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10 Apr 2011: Bt/JI= M , (24) t/JI Bt/J t/J(Mn). and a further differentiation then gives. ... 0.6. xc. 0.5 ---- --------Xc«Mn)a CXl)---------. 0.4. 0.4 0.5 0.6. ka T lu.

24 Apr 2014: and is characterized by four non-dimensional numbers:. Pe= kBTAλ2a. ηf D2, Da= Ka. ... c̃1ρ+ c̃1 φ̃0. ρ=(c c̃0)φ̃1. ρk(ζ)Da k(ζ)c̃0. (3.24). Phoretic self-propulsion at finite Péclet numbers 581.

24 Dec 2014: Emacs Lisp List. Last updated: Wed Dec 24 11:36:00 2014. 1270 entries. ... Sat 24 Jun 2006. Update ell.el to point to ELL at Cambridge.

25 Sep 2015: FL47CH15-Goldstein ARI 1 December 2014 20:34. Green Algae as ModelOrganisms for BiologicalFluid DynamicsRaymond E. GoldsteinDepartment of Applied Mathematics and Theoretical Physics, Centre for MathematicalSciences, University of Cambridge,

12 Aug 2016: 1.24). The reader should note that the original geometry has been recovered in the limit ,u << 1. ... With no precession, (1.22)-( 1.24) is the normal mode problem for a uniformly-rotating basic state within a spheroidal container.

14 Feb 2005: Suppose there exists an engine I which is. 3 THE GRAND CANONICAL ENSEMBLE 24.

6 Oct 2014: components, the possible holonomy groups of these irreducible non–symmetric. Riemannian manifolds have been classified by Berger [24]. ... τ := ξA′(dξA. ′ ξB. ′ΓA. ′B′. ). (2.24). Using τ, we can lift the vector fields ξA′AA′ to F

28 Oct 2006: 1.7.13 Aide Memoire. 24. 2 Partial Differential Equations 25. 2.0 Why Study This? ... You should be able to do example sheets 1/2/3/4 after lectures 6/12/18/24 respectively.

7 Oct 2014: tred around the concept of symmetry reduction. It was noted by Richard Ward [24].

7 Jan 2013: Photosynthetically Active Radiation (Fluora; OSRAM) and 10 h in dark at 24 C.Cells were harvested during the exponential growth phase. ... Phys Rev Lett 105(16):168101. 17. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by

30 Nov 2015: 2.3 Self-adjoint differential operators 22. 2.4 Eigenfunctions and weight functions 24. ... 1)k1. ikeikθ (1.24). do in fact converge on the sawtooth function everywhere except at the discontinuity.

3 Oct 2008: 24. the three coordinate directions. They span a parallelepiped of volume.

5 Dec 2007: Conditions in the outer flow, including the boundary conditions, can be chosen in a special way (Warn & Warn 1978, 56; (2.24) below) such that the changes induced in the outer ... 2.24) jl,n being the nth zero of the Bessel function J1.

31 May 2023: qg = 2πn with n Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2πn with n Z. This, of course, is the Dirac quantisation condition (1.24).

1 Sep 2011: 242.3.3 First estimate for zν. 24. 2.4 Properties of the matrices C. ... i j is js s, |i| :=. s. is. The following lemmas will be used frequently (see [Ka], pp.

20 Jan 2011: We now use(2.16) to find. φAB = 2|K|2 KA′B AA′. (1. ... Substituting (2.24) into (2.23) gives the system (2.18) for the1-forms ei.

10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage.

21 Oct 2020: z O(z 2);. TR: yn =[(. I 12 kA)1 (. I 12 kA)]n. ... 24 / 28. Splitting of inhomogeneous systems. Recall our goal, namely fast methods for the two-dimensionaldiffusion equation.

8 Oct 2004: He found that, provided ka 1, where a is the core radius,σ2 =. ( κ2πh2. )2 [1 khK1(kh) 12(kh). 2ω(akδ)]. [1 khK1(kh) (kh)2K0(kh) ... EP/Uk. 2 =(κ. 2πh. )2k2. [lnh. 2aδ+. 1. 2. ](24). which differs from (18) by 12.

20 Jun 2011: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... 38. Guasto JS, Johnson KA, Gollub JP (2010) Oscillatory flows induced by microorganismsswimming in two dimensions.