Driven and jacked piles are widely used in modern building practice, nevertheless, the
mechanisms of pile installation and pile setup in sand still remain unclear or even unexplored at
present. The main objective of this research is to carry out a comprehensive study in order to
enhance understanding on pile installation and pile setup and to determine the involved
micromechanics.
To explore the mechanisms of a driven pile setup in dry sand, model driven pile tests
were carried out in a custom-made pressurized chamber. A bender element system and tactile
pressure sensors were used in parallel to monitor the stiffness and stress changes in the soil
surrounding the pile during the tests. The experimental results demonstrate that pile setup is not
caused by the increase of at-rest radial stress σ
ps', rather, it is mainly attributed to the increase in
radial stress during pile loading Δσ
pf', as a result of soil aging (or creep). Pile installation
pushes the surrounding soil to the side, thereby imposing additional loading on the soil inside
the influence zone. This loading action initiates an associated aging (or creep) process during
the setup period and the aging effects ultimately give rise to an increase in Δσ
pf' and the pile
shaft resistance. The measurements also reveal that the increase in aging-induced soil stiffness
is due to the contact normal forces among soil particles gradually becoming more homogenized
during the setup period. This suggested setup mechanism can explain the absence of pile setup
in bored piles (non-displacement piles) — the loading action induced by the pile installation is
too insignificant to trigger the required aging process. In addition, in a similar logic, it can
elucidate why the setup rate is higher in large-displacement piles than in small-displacement
piles.
To examine the soil responses in terms of the strain and stress distributions, the stress
paths, the movement of particles and contact force mobilization during monotonic jacking, a
three-dimensional simulation of a centrifuge model pile test was performed using the discrete
element method (DEM). The simulation results show great agreement with the measurements
from the centrifuge model pile tests. The distribution of the incremental deviatoric strain dε
q indicates the formation of a shear band in the shoulder of the ‘nose cone’ that is beneath the pile
base. Based on this effect, the soil mass can be divided into three zones, i.e., the ‘nose cone’
(zone I), the shear band (zone II) and the surrounding soil beyond the shear band (zone III). The
distributions of the radial stress σ
r', hoop stress σ
θ', vertical stress σ
v' and shear stress τ
rv' have
different modes and high-gradient distributions of mean stress p' and deviatoric stress q are
found in zone II. As for the stress paths, the surrounding soil experiences four phases in terms
of changes in p' and q during monotonic jacking, and the change in the soil stress state
decreases with increasing distance from the pile centerline. From a microscopic point of view,
the particles in the shear band rotate strongly in similar directions, fully mobilizing the friction
at the associated contacts. This provides a micromechanical explanation for the soil failure
during monotonic jacking.
To explore the mechanisms of friction fatigue for jacked piles in sand, model jacked
pile tests were carried out in a custom-made pressurized chamber. Tactile pressure sensors were
used to monitor the changes in stresses and interparticle contact forces in the soil surrounding
the pile during cyclic jacking. The measurements suggest that the influence of the cyclic
jacking process on the radial and hoop stresses of the surrounding soils at a certain depth can be
categorized into two stages, i.e., Stage-1 where the pile penetration depth z < the transition
depth z* and Stage-2 where z > z*. The transition depth z* is associated with the maximum
stationary radial stress σ
rs' or hoop stress σ
θs' obtained during the whole pile penetration
process. In Stage-1, the values of the stationary radial stress σ
rs', ultimate radial stress σ
ru', and
the difference lΔσ
r'l = lσ
ru' - σ
rs'l continue to increase with increasing penetration depth z. In
Stage-2, the values of σ
rs', σ
ru', and lΔσ
r'l decrease with increasing z and the associated soil
structure gradually becomes unstable. Similar responses are also observed in the measured
hoop stress. It is also found that z* increases linearly with increasing distance from the pile
centreline. Based on these experimental findings, a simple model is proposed to explain
friction fatigue. In response to the continuous jacking cycles and increasing pile penetration
depths, the base gradually reaches the transition depth of the soil elements surrounding the pile
one by one, followed by the elements gradually entering Stage-2. Hence, the soil structure in the nearer zone becomes more unstable, and the associated ultimate radial stresses gradually
decrease, which in turn leads to decreases in the ultimate radial and shear stresses on the pile
shaft, causing friction fatigue.
To examine the mechanisms of the time-dependent behavior, i.e., variations of the pile
residual resistance under a constant head load, the resistance vs pile-head-settlement response
during static compression load tests and pile serviceability performance with time, of jacked
piles in sand, a jacked model pile test and associated DEM simulations were conducted. The
experimental results demonstrate that for the pile under zero head load, the base residual
resistance increases with time. In addition, during the load test, the base resistance Q
b increases
with time at a relatively small settlement but decreases with time at a relatively large
settlement. As to the shaft resistance Q
s, it decreases and increases with time at a relatively
small settlement and relatively large settlement, respectively. Moreover, the corresponding
resistance vs the pile-head-settlement responses reveal a worse serviceability performance with
elapsed time for the piles mainly supported by the base resistance and a better serviceability
performance with elapsed time for the piles mainly supported by the shaft resistance. The DEM
simulation results demonstrate different modes of particle movement and changes in the
vertical stress in the soil during aging for various magnitudes of the head load. This behavior in
the soil is related to the variations of the resistances applied on the pile. Ultimately, the
consistency between the experimental and DEM simulations demonstrates that the
micromechanical initiation mechanism of all the aforementioned time-dependent behavior
appears to be microfracturing at the contacts leading to friction reduction and packing
re-equilibrium.
Post a Comment