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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. -
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. -
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). -
Hydrodynamic interactions between rotating helices MunJu Kim and…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KimPowers04.pdf2 Sep 2012: Received 5 July 2003; revised manuscript received 20 January 2004; published 4 June 2004). ... Each flagellum consists of arotary motor; a universal joint about 50 nm long, known asthe hook, and a helical filament 20 nm in diameter and about10 mm long. -
Beyond consistent reconstructions: optimality and sharp bounds for…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_10.pdf20 Oct 2012: 11. 10 20 30 40 50. 10-14. 10-11. 10-8. 10-5. 0.0120 40 60 80 100. ... 10-14. 10-11. 10-8. 10-5. 0.01. 20 40 60 80 100. 10-10. -
VOLUME 80, NUMBER 17 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/WigginsGoldstein98.pdf2 Sep 2012: a5. 20. cossvtd. 1 L 24s4 2 6ad sinsvtd 1 O sL 4d ,ytorque. ... Schliwa, J. Cell Sci.109,509 (1996). [20] R. E. Goldstein and S. -
[ 7 9 6 ] WAVE PROPAGATION ALONG FLAGELLA ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Machin58.pdf27 Aug 2012: Putting y. (18). equation (16) gives. or. (20). (21). This represents a progressive wave of bending moment with a wavelength,velocity and direction of propagation similar to the wave of displacement; -
RAPID COMMUNICATIONS PHYSICAL REVIEW E 86, 015301(R) (2012)…
www.damtp.cam.ac.uk/user/hinch/publications/PhysRevE.86.015301.pdf11 Jul 2012: 0.87 2.22 0.11Qwater4 7.5 0.01 36.06 0.20 2.22 0.11Qethanol1 2.36 0.01 8.60 0.51 7.64 0.25. -
Celestial Mechanics and Dynamical Astronomy manuscript No.(will be…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_02.pdf2 Aug 2012: Wecan circumvent this problem if we consider instead the splitting. H̄(q, p, qt, pt) =. (1. 2p>p. )γ. (V (q) pt. )γ. (20). Separable Hamiltonian with kinetic energy quadratic in ... 20 Sergio Blanes, Arieh Iserles. 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.22.
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