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www.elsevier.com/locate/jterra
TerramechanicsJournal of Terramechanics 41 (2004) 25–40
Mechanical properties in relationto vehicle mobility of Sepang peat
terrain in Malaysia
Ataur Rahman *, Azmi Yahya, Mohd. Zodaidie, Desa Ahmad,Wan Ishak, A.F. Kheiralla
Faculty of Engineering, University Putra Malaysia, 43400 UPM Serdang Selangor DE, Malaysia
Abstract
An analytical framework for determining the mechanical properties of peat and predicting
the tractive performance of tracked vehicle is presented. It takes into account the load-sinkage
and shearing characteristics of peat as well as all major design parameters of tracked vehicle.
An experimental study on the mechanical properties of peat soil was conducted at Sepang
area, Selangor, Malaysia. The stiffness values of surface mat and underlying weak peat deposit
from load-sinkage test were determined by specially made bearing capacity apparatus. The
mean values of surface mat stiffness before and after drainage were found to be 31 and 45.62
kN/m3, respectively and the mean values of underlying peat stiffness before and after drainage
were found to be 252 and 380.20 kN/m3, respectively. The mean value of the internal frictional
angle, cohesiveness and shear deformation modulus of the peat soil sample were determined
using a direct shear box apparatus in the laboratory. The mean values of internal friction
angle, cohesiveness and shear deformation modulus before and after drainage were found to
be 22.80� and 24.31�, 2.63 and 2.89 kN/m2, and 1.21 and 1.37 cm, respectively.
� 2004 ISTVS. Published by Elsevier Ltd. All rights reserved.
Keywords: Peat; Bearing capacity; Shear deformation modulus; Shearing stress; Internal frictional angle
and cohesiveness
*Corresponding author.
E-mail address: [email protected] (A. Rahman).
0022-4898/$20.00 � 2004 ISTVS. Published by Elsevier Ltd. All rights reserved.
doi:10.1016/j.jterra.2004.01.002
26 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
1. Introduction
The key to off-road vehicle performance prediction lies in the proper evaluation of
the mechanical properties of the terrain. Peat terrain deformation due to track
motion is dependent upon the applied forces as discussed by Chang and Bekker [1].
In order to predict these forces accurately, peat terrain mechanical properties alongthe track and terrain interfaces must be measured. Peat covers a significant portion
of the plantation land of Malaysia. There are about 2.8 million ha of peat in Ma-
laysia accounting for about 8% of the total land area of the country. Sarawak has the
largest area of peat in the country. This is followed by Peninsular Malaysia which
has about 984,500 ha, comprising 7% of its total area, while Sabah 86,000 ha, rep-
resent 1% of the state [2]. Large tracks of peat lands are being converted for oil palm
plantations as a result of global increase of oil palm demand. At the moment, there is
no appropriate vehicle on the mechanization of oil palm in peat land of Malaysia. Toevaluate the vehicle mobility over this type of terrain, it is important to develop
appropriate methods for identifying and measuring those mechanical properties of
peat that are considered to be relevant to vehicle mobility. To properly identify the
mechanical properties of peat terrain from an off-road vehicle mobility viewpoint,
measurement need to be taken under loading conditions similar to those exerted by a
vehicle. The vertical load that an off-road tracked vehicle exerts on the peat terrain
results in sinkage. A special plate sinkage apparatus has been designed and devel-
oped to evaluate the load-sinkage parameter. Furthermore, an off-road tracked ve-hicle applies horizontal load to the peat terrain surface through its running gear and
this results in the development of shearing strength and associated slip. The digital
shear vane was used in situ to evaluate the shearing strength of the peat terrain. The
digital direct shear box apparatus was used to evaluate the shearing parameters of
peat terrain such as peat cohesiveness, internal frictional angle, shear displacement
and shear deformation modulus.
This paper represents the experimental results on the determination of cohesive-
ness, internal friction angle, shear deformation modulus, vane shearing strength,surface mat stiffness and underlying stiffness of peat and track vehicle tractive per-
formance on peat terrain. Shear deformation model equation by Wong et al. [3] was
used to compute the shear deformation modulus of peat while the pressure-sinkage
model equation by Wong et al. [4] was used to compute the surface mat stiffness and
underlying stiffness of peat.
2. Materials and methods
2.1. Test site
Field tests were carried out at Sepang peat area, located about 45 km from Kuala
Lumpur, Malaysia. The area was heavily infested with palm roots, low shrubs,
grasses, and sedges as shown in Figs. 1 and 2. The field conditions were wet and the
water table was found to be 0–12 cm below the surface level. The surface mat and the
Fig. 1. Tested site before drainage.
Fig. 2. Tested site after drainage.
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 27
peat deposit thickness were not distinct by visual observation. The surface mat
thickness was about 5 to 25 cm at the center location between adjacent palm rowsand 10–35 cm at the palm tree location. The underlying peat deposit thickness for the
whole area was about 50 to 100 cm. The water field capacity was almost at saturation
level and walking on such a terrain condition was only possible with the use of a
Fig. 3. Bearing capacity measuring scenario.
28 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
special made wooden clog as shown in Fig. 3. The dominant features of this site may
be described as high water content and weak underlying peat that could easily bedisturbed by vehicle movements. The overall area was divided into three equal area
blocks and each block was again divided into three equal sub-blocks. Peat moisture
content, bulk density, cohesiveness, internal friction angle, shear deformation
modulus, vane shearing strength, surface mat stiffness, and underlying stiffness of
peat were determined. In situ determinations for vane shearing strength, surface mat
stiffness, and underlying stiffness were carried out at 10, 25 and 40 cm depth in triplet
replications at the center location between adjacent palm rows within each sub-block
in the field during un-drained and drained conditions. Similarly, undisturbed sampleof 216 cm3 volume were taken at the mentioned depths and points in the fields in
triplet replications for the determinations of moisture content, bulk density, cohe-
siveness, internal friction angle, shear deformation modulus of peat. The samples
were wrapped with aluminum foil and sealed in a plastic container before they were
immediately taken to the laboratory for the relevant analysis.
2.2. Cohesiveness, internal friction angle, and shear deformation modulus
A Wykeham Farrance 25402 shear box apparatus as shown in Fig. 4 was used to
determine cohesiveness, internal friction angle, and bulk deformation modulus of
peat. The apparatus was setup to run at a shear rate of 0.25 mm/s and a maximum
shear displacement of 12 mm. Prior to the actual shear test, the prepared test sample
in the rectangular box was subjected to a consolidation load of 1 kg for 24 h.
Readings on the shear displacement in cm and shearing stress in kN/m2 were
Fig. 4. Wykeham Farrance 25402 shear box apparatus.
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 29
recorded every minute until failure on the sample. The same test procedure was
repeated for the consolidation load of 1.5 and 2 kg, and again repeated on samples
taken from different depths, different sampling points, and different drainage
conditions.
The shear deformation modulus of peat was determined by using the equation
proposed by Wong et al. [3]:
K ¼ �P
1� ssmax
� �2
j2
P1� s
smax
� �2
j ln 1� ssmax
� �h i ; ð1Þ
where, K is shear deformation modulus in cm, smax is maximum shearing stress inkg/cm2, s measured shear strength in kg/cm2 and j is corresponding shear strength
in cm.
The relationship between normal stress and shearing stress of peat for different
samples is shown in Fig. 5. From the interpretation of normal strength and shearing
strength, the cohesiveness and the internal frictional angle of peat were computed.
Information of shear deformation modulus, cohesion, and internal frictional angle
could be used in the computation of traction, engine power, drawbar power and
tractive efficiency of a vehicle.
2.3. In situ shearing strength
A RMU I012 digital vane test apparatus shown in Fig. 6 was used to determine
the in situ shearing stress of peat. The apparatus comprises a set of hollow rods for
Fig. 5. (a) Typical trend of shearing stress versus shear displacement (b) typical trend of strength stress
versus normal stress.
Fig. 6. RMU I012 digital vane shear test apparatus.
30 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
holding the vane blade, a twisting instrument on the upper end for twisting the rod
set, and a digital measuring gearbox for measuring the twisting torque. The digital
measuring gearbox is powered by 12 V DC battery Three vane blades having a di-
ameter of 4.4, 5.4 and 6.4 cm were used to shear the peat. This apparatus was setupto run at a twisting torque ranging from 500 to 600 kg cm at an accuracy of 1 kg cm
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 31
resolution. Prior to the actual test, the digital measuring gearbox was calibrated.
During the operation of the apparatus for the shear test, the twisting instrument was
rotated at a speed of 12 �/s to shear the peat. Reading on the twisting torque was
recorded for every 7.5 s until a complete 360� rotation. The maximum twisting
torque of a complete 360� rotation was recorded. The measured value was later used
to compute the shearing stress of the peat. The same test procedure was repeated fordifferent depths, different blades with diameter of 5.4 and 6.4 cm for different sam-
pling points, and different drainage conditions.
The shearing strength of the peat in situ can be calculated using the following
equation:
sf ¼3T
2pr2ð2r þ 3HÞ ; ð2Þ
where, sf is shearing stress in kN/m2, T is torque in kg cm, r is radius of the shear
vane in cm, and H is height of the shear vane in cm.
2.4. Surface mat stiffness and underlying stiffness of peat
A special developed apparatus as shown in Fig. 7 was used to determine the
surface mat stiffness and underlying stiffness of peat. The apparatus comprises of aproof ring with a dial gauge for measuring the force, a shaft with diameter of 1.59 cm
Fig. 7. Bearing capacity measuring apparatus.
32 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
and with length of 45 cm for transferring load to sinkage plate and a rectangular
plate with size of 15� 5� 0.5 cm for measuring the sinkage. Three sinkage plates
having a diameter of 10 and 15 cm and a size of 15� 5 cm were used to determine
the stiffness of peat. This apparatus was setup to run at a proving ring constant of
0.2 kg/division. It was operated manually to determine the stiffness of peat.
Prior to the actual stiffness test, the proof ring dial gauge was calibrated. Duringthe operation of the apparatus for the stiffness test, the long shaft with sinkage plate
diameter of 10 cm was manually pushed down at a approximately speed of 2.5 cm/s
to sink the plate. Reading on the pushing load in kg and sinkage in cm was recorded
for every 2 cm plate sinkage. The measured value was later used to plot a graph as
shown in Fig. 8. The parameter characterizing the behavior of the surface mat that is
represented by ‘m’ was determined from the slope of the Fig. 8 regression line. The
same test procedure was repeated for sinkage plates with diameter of 5.4 and 6.4 cm,
for different sampling points, and different drainage conditions.Surface mat stiffness and underlying stiffness of peat was determined from the
following equation of Wong [5]:
p ¼ 1
100½kpzþ mkpz2ðL=AÞ�; ð3Þ
with
mm ¼ mkp;
where, p is load applied on the handle of the apparatus in kN/m2, A is area of the
plate in m2, L is perimeter of the plate in m, z is sinkage in m, kp is stiffness of the peatin kN/m3, m is a parameter characterizing the behavior of the mat, and mm is surface
mat stiffness in kN/m3.
A split-plot completely randomized block design was adopted in statistical
analysis to reveal the effect of field drainage conditions, on depths, normal loads,vane blade size, and plate sinkage, on cohesiveness, internal friction angle and shear
deformation modulus, and on surface mat stiffness and underlying stiffness of peat.
The effect of field drainage conditions, depths, normal loads, vane blade size, and
plate sinkage at significant (Pr < 0:01) level is considered to be highly significance.
Fig. 8. Typical load-sinkage trend of peat for (a) un-drained and (b) drained.
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 33
3. Results and discussion
3.1. Cohesiveness, internal friction angle, and shear deformation modulus
Shearing stress of peat for un-drained and drained conditions at depths of 10, 25
and 40 and at normal load of 1, 1.5, and 2 kg are shown in Table 1. Typical graph ofconsolidation and shearing stress versus shear displacement is shown in Figs. 9 and
10. Mean shearing stress of peat increased from 14.03 to 16.22 kN/m2 when the field
condition was changed from un-drained to drained.
The following observations were made based on Table 1:
• Before drainage: Shearing stress of the peat soil was increased from 10.68 to 13.63
kN/m2 (decrement of 27.62%) and 10.68–17.79 kN/m2 (decrement of 65.54%)
when the normal stress increased from 2.725 to 4.08 and 2.725 to 5.45 kN/m2,
respectively.• After drainage: Shearing stress of the peat soil was increased from 12.8 to 15.34
kN/m2 (decrement of 19.8%) and 12.8 to 20.48 kN/m2 (decrement of 60.0%) when
the normal stress increased from 2.725 to 4.08 kN/m2 and 2.725 to 5.45 kN/m2,
respectively.
From the analysis of variance it was found that the mean effect of field condition,
depth, normal stress, and the interaction of depth and field condition on shearing
strength of peat are highly significant. The significant (Pr < 0:01) effect of field
condition, depth, and normal stress indicate that the shearing strength of the peatsoil was increased and thus may be due to the draw down of the water table by
drainage. The draw down of the water table resulted in increased consolidation of
the fill and other soft underlying materials. Result from least significance difference
(LSDðPr<0:05Þ) shows that the mean value of the shearing strength increased from
15.15 to 16.13 kN/m2 and decreased from 15.15 to 13.907 kN/m2 when the depth
increased from 10 to 25 and 25 to 40 cm, respectively. Result from LSDðPr<0:05Þ shows
that the mean value of the shear strength increased from 11.14 to 14.34 and 14.34
to 19.14 kN/m2 when the normal load increased from 1 to 1.5 and 1.5 to 2 kg,respectively.
Cohesiveness, internal friction angle, and shear deformation modulus of peat for
un-drained and drained conditions at depths below 10, 25, and 40 cm are shown in
Table 2. Mean cohesiveness increased from 2.65 to 2.89 kN/m2, mean internal
friction angle increased from 22.33� to 23.76�, and mean shear deformation modulus
decreased from 1.16 to 1.14 cm when the field condition was changed from un-
drained to drained.
The following observations were also made based on Table 2:• Before drainage: Mean cohesiveness of peat decreased from 3.37 to 2.75 and 2.75
to 1.77 kN/m2, mean internal friction angle of peat decreased from 26.16� to
23.78� and 23.78 to 18.71�, and mean shear deformation modulus of peat in-
creased from 1.12 to 1.17 and 1.17 to 1.19 cm when the depth increased from
10 to 25 and 25 to 40 cm, respectively.
• After drainage: Mean cohesiveness of peat decreased from 3.59 to 3.13 and 3.23 to
1.95 kN/m2, mean internal friction angle of peat decreased from 28.43� to 25.11�
Table 1
Variation of the shearing strength of peat in laboratory analysis
Depth (cm) Normal
stress
(kN/m2)
Shearing strength (kN/m2)
Block 1 Block 2 Block 3 Mean value Increased (%)
Before
drainage
After
drainage
Before
drainage
After
drainage
Before
drainage
After
drainage
Before
drainage
After
drainage
)10 2.725 10.32 11.41 13.7 15.1 9.66 11.74 11.23 12.75 13.53
4.0875 11.30 13.01 17.7 18.05 12.04 13.23 13.68 14.76 7.89
5.45 15.14 17.27 23.47 25.0 16.17 18.54 18.26 20.27 11.00
)25 2.725 10.89 12.0 13.14 13.75 11.04 14.1 11.69 13.28 13.60
4.0875 17.15 17.68 16.44 16.28 13.2 15.69 15.59 16.55 6.15
5.45 19.01 21.2 20.18 22.85 18.3 20.21 19.16 21.42 11.76
)40 2.725 9.0 12.2 9.39 11.5 9.00 13.4 9.13 12.37 35.48
4.0875 11.79 16.4 11.79 13.0 11.23 14.9 11.62 14.77 27.10
5.45 16.26 21.08 18.63 21.15 13.0 17.10 15.96 19.78 23.93
34
A.Rahmanet
al./JournalofTerra
mech
anics
41(2004)25–40
Fig. 9. Typical consolidation test of peat, (a) un-drained and (b) drained.
Fig. 10. Example of shearing stress variation with shear displacement (a) un-drained and (b) drained.
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 35
and 23.78 to 19.39�, and mean shear deformation modulus of peat increased from
1.1 to 1.14 and 1.14 to 1.18 cm when the depth increased from 10 to 25 and 25 to
40 cm, respectively.
3.2. In situ shearing strength
Shearing stress of peat for un-drained and drained conditions at depths of 10, 25,and 40 cm are shown in Table 3. Typical trend of in situ shearing stress variations
with depth for peat under drained and un-drained field conditions are shown in Fig.
11. Mean shearing stress of peat increased from 1.96 to 2.29 kN/m2 when the field
condition was changed from un-drained to drained. Furthermore, mean shearing
strength of peat decreased from 2.86 to 2.167 kN/m2 (decrement of 24.23%) and
2.167 to 1.78 kN/m2 (decrement of 17.85%) with increasing the vane blade size from
4.4 to 5.4 and 5.4 to 6.4 cm, respectively.
The following observations were also made based on Table 3:
Table 2
Variation of the cohesiveness, internal friction and shear deformation modulus of peat
Depth
(cm)
Block 1 Block 2 Block 3 Shear de-
formation
modulus
(cm)
Cohesiveness
(kN/m2)
Internal
frictional
angle (�)
Cohesive-
ness (kN/
m2)
Internal
frictional
angle (�)
Cohesive-
ness (kN/
m2)
Internal
frictional
angle (�)
)10 5.06 27.22 4.37 23.05 4.68 28.22 1.46
)25 3.33 17.66 2.64 21.5 3.48 24.18 1.31
)40 1.57 18.45 1.36 18.08 2.38 19.6 1.26
Table 3
Variation of the in situ shear shearing stress of peat with depth
Depth
(cm)
Vane
blade size
(cm)
Shearing strength, kN/m2
Block 1 Block 2 Block 3
Before
drainage
After
drainage
Before
drainage
After
drainage
Before
drainage
After
drainage
)10 D ¼ 4:4 1.99 4.08 3.77 2.83 3.77 4.48
D ¼ 5:4 1.53 2.21 2.38 3.23 2.72 3.91
D ¼ 6:4 1.53 1.74 1.94 2.14 2.04 2.24
)25 D ¼ 4:4 1.88 2.38 2.09 2.18 1.86 2.98
D ¼ 5:4 1.98 2.30 1.80 2.12 2.52 2.86
D ¼ 6:4 1.34 1.52 1.49 2.10 1.78 2.186
)40 D ¼ 4:4 1.57 2.59 1.77 1.98 1.57 1.84
D ¼ 5:4 1.41 1.63 1.45 1.51 1.80 2.21
D ¼ 6:4 1.73 1.48 1.61 1.68 1.67 2.14
Fig. 11. Typical trend of shearing stress versus depth, (a) un-drained and (b) drained.
36 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 37
• Before drainage: Shearing stress of the peat soil was deccreased from 2.41 to 1.86
and 1.86 to 1.62 kN/m2 when the depth increased from 10 to 25 and 25 to 40 cm,
respectively.
• After drainage: Shearing stress of the peat soil was decreased from 2.98 to 2.29
and 2.29 to 1.89 kN/m2 when the depth increased from 10 to 25 and 25 to 40
cm, respectively.From the analysis of variance it was found that the mean effects of field condi-
tions, depth, and blade size has high significant effect (Pr < 0:01) on in situ shearing
stress of peat. Result from LSD (Pr < 0:05) shows that mean shearing stress was
increased from 1.96 to 2.58 kN/m2 when the field condition was changed from un-
drained to drained. It may be due to the increase of consolidation rate. Result from
LSD (Pr < 0:05) shows that mean in situ shearing stress of peat decreased from 2.90
to 2.13 and 2.13 to 1.78 kN/m2 when the depth increased from 10 to 25 and 25 to 40
cm, respectively. It may be due to the draw down of the water table.
3.3. Surface mat and underlying stiffness of peat
Surface mat stiffness of peat for un-drained and drained conditions at depth of 10,
25, and 40 cm are shown in Table 4. Mean surface mat stiffness of peat increased
from 27.07 to 44.51 kN/m3 for plate with diameter of 10 cm, 33.93 to 41.79 kN/m3
for plate with diameter of 15 cm, and 32.54 to 50.57 kN/m3 for plate with size of
15� 5 cm when field condition was changed from un-drained to drained.The following observations were also made based on Table 4:
• Before drainage: Mean surface mat stiffness of peat decreased from 41.35 to 33.87
kN/m3 and 33.87 to 18.31 kN/m3 when the depth increased from 10 to 25 and 25
to 40 cm, respectively.
• After drainage: Mean surface mat stiffness of peat decreased from 61.32 to 50.2
and 50.2 to 25.321 kN/m3 when the depth increased from 10 to 25 and 25 to 40
cm, respectively.
Table 4
Variation of the surface mat stiffness of peat with depth
Sinkage
(cm)
Plate size
(cm)
Surface mat stiffness, mm (kN/m3)
Block 1 Block 2 Block 3
Before
drainage
After
drainage
Before
drainage
After
drainage
Before
drainage
After
drainage
)10 D ¼ 10 31.2 52.46 40.21 59.49 34.01 49.4
D ¼ 12 57 59.77 40.89 54.85 44 43
L�B¼ 15� 5 41.4 66.76 39.54 97.68 43.88 68.5
)25 D ¼ 10 22.5 56.76 50.87 67.68 12.5 46.5
D ¼ 12 37.67 39.21 53.91 54.86 13 33.4
L�B¼ 15� 5 44.01 52.4 50.29 48.73 20.12 52.28
)40 D ¼ 10 15.76 23.8 26.44 30.43 10.12 14
D ¼ 12 15.01 36.68 34.69 37.86 9.2 16.32
L�B¼ 15� 5 15.71 24.85 24.01 27.57 13.90 16.4
38 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
From the analysis of variance it was found that the main effect of sinkage, field
condition and the interaction of sinkage, field condition and plate size significantly
effect peat surface mat stiffness. The significant effect of sinkage indicates that surface
mat stiffness decreased with increase of sinkage. Result from LSDðPr<0:05Þ shows that
mean surface mat stiffness decreased from 51.336 to 42.043 and 42.04 to 21.831 kN/
m3 when sinkage increased from 10 to 25 and 25 to 40 cm, respectively. It indicatesthat within the depth from 10 to 25 cm, the peat soil strength is provided mainly by
the surface mat due to tension. Beyond this depth, the strength was provided by the
underlying weak and low bearing capacity peat. Again result from LSDðPr<0:05Þ shows
that mean surface mat stiffness increased from 31.18 to 45.63 kN/m3 when field
condition was changed from un-drained to drained. The significant effect of drainage
indicates that the surface mat stiffness increased with drawdown of water table by
drainage. Due to the drainage of the tested site the effective weight of the soil in-
creased and caused consolidation of the fill and other soft underlying materials.Underlying stiffness of peat for un-drained and drained conditions at depths of 10,
25, and 40 cm are shown in Table 5. Mean underlying stiffness of peat increased from
224.38 to 356.95 kN/m3 for plate with diameter of 10 cm, 274.15 to 378.85 kN/m3 for
plate with diameter of 15 cm, and 257.48 to 404.79 kN/m3 for plate with size of
15� 5 cm when field condition was changed from un-drained to drained.
The following observations were also made based on Table 5:
• Before drainage: Mean underlying stiffness of peat increased from 221.3 to 252.14
and 252.14 to 282.55 kN/m3 when the depth increased from 10 to 25 and 25 to 40cm, respectively.
• After drainage: Mean underlying stiffness of peat increased from 356.76 to 370
and 370 to 413.79 kN/m3 when the depth increased from 10 to 25 and 25 to 40
cm, respectively.
From the analysis of variance it was found that the mean effect of sinkage and
field conditions is significant (Pr < 0:01) on internal peat stiffness. Result from
LSDðPr<0:05Þ shows that mean underlying stiffness of peat increased from 289.03 to
Table 5
Variation of the underlying stiffness of peat with depth
Sinkage
(cm)
Plate size
(cm)
Peat stiffness, kP (kN/m3)
Block 1 Block 2 Block 3
Before
drainage
After
drainage
Before
drainage
After
drainage
Before
drainage
After
drainage
)10 D ¼ 10 228.58 249.01 196.91 339.8 168.65 473.33
D ¼ 12 216.55 342.36 235.82 222.1 212.96 374.66
L�B¼ 15� 5 283.59 465.18 222.39 288.68 226.24 455.72
)25 D ¼ 10 260.68 186.68 218.04 348.21 176.43 523.16
D ¼ 12 267.85 370.46 265.58 284.4 293.78 437.92
L�B¼ 15� 5 255.94 387.90 277.54 301.82 253.43 489.85
)40 D ¼ 10 333.0 380.00 256.94 380.19 180.21 530.26
D ¼ 12 325.00 407.81 288.50 318.3 361.35 453.62
L�B¼ 15� 5 215.86 451.89 291.94 304.3 290.41 497.77
A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40 39
311.09 and 311.09 to 348.19 kN/m3 when sinkage increased from 10 to 25 and 25 to
40 cm, respectively. Again result from LSDðPr<0:05Þ shows that mean underlying
stiffness of peat increased from 244.59 to 380.2 kN/m3 when field condition was
changed from un-drained to drained.
4. Conclusions
(i) Based on the results of laboratory analysis, it appeared that mean effect of drain-
age conditions of the tested site was highly significant on the physical features of
the peat. The mean moisture content decreased to 5.940% and bulk density was
increased to 22.59% when the field condition was changed from un-drained to
drained.
(ii) Based on the results of direct shear test in laboratory on the peat samples, it ap-peared that the mean effect of normal stress, depth and drainage conditions of
the tested site was significant on shearing stress of the peat samples. The mean
shearing stress increased to 22.34% when the normal stress increased from 2.725
to 4.0875 kN/m2 and the mean shearing stress to 63.38% when the normal stress
increased from 4.0875 to 5.45 kN/m2. The mean shearing stress increased 6.4%
and decreased 13.82% when the depth increased from 10 to 25 and 25 to 40 cm,
respectively. Furthermore, the mean direct shearing stress increased 14.68%
when the field condition was changed from un-drained to drained.(iii) Based on the results of in situ shearing stress test, it was found that vane blade
size, depth, and field drainage conditions had significant effect on in-situ shear-
ing stress. Mean in situ shearing stress increased 37.76% and decreased 38.62%
when the vane blade size increased from 4.4 to 6.4 cm and depth increased from
10 to 40 cm, respectively.
(iv) Based on the load-sinkage test, it was found that the plate sinkage increased
with increasing pushing load up to the surface mat thickness and a further in-
crease in plate sinkage caused decrease in pushing load.(v) Based on the results of stiffness of peat, it was found that mean effect of sinkage
and drainage conditions had significant effect at a 99% level of significance on
the surface mat stiffness and underlying stiffness of peat. The mean surface
mat stiffness of peat increased 57.47% and underlying stiffness of peat increased
18.1% when sinkage increased from 10 to 25 and 25 to 40 cm, respectively. Fur-
thermore, the mean surface mat stiffness and underlying stiffness of peat in-
creased 46.48% and 49.46%, respectively when field condition changed from
un-drained to drained.
Acknowledgements
This research project is classified under RM7 IRPA Project No. 01-02-04-0135.
The authors are very grateful to the Ministry of Science, Technology and The En-
vironment of Malaysia for granting the fund for this research project.
40 A. Rahman et al. / Journal of Terramechanics 41 (2004) 25–40
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