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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. -
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. -
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. -
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]. -
LH8417 2..5
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SimhaRamaswamy02.pdf2 Sep 2012: Theirspeeds obey a messy cubic equation which, we can show[20], has real solutions for a finite range of parametervalues. ... These, as wellas other results on SPP nematics on substrates and ananalysis of isotropic SPP suspensions [3], will appear -
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. -
201107046 10391..10395
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Kurtulduetal11.pdf2 Sep 2012: 20 30 40 50 60. rw[µm]. 10 1. 10 2. 10 3. ... 20, 0.03% vv) is added to the mixture to lowerthe surface tension of the cell suspension. -
Direct Measurement of the Flow Field around Swimming Microorganisms…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Drescheretal10.pdf2 Sep 2012: The large differencein organism size between Volvox and Chlamydomonasrequired two distinct methods to measure the flows theycreate [20]. ... 95, 204501 (2005); D.Saintillan and M. J. Shelley, Phys. Fluids 20, 123304(2008); T. -
flm99218a
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/vandeMeentetal10.pdf2 Sep 2012: Velocimetry measurements were performed on a Bruker Spectrospin DMX 200,4.7 T magnet with a 20 mm long solenoid coil of diameter 3 mm; 1H images wereacquired at 199.7 ... 400 –200 200 4000 –40 –20 20 400. Position (μm). x (μm).
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