Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt 309
FLUX ENHANCEMENT BY USING HELICAL BAFFLES IN
ULTRAFILTRATION OF SUSPENDED SOLIDS
Noreddine Ghaffour1,*, Rahim Jassim2 and Tahir khir2
1
Middle East Desalination Research Center (MEDRC), Oman
2
Jeddah College of Technology, KSA
Corresponding author: PO Box 21, Al-Khuwair, PC. 133, Muscat, Sultanate of
Oman
Fax: +968 697107, Email: nghaffour@medrc.org.om
ABSTRACT
The main reason for the flux decline during the initial period of all filtration
processes is the usual phenomena of concentration polarization and fouling. After
this stage follows the cake filtration process that allows to obtain the steady state
flux. The solute accumulated on the membrane surface forms a high concentration
gel layer, which increases the effective membrane thickness and so reduces its
hydraulic permeability. Different techniques are used to reduce this formation and
use of helical baffles inside the membrane element is one of such techniques. The
selection of appropriate helical baffle is vital to get improved permeation flux with
minimum pressure drop for cross-flow feed. The number of helices per unit length
has a considerable influence on the selected helical baffle. All experiments have
been conducted with an inorganic tubular ultrafiltration membrane for filtering a
supernatant from activated sludge plant consisting of suspended and biological
solids. The influence of the operational parameters is studied in this paper.
Nevertheless, the feed temperature and the concentration were kept constant at the
industrial values. We found 1 bar as an optimal pressure, above this pressure the
permeation flux decreases, contrarily to several works, which observe a plateau
after certain value of pressure. Progressive fouling can be limited by use of helical
baffles in the filtration element operated at low pressures and the flocculation of
particles is reduced. On the other hand, we have found that the influence of
Reynolds number inside the membrane tube and the feed flow-rate are similar to
other studies that used different helical baffles.
Keywords: Ultrafiltration, Helical baffles, Tubular membrane, Suspended solids,
Deposited layer
1. INTRODUCTION
One of the most important problems in applying membrane technology is the usual
concentration polarization and membrane fouling, which has very serious
operational, economic and environmental implications. The deposit formed on the
310 Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt
membrane surface, which causes blockage of flow passages, can be removed with
different techniques, mainly the using of helical baffles inside the membrane tube.
The permeation flux limitation is often due to the high concentration of solute on
the membrane surface due to concentration polarization.
Several authors used different techniques to reduce the concentration polarization
and membrane fouling such as use of baffles [3, 12, 17, 20] and spacers [23],
increasing the cross-flow velocity or backflushing [15] and air or gas sparging
during filtration [4, 6, 7, 22].
Gupta et al. [12] reported that the permeate flux increased with increase in number
of helices by unit length. Moreover, visualizing by video camera revealed that
flow was rotational around the baffle axis that was responsible for enhanced
mixing leading to migration of suspended solids away from the membrane surface.
Metal grate type of helical baffles (crimped lozenges meshes type) are also used
by Sebbane [20]. He found that the permeate flow-rate decreases when the
thickness of the fluid vein increases. Other researchers, Bennasar [3], Maubois and
Mocqout [17], using similar helical baffles, found that the ultrafiltration of milk
gave better results when the hydraulic diameter was reduced. The latter thinks that
Dh plays an essential role on the formed layer on the membrane surface and on his
internal fouling.
Sebbane showed that the gel resistance decreases with the hydraulic diameter. The
shear stress can influence on internal fouling while acting on the gel layer, which
lead an increase of the permeate flux more important than foreseen. We can think
also that the gel concentration vary with the hydraulic diameter.
After preliminary screening, we selected the helical baffle since it gave higher
permeate flux. The number of helices per unit length has a big influence on the
selected helical baffle. All experiments have been conducted with an inorganic
tubular membrane manufactured by TechSep. The second step was the study of
the influence of the pressure and flow rate on the flux performance.
2. EXPERIMENTAL
2.1. HELICAL BAFFLE
The helical baffles in this study come from suggestions of several authors [12].
These are wound stems in circular helices, which can consist a variable number of
helices per unit length. To the difference of the systems proposed by Gupta et al.
[12], their installation in the filtration element implies the existence of contact
points between the helix and the membrane wall as shown in Figure 1.
Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt 311
Figure 1. Schematic of the used helical baffle.
The geometric parameters of the used helical baffle are given in the table 1,
knowing that the hydraulic diameter is defined by:
Dh =
4Ω'
Ph
(1)
Table 1. Geometric parameters linked to the used helical baffle.
D (mm)
Membrane tube
6
diameter
(mm2) Membrane cross section 28,3
’ (mm2)
Cross section with
23,3
helical baffle
Ph (mm)
Wetted perimeter
30,8
Dh (mm)
Hydraulic diameter
3
2.2. UNIT AND MEMBRANE
The experimental unit used is shown schematically in Fig. 2. Temperature and
feed concentration were maintained at 35 oC and 5 g/l respectively. Temperature is
maintained homogenous using a helical coil heat exchanger immersed in a 10 liter
feed tank. The selected M9 Carbosep membrane, manufactured by TechSep, was
an inorganic composite membrane whose zirconia-active layer was deposited on a
carbon support. This tubular membrane has an internal 6 mm diameter and a
length of 40 cm. The membrane cut-off as given by the manufacturer is 300 000
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Daltons, which corresponds to a pore diameter of 0.02 µm [2]. All experiments
have been carried out at the optimum values of the operational parameters
obtained without helical baffles.
Flow-meter
Back Pressure
Regulator
Thermoregulation
Membrane
Module
Manometer
Permeate
Manometer
Feed
Reservoir
Screw Pump
Figure 2. Experimental unit.
2.3. SUSPENSIONS AND DETERMINATIONS
The suspensions are made with suspended solids collected from the settler of an
activated sludge plant. The unstable solution was continuously stirred and thermoregulated in a storage tank to keep the feed temperature and concentration
homogeneous. Filtration flow-rate and flux were determined by measuring the
time required to collect a given filtrate volume. The membrane was cleaned
chemically with a 30% sodium hydroxide and 30% nitric acid solutions after each
experiment until the permeability was regained.
3. RESULTS AND DISCUSSION
3.1. INFLUENCE OF THE HELICES PITCH
The general form of the curves, permeate flux against time, is not changed by
changing the pitch but it effected the time necessary to reach the steady state and
its value.
The highest flux is obtained when the baffle has 3 helices every 4 cm (Fig. 3); no
additional pressure drop is observed but the flux decreased when the driving
pressure is higher than 1 bar (Fig. 8). This result is not same as Gupta et al. They
Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt 313
Steady state flux (l/h.m2)
observed that the increase in number of helices per unit length has no effect after
reaching a plateau.
150
120
90
60
30
0
0
1.4
1.6
2.4
3
Helices number/2 cm
Figure 3. Effect of the number of helices per unit length on the steady flux,
1.32 l/min, 1 bar.
The steady state is improved by about 30%, but the pressure drop due to helical
baffle is negligible. In the subsequent experiments, the helical baffle with 3 helices
every 4 cm that gave maximum permeation flux was used.
3.2. INFLUENCE OF THE PRESSURE
The permeate flux decreases with time before reaching the steady state after about
50 minutes except for 0.5 bar where the flux remains noticeably constant (Fig. 4).
Therefore, at 0.5 bar, the fouling is almost avoided and it therefore could be
convenient to operate an industrial membrane at such low pressure. It is probably
the critical flux similar to that defined by Howell et al.. It is remarkable to know
that the critical flux is close to the steady values at high pressures.
500
Flux (l/h.m2)
0.5 bar
400
1 bar
1.5 bars
300
2 bars
200
100
0
0
15
30
45
60
Time (min)
Figure 4. Permeation flux against time for different pressure, 1.32 l/min.
314 Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt
3.3. TRANSIENT FILTRATION
The helical baffle has a beneficial effect on the flux density without changing the
pressure drop. The adequate model, which takes into account both the transient
filtration and the steady state, is the cake deposition with retroflux. The equation
of this model is given by [8,16]:
Qo
−1
t
Q
=k d − k d k p
V
V
(2)
With:
kd =
αx o
AR m
and
kp =
Qr
xo
(3)
Where Q and Qo are respectively the filtrate flow-rate and the initial flow-rate, V
the filtred volume, kd and kp are respectively linked to the deposition and the
retroflux and t the time. Qr is the retroflux flow-rate and xo the volume fraction
occupied by particles in the bulk of the suspension, A is the filtering surface area,
Rm the initial membrane resistance and α the specific resistance per unit length of
deposit.
The linear relation between [(Qo/Q)-1]/V and t/V shown in figure 5 confirms the
validity of the model. The Adjustments are also satisfactory for the feed
concentration. The deposition and retroflux coefficients can be calculated from the
obtained lines.
[(Qo/Q)-1]/V (1/l)
0.5
0.5 bar
0.4
1 bar
1.5 bars
0.3
2 bars
0.2
0.1
0.3
0.4
0.5
0.6
0.7
t/V (h/l)
0.8
0.9
1
Figure 5. Cake deposition with retroflux model for different pressure, 1.2 l/min.
The specific cake resistance against pressure takes the same trend as the cake
coefficient kd, i.e. inversely proportional (Fig. 6). The specific resistance is also
inversely proportional to the feed flow rate (Fig. 7), this phenomenon is not
observed without helical baffle, which explain that using this type of baffles
eliminates the flocculation and the agglomeration of the deposited particles.
Cake resistance (l/m2)
Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt 315
10
8
6
4
2
0
0
0.5
1
1.5
2
2.5
3
Presuure (bar)
Cake specific resistance
(l/m2)
Figure 6. Variation of the specific resistance with the pressure, 1.32 l/min.
16
12
8
4
0
1
1.13
1.2
1.32
1.4
Flow-rate (l/min)
Figure 7. Variation of the specific resistance with the flow rate, 1 bar.
3.4. LIMITING FLUX
We noted that the permeate flux reaches a maximum value at 1 bar and then
decrease very slowly before reaching a plateau (Fig. 8). This is essentially due to
the type of baffle used, which brushes against the internal surface of the
membrane, helping the disruption of the deposit layer at high pressures. The
helical baffle does not do his work. It occupies an important volume of the
membrane tube and creates an obstruction to flow. In presence of another type of
helical baffle, Sebbane [20] showed that the linear part of the curve is more
spread.
Steady state flux (l/h.m2)
316 Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt
200
150
100
50
0
0
0.5
1
1.5
2
2.5
3
Pressure (bar)
Figure 8. Influence of the pressure on the permeate flux, 1.32 l/min.
Steady state flux (l/h.m)
The increase of the feed flow-rate has also a beneficial effect on the permeate flux
(Fig. 9). Beyond 1.2 l/min the flow-rate has no influence on the flux. The cake
already formed could not be pulled out.
160
120
80
40
0
1
1.13
1.2
1.32
Flow-rate (l/min)
Figure 9. Influence of the feed flow-rate on the permeate flux, 1 bar.
Sebbane [20] noted that the turbulence rate at the canal center does not depend on
the Reynolds number, and it is maximal at the neighborhood of the membrane wall
and decreases towards the center at a ratio of the order of 3.
The variations of the steady state flux against the cross-flow velocity in the studied
conditions are linear with a slope equal to 0,68 corresponding to the system of the
flow (Fig. 10). The cross-flow velocity is calculated using free cross sectional
area. The increase of the cross-flow velocity with the influence of helical baffles
leads an increase of turbulence in the membrane tube and mass transfer
coefficient, reduce the effect of concentration polarization and increase the
permeation flux.
Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt 317
5
ln Js
4.8
4.6
4.4
4.2
-0.38
0
0.25
0.4
0.5
ln u
Figure 10. Variation of lnJs with lnUc, 1 bar.
Several authors, using different helical baffles, found similar results. Sebbane
found slope values, close to that of Harriot and Hamilton ones [20], in the order of
0,9 with the helical baffle; in addition they are less sensitive to the evolution of the
fluid vein thickness. On the other hand, without helical baffle they become more
than 1. Quemeneur and Schlumpf [19], Goldsmith [11], Cadanel and Bartoldi [5]
also found, with different devices, slope values of the same order (a=1.1 to 1.5).
Poyen et al. [18] found, with or without helical baffle, in utltrafiltration of an
engine oil additive, slope values equal to 0.6; this is independent of the used
membranes and the hydraulic diameter.
Gekas and Hallstrom [10], Aimar et al. [1] explained the difference in slope values
since the diffusion coefficient, the viscosity and the density (D, and ) depend
on the gel concentration and not on the bulk concentration. Indeed, it is necessary
to know as Jaffrin et al. [14] found that the D and affect the friction at the
membrane wall or the velocity. The oily emulsion could have, as milk, a pseudoplastic behavior. In addition, the influence of the shear should be as much stronger
than the layer is thick.
4. CONCLUSION
The helical baffles allow to increase significantly, by elimination of the formed
layer, the permeate flux without changing the process limiting the transfer flux. At
the optimal conditions, 1 bar and 1.32 l/min, the flux is improved of 30%. The
cake deposition with retroflux model is very satisfactory.
The permeate flux depends, also, on the number of helices per unit length. The
maximum is found for stems behaving 3 helices for every 4 cm and a pressure of 1
bar. At 0.5 bar, the permeate flux remains noticeably constant, it is then the critical
flux as defined by Howell et al.
318 Eighth International Water Technology Conference, IWTC8 2004, Alexandria, Egypt
When a helical baffle is introduced in the filtration element, the progressive
fouling is almost avoided if the driving pressure is maintained at 0.5 bar.
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