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19 Aug 2011: 1 10-6. 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200. ... 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200.

3 Jun 2024: Martin and M. J. Simons, pp. 235-250. Kluwer, Dordrecht (2002). 200.

13 May 2014: 1 10-6. 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200. ... 1.5 10-6. 2 10-6. 0 200 400 600 800 1000 1200.

1 Dec 2023: 4. |Q| (. m/s. ). 10-3. 0 200 400 600 800 1000t (s). ... 0 50 100 150 200. 2. 2.5. 310-3. |Q|. (ms. 1).

13 Dec 2018: ample, without further approximation, evaluation for a. scatterer of around 200 by 60 wavelengths can be car-.

25 Jan 2007: 200. 6 U. nive. rsity. of C. ambr. idge. Not. to b. ... Λa b =x̃a. xb. (113). 23. Cop. yrig. ht. 200. 6 U.

19 Aug 2021: Numerical Balancing Act: Magnetic Graphene. B. 0 200 400 600 800 1000. ... 0. 100. 200. 300. 400. 500. 600. 700. 800. 900. 1000.

10 Apr 2011: Chloroplasts. Indifferent zone. 400. 200. y (μ. m). x (μm). 0. ... 0 200 400–200–400. –200. –400. (b) (c). Figure 1. (a) Internode ‘stalks’ of the Chara Corallina algae consist of single,millimetre-diameter and 10 cm long cells.

22 Jul 2014: 0. 50. 100. 150. 200. 250. 300. 350. 400. 450. 500.

18 May 2022: placed on the wafer using dou-ble layer of Parafilm strips as spacer (total thickness: 200 µ m,Bemis). ... S150B). A(25 x 25) mm glass slide was plasma treated (O2, 40 mL/min,200 W, 5 min, PVA TePla 100) and a droplet of 714 g/L solu-.

31 May 2024: 5.73). – 200 –. We see that the three lines don’t meet.

16 Jan 2005: Firstly, to elucidate the stages of the secondary folding we consider a sequence of fiveamino acid regions each of length i = = 200 in our nondimensional units. ... 0 50 100 150 200. 5. 10. 15. 20. the nonlinear Schrödinger equation.

24 May 2016: Selective deformation of soft continuous microscale bodiesWe fabricate LCE microrobots in the form of long cylinders (about1 mm in length and 200–300µm in diameter), and flat discs (50µmthick and either ... Themixture is then ultraviolet-cured

22 Jul 2014: 12,200 houses; 40% affordable. • Thriving & accessible historic core. •

26 Jul 2013: 1 over 200 s. For these three cases (no swimming,steady swimming, and reciprocal swimming), we also plotas straight lines the theoretical prediction [where D isgiven, respectively, by DkBT, Eqs. ... 1 (averages of 500realizations over 200 s). Top to

26 Jul 2013: 3–200 s [Fig. ... h20. [17] Interestingly, for real spermatozoa, the swimming speedis only a fraction of the actuation speed of its flagel-lum (swimming at about 100–200 m=s with a30–60

3 Feb 2013: The second piece of history that I need to tell you about is from 200 years earlier. ... Newton’s theory had lasted more than 200 years. But Einstein was puzzled.

25 Jun 2004: The results for thedynamics of the vortex line length for three sets of compu-tations withNrare= 0 , 100, and 200 are plotted in Fig. ... Initially the number of rar-efaction pulses isNrare= 200 (green or light gray line).

12 Nov 2009: R = 200 mm,h = 15 & 7 mm,η0 = 1 mm,λ = 50&70 mm,d = 0.5 mm,µ = 0.05 & 1 Pa s. ... L = 2 m, h = 11 & 16 mm, U0/ω 200 mm.

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.

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].

26 Sep 2010: 0. 50,000. 100,000. 150,000. 200,000. 250,000. 300,000. 350,000. 400,000. 450,000. 2009. ... 0. 20,000. 40,000. 60,000. 80,000. 100,000. 120,000. 140,000. 160,000. 180,000. 200,000.

6 Oct 2020: least 200 min. We used custom-written MATLAB scripts to analyze these tracks. ... R2 = 0.001. µ. µ. 0 100 200 300. Time from birth (min).

17 Mar 2010: ω = 200, N=1200. 0 500 1000 1500 2000 2500 3000 3500 40000. ... Figure 6. The spirals v[N](T) for N = 500, ω = 100 andω = 200.

26 Jul 2013: 200. 0 20 40 60 80 100. 0. 5x101. 1x102. 1.5x102. ... 200. 0 5x107 1x108 1.5x108 2x108. Mean. distan. ce. Mea. nd.

29 Jan 2023: Witten. – 200 –. In summary, the low-energy physics of the bosonic string in D1 dimensions consistsof a metric Gµ, two U(1) gauge fields Aµ and õ and two massless scalars

22 Jul 2014: Providing aerospace engineers since the 1960’s. During the last few months we have reviewed over 200 applications for 11 apprentice positions.

3 Sep 2009: 9. Fluid Dyn. Res. 41 (2009) 051403 N G Berloff. t=0 t=200. ... 12. Fluid Dyn. Res. 41 (2009) 051403 N G Berloff. t=0 t=200.

10 Apr 2011: 2, 3, 5 for 0 = 3.8, D0 = 50, = 3, v0 = 0.2, = 3, = 0.5 in the periodic domain of 200 200 units.

29 Apr 2022: A.Arjes, L. Tsimring, and G. M. Süel, Species-independentattraction to biofilms through electrical signaling, Cell 168,200 (2017).

14 Nov 2019: U = 1. 1µc(1, µ)dµ =. k13. =14. (22). The series solution for the concentration converges suf-ficiently quickly for a quantitative comparison, howevereven with 200 non-zero coefficients the analytical

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

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

10 Apr 2011: on. July. 24,. 200. 9 w. ww. sci. ence. mag. org. ... July. 24,. 200. 9 w. ww. sci. ence. mag. org. Dow.

26 Jul 2013: difficult tosolve and double-precision arithmetic (the default precision in Matlab) becomesinadequate above Re 200.

9 Nov 2019: 90 0-40-0-500-80-0-90 0-30-0-400. 70-0-80 0. 20-0-300-60-0-70 0-10-0-200-50-0-60 Below 0.

19 Nov 2007: 0.742 0.789 0 < t < 200. Slow logarithmic approach also in experimental data.

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

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

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].

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.

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.

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

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

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],

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

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

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

26 Mar 2010: N = 100 , 200 , 400 , 800. VnN1/6. 0.