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Axisymmetric viscous gravity currents flowing over a porous medium
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Spannuth-2009.pdf4 Nov 2013: 10 7.37 0.01 401 21.8 1.73 11111 6.63 0.01 401 20.7 1.69 10912 20.35 0.03 401 36.2 2.24 144. -
Floppy swimming: Viscous locomotion of actuated elastica Eric…
www.damtp.cam.ac.uk/user/lauga/papers/16.pdf26 Jul 2013: 0 aRFU 0 , 24. Text = 0 0 00 0 aRFU0 aRFU 0. ... Optimal III 0.24 3.34 12.6 2.6 7.9 0.336. Optimal IV 0.49 3.20 16.9 2.6 5.4 0.465. -
Comparative Hydrodynamics of Bacterial Polymorphism Saverio E.…
www.damtp.cam.ac.uk/user/lauga/papers/48.pdf26 Jul 2013: 2, 0.5) (1.1, 0.4)f (2.2, 0.53) (0.91, 0.29)g (2.3, 0.45) (0.69,1.52) (1.24, 0.52) (1.14, -
Notes for NSTMathematical Methods III† Recommended books: H.F. Jones, …
www.damtp.cam.ac.uk/user/mem/N.pdf16 Oct 2013: m=1. α(m)(t)δmn. = α(n)(t) , (1.24). reproducing (1.23) apart from renaming the indices. ... 24. Chapter 2. 2. Groups. This chapter contains the second set of syllabus items, together with a fewitems anticipating the third set:. -
pnas201302736 14132..14137
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_selforganization.pdf27 Aug 2013: pointed) end to its plus (barbed) end.These cables are bound to the cortically fixed chloroplasts atthe cell periphery (24) in a “barber pole” twist, generating flowspeeds of 50–100 ... Characean algae. Proc Natl Acad Sci USA 73(1):165–167.24. -
flm469.dvi
www.damtp.cam.ac.uk/user/lauga/papers/4.pdf26 Jul 2013: J. Fluid Mech. (2003), vol. 489, pp. 55–77. c 2003 Cambridge University PressDOI: 10.1017/S0022112003004695 Printed in the United Kingdom. 55. Effective slip in pressure-driven Stokes flow. By ERIC LAUGA AND HOWARD A. STONEDivision of Engineering -
Jet propulsion without inertiaSaverio E. Spagnoliea� and Eric Laugab� …
www.damtp.cam.ac.uk/user/lauga/papers/41.pdf26 Jul 2013: Other simple propulsivesystems proposed for locomotion at zero Reynolds numberinclude a deformable two-dimensional loop;18 systems oftwo,19–22 three,21,23,24 or N spheres;25 an oscillating body ... R2. z c. R1, 24. where c = a2 b2, r = x2 y2, r̂ = -
Asymptotic Solvers for Highly Oscillatory Semi-explicit DAEs Marissa…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_08.pdf12 Aug 2013: Cont. Dynamical Sys. 28, 1345–1367. 24. Figure 3.4: The errors for h(t) for ω = 200π (top row) and ω = 2000π(bottom row): from the left 0, 1 and -
Wind-generated water waves: two overlookedmechanisms? MICHAEL E.…
www.damtp.cam.ac.uk/user/mem/oldftp/airsea-ima.pdf19 Oct 2013: Fluid. Dyn. Res., 24, 375–404.Janssen, P. A. E. M. 1982 Quasilinear approximation for the spectrum of wind-generated. -
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.
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