significant when
compared to test To1. For this reason, the stress path in the analysis of test
Ts5 shows a different trend ( Figure 6.21) compared to test To1(Figure 6.11). A
partially drained condition is obtained by the reduction of mean normal
effective stress due to the dissipation of negative excess pore pressure in a
slow excavation work. In conventional engineering practices, typical fully
undrained or fully drained condition are normally idealised in most simplified
analyses. The undrained condition generally under estimates the wall deflection
and ground settlement as the dissipation of negative pore pressure is ignored.
In contrast, drained condition is over estimating the soil movements, and is
more commonly used especially for the long term trend. The real situation is
between these two cases and a better prediction should be modelled by
considering excavation rate and the permeability of the soil.
The CRISP program, using coupled consolidation analysis, are able to handle
such time dependent problem. The preliminary comparison between the experiment
and FEM results shows good agreement and confirms this.
6.8.2 Comparison between the FEM and centrifuge tests
By comparing the results between the FEM and
centrifuge tests, it can be found that the surface ground settlement measured in
centrifuge tests decreases sharply with distance away from excavation which is
in agreement with the behaviour in the field. Typical ground settlement
profiles from centrifuge tests, field observation and from FEM are illustrated
in Figures 6.23 and 6.24. At a distance of 2 times the
excavation depth away from the wall, settlement from FEM is about 10-30% larger
than that from centrifuge and field measurements. This can be considered as
within an acceptable range in design. At a distance further away from the
excavation, difference in settlement between the FEM and centrifuge test results
becomes larger.
6.8.3 Effects of small strain behaviour
Recently, there is an increasing awareness that the soil stiffness at very
small strain is actually much higher than the stiffness obtained from
conventional triaxial testing (Simpson et al. (1979), Jardine et al. (1986),
Burland (1989) and Simpson (1992). As FEM adopted the soil parameters obtained
from triaxial tests, which is a large strain testing, the stiffness used in the
analysis for soil far away from the wall may be too small. Due to this, the
deformation from FEM is considerably larger then the experimental results. A
fact recognised by many engineers now. This aspect looks increasingly important.
6.8.4 Effects of boundary condition, shear slip surface and interface
Some differences are indicated as shown in Figure 6.23 by comparing the
surface settlement profile from centrifuge to that from FEM, which influence the
accuracy of the estimation on the surface settlement. First, the small strain
effect as discussed in the last section is not properly modelled in FEM, as
shown in the Figure 6.23. Second, the existence of a shear slip surface observed
in the centrifuge model tests obviously influenced the soil movement field near
to the retaining wall. The shear band reflecting the discontinuity of the soil
cannot be simulated perfectly by the continuum model in FEM. Third, the
condition of the right boundary of the mesh will also affect the settlement
profile especially the profile near to the boundary. In Figure 6.20, the right
boundary was fixed in vertical direction. In contrast, Figure 6.22 gives the
surface settlement profiles when this right boundary is allowed to move freely
in the vertical direction. The difference of such effect between the free and
fixed conditions is mainly near the boundary and can be reduced effectively by
extending the mesh far enough towards the right.
The incorrect simulation of the interface condition between soil and
diaphragm can be clearly seen in the analysis as explained in Section 6.7.4. Due
to a lack of information and understanding of the behaviour of interface
element, such effect is frequently ignored in engineering practice. The previous
analyses conducted without considering the interface condition, highlighted such
an effect. To verify the improvement in trend if an interface element is
included, another analysis was conducted using the slip element provided in
CRISP. Slip elements are provided along the entire retaining wall on the active
side, but not the passive side. The use of interface elements also on the
passive side and wall toe produce numerical instability which is beyond the
scope of the present study to solve. Figure 6.24 shows an improved simulation of
the ground surface settlement profile when such soil-structure interface
elements are used along the model diaphragm wall. Figures 6.25 and 6.26 give
some detail comparisons to show the effect of interface and boundary condition
on surface settlement profile at excavation depth 50 mm and long term after
excavation, respectively. Soil-structure interface elements used along the model
diaphragm wall effectively increase the settlement near the retaining wall and
reduce the over-estimation of surface settlements further away from the wall.
This resulted in a significantly improved trend of the predicted ground
movement. The parameters of the interface elements used in the analysis are
shown in Table 6.3. This preliminary simulation is just to indicate this effect
and further study on the interface behaviour is still needed.
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