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Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-24-0.html28 Jan 2016: -
dynrel
www.damtp.cam.ac.uk/user/tong/relativity/five.pdf3 Jul 2024: Here’s another example. The question seems a lit-. M m. Figure 24:. -
Dr H. Fawzi Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/user/hf323/M23-II-NA/Lect11.pdf27 Oct 2023: Dr H. Fawzi. Mathematical Tripos Part II: Michaelmas Term 2023. Numerical Analysis – Lecture 11. 3 Spectral Methods. Finite difference schemes rest upon the replacement of derivatives by a linear combination of functionvalues. This leads to the -
Part III Solitons, Instantons, and Geometry, Sheet One Maciej ...
www.damtp.cam.ac.uk/user/md327/PartIII_SIG_1.pdf29 Jan 2023: 22 x. 33 x. 24 = 1 and find its. degree. -
Microswimmers in vortices: dynamics and trapping
www.damtp.cam.ac.uk/user/lauga/papers/214.pdf7 Dec 2023: KaðzÞ)ffiffiffiffiffip2z. re%z 1þ4a. 2 %18z. þð4a2 %1Þð4a2 %9Þ. 128z2! "; (24). -
Cop yrig ht © 201 7 U nive rsity ...
www.damtp.cam.ac.uk/user/examples/3P11c.pdf11 May 2017: For finite action solutions to the Euler Lagrange equations (II.24), the fields |B|,|DΦ| and. ... 0. (iii) a(; z) and φ(, z) solve the Euler Lagrange equations (II.24) at λ = 1. -
Stress-Induced Dinoflagellate Bioluminescence at the Single Cell Level
www.damtp.cam.ac.uk/user/gold/pdfs/lunula.pdf6 Jul 2020: action potential—which arises from nonlinear, excitabledynamics—analysis of the flashes [24] indicates a timecourse much like that of two coupled capacitors chargingand discharging on different timescales. ... exactly [24], thus enabling a global fit -
CV: Matthew J. ColbrookEMAIL: m.colbrook@damtp.cam.ac.ukWEBSITE:…
www.damtp.cam.ac.uk/user/mjc249/pdfs/CV_MColbrook2024.pdf11 May 2024: 24. M.J. Colbrook, B. Roman, A.C. Hansen, How to compute spectra with error control, Physical Review Letters,2019.Cover highlight for issue.Prizes: Grade 1 Smith–Knight/Rayleigh–Knight -
clas
www.damtp.cam.ac.uk/user/tong/dynamics/one.pdf13 Sep 2023: 2.4.1 Noether’s Theorem 24. 2.5 Applications 26. 2.5.1 Bead on a Rotating Hoop 26. ... kinetic energy,. T(t2)T(t1) =X. i. ZFexti dri. X. i 6=j. ZFij dri (1.24). -
PowerPoint Presentation
www.damtp.cam.ac.uk/user/mjc249/talks/CMStats.pdf18 Dec 2022: Slide 24. Slide 25. Slide 26. Slide 27. -
PHYSICAL REVIEW FLUIDS 2, 074001 (2017) Imbibition with swelling: ...
www.damtp.cam.ac.uk/user/drh39/2017_suck.pdf1 Dec 2023: 24)]. 074001-14. IMBIBITION WITH SWELLING: CAPILLARY RISE IN. (a) (b) (c) (d). ... Fluids 17, 087104. (2005).[24] J. L. Sommer and A. Mortensen, Forced unidirectional infiltration of deformable porous media, J. -
J. Fluid Mech. (2017), vol. 829, pp. 89–111. c© ...
www.damtp.cam.ac.uk/user/drh39/2017_stability3d.pdf1 Dec 2023: brar. y of. Mus. ic, o. n 24. Oct. 201. 7 at. ... ic, o. n 24. Oct. 201. 7 at. 14:. 02:3. 6, s. -
On two‐phase modeling of dewatering pulp suspensions
www.damtp.cam.ac.uk/user/drh39/2021_pulp.pdf1 Dec 2023: 23 TMP (West Fraser) 112 580 1.59 36.4. 24 TMP (West Fraser) 229 390 1.50 35.6. ... found in Reference 24. At least four trials for each pulp suspension were. -
Halloween I
www.damtp.cam.ac.uk/user/mem/papers/LHCE/halloween1.html19 Oct 2013: For example, when the TearDrop IP attack was first posted to the web, less than 24 hours passed before the Linux community had a working fix available for download. -
Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...
www.damtp.cam.ac.uk/user/tong/qft/qft.pdf20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. ( -
BMC_talk_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_manchester.pdf18 Jun 2024: 𝑒𝑗 𝑒𝑗1. 𝑈 =. Back to the shift! . 24. 0 1. ... Slide 24: Back to the shift! Slide 25: Back to the shift! -
Preprint typeset in JHEP style - HYPER VERSION Lent ...
www.damtp.cam.ac.uk/user/tong/relativity/dynrel.pdf3 Jul 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25. -
PUBLICATIONS : NICHOLAS STEPHEN MANTON Research Papers 1. The ...
www.damtp.cam.ac.uk/user/nsm10/Publications.pdf17 Jul 2020: 24. Classical and Quantum Dynamics of BPS Monopoles (with G.W. Gibbons), NuclearPhysics B274 (1986) 183-224. ... 3. LMS Annual General Meeting 19/11/04, London Mathematical Society Newsletter 333(2005) 23-24. -
Part III Solitons and Instantons, Sheet Two Maciej Dunajski, ...
www.damtp.cam.ac.uk/user/md327/SIsheet2.pdf7 May 2007: 24 = 1 and find its degree. By calculating. Tr((dg g1)3) at the point on S3 where x4 = 1, or otherwise deduce that the formula. -
covertex-epje150246.dvi
www.damtp.cam.ac.uk/user/lauga/papers/112.pdf14 Nov 2019: This regularisationallows the use of simple, standard quadrature routines forall surface integrals in the regularised boundary integralequation [24]. ... Fauci, A. Medovikov, Phys. Fluids 17, 1. (2005).24. D.J. Smith, Proc. -
PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...
www.damtp.cam.ac.uk/user/drh39/2016_squishy.pdf1 Dec 2023: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H. -
Part III Applications of Differential Geometry to Physics, Sheet ...
www.damtp.cam.ac.uk/user/md327/PartIII_geom_2.pdf20 Jan 2020: 24 = 1 and find its. degree. By calculating Tr((dg g1)3) at the point on S3 where x4 = 1,or otherwise deduce that the formula. -
Limits and Powers of Koopman LearningMatthew J. Colbrook* Igor ...
www.damtp.cam.ac.uk/user/mjc249/pdfs/Koopman_foundations.pdf8 Jul 2024: man and von Neumann [21, 22], modern Koopman theory hasled to a renaissance of data-driven dynamical systems over thepast decade [7, 8, 23, 24, 25, 26, 27, 28]. -
J. Fluid Mech. (2024), vol. 978, R1, doi:10.1017/jfm.2023.849…
www.damtp.cam.ac.uk/user/lauga/papers/222.pdf2 Jan 2024: 24, 313–358.PELLE, D.W., BROKAW, C.J., LESICH, K.A. & LINDEMANN, C.B. 2009 Mechanical properties of the. -
Dancing Volvox: Hydrodynamic Bound States of Swimming Algae Knut ...
www.damtp.cam.ac.uk/user/gold/pdfs/waltzing.pdf10 Apr 2011: 24 APRIL 2009. 0031-9007=09=102(16)=168101(4) 168101-1 2009 The American Physical Society. ... 1) may be reduced, in rescaled coordinates r r=hand t tF=h2 with h R, to [24]. -
Nick_retirement_conference
www.damtp.cam.ac.uk/user/mjc249/talks/Nick_NEP_mjc.pdf17 Aug 2023: Eval #Eval #. 24. Example: Ghost essential spectra. 𝑥. 𝜂(𝑥). truncated domain. ... Slide 24: Example: Instability. Slide 25: Example: Ghost essential spectra. Slide 26: Example: Ghost essential spectra. -
Stochastic Voronoi Tessellations as Models forCellular Neighborhoods…
www.damtp.cam.ac.uk/user/gold/pdfs/Srinivasan_etal110324.pdf11 Mar 2024: 33, 958–972 (1962). [24] P. Rathie, On the volume distribution of the typi-cal Poisson–Delaunay cell, J. -
Multiflagellarity leads to the size-independent swimming speed of…
www.damtp.cam.ac.uk/user/lauga/papers/220.pdf2 Jan 2024: 1B), owing to the cell-to-cell variations inmetabolism and the number and morphology of flagella (24).Thanks to the large sample size of our experiments, we are able tomeasure the -
www.sciencemag.org/cgi/content/full/325/5939/487/DC1 Supporting…
www.damtp.cam.ac.uk/user/gold/pdfs/gears_SM.pdf21 May 2023: Goldstein. To whom correspondence should be addressed. E-mail: R.E.Goldstein@damtp.cam.ac.uk. Published 24 July 2009, Science 325, 487 (2009) DOI: 10.1126/science.1172667. ... Flagellar dynamics experiment. We analyzed 24 different cells and gathered -
Traveling waves are hydrodynamically optimal for long-wavelength…
www.damtp.cam.ac.uk/user/lauga/papers/182.pdf14 Dec 2020: Fluid Mech. 24, 313 (1992).[17] J. S. Guasto, R. Rusconi, and R. ... Fluid Mech. 762,. (2015). 123101-9. ERIC LAUGA. [24] T. D. Montenegro-Johnson and E. -
Lect08.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect08.pdf31 Jan 2005: Theorem 2.24 (The bottom row ofAk1) Suppose that the conditions of Remark 2.23 are satisfied. ... If|λr| is tiny then usually the rightmost sum in (2.5) tends to zero rapidly ask increases, so the convergence result of Theorem 2.24 can be useful for -
Jerome A. NeufeldBP Institute, Bullard Laboratories,Madingley Road,…
www.damtp.cam.ac.uk/user/jneufeld/JANeufeld_CV.pdf6 May 2019: Linden)6/24 lectures given on buoyancy-driven flows at the graduate levelPart III Mathematical Tripos, DAMTP, University of Cambridge. ... 737, 205–231. [24] S.S. Pegler, J.A. Neufeld, H.E. Huppert (2013) Topographic controls on gravity currents -
doi:
www.damtp.cam.ac.uk/user/drh39/2013_thixo.pdf1 Dec 2023: in figures 11 and 12. Figure 11 shows profiles of samples with different ageing timesTage on inclines of 20; figure 12 shows profiles on slightly steeper inclines of 24.As a -
Hypergeometric function - series representation Claim: F (a, b; ...
www.damtp.cam.ac.uk/user/bg268/Hypergeometric%20function%20as%20a%20series.pdf11 Mar 2020: Hypergeometric function - series representation. Claim:. F (a, b; c; z) =n=0. (a)n(b)n(c)n. zn. n!,. where (x)n = x(x 1).(x n 1), (x)0=1, is the Pochhammer symbol. The series is convergent in |z| < 1. The RSP at z = 1 prohibits the series -
4.6 Monodromy: the reason for the logarithmic term in ...
www.damtp.cam.ac.uk/user/bg268/Monodromy%20-%20need%20in%20log%20term.pdf11 Mar 2020: 4.6 Monodromy: the reason for the logarithmic term in the solution. Recall that forw′′ p(z)w′ q(z)w = 0, (1). in the vicinity of a RSP at z = 0 (WLOG - other points obtained by translation),there exist two linearly independent solutions of (1), -
Front-back asymmetry controls the impact of viscoelasticity on…
www.damtp.cam.ac.uk/user/lauga/papers/191.pdf8 Jul 2021: While recent numerical work reported that the elasticstresses in the wake of rigid cylinders depend on the orientation of the cylinder relative to its velocity[24], the dependence of the drag ... symmetry breaking, Phys. Fluids 24, 103102 (2012).[19] J. A -
Biofilm Growth under Elastic Confinement
www.damtp.cam.ac.uk/user/gold/pdfs/biofilms.pdf29 Apr 2022: Rev. 24, 661 (2000). [5] A. van Leeuwenhoek, An abstract of a letter from Mr.Anthony Leewenhoeck at Delft, dated Sep. ... Fluid Mech.778, 335 (2015). [24] R. E. Gibson, R. L. Schiffman, and S. -
Instability of an active fluid jet
www.damtp.cam.ac.uk/user/lauga/papers/212.pdf9 Nov 2022: III and IV. The setup of downward jets is relevant to range of biological situations,including a falling plume of a cell suspension, i.e., bioconvection [22–24]. ... Pedley, Bioconvection, Fluid Dyn. Res. 37, 1 (2005).[24] M. A. Bees, Advances in -
Collective stiffening of soft hair assemblies
www.damtp.cam.ac.uk/user/lauga/papers/178.pdf6 Jul 2020: For apoint force located at a distance h above the flat bottom sur-face, and assuming no-slip boundary conditions, the flow canbe obtained using the hydrodynamic image method ... Like us, they interpreted theirresults using the models of Refs. [24,25]. -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_WT_37C_Dorsal_2008-02-08-0.html28 Jan 2016: -
February 2021 EPL, 133 (2021) 44002 www.epljournal.orgdoi:…
www.damtp.cam.ac.uk/user/lauga/papers/188.pdf8 Jul 2021: 19]. Ex-perimental work on bacteria in their swimming [20–24]or swarming states [25,26], algae [27,28] and sperma-tozoa [29,30] provide diverse examples of correlated,collective dynamics ... 23] Wolgemuth C. W., Biophys. J., 95 (2008) 1564.[24] Sokolov -
3 The Harmonic Oscillator I now want to use ...
www.damtp.cam.ac.uk/user/dbs26/PQM/chap3.pdf18 Oct 2019: 2nm! cncn1 = xn ein. (3.24). Equation (3.23) shows that hXi oscillates sinusoidally at exactly the classical frequency! ... 24 –. appreciable, then, to reasonable accuracy, all the terms that contribute to (3.31) oscillate. -
The non-Gaussian tops and tails of diffusing boomerangs
www.damtp.cam.ac.uk/user/lauga/papers/136.pdf29 May 2017: DOI: 10.1039/c6sm02649d. rsc.li/soft-matter-journal. Soft Matter. PAPER. Publ. ishe. d on. 24. ... L. Ekiel-Jeżewska and E. Wajnryb, J. Chem. Phys., 2015, 142, 214902.24 B. -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-25-0.html28 Jan 2016: -
dynrel
www.damtp.cam.ac.uk/user/tong/relativity/seven.pdf3 Jul 2024: 7. Special Relativity. Although Newtonian mechanics gives an excellent description of Nature, it is not uni-. versally valid. When we reach extreme conditions — the very small, the very heavy or. the very fast — the Newtonian Universe that -
Opto-fluidically multiplexed assembly and micro-robotics
www.damtp.cam.ac.uk/user/lauga/papers/223.pdf28 Feb 2024: With rapid implementation and advanced control,it might be feasible to position one particle every fewmicrometers, which is the typical length scale over whichthe flow fields exhibit significant decay22,24. ... eLight 1, 7 (2021). 24. Liao, W. et al. -
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 -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-08-24-0-c02.html28 Jan 2016: -
How do cicadas emerge together? Thermophysical aspects of their…
www.damtp.cam.ac.uk/user/gold/pdfs/cicadas.pdf1 Feb 2024: Collective behavior via communication [20] is foundin many contexts: bacterial quorum sensing [21], ant foraging[22–24], and bird flocking [25]. ... Acad. Sci. USA 110, 13769 (2013). [24] O. Feinerman, I. Pinkoviezky, A. -
italy_mjc
www.damtp.cam.ac.uk/user/mjc249/talks/Italy_mpEDMD.pdf6 Apr 2024: Slide 23: Convergence of measures. Slide 24: Further convergence. Slide 25: Lorenz system.
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