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A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenShadrin.pdf5 Oct 2013: xm} is a grid of mequispaced points in [1, 1]. In [24] it was shown that. ... Proc. SPIE, 7535, 2010. [24] D. Coppersmith and T. Rivlin. The growth of polynomials bounded at equally spaced points. -
flm971.dvi
www.damtp.cam.ac.uk/user/lauga/papers/6.pdf26 Jul 2013: CA 92093-0411, USA2LadHyX, École Polytechnique-CNRS, 91128 Palaiseau Cedex, France. (Received 28 April 2003 and in revised form 24 March 2004). ... By selecting ξinf = 15.7 andξsup = 24 and defining N = 140 gridpoints via this approach, adequate -
The decay of stabilizability with Reynolds number in a linear model…
www.damtp.cam.ac.uk/user/lauga/papers/3.pdf26 Jul 2013: Received 24 May 2002; accepted 17 December 2002; published online 30 June 2003. -
Global warming preceded by increasing carbon dioxide concentrations…
www.damtp.cam.ac.uk/user/mem/shakun-co2-temp-lag-nat12.pdf8 Jun 2013: simulations. g, North Atlantic sediment core OCE326-GGC5 231Pa/230Th (ref.24). Temperatures are given as deviations from the early Holocene (11.5–6.5 kyr ago) mean. ... Paleoceanography 18, 1087 (2003). 24. McManus, J. F., Francois, R., Gherardi, J.-M., -
The effects of capillary forces on the axisymmetric propagation ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Golding-2013.pdf4 Nov 2013: Fluids 24, 117102 (2012) Effect of fluctuations on the onset of density-driven convection in porous media Phys. ... Fluids 24, 114102 (2012) Absence of subcritical instabilities and global nonlinear stability for porous ternary diffusive-convective -
An experimental study of shear-enhanced convection in a mushy layer
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2008.pdf4 Nov 2013: FC = 24/3λD. (gβ̃. Dν. )1/3(C0 Ci )4/3, (4.3). where λ is a constant. ... 1 9.3 0.1 9 1 10.47 3.73 0.25 unstable230106D 9 1 3.19 0.02 27 0.3 10.47 3.73 0.24 unstable230106E -
Passive hydrodynamic synchronization of two-dimensional swimming…
www.damtp.cam.ac.uk/user/lauga/papers/47.pdf26 Jul 2013: to the cre-ation of flagella bundles propelling the cells forward as theyswim, as well as the disruption of such bundles when thecells change their swimming direction.22–24. ... U =h̄. 2f x. s. 24. Noting that d / dt = U we therefore get an equation -
Bulletin of Mathematical Biology (2010) 72: 973–1005DOI…
www.damtp.cam.ac.uk/user/lauga/papers/39.pdf26 Jul 2013: 24). If we note 〈.〉 the t -averaging operator between t and t 2π, we therefore obtain〈e(j )i. ... 27). From the definition of F and Eqs. (24)–(27), we can write. -
Author's personal copy Physica D 240 (2011) 140–149 Contents ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Neufeld-2011-1.pdf4 Nov 2013: j r)2 α2][(j r)2 (j r) α2 ϵ1]aj. = ϵ1[α2 1 (j r 1)2]aj1, (24). ... book. Of particular relevance to this analysis arethe studies of the hydrodynamic stability of the asymptotic suctionprofile by Hughes and Reid [23], Hocking [24] and Lakin andReid -
Using PHF format
www.damtp.cam.ac.uk/user/lauga/papers/1.pdf26 Jul 2013: have been investigated iRef. 24. P license or copyright, see http://pof.aip.org/pof/copyright.jsp.
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