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3 May 2017: 0. 10. 20. 30. 0. 10. 20. 30. 200 300 400 500 600. ... 200 300 400 500 600 200 300 400 500 600. 500 600 700 800 900.

1 Aug 2008: 2. 0 200. 50. 2. 1. 2. 1500. 1. 0. 200100 50 1500.8. ... left), c = [1,. 77 ,. 7. 7 , 1], m = [2, 1, 1, 2] (right) andω [0, 200].

2 Jul 2024: 6.1.4 Bound States 200. 6.1.5 Resonances 202. 6.2 Scattering in Three Dimensions 206.

14 Jun 2014: fixr0.5_0.7_n_100_rep1.crc.last.ps fixr0.5_0.7_n_200_rep1.crc.last.ps. fixr0.5_0.7_n_300_rep1.crc.last.ps

6 Jul 2020: The wall has a tough outer layer abovea region of cellulose fibrils [26–28], with a thicknessd 200–400 nm: AFM studies [12] show a Young’smodulus E 1 MPa.

13 Oct 2017: Similar relations are not known for theWalsh wavelet case. 0 200 400 600 800 10000. ... 200. 400. 600. 800. 1000. 1200. 1400Slope 1.249. (A) Θ(N; 5) for DB2 with NmaxMmax. =

8 Jul 2021: J. Fluid Mech. (2021), vol. 914, A20, doi:10.1017/jfm.2020.1112. The fluid dynamics of collective vortex structuresof plant-animal worms. George T. Fortune1, Alan Worley2, Ana B. Sendova-Franks2, Nigel R. Franks2,Kyriacos C. Leptos1, Eric Lauga1 and

22 Jul 2014: Energy: Cambridge has over 200 energy researchers working on technology and policy.

11 Apr 2007: 22, xR2, and when the current simplex has the vertices. x0 =. (. 1980.1. ). , x1 =. (. 2000. ). and x2 =. (. 1992.1. ). (2). The values F (x0) = 1982 1, F (x1) = 200. ... Let us assume there are about 1018 different numbers in the interval[10, 101],

22 Jan 2016: v p(µ. m/s. )0 100 200. Area (µm2 ). 0. 10.

5 Mar 2021: J. Fluid Mech. (2021), vol. 914, A20, doi:10.1017/jfm.2020.1112. The fluid dynamics of collective vortex structuresof plant-animal worms. George T. Fortune1, Alan Worley2, Ana B. Sendova-Franks2, Nigel R. Franks2,Kyriacos C. Leptos1, Eric Lauga1 and

4 Feb 2020: 2•. 0.05 -. 0.00. 200 • 600 000 10•0 1200.

13 Dec 2018: Math. 50 (1985),. 193-200. DEPARTMENT OF APPLIED MATHEMATICS AND THEORETICAL PHYSICS, UNIVERSITY OF CAMBRIDGE, CAMBRIDGE CB3 9EW, UNITED KINGDOM.

26 Jul 2013: System size R 250–800 µm 0.3–7 µm 6–12 mm 30 µm 40–200 nm. ... Slip length λeff 2–8 µm 20–90 nm 200–450 µm 1 µm 10–30 nm.

17 Sep 2015: Electrodes were aligned in asquare array, spaced 200 um apart.). 1.

23 Apr 2021: characteristic scale of the strong interactions, QCD 200 MeV. Three of the quarks have masses smaller than QCD. ... QCD 200 MeV than to mup and mdown, which are a few MeV.

10 Apr 2011: Scales are 200 m. (d) Alinear Volvox cluster viewed from above (scale is 1 mm).

3 Oct 2016: of the error of both Filon methods, (3) (green) and (5) (black), for f (x) =(1 x x2)1, g(x) = x, s = 2 and ω [0,200]. ... The error (to logarithmic scale) is displays separately for ω [0,20] andω [0,200].

19 Jul 2013: ω2. )rather than O. (ω1. ). 11. Figure 3.2: |p0(t) y(t)| for ω = 12.5, 50, 200. ... Figure 3.3: |p0(t) p1(t,ω) y(t)| for ω = 12.5, 50, 200.

10 Apr 2011: 6b reveals a peak of 800 ms for acolony of radius 200 m. ... Movies acquired with ananalog charge-coupled device camera (SSC-M374, Sony; 480 640 pixels) consisted of 1,000 images taken at 30 frames pers, averaged over 200 frames.

17 Jan 2021: negligible load [21], whilecargo speeds on oocyte MTs are 200–500 nm=s [14,29,50].Assuming a linear force-velocity relation and a stallforce of 6 pN [21] give a

1 Dec 2023: Journal of Glaciology, 56(200), 1104–1114.Jenkins, A., Dutrieux, P., Jacobs, S. S., McPhail, S.

24 Aug 2007: 100 200 300 400 500 600. 500. 1000. 1500. 2000. 2500. ... T /Tλ. 0 200 400 600 8000. 100. 200. 300. 400.

23 Jul 2016: It is evident that Fourier spectral collocation method is superior. (a) M=200 (b) M=400 (c) M=800. ... Symmetric and arbitrarily high–order time–stepping methods 27. (a) M=100 (b) M=200 (c) M=400.

3 Jul 2024: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2013. Dynamics and RelativityUniversity of Cambridge Part IA Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,.

28 Mar 2014: 200. 250. 300. 350. 400. 450. y/L. vert. ical. flow. rat. ... 104. 102. 100. 0. 100. 200. 300. 400. 500. bending rigidity, B=EI, Pa m4.

10 Apr 2011: 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.

13 May 2009: This behaviour can be expected, since large values of. 23. 0 5 10 15 200. ... 5. 10. 15. 20. 25. 30. 35. 40. α. β. 0 5 10 15 200.

19 Oct 2013: British Higher Education Policy in the last Twenty Years: The Murder of a Profession. Richard F. Gombrich. Tokyo, January 2000. Preamble. This is the text of a lecture I gave on 7 January 2000 in Tokyo at the Graduate Institute of Policy Studies

26 Jul 2013: line. The values of Gmaxare 10, 100, 200, 300, and 400 from the outer to the inner curve.

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

10 Apr 2011: The Atmosphere During the Younger Dryas [pp.195-197]. A 50,000-Year Record of Climate Oscillations from Florida and Its Temporal Correlation with the Heinrich Events [pp.198-200].

31 May 2024: Preprint typeset in JHEP style - HYPER VERSION Michaelmas Term, 2019. General RelativityUniversity of Cambridge Part III Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,.

22 Jul 2014: 0. 50,000. 100,000. 150,000. 200,000. 250,000. 300,000. 350,000. 400,000. 2011 2015 2021 2025 2031.

5 Oct 2013: 50 100 150 200. 10-10. 10-7. 10-4. 0.1 50 100 150 200. ... 10-14. 10-11. 10-8. 10-5. 0.01. 10. 50 100 150 200. 10-14.

10 Apr 2011: relative Volvox carteri [18], aspherical alga (R 200 m) which swims by the action of103 Chlamydomonas-like cells on its surface.

1 Dec 2023: roughly 1–5 m deep) than the formation itself (roughly 200 mdeep) (Bickle et al.

13 Jan 2021: negligible load [21], whilecargo speeds on oocyte MTs are 200–500 nm=s [14,29,50].Assuming a linear force-velocity relation and a stallforce of 6 pN [21] give a

26 Jul 2013: the porous alumina membrane template containing 200 nm-diameter cylindrical pores (Catalog No 6809-6022; Whatman, Maidstone, UK) to serve as a working electrode. ... An open channel of 200 μm wide and 10 mm in length was used to properly visu-alize the

27 May 2019: 0.1. 0.2. 0 0. 0.05. e. 2. 60 300 200 100 0 1000. ... babi. lity. 20. 0 5 10 15 200. 0.02. 0.04. 0.06.

26 Jul 2013: 200. 400. 600. 800. 1000. 1200. 1400. φ3/π. -•o. φ2 = 0φ2 = π/6φ2 = π/2φ2 = 2π/3φ2 = 5π/6. ... 200. 400. 600. 800. 1000. 1200. 1400. FIG. 12. (Color online) Evolution of the rate of energy dissipationwith φ3 for different values of φ2.

13 Dec 2018: 0 50 100 150 200 250 300. x. 0.3. 0.2. 0.1. ... 0 50 100 150 200 250 300. x. 0.2. 0.1. 0.0.

7 Sep 2006: 0 100 200 300 400. 50. 100. 150. 200. 250. p1 p2. ... 100 200 300 400 500 600. 100. 200. 300. 400. 500.

27 Sep 2005: 1-3. 0 100 200 300 400. 50. 100. 150. 200. 250.

7 Jun 2021: 2 A First Look at Quantum Fields. In this section we look in more detail at some of the key features of quantum fields. and their interactions. We illustrate these properties with the simplest quantum force,. electromagnetism. Or, to give it its

31 May 2024: Preprint typeset in JHEP style - PAPER VERSION June 2005. TASI Lectures on SolitonsInstantons, Monopoles, Vortices and Kinks. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,

1 Dec 2023: Dewatering of fibre suspensions by pressure filtrationDuncan R. Hewitt, Daniel T. Paterson, Neil J. Balmforth, and D. Mark Martinez Citation: Physics of Fluids 28, 063304 (2016); doi: 10.1063/1.4952582 View online:

10 Apr 2011: 200 M. Lombardi, C. P. Caulfield, C. Cossu, A. I. Pesci and R. ... Results for Rein = 0.05, Sc = 667 andGr = 49.05 for (a) the base flow and τ = (b) 133.67, (c) 200.33 and (d ) 250.33.

14 Feb 2019: How do we address that? The landscape has changed over the last 200 years.

12 Aug 2016: Lecture 8: Edge Tracking – Walking the Tightrope. Rich Kerswell. In the subcritical transition scenario, there is typically a regime where the linearly stablebasic state coexists with the turbulent state. The simplest model of this is a 1D