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http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM54_423.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 424 E. J. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM56_803.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 804 E. J. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM47_291.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meck. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 292 E. J. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM54_469.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Meoh. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 470 H. A. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM46_685.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 686 L. G. -
jas2538 1315..1326
www.damtp.cam.ac.uk/user/mem/mcintyre-imbalance-jas-09.pdf8 Jul 2009: 1–24 of the Collected Papers, Vol. 3, M. Y. Hussaini, Ed., Oxford. -
Fluctuations and stratification in sedimentation of dilute…
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_21_093304.pdf10 Nov 2009: Received 8 June 2009; accepted 3 August 2009; published online 24 September 2009. -
Paper2A.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_03.pdf30 Nov 2009: 24 H. Brunner, A. Iserles & S.P. Nørsett. Figure 3.3: The number of significant digits in approximating one of the two nonzero eigen-values forKω(x, y) = cos ω(x -
DAMTP 2009/NA06 The BOBYQA algorithm for bound constrained…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_06.pdf12 Aug 2009: 12α2 (1 α)2 ‖y. j xk‖4, αR, (4.24). the last line being due to the positive semi-definiteness of =ZZT. -
Under consideration for publication in J. Fluid Mech. 1 ...
www.damtp.cam.ac.uk/user/hinch/publications/Larrieu_etal_v4d.pdf5 Mar 2009: Under consideration for publication in J. Fluid Mech. 1. Lagrangian drift near a wavy boundary in aviscous oscillating flow. By E. L A R R I E U1, E. J. H I N C H2A N D F. C H A R R U1. 1Institut de Mécanique des Fluides de Toulouse - UMR CNRS/INPT -
PHYSICS OF FLUIDS VOLUME 15, NUMBER 7 JULY 2003 ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_15_1875.pdf10 Jul 2009: The pairs were then processed to find tvelocity-vector map of the flow field by using an adaptsource code and compiled application for PIV developedCardoso.24. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM55_745.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Pluid Mech. ... http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. 746 L. G. -
http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM52_683.pdf24 Aug 2009: http://journals.cambridge.org Downloaded: 24 Aug 2009 IP address: 131.111.16.227. J. Fluid Mech. ... 3A(sin4 8, sin 24,) - 2(A - B)(sin28, sin 24,)}, of, = of. = -
Computer simulations of Brownian motion of complex systems
www.damtp.cam.ac.uk/user/hinch/publications/JFM282_373.pdf14 Jul 2009: Quite clearly the time-step 6 t = 0.03, with the large random displacement (2D6t)'l2 = 0.24, smears out the details which are to be resolved. -
Multivariate modified Fourier series and application to boundary…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_08.pdf21 Apr 2009: Multivariate modified Fourier series and application to boundary. value problems. Ben AdcockDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, Cambridge CB3 0WA. United Kingdom. March 25, 2009. Abstract. In this paper we -
PowerPoint Presentation
www.damtp.cam.ac.uk/user/pvl/GOOSE/cox.pdf20 Sep 2009: Employment has fallen 24,000 in the last quarter. Unemployment now 6.5 per cent (4.6 per cent a year ago). -
Slide 1
www.damtp.cam.ac.uk/user/pvl/GOOSE/cannard.pdf20 Sep 2009: you will help save paper. Responses needed by Tue 24 November 2009. -
PublicationsDavid M.A. Stuart September 2009 1. Sophia Demoulini and…
www.damtp.cam.ac.uk/user/dmas2/public_ps/publistcurrent.pdf28 Sep 2009: Equations, 30 (4), (2007), 523–546.24 pages. ... 24. D. Stuart, “Perturbation theory for kinks”, Communications in Mathematical Physics,149 (1992), 433-462. -
Mathematical Tripos, Part IB : Electromagnetism, Dr Natalia Berloff…
www.damtp.cam.ac.uk/user/ngb23/EM/Chapter1.pdf16 Jan 2009: n E|. =1. ǫ0σ (23). nE|. = 0. (24). b). Let S carry current density s per unit length (charge crossing unit length in S in unittime). -
Mathematical Tripos, Part IB : Electromagnetism 3 Steady electric ...
www.damtp.cam.ac.uk/user/ngb23/EM/Chapter3.pdf29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to. -
feb24a1.eps
www.damtp.cam.ac.uk/user/hinch/talks/IC2009.pdf24 Feb 2009: µe = 0.47 for centre of massIC 2009, runout – p.24/59. -
CURRICULUM VITAE Name Nilanjana Datta Profession Affiliated Lecturer…
www.damtp.cam.ac.uk/user/nila/cv0809.pdf26 Apr 2009: 24) D. Bruss, N.Datta, A. Ekert, L.C. Kwek and C. Macchiavello, Multipartite entangle-. -
Existence and Newtonian limit of nonlinear bound states in ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/ed.pdf15 Oct 2009: 2ψ22) 2me2N Φ21. (e2N 1)2. 2me2Nψ22 4. rΦ1ψ2. = O(1),. (1.24). ... To see this, observe that by (1.24) and the preceding remarks, the equationF(l,Q,N, Φ1,ψ2; 0) = 0 amounts to. -
PII: 0377-0257(91)87016-Q
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM40_323.pdf13 Jul 2009: Lipscombe, R. Kennings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85 [l]). ... References. 1 G.G. Lipscomb, R. Keunings and M.M. Denn, J. Non-Newtonian Fluid Mech., 24 (1987) 85-96. -
Twistor theory and differential equations
www.damtp.cam.ac.uk/user/md327/jphysa09.pdf17 Sep 2009: It has been developed over the last30 years by the Oxford school of Penrose and Atiyah with the crucial early input from Ward[24, 25] and Hitchin [10, 11] and further ... Sächs. Akad. Wiss. Leipzig, Maths. Nat. Kl 69 262–77[24] Ward R S 1977 On -
Digital Object Identifier (DOI) 10.1007/s00220-009-0861-xCommun.…
www.damtp.cam.ac.uk/user/md327/DP09.pdf27 Jul 2009: 4.25)We now consider the reduction of the system (4.23),(4.24). Theorem 1.1 arises as acorollary of Proposition 4.2. ... to a coupled system whichincludes the Z3 two dimensional Toda chain [24] as a special case. -
The millennial atmospheric lifetimeof anthropogenic CO2 David Archer…
www.damtp.cam.ac.uk/user/mem/archer-carbon-tail08.pdf30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future. -
Chlamy_science_full
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Polinetal09.pdf31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,. -
VOLUME 80, NUMBER 4 P H Y S I ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysRevLett.80.704.pdf10 Jul 2009: For the same trial as in Fig. 5, this constantB is found to be20.90 and 24.29 for the large andsmall angle sides, respectively. -
http://journals.cambridge.org Downloaded: 31 Jul 2009 IP address:…
www.damtp.cam.ac.uk/user/hinch/publications/JFM66_1.pdf31 Jul 2009: SZAN-IAWSKI, A. 1972 Arch. Mech. 24, 555. TANNER, R. I. 1971 J. -
IOP PUBLISHING FLUID DYNAMICS RESEARCH Fluid Dyn. Res. 41 ...
www.damtp.cam.ac.uk/user/ngb23/publications/fdr09.pdf3 Sep 2009: V|ψ|2 dx = ψ2u v, (24). where v =. V dx, and by ψ the wavefunction of the bulk: ψ ψ as r. ... For thequartic term in the expression for the energy, we write using equation (24). -
Buoyancy driven miscible front dynamics in tilted tubesT. Séon,a! ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_17_031702.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex, 05, France. ... Rev.Fluid Mech. 24, 21 s1992d. 12F. Viana, R. Pardo, R. Yanez, and J. -
Instability of a high-speed submerged elastic jet
www.damtp.cam.ac.uk/user/hinch/publications/JFM288_311.pdf14 Jul 2009: 0.24 1. 0.18. (T 0.12. 0.06. 0 a. FIGURE 2. The growth rate 0 = aci as a function of wavenumber CI for the varicose mode of a ... The dashed curves are contours of pressure. 0.24. 0.18. 0 0.12. -
98PA207
www.damtp.cam.ac.uk/user/hinch/publications/PRSLA455_3201.pdf10 Jul 2009: The displacements xn as a function of position along theline, n, at different times t = 13.5, 24.5, 35.2, and 45.7. ... The different symbols are different times: , t = 13.5; , t = 24.5; , t = 35.2; ,t = 45.7. -
Noise and Synchronization in Pairs of Beating Eukaryotic Flagella ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinPolinTuval09.pdf16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P. -
334.eps
www.damtp.cam.ac.uk/user/hinch/publications/dropimpact.pdf8 Jun 2009: Calculation) method [24–26]. Although the THINC/WLIC method is a type of VOF method. ... for Fluid Dynamics, Morton KW, Baines MJ (eds) Vol. 24, Academic Press: New York, 1982; 273-. -
Effective dynamics for solitons in the nonlinear Klein Gordon ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/dl_final.pdf15 Oct 2009: Theorem 8 ([24]) If the nonlinearity satisfies the conditions given in 1.3.2 then (POS) is true. ... 24). The stabilityis in the same sense as in the previous theorem, see [17] for full details. -
PII: 0377-0257(93)80029-B
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM50_161.pdf13 Jul 2009: Denn, J. Non-Newtonian Fluid Mech., 24 (1987). 85-96. 6 P.J. Coates, R.C. -
persescribeericalma- trulyinedwith CPUwith iodicpen-la-tua- ize of…
www.damtp.cam.ac.uk/user/hinch/publications/JFG000957.pdf10 Jul 2009: 1 O f 11/3! (24). Figure 3 shows the settling velocity for a simple cubic arrayspherical particles as a function off 1/3. ... It can be seen that thenumerical results, obtained by considering the finite size ofparticles, yield close agreement with the -
Buoyant mixing of miscible fluids in tilted tubesT. Séon, ...
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_16_L103.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France. -
Long slender drops in a simple shear flow
www.damtp.cam.ac.uk/user/hinch/publications/JFM98_305.pdf23 Jul 2009: The differential equation can be integrated directly taking Po = 24 to produce an implicit expression for the shape. ... z = 0s-1 F 24( 1 - F2). which when substituted in the volume constraint yields. -
03pa0244
www.damtp.cam.ac.uk/user/hinch/publications/PRSLA460_2975.pdf10 Jul 2009: π2/24, 24/π) (0.4112, 7.639), although the numerical results suggestthat the analysis of 4 requires β 1 101 rather than β 1. ... 24/(βT ) (lower), wherein the factor 2 has been included to translate the lines. -
doi:10.1016/S0377-0257(97)00022-0
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM72_31.pdf10 Jul 2009: For A60,with an initial capillary pressure of 0.76 times the total elastic modulus, a pre-stretch of 3 anda finite extension of L1 = 24 (cf. ... The continuous curves are (a) for A40,L1 = 77 and P = 5; (b) for A60, L1 = 24 and P = 3; (c) for A80 L1 = 4.5 -
doi:10.1016/j.jnnfm.2006.04.003
www.damtp.cam.ac.uk/user/hinch/publications/JNNFM136_157.pdf8 Jul 2009: σtotn = 1Ca. κn, on ΓM(t). (24). Since there is no fixed boundary in this problem, the purely.Lagrangian approach is well adapted to it. ... Non-Newtonian Fluid Mech. 110 (2–3)(2003) 77–102. [24] R.F. Liang, M.R. Mackley, Rheological -
Rotation of small non-axisymmetric particles in a simple shear flow
www.damtp.cam.ac.uk/user/hinch/publications/JFM92_591.pdf23 Jul 2009: 7 2 13.3 19.7 34.0 % / a , 1.33 1.64 2.13 2-55 3.63 4.24 5. ... Even for r = 30 a 24 Yo variation from axisymmetry produces a drift in 6 from &7r to approximately. -
Generfc5.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_02.pdf13 May 2009: Van,cn(α, β, nz) =. 0(t α)a(t β)cenφ(t) dt, (4.23). withφ(t) = zt log(t α) log(t β) (4.24). ... Iserles (DAMTP, University of Cambridge). 24. References. [1] Milton Abramowitz and Irene A. -
PHYSICS OF FLUIDS 18, 041701 �2006� Laser-induced fluorescence…
www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_18_041701.pdf8 Jul 2009: B. PerrinLaboratoire Pierre Aigrain, UMR 8551, CNRS, Ecole Normale Supérieure, Département de Physique,24 rue Lhomond, 75231 Paris Cedex 05, France. -
Raining into shallow water as a description of the collapse of a…
www.damtp.cam.ac.uk/user/hinch/publications/JFM554_259.pdf8 Jul 2009: 2 a1.02r30. In both geometries, the final slope at the front is much lower than the slope thatwould be given by an internal angle of friction δ = tan1(µ) = 24. -
Shear-induced dispersion in a dilute suspension of rough spheres
www.damtp.cam.ac.uk/user/hinch/publications/JFM309_211.pdf14 Jul 2009: Phys. Fluids A 5, 13-24. SMART, J. R. & LEIGHTON, D. -
Extrinsic1b.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_09.pdf1 Dec 2009: 3.24). The corresponding result is the following. Theorem 2 Let f(y) be constant, then we have θ0 = 0, θ1 = ̺ and. ... θs = (s 1)̺, s 2.Proof We shall use formula (3.24) and proceed along the lines of theproof of Theorem.
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