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19 Oct 2013: Geophys. Astrophys.Fluid Dyn., 9, 185–200. Taylor, G. I. 1915 Eddy motion in the atmosphere.

3 Jan 2013: Sens. Actuators A133, 200–209. (doi:10.1016/j.sna.2006.03.010). 20. Jung K, Nam J, Choi H.

24 Apr 2013: Quasi-stationary space–time averages 〈 〉 were computedover 3000 successive simulation time-steps (t = 0.1) after an initial relaxationperiod of 200 characteristic time units tu = L 4/γ2.

26 Jul 2013: Optimal feeding is optimal swimming for all Péclet numbers. Sébastien Michelin1,a) and Eric Lauga2,b)1LadHyX – Département de Mécanique, Ecole polytechnique, 91128 Palaiseau Cedex, France2Department of Mechanical and Aerospace Engineering,

26 Jul 2013: Propulsion in a viscoelastic fluidEric Laugaa. Department of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge,Massachusetts 02139, USA. Received 20 March 2007; accepted 16 May 2007; published online 24 August

26 Jul 2013: 1 – 104 s1 No-slip –. GlassOTS Glycerol 95 50 – 200 nm LWater 100 50 – 200 nm L.

26 Jul 2013: Floppy swimming: Viscous locomotion of actuated elastica. Eric LaugaDepartment of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA. Received 5 October 2006; published 26 April 2007.

26 Jul 2013: Both the Ni and Au. segments have a diameter of 200 nm.

7 Jan 2013: We determined the temperature-dependent distributions of θfrom more than 200 scattering events by tracking the position of thecell body up to a distance of 70 μm from the corner (Fig.

4 Nov 2013: Reservoir. 25 cm. Glycerineax. q. 200 cm. FIGURE 5. Schematic of the experimental Hele-Shaw cell. ... Colour online) Sequence of photographs showing the progression of experimentB at dimensional times (a) t = 20 s, (b) 100 s and (c) 200 s.