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19 Aug 2013: Small strain-hardening, small shear-thinning. Test of Batchelor φ2 result. µ = µ[.

26 Jul 2013: 1c,d), thus providing ideal systems on which to test fundamental ideas.

19 Oct 2013: some test cases.

5 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.

5 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.

5 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.

3 Feb 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

20 Dec 2013: By ”test body” we mean an uncharged object whose gravitational self-interactionis negligible, and whose size is much less than the length over which external fieldssuch as g vary. ... energy. Thus thefact that the motion of test bodies is consistent

26 Jul 2013: test whether theideas put forward in this paper are valid.

19 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.

19 Oct 2013: measure of the geometry of a test tracer that is advected bythe flow (Haynes and Shuckburgh 2000a,b).

26 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

26 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

4 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

26 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.

7 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

26 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.

24 Apr 2013: To test whether microscopically different active fluidsdo indeed share universal hydrodynamic long-wavelength characteristics will require combinedanalytical, numerical and experimental efforts.

26 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,.

26 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.

8 Jun 2013: 54. See SupplementaryInformation for more discussion of these tests.Model freshwater forcing.

26 Jul 2013: This. simple test illustrates the fundamental difference between the. propulsion of rigid chiral objects and flexible propellers.

26 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,

5 Oct 2013: Using these values, in Figure 3 we plot the errors committed by the two methods for a varietyof different test functions.

5 Oct 2013: Generalized sampling and the stable and accuratereconstruction of piecewise analytic functions from their. Fourier coefficients. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre

26 Jul 2013: The numerical procedure was validated through conver-gence tests and by reproducing previous results for shearflow over sinusoidal surfaces.39 A large number of elements2N is needed when the sheets are

19 Oct 2013: This is a cumulative accuracy test, using the PV-conserving balanced model defined by a normal-mode-based PV inversion operatortogether with the single prognostic equation DQ/Dt = 0, for

4 Nov 2013: The effects of capillary forces on the axisymmetric propagation of two-phase, constant-flux gravity currents in porous mediaMadeleine J. Golding, Herbert E. Huppert, and Jerome A. Neufeld Citation: Phys. Fluids 25, 036602 (2013); doi:

5 Oct 2013: Using these values, in Figure 3 we plot the errors committed by the two methods for a varietyof different test functions.

4 Nov 2013: ln t =m1. ES+ m2 m3 ln(ES ) m4ES. (4.19). This enables us to extract the asymptotic nature of the solution and test the long-time limit (4.17) while

5 Oct 2013: Generalized sampling and the stable and accuratereconstruction of piecewise analytic functions from their. Fourier coefficients. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre

19 Oct 2013: May 31, 2010 Lecture Note Series, IMS, NUS — Review Vol. 9in x 6in lecturenotes˙190410. TRANSPORT AND MIXING OF ATMOSPHERIC. POLLUTANTS. Peter Haynes. Department of Applied Mathematics and Theoretical PhysicsUniversity of Cambridge. Wilberforce

5 Jun 2013: nuclear tests published in 1968. Using an instrumented aircraft, two ma-.

5 Oct 2013: Stable reconstructions in Hilbert spaces and the resolutionof the Gibbs phenomenon. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of

5 Oct 2013: 3.5 Numerical ExamplesIn this section we will test the framework suggested in the previous section with the following frames: let{pk}kN denote the Legendre polynomials on [1, 1] and ... The assertion about K2m,r follows. 4.3 Numerical ExamplesIn this

19 Oct 2013: since its magnitude is O(a2 4). 6. Numerical ray tracingNumerical ray-tracing results are presented now that illustrate and test the.

5 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.

4 Nov 2013: 2007). Several small-scale demonstrationprojects have already commenced, pumping supercritical CO2 into brine-saturatedaquifers to test the viability of this technique. ... 5. Experimental analogueA series of analogue laboratory experiments were

23 May 2013: 4] Davis, C.-I.: Numerical tests of the Fokas method for Helmholtz-type partial differential equations: Dirichlet to Neumann Maps,Masters Thesis, University of Colorado at Boulder (2008).

26 Jul 2013: Recently, a study of light-activated colloidsreported the spontaneous surfing motion of reactive isotropic colloids lying on a solid surface,34 asystem which might be a potential candidate to test, at

26 Jul 2013: computed a linear controlstrategy, it is straightforward to test it on the nonlinearequation, and second, because the nonlinear modelbetter addresses the real problem of interest, that is,.

19 Oct 2013: Animportant test of this picture, after numerical renement, will be quantitativeconsistency between the predicted and observed interior angular velocities.Two quite dierent explanations for the near-uniform interior rotation of the

5 Oct 2013: Stable reconstructions in Hilbert spaces and the resolutionof the Gibbs phenomenon. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of

5 Oct 2013: 3.5 Numerical ExamplesIn this section we will test the framework suggested in the previous section with the following frames: let{pk}kN denote the Legendre polynomials on [1, 1] and ... The assertion about K2m,r follows. 4.3 Numerical ExamplesIn this

5 Oct 2013: On optimal wavelet reconstructions from Fourier samples:. linearity and universality of the stable sampling rate. B. Adcocka, A. C. Hansenb,c, and C. Poonb. aDepartment of Mathematics, Purdue UniversitybDepartment of Applied Mathematics and

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

5 Oct 2013: On optimal wavelet reconstructions from Fourier samples:. linearity and universality of the stable sampling rate. B. Adcocka, A. C. Hansenb,c, and C. Poonb. aDepartment of Mathematics, Purdue UniversitybDepartment of Applied Mathematics and

19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret

5 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.

27 Aug 2013: ResultsTo test the model and understand more about the regimes ofbehavior it possesses, we ran numerical integrations of the sys-tem starting from initial conditions of randomly perturbed totalfilament disorder (Materials ... Such an experiment would