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VOLUME 93, NUMBER 9 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Dombrowskietal04.pdf2 Sep 2012: 2] H. C. Berg and E. M. Purcell, Biophys. J. 20, 193 (1977).[3] J. ... Dombrowski et al. (to be published).[20] Somewhat similar patterns appear on agar substrates;. -
DOI 10.1140/epje/i2012-12045-6 Regular Article Eur. Phys. J. E (2012) …
www.damtp.cam.ac.uk/user/hinch/publications/EPJE35_45.pdf12 Sep 2012: The dispersion medium may be a simple liquid or acomplex fluid itself (a polymer solution for instance) [20].The packing density is approaching the jamming situa-tion. ... J. E 15, 97 (2004).20. H. Van Damme, S. Mansoutre, P. -
max_vel.eps
www.damtp.cam.ac.uk/user/hinch/publications/SIAM71_2151.pdf28 Feb 2012: 0.552. 0.554. 0.556. 0 5 10 15 20 25 0. 1. ... 35–52. << /ASCII85EncodePages false /AllowTransparency false /AutoPositionEPSFiles true /AutoRotatePages /None /Binding /Left /CalGrayProfile (Dot Gain 20%) /CalRGBProfile (sRGB IEC61966-2.1) -
Experimental investigations of elastic tail propulsion at low…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/YuLaugaHosoi06.pdf2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11. ... Two datasets are shown: 1 L = 20 cm, D = 0.5 mm, and a0 = 0.435 rad; 2L = 18 cm, D = 0.61 mm, and a0 = 0.814 rad. -
Flows driven by flagella of multicellular organismsenhance long-range …
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Shortetal06.pdf2 Sep 2012: 12x). To test this model, we measured the f low fields aroundcolonies using methods described elsewhere (4), building onearlier studies (19, 20) and summarized in Methods. ... J. 20, 193–219. 13. Senft, W. H., Hunchberger, R. A. & Roberts, K. -
Effective approximation for the linear time-dependent Schrödinger…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_05.pdf16 Jul 2012: 20 ‘wraparounds’ for the function u(x) = ecos πx and N = ω1/2. ... 102. 103. 104. 105. 10-30. 10-25. 10-20. 10-15. 10-10. 10-5. ω. -
Fluctuations, Dynamics, and the Stretch-Coil Transition of Single…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KantslerGoldstein12.pdf2 Sep 2012: 20 JANUARY 2012. 0031-9007=12=108(3)=038103(5) 038103-1 2012 American Physical Society. ... 20 JANUARY 2012. 038103-4. 23] The case A 0 is solved in E. -
BIT Numerical Mathematics (2008) 48: 743–761 Published online: 28 ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_01.pdf22 Mar 2012: 13, 18, 19, 20, 21, 25, 26].Assuming that f :RRd Rd satisfies the Lipschitz condition, the classicalwaveform Picard algorithm states. ... Sci. Stat. Comput., 8 (1987), pp. 459–482. 20. O. Nevanlinna, Remarks on Picard–Lindelöf iteration. -
Instabilities and Pattern Formation in Active Particle…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SaintillanShelley08.pdf2 Sep 2012: k̂?k̂, where k̂? is any unit vectorperpendicular to k̂. The dispersion relation for these modesis given by [20]. ... the aggregation of particlesby their swimming velocity in regions of rx cn< 0[20]. -
On rapid computation of expansions in ultraspherical polynomials…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_04.pdf28 Feb 2012: Thus, for n = 0. 20. Figure 4.3: log10 |f̂[M]n f̂| for fc. ... Comput. Harmon. Anal. 20, 3–25. Iserles, A. (2011), ‘A fast and simple algorithm for the computation of Legendrecoefficients’, Numerische Mathematik 117, 529–553.
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