Hydrodynamic interaction of two swimming model micro-organisms

By Takuji Ishikawa, M. Simmonds, T. Pedley. Journal of Fluid Mechanics, 2006

413 citations recorded by the source corpus.

Subfields: Biomedical Engineering, Condensed Matter Physics, Ocean Engineering

View Paper: https://www.semanticscholar.org/paper/40c6ab244981311377b7d2eed22cedfcffc4491e

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In Biomedical Engineering

In Condensed Matter Physics

In Ocean Engineering

Citations in the corpus

The hydrodynamics of swimming microorganisms (2008, background): “swimmer surface) [191, 192] and swimming with a single”
Optimal feeding is optimal swimming for all P\'eclet numbers (2011, background): “The second mode (n = 2) defines the local stress applied by the swimmer on the surrounding fluid [8, 24].”
The rheology of a semi-dilute suspension of swimming model micro-organisms (2007, methodology): “That axisymmetric swimming micro-organisms would generate a stresslet of this form was also noted by Pedley & Kessler (1990) and by Hatwalne et al.”
Diffusion of swimming model micro-organisms in a semi-dilute suspension (2007, methodology): “The model micro-organism used in this paper (a squirmer) is the same as the one used by Ishikawa et al. (2006), based on Blake (1971).”
Critical bacterial concentration for the onset of collective swimming (2009, background): “One may, in fact, question the choice of the surface velocity boundary condition chosen by Ishikawa et al. (2006) even in the context of a ciliated organism.”
Development of coherent structures in concentrated suspensions of swimming model micro-organisms (2008, methodology): “We will follow Ishikawa et al. (2006) and omit squirming modes higher than the second (i.e. Bn = 0 in us when n 3), though such a restriction is not required for the numerical methods to work.”
Self-propulsion in viscoelastic fluids: Pushers vs. pullers (2012, background): “As in many previous studies [10, 14, 17, 19], we assume Bn = 0 for n ≥ 3.”
Active suspensions and their nonlinear models (2013, methodology): “The model was also used in numerical simulations to study pair hydrodynamic interactions [74], as well as diffusion [37], collective motion [38,39,75], and rheology [36] in semi-dilute suspensions.”
Low-Reynolds-number swimming in a capillary tube (2013, methodology): “As in many previous studies (Ishikawa et al. 2006; Ishikawa & Pedley 2008), we assume Bn = 0 for n > 2.”