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30 Nov 2015: return to (10.7) but now suppose we impose. φ|Rn{τ} = f(x) (10.20).

5 Aug 2015: coli, with v 20 μm/s and τ 1 s, run 20 μm, but it can be considerably longer for otherbacteria [28]. ... 30, 235 (1971). [20] J. D. Murray, Mathematical Biology II Spatial Models andBiomedical Applications, 3rd ed.

4 Aug 2015: Zenit, Phys. Fluids 25,. 031701 (2013).[19] E. Lauga, Phys. Fluids 19, 083104 (2007).[20] H.

15 Jul 2015: 5. [2] H. Schmitz, D. Tsiklauri, Phys. Plasmas 20, 062903 (2013); http://dx.doi.org/10.1063/1.4812453 [3] R. ... P1.20 Inigo Arregui Title - Model comparison for the density structure across solar coronal loops Authors: I.

3 Apr 2015: 0 (N 1)/20 0 (N 1)/2 0. ,. given on a uniform grid, xm = m/(N 1), is of order p = 2 and skew-symmetric.This example, though, is ... Moreover (and consistently with our former remark),. 20. unless h̃ contains an even,

5 May 2015: 20 A. Iserles, K. Kropielnicka & P. Singh. as the expansion obtained after discarding all O(ε(2p1)σ1.

9 Nov 2015: We already have the Green’s function. solution to the homogeneous problem in (7.20), so we simply need to find a solution to. ... sin x. sin 1. 1. xf(ξ) sin(1 ξ) dξ (7.35). using the result (7.20). –

4 May 2015: 1938 and 1940 [20], [21], [22]. Rossby’s 1938 paper recognized the exact. ... 20 Rotation and Momentum Transport in Magnetized Plasmas. where f is the Coriolis parameter as before, ẑ is a unit vertical vector, and. ‖ ‖

28 Sep 2015: 3. , and solve term by. term. 20. Cop. yrig. ht. ... This is a Lyapunov. function, defined precisely by. Definition 20 (Lyapunov function).

30 Nov 2015: 2 Sturm–Liouville Theory 20. 2.1 Self-adjoint matrices 20. 2.2 Differential operators 21. ... limn. |f(θ) Snf(θ)| = 0 at every point θ S1 , (1.20).