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Research Article
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Evaluation of the Mass Transfer Capacity of a Long Tubular Photobioreactor with Static Mixer and its Outdoor Performance with Microalgal Cultures |
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C.U. Ugwu
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H. Aoyagi
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ABSTRACT
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This study was aimed at improving the performance of a long outdoor tubular photobioreactor for high yield of algal biomass. A long tubular photobioreactor (with total tube length of approximately 20 m) was developed. In order to understand the performance of the tubular photobioreactor, hydrodynamics and gas-liquid transfer characteristics, as well as outdoor cultivation of microalgae were evaluated. Parameters that were used to evaluate the gas-liquid transfer characteristics of the photobioreactor included the overall mass transfer coefficient (kLa) and mixing time at various aeration rates (i.e., 0.05 to 0.35 vvm). At 0.35 vvm, presence of 8 static mixers on the riser section at a spacing of 1 m increased the kLa by 25 fold and prolonged the mixing time by 2.7 fold compared to that of the photobioreactor without static mixers. By using the tubular photobioreactor without static mixers, the average biomass productivities attained with Synechocystis aquatilis (S. aquatilis) and Chlorella sorokiniana (C. sorokiniana) were 0.55 and 0.35 g/L/day, respectively. However, upon installation of static mixers, biomass productivities of S. aquatilis and C. sorokiniana increased by 27 and 49% (i.e., 0.70 and 0.52 g/L/day), respectively. This study has indicated that efficiency of a 20 m long tubular photobioreactors and outdoor biomass productivities with the photobioreactor can be significantly improved when static mixers were 1 m apart from each other.
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Received: February 20, 2011;
Accepted: May 07, 2011;
Published: July 02, 2011
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INTRODUCTION
Photobioreactors have attracted much interest in recent years given their potential
uses in growing microalgae (Hoekema et al., 2002;
Oncel and Akpolat, 2006; Ugwu et
al., 2008; Hsieh and Wu, 2009). Photobioreactors
are used for growing microalgae for two major reasons (1) production of high-value
compounds such as vitamins, amino acids and colorants (Akpolat
and Eristurk, 2008; Harith et al., 2010)
and (2) for environmental sustainability (e.g., biofuel, carbon dioxide mitigation,
bioremediation (Yoshihara et al., 1996; Azmat
et al., 2007; Chisti, 2007; Fereshteh
et al., 2007). Of all the photobioreactors proposed to date, tubular
photobioreactor is one of the most commonly studied closed systems for outdoor
cultivation of microalgae (Torzillo et al., 1991;
Lee and Low, 1991; Briassoulis et
al., 2010). Although there are lots of potential advantages of using
tubular photobioreactors, the limitation in scaling it up has restricted its
application in commercial scale. Scaling up of tubular photobioreactor can be
done either by increasing the length or diameter of the tubes (Grima
et al., 1999; Ugwu et al., 2003).
Nevertheless, just like any other type of reactors, any aspect of scaling up
a tubular photobioreactor to a larger scale would result in decrease in the
mass transfer capacity and consequently, would affect the biomass productivity.
If the scale up method is done by increasing the diameter of the tubes, the
availability of light to the cells has to be taken into consideration to avoid
light stratification in the tubes. It was previously reported that static mixers
would ensure efficient mixing, increased mass transfer capacity and better light
utilization in tubular photobioreactors that were scaled up by increasing the
diameter of the tubes (Ugwu et al., 2005). However,
there is yet no report on the use of static mixers in tubular photobioreactors
with their lengths exceeding 4 m. This study was therefore, aimed at improving
the mass transfer capacity of a 20 m long tubular photobioreactor by using suitable
numbers of static mixers, at an appropriate spacing distance with the ultimate
goal of improving the outdoor microalgal productivities.
MATERIALS AND METHODS
Microorganisms and precultivation: Chlorella sorokiniana (C.
sorokinaiana) IAM-212 and Synechocystis aquatilis (S. aquatilis)
SI-2 were used in this study. C. sorokiniana was grown in culture medium
as previously described (Ugwu et al., 2002) while
S. aquatilis was grown in a modified SOT medium which was composed of
(in 1 L): NaHCO3, 5 g; NaNO3, 4 g; K2HPO4,
0.2 g; MgSO4. 7H2O, 0.1 g; Clewat 32 microelemental mixture,
0.05 g; aged sea water, 0.1 L and tap water 900 mL.
For the pre-cultivation, slant cultures were inoculated into 1.5 L Roux flask that contained 1 L of culture medium. Seven daylight fluorescent lamps (8FL-40-s-PG, National Electric, Tokyo) arranged in parallel on a vertical plane were used to provide light intensity of 350 μmol/m2/sec. The culture was operated for 60 h in Roux flask before they were inoculated to the 25 L outdoor tubular photobioreactor.
The outdoor tubular photobioreactor: The tubular photobioreactor is
shown in Fig. 1. It consisted of two parallel transparent
tubes that were connected by manifolds (i.e., the aeration and upper degasser
ports). The total length of the tubes was 20 m (10 m each for the riser and
downcomer sections). The photobioreactor had a total volume of 25 L. Eight static
mixers were inserted on the riser section at a spacing distance of 1 m. The
tubular photobioreactor was inclined at 8 degrees to the horizontal plane.
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Fig. 1: |
A schematic diagram of an inclined tubular photobioreactor.
Aeration and mixing were applied from the riser tube while the liquid flowed
from the riser to the downcomer sections of the photobioreactor |
Table 1: |
Mass transfer characteristics of a 20 m-long tubular photobioreactors
used for the outdoor cultures |
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Detailed information about the characteristics of the tubular photobioreactors
used for outdoor cultures is summarized in Table 1. Aeration
and mixing of the cultures in the tubular photobioreactor were done by sparging
air (with air pump) and then enriching it with 5% CO2 at 0.15 volume
of air per volume of liquid per min (vvm).
The overall volumetric mass coefficient (kLa), mixing time and gas
holdup were measured as previously described (Ugwu et
al., 2002). Liquid velocity was estimated as the distance travelled
by the tracer (to make a significant change in pH) from the injection point
to the degasser port through the riser section. Solid velocity was calculated
using a 5 mg dried algal cells. Thus, the velocity attained by the cells for
a complete cycle within the photobioreactor was estimated. Cell concentration
was determined as follows; 10 mL culture was centrifuged at 5,000 rpm for 5
min and cells were collected, washed with 0.5 M HCl to remove the precipitated
salts and other non-organic substances. The cells were later on rinsed with
distilled water, dried at 105°C for 24 h, cooled over silica gel in a desiccator
and then weighed. The optical density was measured at 680 nm wavelength using
spectrophotometer (Spectronic 20A, Shimadzu, Tokyo, Japan). The solar light
intensity on the surface of the photobioreactor was measured using photorecorder
(PHR-51, T and D Co., Japan). Dissolved oxygen concentrations in the photobioreactors
were measured using DO controller (Mk-250 DO, B.E. Marubishi Co., Japan). Culture
temperature in the photobioreactor was maintained at 30-35°C for C. sorokiniana
by sprinkling the surfaces of the photobioreactor with tap water. In the case
of S. aquatilis, there was no need to sprinkle the reactor with water
since optimum growth of this strain occurs at relatively high temperatures (i.e.,
between 38 and 40°C). The experiment was carried out during the summer of
2003 (at the Agricultural Research Center, University of Tsukuba, Japan. Biomass
productivities were evaluated at solar radiation between 8 and 10 MJ/m2/day.
The culture was operated at a standing biomass concentration of 0.50 g L-1
and then maintained on a semi-continuous mode by daily dilution of the cultures
with fresh medium. Every morning,the optical density of the cells was measured
to estimate the cell concentrations from a predetermined calibration curve.
The increase in the biomass concentration at 06:00-18:00 was calculated as the
daily productivity (g/L/day).
RESULTS AND DISCUSSION
A general approach to scale up a tubular photobioreactor is to increase the
length or diameter of the tubes (Fig. 2). For instance, when
scaling up a small scale tubular photobioreactor, the tube diameter can be kept
constant while the diameter is being increased. The other option is to keep
the tube diameter constant and then increase the length of the tube. Each of
these options has its prospects and demerits as previously reviewed (Ugwu
et al., 2008).
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Fig. 2: |
Scheme for scaling up tubular photobioreactors by increasing
the length or diameter of the tubes |
It should be noted that small diameter tubular photobioreactors are usually
advantageous since they have lower degree of light/dark effect and thus would
provide better biomass productivity compared to large diameter types. However,
inhibition and accumulation of gradients along the tubes has been noted as the
major constraints in this type of photobioreactor. To overcome this kind of
problem, efficient mixing systems are necessary mixers to improve the gas-liquid
transfer in long tubular photobioreactors. Oxygen transfer in bioprocesses is
one of the major parameters for evaluation of productivity (Garcia-Ochoa
and Gomez, 2009; Sauid and Murthy, 2010). Although
increasing the aeration rate would improve oxygen uptake in bioreactors for
non photosynthetic microorganisms (Jafari et al.,
2007; Emily et al., 2009), very high oxygen
accumulation tends to inhibit the growth of photosynthetic microorganisms (Grima
et al., 1999; Ugwu et al., 2008).
This implies that moderate turbulence that will not affect the growth of microalgae
has to be maintained in photobioreactors. Long tubular photobioreactors, in
particular, are prone to accumulation of much higher dissolved oxygen than other
types of photobioreactors (Grima et al., 1999).
To maintain considerable turbulence by aeration in tubular photobioreactors,
vertical mixing system such as static mixers are desirable. We have previously
reported that when vertical mixing was induced by static mixers, movement of
gas and liquid in the tubular photobioreactors efficiently progressed between
the upper and lower sections of the tubes and thus, improved both mass transfer
capacity of the photobioreactors and algal biomass productivities (Ugwu
et al., 2002, 2003). Figure
3 shows the kLa of tubular photobioreactor without static mixers
and the one with 8 static mixers. The kLa increased in both photobioreactors
when the aeration rate was varied from 0.05 to 0.35 vvm, however, there was
no significant difference in their kLa values at the aeration rate
≤0.05. At 0.35 vvm, installation of 8 static mixers in the tubular photobioreactor
resulted in about 25 fold increase in kLa compared to that at 0.05
vvm.
Although static mixers improved the kLa, their presence resulted
in longer mixing time in the tubular photobioreactors. As shown in Fig.
4, the photobioreactor without static mixers had shorter mixing time compared
to the one without static mixers at all the aeration rates tested. By increasing
the aeration rate from 0.05 to 0.35 vvm, the mixing time became shorter in the
photobioreactors. At 0.35 vvm, installing of static mixers in the tubular photobioreactor
prolonged the mixing time by about 2.7 fold compared to that without any static
mixers. There was no significant change in the mixing times of the photobioreactor
with and without static mixers at aeration rate ≤0.05 vvm. Eight static mixers
were the most suitable among other numbers tested and further attempt to increase
the number above 8 resulted in decrease in kLa and greatly elongate
the mixing time.
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Fig. 3: |
Effect of aeration rate on the kLa of a 20 m long
tubular photobioreactor with static mixers and without static mixers |
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Fig. 4: |
Effect of aeration rate on the mixing time of a 20 m long
tubular photobioreactor with static mixers and without static mixers |
Furthermore, when too many static mixers were installed, algal cells became
flocculated to them, making the cleaning process very difficult after the cultivation.
To improve the installation of the mixers, their removal after cultivation,
as well as for better high liquid-gas exchange, the tubular photobioreactors
were inclined at 8 degrees to the horizontal plane. Although the static mixers
were more efficient at higher aeration rate, 0.15 vvm was considered for outdoor
cultures since it was necessary to make a compromise between the mass transfer
(i.e., kLa) and power consumption. In our previous studies, 4 static
mixers that were placed at spacing distances of 0.25 m apart from each other
proved to be the best in terms of kLa and gas holdup (Ugwu
et al., 2002). However, with the long tubular photobioreactor, such
as the type used in this study indicated that higher aeration rate (greater
than 0.15 vvm) would induce too much turbulence which consequently resulted
in culture crash at the beginning of the experiment. In light of this, the characteristics
features of the tubular photobioreactor with static mixers, indicated a relatively
high mass transfer properties (i.e., kLa, gas holdup, mixing time,
liquid velocity and solid velocity) that were enough to generate good liquid-gas
transfer and thus improved the biomass productivities.
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Fig. 5: |
Outdoor biomass productivities of C. sorokiniana and
S. aquatilis in 20 m long tubular photobioreactor with static mixers
and without static mixers. Three replicate experiments for each of the data
was obtained at 8-10 MJ/m2/day solar radiation |
In this study, the maximum kLa of 0.0025 sec-1 was obtained
at an aeration rate of 0.35 vvm (superficial gas velocity = 0.14 m sec-1).
However, Babcock et al. (2002) reported the maximum
kLa of 0.0022 sec-1 at a superficial gas velocity of 0.025
m sec-1 for a near-horizontal tubular photobioreactor. In an external-loop
airlift tubular which was tested for outdoor cultures of Phaeodactylum tricornutum,
kLa of 0.006 sec-1 was obtained at a superficial gas velocity
of 0.25 m sec-1 (Fernandez et al., 2001).
Figure 5 shows the outdoor biomass productivities of C.
sorokiniana and S. aquatilis that were carried out at solar radiation
between 8 and 10 MJ/m2/day. In the tubular photobioreactor without
static mixers, the biomass productivities for S. aquatilis and
C. sorokiniana were 0.55 and 0.35 g/L/day, respectively. On the other hand,
biomass productivities obtained with S. aquatilis and C. sorokiniana
using the tubular photobioreactor with static mixers were 0.70 and 0.52 g/L/day,
respectively. Higher productivity in S. aquatilis culture can be attributed
to the fact that the strain grows very fast and has optimum growth at high temperatures
above 40°C (Zhang et al., 2002). This implies
that high temperature which is common in summer will rather favor the growth
of this strain. On the other hand, C. sorokiniana cannot withstand temperatures
above 38°C and thus there is a need to sprinkle the tubes with cool tap
water during the outdoor cultures. High dissolved oxygen concentration in narrow
diameter tubular photobioreactors has been reported (Weissman
et al., 1988). In this study, 8 static mixers were efficient in reducing
the dissolved oxygen concentration in the long tubular photobioreactor by 30%.
By using tubular photobioreactor with static mixers, the increase in biomass
productivities compared to the one without static mixers in S. aquatilis
and C. sorokiniana cultures were 27 and 49%, respectively.
CONCLUSION
This study has apparently shown that gas-liquid transfer rate of a 20 m long
tubular photobioreactor was improved upon installation of 8 static mixers on
its riser section at a spacing distance of 1 m apart from each other. Furthermore,
when outdoor biomass cultures of S. aquatilis and C. sorokiniana
were performed with the tubular photobioreactor at an aeration rate of 0.15
vvm, significant improvement in the biomass productivities was observed. In
addition, the static mixers reduced the accumulated dissolved concentration
in the culture by 30%.
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