VIRUS CONCENTRATION BY CROSSFLOW MEMBRANE FILTRATION: EFFECT OF HYDRODYNAMIC CONDITIONS AND MEMBRANE PROPERTIES By Elodie Pasco A DISSERTATION Submitted to Michigan State University In partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Environmental Engineering 2012 ABSTRACT Crossflow membrane filtration is emerging as a concentration method for the recovery and detection of viruses in large volumes of water. To increase virus recovery, the membrane is usually “blocked” with a proteinaceous solution or a chemical dispersant. This study explores a novel approach using controlled and rapid (<1 h) layer-by-layer adsorption of polyelectrolytes to form an anti-adhesive, sacrificial layer on the membrane surface. Membranes coated with polyelectrolyte multilayers (PEMs) can ensure up to 2-fold higher pre-elution recoveries of P22 bacteriophage than membranes blocked with calf serum (CS). Calculations of virus-membrane interaction energies confirm that the higher recoveries with PEM-coated membranes are due to higher charge and hydrophilicity relative to the CS-blocked counterpart. The pre-elution recovery with PEM-coated membranes at high cross flow rates is >70%, which might eliminate the need for elution and backflushing steps, thus reducing both the time required for pathogen concentration and the volume of the final sample. Operating the filter at high transmembrane pressures and crossflow rates leads to a significant increase in the concentration rate; for 2 example, for CS-blocked membranes the initial rate of 5.8 ± 0.3 L/(min·m ) was achieved without affecting P22 recovery; this flux value is almost 4 times higher than values reported in the literature. In addition, the effects of crossflow and high permeate flow rate on the recovery and removal of infective virus from DI and surface water are evaluated using the CS-blocked membrane. An increase in the average permeate flux (up to 5-fold for DI water and 2-fold for surface water over values reported in literature) does not affect the recovery or removal of infective P22. Finally, the performance of the anti-adhesive PEM membrane coatings with complex water matrices is evaluated. The data are only preliminary as only a small number of filtrations have been performed but results seem to indicate that PEM-coated membranes can maintain their advantage over CS-blocked membrane in terms of P22 pre-elution recovery when concentrating viruses from MBR effluent. When challenged by MBR effluent, PEM-coated membranes also appear to be more resistant to fouling than their CS-blocked counterparts. With surface water however, no difference was observed. ACKNOWLEDGEMENTS I would like to thank my advisor Dr. Volodymyr Tarabara for his time and guidance on this research project and his patience and encouragement in difficult times. I would like to thank my committee members Dr. Merlin L. Bruening, Dr. Syed A. Hashsham and Dr. Irene Xagoraraki for their suggestions and help with this project. I would also like to thank Lori Larner for being so helpful and efficient with all administrative matters and more. iv TABLE OF CONTENTS List of Tables ............................................................................................................................... viii List of Figures ................................................................................................................................ ix Abbreviations ................................................................................................................................. xi Chapter 1. Introduction ................................................................................................................... 1 1.1 Waterborne pathogen collection and quantification: importance and challenges ............ 1 1.1.1 Waterborne disease outbreaks................................................................................... 1 1.1.2 Virus detection: Needs, challenges and current methods ......................................... 2 1.2 Polyelectrolyte multilayer films as anti-adhesive recoverable membrane coatings ...... 11 1.2.1 Polyelectrolyte multilayer (PEM) films .................................................................. 11 1.2.2 Anti-adhesive performance of PEMs ...................................................................... 11 1.2.3 PEM films as sacrificial layers ............................................................................... 15 1.3 Virus interaction with inert surfaces: Methods, challenges and current knowledge ...... 15 1.3.1 Virus surface characterization................................................................................. 15 1.3.2 Quantifying interactions between viruses and a surface ......................................... 19 1.3.3 Current knowledge .................................................................................................. 24 1.4 Dissertation overview..................................................................................................... 26 References ................................................................................................................................. 28 Chapter 2. Anti-adhesive membrane films for virus concentration and recovery from water prior to detection .................................................................................................................................... 42 2.1 Introduction .................................................................................................................... 42 2.2 Materials and Methods ................................................................................................... 46 2.2.1 Reagents .................................................................................................................. 46 2.2.2 Bacteriophage ......................................................................................................... 47 2.2.3 Bacteriophage characterization ............................................................................... 47 2.2.4 Crossflow concentration apparatus ......................................................................... 48 2.2.5 Membrane preparation ............................................................................................ 49 2.2.6 Membrane characterization ..................................................................................... 50 2.2.7 Concentration procedure ......................................................................................... 50 2.2.8 Sample analysis....................................................................................................... 52 2.2.9 Data analysis and statistics...................................................................................... 53 2.2.10 Determination of the fouling resistance Rf ............................................................. 54 2.2.11 Blocking law analysis ............................................................................................. 55 2.2.12 Calculation of the energy of interaction between P22 phage and membrane surfaces using the XDLVO approach ................................................................................................. 55 2.2.13 Effect of polyelectrolytes and CS on qPCR analysis .............................................. 57 2.3 Results and Discussion ................................................................................................... 58 2.3.1 PEM selection ......................................................................................................... 58 v 2.3.2 Properties of CS-blocked and PEM-coated membranes and P22 phage ................ 59 2.3.2.1 Membrane permeability and fouling mechanisms .............................................. 59 2.3.2.2 Surface properties of membranes and P22 phage ............................................... 60 2.3.2.3 Virus-membrane interaction energies ................................................................. 64 2.3.3 Virus recovery with PEM-coated and CS-blocked membranes ............................. 65 2.3.3.1 Pre-elution recovery ............................................................................................ 65 2.3.3.2 Post-elution recovery and potential of PEMs as sacrificial coatings .................. 67 2.3.3.3 Reproducibility .................................................................................................... 69 2.3.4 Virus log removal ................................................................................................... 71 2.3.5 Effect of operational conditions on virus concentration ......................................... 72 2.3.5.1 Operational conditions and flux .......................................................................... 72 2.3.5.2 Effect of Jcf / J p on virus recovery ................................................................... 75 2.3.6 Potential for practical applications.......................................................................... 77 Acknowledgements ................................................................................................................... 78 References ................................................................................................................................. 80 Chapter 3. Effect of flow conditions and water composition on the removal and recovery of infective bacteriophage by crossflow filtration with CS-blocked membranes ............................. 86 3.1 Introduction .................................................................................................................... 86 3.2 Material and Methods..................................................................................................... 88 3.2.1 Reagents .................................................................................................................. 88 3.2.2 Water samples ......................................................................................................... 88 3.2.3 Bacteriophage ......................................................................................................... 89 3.2.4 Membrane preparation, crossflow concentration apparatus and concentration procedure............................................................................................................................... 89 3.2.5 Sample analysis....................................................................................................... 90 3.2.6 Calf serum layer stability test ................................................................................. 91 3.3 Results and Discussion ................................................................................................... 92 3.3.1 Effect of filtration conditions on the recovery and removal of infective P22 ........ 92 3.3.2 qPCR vs. plaque assay ............................................................................................ 97 3.3.3 DI water vs. surface water .................................................................................... 100 3.3.4 Effect of filtration condition on CS layer integrity ............................................... 101 3.3.5 Conclusion ............................................................................................................ 103 References ............................................................................................................................... 105 Chapter 4. Virus recovery and concentration from complex water matrices using PEM-coated membranes: Preliminary assessment .......................................................................................... 107 4.1 Introduction .................................................................................................................. 107 4.2 Materials and Methods ................................................................................................. 109 4.2.1 Reagents ................................................................................................................ 109 4.2.2 Water samples ....................................................................................................... 109 4.2.3 Water quality testing. ............................................................................................ 109 4.2.4 Bacteriophage ....................................................................................................... 110 4.2.5 Membrane preparation, crossflow concentration apparatus and concentration procedure............................................................................................................................. 110 4.2.6 Sample analysis..................................................................................................... 111 vi 4.3 Results and Discussion ................................................................................................. 112 4.3.1 Water quality......................................................................................................... 112 4.3.2 P22 recovery and removal from MBR effluent and surface water samples ......... 113 4.3.3 Effect of backflushing on P22 recovery from surface water. ............................... 117 4.3.4 Fouling resistance of CS-blocked and PEM-coated membrane ........................... 117 4.3.5 Conclusion ............................................................................................................ 118 References ............................................................................................................................... 121 Chapter 5. Suggested future research.......................................................................................... 122 APPENDICES ............................................................................................................................ 126 Appendix A. Determination of crossflow and permeate fluxes used by Morales-Morales et al. [1] and Hill et al. [2-4] .................................................................................................... 126 References ....................................................................................................................... 128 Appendix B. Addition of carrier RNA to sample: effect of DNA extraction/detection ...... 130 References ....................................................................................................................... 132 Appendix C. Compaction behavior of PEM-coated membranes and CS-blocked membranes. ............................................................................................................................................. 134 Appendix D. PEM layer stability during filtration and elution. .......................................... 135 Appendix E. Preliminary work on visualization of virus adhesion on surfaces.................. 137 References ....................................................................................................................... 142 vii LIST OF TABLES Table 1.1: Virus recovery using the VIRADEL method ................................................................ 4 Table 1.2: Virus recovery by methods other than crossflow filtration or VIRADEL .................... 9 Table 1.3: Virus recovery by crossflow filtration ......................................................................... 10 Table 2.1: Primer and probe sequence (from Masago et al. [45]) ................................................ 53 Table 2.2 Measured contact angles, calculated surface energy parameters and free energy of interfacial interaction when immersed in water for P22 phage, CS-blocked membranes and PEMcoated membranes. ........................................................................................................................ 63 Table 4.1: MBR effluent and surface water TOC levels ............................................................ 113 Table 5.1: Virus recovery performance of PEM-coated membrane and calf serum-blocked membrane at the pre-elution (rpre), post-elution (rpost) and coating removal - through elution or backflush - (rsacrificial) stages. ................................................................................................... 124 Table B.1: Effect of carrier RNA addition on CP value obtained by qPCR ............................... 131 viii LIST OF FIGURES Figure 2.1: Comparison of the proposed virus pre-concentration approach based on polyelectrolyte multilayer coatings (right) with other current methods. ...................................... 44 Figure 2.2: Crossflow filtration apparatus .................................................................................... 49 Figure 2.3: Filtration conditions in experiments on P22 preconcentration and recovery using CSblocked and PEM-coated membranes.. ......................................................................................... 51 Figure 2.4: Effect of various polyelectrolytes and calf serum on the P22 concentration determined by qPCR. Error bars indicate the standard deviation interval.. ................................. 59 Figure 2.5: Blocking law analysis for fouling of CS-blocked and PEM-coated membranes during filtration of DI water spiked with P22 stock. A) Distributions and contributions of the blocking mechanisms in terms of permeate volume. B) Inverse cumulative flow rate (t/V) as a function of permeate volume V for CS-blocked and PEM-coated membranes. ............................................. 61 Figure 2.6: XDLVO energy profiles for the interaction of P22 with a) CS-blocked membranes and b) PEM-coated membranes at pH = 6 and in 10 mM KCl. .................................................... 65 Figure 2.7: Pre-elution and post-elution (see inset) recovery of P22 from DI water.................... 67 Figure 2.8: Relative frequency of occurrence of P22 (a) pre-elution and (b) post-elution recoveries from DI water under the operational conditions optimized to maximize P22 recovery ....................................................................................................................................................... 70 Figure 2.9: P22 removal from DI water by CS-blocked and PEM-coated membrane at various J cf / J p . ....................................................................................................................................... 71 Figure 2.10: Observed fouling resistance (averaged over the duration of experiment) for CSblocked and PEM-coated membranes during the concentration of 1L of DI water seeded with P22 to 250 mL at various crossflow to permeate flow ratios. ...................................................... 73 Figure 2.11: Filtration conditions: average permeate flux and crossflow flux, used for P22 recovery with CS-blocked membrane and PEM-coated membranes ........................................... 74 Figure 2.12: Pre-elution recovery of P22 from DI water as a function of the fouling resistance to membrane resistance ratio............................................................................................................. 77 Figure 3.1: Filtration conditions in experiments on infective P22 concentration and recovery from DI water and surface water using CS-blocked membranes… ............................................. 90 ix Figure 3.2: Effect of crossflow filtration on a) pre-elution recovery, b) post-elution recovery, c) removal of infective P22 by crossflow filtration with CS-blocked membrane ............................ 94 Figure 3.3: Effect of crossflow filtration conditions on fouling, measured by the ratio of final over initial permeate flux for DI water and surface water. ........................................................... 96 Figure 3.4: Effect of analysis method on P22 a) pre-elution recovery, b) post-elution recovery, and c) removal by crossflow filtration with CS-blocked membrane. One filtration was run for each set of conditions.. .................................................................................................................. 99 Figure 3.5: Dextran rejection by CS-blocked membrane under increasing Jcf / J p during a) filtration and b) elution ............................................................................................................... 102 Figure 4.1: Filtration conditions in experiments on P22 concentration and recovery from MBR ..................................................................................................................................................... 111 Figure 4.2: a) P22 recovery and b) removal from DI water (data from Chapter 2), MBR effluent and surface water with CS-blocked and PEM-coated membranes under “highest recovery” conditions. ................................................................................................................................... 115 Figure 4.3: a) P22 recovery and b) removal from MBR effluent with PEM-coated membrane at high and low permeate fluxes… ................................................................................................. 116 Figure 4.4: Fouling observed for CS-blocked membrane and PEM-coated membrane during filtration tests performed to recover P22 from DI water, MBR effluent and surface water under a) “highest recovery” conditions and b) “fastest filtration” conditions. ......................................... 119 Figure C.1: Compaction and decompaction behavior of bare PES membranes, CS-blocked membranes and PEM-coated membranes. .................................................................................. 134 Figure D.1: Dextran rejection by PEM-coated membrane under increasing Jcf / J p during a) filtration and b) elution.. ............................................................................................................. 136 Figure E.1: AFM topographic images of a) (PDADMA/PSS)4.5 on gold substrate b) and c) (PDADMA/PSS)4.5 on mica dipped in P22 suspension ............................................................. 138 Figure E.2: Fluorescence images of serial dilution samples. a) corresponds to the 1:1000 dilution, 4 5 6 b) to the 1:10 dilution, c) to the 1:10 dilution and d) to the 1:10 dilution ............................. 140 Figure E.3: Fluorescence images of a) (PSS/PAH)4-coated ; b) (PSS/PAH)4.5-coated and c) bare anodisc filters dipped in P22 suspension. ................................................................................... 141 x ABBREVIATIONS AFM atomic force microscopy BE beef extract BSA bovine serum albumin CHI chitosan CN cellulose nitrate CS calf serum DE diatomaceous earth DI deionized DLVO Derjaguin, Landau, Verwey and Overbeek E1 echovirus 1 FLOC flocculation HA hyaluronic acid HAdV human adenovirus HAV hepatitis A virus HE heparin HSA human serum albumin IEP isoelectric point J cf crossflow rate Jp permeate flux LRV log removal xi MBR membrane bioreactor MNoV murine norovirus MWCO molecular weight cut off NaPP sodium polyphosphate NOM natural organic matter NoV norovirus PAA poly(acrylic acid) PAAm polyacrylamide PAH poly(allylamine hydrochloride) PAN polyacrylonitrile PDADMAC poly(dimethyldiallylammonium) PEG poly(ethylene glycol) PEI polyethyleneimine PEM polyelectrolyte multilayer PGA poly(L-glutamic acid) PLL poly(L-lysine) PSU polysulfone PV poliovirus QCM quartz crystal microbalance RV-A group A rotavirus SW sewage TW tap water XDLVO extended Derjaguin, Landau, Verwey and Overbeek xii Chapter 1. Introduction 1.1 1.1.1 Waterborne pathogen collection and quantification: importance and challenges Waterborne disease outbreaks Waterborne diseases are infections transmitted through contact with or consumption of contaminated waters. The main etiological agents are bacteria, protozoa and viruses, and the main reservoirs of concern are recreational waters and surface and groundwater used as sources of drinking water. Progress in drinking water treatment and regulation since the beginning of the th 20 century [1] led to a decrease in the occurrence of waterborne disease outbreaks from exposure to contaminated drinking water. As a result, such outbreaks have become relatively uncommon in the U.S. and other developed countries [2]. For example, the Center for Disease Control listed on average 18 disease outbreaks associated with drinking water per year for the 1999-2008 period in the United States (actual outbreak occurrences might have been higher as it has been suggested that only 10% to 50% of outbreaks are actually reported [1]). These outbreaks resulted in an average of about 1,000 sick individuals and 2 deaths per year [3-7]. Since 2000, approximately 15% of the outbreaks for which the etiological agent was identified have been caused by virus contamination [4-7]. In contrast, occurrences of waterborne disease outbreaks caused by exposure to contaminated recreational water in the U.S. are on the rise from an average of 31 outbreaks resulting in about 1,200 illness per year for the 1999-2004 period to an average of 53 outbreaks resulting in about 4,600 illness per year for the 2005-2008 period [3, 8-11]. Virus-associated outbreaks accounted for 3% to 10% of the events for which the 1 etiological agents has been identified, with norovirus being the most prevalent viral etiological agent identified. A recent review of all published literature on virus-associated waterborne disease outbreaks also found norovirus to be the largest cause of outbreaks with adenoviruses and echoviruses coming in second and third position, respectively [12]. In swimming pools, where almost half of outbreaks occurred, inadequate disinfection was often the culprit. In lakes and ponds, the second largest affected recreational type of water, water quality surveillance is the most effective means of preventing outbreaks [12]. 1.1.2 Virus detection: Needs, challenges and current methods Detection of waterborne pathogens is essential because: i) although deficiencies of the water treatment system can be minimized, zero risk cannot be achieved [13] and the consequences of one incident can be very large such as in the cases of the 2000 Walkerton, ON outbreak that affected over 2,000 people and killed 6 [14]; or the 1993 Milwaukee outbreak where more than 400,000 were affected [1, 15, 16]. And as the number of people more susceptible to infection (individuals with weak immune systems) increases [2], the extent of these consequences can be expected to increase . ii) The detection of pathogen in recreational water is a key factor in preventing outbreaks through this route of exposure [12, 17]. iii) As direct and indirect water reuse increases [18, 19], the potential for drinking water contamination increases and so does the need for monitoring the microbiological quality of water. This is especially true for viruses as several studies have shown that viruses were more resistant than bacteria with respect to environmental conditions and other stressors including disinfection [2]. Infective viruses have been found in 5% of groundwater samples taken from 35 different states 2 [20] and were also found in drinking water that met bacteriological standards and contained an adequate level of chlorine [1, 2, 21]. The methods currently employed to concentrate and quantify pathogens in water are complex and time consuming. The first difficulty is that there is currently no approved method to simultaneously collect and concentrate all microorganisms [22, 23]. The VIRADEL (VIRus ADsorption-ELution) method, which is the EPA-approved method of virus collection, involves the filtration of a large sample (up to 1,000 L for drinking water) with a microfilter either positively charged [24-33] or negatively charged [26, 30, 32, 34-36]. Positively charged filters are usually favored as the use of negatively charged ones requires the acidification of the sample at a pH of 3.5 and sometimes the addition of multivalent cation salts [32, 36], which might affect virus integrity and infectivity [37]. During filtration, viruses are adsorbed by the filter (mostly through electrostatic interactions) and are later eluted using a basic 1.5% to 6% beef extract (BE) solution and/or 0.05 M glycine solution. If further volume reduction is required, this step can be followed by flocculation to precipitate viruses [32]. The method greatly differs from methods of bacteria collection and protozoa collection. The former usually involves collection of bacteria at the surface of a microfiltration membrane [38, 39] while the latter includes depth filtration followed by elution with a detergent solution and centrifugation [40]. 3 Table 1.1: Virus recovery using the VIRADEL method Virus Water 1 Flocculation step 2 Filter (+/-) / 3 Treatment Sample amendment coliphage TW no NA double 1-MDS (+) coliphage TW no NA CN (-)/PEI coliphage TW no NA coliphage SW no coliphage SW Elution 6 Recovery (%) Ref. 3% BE , pH 9 12 ± 6 [25] 4 3% BE, pH 9 44 ± 8 [25] DE (-)/Nalco 5 3% BE, pH 9 – drop by drop 103 ± 7 [25] NA DE (-)/Nalco 3% BE, pH 9 – drop by drop 71 ± 15 [25] no NA double 1-MDS (+) 3% BE, pH 9 39 ± 5 [25] coliphage SW no NA DE (-)/Nalco 3% BE, pH 9 47 ± 15 [25] coliphage SW no NA Double 1-MDS (+) 3% BE, pH 9.5 14 [30] coliphage SW no NA 50 S Zeta Plus (+) 3% BE, pH 9.5 14 [30] coliphage SW no pH 3.5/ AlCl3 Filterite (-) 3% BE, pH 9.5 17 [30] coliphage sea no Prefiltered cellulose ester 1.5% BE, pH 9 27 [37] 4 Table 1.1 (cont’d) MS2 TW no NA DE (-)/FeCl3 + AlCl3 3% BE pH 9 53 ± 12 [41] PV1 TW no NA Nanoceram (+) 1.5 % BE/0.05M Gly pH 9 51 ± 26 [27] PV1 TW no NA 1-MDS (+) 1.5 % BE/0.05M Gly pH 9 67 ± 6 [27] PV1 TW no NA MK (+) 3% BE/0.05M Gly pH 9.5 101 ± 57 [28] PV1 TW no NA 50 S Zeta Plus (+) 0.3% BE/).05 M Gly, pH 9.5 56 ± 8 [29] PV1 sea yes pH 3.5/ AlCl3 epoxy fiberglass (-) 6% BE pH 10.5 36 ± 5 [34] PV3 TW yes NA glass wool 3% BE, 0.5M Gly, PH 9.5 98 ± 24 [42] HNoV TW no 25 mM MgCl2 cellulose esters (-) 0.5 mM H2SO4/1mM NaOH 55 to 104 [26] HNoV river no 25 mM MgCl2 cellulose esters (-) 0.5 mM H2SO4/1mM NaOH 11 to 18 [26] HNoV TW no NA 1-MDS (+) 3% BE pH 9 14 to 46 [26] 5 7 Table 1.1 (cont’d) HAdV TW yes NA glass wool 3% BE, 0.5M Gly, PH 9.5 28 ± 14 [42] HAdV GW yes NA glass wool 3% BE, 0.5M Gly, PH 9.5 8±4 [42] HAdV TW no NA MK (+) 1% BE, 0.25 N Gly, pH 9.5 0.007 to 0.02 [24] 1 2 3 4 5 6 7 type of water: TW: tap water, SW: sewage, GW: groundwater filter surface charge filter pretreatment CN: cellulose nitrate DE diatomaceous earth BE: beef extract Gly: glycine 6 The VIRADEL method also suffers, in some cases, from poor recovery efficiencies and large standard deviations (Table 1.1) [23]. For example, Borrego et al. observed that less than 35% of the indigenous Escherichia coli phages present in tap water spiked with sewage were adsorbed on the Virosorb 1-MDS filter (the only electropositive filter suggested by EPA for the VIRADEL method), and less than 12% were recovered by elution [25]. Low elution recovery number were also observed from Abdelzaher et al. who only eluted up to 35% of the coliphage spiked in seawater and adsorbed on a negatively charged cellulose membrane [37]. The method is also very sensitive to water quality. Haramoto et al. showed that recovery of norovirus (NoV) spiked in surface water was 80% less than the recovery observed when NoV was spiked in deionized water [26]. This leads to unacceptably low recoveries for certain kinds of viruses such as adenovirus for which recovery as low as 0.02% has been reported [24]. Several groups have investigated other positively charged filters as alternatives to Virosorb microfilters, because of Virosorb’s high cost and vulnerability with respect to clogging by colloids [25, 27, 28, 30, 31, 43]. The MK filter was less efficient (lower recovery and greater variability) [28], while Zeta Plus 50S,which seems as efficient as Virosorb to recover virus from various type of water, was not available as a cartridge and thus limited to smaller water volumes [30, 31]. Nanoceram, a cheaper positively charged filter was found to be as efficient as Virosorb [27]. Negatively charged filters made of diatomaceous earth (DE) treated with cationic polymer solution (such as Nalco 7111) showed improved coliphage recovery from sewage and sewage spiked tap water samples [25] when compared with Virosorb filters, but unless a drop by drop elution was performed, coliphage recovery was still less than 50% for sewage effluent samples (data not available for tap water samples). 7 Other methods such as ultracentrifugation [44, 45], centrifugal ultrafiltration [46], flocculation-re-dissolution-ultrafiltration [47], and tangential filtration have also been investigated (Table 1.2). Tangential filtration (also known as crossflow filtration) has emerged as the most promising alternative to VIRADEL [24, 48-54] due to its ability to concentrate large volumes of water relatively fast. Centrifugation-based methods are still of interest for secondary concentration purposes. The crossflow filtration method has been shown to give significantly better results than the VIRADEL method [48] and can also be used to collect and concentrate bacteria and protozoa [55-61]. Crossflow ultrafiltration also presents the advantage of maintaining virus integrity as, ideally, virions remain suspended in the retentate throughout the concentration process. At the same time, low molecular weight solutes, which can potentially inhibit qPCR detection, can pass through the membrane and are not concentrated [22]. In practice, hollow fiber modules have been the most commonly used membrane configuration [48, 50, 51, 60, 61, 65, 66]. These filters have the advantage of a high surface area to volume ratio allowing practical transport of the concentration device to the filtration site if needed and filtration of large volumes of water in a relatively short amount of time. They can also be reusable, thus making the procedure more cost-effective. 8 Table 1.2: Virus recovery by methods other than crossflow filtration or VIRADEL Virus 1 Water Method Recovery (%) Ref. RV-A SW Ultracentrifugation Qbeta TW Electronegative membrane vortex HAdV 2 eluates Centrifugal filtration 33 ± 14 [63] PV1 eluates Centrifugal filtration 95 ± 5 [63] 3 sea ultracentrifugation 76% [64] 3 sea flocculation 22% [64] Viruses Viruses 1 2 34-60 [45] 2 26-67 [62] type of water: TW: tap water, SW: sewage i) Metallic cations are added to water samples. ii) Samples are then filtered on electronegative microporous membranes. iii) Membranes are then vortexed in presence of an elution buffer. iv) the elution buffer is centrifuged to separate membrane debris from viruses in suspension 3 enumerated by epifluorescence and consequently species were not identified (other virus were enumerated by plaque assay or qPCR) Nevertheless, crossflow filtration also requires that the membrane surface be covered or “blocked” by a layer of proteins (beef extract, calf serum, bovine serum albumin) or a chemical dispersant (NaPP) [52, 57, 58] to improve recovery. Protein-blocked membranes might be prone to contamination during storage and transport [57]. In addition, values and reproducibilities of recoveries of certain viruses such as HAdV remain low (Table 1.3) [24]. 9 Table 1.3: Virus recovery by crossflow filtration Virus Water 1 Membrane Blocking Recovery (%) Ref. no blocking 4.5 ± 2.9 [58] DIW + E-coli 15-20 kDa PSU no blocking 29.5 ± 7.1 [58] DIW + E-coli 15-20 kDa PSU 3 % BE 54.3 ± 23.8 [58] MS2 TW 15-20 kDa PSU 0.1 % NaPP 53 ± 13 [61] MS2 TW 15-20 kDa PSU 5% CS 108 ± 16 [57] MS2 TW 15-20 kDa PSU 5% CS 120 ± 22 [56] T1 surface water 50 kDa PAN 5% CS 73 ± 17 [60] PP7 surface water 50 kDa PAN 5% CS 62 ± 5 [60] MNoV DIW 15-20 kDa PSU no blocking 2.0 ± 1.5 [58] MNoV DIW + E-coli 15-20 kDa PSU no blocking 5.3 ± 6.2 [58] MNoV DIW + E-coli 15-20 kDa PSU 3 % BE 63.3 ± 29.7 [58] NoV surface water ND 0.1% BSA <0.95 [24] HAdV surface water ND 0.1 % BSA 3.18 – 6.02 [24] E1 TW 15-20 kDa PSU 0.1% NaPP 49 ± 15 [61] PV1 DIW 10 kDa no blocking 16.9 - 17.8 [52] PV1 Animal-viruses 15-20 kDa PSU MS2 1 DIW MS2 Phages MS2 DIW 10 kDa 3% BE 49.6 – 76.8 [52] type of water: DIW: deionized water, TW: tap water, SW: sewage 10 1.2 1.2.1 Polyelectrolyte multilayer films as anti-adhesive recoverable membrane coatings Polyelectrolyte multilayer (PEM) films PEM films consist of alternating layers of polycations and polyanions. They can form by the simple alternating adsorption of oppositely charged polyelectrolytes on a substrate (layer by layer assembly) through electrostatic interactions [67]. The formation of PEM films through Hbonding has also been shown [68]. By choosing different polyelectrolytes to build the film and by varying the conditions of polyelectrolyte deposition (e.g., pH and ionic strength of the polyelectrolyte solution), films with a wide range of surface charge, hydrophilicity, swellability, and stiffness [69-74] have been prepared. PEM films have been deposited onto porous supports to prepare nanofiltration membranes with unusually large water permeabilities [75-78] but also as anti-adhesive coatings on filtration membranes [79, 80] or other surfaces [68, 72, 81-90], to decrease the adsorption of one or several proteins [68, 72, 80-83, 91, 92], selected mammalian cells [68, 72, 84-88], or selected bacteria [81, 84, 89, 90]. 1.2.2 Anti-adhesive performance of PEMs Meier-Haack and Muller [83, 91] achieved a 10-fold decrease in the amount of human serum albumin (HSA) irreversibly adsorbed on a polypropylene microfiltration membrane during filtration by coating the membrane with a PEM composed of poly(dimethyldiallylammonium) (PDADMAC) and poly(acrylic acid) PAA; coating with the PEM increased HSA rejection but did not impair the filtration flux. Mendelsohn et al. showed that murine fibroblast cell adhesion 11 on a substrate was completely eliminated by coating the surface with ten poly(allylamine hydrochloride) (PAH)/PAA bilayers. Yang et al. achieved the same result with only one bilayer of PAA/polyacrylamide (PAAm), and the film anti-adhesive properties were preserved for more than a month [68, 72]. Lichter et al. have demonstrated that a PAH/PAA coating on a titanium alloy also decreased bacterial adhesion (Staphylococcus epidermis and Escherichia coli) by almost two orders of magnitude [89]. PEMs built using natural polypeptides and polysaccharides have been of particular interest in the field of biomedicine. Richert et al. used hyaluronic acid (HA) and chitosan (CHI) to form PEM films that decreased rat chondrocyte adhesion by more than 90% and bacterial adhesion (E. coli) by approximately 80% [84]. Poly(L-lysine) (PLL)/alginate films and heparin(HE)/CHI films also demonstrated anti-adhesive properties for fibroblast cells and E. coli, respectively [86, 90]. The mechanisms involved in the adhesion of proteins, mammalian cells and bacteria are not fully understood; however, we do know that although proteins play a large role as promoters in mammalian cell and bacteria adhesion, there is not always a correlation between protein adhesion to a surface and mammalian cell or bacteria adhesion to the same surface [72]. Protein adhesion onto PEM films is mostly regulated by electrostatic forces. In conditions where proteins are negatively charged they tend to adsorb a lot more onto a PEM that contains a polycation as the outermost layer and vice versa. In addition pH and ionic strength strongly affect this adsorption behavior by altering the protein and polyelectrolyte charge densities and screening those charges, respectively [72, 80, 81, 83, 91]. When both the protein and the top 12 layer have the same charge, protein adsorption is low unless the pH is close to the protein and top polyelectrolyte layer’s pI, where electrostatic repulsion is low enough that hydrophobic interaction can play a role [91]; as expected in that case, increasing the ionic strength had no effect on the adsorption of proteins [82]. The effect of the charge density of the PEM top layer on adhesion can be of two types. As mentioned earlier, increasing the charge density of the PEM top layer can increase electrostatic repulsion and attraction. In addition, it can also affect the conformation of the layer [74]. At higher charge density, polyelectrolyte chains adopt a flatter conformation and form thinner layer while at lower charge density layers tend to be thicker and loopier [74]. If a condensed high charge density layer is deposited on top a loopier one, it is possible for some loops and segment from the layer before last to reach the PEM surface and affect adsorption behavior [90]. This phenomenon might explain observations by Muller et al. who used a strong polyanion with a high negative charge density, instead of weak polyanions, to build the PEM’s outermost layer and saw an increase in the adsorption of the negatively charged human serum albumin (HSA) [91]. Muller et al. speculated that in the case of PEMs containing strong polyanions, strong attraction between the protein’s positively charged segment (although HSA’s net charge is negative, some segments are positively charged) and the polyanion lead to a reorientation of the protein to favor binding between the two. In the case of PEMs containing weak polyanions, attractive interactions between the protein’s positive segments and the polyanions are not strong enough to orient the protein to allow binding and thus the repulsion between the protein’s negatively charged domains and the polyanions dominate the interaction [91]. Salloum et al. also found that the use of more swellable PEM films decreased significantly the amount of protein adsorbed by the surface compared to other PEMs, including those charged similarly to the sorbing protein. In two other studies, however, no correlation between PEM 13 swelling and protein adsorption was found [72, 82]. The PEM film’s ability to swell was also correlated with its ability to resist adhesion of mammalian cells and bacteria [68, 72, 84]. In fact, poor swellability and stiffness [87, 89], which both depend on the amount of cross-linking between the polycations and the polyanions [72, 87, 88, 92], are the only two properties of the PEM film that could be correlated with the adhesion of bacteria or mammalian cells. Neither the nature (polyanion or polycation) of the outermost layer, the surface charge density, the roughness, the wettability, the conformation of the layer (flat and smooth or thick and loopy) nor the interaction energy (estimated using the Lifshitz-van der Waals acid-base approach described by van Oss [93]) of PEM film was shown to impact cell attachment [72, 89]. To explain the correlation between cell adhesion and swellability, Mendelsohn et al. hypothesized that in solution the water rich structure of the film does not allow cell’s adhesion proteins to adapt a configuration supporting cell adhesion. The environment “looks” more like water than a surface to the cell, which is why cell adhesion does not occur [72]. Lichter et al. showed that a 100-fold increase in elastic modulus resulted in approximately a 100-fold decrease in bacterial adhesion and speculated that as the surface become stiffer, bacteria fimbriae interactions with the surface are altered. More precisely, the fimbriae retraction after collision with the surface is slower with a stiffer surface because there is more mechanical resistance to the retraction; this additional time of contact between the bacteria and the surface would enhance bacterial adhesion [89]. 14 1.2.3 PEM films as sacrificial layers When appropriately constructed, a PEM can be disassembled by way of exposure to high [69, 94], neutral [95, 96] or low [97] pH, higher ionic strength [98-100], a specific solvent [101] or lower [102] or higher [103] temperature. These properties of PEM have been exploited to create micropatterned [95], porous [100] or even self-standing [98] PEM films. For example Dubas was able to create a free standing PSS/PDADMAC multilayer by depositing 20 bilayer of PSS/PDADMAC on top on 20 bilayer layers of PAA/PDADMAC and exposing the film to a salt concentration higher than 0.6 M. In these conditions PAA/PDADMAC dissociates while PSS/PDADMAC remains stable [98]. Sacrificial PEM layers have been considered for the controlled delivery of drugs [101], the development of easy to clean surfaces [97] and the control of membrane fouling during membrane filtration [69]. In that latter study, a PEM was deposited on a UF membrane to create a nanofiltration membrane; once fouled the PEM layer was sacrificed allowing the almost complete removal of both the fouling layer and PEM from the UF membrane surface. The PEM layer could be regenerated to create a new nanofiltration membrane [69]. 1.3 1.3.1 Virus interaction with inert surfaces: Methods, challenges and current knowledge Virus surface characterization To understand virus interaction with surfaces, one must first gather information on the virus’ own surface properties. The surface of a virion (virus particle) consists of a protein shell, called capsid and, in the case of so called enveloped viruses, of a lipid bilayer enveloping the 15 protein shell. Sequencing techniques permit the determination of the composition of the protein shell and theoretical surface properties (e.g. isoelectric point). Such theoretical values, however, do not always accurately predict values measured in experiments [104]. Experimental determination of virus surface properties is thus necessary. Such characterization requires that virions be separated from protein and host cell debris present in the virus growth medium. Purification methods include differential centrifugation and equilibrium gradient centrifugation. In the differential centrifugation method, high and low speed centrifugation are used alternatively to separate soluble components, large macromolecules and cell debris from virions [105]. In the equilibrium gradient centrifugation method, the suspensions of viruses is introduced into a tube where solutions of increasing density have been layered on top of each over. During the centrifugation process virions migrate to the layer corresponding to their density [106, 107]. Others methods have also been used; these include precipitation followed by centrifugation to recover the pellet [108], centrifugal filtration with multiple washings [109], multiple dialysis [110], or successive microfiltration and ultrafiltration using membranes of various molecular weight cut-off (MWCO) values [111]. Once purified, virions can be characterized. The isoelectric point (IEP), a crucial property that indicates if the particle will be positively or negatively charged at a given pH, is determined by analyzing the behavior of the particles in an electric field under different pH conditions. Two methods have been frequently employed: isoelectric focusing (IEF) and determination of the electrophoretic mobility (EM) by light scattering (ELS) or a microscopybased method [112]. In IEF, particles are subjected to an electric field and migrate through a gradient of increasing pH. When the particles reach the pH zone corresponding to its IEP the 16 particle stops. In EM analysis, the electrophoretic mobility, which is the ratio of the migration velocity to the electric field, is measured at various pH values by light scattering or microscopic methods. The EM is used to calculate the zeta-potential for each pH and the pH at which the zeta-potential changes sign is the IEP. Hydrophobicity is another surface characteristic essential for understanding virion interactions with surfaces. When particles are immersed in an aqueous solution, the free energy of cohesion of water drives particles to agglomerate to minimize their surface area exposed to water, this phenomenon is called hydrophobic attraction. Sometimes, this attractive force is attenuated or reversed when interaction between particles and water are preferred to interaction between particles; this component of the total free energy is called hydrophilic repulsion [113]. If hydrophobic repulsion prevails, the material seems to repel water and this property is called hydrophobicity. Van Oss and Giese [114] formally defined the hydrophobicity of a material i based on the interfacial free energy of interaction between two objects of the same material i when immersed in water: Giwi , which is expressed in terms of free energy per unit surface area and can be determined using the following equation: 2   LW      Giwi  2  iLW   w   4  i i   w w   i w   i w      (1.1)   LW  w ,  w and  w are the surface tension parameters of water (the “+”, “-“ and “LW” superscripts correspond to the electron acceptor, the electron donor and the Lifhsitz-van der Waals components of the surface tension, respectively), and  iLW ,  i and  i are the surface tension parameters of the material i . 17 When Giwi is negative, there is a cohesive attraction between the two objects and the material is considered hydrophobic. The magnitude of Giwi can be interpreted as the degree of hydrophobicity [114]. If Giwi is positive the material is hydrophilic. This definition is not yet adopted by the entire scientific community. Often a surface is considered hydrophilic if it is “wetted” by water that is if the water contact angle is smaller than 90º, which does not necessarily corresponds to a positive Giwi . For example dry biological surfaces typically have 2 a negligible  i and a  iLW of approximately 40 mJ/m ; for such surfaces the transition from hydrophilic to hydrophobic corresponds to a water contact angle of approximately 60º (equations 1.1 and 1.2). The surface tension parameters of a given surface can be determined using the extended Young equation (1.2) after measuring the contact angle of three probe liquids with known surface tension parameters  . TOT 1  cos    LW LW      2  s    s   s    (1.2)     In these equations,  is the contact angle for a given probe liquid and the subscripts and  correspond to the solid surface and the liquid probe, respectively. In the case of viruses [115117] and  nanoparticles in general [118, 119], contact angle measurements can be done by  depositing layers of particles on a clean surface and determining the contact angles using the sessile drop method. The roughness of the deposited layer, which can be independently 18 determined by atomic force microscopy (AFM), and remnant contamination will affect the measured contact angle following equations 1.3 and 1.4, respectively: cos apparent  r costheory (1.3) cos apparent  F1 cos1  F2 cos 2 (1.4) where  is the contact angle, r the roughness and Fi the fractional amount of each material present in the layer. It should be noted that in two out of the three studies where the contact angle of a virus was measured [115, 116], the virus suspension was not purified before formation of the virus layer. The measured contact angles were probably significantly affected by the presence of bacterial debris and broth components within the virus deposit. Alternatively, virus hydrophobicity has also been estimated qualitatively by hydrophobic interaction chromatography [120]. 1.3.2 Quantifying interactions between viruses and a surface It is possible to directly measure the interfacial energy of interaction between a surface and a particle using AFM [121-130]. In AFM, a surface is scanned by a tip, which is a part of a flexible cantilever. The position of the cantilever depends on both surface morphology and forces between the cantilever tip and the surface. In force spectroscopy, the vertical movements of the cantilever, proportional to interaction forces, are recorded while the surface is approached and moved away from the tip [131]. A single microparticle composed of silica [121, 123, 125], alumina [121], polystyrene [121, 122], zirconia [124], lactose [127] or a bacterial spore [126], can be glued to a tipless cantilever to study the particle’s interaction with various surfaces. 19 Cantilevers with tips have also been modified with nanoparticles: for example, Vakarelski et al. [130] fabricated a cantilever tip terminated by a single gold nanoparticle; Das et al [129] glued a nanoparticle agglomerate on a cantilever tip and Attinti et al. [117] opted to coat the cantilever tip with nanoparticles. Others chose to deposit microparticles [128] or nanoparticles [132, 133] on the surface scanned by the cantilever, and to functionalize the cantilever tip with molecules of interest such as humic acid [128]. In the field of virology, AFM has mostly been used to image viruses and investigate virus interactions with a host cell or other surfaces through imaging. For example, AFM was used to visualize the pattern formed by phages assembled on a surface and to quantify the number of viruses deposited and/or the presence of aggregates [134-138]). AFM was also used to quantify the binding force between macromolecules present at the surface of a virus capsid and other surfaces by functionalizing the AFM tip with the macromolecules of interest [139]. A few studies used AFM to quantify interaction forces between viruses and surfaces. Attinti et al. [117] studied virus-sand interaction using a virus-coated tip and Liu et al. [140] measured the force of interaction between a tip functionalized with anti-hemagglutinin monoclonal antibody and a single influenza virus deposited on a glass slide. Virus interactions with surfaces such as clay or NOM-coated substrates have also been investigated using Quartz Crystal Microbalance (QCM) gravimetry [141-146]. By measuring very small changes in the mass of material deposited on the crystal surface, QCM enables rigorous quantification of the mass of viruses deposited over time and can be used to study the deposition kinetics. Other methods for studying virus-surface interactions include total internal 20 reflection fluorescence microscopy (TIRF), which has been used to study virus adsorption kinetics [147], other fluorescence microscopies [115], transmission electron microscopy (TEM) [148], and methods that employ radioactively labeled viruses [149]. Finally, in many studies the interaction of a virus with surfaces was evaluated by measuring the difference in the concentration of the virus in suspension (measured by traditional methods such as plaque assay) before and after the suspension is exposed to a surface [116, 120, 150-161]. It should be noted, however, that loss of infectivity or particle aggregation during virus interaction with the surface can affect the results of this test when an infectivity assay is selected as the detection method. Several authors employed the DLVO (Derjaguin, Landau, Verwey and Overbeek) [115, 116, 117, 141, 142, 144, 156, 157, 162-165] and XDLVO (extended DLVO) [115, 116, 117, 156, 157] theories to describe virus attachment to surfaces. The DLVO theory predicts surfacesurface interaction by taking into consideration Liftshitz-van der Waals (U double layer interactions (U considered (U AB EL LW ) and electrostatic ). In the XDLVO model, Lewis acid-base forces are also ). Only one study [115] determined the virus surface tension parameters  LW ,   and   , which allow for the rigorous determination of the Lifshitz-van der Waals and Lewis acid-base interactions; however these viruses were not purified. All but the study by Chattopadhyay et al. [116], computed van der Waals interaction based on the Hamaker method [166]: A rp 132 s U vanderwaal   6h  14h  1      1 (1.5) 21 where r p is the virion radius, h the distance between the virion and the surface,  the characteristic wavelength of the interaction and A132the Hamaker constant for the particlewater-surface system. Most of these studies (7 out of 10) [117, 141, 142, 144, 157, 162, 165] used Hamaker constants based on Murray and Park’s [167] estimation of the poliovirus–waterclay system which itself was based on the Hamaker constant of the polystyrene–water-clay system and the assumption that polystyrene and poliovirus shared similar dielectric properties. By following this approach, these studies did not take into account the potential specificity of each virus surface for the determination of the van der Waals interactions; however, it is true that 2 most biological surfaces have a  LW of about 40 mJ/m ; as a consequence van der Waals interactions between viruses and surface might not differ greatly from one virus species to another [111]. Three studies [156, 163, 164] used the Lifshitz theory [168], which links the substance relative permittivity and refractive index to the Hamaker constant, to determine the virus Hamaker constant. Three studies computed the Lewis acid-base interactions [117, 156, 157] to use the XDLVO model. They did so using Yoon’s empirical approach [169]. which is described in the following equation: K T  cos1  cos 2  U AB   123 with log K123  a b 6h 2   (1.6) where T is the temperature, h the separation distance, 1 and  2 the water contact angles of the virus and the surface and a and b are system specific constants. Yoon’s approach only requires the measurement of the water contact angle rather than the 3 liquid probe contact angles necessary in van Oss’ theoretical approach [113]. Bergendahl and Grasso found that Yoon’s 22 empirical approach and van Oss’s theoretical approach (described in chapter 2) gave similar trends in terms of which interactions were the most attractive; however, calculated values for Lewis acid base interaction energies were quite different; and for one system Lewis acid base interactions were found to be attractive using Yoon’s approach but repulsive using the van Oss rigorous theoretical approach. In Yoon’s approach, variations in water contact angles are used to calculate variations in hydrophobic interactions whereas variations in contact angles are also due to changes in Lifshitz van der Waals interactions. In van Oss’ approach, measuring the contact angle of a completely apolar liquid probe (diiodomethane for example) allows the determination of the Lifshitz van der Waals interaction term independently from the Lewis acid-base term. Additionally, measuring contact angles of two polar liquid probes with different electron donor and electron acceptor characteristics allows the determination of these two parameters for the surface studied [113]. Other models have been used to estimate hydrophobic interaction. Chattopadhyay et al. [116], who defined hydrophobic interaction the same way as van Oss and Giuse [112] ( i.e. hydrophobic interaction is the sum of van der Waals and Lewis acid-base interactions), used the empirical method developed by Neumann et al. [170] to estimate the hydrophobic interaction between bacteriophages and clay. Neumann’s method predicts interfacial tensions between surfaces using only water contact angles [170]; however, several authors have demonstrated that Neumann’s empirical approach is flawed [113, 171]. The hydrophobic interaction term used by Lee et al. did not include the van der Waals interaction and was estimated using an empirical model usually applied to determine protein hydrophobic energy [164]. 23 1.3.3 Current knowledge Sorption of viruses to various surfaces is the subject of numerous studies. Already in 1975 Bitton reviewed more than 50 studies looking at virus adsorption to materials such as activated carbon, nitrocellulose, glass, clays, sands, polyelectrolytes, iron oxides, ion exchange resins and membrane filters [172]. Viruses sorb to a wide range of surfaces including positively charged surfaces such as alumina and cationic polyelectrolytes and negatively charged surfaces such as nitrocellulose, glass, or anionic polymers. Adsorption, especially on negatively charged surfaces, depended on the ionic strength [161, 172]. Indeed high salt concentrations decreased the thickness of the double-layer, allowing negatively charged virus to get close enough to the surface for attractive forces such as van der Waals forces to act. Localized interactions between the positively charged fraction of the virus protein coat and a negatively charged surface could also explain the attachment of viruses to such surfaces [172]. The presence of proteinaceous material such as bovine albumin or bovine serum or natural organic matter hindered virus adsorption on activated carbon, clay, sands, anion exchange resin and membrane filters [160, 172-174]. Some authors suggested these proteinaceous materials competed with virus for the surface adsorption sites [172]; other authors have mentioned the possibility of the thick layer of organic matter on the surfaces increasing steric repulsion between viruses and the surface [174]. It was observed in those earlier studies that not all viruses exhibited similar adsorption behavior; however, only few reports considered viruses’ surface properties and morphologies and how they correlated with the adsorption behavior [175, 176]. It was later found that viruses present a wide range of surface properties and thus a range of sorption behaviors [112, 154]. 24 Michen et al. [112] reviewed 48 studies where the isoelectric point of 104 viruses was measured. The reported IEPs ranged from 1.9 to 8.4 but were mostly below 7, and depended not only on the species but also on the strain. Several viruses (such as poliovirus, mengovirus and coxsackievirus) had 2 IEPs, probably due to a change of conformation of the viral capsid at a certain pH. Viruses also vary widely in terms of their hydrophobicity [116, 117, 120]. An example of a very hydrophilic virus is phiX174 with a water contact angle between 26 ± 2 º [117] and 42 ± 6 º [116]. An example of a hydrophobic virus is T2 with a water contact angle of 96 ± 9 º [116]. The IEP of viruses was a determining factor in virus adsorption indicating the importance of electrostatic interactions for virus attachment to surface [142, 144, 150, 151, 159, 173]. Hydrophobic interactions have also been shown to be important in the attachment of MS2 [116, 151, 153, 156, 157, 173], a hydrophilic virus. In some cases, interaction with hydrophobic surfaces disrupted the virus protein coat and lead to virus disassembly [147]. As ionic strenght increases and repulsive electrostatic interactions decrease, the hydrophobic interaction becomes increasingly important [151]. Other factors that seem to influence virus adsorption include the virus size (higher surface areas present more sorption sites) [114,157], virus morphology (the presence of spikes, fibers, tails, extruding protein loops) [116, 172, 177], and the specific interaction with divalent cations especially Ca 2+ which can form bridges between functional groups on the virus and on the surface [141, 143, 144]. 25 In several studies DLVO theory failed to predict virus attachment behavior [144, 165], probably because of the importance of hydrophobic interaction in virus adsorption to surfaces. Also representing viruses as hard particles in models predicting double layer interactions is not always accurate [178]. Although the XDLVO model predicted the virus attachment experimentally observed in some studies well [116, 157, 164], others found discrepancies between the predicted and experimentally observed virus behavior [117, 156]. 1.4 Dissertation overview This work aims at improving virus recovery and concentration by crossflow filtration. In chapter 2 we designed highly controllable anti-adhesive membrane coatings to replace the traditional protein based blocking layer and assessed their performance in terms of virus recovery and concentration rate, under different filtration conditions that include filtration rates more than double the highest rate reported in the literature. In chapter 3, the effect of high crossflow and high permeate flow rate, which are necessary to hasten the filtration but might affect virus infectivity, on recovery and removal of infective virus from DI and surface water are evaluated using the CS-blocked membrane. 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Chapter 1. 2.1 Introduction Efficient pathogen detection in drinking and recreational water is vital for preventing disease outbreaks. Because waterborne pathogens are present in low concentrations, a fast and reliable concentration step is crucial for their detection. Crossflow filtration with hollow fiber membranes, an emerging technique for concentrating various waterborne pathogens [1-13] including viruses [7-13], offers several advantages over traditional pathogen concentration methods (see below). First, membranes with an appropriate pore size simultaneously concentrate microbial pathogens ranging from protozoa to bacteria to viruses [2, 3, 5, 6] without concentrating molecular toxins and low molecular weight qPCR inhibitors [14]. Second, crossflow decreases membrane fouling and results in increased concentration rates [15]. Third, in contrast to filtration in a dead-end geometry, crossflow minimizes virus-membrane contact so more viruses remain suspended in the retentate throughout the concentration process, facilitating virus recovery [14]. The EPA-approved VIRADEL (VIRus ADsorption-ELution) method [16] for virus concentration includes filtration of a water sample through a positively [7, 16-18] or negatively 42 [16, 18, 19] charged microfilter. During the filtration, viruses adsorb onto the filter, and elution occurs in a high pH solution containing 1.5 to 6% beef extract and/or 0.05 M glycine (Fig. 2.1). If necessary, addition of a flocculant to the eluate can precipitate viruses to further reduce volume [16]. The VIRADEL method often gives low or poorly reproducible recoveries [20]. For example, Virosorb 1-MDS, the only electropositive VIRADEL filter recommended by EPA, adsorbed less than 35% of the indigenous Escherichia coli phages in sewage-spiked tap water, and the eluate contained only 12% of the phages [17]. The VIRADEL method is also sensitive to various water constituents; indeed, norovirus recovery was 92% from deionized (DI) water but only 19% from surface water [18]. In addition, highly adhesive viruses such as human adenovirus (HAdV) [21], give recoveries as low as 0.02% from surface water [7], and norovirus recoveries can also be low [7, 22]. To increase recovery, several studies explored ultracentrifugation [23, 24], centrifugal ultrafiltration (UF) [25], and flocculation-re-dissolutionUF [26]; however, these methods are impractical for large volume samples. Crossflow filtration with a “blocked” membrane (see below) gives recoveries equal to or better than those with VIRADEL for a range of viruses in various types of water [7, 11]. Additionally, the large membrane surface area in hollow fiber cartridges and the use of crossflow to mitigate fouling [15] allow rapid concentration of high-volume samples [2, 4, 6, 11, 12, 27]. Covering or “blocking” the membrane surface with a layer of proteins (beef extract [10, 13], calf serum [13], bovine serum albumin [13]) or glycine [10] is crucial to improve virus recovery during crossflow filtration (Fig. 2.1). 43 Figure 2.1: Comparison of the proposed virus pre-concentration approach based on polyelectrolyte multilayer coatings (right) with other current methods. For interpretation of the references to color in this and all other figures, the reader is referred to the electronic version of this dissertation) These blocking procedures usually employ complex mixtures of macromolecules of various molecular weights to cover virus adsorption sites and possibly minimize virus passage through the membrane filter [2, 3, 5, 7, 11, 28]. Although the term “blocking” has also been used to describe treatment with small molecular weight compounds such as sodium polyphosphate (e.g., 600 Da [3, 6]) and glycine (75 Da), their effect is most likely limited to preventing adsorption of viruses to the membrane surface and does not include true pore 44 blockage. The blocking step can be time consuming (e.g., overnight deposition of a protein layer), and a membrane blocked with proteins might be prone to contamination during storage and transport [3]. In addition for certain viruses such as HAdV recovery values remain low and variable [7] To overcome these challenges we propose coating UF filters with rationally designed polyelectrolyte multilayer (PEM) films [29, 30]. PEM deposition is in effect controlled membrane blocking that employs alternating adsorption of two oppositely charged polymers. PEMs can form quickly (in less than 1 h) and reproducibly [31]. Several studies described antiadhesive PEM coatings on various surfaces [32-35], including membrane filters [36, 37], to decrease the adsorption of selected proteins [32, 33, 36, 37], mammalian cells [32, 34], or bacteria [34, 35]. Although PEMs were employed to create ordered virus monolayers [38, 39], no studies examined virus adhesion to PEM-modified surfaces or applied PEMs to prevent virus adsorption or to enhance recovery for virus concentration and detection. In addition to low and poorly reproducible recoveries, the long duration of the sample concentration step remains a bottleneck in virus detection. For example, concentrating 100 L of tap water to 400 mL takes 2 h with a hollow fiber cartridge, and further volume reduction to a few mL [6] for qPCR analysis requires another 1 to 3 h [6]. Because virus concentrations of less than 1 genomic copy per 100 L of water represent a significant risk of illness [40], virus monitoring often requires testing up to 1,000 L for drinking water [16]. Increasing transmembrane pressure can, in principle, increase filtration rate; however, this may exacerbate membrane fouling, alter virus recovery and offset the gains in the permeate flux. To overcome 45 this limitation we operated the membrane at a high transmembrane pressure while simultaneously increasing the retentate crossflow rate to maintain a high permeate flux while limiting fouling to a manageable level. In summary, this work aims to improve virus concentration by membranes. We designed highly controllable anti-adhesive membrane coatings and assessed their performance in terms of virus recovery and concentration rate. We also evaluated how crossflow rate and permeate flux affect virus rejection, recovery, and rate of concentration with CS-blocked and PEM-coated membranes. The anti-adhesive membrane coating required less than an hour to deposit and increased pre-elution virus recovery up to 2-fold. 2.2 2.2.1 Materials and Methods Reagents Lysozyme (from chicken egg white), ethylenediaminetetraacetic acid (EDTA), calf serum, heparin (sodium salt), chitosan (medium molecular weight), diiodomethane and sodium polyphosphate (NaPP) were purchased from Sigma-Aldrich. Tween 80 (Fisher), tryptic soy broth (Becton, Dickinson) and glycerol (J.T. Baker) were used as received. 46 2.2.2 Bacteriophage Bacteriophage P22 (provided by Prof. Joan B. Rose, MSU) is a non-enveloped, double stranded DNA phage that has been used to understand dsDNA virus assembly [41-44] and as a surrogate for human viruses to understand their fate in the environment [45, 46]. P22 has an icosahedral head with a diameter of 60 nm and a short tail [47]. P22 stock was grown by inoculating Salmonella enterica serovar Typhimurium LT2 (also provided by Prof. Rose) in tryptic soy broth. After incubation bacterial host cells were lysed by adding 0.1 mL of lysozyme (50 mg/mL) and 0.75 mL of EDTA (0.5 M). The culture was then centrifuged for 10 min at 4000 rpm and the supernatant was filtered through a 0.45 μm cartridge filter. P22 stock suspension (~ 3·10 10 plaque forming units per mL) was stored at 4°C. One liter of water was spiked with 1 mL of P22 stock on the day of the filtration. 2.2.3 Bacteriophage characterization To characterize the surface properties of P22 particles, they had to be separated from other components present in the stock, i.e. tryptic soy broth components and host bacteria cell debris. The purification protocol was modified from Mylon et al. [48]. First, 150 mL of P22 stock solution was filtered through a 0.1 μm membrane (Nucleopore, Whatman) using a stirred Amicon 8050 dead-end UF cell (Millipore) to remove molecules and debris larger than 100 nm. The permeate volume was then reduced 5- fold by filtration through a 50 kDa polyethersulfone membrane (Omega, Pall) in an Amicon 8200 filtration cell. At this point the cell was connected to a feed tank containing 1 L of 10 mM KCl. This solution was passed through the 50 kDa 47 membrane to wash away molecules smaller than 50 kDa such as broth components, until only 30 mL remained in the cell. The particle size distribution in this purified stock was measured by dynamic light scattering at pH 6.. The purified P22 stock was then filtered through a 30 kDa polyethersulfone membrane (Omega, Pall) to deposit the equivalent of ~ 9 layers of virus. Contact angles of 3 probe liquids (deionized water, glycerol, diiodomethane) with these layers were measured using the sessile drop method (FTÅ 200 contact angle analyzer, First Ten Angstroms) to determine the surface tension parameters of P22 phage particles (see section 2.2.12). The  -potential of P22 was determined based on electrophoretic mobility using phase 1 analysis light scattering (ZetaPALS, Brookhaven Instrument Corporation) at pH 6 , using purified P22 washed with 1 mM KCl (instead of 10 mM KCl used for particle sizing and contact angle). 2.2.4 Crossflow concentration apparatus Fig. 2.2 shows the schematic of the crossflow concentration unit. A high-pressure peristaltic pump (model 621 CC, Watson-Marlow) drew the solution from the pressurized feed tank to the membrane filtration cell (CF042, Sterlitech), where the membrane surface area exposed to the feed was 41 cm2. The permeate was collected in an Erlenmeyer flask positioned on an electronic mass balance (Adventurer Pro AV8101C, Ohaus) interfaced with a computer. The transmembrane pressure varied from ~ 0.5 bars (7 psi) to ~ 2.8 bars (40 psi). An inline flowmeter (101-7, McMilan) recorded the crossflow velocity. he  -potential of P22 determined with this method is a good descriptor of P22 surface potential only if P22 is a soft particle, which has not been verified here. 48 pressure sensor permeate peristaltic pump membrane module P concentrate flowmeter data acquisition system pressurized 1 L feed tank mass balance Figure 2.2: Crossflow filtration apparatus 2.2.5 Membrane preparation Prior to modification, a polyethersulfone (PES) UF membrane (OMEGA 30 kDa, Pall) was submerged for 24 h in 1 N NaOH and thoroughly rinsed with deionized water. The membrane was either blocked with CS or coated with a PEM film. For CS blocking, the membrane was loaded in the crossflow filtration cell, and 500 mL of 5 % CS solution was circulated over the membrane surface for 16 to 18 h with no pressure differential across the membrane. The filtration unit was then rinsed twice with DI water for 10 min. To coat the membrane with a PEM film, the membrane was placed in a custom-made holder and the membrane surface was alternately exposed to HE solution (1 mg/L, pH 5) and CHI solution (1 mg/L, pH 5) with a 1-min rinse with DI water in between. The duration of each exposure was 5 min. The total number of deposited bilayers was 4.5, where the last half bilayer was HE. Both 49 HE and CHI solutions also contained 0.15 M NaCl. Membranes were prepared immediately prior to filtration. 2.2.6 Membrane characterization The  -potential of the membranes was measured using an electrokinetic analyzer (BIEKA, Brookhaven Instrument Corp.) at pH 6. Membrane hydrophilicity was characterized by measuring water contact angles using the sessile drop method. At least 3 different membranes 2 were used for each analysis. Contact angles of diiodomethane and glycerol were also measured to determine the surface tension parameters of the CS-blocked and the PEM-coated membranes. Water permeabilities of coated membranes were determined before and after membrane compaction by measuring the permeate flux at a transmembrane pressure differential of 40 psi. 2.2.7 Concentration procedure The membranes were first compacted by filtering DI water at 40 psi for 90 min. Filtration of 1 L of the DI water spiked with 1 mL of P22 stock solution was then performed to reduce the volume to 250 mL. The ratio of the crossflow flux to the initial permeate flux, J cf / J p , ranged from 1,500 to 11,100 (Fig. 2.3). Crossflow flux was regulated from 6,800 to 2 26,800 L/(min·m ), which corresponded to Reynolds numbers from 400 to 1,700. 50 this study: CS-blocked membrane initial permeate fllux Jp, L/(min·m2) 10 this study: PEM-coated membrane earlier studies 9 high Jp high Jp 8 high Jcf fastest concentration conditions low Jcf 7 6 5 4 3 (5) 2 (3) (2, 11) 1 highest recovery conditions 0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 crossflow flux Jcf ·104, L/(min·m2) Figure 2.3: Filtration conditions in experiments on P22 preconcentration and recovery using CSblocked and PEM-coated membranes. Number of tests: n=27 for CS, n=22 for PEM. Following the filtration, viruses were eluted from the membrane using 0.01% Tween 80, 0.01% NaPP [2, 3]. The elution occurred with the membrane still in the filtration cell and at the same crossflow rate as in the filtration, but with a retentate pressure of only 2.5 psi, which was due to the crossflow. Aliquots of the feed, retentate, permeate and eluate were stored at 4°C. Samples were also taken during compaction with DI water to verify that no contamination was 51 present before P22 was introduced. A new membrane was used for each filtration and the unit was disinfected with CIDEX (Advanced Sterilization Products) between filtration tests. 2.2.8 Sample analysis The P22 concentration in each sample was determined by qPCR. Within 24 h of the filtration experiment, MagNA Pure Compact System (Roche) was used to extract P22 DNA from 390 μL grab samples into 100 μL eluates. RNA carrier (10 µL, 1 μg/μL) was added to the 390 μL samples before extraction to prevent bacteriophage adsorption on the MagNA Pure system tips and magnetic beads. Each extract was then analyzed by qPCR in triplicate following the protocols described by Masago et al.[45] PCR mixtures (20 μL) contained 5 μL of extracted DNA sample, 2 μL each of forward and reverse primers (5 μmol/μL), 0.3 μL of Taqman Probe (10 μmol/L), 10 μl of PCR master mix (LightCycler 480 Probes, Roche) and 0.7 μL of water. qPCR was performed using the LightCycler 1.5 system (Roche). Primer and probe sequences (Table 2.1), and qPCR conditions were similar to the ones described by Masago et al. [45]. QPCR mixtures were heated at 95°C for 10 min prior to 45 cycles of 95°C for 10 s, 60°C for 20 s and 72°C for 10 s. Finally mixtures were cooled for 30 s at 40°C. To prepare a standard curve linking qPCR crossing-point (CP) values with numbers of P22 DNA copies, P22 DNA standards were prepared following the method described by Xagoraraki et al. [49]. The phage target DNA sequence was amplified by PCR using the same primers that were used for qPCR, and the amplicon was cloned into plasmid vector using the TOPO TA Cloning kit (Invitrogen). Plasmid vector DNA was extracted and purified using QIAprep Spin Miniprep kit (Qiagen) and the DNA concentration was quantified by spectrophotometry using Nanodrop ND-1000 (Thermo Fisher 52 Scientific). The number of DNA copies per unit volume could then be calculated based on the plasmid vector DNA length of 4,000 base pairs (bp) and assuming an average mass per bp of 650 Da. The purified DNA was serially diluted and the dilutions run by qPCR to develop the standard curve. Table 2.1: Primer and probe sequence (from Masago et al. [45]) Primer/probe Sequence Reverse CTT AAC AAG CTC TGA CTG CTC ATC A Forward CCA TCG CCT GTG ACT CGA T Taqman Probe FAM-TCG CAA CGA TGC AGA ACG ACT CGTAMRA 2.2.9 Data analysis and statistics P22 log removal (LRV), percentage of pre-elution recovery ( rpre ), and percentage of post-elution recovery ( rpost ) were calculated using the following equations: C f LRV  log Cp  r pre  (2.1)  ,   (2.2) C rVr  100% , CfVf r post  C rVr  CeVe  100% , CfVf (2.3) 53 where C f , C r , and Ce are P22 concentrations in feed, retentate, and eluate samples, respectively, and V f , V r , and Ve are the volumes of these samples. Virus recovery and virus removal were plotted as a function of the Jcf / J p ratio. The relationships between Jcf / J p , on the one hand, and rpre , rpost and LRV, on the other hand, for the PEM-coated membranes and the CS-blocked membranes were statistically analyzed using the regression procedure of the SAS software. An interaction term (between Jcf / J p and the type of membrane) was introduced in the regression model. The software Minitab was used to statistically characterize the distributions of pre-elution and post-elution recoveries. 2.2.10 Determination of the fouling resistance Rf As we concentrate P22, permeate flux decreases due to fouling of the membrane by virions and other components present in the feed (proteins and bacterial debris). The flow resistance due to fouling at the end of filtration was calculated using the following equation: (2.4) J  R f  Rm  0  1 Jf    Where R f is the resistance due to fouling, Rm the resistance of the blocked or coated membrane, J 0 the average permeate flux during the first minute of filtration and J f is the permeate flux during the last minute of filtration. 54 2.2.11 Blocking law analysis Dead-end filtrations of P22-containing feed solution (1 L of DI water spiked with 1 mL of P22 stock) through CS-blocked and PEM-coated membranes were conducted using an unstirred Amicon 8010 ultrafiltration cell connected to a pressurized feed tank. The permeate flux was recorded continuously for 1 hour using an electronic mass balance connected to a computer. For each experiment the membrane was first compacted for 90 min with DI water. Permeate flux data were then obtained and fitted to the linearized equations describing the four fouling mechanisms: complete blocking, standard blocking, intermediate blocking and cake filtration [50]. To assign a fouling mechanism to each portion of the permeate flux dataset, we used the procedure described by Wang et al. [50]. A core portion of the filtration dataset that 2 fitted a given mechanism with a high coefficient of determination (r > 0.999 unless otherwise specified) was identified and expanded point by point by evaluating if the point belonged to the 95% prediction interval given by the regression. If it did, the point was added to the core and a new linear regression analysis was performed. For more detail on the procedure, please refer to the paper by Wang et al. [50]. 2.2.12 Calculation of the energy of interaction between P22 phage and membrane surfaces using the XDLVO approach The XDLVO theory predicts the energy of interaction between particles and a surface by taking into consideration Lifshitz-van der Waals (LW), electrostatic double layer (EL) and Lewis 55 acid-base (AB) forces [51, 52]. The total energy of interaction between a particle and a plane surface can be written as [52]: (2.5) U XDLVO  U LW  U EL  U AB XDLVO where U EL U is the total energy of interaction, U is the electrostatic interaction energy and U AB LW is the van der Waals interaction energy, is the Lewis acid-base interaction energy. Each of these terms can be expressed as a function of the separation distance ( ) using the following equations [52]: 2 LW d   4   LW   LW   LW   LW  y 0 r p U    p  s     d  d  EL d     r 2  ln 1  e U r 0 p p s  d  1 e        2   2  ln1  e  2d  s     p    (2.6)                     s   p          s   p         exp y0  d  U AB d   4r p                s  p   s  p    (2.7) (2.8) _ LW where   ,   and   are the surface tension parameters of immersion liquid (the + and  superscripts correspond to the electron acceptor and electron donor components of the surface _ LW  tension, respectively),  p ,  p and  p are the surface tension parameters of the particle, _ LW   s ,  s and  s are the surface tension parameters of the planar surface, r p is the particle radius, and  p and  s are the zeta potentials of the particle and the surface. The minimum equilibrium cut-off distance, y 0 , was assigned a value of 0.16 nm [53]. For other symbols, 56  r 0 is the dielectric permittivity of water,  is the inverse of the Debye length and  is the characteristic decay length of Lewis acid-base interactions in water (0.6 nm) [53]. The surface tension parameters of the P22 phage and membrane surfaces were determined using the extended Young equation (2.9) after measuring the contact angle of three probe liquids with known surface tension parameters. (2.9) TOT  2  LW  LW           (1  cos )   s s  s       AB  2    (2.10)  TOT   AB   LW (2.11) In these equations,  is the contact angle for a given probe liquid, and the subscripts and  correspond to the solid surface and the liquid probe, respectively.   2.2.13 Effect of polyelectrolytes and CS on qPCR analysis 8 A P22 solution (~ 3·10 PFU/mL) was prepared by diluting 1 mL of P22 stock with deionized (DI) water. One mL of 0.12 mg/mL solutions of HE, PAA, poly(styrene sulfonate) , CHI and PDADMAC, and 1 mL of a 0.24 mg/mL calf serum solution were seeded with 0.1 mL of the P22 solution. The pH of each resulting solution was adjusted to 6.3 (similar to the feed pH during filtration). The final concentration of polyelectrolyte and calf serum in each solution was 0.11 and 0.22 mg/L respectively, which is 100-fold higher than the concentration we would 57 expect if we would backflush our membrane with 100 ml of solution. The P22 concentration in these samples was determined using the same methodology as for the filtration samples. 2.3 2.3.1 Results and Discussion PEM selection As described in Chapter 1 various polyelectrolytes have been used to prepare anti-adhesive coatings. Based on these studies HA/CHI, HA/PAH, HE/CHI and HE/PAH films were deposited on UF membranes. (PAA/PAH films are not highly permeable.) Contact angles of water with the resulting surfaces and water permeability were measured. Based on a limited set of data it appeared that HE based films were more hydrophilic than their HA counterparts. Additionally we looked at the effect of polyelectrolytes on qPCR analysis. As Fig. 2.4 shows, polycations out of 3 significantly inhibited DNA extraction or qPCR while most polyanions had no effect on qPCR results. Although CHI partially inhibited qPCR, PAH completely annihilated any fluorescence signal and as a consequence P22 could not be detected in samples containing PAH. As a result, CHI was considered a better candidate than PAH and based partly on the results of these inhibition tests and partly on the measured values of water contact angles and water permeabilities of candidate PEMs, we selected (HE/CHI)4.5 as one suitable PEM film. Several polyelectrolytes such as PDADMAC or PAA, not considered in these studies, were more compatible than CHI or HE with qPCR and should be considered in future work 58 Log P22 concentration as determined by qPCR 7 6 5 4 3 2 1 0 potential inhibitors Figure 2.4: Effect of various polyelectrolytes and calf serum on the P22 concentration determined by qPCR. Error bars indicate the standard deviation interval. n=3. 2.3.2 Properties of CS-blocked and PEM-coated membranes and P22 phage 2.3.2.1 Membrane permeability and fouling mechanisms The DI water permeabilities of PES, CS-blocked PES, and PEM-coated PES membranes 2 after compaction were 280  20, 90  20, and 120  30 L/(m ·h·bar), respectively. Thus, the two modification methods yielded membranes of similar permeabilities. We applied blocking laws to P22 dead-end filtration data to interpret how feed components interacted with CS-blocked and 59 PEM-coated membranes. As Fig. 2.5 shows, for both membranes each of the four mechanisms could fit at least a portion of the dataset. Concurrent fits to different mechanisms indicate either a combination of mechanisms or that the data are insufficient to differentiate between mechanisms. Clearly, however, a cake filtration law provides a high quality fit to plots of flux versus time after filtering 5 mL of virus suspension through PEM-coated membranes, but only after filtering 32 mL through CS-blocked membranes. (Filtration of one mL corresponds to one 2 P22 phage, quantified as DNA copies, deposited per 1 μm of membrane). The larger volume required to achieve cake filtration with CS-blocked membranes suggests that P22 (or other components not removed from the growth medium by centrifugation) can partially or fully enter pores in the CS layer. For a description of different blocking mechanisms please refer to the study by Wang et al. [50]. 2.3.2.2 Surface properties of membranes and P22 phage Several studies have shown that blocking the membrane with proteins improves virus recovery [3, 10, 28]. While two studies reported that blocking a membrane with proteins had no [4] or a negative [12] effect on virus recovery, most studies used CS or other proteinaceous solutions to block membranes for microorganism concentration by crossflow filtration [2, 3, 5, 7, 10, 11, 13]. . 60 a) b) 1.4 60 * 1.2 y = 0.0172x + 0.3635 r2 = 0.99965 40 30 * 20 * 0.8 y = 0.003x + 0.7033 R² = 0.5762 0.6 0.4 PEM-coated membrane CS-blocked membrane t/V=f(V) linearisation for V>5ml (PEM) t/V = f(V) linearisation for V>30mL (CS) cake filtration 10 0 complete blocking intermediate blocking standard blocking 1.0 t/V (min/mL) permeate volume (mL) 50 0.2 CS PEM 0.0 0 20 40 V (mL) 60 Figure 2.5: Blocking law analysis for fouling of CS-blocked and PEM-coated membranes during filtration of DI water spiked with 2 P22 stock. a) Distributions and contributions of the blocking mechanisms in terms of permeate volume. * indicates that the r value 2 corresponding to fitting that blocking mechanism with the experimental data was > 0.99. When no * is present, r was > 0.999. b) Inverse cumulative flow rate (t/V) as a function of permeate volume V for CS-blocked and PEM-coated membranes. 61 Some of these studies suggest that treating the membrane with beef extract or CS solutions minimizes viral adsorption to the membrane [10, 13]; however, to our knowledge all evidence for such an effect is indirect and based on higher values for virus recovery. Previous studies did not consider the specific interactions between the virus and the membrane. To quantify the anti-adhesiveness of the CS layer, we measured the surface energy (Table 2.2) and charge of the CS-blocked membrane. Based on literature values of the  -potential and isoelectric point, at least 2 out of the 4 viruses were negatively charged [55, 56] in studies showing that CS or beef extract increased recovery [10, 13, 54]. (Isoelectric points for the other 2 viruses are not known.) Therefore, we expected that CS renders the membrane surface more hydrophilic and negatively charged to make it more anti-adhesive; however, CS-blocked membranes were slightly positively charged at pH 6 (  = 3  2 mV) and not more hydrophilic (  w = 66  13°) than the polyethersulfone support (  w = 67  3°). In fact, the CS-blocked membranes were hydrophobic (see Table 2.2) according to van Oss and Giese’s definition of hydrophobicity (a negative free energy of interfacial interaction when immersed in water; see Chapter 1) [57]. Although the IEP of BSA, the main component of CS, is 4.7 so the protein would have a slight negative charge at pH 6, the CS also includes components other than BSA that might preferentially deposit and be responsible for the slightly positive charge of the CSblocked surface. Thus, although CS can prevent virus attachment to the UF support membrane by occupying adsorption sites, negatively charged viruses might still adsorb onto CS surface during filtration. 62 Table 2.2 Measured contact angles, calculated surface energy parameters and free energy of interfacial interaction when immersed in water for P22 phage, CS-blocked membranes and PEM-coated membranes. 2 Giwi Surface energy parameters (mJ/m ) Probe liquid  LW    AB  TOT Ultrapure water 21.8 25.5 25.5 51.0 34.0 3.9 57.4 30.0 64.0 Diiodomethane 50.8 0.0 0.0 0.0 2 (mJ/m ) 72.8 Glycerol Contact angle (º) 50.8 Material Diiodo- H2O Glycerol methane P22 44 3 57 27 71 25 49 ± 8 75 ± 6 30 ± 2 CS-blocked membrane 41 0.004 17 0.5 42 -24 66 ± 13 64 ± 2 37 ± 3 PEM-coated membrane 42 0.07 53 4 46 36 36 ± 3 55 ± 4 34 ± 5 63 This could suggest that CS blocking improves recovery by limiting virus penetration into the membrane but not by minimizing virus adhesion. Facile elution of viruses attached to the CS might also enhance recovery. In contrast, the PEM-coated membranes were negatively charged at pH 6 (  = -7  3 mV) and considerably more hydrophilic (  w = 36  3°) than the CS-blocked membranes. Given that P22 phages were negatively charged at pH 6 (  = -17  1 mV) and hydrophilic (  w = 49  8°), we expect the PEM to resist P22 adsorption. As a precedent in this area, Hill et al. [3] and Polaczyk et al. [6] evaluated the efficiency of a 15-min blocking of 15-20 kDa UF membrane with a 600 Da NaPP solution. Although surface charges were not measured, they hypothesized that deposition of the polyanion NaPP increased electrostatic repulsion between the membrane and microorganisms. NaPP “blocking” was faster than overnight CSblocking and resulted in similar recovery for MS2 bacteriophage [3, 6]. To further quantify the propensity of P22 to adhere to the CS-blocked and PEM-blocked membranes, we calculated the energy of phage-membrane interactions. 2.3.2.3 Virus-membrane interaction energies The XDLVO theory predicted secondary minima in the energy of the virus-membrane interaction at separations of 4.3 nm and 10.9 nm for the CS-blocked and PEM-coated membranes, respectively (Fig. 2.6). Due to attractive van der Waals and electrostatic interactions between CS-blocked membranes and P22, the secondary minimum (-2.6 kT) could be enough for some P22 to reversibly attach to the membrane surface despite not being able to overcome the repulsive barrier (500 kT) [58]. The depth (-0.6 kT) of the secondary minimum in the PEM-P22 interaction energy was less than the average thermal energy of particles, indicating 64 that attachment of P22 to this membrane was not efficient. This XDLVO analysis only takes into account macroscopic phenomena, and adhesion of P22 to either surface could also occur through microscopic attraction to discreet electron acceptor sites on the membrane surfaces [53] as well as through non-XDLVO interactions. 3 interaction energy, kT units a) b) 3 2 2 1 1 0 0 0 10 van der Waals Lewis acid-base electrostatic total interaction energy 0 20 -1 20 -1 -2 10 -2 -3 -3 separation distance, nm separation distance, nm Figure 2.6: XDLVO energy profiles for the interaction of P22 with a) CS-blocked membranes and b) PEM-coated membranes at pH = 6 and in 10 mM KCl. 2.3.3 Virus recovery with PEM-coated and CS-blocked membranes 2.3.3.1 Pre-elution recovery Figure 2.7 shows P22 recoveries in the retentate as a function of the J cf / J p ratio. The Jcf / J p ratio is important as it influences the transport of viruses to and, possibly, across the 65 membrane [59]. Generally, if permeate flow increases, increased concentration polarization leads to both more particle adhesion to the membrane and more particle passage through the membrane. In contrast, increasing the crossflow velocity decreases concentration polarization and facilitates particle removal from the membrane surface through shear-induced backtransport[15]; however, it has also been shown that, in conditions typical of crossflow ultrafiltration, the minimum Pre-elution recovery with CS-blocked membranes ranged from 22% to 51%. These values are comparable to results of a previous study with CS-blocked UF membranes where pre-elution recoveries were 38  22% for T1 phage and 45  55% for PP7 phage [5]; we should note, however, that this prior study employed surface water that could foul the membrane significantly [9]. When concentrating bacteriophage MS2 from tap water, Hill et al. [3] reported pre-elution recoveries of 84  13%. This high recovery probably stemmed from the relatively simple composition of the water samples combined with the addition of 0.1% NaPP, a negatively charged chemical dispersant thought to enhance charge repulsion between the membrane and viruses by altering the viruses’  -potential [6]. P22 pre-elution recovery with PEM-coated membranes ranged from 32 to 85%. Over the entire range of filtration conditions (Fig. 2.7), PEM-coated membranes statistically outperformed CS-blocked membranes in terms of P22 pre-elution recovery, but the improvement was most pronounced at higher Jcf / J p ratios. We attribute the observed higher pre-elution to the PEM’s anti-adhesiveness stemming from its negative charge [30] and hydrophilicity [29]. 66 recovery postelution, % 100 100 90 recovery pre-elution , % 80 70 90 0 80 CS 60 PEM 50 40 30 20 P22 pre-elution with CS-blocked membrane P22 pre-elution with PEM-coated membrane 10 0 0.0 0.2 0.4 0.6 0.8 1.0 crossflow to permeate flux ratio Jcf/Jp 1.2 104 Figure 2.7: Pre-elution and post-elution (see inset) recovery of P22 from DI water. Because there was no significant dependence of post-elution recovery on the value of Jcf / J p , only the average recovery and the 90% confidence interval are reported. Number of experiments: n = 26 for CS-blocked membranes and n = 22 for PEM-coated membranes. 2.3.3.2 Post-elution recovery and potential of PEMs as sacrificial coatings Post-elution recovery of P22 did not differ significantly between CS-blocked (99  11%) and PEM-coated membranes (96  9%). These values for post-elution recovery were within the 67 range typically reported for crossflow filtration of bacteriophages [2, 5, 6, 11-13, 28]. For example, Hill et al. [2] recovered 86  13% of the ΦX174 phage and 120  22% of MS2 phage from a 100 L tap sample containing 0.01% NaPP. The high post-elution recovery with both CSblocked and PEM-coated membranes may reflect the simplicity of the water matrix or weak adhesion of P22 to surfaces. We expect that with more adhesive viruses, recovery should decrease, and the competitive advantage of the PEM as a more anti-adhesive surface will increase. When 10-L surface water samples were concentrated by crossflow filtration followed by elution, Albinana-Gimenez et al. [7] observed post-elution recoveries of only 18.7% for polyomavirus, 5.06% for adenovirus and less than 0.95% for norovirus. Anti-adhesive properties of PEM-coated membranes, evidenced by high pre-elution recoveries of P22, might help to improve the recovery of such “sticky” and difficult to concentrate human viruses. Treating the PEM film as a sacrificial layer and removing it from the support using a backflush could also increase post-elution recovery. Such removal will not affect the supporting UF membrane and should help to recover surface-associated viruses. After the backflush, a new PEM layer can be deposited at the surface of the same support [61]. To implement such a procedure, however, electrolytes of the dissolved PEM should minimally interfere with qPCR. Tests with select polyelectrolytes indicate that although some polyanions and most polycations interfere with qPCR analysis; there are polyanions and polycations that, at the concentration expected in backflush samples, do not inhibit qPCR or DNA extraction (see Fig. 2.4). Indeed adding PSS, HA, PAA or PDADMAC to P22 samples did not affect the count of P22 by qPCR when compared to the control sample where P22 was suspended in DI water. 68 2.3.3.3 Reproducibility Blocking with CS is inherently poorly reproducible, so we expected the PEM-coated membranes to show more reproducible recoveries than CS-blocked membranes. We performed 15 filtrations under conditions that should lead to the highest recoveries (“low J p ; high J cf ” domain) with CS-blocked membranes, and 14 filtrations under the same conditions with PEMcoated membranes. Figure 2.8 illustrates the distribution of pre-elution and post-elution 3 recoveries under these conditions for both membrane types. The interquartile range (IQR, also called midspread) for pre- and post-elution recoveries were comparable for both types of membranes. IQRs for pre-elution recovery distributions are 15% and 16% for CS-blocked membranes and PEM-blocked membranes respectively, whereas IQRs for post-elution recovery distributions were lower, 10% and 9%, respectively for CS-blocked and PEM-coated membranes. We conclude that there was no significant difference in recovery reproducibility between the two types of membranes. The interquartile range is the difference between the upper and lower quartiles of the cumulative distribution curve. 69 relative frequency of occurrence a) calf serum 0.5 PEM 0.4 0.3 0.2 0.1 0.0 pre-elution recovery (%) relative frequency of occurrence b) 0.5 calf serum PEM 0.4 0.3 0.2 0.1 0.0 post-elution recovery (%) Figure 2.8: Relative frequency of occurrence of P22 (a) pre-elution and (b) post-elution recoveries from DI water under the operational conditions optimized to maximize P22 recovery ( J cf / J p > 6,400). Number of experiments: n= 15 for CS-blocked membranes and n=14 for PEM-coated membranes. 70 2.3.4 Virus log removal LRV values varied in the 3.9  1.2 range for CS-blocked membranes and in the 4.1  1.1 range for PEM-coated membranes (Fig. 2.9). There was no significant difference between the two types of membranes and no significant influence of Jcf / J p on virus removal. 6 CS-blocked membrane PEM-coated membrane log removal 5 4 3 2 1 0 0.0 0.2 0.4 0.6 crossflow to permeate flux ratio Jcf/Jp 0.8 1.0 104 Figure 2.9: P22 removal from DI water by CS-blocked and PEM-coated membrane at various J cf / J p . 71 2.3.5 Effect of operational conditions on virus concentration 2.3.5.1 Operational conditions and flux Figure 2.3 illustrates the range of operational conditions employed in this work. The J p values are the permeate fluxes averaged over the first minute of filtration. For experiments conducted at lower transmembrane pressures (Fig. 2.3; “low J p ” domain), plotted J p values also represent the average J p as minimal or no fouling occurred in these tests. In experiments run at higher transmembrane pressures (Fig. 2.3; two “high J p ” domains) fouling did occur, especially for PEM-coated membranes (Fig. 2.10), so average permeate fluxes were lower than the plotted initial values of J p (Fig. 2.11 shows average rather than initial fluxes). For comparison, Fig. 2.3 and Fig. 2.11 also show J p values from earlier studies where crossflow membrane filtration was used to recover viruses and where values of both J p and J cf were available (see Appendix A). Compared to earlier studies [2, 3, 5, 6, 11, 13], we evaluated a relatively large range of operational conditions by varying both J p (2.0 to 8.6 (L/min·m2)) and J cf (6,800 to 26,800 2 (L/min·m )). This allowed us to assess the virus concentration performance of CS-blocked and PEM-coated membranes under conditions optimal for either highest virus recovery or fastest sample concentration (Fig. 2.7). The highest recovery conditions belong to the “low J p ; high 72 J cf ”domain, while the fastest concentration conditions correspond to the “high J p ; high J cf ” domain (Fig. 2.3 and 2.11). 9.E+12 CS-blocked membrane 8.E+12 fouling resistance Rf × 1012, m-1 PEM-coated membrane 7.E+12 6.E+12 5.E+12 4.E+12 3.E+12 2.E+12 1.E+12 0.E+00 0 0.5 1 1.5 2 crossflow to permeate flux ratio Jcf/Jp × 104 Figure 2.10: Observed fouling resistance (averaged over the duration of experiment) for CSblocked and PEM-coated membranes during the concentration of 1L of DI water seeded with P22 to 250 mL at various crossflow to permeate flow ratios. 73 average permeate fllux Jp, L/(min·m2) this study: CS-blocked membrane this study: PEM-coated membrane earlier studies 6 low Jp high Jp low Jcf 5 high Jcf 4 3 2 (5) (2, 11) 1 low Jp high Jcf (3) 0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 crossflow flux Jcf ·104 , L/(min·m2) Filtration conditions: average permeate flux and crossflow flux, used for P22 recovery with CS-blocked membrane and PEM-coated membranes. n=27 for CS, n=22 for PEM. In contrast to Fig. 2.3, this graph presents values of permeate flux averaged over the duration of filtration experiment rather than over the first minute. Under “high J p ; high J cf ” conditions where J cf was in the 20,400  3,600 2 L/(min·m ) range, fouling decreased the concentration rate; for the CS-blocked membrane, the 2 initial J p (averaged over the first minute of filtration) was 5.8  0.3 L/(min·m ), whereas the 2 J p averaged over the length of the filtration was 4.9  0.3 L/(min·m ). Similarly, for PEM- coated membranes, under the fastest concentration conditions the initial J p was 7.2  1.4 74 2 2 L/(min·m ) and the average J p was 3.9  0.6 L/(min·m ). Thus the concentration rates were similar for CS-blocked and PEM-blocked membranes, but the PEM may show somewhat more fouling due to a higher initial flux. With polysulfone membranes of similar MWCO (30 kDa) blocked with bovine serum, 2 Hill et al. [2, 3, 11] obtained permeate flow rates between 0.4 and 0.6 L/(min·m ) with tap water samples at a transmembrane pressure of ~ 13 psi. Morales-Morales et al.[5] reported a J p of 2 1.5 L/(min·m ) at a transmembrane pressure of 12 psi for surface and tap water samples with a 50 kDa polyacrylonitrile membrane also blocked with CS. By increasing both the transmembrane pressure and cross-flow rate we achieve significantly higher (~ 3-fold) rates of concentration. The comparison is not direct, however, because of different feed water matrices 2 that were spiked by viruses and different concentration ratios: 4.9 mL of feed per cm of 2 membrane surface for surface/tap water in the study by Morales-Morales et al. [5], 5.5 mL/cm 2 for tap water in the study by Hill et al. [2] versus 18.3 mL/cm for DI water in this study. 2.3.5.2 Effect of J cf / J pon virus recovery P22 pre-elution recovery by CS-blocked membranes did not significantly increase with an increase in Jcf / J p (Fig. 2.7). Others looked briefly at the dependence of virus recovery on hydraulic conditions [8]. Belfort et al. noticed no significant difference in poliovirus recovery by filtration through a non-blocked cellulose acetate membrane when tripling the crossflow rate; the 75 observation, however, was based on only one filtration performed at a lower crossflow rate [8]. More recently, Polaczyk et al. [6] observed no statistical difference in recoveries of MS2 phage and echovirus 1 when operating a membrane blocked with NaPP at two different permeate flow rates; however, in their study, the permeate flow rate and crossflow rate were linked, and as a consequence the Jcf / J p ratio changed only from 5,800 to 6,500. In contrast, the pre-elution recovery of P22 with PEM-coated membranes significantly increased with an increase in Jcf / J p . The recovery is 55 ± 15% for the fastest concentration conditions (“high J p ; high J cf ” domain) and 71  11% for the highest recovery conditions (“low J p ; high J cf ” domain). This effect of Jcf / J p on virus recovery is expected. At higher J p , the force driving the virus toward the membrane is higher. In addition at higher Jcf / J p there is more fouling as seen in Fig. 2.10. Fouling can conceal, at least partially, the membrane surface and its anti-adhesive properties which decreased pre-elution recovery as seen in Fig 2.12. Such high recoveries may render the elution step unnecessary. Indeed this level of recovery is comparable to what might be obtained by other virus concentration methods that involve elution. Eliminating the need for elution has several advantages. Time is gained and the volume of the concentrated sample is smaller. In addition, all viruses are recovered pre-elution. These viruses interacted less with the membrane surface than viruses recovered by elution and as a consequence their integrity is better maintained [62]. Post-elution recovery for both types of membrane is not affected by Jcf / J p . 76 P22 pre-elution with CS-blocked membrane 100 P22 pre-elution with PEM-coated membrane 90 recovery pre-elution, % 80 70 60 y = -17.432x + 78.831 R² = 0.4028 50 40 30 20 y = -20.37x + 37.902 R² = 0.1821 10 0 0.0 0.5 1.0 1.5 2.0 2.5 fouling resistance over membrane resistance ratio Figure 2.12: Pre-elution recovery of P22 from DI water as a function of the fouling layer resistance to membrane resistance ratio. 2.3.6 Potential for practical applications Preparation of membranes with a large surface area is critical for successfully scaling up the proposed sample concentration approach [63, 64]. PEMs have already been deposited on flat sheet membranes [65], tubular membranes [66], and hollow fibers [67]. The proposed approach could be scaled-up by depositing a PEM using alternating circulation of cationic and anionic polyelectrolyte solutions through a standard hollow fiber cartridge [2, 3, 5, 6, 11]. Elution, backflushing, and coating removal and regeneration could occur in situ by flushing the cartridge with appropriate solutions. Other components of a scaled-up portable system would include a back77 pressure valve for generating and controlling the transmembrane pressure and a bypass valve for regulating the crossflow rate. When appropriate, the proposed PEM-based approach can be combined with the addition of chemical dispersant, such as NaPP, as described in several earlier studies [2, 3, 5, 6, 11] to further reduce virus attachment to the membrane surface and improve recovery. Acknowledgements This work was supported by the NSF Partnerships for International Education and Research grant OISE-0530174, a U.S. EPA Science to Achieve Results grant R833010, and a MSU Foundation Strategic Partnership grant. The authors would also like to acknowledge Mr. Hang Shi for his help with  -potential measurements and Mr. Tyler Rafferty for his help with filtration tests. 78 REFERENCES 79 REFERENCES 1. Gibson, K.E. and K.J. Schwab, Detection of bacterial indicators and human and bovine enteric viruses in surface water and groundwater sources potentially impacted by animal and human wastes in Lower Yakima Valley, Washington. Applied And Environmental Microbiology, 2011. 77(1): p. 355-362. 2. Hill, V.R., et al., Multistate evaluation of an ultrafiltration-based procedure for simultaneous recovery of enteric microbes in 100-liter tap water samples. Applied and Environmental Microbiology, 2007. 73(19): p. 6327-6327. 3. 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Tieke, Use of polyelectrolyte layer-by-layer assemblies as nanofiltration and reverse osmosis membranes. Langmuir, 2003. 19: p. 2550-2553. 66. Dotzauer, D.M., et al., Catalytic membranes prepared using layer-by-layer adsorption of polyelectrolyte/metal nanoparticle films in porous supports. Nano Lett., 2006. 6(10): p. 2268-2272. 67. Lu, O.Y., et al., Catalytic hollow fiber membranes prepared using layer-by-layer adsorption of polyelectrolytes and metal nanoparticles. Catalysis Today, 2010. 156(3-4): p. 100-106. 85 Chapter 3. Effect of flow conditions and water composition on the removal and recovery of infective bacteriophage by crossflow filtration with CS-blocked membranes 3.1 Introduction As mentioned in Chapter 1, efficient virus detection in drinking and recreational water is vital for preventing disease outbreaks and this requires an efficient concentration method. The ideal concentration/quantification method should be able to differentiate infectious viruses from non-infectious ones [1] as only the former are a concern in terms of public health, and quantification of viral nucleic acid is not necessarily a good indicators of the presence of infectious virus [2]. It is thus important that the concentration method used does not affect virus infectivity. Crossflow filtration is emerging as a concentration method for the collection, concentration and quantification of viruses in large volumes of water [3-9], but has the potential to disrupt virus infectivity. Indeed, a decrease in infective virus titer in the retentate of crossflow filtration units has been observed in several studies [9-12] but others did not observe such trends [13]. In two studies, virus aggregation, which affects virus infectivity assays, was initially considered a culprit but eventually ruled out as the reason for the observed loss of infectivity [11, 12]. In some studies increasing ionic strength was found to correlate with virus loss of infectivity in tap water [11, 12], while others, using more complex water samples did not observe any correlation between sample conductivity (an approximate measure of ionic strength) and loss of infectivity 86 [9]. Virus morphology, the presence of hydrophobic surfaces in the concentration device, and the pumping-induced shear stress, have also been mentioned as possible factors contributing to the loss of viral infectivity during crossflow filtration [10, 11]. Another factor that might influence infectivity assays, and thus recovery of infective viruses by crossflow filtration, is the presence of natural organic matter or cations which have been shown to affect virus aggregation [14]. Finally, changes in filtration conditions such as crossflow rate and permeate flow rate translate into changes in the forces applied to the viruses and, therefore, might affect virus infectivity, virus aggregation, or both. In Chapter 2, we showed that it was possible to increase the initial permeate flux through CS-blocked membranes by up to 4 times (over the values reported in the literature) without affecting P22 recovery as determined by qPCR. In this Chapter we will look at the effect of filtration conditions and water matrix on the removal and the pre- and post-elution recoveries of infective bacteriophage P22 by CS-blocked membranes. In Chapter 2 we also showed that increasing Jcf / J p increased P22 pre-elution recovery by PEM-coated membranes, whereas for CS-blocked membrane, increasing Jcf / J p had no effect on P22 recovery or removal. This was contrary to our expectation. Indeed decreasing J p should decrease concentration polarization and lead to less particle adhesion to the membrane [15]. In addition, increasing the crossflow rate can decrease concentration polarization [15] and has been shown to decrease passage of virus through membrane [15, 16]; however, this effect of crossflow might be minimal for viruses as their size corresponds to a minimum in Brownian and shear-induced particle back-transport from the membrane surface [17]. It is possible that the stable P22 removal at increasing Jcf / J p is a result of two mutually counterbalancing effects: 1) a partial loss of integrity of the 87 CS layer at high crossflow and 2) a decrease in the net flux of viruses towards the membrane surface at higher Jcf / J p . To determine which scenario is operative we assessed the integrity of the CS layer under various filtration conditions. 3.2 3.2.1 Material and Methods Reagents Lysozyme (from chicken egg white), ethylenediaminetetraacetic acid (EDTA), calf serum, sodium polyphosphate (NaPP), and dextran standard (25 kDa) were purchased from Sigma-Aldrich. Tween 80 was purchased from Fisher and tryptic soy broth from Becton, Dickinson. 3.2.2 Water samples Deionized (DI) water was supplied by a commercial ultrapure water system equipped with a terminal 0.2 µm capsule microfilter (PolyCap, Whatman Plc., Sanford, ME). Ten liters surface water samples were collected from Lake Lansing (Lansing, MI) as grab samples in May and September 2009 and in February 2010, and filtered through a 0.45 μm membrane on the day of collection. Samples were kept at 4°C until used. Surface water samples were used as early as the day following their collection and within 4 months of their collection. Before use, the surface water container was agitated to resuspend any settled particles. 88 The total organic carbon (TOC) content of filtered Lake Lansing samples was determined using a Total Organic Carbon analyzer (1010, O I Analytical, USA). Each sample was analyzed in triplicate. Calibration standards and blanks were run for each set of measurements. 3.2.3 Bacteriophage Bacteriophages were cultured as described in Chapter 2, section 2.2.2. 3.2.4 Membrane preparation, crossflow concentration apparatus and concentration procedure The CS-blocked membranes were prepared as described in Chapter 2 section 2.2.5. Membranes were first compacted for 90 min at 40 psi with DI water. The filtration apparatus and concentration procedure are described in Chapter 2 sections 2.2.4 and 2.2.7. Elution was performed with non-spiked surface water amended with 0.01% Tween 80 and 0.01% NaPP. The filtration conditions used in this study are shown in Fig. 3.1. 89 initial permeate fllux Jp, L/(min·m2) 10 DI water 9 surface water earlier studies high Jp high Jp 8 high Jcf low Jcf fastest concentration conditions 7 6 5 4 3 (d) 2 (b, c) (a) 1 0 0.0 0.5 low Jp high Jcf low Jcf 1.0 low Jp highest recovery conditions 1.5 2.0 2.5 3.0 crossflow flux Jcf ·104, L/(min·m2) Filtration conditions in experiments on infective P22 concentration and recovery from DI water and surface water using CS-blocked membranes. Number of tests: n=23 for DI water, n=18 for surface water. Earlier studies: a: Hill et al. [18], b: Hill et al. [19], c: Hill et al. [5], d: Morales-Morales et al. [20]. 3.2.5 Sample analysis The P22 concentration in each sample was determined by plaque assay using the double agar layer procedure within 24 h of the filtration experiment. Ten-fold serial dilutions of each sample were prepared. The bacterial host, S. typhimurium, was grown to log phase in tryptic soy broth and added to a 1% soft agar solution, which was inoculated with 1 mL dilution aliquots and poured on top of an agar plate. Plates were inoculated overnight at 37ºC. Plaques (clear zone of 90 infected bacterial cells) were then counted and this count was used in combination with the dilution factor to determine P22 concentration in plaque forming unit (PFU)/mL in the sample. Plaque assays were run in triplicate for each dilution of each sample. Samples from 3 filtrations corresponding to 3 different filtration conditions (low J p - low Jcf ; low J p - high Jcf and high J p - low Jcf ) were also stored at -80ºC in presence of glycerol (10%) to be later analyzed by qPCR. The procedure for qPCR analysis is described in Chapter 2 section 2.2.8. P22 log removal (LRV) percentage of pre-elution recovery ( r pre ), and percentage of post-elution recovery ( r post ) were calculated using the equations (1), (2) and (3) from Chapter 2. Data were compared with the Student t-test. P < 0.05 was considered to show statistical significance. A Bonferroni correction was performed when multiple comparison were done. 3.2.6 Calf serum layer stability test The stability of the calf serum layer during filtration was tested in the filtration unit described in section 2.2.4. CS-blocked membranes were prepared and compacted as described in section 2.2.5. The membranes were then used to filter a 20 mg/L aqueous solution of 25 kDa dextran using a transmembrane pressure of approximately 40 psi. The crossflow rates was 2 2 increased from 1,500 L/(min m ) to 22,000 L/(min m ), which corresponds to Jcf / J p ratios from 900 to 8,900. Each crossflow rate was maintained for 5 min. and permeate samples were collected before and after the crossflow rate was increased. Retentate samples were also collected several times during the test to monitor dextran concentration. Concentrations of 91 dextran in the retentate and in the permeate were determined using the total organic carbon analyzer. Each sample was analyzed in triplicate. Calibration standards and blanks were run for each set of measurements. Rejection ( R ) of dextran at a given time was determined using equation (3.1): (3.1)  C p (t )    100% R(t )  1   C r (t )    where C p and C r are, respectively, dextran concentrations in the permeate and retentate at that given time. C r at any given time was determined using linear interpolation of retentate concentration values measured at several times during each experiment The stability of the calf serum layer during elution was also tested. The test was similar to the one described above except that pressure was only applied to collect samples. CS layer stability during filtration was tested in triplicate, only one test was performed to determine the CS layer stability during elution. 3.3 3.3.1 Results and Discussion Effect of filtration conditions on the recovery and removal of infective P22 A preliminary test was performed to determine if infective viruses were lost due to the adhesion to the components of the filtration unit, other than the membrane or due to loss of 6 infectivity. We showed that circulating 1 L of DI water spiked with P22 (1.3·10 PFU/mL) for 3 h in the filtration unit, with no membrane in place and no pressure applied, did not affect P22 92 counts in the infectivity assay indicating that there was no loss of infectivity due to contact with components of the concentration unit as some have observed [11] or that this loss of infectivity was coincidentally offset by virus disaggregation. Figure 3.2 shows the recovery and removal of infective P22 from DI water and surface water by CS-coated membrane under various filtration conditions. At the pre-elution level, there was no effect of the filtration conditions on the recovery of infective P22 from either DI water or surface water. At the post-elution level, although the recovery of infective P22 from DI water in the least favorable conditions (high J p , low Jcf ) seemed lower on average than under other conditions, a t-test analysis showed that the difference was not significant. In the case of surface water, again no effect of filtration conditions on infective P22 recovery is observed. Recovery of infective P22 from DI water or surface water was not affected by filtration conditions. As mentioned in Chapter 2, a similar trend has been observed by others [21, 22], however the scope of their studies was limited in terms of the number of filtrations performed [21] or range of Jcf / J p ratios explored [21]. The trend is counterintuitive as it was expected that increasing Jcf / J p would decrease concentration polarization and fouling (Fig. 3.3), which should increase pre-elution recovery as virions have a lesser chance to be trapped near the membrane. 93 pre-elution recovery, % a) 100 DI water surface water 80 60 40 20 0 filtration conditions b) post-elution recovery, % 160 DI water surface water * 120 80 40 0 filtration conditions 94 c) DI water 10 * 8 log removal surface water 6 4 2 0 filtration conditions 95 DI water surface water Jp final/ Jp initial 1.0 0.8 0.6 0.4 0.2 0.0 filtration conditions For microfiltration (MF) membranes it was shown that increasing the Jcf / J p ratio leads to an increase in the removal of MS2 and Q phages [16] and that higher J p and stirring increase removal of poliovirus [23]. In the present study, however, changing filtration conditions had no effect on P22 removal from DI water or surface water. In the case of surface water, the formation of a thicker fouling layer preventing virus passage at lower Jcf / J p might have opposed the effect of increased concentration polarization and helped maintaining removal levels as high as at higher J cf / J p . Others have observed 96 3.3.2 qPCR vs. plaque assay As reported in Chapter 2, no significant effect of Jcf / J p on P22 pre and post-elution recoveries or removal (as determined by qPCR) by CS-blocked membrane was observed. In this Chapter we report the absence of such trends observed for infective P22 as well. In addition, the average removal and pre-elution recoveries of infective P22 observed in this study were not significantly different than the average removal and recoveries based on qPCR analysis as reported in Chapter 2 for CS-blocked-membranes; however, post-elution recovery of infective virus was significantly lower than recovery measured by qPCR (74 ± 31% and 99 ± 11% respectively). Data from the three filtrations for which samples were analyzed by both qPCR and plaque assay, confirm this observation (Fig. 3.4). Similar elution and removal recovery were observed, except at the post-elution level where a significant difference was detected at high J p , low Jcf . If this observation is confirmed to be statistically significant, it would indicate that, under high J p , low Jcf , viruses recovered during elution have either lost infectivity (for example due to interaction with the membrane during the filtration step or because of the additive -Tween 80 and NaPP- used for elution) or have aggregated. Since NaPP is often used as a dispersant when concentrating various pathogens including viruses [20], the decrease in viral count observed by plaque assay was most probably due to the loss of P22 infectivity rather than 97 aggregation of the phage. This could be confirmed by measuring the particle size in the retentate and eluate; however, particle size analysis requires higher virus titer than the one that we had in our filtrations and concentrating those samples was not an option as any concentration could affect the aggregation state of the virus suspension. Another difference between results obtained by qPCR and plaque assay is the reproducibility of virus recovery and removal data. Standard deviations of pre-elution recoveries, post-elution recoveries and LRV values obtained by qPCR (8%, 11% and 1.2 respectively) were lower than standard deviations obtained in plaque assays (17%, 31% and 1.4 LRV respectively). This might be explained by a greater standard deviation associated with the plaque assay method compared to the qPCR method (as seen in Fig. 3.4), which is due, in part, to the fact that plaque assay was performed on 3 different grab samples while qPCR was performed in triplicate on one grab sample. 98 100 pre-elution recovery, % a) plaque assay 80 60 40 20 0 high Jp, low Jcf low Jp, low Jcf low Jp, high Jcf filtration conditions post-elution recovery, % b) 100 plaque assay 80 60 40 20 0 high Jp, low Jcf low Jp, low Jcf low Jp, high Jcf filtration conditions Effect of analysis method on P22 a) pre-elution recovery, b) post-elution recovery, c) removal, by crossflow filtration with CS-blocked membrane. One filtration was run for each set of conditions. The error bar indicates the standard deviation associated with the experimental method. 99 Figure 3.4 (cont’d) c) 5 plaque assay log removal 4 3 2 1 0 high Jp, low Jcf 3.3.3 low Jp, low Jcf filtration conditions low Jp, high Jcf DI water vs. surface water As Fig. 3.2 demonstrates, at the pre-elution level there was no significant difference between in the recovery of infective P22 from surface water and from DI water. At the postelution level, average recovery from surface water was consistently higher than recovery from DI water, however, the difference is not statistically significant. We did not expect post-elution recovery from surface water to be higher than post-elution recovery from DI water, especially under high J p - low Jcf . In these conditions, virus can get trapped in the fouling layer, which is more important for surface water than for DI water (Fig 3.3). 100 3.3.4 Effect of filtration condition on CS layer integrity To explain the absence of influence of Jcf / J p on the recovery and removal of infective P22 and P22 DNA, we hypothesized that the calf serum layer was disintegrating at higher Jcf / J p values thus offsetting the benefit of lower concentration polarization and fouling. However, as seen in Fig. 3.5, 25 kDa dextran rejection by CS-blocked membrane was not affected by filtration conditions, indicating that the layer integrity is maintained. The test was performed at 40 psi and, as a consequence, Jcf / J p values higher than 8,000 were not tested (although those conditions were used in P22 filtration tests). 101 a) 100 90 dextran rejection, % 80 70 60 50 40 30 20 immediately after Jcf increase 5 min after Jcf increase 10 0 0.0 b) 0.2 0.4 0.6 0.8 crossflow to permeate flux ratio Jcf/Jp 104 1.0 100 90 dextran rejection, % 80 70 60 50 40 30 20 immediately after Jcf increase 5 min after Jcf increase 10 0 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 2.4 crossflow flux Jcf 104, L/min.m2 Dextran rejection by CS-blocked membrane under increasing Jcf / J p during a) filtration and b) elution. n=3 for filtration, error bar indicates standard deviation; n=1 for elution. 102 During elution, dextran rejection decreased as Jcf increased, indicating that the layer integrity was compromised. (Additional testing should be performed to confirm this trend as only one elution test was performed). We do not expect this phenomenon, if confirmed, to affect P22 recovery. On the contrary, stripping the layer off the membrane may be an effective approach for recovering those viruses that penetrated that layer during filtration. It is possible that when submitted to the pressure of 20 psi, the calf serum layer also loses integrity, which would balance the effect of decreasing the permeate flux in terms of virus adhesion to the membrane. In addition, increasing crossflow only has a minimal effect on decreasing concentration polarization of P22 [17]. Together, these phenomena could explain the lack of improvement in P22 preelution recovery or removal at increasing Jcf / J p However the calf serum layer stability at 20 psi should be assessed to confirm this hypothesis. 3.3.5 Conclusions Permeate flux and crossflow rate were found to have no statistically significant effect on the recovery and removal of infective P22. The average permeate flux could be increased up to 5-fold for DI water and 2-fold for surface water over values reported in the literature without affecting the recovery or removal of infective P22. However, virus infectivity and/or aggregation did seem to be affected by crossflow filtration. Specifically, under high J p - low Jcf conditions, viruses recovered at the post-elution stage seemed to have lower infectivity or be aggregated, which might be due to interactions with the membrane surface or the presence of additive at the elution stage. 103 REFERENCES 104 REFERENCES 1. Straub, T.M. and D.P. Chandler, Towards a unified system for detecting waterborne pathogens. Journal of Microbiological Methods, 2003. 53(2): p. 185-197. 2. Richards, G.P., Limitations of molecular biological techniques for assessing the virological safety of foods. Journal of Food Protection, 1999. 62(6): p. 691-697. 3. Winona, L.J., et al., Efficient and predictable recovery of viruses from water by small scale ultrafiltration systems. Canadian Journal of Microbiology, 2001. 47(11): p. 10331041. 4. Grassi, T., et al., Rotavirus detection in environmental water samples by tangential flow ultrafiltration and RT-nested PCR. Environmental Monitoring and Assessment, 2010. 164(1-4): p. 199-205. 5. Hill, V.R., et al., Comparison of hollow-fiber ultrafiltration to the USEPA VIRADEL technique and USEPA Method 1623. J. Environ. Qual., 2009. 38(2): p. 822-825. 6. Olszewski, J., L. Winona, and K.H. Oshima, Comparison of 2 ultrafiltration systems for the concentration of seeded viruses from environmnetal waters. Can. J. Microbiol., 2005. 51(4): p. 295-303. 7. Oshima, K.H., et al., The removal of phages T1 and Pp7, and poliovirus from fluids with hollow-fiber ultrafilters with molecular-weight cutoffs of 50000, 13000, and 6000. Can. J. Microbiol., 1995. 41(4-5): p. 316-322. 8. Soule, H., et al., Ultrafiltration and reverse transcription-polymerase chain reaction: An efficient process for poliovirus, rotavirus and hepatitis A virus detection in water. Water Res., 2000. 34(3): p. 1063-1067. 9. Rajal, V.B., et al., Validation of hollow fiber ultrafiltration and real-time PCR using bacteriophage PP7 as surrogate for the quantification of viruses from water samples. Water Res., 2007. 41(7): p. 1411-1422. 10. Sorber, C.A., B.P. Sagik, and J.F. Malina, Virus Rejection by Reverse OsmosisUltrafiltration Processes. Water Research, 1972. 6(11): p. 1377. 11. Furiga, A., et al., Effects of ionic strength on bacteriophage MS2 behavior and their implications for the assessment of virus retention by ultrafiltration membranes. Applied and Environmental Microbiology, 2011. 77(1): p. 229-236. 12. Pierre, G.l., et al., Protocol for the assessment of viral retention capability of membranes. Journal of Membrane Science, 2011. 381(1-2): p. 41-49. 105 13. Michalsky, R., et al., Effects of temperature and shear force on infectivity of the baculovirus Autographa californica M nucleopolyhedrovirus. Journal of Virological Methods, 2008. 153(2): p. 90-96. 14. Mylon, S.E., et al., Influence of salts and natural organic matter on the stability of bacteriophage MS2. Langmuir, 2010. 26(2): p. 1035-1042. 15. Sablani, S.S., et al., Concentration polarization in ultrafiltration and reverse osmosis: a critical review. Desalination, 2001. 141(3): p. 269-289. 16. Herath, G., K. Yamamoto, and T. Urase, The effect of suction velocity on concentration polarization in microfiltration membranes under turbulent flow conditions. Journal of Membrane Science, 2000. 169(2): p. 175-183. 17. Wiesner, M.R. and S. Chellam, Mass-transport considerations for pressure-driven membrane processes. Journal American Water Works Association, 1992. 84(1): p. 88-95. 18. Hill, V.R., et al., Development of a rapid method for simultaneous recovery of diverse microbes in drinking water by ultrafiltration with sodium polyphosphate and surfactants. Applied and Environmental Microbiology, 2005. 71(11): p. 6878-6884. 19. Hill, V.R., et al., Multistate evaluation of an ultrafiltration-based procedure for simultaneous recovery of enteric microbes in 100-liter tap water samples. Applied and Environmental Microbiology, 2007. 73(19): p. 6327-6327. 20. Morales-Morales, H.A., et al., Optimization of a reusable hollow-fiber ultrafilter for simultaneous concentration of enteric bacteria, protozoa, and viruses from water. Applied and Environmental Microbiology, 2003. 69(7): p. 4098-4102. 21. Polaczyk, A.L., et al., Ultrafiltration-based techniques for rapid and simultaneous concentration of multiple microbe classes from 100-L tap water samples. Journal Of Microbiological Methods, 2008. 73(2): p. 92-99. 22. Belfort, G., Y. Rotem, and E. Katzenelson, Virus concentration using hollow fiber membranes. Water Res., 1975. 9(1): p. 79-85. 23. Madaeni, S.S., A.G. Fane, and G.S. Grohmann, Virus removal from water and wastewater using membranes. Journal of Membrane Science, 1995. 102: p. 65-75. 24. Wickramasinghe, S.R., et al., Understanding virus filtration membrane performance. Journal of Membrane Science, 2010. 365(1-2): p. 160-169. 25. Jacangelo, J.G., S.S. Adham, and J.-M. Laine, Mechanism of cryptosporidium, giardia, and MS2 virus removal by MF and UF. American Water Works Association Journal, 1995. 87(9): p. 107-121. 106 Chapter 4. Virus recovery and concentration from complex water matrices using PEM-coated membranes: Preliminary assessment 4.1 Introduction In Chapter 2 we showed that PEM-coated membranes show promising results for the recovery of viruses present in DI water; however, viruses often need to be concentrated from more complex matrices: tap water, groundwater, surface water as well as water treated for reuse applications. It has been shown that increasing water complexity can affect virus recovery by crossflow filtration [1]. For example, Belfort et al. showed that poliovirus recovery decreased from 77% with DI water to 52% with tap water. In at least one study, however, water complexity did not affect virus recovery as there was no significant difference in infective MS2 and PRD1 recovery between drinking and surface water [2]. Even for the same type of water, variation in water composition can greatly affect virus recovery [3, 4]. T1 phage recovery from surface water from 6 different locations varied from 34% to 75% [3], and PP7 recoveries from storm water from 21 different locations varied from 10% to 98 % when assessed by qPCR, and from 25% to 90% when assessed by plaque assay. However, since filtrations were not replicated it is not possible to conclude whether the variations were due to differences in the water composition or to an inherent irreproducibility of the combination of the recovery and detection methods. In a study on virus recovery from drinking water from 8 different locations, Hill et al. [5] did perform replicate measurements and found no statistically significant correlations between the 7 parameters tested (pH, turbidity, 107 alkalinity, conductivity, iron concentration, TOC, and DOC) and recoveries of MS2 or ΦX174 phages. Water composition can affect both concentration and quantification steps. The formation of a cake layer may prevent virus passage through the membrane [6, 7] or conceal a membrane’s anti-adhesive properties with respect to a virus. Virus surface properties also depend on the solution makeup (such as ionic strength, presence of divalent cations and dissolved NOM). In addition, materials present in the water might affect the detection method [8], especially in the case of highly concentrated samples. This is why it is important to evaluate the concentration and detection methods with a wide range of water compositions. In this Chapter the performance of PEM-coated membrane in recovering P22 from MBR effluent and surface water is evaluated and compared to the performance of CS-blocked membrane. The effect of adjusting TOC levels in samples before DNA extraction is assessed so that we can determine if the observed effects of water complexity on recovery or removal occurred at the concentration or detection steps. In addition, since the possibility of virion entrapment at the membrane surface increases with water complexity, the effect of adding a backflush step after elution on final P22 recovery is studied for surface water samples. 108 4.2 4.2.1 Materials and Methods Reagents The reagents used in this chapter were the same as those described in corresponding sections of previous Chapters. 4.2.2 Water samples A 25 L membrane bioreactor (MBR) effluent sample was collected from the Traverse City wastewater treatment plant (Traverse City, MI) as a grab sample in August 2011. A 10 L surface water sample was collected from Lake Lansing (Lansing, MI) as a grab sample in September 2011, and filtered through a 0.45 μm membrane on the day of collection. Samples were kept at 4°C until used. Water samples were used as early as the day following their collection and within 1 months of their collection. Before use, the surface water container was agitated to resuspend any settled particles. 4.2.3 Water quality testing. Total organic carbon (TOC) contents of MBR effluent sample and filtered Lake Lansing water were determined using a Total Organic Carbon analyzer (1010, O I Analytical, USA). To determine how filtration affected the TOC content of retentate and permeate samples, filtrations of MBR effluent and surface water were performed with a PEM-coated membrane and a CS109 blocked membrane in conditions similar to the ones used in virus concentration tests (except for the filtration of MBR effluent with a CS-blocked membrane which was performed at 40 psi instead of 20 psi), and TOC analysis was performed on feed, retentate and permeate samples. Each sample was analyzed at least in triplicate. Calibration standards and blanks were run for each set of measurements. 4.2.4 Bacteriophage Bacteriophages were cultured as described in Chapter 2, section 2.2.2. 4.2.5 Membrane preparation, crossflow concentration apparatus and concentration procedure The PEM-coated membranes and CS-blocked membranes were prepared as described in Chapter 2 section 2.2.5. The filtration apparatus and concentration procedure are described in Chapter 2 sections 2.2.4 and 2.2.7. For both types of water, filtrations at high J cf and low J p (i.e., “highest recovery conditions”) were performed at least in triplicate. For the MBR effluent, PEM performance at high J cf and high J p was also evaluated. Filtration conditions used in this study are shown in Fig. 4.1. Elution was performed with 500 mL of permeate amended with 0.01% Tween 80 and 0.01% NaPP. Filtrations with surface water included an additional backflush step after elution. To backflush the membrane, it was flipped in the filtration cell so that the membrane skin, coated by PEM or blocked with CS, was on the permeate side. The backflush was performed by filtering 100 mL of permeate through the membrane at the applied transmembrane pressure of approximately 40 psi. 110 MBR effluent with CS-blocked membrane surface water with CS-blocked membrane MBR effluent with PEM-coated membrane surface water with PEM-coated membrane earlier studies initial permeate fllux Jp, L/(min·m2) 10 9 8 7 6 high Jp high Jcf fastest concentration conditions 5 4 3 (5) 2 (2, 11) (3) 1 low Jp high Jcf highest recovery conditions 0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 crossflow flux Jcf ·104, L/(min·m2) Figure 4.1: Filtration conditions in experiments on P22 concentration and recovery from MBR effluent and surface water using CS-blocked membranes and PEM-coated membrane. Number of tests: n=9 for MBR effluent (3 with CS-blocked membranes, 6 with PEM-coated membranes), n=7 for surface water (3 with CS-blocked membranes, 4 with PEM-coated membranes). 4.2.6 Sample analysis P22 concentration in feed, retentate, permeate, eluate and backflush samples were measured by qPCR as described in Chapter 2 section 2.2.8. For comparison, all samples except the one from filtration tests performed in “fastest concentration” conditions were also run as described in Chapter 2 section 2.2.8 with the exception that prior to DNA extraction, retentate and feed samples were diluted with PCR grade water (Roche) so that TOC levels in those 111 samples matched TOC levels in permeate samples. Values of P22 recovery and removal from MBR effluent and surface water samples were compared to corresponding values recorded in an experiment that used DI water and was run in similar filtration conditions (data from Chapter 2). Data were compared using the Student t-test. P < 0.1 was considered to show statistical significance. A Bonferroni correction was performed when multiple comparisons were done. 4.3 4.3.1 Results and Discussion Water quality Results from TOC analysis are presented in Table 4.1. TOC levels in surface water, 9.0 ± 0.2 ppm, are slightly higher than TOC levels in MBR effluent, 7.3 ± 1.0 ppm. TOC from surface water seemed to be better recovered than TOC from MBR effluent by both CS-blocked and PEM-coated membranes. (The experiment should be replicated to determine if the difference is statistically significant.) When surface water was filtered through CS-blocked membranes, the combined TOC values of the permeate and the retentate exceeded the TOC values measured in the feed. This could either be due to calf serum shed by the blocking layer to the retentate stream, or the result of an experimental error. Additional experiments are necessary to identify which explanation is valid. 112 Table 4.1: MBR effluent and surface water TOC levels Type of water TOC level TOC TOC (ppm) rejection recovery Feed (1L) 8.0 13 % 27 % Retentate (250 mL) 8.5 Permeate (750 mL) CS-blocked Sample (Sample volume) MBR effluent Membrane 7.0 18 % 28 % 5% 41% 19% 36% PEM-coated Feed (1L) 6.6 Retentate (250 mL) Permeate (750 mL) Feed (1L) 8.8 15.5 Permeate (750 mL) CS-blocked 5.4 Retentate (250 mL) Surface water 7.2 8.4 PEM-coated Feed (1L) 9.1 Retentate (250 mL) Permeate (750 mL) 4.3.2 13.7 7.4 P22 recovery and removal from MBR effluent and surface water samples We expected that the higher TOC levels in the retentate samples would enhance P22 DNA extraction in retentate sample compared to P22 extraction from samples with lower TOC (feed and permeate). Indeed the presence of organic matter in samples has been shown to increase P22 extraction by MagNA Pure Compact system hypothetically by blocking adsorption sites on the surfaces of various system components such as tips or magnetic particles to prevent 113 the loss of P22 DNA due to adsorption (see Appendix B). As a consequence, any observed increase in recovery could be due to either a more efficient collection/concentration step or only a more efficient DNA extraction/detection step. For this reason, TOC levels in feed and retentate were adjusted to the TOC level in the permeate by dilution with PCR grade water. As can be seen in Fig. 4.2, except for the recovery of P22 from MBR effluent with PEM-coated membranes, recoveries obtained from TOC-adjusted qPCR analyses were on average lower than when TOC levels were not adjusted, however, the difference was not significant. Under the “highest recovery” conditions the pre-elution recovery of P22 by PEM-coated membranes was lower on average for MBR effluent and surface water than for DI water but the difference was not statistically significant. Lower pre-elution recovery recoveries may result from the “masking” of the anti-adhesive properties of the membrane by the organic fouling layer, from the entrapment of viruses within this fouling layer, or from both of these phenomena (Fig. 4.2). The post-elution recovery by PEM membranes was not significantly affected by the type of water. Increasing the permeate flux did not significantly affect the pre-elution or post-elution recovery of P22 from MBR effluent using PEM membranes (Fig. 4.3). For CS-blocked membrane, pre-elution and post-elution recoveries were not significantly different for DI water, MBR effluent and surface water. 114 a) post-elution pre-elution TOC adjusted TOC not adjusted 120 recovery, % 100 80 60 40 20 0 CS PEM CS DI water PEM MBR effluent CS PEM Surface water Type of membrane and type of water b) TOC adjusted 6 TOC not adjusted 5 log removal 4 3 2 1 0 CS PEM DI water CS PEM MBR effluent CS PEM Surface water Type of membrane and type of water Figure 4.2: a) P22 recovery and b) removal from DI water (data from Chapter 2), MBR effluent and surface water with CS-blocked and PEM-coated membranes under “highest recovery” conditions. Error bars indicate standard deviation. 115 a) b) 120 post-elution 5 pre-elution 4 80 log removal recovery, % 100 60 40 2 1 20 0 3 0 high Jp low low high Jcf high Jp, high Jcf Jp, Jp high Jcf high Jcf filtration conditions low Jp low Jp, high Jcf high highhigh Jcf Jp, Jp high Jcf high Jcf filtration conditions Figure 4.3: a) P22 recovery and b) removal from MBR effluent with PEM-coated membrane at high and low permeate fluxes. Error bars indicate standard deviation. Data reported here corresponds to samples where TOC was not adjusted. Although pre-elution recovery from MBR effluent by PEM-coated membranes was noticeably higher than by CS-blocked membrane, the difference was not significant. No difference was observed for surface water. At the post-elution level there was no difference between CS-blocked membranes and PEM-coated membranes for both types of water, which is also what was observed for DI water and was attributed to the weak adhesion of P22 to surfaces compared to other viruses. P22 removal was not significantly affected by the type of membrane or the type of water. 116 4.3.3 Effect of backflushing on P22 recovery from surface water. The fouling layer can entrap virions and render them less recoverable by elution. In that case adding a backflushing step can help recover viruses entrapped in the fouling layer. We performed backflushing after tests on the filtration of surface water spiked with P22. For these tests, we already showed (Table 4.2) that post-elution recoveries were not significantly lower than post-elution recoveries from DI water which means that the loss of viruses due to entrapment was probably minimal. It is thus not surprising that backflushing did not significantly increase P22 recovery. For all 6 filtrations where a backflush was performed, the post-backflush recovery was only marginally (less than 1%) higher the post- elution recovery. 4.3.4 Fouling resistance of CS-blocked and PEM-coated membrane Figure 4.4 shows the ratio of final to initial permeate flux. This ratio is a measure of the amount of fouling occurring during filtration. Initial and final permeate flux were averaged over the first and last minute of filtration, respectively. For DI water experiments the permeate flux reduction was higher for PEM-coated membranes than for CS-blocked membranes. For MBR effluent, the trend seemed to be reversed and PEM-coated membranes seemed to experience less fouling under both “highest recovery” and “fastest filtration” conditions (the difference was only significant under “fastest filtration” conditions) compared to CS-blocked membranes. Fouling resistance of the PEM-coated membranes stemmed from its higher hydrophilicity compared to CS--blocked membranes (see Chapter 2). For surface water, the amount of fouling observed for 117 CS- blocked membranes was higher on average than for PEM-coated membrane, but the difference was not statistically significant. 4.3.5 Conclusion Due to the small number of filtrations performed the data presented here are only preliminary. It was not possible to observe significant difference between PEM-coated membrane and CSblocked membrane in complex water matrices. However, PEM-coated membranes seemed to maintain their advantage in terms of P22 pre-elution recovery when concentrating viruses from MBR effluent. PEM-coated membranes also seemed to be more resistant to fouling. In experiments with surface water, however, no difference was observed. Additional filtration tests are needed to validate these trends. 118 a) Jp final/ Jp initial 1.0 CS-blocked membrane highest recovery conditions 0.8 0.6 0.4 0.2 0.0 DI water MBR effluent surface water type of water b) 1.0 CS-blocked membrane fastest concentration conditions Jp final/ Jp initial 0.8 0.6 0.4 0.2 0.0 DI water MBR effluent type of water Figure 4.4: Fouling observed for CS-blocked membrane and PEM-coated membrane during filtration tests performed to recover P22 from DI water, MBR effluent and surface water under a) “highest recovery” conditions and b) “fastest filtration” conditions. 119 REFERENCES 120 REFERENCES 1. Belfort, G., Y. Rotem, and E. Katzenelson, Virus concentration using hollow fiber membranes .2. Water Res., 1976. 10(4): p. 279-284. 2. Gibson, K.E. and K.J. Schwab, Tangential-flow ultrafiltration with integrated inhibition detection for recovery of surrogates and human pathogens from large-volume source water and finished drinking water. Applied and Environmental Microbiology, 2011. 77(1): p. 385-391. 3. Olszewski, J., L. Winona, and K.H. Oshima, Comparison of 2 ultrafiltration systems for the concentration of seeded viruses from environmnetal waters. Can. J. Microbiol., 2005. 51(4): p. 295-303. 5. Rajal, V.B., et al., Validation of hollow fiber ultrafiltration and real-time PCR using bacteriophage PP7 as surrogate for the quantification of viruses from water samples. Water Res., 2007. 41(7): p. 1411-1422. 6. Hill, V.R., et al., Multistate evaluation of an ultrafiltration-based procedure for simultaneous recovery of enteric microbes in 100-liter tap water samples. Applied and Environmental Microbiology, 2007. 73(19): p. 6327-6327. 6. Jacangelo, J.G., S.S. Adham, and J.-M. Laine, Mechanism of cryptosporidium, giardia, and MS2 virus removal by MF and UF. American Water Works Association Journal, 1995. 87(9): p. 107-121. 7. Wickramasinghe, S.R., et al., Understanding virus filtration membrane performance. Journal of Membrane Science, 2010. 365(1-2): p. 160-169. 8. Guy, R.A., et al., Real-time PCR for quantification of Giardia and Cryptosporidium in environmental water samples and sewage. Applied and Environmental Microbiology, 2003. 69(9): p. 5178-5185. 121 Chapter 5. Suggested future research Chapters 2 and 4 describe results of what is to our knowledge the first study of PEM membranes’ ability to remove and concentrate viruses. The membranes showed promising performance in terms of virus removal and pre-elution recovery; the latter was attributed to the negative charge and hydrophilicity of the PEM surface that resulted in unfavorable virus-PEM interactions. Our findings regarding the performance of PEM-coated membrane and calf serumblocked membrane are summarized in Table 5.1. A large number of experiments was necessary to evaluate the effect of crossflow and permeate flow rates on virus recovery. To make such screening feasible, we chose to work with the bacteriophage P22, which is a non-pathogenic virus. This choice was later proved be not optimal as relatively high post-elution recovery of P22 could be achieved by an existing method (using CS-blocked membranes). We expect that in the case of more adhesive viruses, such as adenovirus, the competitive advantage of the anti-adhesive PEM surface will be more evident. Specifically we expect the post-elution recovery obtained with PEM-coated membranes to be significantly higher than the one obtained with CS-blocked membranes. Thus, we suggest that PEM membranes are evaluated with adhesive, difficult-to-recover viruses. We also propose that these tests include backflushing the membrane to recover viruses that do attach to the surface. The performance of PEM-coated membranes in recovering viruses from complex water was evaluated with only three filtration tests for each water matrix (MBR effluent and surface water). Additional tests should be performed to confirm or disprove the advantage of PEM122 coated membrane over CS-blocked membranes in terms of recovery and/or reproducibility at the post-elution stage. Using a backflushing step instead of the elution step should also be evaluated as a possibility to improve reproducibility. The polyelectrolytes used in this study inhibited P22 infectivity and as a consequence the performance of PEM-coated membranes for the recovery of infective virus was not investigated. Future work should consider alternative PEM coatings that would not inhibit infectivity assay; in this context, multilayer formed through H-bonding rather polyelectrolyte interaction are an interesting option. Finally the PEM-based approach should be evaluated in a scaled-up system with a reusable, high surface area hollow fiber cartridge to concentrate large-volume samples. As both membrane surface area and sample volume will be increased proportionally, we expect that PEM-coated membrane performance will be maintained. The role of surface properties such as hydrophobicity, charge, roughness and stiffness in determining virus adhesion needs to be better understood. We suggest experimenting with carefully selected bacteriophages that present a wide range of surface properties and using a QCM-D instrument to rigorously quantify bacteriophage adhesion to various PEMs. Both PEMcoated surfaces, prepared using various polyelectrolytes combinations as well as various pH and ionic strength, and phage surfaces would need to be thoroughly characterized to determine their surface tension parameters and surface charge. In addition, atomic force microscopy would need to be used to characterize PEMs in terms of their roughness, swelling and stiffness. Based on the comparison of results of QCM-D tests, results of AFM measurements, and computed XDLVO energies of virus-PEM interactions, conclusions may be drawn on the factors determining virus adhesion to surfaces. 123 Table 5.1: Virus recovery performance of PEM-coated membrane and calf serum-blocked membrane at the pre-elution (rpre), post-elution (rpost) and coating removal - through elution or backflush with an adequate solution - (rsacrificial) stages. Note: +and ++ indicate that we expect the membrane well and very well, respectively. – indicates that we expect the membrane to perform poorly and ? indicates that additional experiments need to be performed to confirm our assumption rpre PEM-coated membrane rpost rsacrificial 2 -? ++ + infective virus - - ? total virus 1 +? total virus calf serum-blocked membrane infective virus - + 1 ? P22-specific inhibition If PEM used does not inhibit qPCR 124 1 + 2 APPENDICES 125 Appendix A. Determination of crossflow and permeate fluxes used by Morales-Morales et al. [1] and Hill et al. [2-4] Morales-Morales et al. [1] reported concentrating pathogen from a 10 L sample using a permeate flow of 300 mL/min and a crossflow rate of 3600 mL/min in a Microza hollow fiber cartridge 2 with 0.2 m membrane surface (model (AHP-1010). The permeate flux obtained by dividing the 2 permeate flow by the membrane surface area was 1.5 L/(min·m ). Pall Corporation, Microza’s manufacturer, reports on its website [5] that a crossflow rate of 724 L/h corresponds to a velocity of 1 m/s. For a 3,600 mL/min crossflow rate the velocity was thus 0.3 m/s, so the fluid 3 2 2 volumetric flux is 0.3 m /(m ·s) (or 18,000 L/(min·m )) [6]. In 2005, Hill et al. [2] reported concentrating pathogen from 10 L tap water samples with a permeate flow of 800 mL/min and a crossflow rate of 900 mL/min using a Fresenius Hemaflow 2 F80A hollow fiber filter with a membrane surface of 1.8 m . Again by dividing the permeate 2 flow by the membrane surface area gives a permeate flux of 0.44 L/(min·m ). Ronco et al. [7] reported that the Hemaflow F80A cartridge contains 12,288 fibers, each with an inner diameter -4 2 of 200 μm corresponding to a total crossflow cross-sectional area of 3.86·10 m . Thus, a 2 crossflow rate of 900 mL/min corresponds to a crossflow volumetric flux of 2,300 L/(min·m ). 126 In 2007 and 2009, Hill et al. [3, 4] used a Fresenius F200NR hollow fiber cartridge with a crossflow rate of 1,700 mL/min and a permeate flow rate of 1,200 L/min. The membrane surface 2 2 area was 2 m , which corresponds to a permeate flux of 0.6 L/(min.m ). The Fresenius F200NR was also described by Ronco et al. [7] The cartridge contained 13,824 fibers, each with an inner -4 2 diameter of 200 μm, which corresponded to a total cross-sectional area of 4.24·10 m . We thus determined that a crossflow rate of 1,200 L/min corresponds to a crossflow volumetric flux of 2 3,900 L/(min.m ). 127 REFERENCES 128 REFERENCES 1. Morales-Morales, H.A., et al., Optimization of a reusable hollow-fiber ultrafilter for simultaneous concentration of enteric bacteria, protozoa, and viruses from water. Applied and Environmental Microbiology, 2003. 69(7): p. 4098-4102. 2. Hill, V.R., et al., Development of a rapid method for simultaneous recovery of diverse microbes in drinking water by ultrafiltration with sodium polyphosphate and surfactants. Applied and Environmental Microbiology, 2005. 71(11): p. 6878-6884. 3. Hill, V.R., et al., Multistate evaluation of an ultrafiltration-based procedure for simultaneous recovery of enteric microbes in 100-liter tap water samples. Applied and Environmental Microbiology, 2007. 73(19): p. 6327-6327. 4. Hill, V.R., et al., Comparison of hollow-fiber ultrafiltration to the USEPA VIRADEL technique and USEPA Method 1623. J. Environ. Qual., 2009. 38(2): p. 822-825. 5. Microza membranes. 2012 [cited 2012; Available from: http://www.pall.com/main/Food-and-Beverage/Product.page?id=41053. 6. Reible, D.D., Fundamentals of engineering1999: CRC Press LLC. 7. Ronco, C., et al., Flow distribution analysis by helical scanning in polysulfone hemodialyzers: Effects of fiber structure and design on flow patterns and solute clearances. Hemodialysis International, 2006. 10(4): p. 380-388. 129 Appendix B. Addition of carrier RNA to sample: effect of DNA extraction/detection QPCR analysis of sample of P22 spiked in DI water and extracted using Roche’s MagNA Pure resulted in higher CP value than expected. This phenomenon (lower CP value for DNA material extracted from “clean samples” using MagNA Pure compared to environmental samples) had also been observed by Dr. Kelvin Wong when he was working in Dr. Xagoraraki’s lab and was attributed to the adsorption of virions and DNA to the magnetics beads and other components of the MagNA Pure instrument. The solution developed by Dr. Wong was to add carrier RNA to the sample before the extraction step. Carrier RNA had been used previously to increase DNA extraction efficiency [1]. In Table A.1 we show the results of tests we performed to determine the optimal amount of carrier RNA to add to filtration samples. Carrier RNA (obtained from Qiagen) solutions were prepared at a concentration of 1 mg/mL in PCR grade water or at a concentration of 0.01 mg/mL in viral lysis buffer (buffer AVL from Qiagen) and amount ranging from 5 µL to 15 µL of carrier RNA solution were added to 385 µL P22 in DI water samples. Samples were extracted using MagNA Pure instruments and qPCR was run in triplicate as described in Chapter 2 section 2.2.8. 130 Table B.1: Effect of carrier RNA addition on CP value obtained by qPCR Tube number Volume introduced (µL) 1 2 3 4 6 sample 385 385 385 385 385 Carrier RNA in water NA NA 10 NA NA 5 10 NA 15 NA PCR grade water 10 5 5 NA NA total 400 400 400 400 400 qPCR results (mean CP 19.81 ± 0.22 19.66 ± 19.18 ± 19.63 ± 23.62 ± 0.01 0.03 0.12 0.02 (1 mg/mL) Carrier RNA in buffer (0.01 mg/mL) value ± stdev) The lowest CP value, corresponding to the highest P22 concentration detected, was obtained for tube number 3 (which corresponds to the addition of 10 µL of carrier RNA at 1 mg/mL in qPCR grade water). Ten microliters of carrier RNA (1 mg/mL) were added to all samples used in this study before DNA extraction. 131 REFERENCES 132 REFERENCES 1. Kishore, R., et al., Optimization of DNA Extraction from Low-Yield and Degraded Samples Using the BioRobot® EZ1 and BioRobot® M48. Journal of Forensic Sciences, 2006. 51(5): p. 1055-1061. 133 Appendix C. Compaction behavior of PEM-coated membranes and CS-blocked membranes. Permeate flux data were averaged over the first and last minute of compaction and over the first minute of filtration in order to look at possible difference of behavior during compaction and decompression (between the compaction stage and the filtration stage) of the membrane. Results are shown in Fig. C.1. There is no significant difference of behavior between CS-blocked membrane and PEM-coated membrane. 600 compaction initial compaction final Filtration initial permeability (L/hr.m2.bar) 500 400 300 200 100 0 bare PES 30kDa CS Type of membrane PEM Compaction and decompaction behavior of bare PES membranes, CS-blocked membranes and PEM-coated membranes. Error bar indicates the 95% confidence intervals. Number of test: n = 3 for bare PES membrane, n = 72 for CS-blocked membrane and n = 37 for PEM coated membrane 134 Appendix D. PEM layer stability during filtration and elution. The stability of the PEM layer during filtration was tested as described in section 3.2.6. The test was performed in triplicate for filtration and elution conditions. On Fig D.1 we can see that 25 kDa dextran rejection by (HE/CHI)4.5 was highly variable and was only approximately 50% on average (whereas CS-blocked membrane rejected approximately 60 to 70 % of 25 kDa dextran). A higher molecular weight dextran might have been a better probe to assess the stability of (HE/CHI)4.5. The PEM stability seems to be maintained at low Jcf / J p however, for Jcf / J p value higher than 7,000 rejection of 25 kDa dextran seems to decrease. During elution, dextran rejection dramatically decreased even at the lowest crossflow rate used in these experiments which indicates that (HE/CHI)4.5 probably lose integrity during elution. 135 a) 100 immediately after Jcf increase 5 min after Jcf increase 90 dextran rejection, % 80 70 60 50 40 30 20 10 0 0.0 0.2 0.4 0.6 0.8 1.0 crossflow to permeate flux ratio Jcf/Jp 1.2 104 b) 100 immediately after Jcf increase 5 min after Jcf increase 90 dextran rejection, % 80 70 60 50 40 30 20 10 0 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 2.4 crossflow flux Jcf 104, L/min.m2 Dextran rejection by PEM-coated membrane under increasing Jcf / J p during a) filtration and b) elution. n=3 for filtration and elution, error bar indicates standard deviation. 136 Appendix E. Preliminary work on visualization of virus adhesion on surfaces As mentioned in Chapter 1 it is possible to visualized virions and aggregates deposited on surfaces using AFM [1-5]. Aside from Pereira et al. study [5], viruses were deposited on clean and smooth surface such as silicon or mica. In Pereira study, dengue virus adsorption on silicon wafers and protein covered silicon wafers. On those they were observed aggregated and isolated particles with height of approximately 10 to 15 nm which the authors considered to be hemagglutinins particles secreted by dengue virus, and 25 to 30 nm which the authors considered to be dengue particles with a collapsed lipid envelope [5]. In this preliminary study (PDADMA/PSS)4.5 were deposited on mica support (polyelectrolyte solution were prepared at a polyelectrolyte concentration of 0.02M and a NaCl concentration of 0.5M). The PEM-coated supports were then dipped for 30 min. in P22 suspension. To prepare this suspension, P22 stock was purified by centrifugal filtration at 4000 rpm using Amicon Ultra 4 centrifugal filter device with a 100,000 kDa cellulose membrane (Millipore). The virions retained by the membrane were resuspended in KCl 0. M. P22 concentration was approximately 9 10 PFU/mL. The supports were then dried and analyzed by AFM using the Nanoscope IV Multimode SPM from Veeco in tapping mode at room temperature using silicon cantilever with NSC15 tip from Mikromasch. The obtained AFM topographic imaged are shown in Fig. E.1 137 a) b) 90 nm 80 nm 2 4 6 8 µm 6 4 2 10 c) 8 µm 40 nm 20 nm 0 nm 0 0 10 µm AFM topographic images of a) (PDADMA/PSS)4.5 on gold substrate b) and c) (PDADMA/PSS)4.5 on mica dipped in P22 suspension In Fig. E.1, image b which is the (PDADMA/PSS)4.5 dipped in P22 suspension scan, shows more high structure (up to 80 nm) than image a which is the scan of a (PDADMA/PSS)4.5 which could be attributed to P22 particles (~60 nm). However, it is not possible to make a direct comparison as the layers were not deposited on similar surface. 138 Another potential method to visualize virus is epifluorescence [4]. Epifluorescence has been used to enumerate virions from water samples [4, 6-11]. Viruses are recovered on a filter which is strained with SYBR Green, DAPI or Yo-Pro (fluorescent dyes that specifically bind to DNA). The virus can then be visualized and enumerated by epifluorescence microscopy. In this preliminary study a serial dilution of P22 suspensions was prepared. Ten milliliters from each dilution was filtered with 0.02µm anodisc filter from Whatman backed with a 0.45 µm cellulose ester filter. The filters were then dried and following Noble 2001 protocols a drop of staining solution (0.25% SYBR Green I gel strain from Invitrogen) was placed on the filter for 15 min, the drop was then removed and the filter dried. The filter was mounted on a glass slide with a drop of anti-fading solution (0.1% p-phenylenediamine in a mixture of 50% glycerol and 50% phosphate buffer saline) between the sample and the cover slip. Samples were frozen until analyzed using a Zeiss Pascal laser scanning confocal microscope with a 488 nm illumination. The emission was detected through a long pass 505 nm filter. In addition to the serial dilution (PSS/PAH)4.5 and (PSS/PAH)4 were deposited on anodisc filters 8 which were then dipped for 30 min in P22 suspension (~10 PFU/mL). The filters were then dried and stained as described above. Results are shown in Fig. E.2 and E.3. 139 a) 50 µm 50 µm c) d) 50 µm 50 µm Fluorescence images of serial dilution samples. a) corresponds to the 1:1000 4 5 6 dilution, b) to the 1:10 dilution, c) to the 1:10 dilution and d) to the 1:10 dilution Pictures were taken at ×40 magnification There does not seem to be any correlation between the number of fluorescent spots and the dilution factor. One possibility is that focusing was done on viral aggregates and that the rest of the virions would be visible at a different focal plan. 140 a) b) 100 µm 100 µm c) 100 µm Fluorescence images of a) (PSS/PAH)4-coated ; b) (PSS/PAH)4.5-coated and c) bare anodisc filters dipped in P22 suspension. Pictures were taken at ×20 magnification Fluorescent spots are visible on both PEM-coated anodisc but barely any are visible on the bare anodisc filter. Unfortunately, because no controls were performed it is not possible to say if these fluorescent spot are attributable to P22 particles or caused by agglomerates of polyelectrolyte itself. 141 REFERENCES 142 REFERENCES 1. Ikai, A., et al., Atomic force microscope of bacteriophage T4 and its tube-baseplate complex. FEBS Letters, 1993. 326(1-3): p. 39-41. 2. Kolbe, W.F., D.F. Ogletree, and M.B. Salmeron, Atomic Force Microscopy Imaging of T4 Bacteriophages on Silicon Substrates. Ultramicroscopy, 1992. 42: p. 1113-1117. 3. Dubrovin, E.V., et al., Atomic force microscopy as a tool of inspection of viral infection. Nanomed. Nanotechnol. Biol. Med., 2007. 3(2): p. 128-131. 4. Zago, M., et al., Epifluorescence and atomic force microscopy: Two innovative applications for studying phage-host interactions in Lactobacillus helveticus. Journal of Microbiological Methods, 2012. 88(1): p. 41-46. 5. Pereira, E.M.A., et al., Binding of dengue virus particles and dengue proteins onto solid surfaces. ACS Applied Materials & Interfaces, 2010. 2(9): p. 2602-2610. 6. Noble, R.T. and J.A. Fuhrman, Use of SYBR green I for rapid epifluorescence counts of marine viruses and bacteria. Aquat. Microb. Ecol., 1998. 14: p. 113-118. 7. Hara, S., K. Terauchi, and I. Koike, Abundance of viruses in marine waters - Assessment by epifluorescence and transmission electron-microscopy. Applied and Environmental Microbiology, 1991. 57(9): p. 2731-2734. 8. Hennes, K.P. and C.A. Suttle, Direct counts of viruses in natural waters and laboratory cultures by epifluorescence microscopy. Limnol. Oceanog., 1995. 40: p. 1050-1055. 9. Weinbauer, M.G. and C.A. Suttle, Comparison of epifluorescence and transmission electron microscopy for counting viruses in natural marine waters. Aquat. Microb. Ecol., 1997. 13: p. 225-232. 10. Wen, K., A.C. Ortmann, and C.A. Suttle, Accurate estimation of viral abundance by epifluorescence microscopy. Applied and Environmental Microbiology, 2004. 70(7): p. 3862-3867. 11. Rinta-Kanto, J.M., et al., Rapid enumeration of virus-like particles in drinking water samples using SYBR green I-staining. Water Research, 2004. 38(10): p. 2614-2618. 143