2015
DOI: 10.1021/acs.est.5b01414
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Microbial Transport, Retention, and Inactivation in Streams: A Combined Experimental and Stochastic Modeling Approach

Abstract: Long-term survival of pathogenic microorganisms in streams enables long-distance disease transmission. In order to manage water-borne diseases more effectively we need to better predict how microbes behave in freshwater systems, particularly how they are transported downstream in rivers. Microbes continuously immobilize and resuspend during downstream transport owing to a variety of processes including gravitational settling, attachment to in-stream structures such as submerged macrophytes, and hyporheic excha… Show more

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Cited by 55 publications
(72 citation statements)
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References 56 publications
(124 reference statements)
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“…Additionally, other size fractions, likely larger particles, appear to get caught in the porous medium or on biofilm, either permanently or at least over the timescales of our current experiments with less mass breaking through the system than being injected into it, although the fraction of mass retained varied significantly from experiment to experiment with no clear and identifiable control on what drove this behaviour. Similar results have been shown in sand-packed columns for monodisperse particles such as Cryptosporidium oocysts [48] and for E. coli [49]; however, eDNA that is shed from macroorganisms is a particle with a wider range of sizes and sources than noted in the microbial transport literature [29,30]. In another context, organic particles have been shown to slowly release after initial deposition [49,50]; for the case of NOM, which is also polysdisperse, but more homogeneous than eDNA, different size fractions are adsorbed and released at different rates [45] leading to a broad distribution of travel times and models that reflect these broad distributions appear capable of describing their anomalous behaviour [46,47].…”
Section: Discussionsupporting
confidence: 86%
“…Additionally, other size fractions, likely larger particles, appear to get caught in the porous medium or on biofilm, either permanently or at least over the timescales of our current experiments with less mass breaking through the system than being injected into it, although the fraction of mass retained varied significantly from experiment to experiment with no clear and identifiable control on what drove this behaviour. Similar results have been shown in sand-packed columns for monodisperse particles such as Cryptosporidium oocysts [48] and for E. coli [49]; however, eDNA that is shed from macroorganisms is a particle with a wider range of sizes and sources than noted in the microbial transport literature [29,30]. In another context, organic particles have been shown to slowly release after initial deposition [49,50]; for the case of NOM, which is also polysdisperse, but more homogeneous than eDNA, different size fractions are adsorbed and released at different rates [45] leading to a broad distribution of travel times and models that reflect these broad distributions appear capable of describing their anomalous behaviour [46,47].…”
Section: Discussionsupporting
confidence: 86%
“…However, the low particle retention rates within the restored stream indicate low potential for clogging of interstitial pores. These results support previous observations showing that processes such as filtration initially immobilize particles within the streambed, but other processes such as scour and fill resuspend accumulated fine particle deposits and drive particle deposition deeper in the bed (Drummond et al, ; Gartner et al, ; Rehg et al, ). Thus, the long‐term maximum depth of fine particle infiltration is ultimately limited by a combination of particle infiltration in the bed, deposition within the bed, and the depth to which scour remobilizes sediment and restores the permeability and porosity of the bed.…”
Section: Resultssupporting
confidence: 91%
“…For the same reason, we assume that delivery of fine particles to transient storage areas is controlled purely by advective exchange and that gravitational settling is negligible. In this case, hyporheic exchange of solute and fine particles is also similar, and Λ S ≈ Λ P. Based on prior investigations of solute and fine particle dynamics in rivers (Boano et al, ; Drummond, Davies‐Colley, et al, ; Drummond et al, ; Haggerty et al, ; Stonedahl et al, ), we assume a power law residence time distribution within the immobile region, φ S ( t ) ~ t()1+βS for 0 < β S < 1.…”
Section: Theory/calculationmentioning
confidence: 99%
“…A more detailed description of the model, previously applied to solute and fine particle transport in rivers in Drummond et al . [; ] without any modifications, is included in the supporting information [ Cortis and Berkowitz , ; Boano et al ., ]. Here we provide a brief review of the key equation and parameters.…”
Section: Model Analysismentioning
confidence: 99%