Pseudomonas aeruginosa

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Supporting Information
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Comparison of the transport and deposition of
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Pseudomonas aeruginosa under aerobic and anaerobic
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conditions
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Huixin Zhanga, Hongbo Zengb, Ania C. Ulricha, Yang Liua*
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a
Department of Civil and Environmental Engineering
University of Alberta, Edmonton, AB T6G 2W2, Canada
b
Department of Chemical and Materials Engineering
University of Alberta, Edmonton, AB T6G 2V4, Canada
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*Corresponding author: Department of Civil and Environmental Engineering, University
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of Alberta, 3-095 Markin/CNRL Natural Resources Engineering Facility, 9105 116
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Street, Edmonton, Alberta, T6G 2W2, Canada. Tel: (780) 492-5115; E-mail:
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yang.liu@ualberta.ca
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1.
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To better understand the mechanism controlling the observed PAO1 transport and
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deposition behaviors in column experiments, the DLVO theory was used to estimate the
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total interaction energy as the bacterial cells approaching a glass bead in each condition.
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The total interaction energy, including the sum of van der Waals forces and electrostatic
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double layer interactions, was determined by modeling the microbial cell-glass bead
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system as a sphere-plate interaction [Redman et al., 2004; Tufenkji and Elimelech, 2004].
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The electrostatic double layer interaction energies (ΦEDL) were calculated using the
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expression derived by Hogg et al. [Hogg et al., 1966]:
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Φ𝐸𝐷𝐿 = πœ‹πœ€0 πœ€π‘Ÿ π‘Žπ‘ {2πœ“π‘ πœ“π‘ 𝑙𝑛 [1−exp⁑(−πœ…β„Ž)] + (πœ“π‘2 + πœ“π‘2 )𝑙𝑛[1 − exp⁑(−2πœ…β„Ž)]}
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where ε0 is the dielectric permittivity in a vacuum, εr is the relative dielectric permittivity
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of water, ap is the microbial radius, κ is the inverse Debye length, h is the separation
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distance between the microorganism and the collector surface, and ψp and ψc are the
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surface potentials of the microbial cell and bead collector, respectively. The retarded van
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der Waals attractive interaction energy was calculated based on [Elimelech and Omelia,
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1990; Gregory, 1981]:
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Φπ‘‰π·π‘Š = −
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where A is the Hamaker constant of the interacting media (microorganism – water – glass
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bead) and λ is the characteristic wavelength of the dielectric (assumed to be 100 nm). A
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value of 4.16 × 10-21 J was used for the Hamaker constant implying an attractive van der
Derjaguin-Landau-Verwey-Overbeek (DLVO) interaction energy calculations
1+𝑒π‘₯𝑝(−πœ…β„Ž)
π΄π‘Žπ‘
6β„Ž
[1 +
14β„Ž −1
πœ†
]
(S1)
(S2)
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Waals interaction as a microbial cell approaches a glass bead-water interface [Chen and
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Walker, 2012; Israelachvili, 2011; Lerner et al., 2012].
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References
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Chen, G., and S. L. Walker (2012), Fecal Indicator Bacteria Transport and Deposition in
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Saturated and Unsaturated Porous Media, Environmental science & technology, 46(16),
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8782-8790.
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Elimelech, M., and C. R. Omelia (1990), Effect of Particle-Size on Collision Efficiency in the
Deposition of Brownian Particles with Electrostatic Energy Barriers, Langmuir, 6(6), 1153-1163.
Gregory, J. (1981), Approximate Expressions for Retarded Vanderwaals Interaction, Journal of
colloid and interface science, 83(1), 138-145.
Hogg, R., T. W. Healy, and Fuersten.Dw (1966), Mutual Coagulation of Colloidal Dispersions,
Transactions of the Faraday Society, 62(522P), 1638-&.
Israelachvili, J. N. (2011), Intermolecular and surface forces, 3rd ed, xxx, 674 p. : ill. pp., Academic
Press, Burlington, MA.
Lerner, R. N., Q. Lu, H. Zeng, and Y. Liu (2012), The effects of biofilm on the transport of
stabilized zerovalent iron nanoparticles in saturated porous media, Water research, 46(4), 975985.
Redman, J. A., S. L. Walker, and M. Elimelech (2004), Bacterial adhesion and transport in porous
media: Role of the secondary energy minimum, Environmental science & technology, 38(6),
1777-1785.
Tufenkji, N., and M. Elimelech (2004), Deviation from the classical colloid filtration theory in the
presence of repulsive DLVO interactions, Langmuir, 20(25), 10818-10828.
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