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16 Jul 2018: a cell with flagellar filaments undergoing normal CCW rotation) with two different hook stiffnesses over a time scale t = 200 (time nondimensionalised by the rotation rate of the flagella). ... stiff hook. (A) Initial position and conformation of each

3 Apr 2018: 0. 0.5. 1. x. VD. VD/200. |u0||uD(T)|. 5 0 50.5. 0. ... 0.5. 1. x. VS. VD/200. |u0||uS(T)|. 5 0 50. 0.5. 1.

18 Nov 2018: Introduction Schrödinger and PDEs Discrete operators Numerical Examples Conclusion Definitions. The Computational Spectral Problem. and a New Classification TheoryNovel Algorithms, Impossibility Results and Computer Assisted Proofs. Matthew

16 Nov 2018: Introduction Schrödinger and PDEs Discrete operators Numerical Examples Conclusion Definitions. The Computational Spectral Problem. and a New Classification TheoryNovel Algorithms, Impossibility Results and Computer Assisted Proofs. Matthew

14 May 2018: the contrary. – 149 –. scale at which QCD becomes strongly coupled is 200 MeV.

27 Nov 2018: 5(f). FIG. 7. The concentration field in a channel with width3.125 < Ls = 5.5 at times t = 0, 100, 200, 300 for (a) neutral, (b)puller, and (c) pusher ... FIG. 8. The concentration field under an imposed chemoat-tractant gradient in a channel with width 3

8 Jan 2018: m0 20 40 60 80 100 120 140 160 180 200 2200. ... al. (2010), the boundary region studied is x [200, 400], where the leading edge is at x = 0and the evolving disturbance is forced to vanish at .

27 Feb 2018: Concentrationc L. 0 100 200 300Time t. 0.0. 0.1. 0.2. 0.3.

2 Nov 2018: Opt. Commun. 200, 321–330. Berry, M., Storm, C. & Saarloos, W.

17 Apr 2018: Orthogonal systems with a skew-symmetric. differentiation matrix. Arieh IserlesDepartment of Applied Mathematics and Theoretical Physics. Centre for Mathematical SciencesUniversity of Cambridge. Wilberforce Rd, Cambridge CB4 1LEUnited Kingdom.