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1 Oct 2016: Other measurements reports significantly larger sizes, withwidths that can range 100–300 µm and length 200–500 µm[21, 23, 24]. ... hydrodynamics and flow sensing. Annu Rev Fluid Mech. (2016) 48:1–24. doi:.

18 Feb 2016: Manuscript received 9 December 2014, in final form 24 September 2015).

25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Flagellum: organellecomprising the rotarymotor, hook, andfilament. ... sona. l use. onl. y. FL48CH05-Lauga ARI 24 November 2015 12:50.

12 Aug 2016: for m0 = 3 at (M, N, L) = (8, 24, 5) and α = 2.44. ... 18. Figure 6. The continuation curve for m0 = 3, α = 2.44 at Re = 2200 (Acrit = 1.182 104,truncation (8,24,5)).

22 Jan 2016: algae ingravitational fields [22] and can be treated analytically [23].However, the present internal torques can be treatedanalytically only in two dimensions [24] and numerical[25] or approximative [26] methods are ... 24] S. van Teeffelen and H. Löwen,

28 Jan 2016:

13 Dec 2016: Many surrogate models for flagellar dynamics have been proposed [13–24],typically with a set geometry that fixes the range and coupling between oscillators. ... R. Soc. Interface 10, 20130571 (2013). [24] I. Kavre, A. Vilfan, and D.

6 Oct 2016: i. |hi|2. where := cos(π/N) x F(N,C). 15 / 24. ... and the sos hierarchy needs only dN/4e levels. 24 / 24.

1 Oct 2016: In order to solve Eqs. (1) in the fluid surrounding the nematode, we employ the regularizedstokeslet boundary element method [23,24]. ... Analysis, validation, and application to helical swimming, Phys. Fluids 17, 031504 (2005).[24] D.

2 Nov 2016: large. However, it is well knownthat use of the leading-order approximation of slender body hydrodynamics for larger values of isrobust [24,25]. ... A(τ ) =(. Be2(2k2k4 )τ 3k. 4. 4(2 k2))1/2. (24). 073201-8.