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12 Aug 2016: 200. 220. 240. 260. 280. 300. 320. 340. 0 50 100 150 200 25010-12. ... 10-5. 10-4. 10-3. 10-2. 10-1. 100. 0 50 100 150 200 250 300time (D/U).

24 Oct 2016: 20 15 10 5 0 5 10 15 200. 0.1. 0.2. ... 0.016. 0.018. 0.02. (a) Original Coherences. 0. 50. 100. 150. 200.

1 Jun 2016: 16. 14. 12. 10. 8. 6. 4. 2. 040 80 120 160 200 240. ... 200. 0. –200. –40024 ms. (a) (b). (c). FIGURE 4. Experimental flow fields.

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

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].

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.

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

11 Jan 2016: 0 100–100 200–200 300–300 400–400. 6. 2. 0. 4. 0.5. 0. ... 0 100–100 200–200 300–300 400–400. 15. 20. 5. 0. 10. 15.

24 Oct 2016: 20 15 10 5 0 5 10 15 200. 0.1. 0.2. ... 0.016. 0.018. 0.02. (a) Original Coherences. 0. 50. 100. 150. 200.

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

11 Jan 2016: Inlet. Outlet. Glycerine. 200 cm. Air6 cm 14 cm. FIGURE 10. ... predictions. Our experiments were performed in a Hele-Shaw cell composed of twoacrylic sheets, each 200 cm long and 14 cm high (see figure 10) and spacing w 0.38

6 Oct 2016: For this. 0 5 10 15 200. 0.2. 0.4. 0.6. 0.8. ... Fordifferent values of q between 1 and 34, we ran 200 simulationswith different sets of attacked sensors K of cardinality q, anddifferent initial conditions x(0).

3 Oct 2016: b) A membrane extension drawn from afluctuating vesicle using optical tweezers (830 nm single-moddiode, 200 mW).

1 Oct 2016: Other measurements reports significantly larger sizes, withwidths that can range 100–300 µm and length 200–500 µm[21, 23, 24]. ... pp. 1171–200. 26. Berdyyeva TK, Woodworth CD, Sokolov I. Human epithelial cells increase.

1 Apr 2016: 0 0.5 1-0.5-1Mean vortex spin. 0. 100. 200. 300. Freq. uenc. ... 1Stag. gere. dvo. rtex. spin. t = 50 t = 100 t = 150 t = 200 t = 250 t = 300.

12 Aug 2016: Finally, anasymptotic regime is approached for Re & 50. The preliminary calculations performedhere for 100 < Re < 200 tentatively support the asymptotic scaling laws D Re1/2and U :=2E Re2/5 although the ... Re. 0.5. 0.6. 0.7. 0.8. 0.9. 1.0. 50 100 200. 0.

1 Apr 2016: graphene. Nature 438, 197–200 (2005).25. Drut, J. E. & Lähde, T.

13 Dec 2016: Using the average values Ā and ̄ for t > 200 s[Figs.

26 Feb 2016: 0.6. 0.7. 0.8. 0.9. 1. 0 100 200 300 400 500 600 700.

19 Oct 2016: Comput. Phys. 200,. 299 (2004).[14] W. H. I. Meeks, The classification of complete minimal surfaces in R3 with total curvature greater than.

6 Oct 2016: For differentvalues of |K| (number of attacked sensors) and |L| (numberof attacked actuators), we ran the decoder on 200 differentinitial conditions and attack sets and we recorded the successrate of the

6 Oct 2016: I Used 1/2 decoder. 0 5 10 15 200. 0.2. 0.4. ... For each value of q, 200 simulations were carried out. with different initial conditions and different sets of attacked sensors.

18 May 2016: Coordinated beating of algal flagella is mediated bybasal couplingKirsty Y. Wana and Raymond E. Goldsteina,1. aDepartment of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, United Kingdom. Edited by Peter Lenz

11 Jan 2016: Thermal conductivity k W m1 K1 36 – 200 Stacey & Davis (2008); de Koker et al. ... For ex-ample a thermal conductivity of 200 W m1 K1 requires QCMB 32 TW for the inner core to be thermally unstable (̄ > 0) andconvect.

20 Jul 2016: ωMethod 0 100 200 300 400 500. Fig. 1.1 9.2102 1.4207 9.0209 1.8009 5.6710 2.2910Fig.

22 Sep 2016: 140 000. 160 000. 180 000. 200 000. 00 2 4 6 8 10.

24 Nov 2016: b)(a). 500. 0. 500. y (. m). (c). 0 50 100 150 200.

21 Jan 2016: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

8 Mar 2016: Cop. yrig. ht. 201. 6 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Prepared for submission to JHEP. Supersymmetry. B. C. Allanacha F. Quevedoa. aDepartment of Applied Mathematics and

25 Feb 2016: PHYSICS OF FLUIDS 28, 013101 (2016). Slender-ribbon theoryLyndon Koens. a). and Eric Lauga. b). Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Wilberforce Road, Cambridge CB3 0WA, United Kingdom. (Received 20 May

21 Jan 2016: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

10 Nov 2016: The Evolution of Silicon Transport in Eukaryotes. Alan O. Marron,1,2 Sarah Ratcliffe,3 Glen L. Wheeler,4 Raymond E. Goldstein,1 Nicole King,5 Fabrice Not,6,7. Colomban de Vargas,6,7 and Daniel J. Richter5,6,71Department of Applied Mathematics and

2 Oct 2016: Annu. Rev. Fluid Mech. 1995. 27: 169-93 Copyright 1995 by Annual Reviews Inc. All rights reserved. CONSTITUTIVE EQUATIONS FOR. POLYMERIC LIQUIDS. R. Byron Bird. Department of Chemical Engineering and Rheology Research Center, University of Wisconsin,

12 Aug 2016: For the Earth,. 115. 1 200. R, = 4 x 10 - << q x - << 1,.