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Breaking the coherence barrier: asymptoticincoherence and asymptotic…
www.damtp.cam.ac.uk/user/abr28/AHPRSampta13.pdf5 Oct 2013: influence of the problem resolution.Naı̈ve simulations with standard, low-resolution test imagesmay very well lead to incorrect conclusions about the efficacyof compressed sensing as a tool for image reconstruction. -
A smooth future?
www.damtp.cam.ac.uk/user/lauga/papers/51.pdf26 Jul 2013: 1c,d), thus providing ideal systems on which to test fundamental ideas. -
Haynes_chapter2_overviewV1 (final draft)
www.damtp.cam.ac.uk/user/phh/papers/lagrangian2013.pdf19 Oct 2013: some test cases. -
On the Order of Deferred Correction ANDERS C. HANSENDepartment ...
www.damtp.cam.ac.uk/research/afha/anders/Deferred10.pdf5 Oct 2013: 5 Numerical examples. In this section we will test the method on a standard example; the Van der Pol equation. ... The test has been carried out as in the previous examples, and the results aredisplayed in Table 5.4 similar to Table 5.1. -
Breaking the coherence barrier: asymptoticincoherence and asymptotic…
www.damtp.cam.ac.uk/research/afha/anders/AHPRSampta13.pdf5 Oct 2013: influence of the problem resolution.Naı̈ve simulations with standard, low-resolution test imagesmay very well lead to incorrect conclusions about the efficacyof compressed sensing as a tool for image reconstruction. -
On the Order of Deferred Correction ANDERS C. HANSENDepartment ...
www.damtp.cam.ac.uk/research/afha/people/anders/Deferred10.pdf5 Oct 2013: 5 Numerical examples. In this section we will test the method on a standard example; the Van der Pol equation. ... The test has been carried out as in the previous examples, and the results aredisplayed in Table 5.4 similar to Table 5.1. -
Local Mass Conservation and Velocity Splitting in PV-Based Balanced…
www.damtp.cam.ac.uk/user/mem/papers/ENCYC/hyperb-1-published.pdf19 Oct 2013: The question of numerical accuracy is ad-dressed in Part II. It demands exceedingly careful anddelicate numerical tests. ... Why this is so remains myste-rious. Of course numerical tests can never cover allpossible flows. -
Book.dvi
www.damtp.cam.ac.uk/user/phh/papers/ictam_haynes_4a.pdf19 Oct 2013: measure of the geometry of a test tracer that is advected bythe flow (Haynes and Shuckburgh 2000a,b). -
doi:
www.damtp.cam.ac.uk/user/lauga/papers/73.pdf26 Jul 2013: Similar numerical tests performed on less efficient swimmers than strokeA (that is, swimming strokes for which mode 1 is not dominant) did not modify thisobservation significantly, and restricting the computation to -
PHYSICS OF FLUIDS 25, 071904 (2013) The wobbling-to-swimming…
www.damtp.cam.ac.uk/user/lauga/papers/81.pdf26 Jul 2013: 27), the wobbling angle is observed toincrease as the frequency decreases, from zero up to a maximum of 90 at the lowest test frequency(meaning that, in this limit, the helix -
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: In particular, the form and structure of hydrodynamicboundary layers is coupled to moving phase boundaries, providingan ideal test bed for a number of general ideas including singular. ... in addition to its ease of handling, has made it a -
flm971.dvi
www.damtp.cam.ac.uk/user/lauga/papers/6.pdf26 Jul 2013: J. Fluid Mech. (2004), vol. 512, pp. 343–374. c 2004 Cambridge University PressDOI: 10.1017/S0022112004009711 Printed in the United Kingdom. 343. Performance of a linear robust controlstrategy on a nonlinear model of. spatially developing flows. -
pnas201210548 1..6
www.damtp.cam.ac.uk/user/gold/pdfs/ciliary_contact_plus_SI_online.pdf7 Jan 2013: That microfluidic circuits provide an excel-lent test bed for developing and assessing new strategies for thecontrol of cell motility was recently demonstrated by the rectifi-cation of random bacterial swimming ... Flagella-Induced Scattering of -
PHYSICS OF FLUIDS 24, 051902 (2012) Self-propulsion in viscoelastic…
www.damtp.cam.ac.uk/user/lauga/papers/66.pdf26 Jul 2013: the test function for τ p , h is the characteristic length-scale of the element and UCis the magnitude of the local characteristic velocity. -
minimal
www.damtp.cam.ac.uk/user/gold/pdfs/minimal.pdf24 Apr 2013: To test whether microscopically different active fluidsdo indeed share universal hydrodynamic long-wavelength characteristics will require combinedanalytical, numerical and experimental efforts. -
Optimal feeding is optimal swimming for all Péclet numbers ...
www.damtp.cam.ac.uk/user/lauga/papers/59.pdf26 Jul 2013: 1: (33b). Multiplying Eq. (33a) by a test function g and integratingover the entire fluid domain Vf, one obtains after integrationby part that, at leading order,. -
PHYSICS OF FLUIDS 17, 103102 �2005� Brownian motion near ...
www.damtp.cam.ac.uk/user/lauga/papers/11.pdf26 Jul 2013: In Sec. IV, we consider the coupled mobilities/diffusivities of two small particles, and propose alternate ex-perimental tests for slip to complement those in Sec. -
Global warming preceded by increasing carbon dioxide concentrations…
www.damtp.cam.ac.uk/user/mem/shakun-co2-temp-lag-nat12.pdf8 Jun 2013: 54. See SupplementaryInformation for more discussion of these tests.Model freshwater forcing. -
C1SM05503H 8169..8181
www.damtp.cam.ac.uk/user/lauga/papers/56.pdf26 Jul 2013: This. simple test illustrates the fundamental difference between the. propulsion of rigid chiral objects and flexible propellers. -
PHYSICS OF FLUIDS 24, 103102 (2012) Micropropulsion and microrheology …
www.damtp.cam.ac.uk/user/lauga/papers/72.pdf26 Jul 2013: S hc. Ucu S, τ p De(u τ p GT τ p τ p G) (1 ζ )(G GT ). }= 0, (13). where S denotes the test function for τ p,
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