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19 Oct 2016: V 20 cRa. ). 17. Suspensions: what happened in parallel. ... producing 8 of his top 10 most cited papers. 20.

12 Aug 2016: 1 20 R. R. KERSWELL. and the conclusion that. i ( i a I.,) 2.

12 Nov 2016: 8. By considering the Fourier transform of the function. f(x) =. {cos x for |x| < π/20 for |x| π/2 ,. David Skinner d.b.skinner@damtp.cam.ac.uk.

11 Jan 2016: qcond = qadiabat qdiff , (20)and may be evaluated from the temperature gradient at the ICB,.

22 Oct 2016: Basic properties and related later work are highlighted in [20], see also[18, 23]. ... 12. Theorem 7.3. We have pP0. Vp(a) = σ̂(a). (7.2). For a proof see [34] or [20].

29 May 2016: This has been explained in detail in previous papers [18, 19, 20, 21, 22, 24].

12 Aug 2016: Angew. Math. Phys., 20 (1969), pp. 1–14. 10. [5] O. Dauchot and F. ... 20] F. Waleffe, Homotopy of exact coherent structures in plane shear flows, Phys.

2 Oct 2016: Bioconvection. Bioconvective Rolls. Slide Number 18. Classical Turing Patterns. Slide Number 20.

1 Apr 2016: e. b. f. 0 5 15 20 25wcrit. 0.1. 0.2. 0.1. ... 0.20. 0.25. ki. Time (s). Vort. ex s. pin 0. 1.

12 Aug 2016: DOI: 10.1103/PhysRevLett.105.154502 PACS numbers: 47.20.Ft, 47.20.Ky, 47.27.Cn, 47.27.nf. Shear flows are ubiquitous in nature and engineering,and understanding how ... Thereasons for this energy ‘‘gap’’ are unclear and leave open. 0 5 10 15 20

27 Oct 2016:  and P =1/2 0 1/20 1 0. 1/. 2 0 1/.

12 Aug 2016: As Re increases, these waves turn out to appear before the original less-symmetric TWs found in [4, 20]. ... Rev. Lett., 98, 204501, 2007. [20] H. Wedin & R.R. Kerswell, Exact coherent structures in pipe flow: travelling wavesolutions, J.

22 Jan 2016: It has previously been shownthat reciprocal swimming enhances diffusion [20], and thelast terms of Eq. ... Phys.Condens. Matter 23, 194119 (2011). [20] E. Lauga, Enhanced Diffusion by Reciprocal Swimming,Phys.

1 Oct 2016: The resulting flow fields can be used to probe properties of both theswimmer and fluid, providing new insights into the physics of undulatory propulsion [11–15,18–20]. ... The depth offocus of the objective is approximately 20 μm, and we ensure that

22 Feb 2016: Fluid Mech. 1994. 0. 20. 40. 60. 80. 100. 0 0.5 1 1.5 2. ... 1. 2. 3. 4. 5. 6. 7. 8. 10 20 30 40 50 60.

22 Feb 2016: 20. Flow past a sphere Lagrangian unsteady. Numerical Oldroyd-B. DragStokes. Uτ/L. ... a. 1e-05. 0.0001. 0.001. 0.01. 0 5 10 15 20. t.

2 Nov 2016: First, the multilevel samplingstrategies we introduced have been extended to block sampling strategies [10, 12, 20, 21], which are morepractical for applications such as MRI.

1 Oct 2016: Detailed studies exist on rats [14, 15], mice[16], porcupine [17], wild boar and pig [18], and humans [19,20]. ... u(y) VWL. H2 (20). Using Equation (16), we thus obtain a typical deflection.

1 Oct 2016: The two commonly used theoriesare resistive-force (or local-drag) theory, which is analyticalbut only logarithmically correct [2,19,20], and slender-bodytheory, which has to be implemented numerically in generalbut ... R(t )1L ={ L. 33 L31. L33 L31ω,0,0.

1 Oct 2016: Kessler, Phys. Rev. Lett. 93, 098103 (2004).[20] A. Sokolov, I. S.

13 Dec 2016: anddriven by feedback-controlled time-shared (20 kHz) optical tweezers (OTs) based on acousto-opticaldeflection of a 1064-nm-wavelength diode-pumped solid-state laser (CrystaLaser IRCL-2W-1064)as previously ... The oscillators are imaged using a Nikon

2 Nov 2016: 2h1. x2. )3, (20). where A, B, C, and D are heuristic parameters of the model. ... 0 20 40 600. 10. 20. ||h1-h2||. =0.05=0.10. =0.20. 2. FIG.

11 Oct 2016: Landau level. The wavefunction (1.20) depends on two quantum numbers, n and k but. ... in the presence of magnetic fields. – 20 –. Total number of states with energy En is.

3 Oct 2016: 5]. PACS numbers: 87.22.Bt, 47.20.Hw, 68.10.Cr, 82.65.Dp. ]. r-ve. pe. in. r-gs. ... Martinot-Lagardeet al., Ann. Phys.(France)20, 127 (1995). [7] See, e.g., H. Flyvbjerg, T.

26 Feb 2016: A stereo pair containing two 120 120 pixel images wasgenerated in which 20% of pixels were set to black. ... 11. -10.5. -10. -9.5. -9. -8.5. -80 -60 -40 -20 0 20 40 60 80.

12 Aug 2016: where. (2.19). (2.20). (2.21). 9; = (9:), and with quadratic and higher terms in p neglected. ... fin, h,,,p",,] = [ f i , ( ) , h , ( ) , j , ( ) ] eintim@-(l-R)'s(s), (3.20).

27 Jan 2016: Spain.07/09/2009-11/07/2009 LOC of the LISA AstroGR Barcelona. Spain.16/06/2008-20/06/2008 LOC of the 7th International LISA Symposium.

1 Nov 2016: 2. The solid curve corresponds to configurations shown in (a) and (b) with collar openingangle 20. ... Streamlines are calculated in the swimming frame from y = 20 μm, z = 0.1 μm and projected onto thez = 0 plane.

12 Aug 2016: δu π〉. (20). Combining all these gives. T. 0. 〈. δG. δu δu. 〉. = 〈δu(x, T ) {u(x, T ) ν(x, T )}〉. 〈δu(x, 0) {λu(x, 0) ν(x, 0)}〉. T.

1 Oct 2016: 0. 20. 40. Vel. ocity. mag. nitu. de(μ. m/s). FIG. 6. ... x (μm). x (μm). y(μ. m). y(μ. m). 10. 20. 30.

4 Mar 2016: The. results, which can be found in several articles,9,19,20 are writ-. ... 12) and(19) to get the results Eqs. (13) and (20). The second part of.

12 Aug 2016: 15. 20. 25. 30. 35. 40. 45. 50. 0.25. 0.30. 0.35. ... 0.1 or 0.2 units in time (which is anything from 20 to 100numerical time steps).

6 Oct 2016: 1. number of attacked sensors (q). frac. tion. fraction of initial conditionsrecovered in less than 20 steps. ... 2. IEEE 14-bus power network [9]. 5 10 15 20 25 300.

3 Oct 2016: 4 Jing Gao and Arieh Iserles. Fig. 1 The left: the interpolation points of (5) with s = 5, k = 1, ,4, θ = 15 and ω [0,20];The right: the logarithm ... The error (to logarithmic scale) is displays separately for ω [0,20] andω [0,200].

2 Nov 2016: First, the multilevel samplingstrategies we introduced have been extended to block sampling strategies [10, 12, 20, 21], which are morepractical for applications such as MRI.

18 Feb 2016: Jupiter’s Unearthly Jets: A New Turbulent Model Exhibiting StatisticalSteadiness without Large-Scale Dissipation. STEPHEN I. THOMSON1 AND MICHAEL E. MCINTYRE. Department of Applied Mathematics and Theoretical Physics, University of Cambridge,