Arabian Journal for Science and Engineering
https://doi.org/10.1007/s13369-019-04299-3
RESEARCH ARTICLE - CIVIL ENGINEERING
Behavior of Geotextile‑Encased Single Stone Column in Soft Soils
Rowad Esameldin Farah1 · Zalihe Nalbantoglu1
Received: 30 July 2019 / Accepted: 23 December 2019
© King Fahd University of Petroleum & Minerals 2020
Abstract
Stone columns have become a widely used method of increasing bearing capacity of soft soils. This study investigates
floating stone columns with and without encasement in soft soils. Although the stone columns in single-layered soil have
been studied extensively, stone columns constructed in a base of varying soil layers are not fully understood. In the present
study, the behavior of both single-layered soft soil and layered soil consisting of loose sand overlaying the soft soil was
investigated by using small-scale laboratory pilot tests. The bearing capacity of soft soil was improved in all cases of stone
column application. The contribution of stone columns on the bearing capacity of soft soil was presented by the term bearing improvement ratio (BIR). With a non-encased stone column in single-layered soft soil, the BIR was about 3.3-fold and
with geotextile encasement in the same soil, the improvement ratio increased to 3.4-fold. For a non-encased stone column in
layered soils, the BIR was about 2.0-fold and with geotextile enhancement in the same soil, this improvement ratio increased
to 4.0-fold. The inclusion of geotextiles resulted in improved bearing capacity by distributing the induced stresses over larger
areas. The maximum bulging of non-encased stone column in single-layered soft soil was observed at the depth of 1.5 times
the original diameter of the stone column from the top, whereas for encased stone column in single-layered soft soil, the
maximum bulging was transferred to a depth of 3.0 times the original diameter of the stone column.
Keywords Stone column · Column bulging · Floating column · Layered soil · Soft soil · Geotextile
1 Introduction
Structures constructed on soft soils experience problems
such as total and differential settlements, liquefaction, and,
over the long term, instability and poor durability [1–3].
Among a variety of methods used for ground improvement, stone column application is a method widely used to
improve soil conditions [4–9].
Stone columns gain their bearing capacity from their confinement by the surrounding soils. However, stone columns
in very soft soils experience excessive bulging due to very
low lateral confinement by the surrounding soils. Confinement provided by such soils may not be adequate to develop
the required bearing capacity of the stone columns [2, 10].
* Rowad Esameldin Farah
[email protected]
Zalihe Nalbantoglu
[email protected]
1
Department of Civil Engineering, Eastern Mediterranean
University, Via Mersin 10, Famagusta, North Cyprus,
Turkey
Improvement in the bearing capacity of the stone column
can be achieved by the encasement of stone columns by
using geotextiles [11]. The increase in the confinement of
the stone column prevents the squeezing of the stone column
materials into the surrounding soils, reduces the lateral bulging and transfers the loads to deeper layers and thus results
in an increase in the bearing capacity of the stone column
[12, 13]. The higher the confinement provided by the geotextile, the greater the increase in the bearing capacity of
the stone column.
For the improvement of soft soils where the hard stratum
lies at deeper layers, the choice of floating stone columns
may be one of the best options [6]. The literature review
indicated that most of the studies on the performance of
stone columns focus on end-bearing stone columns [14–16].
There has been very limited research performed on the bearing capacity of floating stone columns [14–16]. Hence, in
the present study, small-scale laboratory model tests were
performed to evaluate the effectiveness of floating stone columns with and without geotextile encasement.
Studies in the literature [2, 3, 5] investigated the performance of stone columns in the settlement and bearing
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Arabian Journal for Science and Engineering
capacity of soft single-layered soils. There has been very
limited research conducted on the behavior of stone columns in layered soils [9, 17–19]. However, in reality, footings are usually set in multi-layered soils and understanding the behavior of stone columns in layered soils is very
important for civil engineers [17–21]. In the literature,
the condition of layered soils was generally considered to
be a soft soil overlaying a very soft soil, each of varying
thicknesses [9, 18, 19]. Some studies considered the performance of stone columns in layered soils consisting of
soft soils overlaying a relatively stronger silty soil [9, 18].
After an extensive literature review, it has been observed
that the performance of stone columns in loose sand overlaying a soft soil has not been considered. Therefore, in
the present study, the performance of stone columns in
layered soil consisting of loose sand overlaying a soft soil
was studied in a small-scale laboratory model test tank
with the single stone column at the center and the layered
soil surrounding it. Hasan and Samadhiya [22] stated that
the single granular pile behavior with unit cell concept
simulates the field behavior for an interior pile when large
number of piles is simultaneously loaded. Hughes and
Withers [4] were among the first researchers to analyze
the complex behavior of stone columns. They developed
the unit cell concept to predict the capacity of the stone
columns, where the capacity of a group of stone columns
is equal to the sum of the capacity of the individual columns in the group. In the literature, the existing design
techniques for settlement control related to large group
of stone column configurations are analyzed based on the
performance of an isolated stone column under unit cell
concept [3, 20, 23]. The unit cell model involves a single
stone column and an equivalent circular influence zone
[3]. This approach was found to provide a good correlation with actual observed field behavior for infinite groups
[3, 20].
In the present study, bearing capacity of stone columnimproved ground was designed based on the simplified
geometrical unit cell model approach by considering one
single stone column at the center of the tank and the soft
soil surrounding it.
Stone columns can increase the bearing capacity of soft
soils. Bearing capacity of stone columns is a function of
column arrangement, stone column encasement, length to
diameter ratio, column spacing, etc. Various researchers
performed a series of laboratory tests to evaluate the performance of stone columns on bearing capacity of soft
soils [2–6]. In the present study, the effect of geotextile
encasement on the performance of stone columns in single-layered and layered soils was investigated. To obtain
the degree of improvement achieved, the results were
plotted as bearing improvement ratio and denoted as qr/qu
where qr is the vertical stress of reinforced soil at a given
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settlement and qu is the vertical stress of unreinforced soil
at the same settlement.
The bearing capacity and settlement behavior of a single
stone column is significantly influenced by the method of
applying the vertical load over the stone column [3, 20].
Applying the load through a rigid foundation over an area
greater than the stone column diameter increases the vertical and lateral stress in the surrounding soft soil [3, 20].
The larger bearing area together with the additional support of the stone column results in less bulging and greater
ultimate load capacity of the stone column [20]. Barksdale
and Bachus [20] stated that by applying the load on the
soil–stone column composite, the bearing capacity of the
composite increases to more than the bearing capacity of the
stone column alone. In this study, in order to evaluate the
effectiveness of stone columns in soft soil improvement, the
worst condition was tried to be simulated in the vertical load
application so that the bearing capacity of the stone column
alone could be evaluated. Therefore, in the study, a footing
diameter of 5 cm was used as the same diameter of the stone
column and the vertical load was applied just over the area
of the stone column.
The main objective of this research was to evaluate the
effectiveness of a single stone column in layered soils on
which limited research findings existed in the literature [9,
17–19]. The majority of the laboratory-scale testing carried
out on stone columns referred only to initial compression
and primary consolidation settlement [22–26] with no distinction between initial compression, primary consolidation
settlement, and creep [27]. Within the scope of the present
study, in order to compare the obtained results with the existing findings in the literature, only the initial compression of
the single stone column was measured and the effectiveness
of the stone column in single-layered and layered soil was
discussed.
2 Modelling Considerations
In laboratory conditions, it is quite expensive and time-consuming to test full-scale stone column-reinforced soft soils.
For these reasons, experiments performed in laboratory are
usually limited to observation of the behavior of small models which simulate the actual foundations at a predefined
ratio [28]. The main difficulty in laboratory tests is the scaling effect. Allersma [29] stated that four types of physical
models can be identified according to the scale of the model.
These types are the full-scale field tests, small-scale physical
field tests, small-scale physical laboratory tests (1 g), and
small-scale centrifuge tests. According to Altaee and Fellenius [28], the chief condition for agreement between the
small-scale model and the prototype is that the initial soil
states of both must be at equal proximity to the steady-state
Arabian Journal for Science and Engineering
line. Then, when stresses are normalized to the initial mean
stress, the small-scale model will, in all respects, behave
similarly to the prototype [28]. Altaee and Fellenius [28]
indicated that the soil in the small-scale model can be no
looser than the maximum void ratio of the soil in the prototype and it must not be denser than a value that corresponds
to a prototype soil at the minimum void ratio.
Debnath and Dey [12] defined a similitude ratio as the
ratio of any linear dimension of the prototype to the equivalent dimension of the small-scale model. Debnath and Dey
[12] stated that typically the prototype stone columns have
a diameter (dp) ranging from 0.6 m to 1.0 m and the column
length to diameter ratio (l/dp) varies between 5 and 20 [30].
Muir Wood et al. [31] specified that the particle size of the
aggregates (ds) used in the prototype stone columns range
from 25 mm to 50 mm and the dp/ds ratio varies between
12 and 40.
Within the scope of this study, the small-scale laboratory
model tests were not performed with any particular prototype in mind; rather, the tests were completed as a generic
study. The diameter and the length of the stone column in
the model test setup were designed along the lines exemplified by Debnath and Dey [12]. As well, the particle sizes of
the column aggregates were designed as previously demonstrated by Muir Wood et al. [31]. More details related to the
model design of this study are given in Sect. 3.
3 Experimental Investigation
3.1 Materials Used
3.1.1 Soft Soil
For the model test, soft soil, sand, crushed stone aggregates,
and geotextiles were used as materials. Table 1 introduces
some of the properties of the materials used in this study.
The soft soil has been excavated from a depth of approximately 1 m from the ground surface in Famagusta, North
Cyprus. All the physical and index property tests on the soft
soil were performed according to the American Society for
Testing and Materials (ASTM) standards. The physical and
compressibility characteristics of the soft soil are shown in
Table 1. Test results indicated that the soil did not contain
any organic matter. According to the Unified Soil Classification System (USCS), the soil was classified as silt with high
plasticity (MH).
To create soil samples at different consistencies according to the relationship between consistency and unconfined
compressive strength (UCS), as suggested by Das [39], test
specimens were compacted at standard Proctor compaction
energy with varied water content and UCS tests were performed on these specimens. Test results indicated that the
Table 1 Physical properties of the materials used in the study
Properties
Index properties of soft soil
Fraction of clay size (< 2 μm)a (%)
Fraction of silt size (2–74 μm) a (%)
In situ bulk density, ρbb (g/cm3)
In situ moisture contentb (%)
Specific gravityc, (Gs)
Liquid limitd, LL (%)
Plastic limitd, PL (%)
Plasticity indexd, PI
Compression index, Cc
Rebound index, Cr
Activityd
Soil classificatione
Properties of Bedis sand
Specific gravityc
Maximum dry densityf, ρd(max) (g/cm3)
Minimum dry densityf, ρd(min) (g/cm3)
Internal friction angle, ϕ° at loose state (°)
Uniformity coefficient (Cu)g
Coefficient of curvature (Cc)g
Mean diameter, D50 (mm)
Soil classificatione
Properties of the crushed stone aggregates
Specific gravityc
Maximum dry densityf, ρd(max) (g/cm3)
Minimum dry densityf, ρd(Min) (g/cm3)
Internal friction angle, ϕ° (at 70% relative density) (°)
Bulk density (at 70% relative density), (g/cm3)
Uniformity coefficient (Cu)g
Coefficient of curvature (Cc)g
Mean diameter, D50 (mm)
Soil classificatione
a
Values
48.0
52.0
1.77
30.0
2.65
58.0
30.0
28.0
0.20
0.21
0.58
MH
2.65
1.55
1.46
31.0
1.29
1.06
0.22
SP
2.48
1.61
1.49
46.0
1.57
1.67
0.99
3.00
SP
According to ASTM D 422-98 [32]
b
According to ASTM D 2937-17 [33]
c
According to ASTM D 854-06 [34]
d
According to ASTM D 4318 [35]
e
According to ASTM D 2487-00 (Unified Soil Classification System)
[36]
f
According to Impact method [37]
g
According to ASTM D 2487-06 [38]
soil sample compacted at 33% water content resulted in a
UCS value of 33 kPa. According to Das [39], soil at this
UCS value is determined to be soft.
The bulk density of the soil at the same water content
(33%) was found to be 1.81 g/cm3. In order to achieve the
same soil consistency throughout the tests, all the soil specimens were compacted to this density and water content for
the study.
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Arabian Journal for Science and Engineering
3.1.2 Sand
The sand used in the study was taken from Bedis Beach in
Famagusta, North Cyprus. The properties of the Bedis sand
are presented in Table 1. According to the Unified Soil Classification System, the Bedis sand was classified as poorly
graded sand (SP).
in granular piles is maintained at 400 kN/m, whereas in
laboratory model tests, the tensile strength of geosynthetics
material was within the range of 1.5–20 kN/m [2, 40–42].
In this study, the geotextile material had a tensile strength
of 7 kN/m. The properties of the non-woven geotextile used
in this study are presented in Table 2.
3.2 Experiment Setup
3.1.3 Crushed Stone Aggregate
3.2.1 Model Design
The crushed stone aggregate used in the construction of the
stone columns had sizes ranging between 1 mm and 5 mm.
The properties of the crushed stone aggregate are shown in
Table 1. The particle size distribution of the crushed stone
aggregates, soft soil, and sand are given in Fig. 1.
3.1.4 Geotextile
Non-woven geotextile was utilized to encase and increase
the confinement of material in the stone column. In practice, the tensile strength of geosynthetics materials utilized
Fig. 1 Particle size distribution
of soft soil, sand and crushed
stone aggregates used in the
study
As aforementioned, in the present study, the diameter (d)
and the length (l) of the stone column in the model tests
were designed along similar lines as Debnath and Dey [12]
utilized. The diameter (d) and the length (l) of the stone
column in the model test were 5 cm and 50 cm, respectively.
Therefore, the l/d ratio was 10, placing it in the 5–20 range
as suggested by Debnath and Dey [12]. The particle size of
the stone column aggregates (ds) used in the study ranged
between 1 mm and 5 mm, and the mean particle size diameter (D50) was 3 mm resulting in d/D50 ratio of 17 which
100
90
80
Passing (%)
70
60
50
40
30
20
Soft soil
Crushed stone aggregates
10
0
0.000
Table 2 Properties of the nonwoven geotextile [43–49]
13
Sand
0.001
0.010
0.100
1.000
Particle Size (mm)
10.000
100.000
Test
Standard
Value
Unit
Weight
Thickness (2 kPa)
Tensile strength (longitudinal transverse)
Break extension (longitudinal-cross)
Static puncture
Dynamic puncture
Water permeability, VH50
Visible pore size, O90
EN ISO 9864
EN ISO 9863-1
EN ISO 10319
EN ISO 10319
EN ISO 12236
EN ISO 13433
EN ISO 11058
EN ISO 12956
500
2.7
7
min. 60
2040
10.04
0.034
0.070
gr/m2
mm
kN/m
%
N
mm
l/s * m2
mm
Arabian Journal for Science and Engineering
was in the 12–40 range suggested by Muir Wood et al. [31].
The selected dimensions of the model test in this study fit
the suggested similitude ratio of Debnath and Dey [12] and
Muir Wood et al. [31].
In the model test, the layered soil consists of loose sand
overlaying soft soil. Altaee and Fellenius [28] stated that
physical modelling in sand depends mainly on the initial
mean effective stress and the initial void ratio of the prototype soil. Since there was no specific prototype in mind
and the maximum void ratio of loose sand used in this study
was known, the maximum void ratio of the loose sand was
assumed to be the initial void ratio in the model test.
The physical laboratory model tests performed here were
just a pilot test and were intended to be purely illustrative.
Full understanding of the stone column in soft soils can only
be possible through full-scale tests on prototypes and that is
beyond the scope of the present study.
In previous studies, some researchers [50, 51] stated that
the failure wedge in a foundation bed spreads to within two
to two and half times the footing width from its center. Meyerhof and Sastry [52] noted that the failure zone under rigid
piles reached to a depth two times its diameter. Barksdale
and Bachus [20] noted that bulging depth of the stone column was about two to three times the stone column’s diameter. Considering these previous findings, a circular steel test
tank of 40 cm diameter and 80 cm deep was used in the present study. In order to avoid interference between the chamber wall and the failure wedge, a circular steel plate of 5 cm
diameter was used for loading. The distance of the chamber
walls from the center of the footing was about 20 cm.
Finally, the load-settlement tests were performed sequentially with first the single-layered soft soil then the layered
soil. The load-settlement behavior of the natural (non-reinforced) soft soil bed was tested in the model test tank, and
then, the load-settlement behavior of stone column-reinforced soft bed with and without geotextile was examined.
3.2.3 Preparation of Single‑Layered Soft Soil in the Test
Tank
In the study, the single-layered soft soil bed was placed in
the test tank at 33% water content and 1.81 g/cm3 bulk unit
weight. Before placing the soft soil in the test tank, lubricating oil was applied on the walls of the test tank and a nylon
sheet was placed in order to ease the removal of the soil sample after testing. A sand bed of 5 cm thickness was placed in
the bottom of the test tank for drainage purpose. To achieve
identical soil samples in all tests, the required amount of soft
soil to fill the test tank was calculated and divided into seven
equal layers of 10 cm thickness and placed in the test tank.
After placing the soft soil in the test tank, a circular plate
with the same diameter of the test tank was placed on top
of the soft soil bed surface. To simulate the situation in the
field, a surcharge pressure of 9.05 kPa was applied to the circular plate as in situ overburden pressure to consolidate the
soft soil in the test tank. Two dial gauges with an accuracy
of 0.002 mm were attached to the circular plate to measure
the settlement. The measurement of the settlement was continued until 0.04 mm/day was reached. The consolidation of
the soft soil was completed in 5 days.
3.2.4 Preparation of Layered Soil in the Test Tank
3.2.2 Test Setup and Procedure
The depth of the single-layered soft soil bed in the test tank
was 70 cm. Further explanation of the soft soil preparation
in the test tank is given in Sect. 3.2.3. Floating stone columns with l = 50 cm were used in the study. The diameter
of the stone column was selected to be 5 cm in all tests. A
5-cm-diameter steel auger was utilized to drill the 5-cmcircular hole for the construction of the single stone column
in the test tank. A steel rod of 2 cm diameter was used for
the compaction of the stone column material to reach the
required density. The load was applied via a 5-cm-diameter
circular steel plate with 38 mm thickness. Two linear variable differential transformers (LVDT) were used to measure
the settlement of the loading plate.
For testing the layered soil in the model test tank, 35 cm
of soft soil was placed in the tank and then 35 cm of loose
sand was spread on top of it. Further explanation of this soil
preparation is given in Sect. 3.2.4. The same steps as used
for the single-layered soft soil bed preparation were then
followed.
For the preparation of layered soil, the same procedure was
followed as for the single-layered soft soil. The thickness
of the soft soil and the loose sand were each 35 cm. After
placement and complete consolidation of the soft soil layer,
the sand layer was spread over it. For the placement density
of the sand layer, the minimum index density of 1.46 g/cm3
was utilized as shown in Table 1. Tables 3 and 4 show the
details of the stone columns constructed in the single-layered
soft soil and layered soils in the test tank.
Table 3 Details of the stone columns constructed in the single-layered soft soil
Sample no
Thickness
of soft soil
(cm)
Stone
column
diameter
(cm)
Stone
column
length
(cm)
Geotextile used
1
2
3
70
70
70
–
5
5
–
50
50
No
No
Yes
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Arabian Journal for Science and Engineering
Table 4 Details of the stone
columns constructed in the
layered soil
Sample no
Thickness of
layered soils
(cm)
Layers formation
1
70
A (Top) + B (Bottom)
2
70
A (Top) + B (Bottom)
3
70
A (Top) + B (Bottom)
A = Sand (35 cm in thickness)
B = Soft soil (35 cm in thickness)
3.2.5 Construction of the Single Stone Column
After the placement of the soft soil bed in the test tank,
a cylindrical hole of 5 cm in diameter was made at the
center of the bed using a 5-cm-diameter steel auger. The
internal and external surfaces of a hollow steel pipe were
coated with oil to prevent friction between the pipe and
the surrounding soil. The pipe was vertically set into the
hole to aid the placement of the crushed stone aggregate.
The upright position of the pipe was carefully checked
with a level. The selected relative density of the crushed
stone aggregate was 1.57 g/cm 3 which corresponded to
70% relative density (dense state). The weight of crushed
stone aggregate to be placed in the hole was calculated
according to the chosen relative density (1.57 g/cm3) and
the volume of the hole. To form the floating stone column, the calculated amount of crushed stone aggregate
was divided into five equal batches. Each batch was poured
into the hole and lightly compacted using a 2-cm-diameter
tamping rod until reaching the required height of 50 cm.
The light compaction was performed to avoid lateral deformation during the construction of the stone column. The
tamping rod was dropped 25 times from a height of 10 cm.
For encasement of the stone column with geotextile, the
required area of geotextile was calculated and cut according to the volume of the hole plus 2 cm. The geotextile
was formed into a cylindrical shape with the two edges
overlapping by 2 cm. Then, the fabric of the areas of overlap was bonded together with epoxy which was allowed to
set-up for 24 h. For the encased stone columns, a tubular
steel pipe with a 4 cm outer diameter was used for vertical
insertion of the geotextile into the bored hole. The same
series of procedure and conditions were applied in layered
as were applied in single-layered soils.
After the preparation of the soil and column specimens
in the test tank, the vertical load was applied over the area
of the stone column at a constant rate of 1.2 mm/min up
to 30 mm vertical settlement of the footing. The loading
period was kept short to simulate undrained conditions
during construction. Figure 2 presents the schematic diagram of the single floating stone column in the singlelayered and layered soils used in this study, respectively.
13
Stone column
diameter (cm)
Stone column length
(cm)
Geotextile used
–
5
5
–
50
50
No
No
Yes
After completion of each test, the crushed stone aggregate in the stone column was carefully scooped out and then
a cement paste was poured into the hole to maintain the
shape of bulging formed during loading. After hardening of
the cement paste, the surrounding soil was removed carefully and then the deformed shape of the stone column was
extracted. The diameter of the bulged shape of the stone
column was measured.
4 Results and Discussion
4.1 Bulging Failure of Stone Columns
Figure 3 shows the picture of the stone columns with and
without geotextile encasement in layered soil after loading.
In the present study, in the case of stone column in layered
soil, the bulging failure of the stone column after loading
could not be investigated due to the lack of lateral confinement provided by the loose sand surrounding the stone column. Under the applied loading, the stone column materials
spread out unevenly toward the loose sand and did not show
typical bulging failure. For this reason, the deformed shapes
of the stone column from the hardened cement paste in layered soil could not be obtained. This behavior of the stone
column in loose sand can be seen in Fig. 3a.
Muir Wood et al. [31] stated four modes of deformation
of stone columns: bulging, shearing, punching, and bending.
Single stone columns tend to bulge or punch, depending on
column length, whereas groups of stone columns exhibit
bulging, punching, shearing, and bending [31]. As Nazariafshar et al. [13] stated in single stone column application,
the stresses due to loading around the single stone column
are uniform because the stone column is located at the center
of the loading plate. However, in group of stone columns
since the columns are not located at the center of the loading plate, the induced stresses around the stone columns are
not uniform and the deformations generated are the combinations of bulging and lateral deflection (bending) in the
group of stone columns [13]. Bulging failure usually occurs
based on whether the base of the stone column is floating in
soft soil or resting on a hard layer. In a long stone column
Arabian Journal for Science and Engineering
Fig. 2 The schematic diagram for single floating stone column in; a single-layered soft soil; b layered soil
with a length to diameter ratio over 5, failure occurs due to
bulging [20, 42, 53–56]. In a floating stone column, with a
length to diameter ratio less than 3 (a short stone column),
the ultimate vertical stress is determined by the punching
failure [13, 57]. General shear failure occurs in short stone
columns that rest on hard layers [20, 58]. Some researchers [13, 22, 59] stated that bulging modes of deformation
was the governing failure mechanism in all non-encased
and encased single stone column applications. In the present study, the length to diameter ratio of the encased and
non-encased stone columns was 10 which was greater than 5
and according to some researchers [20, 42, 53–56], the bearing capacity of the encased and non-encased stone columns
was controlled by bulging failure. This statement was in line
with the measured deformed shapes of the stone columns
shown in Fig. 4.
Figure 4 shows the non-dimensional bulging profile for
non-encased and encased floating stone columns in singlelayered soft soil. In the figure, bulging was expressed as a
percentage of the diameter of the stone column (Db − D0)/D0
(%), where Db is the bulging diameter of stone column and
D0 is the original diameter of the stone column. The profile
showed the variation of the non-dimensionalized bulging
with normalized depth (Z/D0), where Z is the total length
of the stone column. According to McKelvey et al. [1], the
axial load transfer from the foundation to the stone column
was higher near the top part of the stone column, whereas,
in the lower part, the stone column carried little loads or
no load transfer. In the present study, for the non-encased
floating stone column, the maximum bulging was found to
occur at a depth of 1.5 times the original diameter of the
stone column from the top of the stone column (7.5 cm),
whereas for encased floating stone column, the maximum
bulging was found to occur at a depth of 3.0 times the original diameter of the stone column from the top (15.0 cm).
The maximum bulging for non-encased and encased floating stone columns were 16.5% and 11.4%, respectively. It
became clear that when the stone column was encased in
geotextile, the maximum bulging depth increased, whereas
the maximum bulging diameter was reduced by about 30%
compared to the non-encased floating stone column. Due to
the additional confinement of the stone column provided by
the geotextile, excessive bulging into the surrounding soft
soil was prevented and the applied axial load was transferred
to deeper layers, resulting in higher bearing capacity of the
encased stone column.
The total length of the non-encased floating stone column
experiencing bulging was found to be within the depth of
0.0–17.5 cm (3.5D0) of the stone column, whereas, in the
encased floating stone column, the total length of bulging
was within the depth of 2.5 cm to 27.5 cm (0.5D0–5.5D0) of
the stone column.
Tables 5 presented the bulging failure for non-encased
and encased floating stone columns. The comparison of
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these findings indicated that the obtained results of the present study were in close agreement with the existing findings
[12, 22, 60].
4.2 Vertical Stress‑Settlement Behavior
In the small-scale laboratory model tests reported in the literature, different settlement values were considered in the
determination of the ultimate vertical stress of the stone column. Some researchers [22, 26] considered the ultimate vertical stress corresponding to 30 mm settlement. Malarvizhi
and Ilamparuthi [61] considered the ultimate vertical stress
at the settlement value corresponding to 10% of the diameter
of the stone column, whereas Debnath and Dey [12] and
Deb et al. [60] determined the ultimate vertical stress corresponded to a settlement of 20% of the diameter of the footing. A comprehensive literature review has shown that there
is no specific standard on this. Hughes and Withers [4] stated
that the ultimate bearing capacity of the stone column was
reached at a vertical displacement of 58% of the stone column diameter, whereas Al-Mosawe et al. [62] found that the
ultimate bearing capacity of the stone column was obtained
at a vertical displacement of 60% of the diameter of the stone
column. In the present study, in order to reach the clear ultimate load in the load-settlement curves of each stone column
application, the loading of the stone column was continued
until 30 mm settlement which was corresponding to 60%
of the diameter of the stone column and the vertical stress
corresponding to this settlement value was considered to be
the ultimate vertical stress of the stone column.
(a)
(b)
Fig. 3 Stone columns in layered soil after loading; a without encasement; b with encasement
Lateral bulging, (Db-D0)/D0) (%)
0
2
3
4
5
6
7
8
9 10 11 12 13 14 15 16 17 18 19 20
1
2
3
4
5
6
7
8
Encased floating stone column
9
10
13
1
0
Depth of stone column /Original diameter of stone
column, Z/D0
Fig. 4 Variation of the nondimensionalized bulging profile
with normalized depth for nonencased and encased floating
stone columns in single-layered
soft soil
Non-encased floating stone column
Arabian Journal for Science and Engineering
Table 5 Bulging failure for non-encased and encased floating stone columns
Stone column
Bulging depth
and
diameter
Present
study
Hasan and
Samadhiya
[22]
Deb et al. [60]
Debnath and Dey [12]
Non-encased
floating stone column
Max bulging depth
5.0 cm from the surface
(1.0 * dstone)
5.82 cm
(1.16 * dstone)
15 cm from the surface
(3 * dstone)
5.57 cm (1.114 * dstone)
(1–1.6) * dstone
1.20 * dstone
–
–
1.24 * dstone
–
–
–
2.84 * dstone
–
–
1.08 * dstone
Max bulging diameter
Encased floating stone column
Max bulging depth
Max bulging diameter
Fig. 5 Vertical stress of stone
columns in single-layered soft
soil with and without encasement
Vertical Stress (kPa)
0
100
200
300
400
500
600
700
800
900
0
5
Settlement (mm)
10
15
20
25
30
Single-layered soft soil
35
40
Non-encased floating stone column
Encased floating stone column column
Figure 5 shows the vertical stress-settlement curves of
stone columns in single-layered soft soil with and without encasement. The ultimate vertical stress value of the
non-encased floating stone column was about 650.4 kPa
at 30 mm settlement. The encased floating stone column
gave higher vertical stress value than the non-encased
floating stone column after attaining 24 mm settlement.
The vertical stress value of this soil at 24 mm settlement
was 640.0 kPa; this value increased further and reached
692.5 kPa at 30 mm settlement. This behavior of the
encased stone column could be explained due to the radial
elongation of the geotextile under increasing loading [2].
As the geotextile expanded further toward the surrounding soil, more interaction between the geotextile and the
surrounding soil was achieved and this resulted in higher
ultimate vertical stress of the encased stone column.
Figure 6 illustrates the vertical stress of the stone columns in layered soil, loose sand overlaying the soft soil
with and without column encasement. It was observed
that the inclusion of non-encased and encased floating
stone columns in soft layered soil enhanced the ultimate
vertical stress. The ultimate vertical stress value of the
non-encased floating stone column was about 90.9 kPa at
30 mm settlement. The same behavior of stress gain was
obtained for the layered soils as was obtained in the singlelayered soft soil. The encased floating stone column produced a higher vertical stress value than the non-encased
floating stone column after reaching 16 mm settlement.
The vertical stress value of this soil at 16 mm settlement
was 189 kPa and then, due to the further expansion of the
geotextile, this value increased and reached to 367.5 kPa
at 30 mm settlement.
13
Arabian Journal for Science and Engineering
Fig. 6 Vertical stress of stone
columns in layered soil with and
without encasement
Vertical Stress (kPa)
0
50
100
150
200
250
300
350
400
450
500
0
Natural layered soil
Non-encased floating stone column
5
Encased floating stone column
Settlement (mm)
10
15
20
25
30
35
The shape of the curves obtained in Fig. 6 for the nonencased and encased floating stone columns in layered soil
were very similar to the one obtained in Fig. 5 for the single-layered soft soil. However, comparison of the values of
the ultimate vertical stresses in single-layered and layered
soils indicated that there was a significant reduction in the
ultimate vertical stress values obtained for the layered soil.
That result could be explained by the presence of loose sand
overlaying the soft soil. Very little confinement provided by
the surrounding loose sand caused a reduction in the bearing
capacity of the layered soil, whereas in single-layered soil,
higher confinement of the surrounding soft soil caused an
increase in the ultimate vertical stress values of the stone
column.
Table 6 Comparison of the
predicted and measured ultimate
vertical stress values of nonencased floating stone column
in single-layered soft soil
Table 6 shows the comparison of the ultimate vertical
stress of non-encased floating stone column in single-layered
soft soil with the existing derived formulas in the literature.
As it can be seen from Table 6, the findings of Hughes and
Withers [4] and Christouls et al. [56] were in good agreement with the present study. For the layered soil condition,
since the same layered soil condition (loose sand overlying
soft soil) was not studied in the literature, no comparison of
the findings was given for this case.
4.3 Bearing Improvement Ratio of Stone Column
To evaluate the efficiency of stone columns on the bearing
capacity of soft soils, the bearing improvement ratio (BIR)
Derived formula
Reference
Predicted value
(kPa)
Measured value
(kPa)
1+sin 𝜙�s
Hughes and Withers [4]
607.0
650.4
Mitchell [63]
Christouls et al. [56]
413.0
660.0
1−sin 𝜙s�
(𝜎r� + 4Cu ) = qult
CuNp = qult
𝜋D×L×Cu
As
= qult
ϕs = Internal friction angle of stone column
𝜎r′ = Effective radial stress
Cu = Undrained shear strength
qult = Ultimate vertical stress of stone column
Np = Bearing capacity factor
D = Stone column diameter
L = Stone column length
As = Stone column area
13
Arabian Journal for Science and Engineering
Fig. 7 BIR of stone columns in
single-layered soft soil with and
without encasement
0
10
20
30
s/D (%)
40
50
60
70
0
Bearing Improvement ratio, BIR (qr/qu)
Encased floating stone column
0.5
Non-encased floating stone
column
1
1.5
2
2.5
3
3.5
4
Table 7 The bearing improvement ratio of stone columns in case of
single-layered and layered soils with and without encasement
Stone column
Single-layered soil
Non-encased floating stone column
Encased floating stone column
Layered soil
Non-encased floating stone column
Encased floating stone column
BIR
(corresponding to
30 mm settlement)
3.29
3.42
2.05
4.04
was presented. The BIR represents the ratio of vertical stress
of reinforced soil at a given settlement to vertical stress of
unreinforced soil at the same settlement (qr/qu).
Figure 7 illustrates the BIR of stone columns in singlelayered soft soil with and without encasement. In the figure,
the corresponding settlement values (s) to bearing improvement ratio were normalized by footing diameter (D) and the
values were given as s/D in percentages. Table 7 gives the
calculated BIRs corresponding to 30 mm settlement. From
the values in Table 7, the BIR of encased floating stone columns was slightly higher than the non-encased floating stone
column.
Figure 8 shows the BIR versus the normalized settlement
curves of stone columns in layered soil with and without
encasement. The BIR values corresponding to 30 mm settlement for non-encased and encased floating stone columns
are also given in Table 7. From the table, it can be seen that
in both cases of soil layering conditions, the BIR values
increased with geotextile encasement of the stone columns.
Compared with the BIR value of the non-encased floating
stone column in single-layered soft soil, the BIR value of
the encased floating stone column in single-layered soft soil
increased by 1.04-fold. The BIR value of the non-encased
floating stone column in layered soil was much lower than
the BIR value of the encased floating stone column in layered soil. With geotextile enhancement, the BIR value of
the encased floating stone column in layered soil increased
by 1.97 times the BIR value of the non-encased floating
stone column in layered soil. The smaller value of the BIR
in non-encased floating stone column in layered soil was due
to the presence of loose sand surrounding the stone column.
The BIR value of the non-encased floating stone column in
single-layered soft soil was approximately 1.60 times higher
than the BIR value of the non-encased floating stone column
in layered soil. This is due to the insufficient lateral confinement provided by the loose sand which caused reduction in
the BIR value of the non-encased floating stone column in
layered soil. These findings indicate the effectiveness of geotextile in the improvement of bearing capacity of the stone
columns. The inclusion of geotextile in the stone column
increased the bearing capacity of both single-layered and
layered soils and resulted in higher BIR values compared to
the BIR values of the non-encased floating stone columns.
5 Conclusions
Based on the small-scale laboratory pilot test results, the
following conclusions were drawn from this study:
13
Arabian Journal for Science and Engineering
Fig. 8 BIR of stone columns in
layered soil with and without
encasement
s/D (%)
0
10
20
30
40
50
60
70
Bearing Improvement ratio, BIR (qr/qu)
0
Non-encased floating stone column
0.5
1
Encased floating stone column
1.5
2
2.5
3
3.5
4
4.5
• The bearing capacity of soft soils has been improved in
all cases of stone column application. The non-encased
stone column increased the bearing capacity of singlelayered soft soil by at most 3.3 times. With geotextile
encasement, the bearing capacity of single-layered soft
soil increased by 3.4 times, whereas, for the non-encased
stone column, the increase in the bearing capacity of
layered soil was found to be 2.0 times and with geotextile encasement, the bearing capacity of layered soil
increased by 4.0 times.
• In single-layered soft soil, the maximum bulging for
non-encased and encased stone columns were 16.5% and
11.4% of the original diameter of stone column, respectively. As compared to non-encased stone column, about
a 30% reduction in the maximum bulging diameter can
be achieved with the provision of an encased stone column.
• The inclusion of geotextile encasement with stone
columns resulted in further improvement of soft soils
by distributing the induced stress over larger areas. In
single-layered soft soil, the maximum bulging depth of
the non-encased stone column was 1.5 times the original diameter of the stone column from the top, whereas,
with geotextile encasement, the maximum bulging depth
increased by 3.0 times the original diameter of the stone
column from the surface.
The present laboratory study evaluated the performance
of single stone column in soft soil under short-term loading
condition. The long-term settlement of the stone column is
one of the research topics to be further studied and it is also
among the ongoing research topics of the authors.
13
Acknowledgements The support is appreciated from civil engineering
department, Eastern Mediterranean University while using the laboratory facilities during the study.
Compliance with Ethical Standards
Conflict of interest The authors declare that they have no conflict of
interest.
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