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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: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P. -
[ 7 9 6 ] WAVE PROPAGATION ALONG FLAGELLA ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Machin58.pdf27 Aug 2012: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14. -
Digital Object Identifier (DOI) 10.1007/s00205-012-0523-6Arch.…
www.damtp.cam.ac.uk/user/dmas2/public_ps/wk.pdf10 Oct 2012: Therefore, (3.24) follows.The term Q1 is estimated using the bound. |Q1| = G. ... Fiα(λF) >= A Fiα (F) and the estimation (in. the spirit of (3.24)). -
microswimmers
www.damtp.cam.ac.uk/user/gold/pdfs/microswimmers.pdf3 Sep 2012: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum -
P H Y S I C A L R ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Hatwalneetal04.pdf2 Sep 2012: On time scales shorter than , effects associ-ated with spatiotemporal correlations in Q [23] intervene.For a drop [24] or a film [22] of size L, the tails will be cutoff ... Tu, Phys. Rev. E 64, 011902. (2001).[24] G.V. Soni et al., Biophys. -
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: In a preliminary work [23, 24] we explored some mor-phological aspects of the fracture profiles obtained inplane-plane debonding experiments performed with gran-ular adhesives (crushed sand in an acrylic ... Van Damme, Fractals 1, 968 (1993).24. H. Van -
Synchronization and Collective Dynamics in a Carpet of Microfluidic…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian10.pdf2 Sep 2012: On the other hand, recent advances frommicron-scale magnetically actuated tails [24] to syntheticmolecular rotors [25] now allow fabrication of arrays ofactive tails that can stir up the fluid. ... 2007); Small 4, 111 (2008).[24] R. Dreyfus et al., -
IMAGE DENOISING: LEARNING NOISE DISTRIBUTION VIAPDE-CONSTRAINED…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_04.pdf16 Jul 2012: λ1 1270.9 1103.4 1100.7 1099.8 1189.8λ2 26.39 48.24 46.37 44.92 28.13. ... 24] K. Frick, P. Marnitz, A. Munk, Statistical Multiresolution Estimation for Variational Imaging:With an Application in Poisson-Biophotonics, J. -
BIT Numerical Mathematics (2008) 48: 743–761 Published online: 28 ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_01.pdf22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein, -
Nature’s Microfluidic Transporter: Rotational Cytoplasmic Streaming…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/vandeMeentTuvalGoldstein08.pdf2 Sep 2012: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.
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