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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,

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.

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.

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.

1 Jul 2016: Equation (6) givesthe spatial part of the Lagrangian for a scalar ϕ4 theory onthe circle [24,25], and ϕ may be thought of as analogousto the field u in the SSH ... Acad. Sci. U.S.A. 111, 13004 (2014). [24] N. S. Manton and P.

12 Aug 2016: Formally, the appropriate hydromagnetic inner product (i.e. the modified version of (2.24) taking account of the dipolar field) is required here to suitably weight the momentum and induction equations. ... 2 2 ). ( 3. 2 3 ). (3.24). so that the normal

1 Apr 2016: 8, 899–911 (2013).24. Novoselov, K. S. et al. Two-dimensional gas of massless Dirac fermions in.

1 Jul 2016: Electrostatic anchoring on a specialized con-trolled surface allows selective control among identicalrobots by preventing motion [24]. ... J. Nelson, Adv. Mater.24, 811 (2012). Copyright 2012, WILEY-VCH VerlagGmbH & Co.

28 Jan 2016:

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).

1 Oct 2016: coli swarm near its advancing edge revealed that the top swarm-air surface isin fact stationary [24]. ... ρ = ξ‖ξ. = 1γ1. = 0.4, (24). 043202-8. FLAGELLAR FLOWS AROUND BACTERIAL SWARMS.

20 Jul 2016: s ν d The constant. 4 2 16 2.43173 18 8.83214 20 3.06245 22 9.83286 24 2.8731. ... Numer. Anal. 24(3), 365–391. Iserles, A. & Nørsett, S. P. (2004), ‘On quadrature methods for highly oscillatory integrals.

24 May 2016: future. Soft Robot. 1, 5–11 (2013).24. Kim, S., Laschi, C. & Trimmer, B. ... Adv. Mater. 24, 2710–2714 (2012). 46. Zeng, H. et al. High-resolution 3D direct laser writing for liquid-crystallineelastomer microstructures.

28 Jan 2016:

29 May 2016: This has been explained in detail in previous papers [18, 19, 20, 21, 22, 24].

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