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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:

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:.

25 Feb 2016: Shortly thereafter, Lighthill proposed a derivation which was accurate toorder 1/2.21,24 This was a vast improvement on the earlier methods but still did not account for theends of ... 2n̂. s. 1. O(b3), (24). R. 0. =b 1,bt̂ b2 21,b.

1 Oct 2016: For example, some eukaryoticmicroorganisms have evolved hairs along their flagella calledmastigonemes [23,24]. ... F(t ) = ζ. Udef ds = {0,0,0}, (24). L(t ) = ζ.

1 Oct 2016: The stresslet also controlsthe interactions of active organisms with their environment[21,22], enhanced transport through biological fluids[23,24], and the rheology of active fluids [25].If the stresslet of ... cζ dζ: ð26Þ. Using Eq. (24), the

12 Aug 2016: f 6 fbound = (1 n)1n(1 n)1nDmax as Re , (4.24). ... D = Dv = 24/3D. 1/3lamD2/3max O(Re8/3), Dm = 22/3D2/3lamD1/3max O(Re7/3), (4.34).

13 Mar 2016: Frontiers in Computational Neuroscience 7:24.

28 Jan 2016:

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.