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Experimental Investigation of the Effects of DifferentParameters on the Rate of Asphaltene Deposition inLaminar Flow and Its Prediction Using Heat TransferApproachFarhad Salimi a , Mohsen Vafaie Seftie a & Shahab Ayatollahia ba Chemical Engineering Department , Tarbiat Modares University , Tehran , Iranb Enhanced Oil Recovery (EOR) Research Center and Shiraz University , Shiraz , IranAccepted author version posted online: 14 Jun 2013.
To cite this article: Journal of Dispersion Science and Technology (2013): Experimental Investigation of the Effects ofDifferent Parameters on the Rate of Asphaltene Deposition in Laminar Flow and Its Prediction Using Heat Transfer Approach,Journal of Dispersion Science and Technology, DOI: 10.1080/01932691.2013.763729
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Experimental Investigation of the Effects of Different Parameters on the Rate of Asphaltene Deposition in Laminar Flow and Its Prediction Using Heat Transfer
Approach
Farhad Salimi1, Mohsen Vafaie Seftie1,, Shahab Ayatollahia2
1Chemical Engineering Department, Tarbiat Modares University, Tehran, Iran,
2Enhanced Oil Recovery (EOR) Research Center and Shiraz University, Shiraz, Iran
Received 8 December 2012; Accepted 3 January 2013.
Address correspondence to Mohsen Vafaie Seftie, Chemical Engineering Department, Tarbiat Modares University, Tehran, Iran. E-mail: [email protected]
Abstract
In this study, asphaltene deposition from crude oil on the pipe surface has been studied
experimentally using a novel designed test loop. Washing technique is used to
quantitatively measure the rate of asphaltene deposition during laminar flow in the steel
pipe. The effects of oil velocity, asphaltene content and surface temperature on the
thickness of asphaltene deposition are investigated. The results show that the asphaltene
deposition rate increases with increasing surface temperature, results in asphaltene
content reduction of the flowing crude oil. As the oil velocity increases, less deposition
was noticed on the surface of the pipe. Besides, thermal approach was applied to the
experimental procedure which shows good agreements between the predicted thickness
and the measured value from the test loop.
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KEYWORDS: asphaltene, deposition, pipeline, Washing Method, laminar flow,
1. INTRODUCTION
Flow assurance is referred to a technique to assess the ability of production facilities to
transfer multi-phase fluids from the reservoir to the market. The fluid behavior is tested
for any possible interruption during this fluids flow process. Flow assurance includes
factors such as asphaltene and wax deposition, hydrate formation, scale, slugging and
corrosion1. Asphaltenes deposition insides the oil reservoirs and production facilities is
known as the main flow assurance problem in the oil industry.
Generally, asphaltenes are regarded as part of the crude oil that is insoluble in normal
alkanes such as pentane and heptane but soluble in aromatics such as toluene and
benzene. Also Asphaltenes are known as highest molecular weight and most polar oil
components2-4.Asphaltenes composition, structure and stability are dependent on its
source, and the type of solvent used for the extraction of oil5-9.Furthermore, the
absorption and deposition of asphaltenes on steel surface would restrict oil flow in the
transportation pipelines10, 11.The remediation of asphaltene is very costly which limits the
production design of many asphaltenic crude oil reserves9, 12.
In many cases, the potential of organic solids depositions force the field managers to rely
mostly on the chemical and mechanical remediation methods13-17. Therefore, better
understanding of the mechanism of solid deposition is required to better design
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treatments, including the effect of pressure, temperature, composition, additives and flow
conditions. These are the most important parameters during flow assurance process.
Literature study on asphaltene deposition reveals that few works on asphaltene deposition
at real pipe conditions have been reported18-21. The aim of this work is a mechanistic
study of asphaltene deposition in laminar flow to investigate the effects of oil velocity,
temperature and asphaltene content on the rate of asphaltene deposition.
2. EXPERIMENTAL PART
2.1. Experimental Procedure
A test loop is used to investigate asphaltene deposition inside the pipe using an Iranian
asphaltenic crude oil. The fractions of saturates, aromatics, resins and asphaltenes in the
oil were obtained from the so-called SARA test depicted in Table 1.
In this work, the deposited asphaltene inside of tube was measured by “washing method”.
For this purpose the tube was rinsed with Heptane first to wash out non-asphaltene
hydrocarbons, where asphaltenic components remained there attached to the wall.In the
next step the deposited materials inside the tube were washed out using toluene and its
weight was measured after evaporating of the toluene.
The following procedure was used to measure the asphaltene fraction of deposited
materials inside the pipe. The collected asphaltenes from the previous step, “washing
method”, was first precipitated with n-heptane at 40:1 volume ratio of n-heptane to
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sample solution. Then the mixture was left to equilibrate for 20 to 24 hours, and finally
the sample was filtered by filter paper (Whatman Grade No. 42). The Filter with
asphaltene was crumpled and placed in a Soxhlet apparatus and refluxed with n-heptane
for 2 hours. The deposited material retained on the filter paper was considered as
asphaltene after drying process. Table 1
2.2. Experimental Apparatus
Figure 1 shows schematic view of the novel designed flow assurance test loop which has
been used to measure the thickness of asphaltene deposition as a function of time at
different condition. The apparatus is made of a well-controlled temperature bath
containing long stainless steel tube in coil shape. The temperature of the bath was
maintained constant using heat source, controlling unit and stirrer. The long test tube was
equipped with accurate pressure transducers and thermocouples at several intervals;
transferring all the information into a data acquisition system. The feed was prepared and
transferred into feed storage and its temperature was maintained at pre-set temperature
prior to flow through the pump into the flowing loop.
For this study, the pipe test section was made of1m length stainless steel tube (seamless,
Fitok Company)with 3.74mm inside diameter, which was coiled and placed inside the
bath. The bulk temperature of the oil is measured with K-type thermocouples which are
located in the tank and in mixing chambers before and after of the test section. The
temperature of the bath was controlled within ±0.1oC,holding the stainless steel pipe. The
absolute pressure at the outlet of the tube was controlled with back pressure control
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regulator (model of BP-66). The oil flow rate was controlled by the constant rate pump.
A data acquisition system is used to monitor the temperature at various point of both bath
and tube.Figure 1
3. RESULTS AND DISCUSSION
The results are tabulated in Table 2. These eight set of tests were designed to check the
effects of oil velocity and surface temperature on the rate of asphaltene deposition. This
procedure (Washing Method) could be used to find the deposition rate by carefully
monitoring the temperature difference between the outlet and inlet and also bath
temperature. The results for the asphaltene deposition rates are presented and discussed in
the following sections. Also the analytical tests of the deposited materials show that the
amount of asphaltene in the deposited layer is significant.
3.1.Concentration Measurement Of Flocculated Asphaltene
The first step to study the mechanisms of asphaltene deposition is to determine the
concentration of flocculated asphaltene particles in the oil at specified temperatures. One
of the methods used to measure the amount of precipitated asphaltenes due to the solvent
is scaling method. Mathematical correlations of this method is very simple and do not
need the oil specification. This method was first proposed by Rassamdana et al22. Their
results showed that all asphaltene titration curves of the dead oil by solvents of normal
alkane correlate into a single curve. This function is as follows:
2 30 1 2 3Y A A X A X A X= + + + (1)
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Parameters A0 to A3 are constant and indicate the scaling coefficients. The three main
variables of titration of dead oil curves are the weight percentage of precipitated
asphaltene W, the solvent to oil dilution ratio Rm and the molecular weight of the solvent.
Rassamdana et al23 lumped these three parameters into two variables X and Y of the
scaling equation:
mz z
m
R WX and YM R ′= = (2)
Adjustable parameters are z and z’ which must be carefully tuned to find the best fitting
of the experimental data. They suggested Z’ = -2 and Z = 0.25 in spite of oil and type of
precipitant material used. In recent years, several investigators have verified the scaling
model23-26.Ashoori et al (2010) modified the scaling equations and considered the scaling
variables X and Y as follows26:
( )n Z ZV W t VX R / T .M and Y W / R ′= = (3)
The exponent n is a constant and its value is between 0.10 and 0.25. Two other constants,
Z and Z', are the same as the first scaling equation, i.e. Z=0.25 and Z'=−2.
The measured mass of precipitated asphaltene as a function of the volumetric dilution
ratio (n-heptane/oil) for several temperatures in this work has been shown in figure 2.
The mass of asphaltene deposition versus dilution volume ratio found here is based on
work of Ashoori et al26. Figure 2
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3.2. Mechanism Of Asphaltene Deposition
The published works show that no comprehensive model to describe the effect of
operating conditions on the mechanism of asphaltene deposition in the pipes is
available27. Broseta et al28 (2000) and Wang et al (2004)19 investigated asphaltene
deposition in a capillary tube. Jamialahmadi et al (2009) investigated the mechanisms of
deposition of flocculated asphaltene under forced convective conditions and turbulence
condition21. Results showed that the rate of asphaltene deposition increases with
increasing flocculated asphaltene concentration and temperature while it decreases with
increasing oil velocity.
There are likely several steps in deposition process for asphaltenes: precipitation,
flocculation, surface contact and adhesion18. Asphaltenes could be directly absorbed on
the solid surfaces if no precipitation has been occurred however, it is expected that for
this case the amount of absorption is negligible29. To predict asphaltene deposition
accurately one needs to understand the fundamental mechanism for each step. Fouling in
the heat transfer cases can be used to make an analogy for the asphaltene
deposition/release mechanism that was presented by Kern and Seaton30 (1959). The net
rate of growth of asphaltene deposit is the difference between the rate of deposited of
material md and the rate of its removal mr expressed as follows:
d rdm m mdt
= − (4)
3.3. Effect Of Asphaltene Concentration
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One of the main reasons of asphaltene deposition is the concentration of flocculated
asphaltene in the flowing oil. So long as the removal rate can be ignored and all particles
arriving at the heat transfer surface are deposited, the rate of deposition may be generally
expressed as:
( )nd t Asm k C= (5)
where CAS is the flocculated asphaltene concentration at the surface conditions. For mass
transfer and surface deposition controlled processes n generally varies between 1 and 2.
Equation 5 shows that the concentration has a strong effect on deposition, regardless of
the mechanism of deposition. The effect of asphaltene concentration on rate of deposition
at a Reynolds numberabout1000 and constant bulk and bath temperature is shown in
Fig.3. The results indicate that the increase of asphaltene concentration lead to enhance
the rate of asphaltene deposition. The results indicate that there are a linear relation
between rate of asphaltene deposition and asphaltene concentration and the best n for
fitting �� versus concentration of asphaltene is approximately equal to 1.2.
3.4. Effect Of Wall Temperature
To study the effect of wall temperature on asphaltene deposition, three different tests at
different wall temperatures were performed at constant oil velocity, bulk temperature and
asphaltene concentration. The rate of asphaltene deposition is plotted at different wall
temperature in Figures 4 where shows that the deposition thickness increases at higher
wall temperature.
3.5. Effect Of Oil Velocity
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In this section, the effect of velocity on the deposition thickness in the range of 0.23 to
0.67 m/s is discussed. Figure 5 shows the rate of asphaltene deposition for different oil
velocities which were measured using the “Washing Method”. This clearly indicates that
the deposition rate is decreased significantly when the oil velocity is increased. Figures 3,
4 and 5
4. THE MODEL
Fouling method was used to predict the rate of asphaltene deposition on pipe surface, and
an equation was developed. The models describing fouling usually are based on the well-
known concept of Kern and Seaton (1959) approach where the net fouling rate is the
difference between the rates of deposition and removal: Fouling Rate=Rate of deposition-
Rate of removed
According toEquation17, it can be put the fouling model in Kt coefficient(overall transfer
coefficient) and used it for predicting of deposition. Soitcan bedoneas follows:
Kt =Rate of deposition-Rate of removed
The type of the description of the deposition and removal terms is the basic differences
between various models reported in literature. The rate of deposition is described by
either a transport-reaction model or reaction alone model while the rate of removal is
described either by shear-related or mass-transfer related expressions. The first term of
the right-hand side of this expression is dependent on both the surface temperature and
also rate of transport the particles from the fluid bulk toward the wall.
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The rate of fouling increases exponentially with increasing surface temperature for
almost all fouling mechanisms31-34. which is generally expressed by an Arrhenius-type
equation.
However, the rate of particle transport from balk toward wall depends on the type of flow
regime. In this work, regime of flow is laminar and the Sieder–Tate correlation35 is used.
Rate of deposition is obtained by substituting of terms includes wall temperature and rate
of particle transport as follows:
Rate of deposition (Re. Pr (D/L))1/3 (µ/µw)0.14 * exp(Ea/RTW)
Both length and diameter are constant and do not change during experiments, so the
equation can be simplified as follows:
Rate of deposition = Kd*(Re. Pr)1/3* exp(Ea/RTW)
where Kd is constant and can be determined from the experimental data. As it was already
described, there are two proposed mechanisms for the removal rate which are expressed
as follows:
1. The rate of removal depends on shear-related or velocity flow which is expressed
as follows: Rate of removed=Kremoval*τw
2. The rate of removal instead of being dependent on the shear stress is affected
bytherate of mass-transfer which was already proposed by Polley et al36. Rate of
removed=Kremoval*Ren
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Which Kremoval and n constants have been obtained by curve-fitting experimental data in
final model. After substituting equations in equations, following equations are obtained:
( )1
1.23 exp ad e r removal W Ab
W
Em k R P K CRT
τ
= − (6)
( )1/3 1.2exp nad e r removal e Ab
W
Em k R P K R CRT
= −
(7)
Results of curve-fitting will tabulate in table 3. Results in table 3 indicate that the
equation 7 is better than the equation 6 for fitting of data. It seems that curve-fitting is
better when the rate of removal is dependent on rate of the rate of mass-transfer. Table 3
5. CONCLUSIONS
In the present study, after carefully verifying of the use of “Washing Method” for the
measurements of asphaltene deposition thickness, the effects of operating parameters
such as oil velocity and pipe surface temperature on the deposition process in asphaltenic
crude oil in a tube was investigated. The results showed that the deposition rate was
increased as the surface temperature and asphaltene concentration were increased. The
experimental results also indicate that the deposition rate is inversely proportional to the
oil velocity and the thickness of deposited components was decreased as the oil velocity
was increased. Besides, fouling model was employed to predict value of asphaltene
deposition from the test loop and good agreement between the predicted thickness and
the measured value was noticed.
ACKNOWLEDGMENTS
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The authors would like to express their sincere gratitude to NPF Co (Mr. Tohidi and Mr.
Moazed), for their kind collaboration and help during the installation and setup of the
apparatus used in this study.
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31. Eaton, P. and Lux, R. (1984) ASME HTD., 35: 33-42
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TABLE 1. Analysis of SARA
Fractions %wt
Asphaltenes 13.84
Resins 13.46
Saturates 30.31
Aromatics 42.4
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Table 2. A summary of the experimental results
Test
Number
Casph Toil1 Tbath Velocity Time Mass of
deposit(kg/m2)
%
Asphaltene
(gr/cm3) (oC) (oC) (m/s) (hr) (Washing
method)
in
the deposit
Test 1 1.5 51.5 70 0.23 70 0.4 63.3
Test 2 1.5 52.5 70 0.51 70 0.22 82
Test 3 1.5 50 70 0.67 70 0.118 87
Test4 3 50 70 0.27 52 0.144 83.3
Test5 5 50 70 0.17 47 0.208 85
Test6 5 57 70 0.333 40 0.094 85
Test 7 1.5 57 80 0.333 24 0.103 84
Test 8 1.5 57 90 0.333 23 0.21 87
1Average oil temperature of the input and output in the pipe
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TABLE 3. Results of curve-fitting
Constants %Absolute Average Error
Equation 6
Kd=148 m/s
Kremoval=4.23*10-8 .
mPa s
EaR
= 7788.6 K
38
Equation 7 Kd=-139266m/s
Kremoval=-101.59 m/s
EaR
= 10291.9 K
n=-3.267
13.9
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FIG.1. Schematic of the experimental apparatus.
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FIG.2. Variation of mass of asphaltenes precipitation with dilution ratio at various
temperatures.
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FIG.3. Variation of asphaltene deposition rate with flocculated asphaltene concentration.
(Re=1000, Tbath=70C, Tbalk=50C)
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FIG.4. Variation of asphaltene deposition rate with wall temperature(v=0.33m/s,
Tbalk=57C).
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a St
ate
Uni
vers
ity]
at 0
1:55
08
Sept
embe
r 20
13