2003
DOI: 10.1093/qjmam/56.1.65
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Nutrient Uptake by a Self-Propelled Steady Squirmer

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Cited by 138 publications
(169 citation statements)
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“…The retention of the time variation in fluid and particle motion permits a general solution that collapses to the steady solution and resolves time-dependent phenomena that might occur at the same time scale as the viscous diffusion. For swimming microorganisms ranging in diameter from d = 1 to 100 µm the Reynolds number can range between Re = 10 −5 and 10 −1 (Magar et al 2003). In this low-Reynolds-number flow regime, convection in the fluid is negligible and the unsteady Stokes' equations for fluid flow apply.…”
Section: Governing Equationsmentioning
confidence: 99%
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“…The retention of the time variation in fluid and particle motion permits a general solution that collapses to the steady solution and resolves time-dependent phenomena that might occur at the same time scale as the viscous diffusion. For swimming microorganisms ranging in diameter from d = 1 to 100 µm the Reynolds number can range between Re = 10 −5 and 10 −1 (Magar et al 2003). In this low-Reynolds-number flow regime, convection in the fluid is negligible and the unsteady Stokes' equations for fluid flow apply.…”
Section: Governing Equationsmentioning
confidence: 99%
“…Koch & Subramanian 2011). However, only a few of the numerical studies of individual swimming particles, including biofilms, that provide insight into the behaviour of active suspensions include mass transfer and nutrient uptake (Magar, Goto & Pedley 2003;Magar & Pedley 2005;Michelin & Lauga 2011;Taherzadeh, Picioreanu & Horn 2012). In these studies, the concentration of nutrients in the fluid medium are typically treated as a passive scalar.…”
Section: Introductionmentioning
confidence: 99%
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