<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JBNB</journal-id><journal-title-group><journal-title>Journal of Biomaterials and Nanobiotechnology</journal-title></journal-title-group><issn pub-type="epub">2158-7027</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbnb.2013.42A001</article-id><article-id pub-id-type="publisher-id">JBNB-29819</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Growth Enhancement of Dunaliella salina by Microbubble Induced Airlift Loop Bioreactor (ALB)—The Relation between Mass Transfer and Growth Rate
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ezhen</surname><given-names>Ying</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Daniel</surname><given-names>J. Gilmour</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yuzhen</surname><given-names>Shi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>William</surname><given-names>B. Zimmerman</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Chemical and Biological Engineering, University of Sheffield, Sheffield, UK</addr-line></aff><aff id="aff2"><addr-line>Department of Molecular Biology and Biotechnology, University of Sheffield, Sheffield, UK</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>cpp09ky@sheffield.ac.uk(EY)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>04</month><year>2013</year></pub-date><volume>04</volume><issue>02</issue><fpage>1</fpage><lpage>9</lpage><history><date date-type="received"><day>January</day>	<month>15th,</month>	<year>2013</year></date><date date-type="rev-recd"><day>February</day>	<month>17th,</month>	<year>2013</year>	</date><date date-type="accepted"><day>April</day>	<month>4th,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   The efficiency of a novel microalgal culture system (an airlift loop bioreactor [ALB] engaged with a fluidic oscillator to produce microbubbles) is compared with both a conventional ALB (producing fine bubbles without the fluidic oscillator) and non-aerated flask culture. The impact of CO<sub>2</sub> mass transfer on Dunaliella salina growth is assessed, through varying the gas (5% CO<sub>2</sub>, 95% N<sub>2</sub>) dosing flow rate. The results showed that approximately 6 - 8 times higher chlorophyll content was achieved in the aerated ALB cultures than in the non-aerated flasks, and there was a 20% - 40% increase in specific growth rate of D. salina in the novel ALB with microbubbles when compared with the conventional ALB cultures. The increase in chlorophyll content was found to be proportional to the total amount of CO<sub>2</sub> mass transfer. For the same dosing time and flow rate, higher CO<sub>2</sub> mass transfer rate (microbubble dosing) resulted in a greater growth rate.
     
 
</p></abstract><kwd-group><kwd>Airlift Bioreactor; Fluidic Oscillator; &lt;i&gt;Dunaliella salina&lt;/i&gt;; Specific Growth Rate</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Microalgae have been considered for CO<sub>2</sub> capture from flue gas by many industries recently, due to their high CO<sub>2</sub> uptake efficiencies which are one order of magnitude (10 to 50 times) higher than those of terrestrial plants [<xref ref-type="bibr" rid="scirp.29819-ref1">1</xref>]. Industry is one of the major CO<sub>2 </sub>producers and fossil fuel consumers, responsible for more than 7% of total world CO<sub>2</sub> emissions [<xref ref-type="bibr" rid="scirp.29819-ref2">2</xref>], while the flue gas produced, containing various percentages of CO<sub>2</sub>, actually can provide a carbon-rich source for microalgae cultivation. Microalgae capture CO<sub>2</sub> for their growth, saving the costs of adding CO<sub>2 </sub>scrubbing systems [<xref ref-type="bibr" rid="scirp.29819-ref3">3</xref>]. Some microalgae species show a good tolerance to NO<sub>x</sub>/SO<sub>x</sub>, and can even capture them as nutrients for growth [4,5]. The products from microalgae culture can be used as food, animal feed, fertilizers, valuable chemicals and as a source of biofuel production etc. [6,7]. These high value commercial products can be expected to offset the capital and operating costs.</p><p>Many studies have demonstrated the correlation between light intensity and algal productivity based on the assumption of unlimited CO<sub>2</sub> supply, however, in practice CO<sub>2</sub> mass transfer was always limited due to conventional bubble dosing. In order to achieve sufficient CO<sub>2</sub> dissolution, higher dosing rate and longer dosing time (e.g. 24 hrs/d) were employed to compensate for the lower mass transfer. Nevertheless, by doing so, under higher aerating flow rate, most of the gas was wasted due to low mass transfer, and the intensive agitation could cause damage to the algal cells. Besides, longer dosing time means more energy consumption which would result in a low yield/power ratio. Therefore, design of a CO<sub>2</sub> dosing system with a relatively high gas mass transfer and low energy cost tends to be a major consideration for cost-competitive microalgae culture. Since an energy efficient microbubble dosing system has been developed [<xref ref-type="bibr" rid="scirp.29819-ref8">8</xref>] and proved to have a relatively higher mass transfer coefficient than normal bubble dosing [9,10], the same level of dissolved CO<sub>2</sub> concentration can be achieved at relatively lower dosing flow rate, consequently, considerable energy saving along with higher productivity will be made. To further study the impact of microbubbles produced by fluidic oscillation, a range of ALB bench cultures of D. salina were set up to discover 1) the contrast between aerated ALB cultures and non-aerated flask cultures, 2) the difference between microbubble dosing and fine-bubble dosing and 3) the correlation between mass transfer and D. salina growth.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Design of Lab Scale Airlift Loop Bioreactor (ALB)</title><p>Zimmerman et al. [<xref ref-type="bibr" rid="scirp.29819-ref11">11</xref>] introduced the design of the microbubble mediated ALB for a large lab scale 250 L volume. To further study the impact of using innovative ALB on microalgal cultivation, twelve 3L-ALBs were made for screening purposes, based on a similar design. <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref> shows the configuration of a 3L-ALB. Generally, the bioreactor is made of acrylic material, with the dimension of 285 mm in height and 124 mm in diameter. The air lift loop design consists of a ceramic diffuser (diameter of 78 mm, pore size of 20 &#181;m) fixed at bottom and an internal draught tube (H: 170 mm, D: 95 mm) hung 30 mm above the diffuser. The flow pattern of airlift loop has been discussed in detail in previous studies [9,10,12].</p></sec><sec id="s2_2"><title>2.2. Experimental Setup and Processes</title><p>The experimental setup for lab bench ALB cultures is shown in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>. Generally, twelve ALBs were arranged into two rows. Each row contains a flask culture and five ALB cultures under different dosing conditions (0.3 L·min<sup>−1</sup>, 0.5 L·min<sup>−1</sup>, 0.7 L·min<sup>−1</sup>, 0.9 L·min<sup>−1</sup> and 1.1 L·min<sup>−1</sup>, all under 1 atm pressure). For each ALB culture flow rate was monitored through the rotameter directly connected to the output port of ALB. For the five ALBs connected to a fluidic oscillator (FO) CO<sub>2</sub> was dosed through microbubbles (300 &#181;m), while another five ALBs were dosed with fine-bubbles (600 &#181;m). The two flask cultures (without gas dosing) were run in parallel for error estimates. Two fluorescent lamps, one per each row, provided continuous illumination of 90 &#181;mol·m<sup>−2</sup>·s<sup>−1</sup>. The temperature for each culture was maintained around 24˚C, due to the empirical heat transfer from the fluorescent lamps. The algal species for this study was Dunaliella salina [<xref ref-type="bibr" rid="scirp.29819-ref12">12</xref>], which has a wide pH range from 6 to 9. The strain was obtained from the Culture Centre of Algae and Protozoa, SAMS, Oban, UK as CCAP 19/30. The unbuffered culture medium i.e. without 20 mM HEPES buffer, is shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>D. salina was pre-cultured in a growth room (25˚C &#177; 2˚C, light intensity 50 &#181;mol·m<sup>−2</sup>·s<sup>−1</sup>) in a similar culture medium, but with added HEPES (20 mM) as a buffer (pH 7.5). At the beginning of the main experiments, 50 ml of pre-cultured D. salina was added to 2.5 L of fresh culture medium for each culture. Each ALB culture was</p><p><xref ref-type="table" rid="table1">Table 1</xref>. D. salina culture medium.</p><p><img src="1-3200254\4b4c67d5-c3a5-4758-b56b-cd4a6ed1706e.jpg" /></p><p>dosed with CO<sub>2</sub> enriched gas (5% CO<sub>2</sub>, 95% N<sub>2</sub>) for 30 minutes per day. 50 ml algal samples were taken after gas dosing or mixing (for flask cultures), followed by topping up the culture with 50 ml of fresh medium. pH and DO levels in each of the bioreactors were measured daily before and after gas dosing using a SevenGo Duo Pro pH/DO meter.</p></sec><sec id="s2_3"><title>2.3. Analysis Methods</title><sec id="s2_3_1"><title>2.3.1. Measurements of Algal Growth</title><p>The chlorophyll content of the samples of D. salina culture taken each day was determined by measuring the optical density at wavelengths of 645 nm and 663 nm using the method described by Zimmerman et al. [<xref ref-type="bibr" rid="scirp.29819-ref12">12</xref>]. The overall specific growth rate were obtained at the end of the culture growth period as described by Scragg [<xref ref-type="bibr" rid="scirp.29819-ref13">13</xref>], which was estimated from the slope of a semilog plot of ln(C<sub>t</sub>/C<sub>0</sub>) versus t.</p></sec><sec id="s2_3_2"><title>2.3.2. Measurements for CO<sub>2</sub> Uptake Estimation</title><p>The CO<sub>2</sub> concentration dissolved in the medium was calculated from the current pH using Equation (2), of which the detailed derivation is shown in Appendix A.</p><disp-formula id="scirp.29819-formula6075"><label>(2)</label><graphic position="anchor" xlink:href="1-3200254\1e525077-6880-48c5-af7d-59d076a08f8a.jpg"  xlink:type="simple"/></disp-formula><p>Each day, the difference between the concentration of dissolved CO<sub>2</sub> before and after dosing, calculated based on the pH, indicates the amount of CO<sub>2 </sub>that has been transferred into the medium (dosed CO<sub>2</sub>). The reading taken the following day before dosing indicates the decrease in the dissolved CO<sub>2 </sub>and gives the amount of CO<sub>2 </sub>uptake by D. salina.</p></sec></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Comparisons between ALB Culture and Conventional Flask Culture</title><sec id="s3_1_1"><title>3.1.1. Chlorophyll Content</title><p><xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref> gives the plot of chlorophyll content versus culture time for ALB cultures and flask cultures. Generally, the D. salina cells cultured in ALB, either with or without fluidic oscillator engaged, were growing faster compared with the flask culture. As can be seen in <xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref>, for the flask culture, without daily gas supply the microalgae were growing relatively slowly, with the chlorophyll content increasing from about 0.15 mg·L<sup>−1</sup> to eventually 4.30 mg·L<sup>−1</sup> through 18 days. In contrast, the algal chlorophyll content in all ALB cultures increased from the similar initial concentration to an even higher point (4.73 - 7.24 mg·L<sup>−1</sup>) within only 6 days. For these ALB cultures, the active growth phase started from the third day and lasted about 13 days, with the peak varying from 26.43 to 32.65 mg·L<sup>−1</sup> (depending on flow rate and dosing method). Entry into stationary phase was observed after about 15 days. In general, about 6 - 8 times higher chlorophyll content was achieved in ALB cultures</p><p>than in the flask cultures for the same culture period. It is easily understood that the ALB engaged with microbubble/fine-bubble dosing enables a high mass transfer of CO<sub>2</sub> dissolution and O<sub>2</sub> removal, which makes the culture both CO<sub>2</sub> sufficient and O<sub>2</sub> stripped, therefore, algae grew better in such “well served” circumstances. Zimmerman et al. [<xref ref-type="bibr" rid="scirp.29819-ref12">12</xref>] demonstrated a pilot scale microalgal culture using a similar design of ALB as in this study, the results also showed that such ALB culture was neither CO<sub>2</sub> limited nor O<sub>2</sub> inhibited, which led to a high algal growth rate.</p></sec><sec id="s3_1_2"><title>3.1.2. pH Changes</title><p>Apart from the relatively higher CO<sub>2</sub> mass transfer and an appreciable O<sub>2</sub> stripping by “micro/fine-bubbling”, a better pH control is also one of the reasons that explain why ALB cultures exceeded the flask cultures in productivity. Commonly, pH in the culture medium increases as the algae grows, and when the pH increases beyond the optimum range, the culture may be adversely affected. As algae grow, the photosynthetic uptake of CO<sub>2</sub> leads to the increase in pH, but as a consequence of increasing pH, <img src="1-3200254\a93d0553-516e-4ca9-8b4b-59a2a2ab86d4.jpg" />increases while <img src="1-3200254\82ec877b-c229-4f69-b886-c5f7ad5b847f.jpg" /> and CO<sub>2</sub> decrease, which inhibits the photosynthetic reaction and improves the rate of algal respiration [<xref ref-type="bibr" rid="scirp.29819-ref14">14</xref>]. Therefore, for many algal cultures, either buffer solutions (e.g. HEPES) are usually included in culture medium or acid is added when pH increases over a suitable level via an auto-controlled system. However, in this study, neither buffer solution nor acid is added, because it was expected that the increasing pH could be neutralized by daily CO<sub>2</sub> supply via microbubble dosing technique, and indeed the results strongly supported this hypothesis.</p><p><xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref> shows the daily pH changes in ALB cultures (either with or without fluidic oscillator) and in control experiment (flask cultures). For control experiment, because of the absence of CO<sub>2</sub> supply and the accumulation of O<sub>2</sub>, D. salina grew relatively slowly in the first 9 days, with its chlorophyll content increased from 0.15 mg·L<sup>−1</sup> to only 3.04 mg·L<sup>−1</sup> (<xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref>). Correspondingly, its pH also increased slowly, rising from 7.9 to 9.1 through the first 9 days (<xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref>). However, after 9 days the pH barely increased and was maintained at 9.1 - 9.5, whilst the algae almost stopped growing as well, with its chlorophyll content maintained at 3.04 - 3.33 mg·L<sup>−1</sup>. One of the reasons is that, after pH went above 9 the culture was inhibited, because for most microalgae the suitable pH ranges from 6 to 9 [<xref ref-type="bibr" rid="scirp.29819-ref15">15</xref>], and over this range inhibition of</p><p>growth occurs. In terms of ALB cultures (FO engaged or not), chlorophyll increased dramatically (from around 0.05 - 0.15 mg·L<sup>−1</sup> to 26.43 - 32.65 mg·L<sup>−1</sup>) until the growth entered steady phase (the last 3 days). Correspondingly, pH was supposed to rise even faster than control culture, however, due to daily micro-bubble (300 μm) or fine-bubble (600 μm) dosing, the culture pH was maintained in a suitable range of 6.5 - 8.5 (<xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref>). As can be seen, for each day, after 30 min of 5% CO<sub>2</sub> dosing, pH was reduced to around 7, but because of the desirable culture condition (CO<sub>2</sub> unlimited and O<sub>2</sub> free), pH increased back to about 9 within only one day. The next day, another 30 min of dosing dragged it back to around 7 again. Such a virtuous cycle kept pH within a desirable range, making the culture also not limited by pH.</p><p>One thing needs to be clarified that for all ALB cultures in this study, the pH value seems to be similar despite the different dosing flow rates or dosing methods. But theoretically, for various dosing conditions with different mass transfer capabilities, the dissolved CO<sub>2</sub> in the culture medium differs, correspondingly, the pH value indicating the amount of dissolved CO<sub>2</sub> differs as well. Such a ‘contradiction’ can be explained by <xref ref-type="table" rid="table2">Table 2</xref>. As can be seen, one magnitude of difference in the concentration (mol/L) of dissolved CO<sub>2</sub> only changes the pH by one unit, while the difference in the total CO<sub>2 </sub>mass transfers (daily) for this study are in the range of 10<sup>−4</sup> to 10<sup>−3</sup> mol/L, for different dosing conditions. Therefore, the difference in the pH value was barely affected by the different mass transfer capabilities. This also supports the hypothesis that the pH was scientifically controlled in the study, and it can be considered as a controlled parameter when comparing the impact of mass transfer on the algal growth (see 3.2).</p></sec></sec><sec id="s3_2"><title>3.2. Comparisons between FO Engaged ALB Culture and Conventional ALB Culture</title><sec id="s3_2_1"><title>3.2.1. Effect of Fluidic Oscillator (Comparing Microbubble Dosing with Fine Bubble Dosing)</title><p><xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref> shows the comparison between the ALB cultures with fluidic oscillator engaged and normal ALB</p><p><xref ref-type="table" rid="table2">Table 2</xref>. The corresponding dissolved CO<sub>2</sub> for different pH values. The amount of CO<sub>2</sub> was calculated based on Equation (2) and on the particulate NaHCO<sub>3</sub> concentration in medium.</p><p><img src="1-3200254\d54e450f-480c-4e5f-a0f2-f2d5e1ef02ca.jpg" /></p><p>culture. Generally, for each dosing flow rate D. salina grew better in FO engaged ALBs (microbubble dosing) than in normal ALBs (fine-bubble dosing). The peak chlorophyll content reached 27.03 - 32.65 mg·L<sup>−1</sup> when FO was applied, while only 23.13 - 26.47 mg·L<sup>−1</sup> was achieved without FO. To quantify the comparison of D. salina growth under different dosing conditions, the overall specific growth rate was estimated from the slope of a semilog plot of ln(C<sub>t</sub>/C<sub>0</sub>) versus time. Hence the specific growth rate under each ALB dosing condition was obtained, which was plotted in <xref ref-type="fig" rid="fig5"><xref ref-type="fig" rid="fig">Figure </xref>5</xref>. Generally, fluidic oscillator engaged ALB cultures presented a higher algal specific growth rate (μ), showing an approximately 20% - 40% enhancement compared with conventional ALB cultures. The highest specific growth rate (near 0.13 d<sup>−1</sup>) for normal ALB culture was achieved at a dosing flow rate of 1.1 L·min<sup>−1</sup>, while the similar specific growth rate for ALB culture (with FO) was achieved at only 0.1 L·min<sup>−1</sup>, which shows a considerable energy saving potential.</p></sec><sec id="s3_2_2"><title>3.2.2. Effect of Flow Rate (Comparing the Impact of Different Dosing Flow Rates on D. salina Growth)</title><p>Generally, the specific growth rate (μ) was found to increase along with dosing flow rate, either with or without FO engaged. The maximum μ of 0.13 d<sup>−1</sup> and 0.17 d<sup>−1</sup> was achieved at flow rate of 0.9 L·min<sup>−1</sup> (without FO) and at 1.1 L·min<sup>−1</sup> (with FO), respectively. This overall trend was found similar to gas-liquid mass transfer study [<xref ref-type="bibr" rid="scirp.29819-ref10">10</xref>] (see Figures S1(a) and (b) in Supplementary information). Considering both algal specific growth rate</p><p>(<xref ref-type="fig" rid="fig5"><xref ref-type="fig" rid="fig">Figure </xref>5</xref>) and mass transfer coefficient (Figures S1(a) and (b)) under different dosing flow rates, the algal growth appears to be correlated to mass transfer via following hypothesis.</p><p>For the ALB cultures with fine-bubble dosing (NoFO), within the flow rate range of 0.3 - 1.1 L·min<sup>−1</sup>, mass transfer coefficient K<sub>l</sub>a (either for CO<sub>2</sub> dissolution or for O<sub>2</sub> removal) increased with flow rate, and consequently CO<sub>2</sub> dissolution and O<sub>2</sub> stripping efficiency were enhanced. The culture therefore had more dissolved CO<sub>2</sub> available for algal uptake and less O<sub>2</sub> inhibition. Thus, specific growth rate increased as the flow rate went up. The same scenario was observed for the novel ALB cultures (microbubble dosing) under the flow rate of 0.3 - 0.7 L·min<sup>−1</sup>. However, the specific growth rate did not significantly increase by further increasing the flow rate when it exceeded 0.7 L·min<sup>−1</sup>. This can be explained by assuming that for 0.3 - 1.1 L·min<sup>−1</sup> of dosing (ALB cultures, NoFO) and 0.3 - 0.7 L·min<sup>−1</sup> of dosing (ALB cultures, FO), the daily total amount of CO<sub>2</sub> mass transfer (average CO<sub>2</sub> mass transfer rate &#215; dosing time) did not reach or exceed the saturation concentration, therefore higher mass transfer led to a greater amount of available CO<sub>2</sub>, which consequently resulted in a higher growth rate. For the flow rate of 0.9 - 1.1 L·min<sup>−1</sup> with mcirobubble dosing, the total CO<sub>2</sub> mass transfer is likely to be excessive (average CO<sub>2</sub> mass transfer rate &#215; dosing time &gt; CO<sub>2</sub> saturation). The extra CO<sub>2</sub> was therefore released to the atmosphere and did not contribute to the algal growth. Thus increasing the flow rate over a valid range may not effectively improve the growth. Based on the above discussion, 30 min·d<sup>−1</sup> of dosing under 0.7 L·min<sup>−1</sup>, close enough to reach CO<sub>2</sub> saturation, turns out to be the optimal dosing condition for the 3L-ALB culture (with microbubble dosing).</p></sec></sec><sec id="s3_3"><title>3.3. Relation between CO<sub>2</sub> Mass Transfer and D. salina Growth</title><p>For the ALB cultures under each condition, the amount of total CO<sub>2</sub> uptake and the increase in the chlorophyll content were calculated for certain culture periods, which are shown in <xref ref-type="fig" rid="fig6"><xref ref-type="fig" rid="fig">Figure </xref>6</xref>(a). The chlorophyll content increase shown was found commensurate with the amount of CO<sub>2</sub> uptake within the same culture period. It can be simply understood by the basic photosynthetic equation 6CO<sub>2 </sub>(aq) + 12H<sub>2</sub>O (liq) + photons → C<sub>6</sub>H<sub>12</sub>O<sub>6</sub> (aq) + 6O<sub>2</sub> (g) + 6H<sub>2</sub>O (liq), the amount of algal growth is speculated to be proportional to the CO<sub>2</sub> concentration. An equation describing the relation between chlorophyll increase and CO<sub>2</sub> consumption for the D. salina cultures in this study is therefore obtained via linear regression.</p><disp-formula id="scirp.29819-formula6076"><label>(3)</label><graphic position="anchor" xlink:href="1-3200254\7d53d685-4932-4ed5-840f-b86334d72314.jpg"  xlink:type="simple"/></disp-formula><p>Therefore, an assumption can be made that in the same time period, the CO<sub>2</sub> uptake rate should be proportional to the instant algal concentration (chlorophyll content), which is shown as follows:</p><p><img src="1-3200254\e77cbd8c-67cd-46a6-b736-ac7673270b4a.jpg" /></p><p>where μ is the overall specific growth rate (constant for a certain culture condition); V<sub>Chl</sub> and <img src="1-3200254\e398f996-4f21-408d-bc29-09089e39f2c6.jpg" /> represent chlorophyll growth rate and CO<sub>2</sub> uptake rate, respectively; [Chl] and [CO<sub>2</sub>] mean the chlorophyll content and CO<sub>2</sub> concentration, separately.</p><p>Indeed, the experimental data, shown in <xref ref-type="fig" rid="fig6"><xref ref-type="fig" rid="fig">Figure </xref>6</xref>(b), strongly support this assumption. The daily CO<sub>2</sub> uptake rate is in direct proportion to the concentration of chlorophyll content, of which the equation is shown as</p><disp-formula id="scirp.29819-formula6077"><label>. (4)</label><graphic position="anchor" xlink:href="1-3200254\2c4feb3b-b0fe-4205-b4c9-dc2c2b7d6c5e.jpg"  xlink:type="simple"/></disp-formula><p>In order to correlate the algal growth to CO<sub>2</sub> mass transfer, the correlations between the amount of CO<sub>2</sub> uptake and the CO<sub>2</sub> transferred to the liquid still needs to be understood, which is presented in <xref ref-type="fig" rid="fig6"><xref ref-type="fig" rid="fig">Figure </xref>6</xref>(c). As can be seen, the amount of daily CO<sub>2</sub> uptake was equal to the valid amount of CO<sub>2</sub> dosed, which can be described as:</p><disp-formula id="scirp.29819-formula6078"><label>, (5)</label><graphic position="anchor" xlink:href="1-3200254\f1311143-ea0a-4fe1-807c-b269e078df21.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-3200254\57916d2d-f88f-4336-b882-4b7f9a8c8e99.jpg" /> represents CO<sub>2</sub> average mass transfer rate; t<sub>dosing</sub> means the dosing time.</p><p>By combining Equation (3) and Equation (5), it gives</p><disp-formula id="scirp.29819-formula6079"><label>. (6)</label><graphic position="anchor" xlink:href="1-3200254\30397999-6bc0-4730-87ce-1446d8690a5e.jpg"  xlink:type="simple"/></disp-formula><p>From Equation (6), the chlorophyll content increase has been shown to be in direct proportion to the mass transfer rate for the ALB cultures in this study, which again explains why the ALB cultures with microbubble dosing have higher growth rates than the ones with finebubble dosing.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>An about 6 to 8 times enhancement of D. salina growth was found in ALB cultures, compared with the flask incubation. Instead of buffer solution (e.g. HEPES), daily 30 minutes of 5% CO<sub>2</sub> gas dosing maintained pH at a suitable level (6.5 - 8.5). Besides approximately 20% -</p><p>40% increase in specific growth rate was found in the FO engaged ALB cultures, over a wide range of gas dosing flow rate. Furthermore, the chlorophyll content (growth) was found to be directly proportional to the mass transfer rate for D. salina ALB cultures. Further modelling of these observations is being carried out.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>WZ would like to thank the Royal Society for a Brain Mercer Innovation Award. We acknowledge support for microbubble dynamics from EPSRC. DJG would like to acknowledge support from Carbon Trust.</p></sec><sec id="s6"><title>REFERENCES</title></sec><sec id="s7"><title>Appendix: [CO<sub>2</sub>] Estimation Based on pH in Medium (with NaHCO<sub>3</sub>)</title><p>The dissolved CO<sub>2</sub> is in equilibrium with <img src="1-3200254\3e556bbc-deb7-45c9-a49d-83a3c29e4dfa.jpg" /> and<img src="1-3200254\064a3d84-d1eb-4654-a317-f188d9e65471.jpg" />, which can be described by the following chemical reactions [16,17].</p><p><img src="1-3200254\7187a814-1c58-497f-a66a-2403321b914b.jpg" /><img src="1-3200254\e04e0425-fa38-4b10-b659-88d196cc8cc4.jpg" /><img src="1-3200254\1e7468cf-3e98-4816-acb7-b529b1d96b16.jpg" /></p><p>where the relevant equilibrium constants are:</p><p><img src="1-3200254\a1919433-5e77-49b4-84ce-31e82233aaf2.jpg" /></p><p><img src="1-3200254\257de621-e823-4d09-b2f2-443a0fab6f49.jpg" /></p><p><img src="1-3200254\baf4958c-f872-4576-ac02-b0cc30fc9c77.jpg" />.</p><p>The system must satisfy the electro-neutrality constraint, therefore</p><p><img src="1-3200254\4679ef66-1158-4cb4-8824-c43300386a45.jpg" /></p><p>Assuming constant concentrations of other cations and anions, it gives</p><p><img src="1-3200254\99a02d5d-706f-4942-a4d1-982b8d8fbcf2.jpg" /></p><p>By solving above equations, it gives</p><disp-formula id="scirp.29819-formula6080"><label>(1)</label><graphic position="anchor" xlink:href="1-3200254\ec24db98-b932-4d36-9d67-88efada27928.jpg"  xlink:type="simple"/></disp-formula><p>However Equation (1) can only be used to calculate the concentration of CO<sub>2</sub> in water and when the pH is less than 7. For the [CO<sub>2</sub>] estimation in the medium containing NaHCO<sub>3</sub> modification needs to be made. The system would still need to satisfy the electro-neutrality constraint. But since NaHCO<sub>3</sub> is added into medium, other cations and anions are not equal.</p><p><img src="1-3200254\8294f9e1-b774-4227-9c63-df9cd291289d.jpg" /></p><p>Therefore, the additional amount of Na<sup>+ </sup>needs to be taken into consideration:</p><p><img src="1-3200254\dc2c30b7-bcc2-47d1-8cb6-9212207ab8bf.jpg" /></p><p>Finally, Equation (1) is modified as:</p><disp-formula id="scirp.29819-formula6081"><label>(2)</label><graphic position="anchor" xlink:href="1-3200254\d2f30f8f-2489-4d3d-add2-0316f02f17d2.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s8"><title>Supplementary Information: The Relation between Mass Transfer and Dosing Flow Rate</title><p><img src="1-3200254\742a359d-aab7-4fdf-ada9-fd1482ba4feb.jpg" /></p><p>(a)</p><p><img src="1-3200254\0584cc5e-1e6f-47c8-b098-6976728b0866.jpg" /></p><p>(b)</p><p><xref ref-type="fig" rid="fig">Figure </xref>S1. (a) Effect of FO on mass transfer coefficient for carbon dioxide dissolution; (b) Effect of FO on mass transfer coefficient for oxygen removal [<xref ref-type="bibr" rid="scirp.29819-ref10">10</xref>].</p></sec></body><back><ref-list><title>References</title><ref id="scirp.29819-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Y. Li, M. Horsman, B. Wang, N. Wu and C. Q. Lan, “Effects of Nitrogen Source on Cell Growth and Lipid Accumulation of Green Alga Neochloris oleoabundans,” Applied Microbiology and Biotechnology, Vol. 81, No. 4, 2008, pp. 629-636. doi:10.1007/s00253-008-1681-1</mixed-citation></ref><ref id="scirp.29819-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">N. Sakai, Y. Sakamoto, N. Kishimoto, M. Chihara and I. Karube, “Chlorella Strains from Hot Springs Tolerant to High Temperature and High CO2,” Energy Conversion and Management, Vol. 36, No. 6-9, 1995, pp. 693-696. 
doi:10.1016/0196-8904(95)00100-R</mixed-citation></ref><ref id="scirp.29819-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">B. Wang, Y. Li, N. Wu and C. Q. Lan, “CO2 Bio-Mitigation Using Microalgae,” Applied Microbiology and Biotechnology, Vol. 79, No. 5, 2008, pp. 707-718. 
doi:10.1007/s00253-008-1518-y</mixed-citation></ref><ref id="scirp.29819-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">H. Matsumoto, A. Hamasaki, N. Sioji and Y. Ikuta, “Influence of CO2, SO2 and NO in Flue Gas on Microalgae Productivity,” Journal of Chemical Engineering of Japan, Vol. 30, No. 4, 1997, pp. 620-624.  
doi:10.1252/jcej.30.620</mixed-citation></ref><ref id="scirp.29819-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">H. Nagase and K. Eguchi, “Improvement of Microalgal Nox Removal in Bubble Column and Airlift Reactors,” Journal of Fermentation and Bioengineering, Vol. 86, No. 4, 1998, pp. 421-423. 
doi:10.1016/S0922-338X(99)89018-7</mixed-citation></ref><ref id="scirp.29819-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">P. Chelf, L. M. Brown and C. E. Wyman, “Aquatic Biomass Resources and Carbon Dioxide Trapping,” Biomass Bioenergy, Vol. 4, No. 3, 1993, pp. 175-183. 
doi:10.1016/0961-9534(93)90057-B</mixed-citation></ref><ref id="scirp.29819-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">M. A. Borowitzka and L. J. Borowitzka, “Micro-Algal Biotechnology,” Cambridge University Press, Cambridge, 1988.</mixed-citation></ref><ref id="scirp.29819-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">W. B. Zimmerman, V. Tesar and H. C. H. Bandalusena, “Towards Energy Efficient Nanobubble Generation with Fluidic Oscillation,” Current Opinion in Colloid &amp; Interface Science, Vol. 16, No. 4, 2011, pp. 350-356. 
doi:10.1016/j.cocis.2011.01.010</mixed-citation></ref><ref id="scirp.29819-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">M. K. H. Mashhadani, H. C. H. Bandalusena and W. B. Zimmerman, “CO2 Mass Transfer Induced through an Airlift Loop by a Microbubble Cloud Generated by Fluidic Oscillation,” Industrial &amp; Engineering Chemistry Research, Vol. 51, No. 4, 2012, pp. 1864-1877.  
doi:10.1021/ie200960v</mixed-citation></ref><ref id="scirp.29819-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">K. Ying, K. H. M. Al-Mashhadani and W. B. Zimmerman, “The Effect of Flow Rate on Enhancement of O2 Removal and CO2 Dissolution by Using Novel Microbubble Generation System in Airlift Bioreactor,” Unpublished, 2012.</mixed-citation></ref><ref id="scirp.29819-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">W. B. Zimmerman, B. N. Hewakandamby, V. Tesar, H. C. H. Bandalusena and O. A. Omotowa, “On the Design of Simulation of an Airlift Loop Bioreactor with Microbubble Generation by Fluidic Oscillation,” Food and Bioproducts Processing, Vol. 87, No. 3, 2009, pp. 215-227. 
doi:10.1016/j.fbp.2009.03.006</mixed-citation></ref><ref id="scirp.29819-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">W. B. Zimmerman, M. Zandi, H. C. H. Bandulasena, V. Tesar, D. J. Gilmour and K. Ying, “Design of an Airlift Loop Bioreactor and Pilot Scales Studies with Fluidic Oscillator Induced Microbubbles for Growth of a Microalgae Dunaliella Salina,” Applied Energy, Vol. 88, No. 10, 2011, pp. 3357-3369.  
doi:10.1016/j.apenergy.2011.02.013</mixed-citation></ref><ref id="scirp.29819-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">A. H. Scragg, “Bioreactors in Biotechnology: A Practical Approach,” Ellis Horwood, London, 1991, pp. 47-48.</mixed-citation></ref><ref id="scirp.29819-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">N. E. Steenman, “Marine Photosynthesis with Special Emphasis on the Ecological Aspects,” Elsevier Scientific Publishing Co., New York, 1975.</mixed-citation></ref><ref id="scirp.29819-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">P. Coutteau, “Micro-Algae,” In: P. Lavens and P. Sorgeloos, Eds., Manual on the Production and Use of Live Food for Aquaculture, FAO Fisheries Technical Paper No. 361, Laboratory of Aquaculture &amp; Artemia Reference Center, University of Gent, Belgium, 1996.</mixed-citation></ref><ref id="scirp.29819-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">K. Livansky, “Losses of CO2 in Outdoor Mass Algal Cultures: Determination of the Mass Transfer Coefficient KL by Means of Measured pH Course in NaHCO3 Solution,” Algological Studies, Vol. 58, 1990, pp. 87-97.</mixed-citation></ref><ref id="scirp.29819-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">R. F. Camacho, “Prediction of Dissolved Oxygen and Carbon Dioxide Concentration Profiles in Tubular Photobioreactors for Microalgal Culture,” Biotechnology and Bioengineering, Vol. 62, No. 1, 1999, pp. 71-84.  
doi:10.1002/(SICI)1097-0290(19990105)62:1&lt;71::AID-BIT9&gt;3.0.CO;2-T</mixed-citation></ref></ref-list></back></article>