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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 84
A DUAL MECHANISM OF THE DRAG REDUCTION BY RIGID
POLYMERS AND CATIONIC SURFACTANT: COMPLEX AND
NANOFLUIDS OF XANTHAN GUM AND HEXADECYL TRIMETHYL
AMMONIUM CHLORIDE
Edward Oluwasoga Akindoyo1
, Hayder A Abdulbari2
, Zainab Yousif3
1
PhD Scholar, Faculty of Chemical and Natural Resources Engineering, University Malaysia Pahang, Lebuhraya Tun
Razak 26300, Gambang, Kuantan, Pahang, Malaysia.
2
Associate Professor and Director, Center of Excellence for Advanced Research in Fluid Flow (CARIFF), University
Malaysia Pahang, Lebuhraya Tun Razak 26300, Gambang, Kuantan, Pahang, Malaysia
3
PhD Scholar, Faculty of Chemical and Natural Resources Engineering, University Malaysia Pahang, Lebuhraya Tun
Razak 26300, Gambang, Kuantan, Pahang, Malaysia
Abstract
Several approaches have been employed to reduce the high cost of energy associated with the way liquids are transported in
pipelines. Polymers have been widely explored to replace the pumping stations and other high energy cost mechanisms, but
degrade over a period of time due to the accompanying turbulent mode of such transportation. Surfactants which are better
alternatives with the ability to reenact their lost efficiency, are less effective, there is therefore the need for an alternative
mechanism for drag reduction. In this present work, drag reduction efficacy of dispersed silica nanoparticle additives with polar
additives as complexes and nanofluid have been investigated as a new method to reduce drag. Thus the present work was carried
out with Xanthan gum which is able to withstand degradation compared to the flexible polymers, hexadecyltrimethyl ammonium
chloride as the surfactant and sodium salicylate as the counterion. In the study both complexes and nanofluid were able to reduce
drag as well as withstand shear stresses, although at different concentration which could be as a result of the different
approaches of working, about 60% drag reduction was observed. It could thus be concluded that, these materials are able to
reduce drag both as complex or nanofluid, only that, they could do that at different concentrations.
Keywords: Nanofluid, Polymers, Surfactants, Drag reduction, rotating disk apparatus, degradation
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
The concept of frictional drag is not a new one, as it is a part
of our daily activities. In air craft, liquid transportation or in
the petroleum industries. Right from the earliest discovery in
1948 [1], numerous efforts have been made to explain the
real mechanism associated with it as well as the best way to
reduce such. The concept, otherwise referred to as drag
reduction. As a result of this, many authors have contributed
significantly to the study of drag reduction [2-6].
In the course of these investigations, many materials
otherwise called “drag reduction agents” have as well been
employed. Among these DRAs, Polymers, as discovered by
Toms [1] have been the greatest explored and investigated.
Nevertheless, they are prone to the challenge of mechanical
degradation, especially under the influence of shear stress or
temperature increase, which invariably reduce their
efficiency [7]. Another set of material are the surfactants
which have been investigated by many authors [8-11.], they
offer an advantage of self-repair through micelles formation
after degradation [12-14], but are less effective when
compared to the polymers. Few other materials which have
been investigated as drag reduction agents are fibers [15]
bubbles [16] solid particles etc. which have been proven less
effective as well as of different physical working
mechanism and more prone to degradation compared to the
polymers [17]. Thus, there is yet to be a universal acceptable
material on this subject matter. This has initiated continuous
efforts to research other materials.
In a study [15], suggests a combination of polymers and
fibers as significant drag reduction with better stability
against degradation compared to polymers alone. In view of
this, Carbon nanotube nanofluid have been investigated to
reduce drag and are mechanically stable as a result of their
outstanding physical and chemical features [18]. In a recent
study [19], carbon nanotube were as well used to form
nanofluid which enhanced the drag reduction ability of
polymeric additives. Nevertheless, CNT are very expensive
and if cost it to be considered, then, alternative cheaper and
cost effective materials should be explored.
As a result of this, a close substitute for CNT are the silica
nanoparticles which have been confirmed of good stability
in organic solvents, good dispersivity as well as lubrication
additives [20-22]
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 85
This has been confirmed with the study by [23]. However,
most of these studies were carried out in pipe flow system
and with flexible polymer additives. Thus, there is need to
investigate the role of these materials with rigid polymers
which is the major motivation for this work.
In this present work, cost effective and efficient SiO2
nanoparticles were used for the first time, to modify rigid
polar additives and to produce nanofluids which are
investigated at various operating conditions in a rotating
disk apparatus. Different operating parameters were as well
experimented to verify their drag reduction efficacy.
1.1 Experimental Materials
Materials employed in this study were all supplied by Sigma
Aldrich, Malaysia and used without further treatment. They
are glycerine, Xanthan gum; 2.4 g/ cm3
density, 20–30 nm
length and 180–600 m2/g specific surface area (SSA) silica
nanoparticle; hexadecyltrimethyl ammonium chloride
(CTAC) of molecular weight 364 kg kmol−1
and Sodium
salicylate (NaSal) of molecular weight 160 kg kmol−1
as
counterion and sodium dodecyl sulfate (SDS) as dispersant
1.2 Experimental Procedure
The surfactant-counterion was prepared by accurately
measuring both materials and dissolved in double deionzed
water of about 5.07 kg, after which their mixture was
mechanically agitated for a period of 15 min, this was
carried out for a homogenous sample.
Polymers and Complexes were prepared by measuring the
required concentrations of both polymers and surfactants,
these were as well dissolved in double deionzed water of
about 5.07 kg as stock concentration until the final
concentration were prepared as the case may be for the
experiment.
The Nanofluid was however prepared by dissolving the
surfactant in the base liquid at 0.5 wt % and thereafter
mixed with the silica nanoparticle in an ultrasonic bath for
12 h for the well dispersed homogenous suspension for this
study. Detailed explanation is reported in Section 1.3.
1.3 Nano Fluid Preparation
In this present work, the first mixture to be prepared was a
baseline which is a combination of glycerine and double
deionized water in the ratio of 60wt% to 40wt%
respectively, this was able to achieve our desired viscosity
of approximately 8.10*10-3
Pa.s. This was followed by
preparing a conventional polymer drag reducing fluid
mixture by mechanically mixing the Xanthan gum of Mv =
2.0*106
g/mol with water–glycerin solution baseline, we
then prepared another mixture, comprising of the baseline
and 20–30 nm silica nanoparticle of 2.4 g/ cm3
density and
specific surface area (SSA), 180–600 m2
/g, this was done to
compare between these mixtures. Lastly Nano fluid was
prepared by dissolving 70ppm of 20–30 nm silica
nanoparticle of 2.4 g/ cm3
density and specific surface area
(SSA), 180–600 m2
/g and 100ppm of Xanthan gum of Mv =
2.0*106
g/mol which were all mixed and magnetically
stirred. But it is of interest to note that, these materials are
prone to agglomeration, thus, we dispersed them before
further investigations. In most of the literatures, Nano fluids
have been well dispersed by (a) sonication in ultrasonic bath
for a period of time, (b) Dispersed in distilled water
containing other dispersant at known adjusted PH, (c) High
shear homogenizer treatment for some time, all of these
have been reported and according to [24], Nano fluids
produced in this manner are stable for months without any
form of sedimentations. But in this present work, a
surfactant, sodium dodecyl sulfate (SDS) was used as the
dispersant where it was initially dissolved in the base fluid,
at 0.5 wt.% with magnetic stirrer followed by the
introduction of other materials as initially explained in this
section and further sonicated with 9 W of 30 kHz ultrasonic
processor for a period of 12h. Nano fluids were then
produced within the range of 0.4-1.0 wt. % nanoparticle
concentrations
1.4 Rotating Disk Apparatus (RDA)
The schematic representation of the Rotating Disk
Apparatus (RDA) used in this present study is denoted by
Figure 1. It is used to stimulate external flow of the sample
thereby recoding the influence of Torque against their
respective rotational speed. The equipment consists of a
stainless steel solution container and a lid of about 165
diameter and 88mm height and 60 mm thickness for the
container and lid dimensions respectively, maximum
solution capacity of about 1200mL, an accompanying disk
of about 3mm thickness and 148mm in diameter. For data
collection and recording, the RDA has a computer display
system where the torque is taken supported by the inbuilt
motor assembly which enable the disk to be operated, it
consists of a servo driver DS2-20P7-AS of motor capacity
0.75 kW by Xin Jie Electronic Co. Ltd, Malaysia. The
equipment is operated at a maximum operated rotational
disk speed of 3000 rpm with excellent rotational
acceleration.
There is direct connection between the servo motor and an
interface which captures the torque values at every
rotational speed of the motor thereby converting to readable
form in the computer display system with a SCADA
software.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 86
Fig 1: Graphical image of a rotating disk apparatus for the drag reduction measurement: (1) speed controller, (2) thermocouple,
(3) motor, (4) solution container, (5) water bath, (6) water-circulating system, (7) thermometer, and (8) PC.
1.5 Calculations
For data acquisition, materials tested were fed into the
chamber of approximately 1200Ml, as the disk were rotated
from 50-3000rpm, data were taken and recorded while
maintaining the temperature at 25⁰C ±0.05⁰C. Thus, the
percentage drag reduction was calculated as:
Ti and Ta denote torques reading before and after adding the
polymeric additive respectively. Flow parameters are
depicted by rotational Reynolds number NRe obtained as:
From the equation above ω, μ, ρ, R represent disk rotational
speed, fluid viscosity, fluid density and disk radius
respectively.
2. RESULTS AND DISCUSSIONS
2.1 Effects of Additive Concentration
Figures 2, 3 and 4 depict the impact of additive
concentration on Torque as the rotational speed increased,
despite the effects of the torque which invariably exerts high
shear forces on the additive molecules, increase in the
concentration were able to withstand degradation in all these
additives, from this observation, the concentration played
important role in all. It could thus be opined that all these
materials are effective drag reducers. In addition, their
mechanism of working could be based on the increase in
percentage drag reduction molecules which is favored by the
increase in their respective concentrations. Therefore, any
further increase in the additive concentrations has a direct
drastic increase in the solution viscosity which decreases
the turbulent strenght, other wise referred to as the reduction
of Reynolds number, Nre. As the process continued, the
frictional drag increases. It could be clearly seen in these
Figures that the energy dissipated due to friction by the
rotation of the disk could be taken which indicate the rate of
additives stability against degradation, owing to the fact
that, rotational flow is a drag induced flow. From the
Figures 1,2 and 3 there are no much difference in the
Torque reading at lower Nre, which are the initial readings
from 50-400rpm, but as they move further, there are
noticeable impact of the torque, yet, as a result of the
concentration increase, they were observed to be stable.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 87
Fig 2: Torque effects on different concentrations of XG
Fig 3: Torque effects on different concentrations of HTAC
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 88
Fig 4: Torque effects on different concentrations of SP
Fig 5: Torque effects on additives and 2D complex
2.2 Drag Reduction of all Samples
The Drag reduction ability of all samples is reported in Figures 2-8. This was achieved from the Torque reading, the data obtained
from this investigation are the only prerequisite measurement required for fluid drag reduction calculations with repect to the pure
solvent as explained in section 1.5. In all the additives, they all showed drag reduction capability, only that, their concentration,
mechanism are not the same.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 89
Fig 6: Torque effects on additives and 3D complex
2.3 Drag Reduction of the Polar Additives
Drag reduction efficacy of the polymer and the surfactant
are clearly shown in figures 2 and 3 respectively, from the
Figures, it could be seen that the two additives were able to
reduce drag. Neverthless, the drag reduction by the polymer
is more pronounced than in the surfactant, this could be as a
result of the viscoelastic nature of the polymer which is less
with the surfactant. However, the surfactant has ability to
form micelles which is why they were able to withstand the
degradation under the influence of shear stress, this could be
seen in Figure 3 at 1750 rotaional speed, this is the major
attribute which initiated their combination with polymer as
complex mixture. Although it has been argued that, the
mechanism of their drag reduction is different from that of
the polymer as well as less effective to the polymer [17],
nevertheless, the two materials were able to reduce drag to
an extent.
2.4 Drag Reduction Effects of Nano Silica
Figure 4 shows the drag reduction investigation of the silica
nanoparticle, it is also observed that these materials were
able to reduce drag as well as influence the drag reduction
capability of the other materials, although they exhibit a
slight behavior than the water alone, the slightest drag
reduction behavior noticed with them could have been as a
result of the present of the baseline in the sample. These
materials were tested on preparing different concentrations
and investigated in the rotating disk apparatus. In addition,
combining these materials with other drag reduction
additives yielded better impact on their drag reducing
efficacy, moreover they greatly influence the drag reduction
ability in the Nano fluid. All these could have been made
possible due to the role of the baseline, polymer and the
surfactants. From this, it could be opined that silica
nanoparticles could augment the drag reducing ability of
xanthan gum and Nano fluids.
2.5 Drag Reduction Effects of Complex and Nano
Fluid
Figures 5 and 6 show drag reduction capability of the
complex mixtures produced from the individual additives
without and with the introduction of nanosilica particles
respectively. It is of interest that both complexes were able
to reduce drag as well as great stability, this is as a result of
the data from the Torque reading with respect to the
rotational speed of the disk in each case. However, the
introduction of the silica nanoparticle in Figure 6 enhanced
greater stability than in the two dimensional complex of
Figure 5, this could be as a result of the great attributes of
the materials as enumerated by [20-22]. On the other hand,
Figures 7 and 8 depict the results of the Nano fluids
prepared from the baseline, polymer and the silica
nanoparticles where the Torque percent is related to the
respective rotational speed, overall, the materials were able
to reduce drag, despite the fact that there are different types
prepared, from these Figures, at very low concentration of
the silica nanoparticle, there was no much impact on the
drag reduction as all the material exhibit almost same
characteristic like the water, from this behavior, one could
opine that the inability of the disk wall to be well by the
presence of the nano-SiO2 could have resulted into such, in
contrast, an entirely different observation was noticed when
there was increase in the concentration as there was
effective drag reduction. This observation suggests the
availability of reasonable quantity of nano-SiO2 available to
smoothen the disk surface, a similar study was reported by
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 90
[23], which was investigated in pipe while this is the first
time such will be investigated in a rotating disk apparatus.
From this behavior, it could be said that surface
modification is one of the most important mechanism
through which these materials reduce drag with Nano fluid
of nano-SiO2, initiated by their rigid nature. In addition to
this, presence of well dispersed nano-SiO2 in the complex
mixture could have initiated their ability to influence these
materials whereas their rigidity might have prevented them
from reducing drag when solely applied but were able to
interact with other DRAs to give structures which could
influence them and also enhance their mechanical
degradation while maintaining some flexibility, in a similar
study by [19] with CNT and PEO in pipes, same was
reported, but for the first time, similar study is undertaken in
a RDA.
Fig 7: Torque effects on the nanofluid without counterion
Fig 8: Torque effects on the nanofluid with counterion
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 91
2.6 Degradation Effects of Complex and Nano Fluid
Xanthan gum are able to reduce drag as well as withstand
mechanical degradation than the flexible polymers,
nevertheless, when a complex mixture was prepared with
the surfactant, they improve greatly the drag reduction
capability and they tend to perform better than the individual
drag reducing agents, this could have been made possible
due to the presence of the surfactants owing to the fact that
they are able to realign after degradation, thus, introducing
them into the polymer, they exhibit such characteristics
whereby they withstand degradation over a period of time.
Apart from this, introducing the silica nanoparticle has
greatly improved such drag reducing ability. Moreover,
Nano fluids produced from these combination were able to
reduce drag, while comparing the complex and the Nano
fluid, it is interesting to observe that the duo were able to
reduce drag accordingly, one important observation to note
here is that the micelles formed in the complex and Nano
fluids with noticeable volume increase in larger assemblies
of wormlike micelles observed in these mixtures could have
been as a result of the counterion used with this surfactant, it
could be opined that the counterion modified the packing
parameter which reduce distances between surfactant
molecules head groups and the effective surface area of the
head group at micelle interface. Similar observation have
been observed in the study by [10, 25, 26]
2.7 Comparing the Complex with Nano Fluids
The ability of nano-sio2 to influence the drag reduction
capability of both polymer and complex mixture could be
confirmed while comparing their complex mixtures and the
nano fluid, the ability of these materials enhance such
mixtures in the dual nature has proven beyond reasonable
doubts that they play a role in their host fluids, nevertheless,
they were able to perform at different concentration and
efficacy. Direct comparison of the influence of counterion
on the drag reduction effectiveness in these mixtures shows
a diminish drag reduction effectiveness in the absence of
counterion in the complex mixture while it was the opposite
when counterion was introduced, in similar study, the nano
fluid behavior was opposite to the behavior with the
complex, this is because there was improved drag reduction
when counterion was absent in the nano fluid and opposite
without.
2.8 Drag Reduction With Respect To Reynolds
Number
Figures 9 and 10 show the roles of Reynolds number on the
drag reduction percent of the naofluid prepared without and
with counterion respectively, in both, drag reduction were
observed, but their mechanical stability were different. It is a
well known that there is a critical point and maximum point
where drag reduction is observed with additives. From the
Figures, the maximum drag reduction were observed at
Nre=5*106
. From the two Figures, increase in the nanofluid
concentration affected their respect stability. Since the best
stability was noticed with the nanofluid prepared without
counterions, thus, it could be realized that the counterion has
little or no effects on the nanofluid, especially when they are
preapared from rigid polymers. Virk [27] has been able to
classify gross flow of polymeric additives solution in pipe as
laminar, transitional, turbulent flow with or without drag
reduction, decrease in the DR% behaviour of these
nanofluids could be as a response to these flow behaviour
until the final collapse. Thus, such classification couldd be
applicable with rotating disk flow systems.
Fig 9: %DR at various Reynolds number of nanofluids
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 92
Fig 10: %DR at various Reynolds number of nanofluids with counterion
3. CONCLUSION
Several work as reported in this study, were undertakenin a
rotating disk apparatus using rigid polymers and surfactants
as complex mixtures and nanofluid. There was good
agreement between the dual nature of the mixtures produced
from these additives, although with different concentrations
and materials substitutions. Major observation was the
availability of reasonable quantity of nano-SiO2 available to
smoothen the disk surface in either of the cases. Moreover,
the increase in drag reduction is enhanced with additive
concentration.
Drag reduction and mechanical stability was more with the
three dimensional complex which is augmented with silica
nanoparticles and less with the two dimensional without
nanoparticles.
Moreover, the impact of counterion in each case also has a
role to play where it favored the complex mixtures and the
opposite with the nanofluid.
Lastly, the silica nanoparticle has a major role in the
stability of these materials as they augment them, thereby
preventing their degradation over a period of time.
ACKNOWLEDGEMENTS
The authors of this paper wish to express their profound
gratitude to the Universiti Malaysia Pahang for funding this
research work with RDU 1403169.
REFERENCES
[1]. Toms, B. A., (1948). Some observations on the flow of
linear polymer solutions through straight tubes at large
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Congress on Rheology. 2; 135–141, Amsterdam, The
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[2]. Benzi, R., (2010). A short review on drag reduction by
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[3]. Lumley, J.L., (1969). Drag reduction by additives.
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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 93
[13]. Lu, B., Li, X., Scriven, L.E., Davis, H.T., Talmon, Y.,
Zakin, J.L. (1998). Effect of chemical structure on
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[14]. Qi, Y., Littrell, K., Thiyagarajan, P., Talmon, Y.,
Schmidt, J., Lin, Z., Zakin, J.L. (2009). Small angle
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Shaqfeh, E., Moin, P. (2004). Numerical simulation of
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[17]. Liu, Z-H., Liao, L. (2010). Forced convective flow and
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[24]. Yulong, D. , Hajar, A., Dongsheng, W., Richard A. W.
(2006). International Journal of Heat and Mass Transfer. 49;
240–250
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T., Talmon, Y. and Miller, W. G. (1992). Viscoelastic
micellar solutions: microscopy and rheology. Journal of
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[27]. Virk, P. S., (1975). Drag reduction fundamentals.
AIChE Journal. 21(4); 625–656.
BIOGRAPHIES
Edward Oluwasoga Akindoyo is a PhD
student under Assoc. Prof. Dr. Hayder
Abdulbari, Faculty of Chemical and Natural
Resources Engineering, Universiti Malaysia
Pahang, Malaysia
Assoc. Prof. Dr. Hayder Abdulbari is the
Director, Centre of Excellence for Advanced
Research in Fluid flow (CARIFF), and a
Lecturer, Universiti Malaysia Pahang,
Malaysia, He specializes in Fluid Flow.
Zainab Yousif is a PhD student under
Assoc. Prof. Dr. Hayder Abdulbari, Faculty
of Chemical and Natural Resources
Engineering, Universiti Malaysia Pahang,
Malaysia

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A dual mechanism of the drag reduction by rigid polymers and cationic surfactant complex and nanofluids of xanthan gum and hexadecyl trimethyl ammonium chloride copy

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 84 A DUAL MECHANISM OF THE DRAG REDUCTION BY RIGID POLYMERS AND CATIONIC SURFACTANT: COMPLEX AND NANOFLUIDS OF XANTHAN GUM AND HEXADECYL TRIMETHYL AMMONIUM CHLORIDE Edward Oluwasoga Akindoyo1 , Hayder A Abdulbari2 , Zainab Yousif3 1 PhD Scholar, Faculty of Chemical and Natural Resources Engineering, University Malaysia Pahang, Lebuhraya Tun Razak 26300, Gambang, Kuantan, Pahang, Malaysia. 2 Associate Professor and Director, Center of Excellence for Advanced Research in Fluid Flow (CARIFF), University Malaysia Pahang, Lebuhraya Tun Razak 26300, Gambang, Kuantan, Pahang, Malaysia 3 PhD Scholar, Faculty of Chemical and Natural Resources Engineering, University Malaysia Pahang, Lebuhraya Tun Razak 26300, Gambang, Kuantan, Pahang, Malaysia Abstract Several approaches have been employed to reduce the high cost of energy associated with the way liquids are transported in pipelines. Polymers have been widely explored to replace the pumping stations and other high energy cost mechanisms, but degrade over a period of time due to the accompanying turbulent mode of such transportation. Surfactants which are better alternatives with the ability to reenact their lost efficiency, are less effective, there is therefore the need for an alternative mechanism for drag reduction. In this present work, drag reduction efficacy of dispersed silica nanoparticle additives with polar additives as complexes and nanofluid have been investigated as a new method to reduce drag. Thus the present work was carried out with Xanthan gum which is able to withstand degradation compared to the flexible polymers, hexadecyltrimethyl ammonium chloride as the surfactant and sodium salicylate as the counterion. In the study both complexes and nanofluid were able to reduce drag as well as withstand shear stresses, although at different concentration which could be as a result of the different approaches of working, about 60% drag reduction was observed. It could thus be concluded that, these materials are able to reduce drag both as complex or nanofluid, only that, they could do that at different concentrations. Keywords: Nanofluid, Polymers, Surfactants, Drag reduction, rotating disk apparatus, degradation --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION The concept of frictional drag is not a new one, as it is a part of our daily activities. In air craft, liquid transportation or in the petroleum industries. Right from the earliest discovery in 1948 [1], numerous efforts have been made to explain the real mechanism associated with it as well as the best way to reduce such. The concept, otherwise referred to as drag reduction. As a result of this, many authors have contributed significantly to the study of drag reduction [2-6]. In the course of these investigations, many materials otherwise called “drag reduction agents” have as well been employed. Among these DRAs, Polymers, as discovered by Toms [1] have been the greatest explored and investigated. Nevertheless, they are prone to the challenge of mechanical degradation, especially under the influence of shear stress or temperature increase, which invariably reduce their efficiency [7]. Another set of material are the surfactants which have been investigated by many authors [8-11.], they offer an advantage of self-repair through micelles formation after degradation [12-14], but are less effective when compared to the polymers. Few other materials which have been investigated as drag reduction agents are fibers [15] bubbles [16] solid particles etc. which have been proven less effective as well as of different physical working mechanism and more prone to degradation compared to the polymers [17]. Thus, there is yet to be a universal acceptable material on this subject matter. This has initiated continuous efforts to research other materials. In a study [15], suggests a combination of polymers and fibers as significant drag reduction with better stability against degradation compared to polymers alone. In view of this, Carbon nanotube nanofluid have been investigated to reduce drag and are mechanically stable as a result of their outstanding physical and chemical features [18]. In a recent study [19], carbon nanotube were as well used to form nanofluid which enhanced the drag reduction ability of polymeric additives. Nevertheless, CNT are very expensive and if cost it to be considered, then, alternative cheaper and cost effective materials should be explored. As a result of this, a close substitute for CNT are the silica nanoparticles which have been confirmed of good stability in organic solvents, good dispersivity as well as lubrication additives [20-22]
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 85 This has been confirmed with the study by [23]. However, most of these studies were carried out in pipe flow system and with flexible polymer additives. Thus, there is need to investigate the role of these materials with rigid polymers which is the major motivation for this work. In this present work, cost effective and efficient SiO2 nanoparticles were used for the first time, to modify rigid polar additives and to produce nanofluids which are investigated at various operating conditions in a rotating disk apparatus. Different operating parameters were as well experimented to verify their drag reduction efficacy. 1.1 Experimental Materials Materials employed in this study were all supplied by Sigma Aldrich, Malaysia and used without further treatment. They are glycerine, Xanthan gum; 2.4 g/ cm3 density, 20–30 nm length and 180–600 m2/g specific surface area (SSA) silica nanoparticle; hexadecyltrimethyl ammonium chloride (CTAC) of molecular weight 364 kg kmol−1 and Sodium salicylate (NaSal) of molecular weight 160 kg kmol−1 as counterion and sodium dodecyl sulfate (SDS) as dispersant 1.2 Experimental Procedure The surfactant-counterion was prepared by accurately measuring both materials and dissolved in double deionzed water of about 5.07 kg, after which their mixture was mechanically agitated for a period of 15 min, this was carried out for a homogenous sample. Polymers and Complexes were prepared by measuring the required concentrations of both polymers and surfactants, these were as well dissolved in double deionzed water of about 5.07 kg as stock concentration until the final concentration were prepared as the case may be for the experiment. The Nanofluid was however prepared by dissolving the surfactant in the base liquid at 0.5 wt % and thereafter mixed with the silica nanoparticle in an ultrasonic bath for 12 h for the well dispersed homogenous suspension for this study. Detailed explanation is reported in Section 1.3. 1.3 Nano Fluid Preparation In this present work, the first mixture to be prepared was a baseline which is a combination of glycerine and double deionized water in the ratio of 60wt% to 40wt% respectively, this was able to achieve our desired viscosity of approximately 8.10*10-3 Pa.s. This was followed by preparing a conventional polymer drag reducing fluid mixture by mechanically mixing the Xanthan gum of Mv = 2.0*106 g/mol with water–glycerin solution baseline, we then prepared another mixture, comprising of the baseline and 20–30 nm silica nanoparticle of 2.4 g/ cm3 density and specific surface area (SSA), 180–600 m2 /g, this was done to compare between these mixtures. Lastly Nano fluid was prepared by dissolving 70ppm of 20–30 nm silica nanoparticle of 2.4 g/ cm3 density and specific surface area (SSA), 180–600 m2 /g and 100ppm of Xanthan gum of Mv = 2.0*106 g/mol which were all mixed and magnetically stirred. But it is of interest to note that, these materials are prone to agglomeration, thus, we dispersed them before further investigations. In most of the literatures, Nano fluids have been well dispersed by (a) sonication in ultrasonic bath for a period of time, (b) Dispersed in distilled water containing other dispersant at known adjusted PH, (c) High shear homogenizer treatment for some time, all of these have been reported and according to [24], Nano fluids produced in this manner are stable for months without any form of sedimentations. But in this present work, a surfactant, sodium dodecyl sulfate (SDS) was used as the dispersant where it was initially dissolved in the base fluid, at 0.5 wt.% with magnetic stirrer followed by the introduction of other materials as initially explained in this section and further sonicated with 9 W of 30 kHz ultrasonic processor for a period of 12h. Nano fluids were then produced within the range of 0.4-1.0 wt. % nanoparticle concentrations 1.4 Rotating Disk Apparatus (RDA) The schematic representation of the Rotating Disk Apparatus (RDA) used in this present study is denoted by Figure 1. It is used to stimulate external flow of the sample thereby recoding the influence of Torque against their respective rotational speed. The equipment consists of a stainless steel solution container and a lid of about 165 diameter and 88mm height and 60 mm thickness for the container and lid dimensions respectively, maximum solution capacity of about 1200mL, an accompanying disk of about 3mm thickness and 148mm in diameter. For data collection and recording, the RDA has a computer display system where the torque is taken supported by the inbuilt motor assembly which enable the disk to be operated, it consists of a servo driver DS2-20P7-AS of motor capacity 0.75 kW by Xin Jie Electronic Co. Ltd, Malaysia. The equipment is operated at a maximum operated rotational disk speed of 3000 rpm with excellent rotational acceleration. There is direct connection between the servo motor and an interface which captures the torque values at every rotational speed of the motor thereby converting to readable form in the computer display system with a SCADA software.
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 86 Fig 1: Graphical image of a rotating disk apparatus for the drag reduction measurement: (1) speed controller, (2) thermocouple, (3) motor, (4) solution container, (5) water bath, (6) water-circulating system, (7) thermometer, and (8) PC. 1.5 Calculations For data acquisition, materials tested were fed into the chamber of approximately 1200Ml, as the disk were rotated from 50-3000rpm, data were taken and recorded while maintaining the temperature at 25⁰C ±0.05⁰C. Thus, the percentage drag reduction was calculated as: Ti and Ta denote torques reading before and after adding the polymeric additive respectively. Flow parameters are depicted by rotational Reynolds number NRe obtained as: From the equation above ω, μ, ρ, R represent disk rotational speed, fluid viscosity, fluid density and disk radius respectively. 2. RESULTS AND DISCUSSIONS 2.1 Effects of Additive Concentration Figures 2, 3 and 4 depict the impact of additive concentration on Torque as the rotational speed increased, despite the effects of the torque which invariably exerts high shear forces on the additive molecules, increase in the concentration were able to withstand degradation in all these additives, from this observation, the concentration played important role in all. It could thus be opined that all these materials are effective drag reducers. In addition, their mechanism of working could be based on the increase in percentage drag reduction molecules which is favored by the increase in their respective concentrations. Therefore, any further increase in the additive concentrations has a direct drastic increase in the solution viscosity which decreases the turbulent strenght, other wise referred to as the reduction of Reynolds number, Nre. As the process continued, the frictional drag increases. It could be clearly seen in these Figures that the energy dissipated due to friction by the rotation of the disk could be taken which indicate the rate of additives stability against degradation, owing to the fact that, rotational flow is a drag induced flow. From the Figures 1,2 and 3 there are no much difference in the Torque reading at lower Nre, which are the initial readings from 50-400rpm, but as they move further, there are noticeable impact of the torque, yet, as a result of the concentration increase, they were observed to be stable.
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 87 Fig 2: Torque effects on different concentrations of XG Fig 3: Torque effects on different concentrations of HTAC
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 88 Fig 4: Torque effects on different concentrations of SP Fig 5: Torque effects on additives and 2D complex 2.2 Drag Reduction of all Samples The Drag reduction ability of all samples is reported in Figures 2-8. This was achieved from the Torque reading, the data obtained from this investigation are the only prerequisite measurement required for fluid drag reduction calculations with repect to the pure solvent as explained in section 1.5. In all the additives, they all showed drag reduction capability, only that, their concentration, mechanism are not the same.
  • 6. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 89 Fig 6: Torque effects on additives and 3D complex 2.3 Drag Reduction of the Polar Additives Drag reduction efficacy of the polymer and the surfactant are clearly shown in figures 2 and 3 respectively, from the Figures, it could be seen that the two additives were able to reduce drag. Neverthless, the drag reduction by the polymer is more pronounced than in the surfactant, this could be as a result of the viscoelastic nature of the polymer which is less with the surfactant. However, the surfactant has ability to form micelles which is why they were able to withstand the degradation under the influence of shear stress, this could be seen in Figure 3 at 1750 rotaional speed, this is the major attribute which initiated their combination with polymer as complex mixture. Although it has been argued that, the mechanism of their drag reduction is different from that of the polymer as well as less effective to the polymer [17], nevertheless, the two materials were able to reduce drag to an extent. 2.4 Drag Reduction Effects of Nano Silica Figure 4 shows the drag reduction investigation of the silica nanoparticle, it is also observed that these materials were able to reduce drag as well as influence the drag reduction capability of the other materials, although they exhibit a slight behavior than the water alone, the slightest drag reduction behavior noticed with them could have been as a result of the present of the baseline in the sample. These materials were tested on preparing different concentrations and investigated in the rotating disk apparatus. In addition, combining these materials with other drag reduction additives yielded better impact on their drag reducing efficacy, moreover they greatly influence the drag reduction ability in the Nano fluid. All these could have been made possible due to the role of the baseline, polymer and the surfactants. From this, it could be opined that silica nanoparticles could augment the drag reducing ability of xanthan gum and Nano fluids. 2.5 Drag Reduction Effects of Complex and Nano Fluid Figures 5 and 6 show drag reduction capability of the complex mixtures produced from the individual additives without and with the introduction of nanosilica particles respectively. It is of interest that both complexes were able to reduce drag as well as great stability, this is as a result of the data from the Torque reading with respect to the rotational speed of the disk in each case. However, the introduction of the silica nanoparticle in Figure 6 enhanced greater stability than in the two dimensional complex of Figure 5, this could be as a result of the great attributes of the materials as enumerated by [20-22]. On the other hand, Figures 7 and 8 depict the results of the Nano fluids prepared from the baseline, polymer and the silica nanoparticles where the Torque percent is related to the respective rotational speed, overall, the materials were able to reduce drag, despite the fact that there are different types prepared, from these Figures, at very low concentration of the silica nanoparticle, there was no much impact on the drag reduction as all the material exhibit almost same characteristic like the water, from this behavior, one could opine that the inability of the disk wall to be well by the presence of the nano-SiO2 could have resulted into such, in contrast, an entirely different observation was noticed when there was increase in the concentration as there was effective drag reduction. This observation suggests the availability of reasonable quantity of nano-SiO2 available to smoothen the disk surface, a similar study was reported by
  • 7. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 90 [23], which was investigated in pipe while this is the first time such will be investigated in a rotating disk apparatus. From this behavior, it could be said that surface modification is one of the most important mechanism through which these materials reduce drag with Nano fluid of nano-SiO2, initiated by their rigid nature. In addition to this, presence of well dispersed nano-SiO2 in the complex mixture could have initiated their ability to influence these materials whereas their rigidity might have prevented them from reducing drag when solely applied but were able to interact with other DRAs to give structures which could influence them and also enhance their mechanical degradation while maintaining some flexibility, in a similar study by [19] with CNT and PEO in pipes, same was reported, but for the first time, similar study is undertaken in a RDA. Fig 7: Torque effects on the nanofluid without counterion Fig 8: Torque effects on the nanofluid with counterion
  • 8. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 91 2.6 Degradation Effects of Complex and Nano Fluid Xanthan gum are able to reduce drag as well as withstand mechanical degradation than the flexible polymers, nevertheless, when a complex mixture was prepared with the surfactant, they improve greatly the drag reduction capability and they tend to perform better than the individual drag reducing agents, this could have been made possible due to the presence of the surfactants owing to the fact that they are able to realign after degradation, thus, introducing them into the polymer, they exhibit such characteristics whereby they withstand degradation over a period of time. Apart from this, introducing the silica nanoparticle has greatly improved such drag reducing ability. Moreover, Nano fluids produced from these combination were able to reduce drag, while comparing the complex and the Nano fluid, it is interesting to observe that the duo were able to reduce drag accordingly, one important observation to note here is that the micelles formed in the complex and Nano fluids with noticeable volume increase in larger assemblies of wormlike micelles observed in these mixtures could have been as a result of the counterion used with this surfactant, it could be opined that the counterion modified the packing parameter which reduce distances between surfactant molecules head groups and the effective surface area of the head group at micelle interface. Similar observation have been observed in the study by [10, 25, 26] 2.7 Comparing the Complex with Nano Fluids The ability of nano-sio2 to influence the drag reduction capability of both polymer and complex mixture could be confirmed while comparing their complex mixtures and the nano fluid, the ability of these materials enhance such mixtures in the dual nature has proven beyond reasonable doubts that they play a role in their host fluids, nevertheless, they were able to perform at different concentration and efficacy. Direct comparison of the influence of counterion on the drag reduction effectiveness in these mixtures shows a diminish drag reduction effectiveness in the absence of counterion in the complex mixture while it was the opposite when counterion was introduced, in similar study, the nano fluid behavior was opposite to the behavior with the complex, this is because there was improved drag reduction when counterion was absent in the nano fluid and opposite without. 2.8 Drag Reduction With Respect To Reynolds Number Figures 9 and 10 show the roles of Reynolds number on the drag reduction percent of the naofluid prepared without and with counterion respectively, in both, drag reduction were observed, but their mechanical stability were different. It is a well known that there is a critical point and maximum point where drag reduction is observed with additives. From the Figures, the maximum drag reduction were observed at Nre=5*106 . From the two Figures, increase in the nanofluid concentration affected their respect stability. Since the best stability was noticed with the nanofluid prepared without counterions, thus, it could be realized that the counterion has little or no effects on the nanofluid, especially when they are preapared from rigid polymers. Virk [27] has been able to classify gross flow of polymeric additives solution in pipe as laminar, transitional, turbulent flow with or without drag reduction, decrease in the DR% behaviour of these nanofluids could be as a response to these flow behaviour until the final collapse. Thus, such classification couldd be applicable with rotating disk flow systems. Fig 9: %DR at various Reynolds number of nanofluids
  • 9. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 92 Fig 10: %DR at various Reynolds number of nanofluids with counterion 3. CONCLUSION Several work as reported in this study, were undertakenin a rotating disk apparatus using rigid polymers and surfactants as complex mixtures and nanofluid. There was good agreement between the dual nature of the mixtures produced from these additives, although with different concentrations and materials substitutions. Major observation was the availability of reasonable quantity of nano-SiO2 available to smoothen the disk surface in either of the cases. Moreover, the increase in drag reduction is enhanced with additive concentration. Drag reduction and mechanical stability was more with the three dimensional complex which is augmented with silica nanoparticles and less with the two dimensional without nanoparticles. Moreover, the impact of counterion in each case also has a role to play where it favored the complex mixtures and the opposite with the nanofluid. Lastly, the silica nanoparticle has a major role in the stability of these materials as they augment them, thereby preventing their degradation over a period of time. ACKNOWLEDGEMENTS The authors of this paper wish to express their profound gratitude to the Universiti Malaysia Pahang for funding this research work with RDU 1403169. REFERENCES [1]. Toms, B. A., (1948). Some observations on the flow of linear polymer solutions through straight tubes at large Reynolds numbers, in Proceedings of the First International Congress on Rheology. 2; 135–141, Amsterdam, The Netherlands. [2]. Benzi, R., (2010). A short review on drag reduction by polymers in wall bounded turbulence. Physica D 239; 1338– 1345. [3]. Lumley, J.L., (1969). Drag reduction by additives. Annual Review of Fluid Mechanics. 11; 367–384. [4]. Dubief, Y., White, C.M., Terrapon, V.E., Shaqfeh, E.S.G., Moin, P & Lele, S.K. (2004). On the coherent drag- reducing and turbulence-enhancing behaviour of polymers in wall flows. Journal of Fluid Mechanics. 514; 271–280. [5]. Tabor, M., De Gennes, P.G., (1986). A cascade theory of drag reduction, Europhysics Letter. 7 ;519–522. [6]. A.S. Pereira et al. (2013). Journal of Non-Newtonian Fluid Mechanics. 202; 72–87. [7]. Pereira, A.S., Andrade, R.M., Soares E.J. (2013). Drag reduction induced by flexible and rigid molecules in a turbulent flow into a rotating cylindrical double gap device: comparison between poly (ethylene oxide), polyacrylamide, and xanthan gum. J Non-Newtonian Fluid Mech. 202:72 [8]. Gurka, R., Liberzon, A., Hetsroni, G. (2004). Characterization of turbulent flow in a flume with surfactant. J. Fluids Eng. 126; 1054–1057. [9]. Warholic, M.D., Schmidt, G.M., Hanratty, T.J. (1999). The influence of a drag-reducing surfactant on turbulent velocity field. J. Fluid Mech. 388; 1–20. [10]. Qi, Y., Zakin, J.L.(2002). Chemical and rheological characterization of drag-reducing cationic surfactant systems. Ind. Eng. Chem. Res. 41; 6326–6336. [11]. Li, ,F.-C., Kawaguchi, Y., Yu, B., Wei, J.-J., Hishida, K. (2008). Experimental study of dragreduction mechanism for a dilute surfactant solution flow. Int. J. Heat Mass Transfer 51; 835–84. [12]. Ge, W., Kesselman, E., Talmon, Y., Hart, D.J., Zakin, J.L. (2008). Effects of chemical structures of para- halobenzoates on micelle nanostructure, drag reduction and rheological behaviors, of dilute CTAC solutions. J. Non- Newton. Fluid Mech. 154;1–12.
  • 10. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 02 | Feb-2015, Available @ http://www.ijret.org 93 [13]. Lu, B., Li, X., Scriven, L.E., Davis, H.T., Talmon, Y., Zakin, J.L. (1998). Effect of chemical structure on viscoelasticity and extensional viscosity of drag-reducing cationic surfactant solutions. Langmuir. 14; 8–16. [14]. Qi, Y., Littrell, K., Thiyagarajan, P., Talmon, Y., Schmidt, J., Lin, Z., Zakin, J.L. (2009). Small angle neutron scattering study of shearing effects on drag-reducing surfactant solutions. J. Colloid Interface Sci. 337; 218–226. [15]. Paschkewitz, J.S., Dubief, Y., Dimitropoulos, C., Shaqfeh, E., Moin, P. (2004). Numerical simulation of turbulent drag reduction using rigid fibres. J Fluid Mech. 518;281. [16]. van Gils, D.P.M., Guzman, D.N., Sun, C., Lohse, D. (2013). The importance of bubble deformability for strong drag reduction in bubbly turbulent Taylor-Couette flow. J Fluid Mech. 722;317. [17]. Liu, Z-H., Liao, L. (2010). Forced convective flow and heat transfer characteristics of aqueous drag-reducing fluid with carbon nanotubes added. Int J Therm Science. 49; 2331 [18]. Salvetat-Delmotte, J.P., Rubio, A. (2002). Mechanical properties of carbon nanotubes: a fiber digest for beginners. Carbon. 40;10. [19]. Adam, S., Ilker, S. B., Eric, L., (2014). CARBON. 77; 1183 – 1186 [20]. Ma, S.Y., Zheng, S.H., Ding, H.Y., Li, W. (2009). Advances in Materials Research. 79–82; 1863 [21]. Garbacz, H., Gradzka-Dahlke, M., Kurzydłowski, K.J. (2007). Wear. 263; 572. [22]. Wu, Y.Y., Tsui, W.C.,. Liu, T.C. (2007). Wear. 262; 819. [23]. Pouranfard A.R. et al. (2014). Journal of Industrial and Engineering Chemistry. 20; 633–637 [24]. Yulong, D. , Hajar, A., Dongsheng, W., Richard A. W. (2006). International Journal of Heat and Mass Transfer. 49; 240–250 [25]. Clausen, T. M., Vinson, P. K., Minter, J. R., Davis, H. T., Talmon, Y. and Miller, W. G. (1992). Viscoelastic micellar solutions: microscopy and rheology. Journal of Physical Chemistry. 96 (1); 474–484. [26]. Myska, J. and Mik, V. (2004). Degradation of surfactant solutions by age and by a flow singularity. Chemical Engineering and Processing. 43; 1495-1501. [27]. Virk, P. S., (1975). Drag reduction fundamentals. AIChE Journal. 21(4); 625–656. BIOGRAPHIES Edward Oluwasoga Akindoyo is a PhD student under Assoc. Prof. Dr. Hayder Abdulbari, Faculty of Chemical and Natural Resources Engineering, Universiti Malaysia Pahang, Malaysia Assoc. Prof. Dr. Hayder Abdulbari is the Director, Centre of Excellence for Advanced Research in Fluid flow (CARIFF), and a Lecturer, Universiti Malaysia Pahang, Malaysia, He specializes in Fluid Flow. Zainab Yousif is a PhD student under Assoc. Prof. Dr. Hayder Abdulbari, Faculty of Chemical and Natural Resources Engineering, Universiti Malaysia Pahang, Malaysia