1 Supporting Information 2 Comparison of the transport and deposition of 3 Pseudomonas aeruginosa under aerobic and anaerobic 4 conditions 5 6 Huixin Zhanga, Hongbo Zengb, Ania C. Ulricha, Yang Liua* 7 8 9 10 11 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 12 13 14 *Corresponding author: Department of Civil and Environmental Engineering, University 15 of Alberta, 3-095 Markin/CNRL Natural Resources Engineering Facility, 9105 116 16 Street, Edmonton, Alberta, T6G 2W2, Canada. Tel: (780) 492-5115; E-mail: 17 yang.liu@ualberta.ca 1 18 1. 19 To better understand the mechanism controlling the observed PAO1 transport and 20 deposition behaviors in column experiments, the DLVO theory was used to estimate the 21 total interaction energy as the bacterial cells approaching a glass bead in each condition. 22 The total interaction energy, including the sum of van der Waals forces and electrostatic 23 double layer interactions, was determined by modeling the microbial cell-glass bead 24 system as a sphere-plate interaction [Redman et al., 2004; Tufenkji and Elimelech, 2004]. 25 The electrostatic double layer interaction energies (ΦEDL) were calculated using the 26 expression derived by Hogg et al. [Hogg et al., 1966]: 27 ΦπΈπ·πΏ = ππ0 ππ ππ {2ππ ππ ππ [1−expβ‘(−π β)] + (ππ2 + ππ2 )ππ[1 − expβ‘(−2π β)]} 28 where ε0 is the dielectric permittivity in a vacuum, εr is the relative dielectric permittivity 29 of water, ap is the microbial radius, κ is the inverse Debye length, h is the separation 30 distance between the microorganism and the collector surface, and ψp and ψc are the 31 surface potentials of the microbial cell and bead collector, respectively. The retarded van 32 der Waals attractive interaction energy was calculated based on [Elimelech and Omelia, 33 1990; Gregory, 1981]: 34 Φππ·π = − 35 where A is the Hamaker constant of the interacting media (microorganism – water – glass 36 bead) and λ is the characteristic wavelength of the dielectric (assumed to be 100 nm). A 37 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+ππ₯π(−π β) π΄ππ 6β [1 + 14β −1 π ] (S1) (S2) 2 38 Waals interaction as a microbial cell approaches a glass bead-water interface [Chen and 39 Walker, 2012; Israelachvili, 2011; Lerner et al., 2012]. 40 References 41 Chen, G., and S. L. Walker (2012), Fecal Indicator Bacteria Transport and Deposition in 42 Saturated and Unsaturated Porous Media, Environmental science & technology, 46(16), 43 8782-8790. 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 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. 60 61 3