Thesis (MEng)--Stellenbosch University, 2015. / ENGLISH ABSTRACT: The expansion of the global fuels industry has caused an increase in the quantity of hydrocarbons produced as a by-product of refinery gas-to-liquid processes. Conversion of hydrocarbons to higher value products is possible using bioprocesses, which are sustainable and environmentally benign. Due to the deficiency of oxygen in the alkane molecule, the supply of sufficient oxygen through aeration is a major obstacle for the optimization of hydrocarbon bioprocesses. While the oxygen solubility is increased in the presence of hydrocarbons, under certain process conditions, the enhanced solubility is outweighed by an increase in viscosity, causing a depression in overall volumetric oxygen transfer coefficient (KLa). The rate at which oxygen is transferred is defined in terms of a concentration driving force (oxygen solubility) and the overall volumetric oxygen transfer coefficient (KLa). The KLa term comprises an oxygen transfer coefficient (KL) and the gas-liquid interfacial area (a), which are dependent on the uid properties and system hydrodynamics. This behaviour is not well understood for hydrocarbon bioprocesses and in a bubble column reactor (BCR). To provide an understanding of oxygen transfer behaviour, a model hydrocarbon bioprocess was developed using a BCR with a porous sparger. To evaluate the interfacial area, the Sauter mean bubble diameter (D32) was measured using an image analysis algorithm and gas holdup (ϵG) was measured by the change in liquid height in the column. Together the D32 and ϵG were used in the calculation of interfacial area in the column. The KLa was evaluated with incorporation of the probe response lag, allowing more accurate representation of the KLa behaviour. The probe response lag was measured at all experimental conditions to ensure accuracy and reliability of data. The model hydrocarbon bioprocess employed C14-20 alkane-aqueous dispersions (2.5 - 20 vol% hydrocarbon) with suspended solids (0.5 - 6 g/l) at discrete super ficial gas velocity (uG) (1 - 3 cm/s). For systems with inert solids (corn our, dp = 13.36 m), the interfacial area and KLa were measured and the behaviour of KLa was described by separation of the in uences of interfacial area and oxygen transfer coefficient (KL). To further the understanding of oxygen transfer behaviour, non-viable yeast cells (dp = 5.059 m) were used as the dispersed solid phase and interfacial area behaviour was determined. This interfacial area behaviour was compared with the behaviour of systems with inert solids to understand the differences with change in solids type. In systems using inert solids, a linear relationship was found between G and uG. An empirical correlation fo rthe prediction of this behaviour showed an accuracy of 83.34% across the experimental range. The interfacial area showed a similar relationship with uG and the empirical correlation provided an accuracy of 78.8% for prediction across the experimental range. In inert solids dispersions, the KLa increased with uG as the result of an increase in interfacial area as well as increases in KL. An increase in solids loading indicated an initial increase in KLa, due to the in uence of liquid-film penetration on KL, followed by a decrease in KL at solids loading greater than 2.5 g/l, due to diffusion blocking effects. In systems with yeast dispersions, the presence of surfactant molecules in the media inhibited coalescence up to a yeast loading of about 3.5 g/l, and resulted in a decrease in D32. Above this yeast loading, the fine yeast particles increased the apparent viscosity of the dispersion sufficiently to overcome the in uence of surfactant and increase the D32. The behaviour of G in yeast dispersions was similar to that found with inert solids and demonstrated a linear increase with uG. However, in yeast dispersions, the interaction between alkane concentration and yeast loading caused a slight increase in dispersion viscosity and therefore G. An empirical correlation to predict G behaviour with increased uG was developed with an accuracy of 72.55% for the experimental range considered. Comparison of yeast and inert solids dispersions indicated a 37.5% lower G in yeast dispersions compared to inert solids as a result of the apparent viscosity introduced by finer solid particles. This G and D32 data resulted in a linear increase in interfacial area with uG with no significant in uence of alkane concentration and yeast loading. This interfacial area was on average 6.7% lower than interfacial area found in inert solid dispersions as a likely consequence of the apparent viscosity with finer particles. This study provides a fundamental understanding of the parameters which underpin oxygen transfer in a model hydrocarbon bioprocess BCR under discrete hydrodynamic conditions. This fundamental understanding provides a basis for further investigation of hydrocarbon bioprocesses and the prediction of KLa behaviour in these systems. / AFRIKAANSE OPSOMMING: Die uitbreiding van die internasionale brandstofbedryf het 'n toename veroorsaak in die hoeveelheid koolwaterstowwe geproduseer as 'n deur-produk van raffinadery gas-tot-vloeistof prosesse. Omskakeling van koolwaterstowwe na hoër waarde produkte is moontlik met behulp van bioprosesse, wat volhoubaar en omgewingsvriendelik is. As gevolg van die tekort aan suurstof in die alkaan molekule, is die verskaffing van voldoende suurstof deur deurlugting 'n groot uitdaging vir die optimalisering van koolwaterstof bioprosesse. Terwyl die suurstof oplosbaarheid verhoog in die teenwoordigheid van koolwaterstowwe, onder sekere proses voorwaardes is die verhoogde oplosbaarheid oortref deur 'n toename in viskositeit, wat 'n depressive veroorsaak in die algehele volumetriese suurstofoordragkoëffisiënt (KLa). Die suurstof oordrag tempo word gedefinieer in terme van 'n konsentrasie dryfkrag (suurstof oplosbaarheid) en KLa. Die KLa term behels 'n suurstofoordragkoëffisiënt (KL) en die gas-vloeistof oppervlakarea (a), wat afhanklik is van die vloeistof eienskappe en stelsel hidrodinamika. Hierdie gedrag is nie goed verstaan vir koolwaterstof bioprosesse nie, asook in kolom reaktors (BCR). Om 'n begrip van suurstof oordrag gedrag te voorsien, is 'n model koolwaterstof bioproses ontwikkel met 'n BCR met 'n poreuse besproeier. Om die oppervlakarea te evalueer, is die gemiddelde Sauter deursnit (D32) gemeet deur 'n foto-analise algoritme en gas vasvanging ( G) is gemeet deur die verandering in vloeibare hoogte in die kolom. Saam is die D32 en G gebruik in die berekening van die oppervlakarea in die kolom. Die KLa is geëvalueer met insluiting van die meter se reaksie sloering, om n meer akkurate voorstelling van die KLa gedrag te bereken. Die meter reaksie sloering was gemeet op alle eksperimentele toestande om die akkuraatheid en betroubaarheid van data te verseker. Die model koolwaterstof bioproses gebruik n-C14-20 alkaan-water dispersies (2.5 - 20 vol% koolwaterstof) solide partikels (0.5 - 6 g/l) op diskrete oppervlakkige gas snelhede (1 - 3 cm/s). Vir stelsels met inerte solides (koring meel, dp = 13.36 m), is die oppervlakarea en KLa gemeet en die gedrag van KLa beskryf deur skeiding van die invloede van oppervlakarea en KL. Om die begrip van suurstof oordrag se gedrag te bevorder, is nie-lewensvatbare gisselle (dp = 5.059 m) gebruik as die verspreide solide fase en oppervlakarea is bepaal. Hierdie oppervlakarea gedrag is vergelyk met die van stelsels met inerte solides om die verskille met verandering in solide tipes te verstaan. In stelsels met inerte solides, is 'n line^ere verwantskap gevind tussen G en uG. 'n Empiriese korrelasie vir die voorspelling van hierdie gedrag is opgestel met 'n akkuraatheid van 83.34% in die eksperimentele reeks. Die oppervlakarea het 'n soortgelyke verhouding met uG en die empiriese korrelasie verskaf 'n akkuraatheid van 78,8% vir die voorspelling van oppervlakarea oor die eksperimentele reeks. In inerte solide dispersies, het die KLa toegeneem met uG as die gevolg van 'n toename in grens oppervlak asook stygings in KL. 'n Toename in solides belading het n aanvanklike styging in KLa aangedui, as gevolg van die invloed van die vloeistof-film penetrasie op KL, gevolg deur 'n afname in KL op vastestowwe ladings groter as 2.5 g/l, te danke aan diffusie blokkeer effekte. In stelsels met gis dispersies, het die teenwoordigheid van benattings molekules in die media samesmelting geïnhibeer tot 'n gis lading van ongeveer 3.5 g/l, en het gelei tot 'n afname in D32. Bo hierdie gis lading, het die fyn gis partikels die skynbare viskositeit van die verspreiding verhoog genoegsaam om die invloed van benattings molekules te oorkom en die D32 te verhoog. Die gedrag van G in gis dispersies was soortgelyk aan die van inerte solides en dui op 'n lineêre toename met uG. Maar in gis dispersies, het die interaksie tussen alkaan konsentrasie en gis lading 'n effense toename veroorsaak in die verstrooiing viskositeit en dus in G. 'n Empiriese korrelasie is ontwikkel om G gedrag te voorspel en het 'n akkuraatheid van 72,55% vir die eksperimentele verskeidenheid beskou. Vergelyking van gis en inerte patrikel dispersies wys 'n 37.5% laer G in gis dispersies in vergelyking met inerte vaste stowwe as 'n gevolg van die skynbare viskositeit bekendgestel deur fyner vastestowwe partikels. Hierdie G en D32 data het gelei tot 'n linere toename in grens oppervlak met uG met geen beduidende invloed van alkaan konsentrasie en gis lading nie. Die oppervlakarea was gemiddeld 6.7% laer as oppervlakarea gevind in inerte partikel dispersies as 'n waarskynlike gevolg van die skynbare viskositeit met fyner partikels. Hierdie studie bied 'n fundamentele begrip van die veranderlikes wat die suurstof oordrag definieer in 'n model koolwaterstof bioproses BCR onder diskrete hidrodinamiese voorwaardes. Hierdie fundamentele begrip bied n basis vir verdere ondersoek van koolwaterstof bioprosesse en en die voorspelling van KLa gedrag in hierdie stelsels.

In this investigation, two separate methods for determining oxygen transfer rates were applied to the oxidation ditches of an activated sludge plant. Steady state oxygen uptake rate testing and an oxygen mass balance technique were used to propose an in-process procedure for monitoring aeration efficiency using available resources. Although some overall averages offered promise, the testing results revealed that the mass balance analysis yielded results that do not accurately represent the oxygen transfer capabilities within the individual reactors due to shared variables that control the oxygen transfer rate. The steady state method provided more favorable results. Overall averages of daily oxygen transfer rates determined using the steady state method displayed a ratio of oxygen transfer rate between the reactors that corresponds to the expected ratio of 5/6 derived from the linear feet of aerator rotor present in each reactor.

When evaluating the performance of horizontal rotor mechanical surface aeration equipment in accordance with the ASCE Standard for Measurement of Oxygen Transfer in Clean Water, several factors should be considered with regard to their impact on the reported performance. These include basin geometry and testing volume, source water quality, dissolved oxygen measurement location, and external environmental factors including air temperature and humidity. Each of these factors may influence the reported performance of mechanical surface aeration equipment, specifically horizontal rotor aeration devices, resulting in an inaccurate estimation of the true equipment performance that should be expected in practical applications.

The high cell density fermentation of recombinant Pichia pastoris for human serum albumin (HSA) production is a high oxygen demand process. The oxygen demand is usually met by increased agitation rate and use of oxygen-enriched air. Microbubble fermentation however can supply adequate oxygen to the microorganisms at relatively low agitation rates because of improved mass transfer of the microbubbles used for the sparging. Conventionally sparged fermentations were conducted for the production of HSA using P. pastoris at agitation rates of 350, 500, and 750 rpm, and were compared to MBD sparged fermentation at 150, 350, and 500 rpm agitation rates. The MBD improved the volumetric oxygen transfer coefficient (kLa) and subsequently increased the cell mass and protein production compared to conventional fermentation. Cell production in MBD fermentation at 350 rpm was 4.6 times higher than that in conventional fermentation at 350 rpm, but similar to that in the conventional 750 rpm. Maximum cell mass productivity in the conventional 350 rpm was only 0.37 g / (L·h), while the maximum value in MBD 350 rpm was 2.0 g / (L·h), which was similar to 2.2 g / (L·h) in the conventional 750 rpm. Biomass yield on glycerol Ys (g cell/ g glycerol) was 0.334 g / g in the conventional 350 rpm, 0.431 g / g in MBD 350 rpm and 0.438 g / g in the conventional 750 rpm. Protein production in MBD 350 rpm was 7.3 times higher than that in the conventional 350 rpm, but similar to the conventional 750 rpm. Maximum protein productivity in the conventional 350 rpm was 0.37 mg / (L·h), 2.8 mg / (L·h) in MBD 350 rpm, and 3.3 mg / (L·h) in the conventional 750 rpm. Protein yield on methanol Yp (mg protein / g methanol) was 1.57 mg /g in the conventional 350 rpm, 5.02 in MBD 350 rpm, and 5.21 in the conventional 750 rpm. The volumetric oxygen transfer coefficient kLa was 1011.9 h-1 in MBD 350 rpm, which was 6.1 times higher than that in the conventional 350 rpm (164.9 h-1) but was similar to the conventional 750 rpm (1098 h-1). Therefore, MBD fermentation results at low agitation of 350 rpm were similar to those in the conventional fermentation at high agitation of 750 rpm. There was considerable improvement in oxygen transfer to the microorganism using MBD sparging relative to the conventional sparging. Conventional fermentations were conducted both in a Biostat Q fermenter (small) at 500 rpm, 750 rpm, and 1000 rpm, and in a Bioflo III fermenter (large) at 350 rpm, 500 rpm, and 750 rpm. At the same agitation rate of 500 rpm, cell production in the large reactor was 3.8 times higher than that in the small one, and no detectable protein was produced in the small reactor at 500 rpm. At the same agitation rate of 750 rpm, both cell production and protein production in the large reactor were 4.6 times higher than the small reactor. Thus, the Bioflo III fermenter showed higher oxygen transfer efficiency than the Biostat Q fermenter, because of the more efficient aeration design of the Bioflo III fermenter. / Master of Science

In the large-scale production of <i>Saccharomyces cerevisiae</i> (baker's yeast), oxygen transfer, which is one of the major limiting factors, is improved by using high agitation rates. However, high agitation rates subject the microorganisms to high shear stress and caused high power consumption. A microbubble dispersion (MBD) method was investigated to improve oxygen transfer at low agitation rates and thus reduce power consumption and shear stress on the microorganisms. The experiments were conducted at the 1-liter level and subsequently scaled-up to 50-liters using a constant volumetric oxygen transfer coefficient (<i>k_La</i>) method for scaling. In comparison to a conventional air-sparged fermentation, the MBD method considerably improved the cell mass yield, growth rate and power consumption in the 50-liter fermentor. Cell mass production in the MBD system at agitation rate of 150 rpm was about the same as those obtained for a conventional air-sparged system agitatid at 500 rpm. Power consumption in the conventional air-sparged system was three-fold that required for the same biomass yield in the MBD system. However, at the 1-liter scale, the MBD system did not show any significant advantage over the air-sparged system because of the high power consumption. / Master of Science

Thesis (MScEng (Process Engineering))--University of Stellenbosch, 2010. / ENGLISH ABSTRACT: Hydrocarbons provide excellent feed stocks for bioconversion processes to produce value added products using various micro-organisms. However, hydrocarbon-based aerobic bioprocesses may exhibit transport problems where the bioconversion is limited by oxygen supply rather than reaction kinetics. Consequently, the overall volumetric oxygen transfer coefficient (KLa) becomes critical in designing, operating and scaling up of these processes. In view of KLa importance in hydrocarbon-based processes, this work evaluated KLa measurement methodologies as well as quantification of KLa behavior in aerated agitated alkane-solid-aqueous dispersions. A widely used KLa measurement methodology, the gassing out procedure (GOP) was improved. This improvement was done to account for the dissolved oxygen (DO) transfer resistances associated with probe. These resistances result in a lag in DO response during KLa measurement. The DO probe response lag time, was incorporated into the GOP resulting in the GOP (lag) methodology. The GOP (lag) compared well with the pressure step procedure (PSP), as documented in literature, which also incorporated the probe response lag time. Using the GOP (lag), KLa was quantified in alkane-solid-aqueous dispersions, using either inert compounds (corn flour and CaCO3) or inactive yeast cells as solids to represent the micro-organisms in a hydrocarbon bioprocess. Influences of agitation, alkane concentration, solids loading and solids particle sizes and their interactions on KLa behavior in these systems were quantified. In the application of an accurate KLa measurement methodology, the DO probe response lag time was investigated. Factors affecting the lag, which included process conditions such as agitation (600-1200rpm), alkane concentration (2.5-20% (v/v), alkane chain length (n-C10-13 and n-C14-20), inert solids loading (1-10g/L) and solids particle sizes (3-14μm) as well as probe characteristics such as membrane age and electrolyte age (5 day usage), were investigated. Kp, the oxygen transfer coefficient of the probe, was determined experimentally as the inverse of the time taken for the DO to reach 63.2% of saturation after a step change in DO concentration. Kp dependence on these factors was defined using 22 factorial design experiments. Kp decreased on increased membrane age with an effect double that of Kp decrease due to electrolyte age. Additionally, increased alkane concentration decreased Kp with an effect 7 times higher compared to that of Kp decrease due to increased alkane chain length. This was in accordance to Pareto charts quantification. KLa was then calculated, using the GOP (lag), according to equation [1] which incorporates the influence of Kp. Equation 1 is derived from the simultaneous solution of the models which describe the response of the system and of the probe to a step change in DO. 1 1 * L p p p K at K t L p p La C K e K ae C K K = -  - - -  -   [1] The KLa values documented in literature from the PSP and KLa calculated by the GOP (lag) showed only a 1.6% difference. However KLa values calculated by the GOP (lag) were more accurate than KLa calculated by the GOP, with up to >40% error observed in the latter according to t-tests analyses. These results demonstrated that incorporating Kp markedly improved KLa accuracy. Consequently, the GOP (lag) was chosen as the preferred KLa measurement methodology. KLa was determined in n-C14-20-inert solid-aqueous dispersions. Experiments were conducted in a stirred tank reactor with a 5L working volume at constant aeration of 0.8vvm, 22ºC and 101.3kPa. KLa behavior across a range of agitations (600- 1200rpm), alkane concentrations (2.5-20% (v/v)), inert solids loadings (1-10g/L) and solids particle sizes (3-14μm) was defined using a 24 factorial design experiment. In these dispersions, KLa increased significantly on increased agitation with an effect 5 times higher compared to that of KLa increase due to interaction of increased alkane concentration and inert solids loading. Additionally, KLa decreased significantly on increased alkane concentration with an effect 4 times higher compared to both that of increased solids particle sizes and the interaction of increased agitation and solids particle size. In n-C14-20-yeast-aqueous dispersions, KLa was determined under narrowed process conditions better representing typical bioprocess conditions. KLa behavior across a range of agitations (600-900rpm), alkane concentrations (2.5-11.25% (v/v)) and yeast loadings (1-5.5g/L) using a 5μm-yeast cell was defined using a 23 factorial design experiment. In these dispersions, KLa increased significantly on increased agitation. Additionally, KLa decreased significantly on increased yeast loading with an effect 1.2 times higher compared to that of KLa decrease due to interaction of increased alkane concentration and yeast loading. In this study, the importance of Kp for accurate KLa measurement in alkane based systems has been quantified and an accurate and less complex methodology for its measurement applied. Further, KLa behavior in aerated alkane-solid-aqueous dispersions was quantified, demonstrating KLa enhancement on increased agitation and KLa depression on increased alkane concentration, solids loading and solids particle sizes. / AFRIKAANSE OPSOMMING: Koolwaterstowwe dien as uitstekende voervoorraad vir ´n verskeidenheid van mikroorganismes wat aangewend word in biologiese omsettingsprosesse ter vervaardiging van waardetoevoegende produkte. Hierdie biologiese omsettingsprosesse word egter vertraag weens die gebrek aan suurstoftoevoer onder aerobiese toestande. Die tempo van omsetting word dus beheer deur die volumetriese suurstofoordragkoeffisiënt (KLa) eerder as die toepaslike reaksiekinetika. Die bepaling van ´n akkurate KLa word dus krities tydens die ontwerp en opskalering van hierdie prosesse. Met dit in gedagte het hierdie studie die huidige metodes om KLa te bepaal geëvalueer en die gedrag van KLa in goed vermengde en belugde waterige alkaanmengsels met inerte vastestowwe, soos gisselle, in suspensie ondersoek. ´n Deesdae populêre metode om KLa te bepaal, die sogenaamde gasvrylatingsprosedure (GOP) is in hierdie studie verbeter. Die verbetering berus op die ontwikkeling van ´n prosedure om die suurstofoordragsweerstand van die pobe wat die hoeveelheid opgeloste suurstof (DO) meet, in berekening te bring. Hierdie weerstand veroorsaak ´n vertragin in the responstyd van die probe. Die verbeterde metode, GOP (lag), vergelyk goed met die gepubliseerde resultate van die drukstaptegniek (PSP) wat ook die responstyd in ag neem. GOP (lag) is ingespan om KLa te gekwantifiseer vir waterige alkaan-vastestof suspensies. Inerte componente soos mieliemeel, kalsiumkarbonaat en onaktiewe gisselle het gedien as die vastestof in suspensie verteenwoordigend van die mikroörganismes in ´n koolwaterstof bio-proses. Die invloed van vermengingstempo, alkaan konsentrasie, vastestof konsentrasie en partikelgrootte asook die interaksie van al die bogenoemde op KLa is kwatitatief bepaal in hierdie studie. Faktore wat die responstyd van die DO probe beïnvloed is ondersoek. Hierdie faktore is onder meer vermengingstempo (600-1200opm), alkaankonsentrasie (2.5-20% (v/v)), alkaankettinglengte (n-C10-13 en n-C14-20), vastestofkonsentrasie (1-10g/L) en partikelgrootte (3-14 μm). Faktore wat die eienskappe van die probe beïnvoed, naamlik membraan-en elektrolietouderdom (5 dae verbruik), is ook ondersoek. Kp, die suurstofoordragskoeffisiënt, is bepaal deur ´n inkrementele verandering in die suurstofkonsentrasie van die mengsel te maak en die tyd vir 63.2% versadiging van die probelesing te noteer. Die genoteerde tyd is die response tyd van die probe en Kp, die inverse van hierdie tyd. Die afhanklikheid van Kp op die bogenoemde faktore is ondersoek in ´n 22 faktorieël ontwerpte reeks eksperimente. Kp toon ´n afname met ´n toename in membraanouderdom. Hierdie afname is dubbel in grootte as dit vergelyk word met die afname relatief tot die toename in elektrolietouderdom. Verder toon Kp ´n afname met ´n toename in alkaankonsentrasie. Hierdie afname is 7 keer groter relatief tot die afname gesien met die toename in alkaan kettinglengte. Hierdie is in goeie ooreenstemming met Pareto kaarte as kwantifiseringsmetode. KLa is bereken met die inagname van Kp volgens vergelyking [1]: 1 1 * L p p p K at K t L p p La C K e K ae C K K = -  - - -  -   [1] Vergelyking [1] is afgelei vanaf die gelyktydige oplossing van die bestaande modelle wat die responstyd van die pobe vir ´n stapverandering in DO bereken. Die KLa waardes van die PSP metode uit literatuur verskil in die orde van 1.6% van dié bereken deur vergelyking [2]. Hierdie verskil is weglaatbaar. Die KLa waardes verkry uit die GOP metode wat nie Kp in berekening bring nie, verskil met meer as 40% van die huidige, verbeterde metode volgens die statistiese t-test analiese. Dit bewys dat die inagname van Kp ´n merkwaardige verbetering in die akuraatheid van KLa teweeg bring. GOP (lag) kry dus voorkeur vir die berekening van KLa verder aan in hierdie studie. KLa is bereken vir n-C14-20-water mengsels met inerte vastestofsuspensies. Die eksperimente is uitgevoer in ´n 5L geroerde reaktor met ´n konstante belugting van 0.8vvm (volume lug per volume supensie per minuut), 22ºC en 101.3kPa. Die gedrag van KLa met betrekking tot vermengingstempo (600-1200opm), alkaankonsentrasie (2.5-20% (v/v)), vastestofkonsentrasie (1-10g/L) en partikelgrootte (3-14μm) is ondersoek in ´n 24 faktorieël ontwerpte reeks eksperimente. Verder is die invloed van vloeistofviskositeit en oppervlakspanning op KLa ondersoek in ´n 23 faktorieël ontwerpte reeks eksperimente. KLa het ´n beduidende toename getoon met ´n toename in vermengingstempo. Hierdie toename was 5 keer groter as die toename relatief tot die interaksie van alkaan-en vastestofkonsentrasie. KLa het ook beduidend afgeneem met ´n toename in alkaankonsentrasie. Die toename was 4 keer groter as die toename relatief tot die toename in partikelgrootte en die interaksie van vermengingstempo en partikelgrootte. In n-C14-20-water mengsels met gisselsuspensies is KLa bepaal onder kondisies verteenwoordigend van tipiesie biologiese omsettingsprosesse. Die gedrag van KLa met betrekking tot vermengingstempo (600-900opm), alkaankonsentrasie (2.5-11.25% (v/v)) en giskonsentrasie (1-5.5g/L) met ´n partikelgroote van 5μm is ondersoek in ´n 23 faktorieël ontwerpte reeks eksperimente. Hierdie eksperimente het ´n beduidende toename in KLa met ´n toename in vermengingstempo getoon sowel as ´n beduidende afname met ´n toename in giskonsentrasie. Hierdie afname is in die orde van 1.2 keer groter in vergelyking met die interaksie van alkeen- en giskonsentrasie. Hierdie studie bring die kritieke rol wat Kp speel in die akkurate bepaling van KLa in waterige alkaansisteme met inerte vastestofsuspensies na vore. Dit stel verder ´n metodiek voor vir die akurate meting van en kwantifisering van beide Kp en KLa onder aerobiese toestande met betrekking tot vermengingstempo, alkaankonsentrasie, vastestofkonsentrasie en partikelgrootte.

Thesis (MScEng (Process Engineering))--University of Stellenbosch, 2007. / Adequate provision of oxygen to aerobic bioprocesses is essential for the optimisation of process kinetics. In bioprocesses in which the feedstock is an alkane, the supply of sufficient oxygen is of particular concern because the alkane molecular structure is deficient in oxygen. As a result, the oxygen demand has to be met solely by transfer of oxygen to the culture, necessitating a proportionately higher requirement for oxygen transfer. Maximisation of the rate of oxygen transfer is therefore of key importance in optimising the potential for alkane bioconversion, with respect to both operation and scale up. Nevertheless, the oxygen transfer rate (OTR), and its dependence on the overall volumetric mass transfer coefficient (KLa) in alkane-aqueous dispersions is not yet well understood. In view of the importance of an adequate OTR in the optimisation of alkane bioconversion, this study has focused on the identification and elucidation of the factors which underpin the behaviour of KLa in an alkane-aqueous dispersion. KLa behaviour was quantified in terms of the pressures imposed by turbulence and alkane fluid properties, through their influence on the Sauter mean diameter (D32), gas hold up, gas-liquid interface rigidity and gas-liquid interfacial area per unit volume. These properties were correlated with KLa over a wide range of agitation rates and alkane concentrations in alkane-aqueous dispersions. Experiments were conducted in a 5 litre aerated and agitated bioreactor at agitation rates of 600, 800, 1000 and 1200 rpm and alkane (n-C10-C13 cut) concentrations of 0, 2.5, 5, 10, and 20% (v/v). KLa determination was executed using both the gassing out and pressure step methods. The accuracy and reliability of these methods were compared under the full range of agitation rates and alkane concentrations. The pressure step method was conclusively shown to be superior provided that probe response was taken into account, and was therefore used in the correlations. The interfacial areas corresponding to the KLa values were calculated from the combined effects of D32 and gas hold up. D32 was determined from the measurement of the dispersed air bubble diameters by means of a photographic technique and image analysis. Image analysis was performed by a program that was developed in Matlab® using image acquisition and image processing techniques. This program used these techniques to extract information of the gas bubbles in the image. The gas hold up was determined using the dispersion height technique. The behaviour of KLa was shown to be dependent on both agitation and alkane concentration. Increasing agitation from 600 to 1200 rpm increased KLa for each of the alkane concentrations. The influence of agitation on the interfacial area was evaluated over the same range of agitation rates and the relationship between the corresponding KLa values and interfacial areas assessed. Increasing agitation rate similarly enhanced the interfacial area available for transfer for each of the alkane concentrations, resulting in the concomitant increase in KLa. This increase in interfacial area was related directly to a shear-induced decease in D32 and indirectly to an increased gas holdup as a result of the lower rise velocity of the smaller bubbles. In addition to the agitation, the presence of alkane markedly influenced KLa behaviour, but in different ways, depending on the alkane concentration. Alkane concentration between 2.5 and 5% (v/v) reduced D32 at constant agitation of 800, 1000 and 1200 rpm, a likely consequence of decreased surface tension and retarded coalescence conferred by the alkane. The smaller D32 and the consequential enhanced gas hold up served to amplify KLa through increased interfacial area. However, as alkane concentration was increased above 5% (v/v), the gas hold up decreased despite a continued decrease in D32, resulting in a corresponding decrease in both the interfacial area and KLa. This suggests that at the higher alkane concentrations, the influence of viscosity predominated, exerting multiple negative influences on the interfacial area and oxygen transfer coefficient. The trends were however, not observed at the low agitation of 600 rpm, where turbulence was significantly reduced and KLa was repressed for all alkane concentrations. The pressures imposed by turbulence and alkane properties on the interfacial area defined locales of KLa behaviour and three distinct KLa behavioural trends were identified, depending on the agitation rate and alkane concentration. Regime 1 was constrained between 2.5 and 5% (v/v) for agitation rates of 800 rpm and above. Here KLa enhancement was directly associated with increased interfacial area which was the major factor defining KLa in this regime. Regime 2 was constrained by alkane concentrations higher than 5% (v/v) for agitation rates of 800 rpm and above. In this regime, the KLa depression was observed with increasing alkane concentration suggesting a predominant influence of viscosity which would be likely to exert multiple negative influences on KLa, through both the interfacial area and KL. The interfacial area in this regime decreased mainly due to the negative effect of viscosity on gas holdup. Regime 3, characterised by a decline in KLa irrespective of the alkane concentration, occurred at agitation rates smaller than 800 rpm. It is likely that at low agitation rates, the contribution of turbulence was insufficient to exert a positive influence on the interfacial area In this regime, the interfacial decreased through the combined negative effect of increased D32 and decreased gas holdup. The resultant variation in OTR depended directly on the relative magnitudes of the KLa and oxygen solubility and indirectly on the process conditions which defined these magnitudes. Under conditions of enhanced KLa, OTR benefited from the combined increases in KLa and oxygen solubility. However, under conditions of KLa depression, the elevated oxygen solubility did not invariably outweigh the influence of KLa depression on OTR. Consequently, despite the considerably increased solubility of oxygen in alkane-based bioprocesses a potential decrease in OTR through depressed KLa underlines the critical importance of the quantification of this parameter in alkane-aqueous dispersions and the necessity for a definition of the locales of optimal KLa. Through the identification of the parameters which underpin the behaviour of KLa in alkane-aqueous dispersions and the quantification of the effect of process conditions on these parameters, a fundamental understanding of the KLa and OTR in alkane-aqueous dispersions has been developed. This provides a knowledge base for the prediction of optimal KLa in these systems and has wide application across all alkane-based bioprocesses.

De par ses propriétés physiques et chimiques particulières du bois de chêne, une barrique est le siège de phénomènes de transfert très complexes. Les tonnelleries souhaitent apporter de plus en plus de précision pour le choix des barriques en ce qui concerne les arômes transmis au bois mais aussi en ce qui concerne les échanges entre l’atmosphère du chai et le vin. Le projet a permis d’améliorer les connaissances sur les phénomènes de transfert d’oxygène au travers des douelles et à l’inter-douelle et de quantifier l’importance des paramètres interagissant sur les transferts tels les phénomènes d’absorption, le type de chauffe et les caractéristiques du bois. Cette étude a permis de définir des paramètres de caractérisation des barriques par rapport au transfert d’oxygène afin de mieux conseiller les utilisateurs pour le choix des barriques et leur mise en œuvre. L’objet du projet repose sur une approche pluridisciplinaire. Nous avons caractérisé les barriques pour émettre des hypothèses de transfert, puis nous avons quantifié la cinétique de désorption d’oxygène du bois et de son imprégnation. De plus, nous avons évalué la quantité d’oxygène consommé par les polyphénols. Enfin, grâce au développement d'un perméamètre permettant de placer les morceaux de douelles dans des conditions opératoires variées, nous avons mesuré des flux d’oxygène de part et d’autre de la cellule. La désorption est le phénomène prépondérant dans l'apport d'oxygène. Le transfert d'oxygène se fait essentiellement à l'inter-douelle dans les zones de faibles pressions. / Many complex transfer phenomena occur in Oak barrels, due to the physical and chemical properties of Oak wood. Coopers want to provide their consumers with more and more advice according to the aromas given by the wood of the barrel to the wine but also according to the interactions between the winery atmosphere and the wine. The aim of this project is to improve the knowledge of oxygen transfer through staves and between two staves. It is also to quantify the parameters that influence the oxygen transfer such as absorption phenomena, type of barrel toasting and oak wood characteristics. This study should bring to light characteristic parameters of barrels according to oxygen transfer in order to give better advice to users. This would allow them to choose the best barrels and know how to implement them. This project uses a multidisciplinary approach. The first part is to characterize barrels is order to suggest hypothesis about transfer phenomena. Then, kinetics of impregnation and desorption of oxygen contained in oak wood are quantified. Moreover, we try to evaluate the quantity of oxygen consumed by polyphenols. Finally, oxygen transfer evaluation is possible thanks to the development of a new cell allowing us to place a piece of stave in various operating conditions and to measure the flux of oxygen on both sides of the cell. Thus, the laws of transfer can be described; modeling of the quantity of oxygen transferred to wine could be done according to the utilization conditions and to the type of staves.

This work concerns the efficient treatment of wastewaters from pulp and paper mills by means of aerobic biological processes. For treatment processes there are many aspects of efficiency and the present study investigates both energy efficiency and purification efficiency during disturbances. Special focus is put on wood extractives, such as resin acids and fatty acids, since they can cause negative effects in fish and other organisms in the receiving waters. They can furthermore be toxic to microorganisms in a biological treatment plant. They also affect oxygen transfer, which is important for energy efficient aeration of aerobic biological treatment processes. This thesis includes five papers/studies and presents a strategy for efficient treatment of forest industrial wastewaters. The results should help creating resilient wastewater treatment strategies with efficient use of energy. One new strategy proposed here includes separation of extractives before the wastewater is treated biologically, and the use of the extra amount of sludge as an energy source, shifting the energy balance from negative to positive.

In this study, the effects of bioprocess operation parameters on recombinant human growth hormone (rhGH) production by P. pastoris were systematically investigated. In this frame, first, for the extracellular expression and purification of human growth hormone by recombinant P. pastoris the cDNA of hGH, fused with a polyhistidine tag and also fused with a target site for the Factor Xa protease in which cleavage produces a mature N- and C- termini of rhGH, was cloned into pPICZ&amp / #945 / A plasmid and the constructed system within the plasmid, pPICZ&amp / #945 / A::hGH, was integrated to AOX1 locus of P. pastoris and expressed under alcohol oxidase promoter which is induced by methanol. With dot-blot analysis, the appropriate two strains producing human growth hormone at high levels and having different methanol utilization phenotype (Mut+ and Muts) were chosen among the other transformants. Then, the effects of methanol concentrations on the expression of rhGH and cell growth were analyzed and both of the phenotypes were compared in defined and complex media in laboratory scale air filtered shake bioreactors. The highest rhGH concentration for Mut+ and MutS, was found as 0.052 kg m-3 and 0.16 kg m-3, respectively, at 2 %(v/v) methanol concentration in complex medium. When methanol was used as the sole carbon source in defined medium, Muts phenotype had very low specific growth rate on methanol due to the intrinsic characteristics of it, therefore detectable rhGH was not observed, on the other hand, optimum rhGH concentration produced by Mut+ strain was found as 0.032 kg m-3 at 3% (v/v) methanol concentration in defined medium. In mixed system (glycerol/methanol) which is also defined, when the optimum glycerol concentration, 30 kg m-3, was used, Muts produced the highest rhGH, 0.110 kg m-3, at 1% (v/v) methanol concentration and any increase in methanol concentration resulted in lower rhGH production, on the other hand, Mut+ strain produced 0.060 kg m-3 rhGH at 4% (v/v) methanol concentration, which indicated that higher rhGH production capacity of Mut+ strain was obtained at high methanol concentrations. Using the designed defined medium for Mut+ phenotype where methanol was used as the sole carbon source with an optimum concentration of 3% (v/v), the effects of oxygen transfer on rhGH production, by-product formation, and cell growth, oxygen transfer and fermentation characteristics were investigated by using pilot scale bioreactor. Oxygen transfer effects on rhGH production were investigated at QO/VR=0.5 vvm / N=250, 500, 625, 750 min-1 conditions. The variations in rhGH , cell, amino acid and organic acid concentrations with the cell cultivation time, specific cell growth rate, the oxygen uptake rate, the liquid phase coefficient by using the dynamic method, maintenance coefficient for oxygen and yield coefficients were determined. The highest rhGH concentration was obtained at 0.5 vvm, 500 min-1 condition as 0.023 kg m-3 with 5.37 kg m-3 cell density.