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2 Sep 2012: 400 –200 200 4000 –40 –20 20 400. Position (μm). x (μm). ... 1). u the. ory. (μm. s–1. ). uNMR (μm s–1). –400 –200 200 400.

27 Dec 2012: Volvox is composed of thousandsof biflagellate somatic cells embedded in a sphericalextracellular matrix of radius R 200 m, beatingtowards the colony posterior with a nearly planar wave-form. ... gle. 15.00. 400. 200. 0. -400. -200. m/s. symplectic

2 Sep 2012: carteri using standard biological oxygen demand(BOD) bottles. We find Rb 50 –200 m. ... 2), viewedat 4 magnification on the stage of an inverted microscope(Nikon Diaphot 200).

19 Dec 2012: ήταν κατά 60% μεγαλύτερη απ’ αυτή που ζητού-σε το Μνημόνιο; Ας αναφέρω ακόμα μία από τις 200 ενέργει-ες του πρώτου Μνημονίου: «Ενας

2 Sep 2012: Figure 5(a) shows the. 0 50 100 150 200 2500. 50. ... 100. 150. 200. X (µm). Y (µm. ). FIG. 4. Flows at the bottom of a pendant drop.

3 Oct 2012: 1111. 2222. 3333. 4444. 5555CaClCaClCaClCaCl2222. 0 50 100 150 200 250 3000 50 100 150 200 250 3000 50 100 150 200 250 3000 50 100 150 200 250 300. ... 100100100100. 200200200200. 300300300300. 400400400400. 0. 100. 200. LaClLaClLaClLaCl3333. D(F=2 pN)D(F

2 Sep 2012: θ/. π. t/. (a). (b). (c). 200 400 600 8000.0. 0.1. ... M = 22.0M (mN-m). T/T. 0. 0 200 400 600 800.

2 Sep 2012: 0.0 75.0 150.0 225.0 300.0x[µm]. 0.0. 50.0. 100.0. 150.0. 200.0y[. µm]. ... than DD0 2;200 at Φ 10% (5.4 1010 cellsmL)for E.

19 Jan 2012: 1), manufactured inpolydimethylsiloxane by soft lithography [18]. Filamentswere studied near the stagnation point by epifluorescencemicroscopy with a 100 oil-immersion objective (numeri-cal aperture 1.4) on a Zeiss Axiovert 200

2 Sep 2012: 1), manufactured inpolydimethylsiloxane by soft lithography [18]. Filamentswere studied near the stagnation point by epifluorescencemicroscopy with a 100 oil-immersion objective (numeri-cal aperture 1.4) on a Zeiss Axiovert 200

28 Feb 2012: 200 and different values of αand ρ > 1. In each plot the bottom curve corresponds to n = 16, the next to n = 64,then n = 256 and finally n = 1024. ... 200 and different values ofα and ρ (0, 1). In each plot the bottom curve corresponds to n = 16, the

2 Sep 2012: R 200–400 m) there is the striking con-clusion that R; the Stokeslet dominates the flow field.It was therefore suggested [5] that suspensions of Volvoxwould be more similar to

28 Feb 2012: 0.0036. 0 200 400 600 800 1000 1200 1400. SimulationsLinear theory. ... 0.03. 0 100 200 300 400 500t. Max. imum. velocity. Fig.

16 Jul 2012: 2 = 73.45 were computed on a grid with mesh. size step h = 1/200. ... 21. Fig. 4.5. Noised (left), de-noised (center) and original (right) images, γ = 50, = 1e12, h =1/200.

3 Oct 2012: R. Querry, “Optical Constants of Water in the 200-nm to 200-micrometer Wavelength Re-gion,” Appl. ... Calibration was carried out at five different laser powers: 200 mW, 150 mW, 100 mW, 50 mWand 25 mW (top to bottom in Fig.

2 Sep 2012: a. eff. 04 nm (. M. 200) (Robinson & Stokes 1959; Fig.

2 Sep 2012: ARTICLE IN PRESS. 0022-5193/$ - se. doi:10.1016/j.jtb. Tel.: 1 314E-mail addr. 1The complem. similarly. Journal of Theoretical Biology 240 (2006) 288–301. www.elsevier.com/locate/yjtbi. Absorption by a moving spherical organelle in a

3 Sep 2012: Ni, using the standard electroformation method.22 Sucrose. solutions (50 mM and 200 mM) were used as the internal fluid.

28 Feb 2012: where α > 0 (Rainville 1960, p. 200). Lemma 2 The representation (1.2) for Laguerre polynomials is.

2 Sep 2012: grownfor 7 h on a rotary shaker (200 rpm) at 33 C.

1 Apr 2012: at speeds of 200–1000 f.p.s., and equipped with an SLR lens (Nikon 50 mm f/1.4).The drops were illuminated with a 19 cm inner diameter 22 ... We use a vapourdensity ρv = 1 kg m3 and viscosity µ= 3 105 Pa s appropriate for air at 200 C.Figure 8(a)

27 Jul 2012: DAMTP/91-1. Weyl Consistency Conditions and a Local Renormalisation Group Equation. for General Renormalisable Field Theories. H. Osborn. Department of Applied Mathematics and Theoretical Physics,Silver Street, Cambridge, UK. A local renormalisation

2 Sep 2012: Sokolov & Aranson (2009) measured the viscosity of a 200-μm-thick film of B. ... In this case, they waited until the velocity of thevortex was 200–500 μm s1 or smaller before analyzing the decay and extracting the viscosity.The delay in the

2 Sep 2012: Typical f luid velocities atthe free surface are in the range of 20 –200 ms, acceleratingas the meniscus slope increases near the contact line. ... Experimental observations and numerical results presentedare as described for Fig. 2, with A and A at

22 Mar 2012: I[f] =. 10. cos(x)eiωxdx, 100ω 200. Both methods have the same asymptotic order and use exactly the same in-formation; however as we can see fromFigure 1.1, the ... Figure 1.1: The error of the asymptotic method QA2 (right) and theFilon-typemethodQF2

27 Aug 2012: Eukaryotic flagella and cilia are much larger than bacterialflagella, with a typical diameter of 200 nm, and withan intricate internal structure [21]. ... A human spermatozoon with U 200 µm s1and L 50 µm moves with Re 102.

2 Sep 2012: 128.2. ( b ) w-7. 0.5 1 2. 2465 197.0 19.9 2467 197.3 20.1 2470 198.5 20.5 2476 200.5 21.3 2485

5 Sep 2012: Images were acquired at 40 fps in 2D (camera: Pike, AlliedVision Technologies), and 100 fps and 200 fps in 3D (camera: Phantom v9.1,Vision Research).

27 May 2012: recently because phylogenetic analyses indicate that mul-ticellularity evolved in volvocine green algae ‘only’approximately 200 million years ago [59], which is muchmore recently than in any other group, and inversionmust

2 Sep 2012: Dynamics of filaments and membranes in a viscous fluid. Thomas R. Powers. Division of Engineering, Brown University, Providence, Rhode Island 02912, USA. Published 19 May 2010; corrected 3 June 2010. Motivated by the motion of biopolymers and

19 Sep 2012: Movies S1 and S2 were 200–500frames long with a scan speed of 200 Hz (1 frame every 5.179 seconds).For simultaneous imaging of both microtubules and auto-fluorescent vesiclesoocytes

31 Oct 2012: Available online at www.sciencedirect.com. Physics Reports 386 (2003) 29 – 222www.elsevier.com/locate/physrep. Front propagation into unstable states. Wim van Saarloos. Instituut-Lorentz, Universiteit Leiden, Postbus 9506, 2300 RA Leiden, The

27 Aug 2012: Their mean diameters lie in the range from I to 200 jlm.

2 Sep 2012: 2tdt, where the finitetime difference dt is taken to be the longest time of themeasurements, 200 , t , 300 s.

22 Aug 2012: STRATOSPHERE-TROPOSPHERE EXCHANGE. James R. Holton • Peter H. Haynes 2 and Michael E. Mcintyre 2 Anne R. Douglass 3 and Richard B. Rood 3 Leonhard Pfister 4. Abstract. In the past, studies of stratosphere-tropo- sphere exchange of mass and

2 Sep 2012: It typifies many biflagellatedmicroorganisms with two anterior 10–12 m long flagellathat beat at 50–60 Hz propelling the cell in an oscillatorymanner at a mean speed of 100–200

5 Sep 2012: 100. 200. 300. 400. T. log. 10(G. E). Global errors of the method DSM11. ... DSM11. 100 80 60 40 20 00. 100. 200. 300. 400.

2 Sep 2012: relative Volvox carteri [18], aspherical alga (R 200 m) which swims by the action of103 Chlamydomonas-like cells on its surface.

2 Sep 2012: W. & McClelland, G. B. (1997) J. Exp. Biol. 200, 381–386.15. ... Exp. Biol. 200, 203–216.21. Norris, A. J., Martin, S. S., Harita, T., Nelson, J.

2 Sep 2012: c) Boundary layer scale near IZþ vs time forPe 0, 10, 50, 200, 103, 5 103, 2 104.