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27 Nov 2011: Experiments were done at 24.0C and16.2C, with initial speeds indicating operation well into thehigh-speed, low-torque regime. ... Fig. 3. (a) Data from five bacteria at 24.0C were plotted on the same graph andmarked with different symbols (with the data

2 Nov 2011: 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,

25 Nov 2011: It considers a forcing term that is oscillatory in space. tu = 2x b sin ωx, (3.24). ... 2t cos ω xbeω2t sin ω,. 21. Figure 3.1: The solution of (3.24) for different values of ω.

10 Apr 2011: 0.947 1.422 0.380 0.589. 291.155 265.827 31.473 24.649 3.488 6.172. 3626.522 116.233 18.702 14.883 2.529

10 Apr 2011: The identity22,23,24. exp[ -A3({P})]. = exp[ - A 3 ( {81M}) ]exp(f dr J(r) p (r») I J= 0' (2.22). ... f/Jc. where the N independent amplitude is. 1 (w) _ '24 [g2(X) p/2 1/2 -yk ()[ ()]1/2 gl X -g4 X.

10 Apr 2011: As the lower values of viscosity ratio are approachthe boundary integral method eventually fails to consevolume.24 In Fig.

6 Jul 2011: Annu Rev Fluid Mech 24:313–358. 2. Aranson IS, Sokolov A, Kessler JO, Goldstein RE (2007) Model for dynamical coherencein thin films of self-propelled microorganisms.

1 Sep 2011: F0 = 1 < F2 =π2. 8< < 4. π< < F3 =. π3. 24< F1 =. π. 2. In this section we obtain a difference analogue of the Bohr-Favard inequality in theform. ... 1. 24. ]= 1. 325. 192. 1. α4. With α = 1 and α = 2, we obtain c4(πn ) =. 517192. = 2.6927, and c4

10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

14 Feb 2011: 0.0997679 0.0314839 0 23 0 199.5 15.5 0.155559 -0.167651 0 24 0 207.5 15.5 -0.00544606 -0.227898 0 25 0 215.5 ... 1 199.5 23.5 0.610019 0.125893 0 24 1 207.5 23.5 0.668408 0.386805 0 25 1 215.5 23.5 0.565238 0.810526