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Optimal wavelet reconstructions from Fourier samples viageneralized…
www.damtp.cam.ac.uk/research/afha/anders/samptaFinal.pdf5 Oct 2013: In other words, if the reconstruction constant. C(FN,M ) = max{κ(FN,M ),µ(FN,M )},. is small. II. REDUCED CONSISTENCY SAMPLING. This problem of generalized sampling is not new -
Dynamic mechanisms for apparent slip on hydrophobic surfaces Eric ...
www.damtp.cam.ac.uk/user/lauga/papers/7.pdf26 Jul 2013: 25] J. Israelachvili,Intermolecular and Surface Forces(Academic,. New York, 1992).[26] A. Carambassis, L.C. -
Reciprocal locomotion of dense swimmers in Stokes flow
www.damtp.cam.ac.uk/user/lauga/papers/26.pdf26 Jul 2013: 13] Najafi A and Golestanian R 2004 Phys. Rev. E 69 062901[14] Avron J E, Kenneth O and Oaknin D H 2005 New J. -
, 20120576, published 2 January 2013469 2013 Proc. R. ...
www.damtp.cam.ac.uk/user/md327/skyrmion_proc.pdf14 Aug 2013: 171–184. New York,NY: Dekker. 7. Atiyah MF, Hitchin NJ. 1985 Low energy scattering of nonabelian monopoles. ... 1977 Space–time topology and a new class of Yang–Mills instanton. Phys.Lett. -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenSampTA.pdf5 Oct 2013: Emails: ben adcock@sfu.ca, a.hansen@damtp.cam.ac.uk. ABSTRACTWe present a new approach for the problem of reconstructingan element of a Hilbert space in an arbitrary reconstruction basisgiven ... Marcel Dekker Inc., New York, 2001. [8] A. C. Hansen. -
Axisymmetric viscous gravity currents flowing over a porous medium
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Spannuth-2009.pdf4 Nov 2013: GRAE WORSTER 2. 1Department of Geology and Geophysics, Yale University, New Haven, CT 06520, USA2Institute of Theoretical Geophysics, Department of Applied Mathematics and Theoretical Physics,. ... University of Cambridge, Wilberforce Road, Cambridge CB3 -
A General Allometric and Life-History Model for Cellular…
www.damtp.cam.ac.uk/user/gold/pdfs/amnat.pdf7 Mar 2013: Volvocales havea discrete generation time; when new colonies hatch, themother colony disintegrates through apoptosis. ... Hulin, L. Petit, and C. D. Mitescu. 2001. Physicalhydrodynamics. Oxford University Press, New York. -
Propulsion in a viscoelastic fluidEric Laugaa� Department of…
www.damtp.cam.ac.uk/user/lauga/papers/18.pdf26 Jul 2013: the kinematics of transport andlocomotion in a manner which is not possible with a New-tonian fluid. ... 5D. Bray, Cell Movements Garland, New York, 2000.6E. P. Lillehoj and K. -
PHYSICS OF FLUIDS 25, 071904 (2013) The wobbling-to-swimming…
www.damtp.cam.ac.uk/user/lauga/papers/81.pdf26 Jul 2013: Ajdari, “Designing phoretic micro- and nano-swimmers,” New J. Phys. 9, 126(2007). ... surface,” in Proceedings of the 2010 IEEE International Conference on Robotics and Automation (IEEE, New York, NY,2010), pp. -
Gauge Dynamics and Topological Insulators David Tong Back in ...
www.damtp.cam.ac.uk/user/tong/talks/gtop.pdf18 Jul 2013: the fermionic bilinear ψ̄ψ is odd under time reversal. However, we can define a new. ... The operator. (4.1) is invariant under this new symmetry and it also preserves charge conjugation. -
PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: We observe uniformconvergence of the reflections toward zero. Numerically, westop implementing new reflections when adding one improves. ... Bray, Cell Movements (Garland Publishing, New York, 2000).[4] L. J. Fauci and R. -
Proc. July 2007 Conf. onUnsolved Problems in Stellar Physics, ...
www.damtp.cam.ac.uk/user/mem/papers/SQBO/woodmcintyre-preprint.pdf19 Oct 2013: We report a new family of exact steadysolutions of the nonlinearequations showing how all these elements fit together, confining Bi within a layer ofthickness scaleδ = η/U while transmitting a retrograde -
Membrane Viscosity Determined from Shear-Driven Flow in Giant…
www.damtp.cam.ac.uk/user/gold/pdfs/membrane_viscosity.pdf17 Jul 2013: difficult to measure. Here we introduce a new method based on quantification of the large-scale circulation. -
Shaking-induced motility in suspensions of soft active particles…
www.damtp.cam.ac.uk/user/lauga/papers/35.pdf26 Jul 2013: This leads to a natural question to ask:can the hydrodynamic coupling between the unsteady con-formation and the particles positions yield unexpected phasebehavior and new modes of locomotion in suspensions ... A. Shapiro and M. Dworkin Ox-ford -
pnas201210548 1187..1192
www.damtp.cam.ac.uk/user/gold/pdfs/ciliary_contact.pdf3 Feb 2013: A more detailed understanding of these interactions promisesnot only new biological insights into structure and dynamics of fla-gella and cilia but may also lead to new microfluidic techniques forcontrolling cell ... interfaces. Froma general perspective, -
Fluid Dynamics of Bacterial Turbulence Jörn Dunkel,1 Sebastian…
www.damtp.cam.ac.uk/user/gold/pdfs/bacterial_turbulence.pdf29 May 2013: Princeton University, Princeton, New Jersey 08544, USA4Laboratoire de Physique des Solides, Université Paris-Sud 11 and CNRS, Bâtiment 510, 91405 Orsay Cedex, France. ... E. Goldstein,New J. Phys. 15, 045016 (2013). [29] I. Tuval, L. -
On the Order of Deferred Correction ANDERS C. HANSENDepartment ...
www.damtp.cam.ac.uk/research/afha/anders/Deferred10.pdf5 Oct 2013: family. Since there previously didnot exist any convergence proof for this method, new theoretical tools had to be built. ... Springer-Verlag,New York, 1973. Springer Tracts in Natural Philosophy, Vol. 23. [16] P. -
PHYSICS OF FLUIDS 24, 051902 (2012) Self-propulsion in viscoelastic…
www.damtp.cam.ac.uk/user/lauga/papers/66.pdf26 Jul 2013: If we use B′1 to denote the new value of B1, constantpower requirement is written as. ... 17. Finally, we obtainthe new definition of the stresslet. S =. AS. [1. 2{(σ n) x x (σ n)} 1. 3x σ nI β (un nu). -
Adhesion transition of flexible sheets Arthur A. Evans1,* and ...
www.damtp.cam.ac.uk/user/lauga/papers/27.pdf26 Jul 2013: New York, 1992.10 B. Chen, P. D. Wu, and H. Gao, Proc. -
On skew-symmetric differentiation matrices Arieh Iserles January 9,…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_01.pdf9 Jan 2013: Rep. 2012/NA05, University of Cambridge. Bejan, A. (2004), Convection Heat Transfer, 3rd edn, Wiley, New York. ... Richtmyer, R. D. & Morton, K. W. (1967), Difference Methods for Initial-Value Prob-lems, 2nd edn, Wiley-Interscience, New York. -
DOI 10.1140/epje/i2012-12068-y Regular Article Eur. Phys. J. E (2012) …
www.damtp.cam.ac.uk/user/lauga/papers/70.pdf26 Jul 2013: 12), re-spectively. The two new coefficients are. M5 = iμ. j =i[1 exp(iq Rij )] θvsx(Rij , x̂), (26). ... Thutupalli, R. Seemann, S. Herminghaus, New J. Phys.13, 073021 (2011). 19. -
Digital Object Identifier (DOI) 10.1007/s00220-013-1729-7Commun.…
www.damtp.cam.ac.uk/user/md327/CDT13_file.pdf14 Aug 2013: Oxford, UK: Clarendon. LMS monographs, new series: 15, 199621. Mettler, T.: Reduction of beta-integrable 2-Segre structures. ... Twistor Theory. Ed. S. Huggett. Lect. Notes Pure Appl. Math., 169, New York: Marcel Dekker, 199530. -
atsc_59_2106.2878_2882.tp
www.damtp.cam.ac.uk/user/mem/papers/SSREPLY/saujani-reply02.pdf19 Oct 2013: The new insight comes via the so-called velocity split-ting phenomenon, first noticed in the context of Ham-iltonian balanced models (Salmon 1988; McIntyre andRoulstone 2002, and references therein), but -
PHYSICS OF FLUIDS 24, 072102 (2012) Buckling instability of ...
www.damtp.cam.ac.uk/user/lauga/papers/67.pdf26 Jul 2013: Quéré, Capillarity and Wetting Phenomena (Springer Science BusinessMedia, Inc., New York, 2004). ... Tyuptsov, Low-gravity Fluid Mechanics. (Springer-Verlag, New York, 1987).23 P. T. Nagy and G. -
Optimal wavelet reconstructions from Fourier samples viageneralized…
www.damtp.cam.ac.uk/research/afha/people/anders/samptaFinal.pdf5 Oct 2013: In other words, if the reconstruction constant. C(FN,M ) = max{κ(FN,M ),µ(FN,M )},. is small. II. REDUCED CONSISTENCY SAMPLING. This problem of generalized sampling is not new -
The decay of stabilizability with Reynolds number in a linear model…
www.damtp.cam.ac.uk/user/lauga/papers/3.pdf26 Jul 2013: R. Bewley. The identi cation of these inherent properties in high- delity models of spatiallydeveloping ow systems should provide us with important new insights into thedesign of eective control strategies. ... In New trends in nonlinear dynamics and -
PHYSICAL REVIEW E 83, 011901 (2011) Locomotion by tangential ...
www.damtp.cam.ac.uk/user/lauga/papers/46.pdf26 Jul 2013: 2] D. Bray, Cell Movements (Garland Publishing, New York, NY,2000). [3] H. ... 2: Kinetic Theory, 2nd ed.(Wiley Interscience, New York, NY, 1987). [25] R. -
Crawling beneath the free surface: Water snail locomotionSungyon…
www.damtp.cam.ac.uk/user/lauga/papers/22.pdf26 Jul 2013: 2008 American Institute of Physics. DOI: 10.1063/1.2960720. I. INTRODUCTION. Engineers often look to nature’s wide variety of locomo-tion strategies to inspire new inventions and ... M. WilburAcademic, New York, 1985, Vol. 8, Chap. 1, pp. 59–64. -
Using PHF format
www.damtp.cam.ac.uk/user/lauga/papers/1.pdf26 Jul 2013: PHYSICS OF FLUIDS VOLUME 11, NUMBER 12 DECEMBER 1999. Vortices in rotating systems: Centrifugal, elliptic and hyperbolictype instabilities. D. Sipp, E. Lauga, and L. JacquinONERA, 29 avenue de la Division Leclerc, BP 72, F-92322 Chatillon Cedex, -
PHYSICAL REVIEW E 87, 023015 (2013) Interface pinning of ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Zhao-2013.pdf4 Nov 2013: University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, UK5School of Mathematics, University of New South Wales, Kensington, Australia. ... 1] R. M. Iverson, Rev. Geophys. 35, 245 (1997).[2] J. Bear, Dynamics of Fluids in Porous Media (Elsevier, New -
1B Methods 27 . 1B METHODS LECTURE NOTES Richard ...
www.damtp.cam.ac.uk/user/examples/B8Lb.pdf4 Oct 2013: The latter quantities define the new amplitudes and phases via their moduli and argu-ments. -
Proc. NATO Adv. Res. Workshop ARW 920946, Paris, October ...
www.damtp.cam.ac.uk/user/mem/oldftp/qbosolar.pdf19 Oct 2013: interpretation of recent helioseismic results, which give a new twist to the story. ... new observational data, obtained as a result of concerns about stratospheric ozone-layer. -
Three-dimensional flows in slowly varying planar geometriesEric…
www.damtp.cam.ac.uk/user/lauga/papers/5.pdf26 Jul 2013: Abraham D. StroockSchool of Chemical and Biomolecular Engineering, Cornell University, Ithaca, New York 14853. ... thesis, Stanford University1972! 26M. Abramowitz and I.A. Stegun,Handbook of Mathematical FunctionsDover, New York, 1972! -
Swimming in Circles: Motion of Bacteria near Solid Boundaries ...
www.damtp.cam.ac.uk/user/lauga/papers/12.pdf26 Jul 2013: model for the motion of E. coli near solid boundaries. Wefirst summarize our experiments to obtain a new set of data. ... of E. coli near solid boundaries and compared it to a new set ofmeasurements of cell velocities and trajectories. -
Wind-generated water waves: two overlookedmechanisms? MICHAEL E.…
www.damtp.cam.ac.uk/user/mem/oldftp/airsea-ima.pdf19 Oct 2013: 1985)and two recent reviews of mine (2000, 2002). The history takes on a new interest when. † ... Solan, Z.Hashin, 459 pp; Amsterdam, New York, Elsevier, 281–304. McIntyre, M. -
Comparative Hydrodynamics of Bacterial Polymorphism Saverio E.…
www.damtp.cam.ac.uk/user/lauga/papers/48.pdf26 Jul 2013: 5] E. Leifson, Atlas of Bacterial Flagellation (AcademicPress, New York and London, 1960); R. -
Optimal feeding is optimal swimming for all Péclet numbers ...
www.damtp.cam.ac.uk/user/lauga/papers/59.pdf26 Jul 2013: rkJ rbJ bðkÞ rbJ. bðkÞ: (38). 4. rkJ defines the steepest ascent direction on the unithypersphere in b-space and the next iteration is carried ata new guess for the optimal ... is not possible to find a new guess with J(k þ 1) > J(k) usingthis -
PHYSICS OF FLUIDS 24, 103102 (2012) Micropropulsion and microrheology …
www.damtp.cam.ac.uk/user/lauga/papers/72.pdf26 Jul 2013: In essence, as complex fluids lead to new modes of small-scalepropulsion, symmetrically the presence of propulsion in an environment can be used to locally probethe rheological properties of the fluid. ... III B 2 and thereforeEq. (36), we need two new -
b924548k 1737..1747
www.damtp.cam.ac.uk/user/lauga/papers/40.pdf26 Jul 2013: additional constraints. First, the integrated mean curvature M is. controlled, Ms p(rK sinj), and second, a new Lagrangianconstraint enters, Qs 0. -
§4 FLOWS WITH A FREE SURFACE Such flows are ...
www.damtp.cam.ac.uk/user/mem/FLUIDS-IB/waves.pdf19 Oct 2013: This was done by setting up measuring stations in New Zealand, in Alaska, and on someintervening Pacific islands. -
Book.dvi
www.damtp.cam.ac.uk/user/phh/papers/ictam_haynes_4a.pdf19 Oct 2013: Geophys. Res., 99, pp.1071–1088, 1994. Wiggins, S., Chaotic transport in dynamical systems, New York, Spring-Verlag, pp.301,1992. -
1B Methods 62 . 1B METHODS LECTURE NOTES Richard ...
www.damtp.cam.ac.uk/user/examples/B8Lc.pdf4 Oct 2013: The key new ideahere is the following procedure: we first consider G’s that arise from honest functions gand then express the action of g′ (or any other modified version of ... 1B Methods 82. This is a very useful observation for obtaining new FTs: -
Propulsion by passive filaments and active flagella near boundaries…
www.damtp.cam.ac.uk/user/lauga/papers/43.pdf26 Jul 2013: C. Berg, E. Coli in Motion Springer-Verlag, New York,. 2004.4 C. -
The optimal elastic flagellumSaverio E. Spagnoliea� and Eric Laugab�…
www.damtp.cam.ac.uk/user/lauga/papers/36.pdf26 Jul 2013: Continuous advances in imaging re-vealed new details regarding the structure and kinematics. ... The paper is structured as follows. In Sec. II we intro-duce the notation for the swimming kinematics, as well asthe new swimming energy measures we use in -
Floppy swimming: Viscous locomotion of actuated elastica Eric…
www.damtp.cam.ac.uk/user/lauga/papers/16.pdf26 Jul 2013: Floppy swimming: Viscous locomotion of actuated elastica. Eric LaugaDepartment of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA. Received 5 October 2006; published 26 April 2007. -
C2SM27089G 1711..1720
www.damtp.cam.ac.uk/user/lauga/papers/74.pdf26 Jul 2013: for y(s) f sin(ks). For k [ 1, we are led to write the integrationover a new inner variable s0 s x/k, so that. -
www.damtp.cam.ac.uk/user/mem/papers/LHCE/dilnot-pat-analysis.txt
www.damtp.cam.ac.uk/user/mem/papers/LHCE/dilnot-pat-analysis.txt19 Oct 2013: DILNOT Patents regimes can be abused to block new ideas, not just to encourage them. ... Elizabeth Harding. HARDING Part of the difficulty is trying to fit an old law to new technology. -
C1SM05503H 8169..8181
www.damtp.cam.ac.uk/user/lauga/papers/56.pdf26 Jul 2013: flexible filaments for propulsion. The new nanomotor presented. Soft Matter, 2011, 7, 8169–8181 | 8169. ... was passive. In the current paper, we present both a new design and. -
On the Order of Deferred Correction ANDERS C. HANSENDepartment ...
www.damtp.cam.ac.uk/research/afha/people/anders/Deferred10.pdf5 Oct 2013: family. Since there previously didnot exist any convergence proof for this method, new theoretical tools had to be built. ... Springer-Verlag,New York, 1973. Springer Tracts in Natural Philosophy, Vol. 23. [16] P. -
flm1100223a
www.damtp.cam.ac.uk/user/lauga/papers/54.pdf26 Jul 2013: Previous work considered how the unsteady deformation of softsurfaces generated by time-reversible flows could provide new modes of locomotionand pumping (Trouilloud et al. ... Thetwo-dimensional assumption, although idealized and not directly relevant
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