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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. -
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. -
Dr H. Fawzi Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/user/hf323/M23-II-NA/Lect12.pdf30 Oct 2023: If. u(x,y) =k,lZ. ûk,leiπ(kxly). 24. is the Fourier expansion of u, the bivariate versions of the algebra of Fourier expansions gives(denoting ux = u/x and -
3C10b.dvi
www.damtp.cam.ac.uk/user/examples/3C10b.pdf26 Feb 2017: Cop. yrig. ht. 201. 7 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Quantum Fluids: Example Sheet 2. Problem 1. Mixtures of condensates. Consider a mixture of two different species ofbosons -
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 -
Microscopics
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/1415Lecture7.pdf27 Oct 2014: Some More on Curve Motion. Curve Motion - continued. Curve Motion - continued. Buckling Microtubules in Vesicles. Fygenson, et al, PRE 55, 850 (1997). Euler Buckling. Euler Buckling - continued. Euler Buckling - continued. Post-Buckling Behaviour. -
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. -
Action Principles
www.damtp.cam.ac.uk/user/examples/A11Lh.pdf22 May 2019: particles ‘talk’ to one another. Simplest is SU(5) with 52-1 = 24. -
The Architecture of Sponge Choanocyte Chambers MaximizesMechanical…
www.damtp.cam.ac.uk/user/gold/pdfs/sponges.pdf22 Feb 2024: 22].c Data from Ludeman et al. [24].d Data from Dahihande et al. ... 24]; Amphime-don queenslandica from Sogabe et al. [53]. indicates the hy-pothetical minimum diameter of E. -
University of Cambridge, DAMTP: Goldstein Lab
www.damtp.cam.ac.uk/user/gold/old_literature.html1 Aug 2019: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. References from article. More classic papers from the old literature. Contributions from Phil Nelson. J.C. Maxwell, "Solutions of problems," Camb. Dublin Math. J. 8,188 (1853) -
Publications: Refereed Journals Jing Gao & Arieh Iserles, "A …
www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/Papers.html22 Feb 2024: Num. Anal. 24 (2004), 365–391. A. Iserles, "On the global error of discretization methods for highly-oscillatory ordinary differential equations'', BIT 42 (2002), 561–599. ... Comp. Maths 14 (2001), 1–24. A. Iserles, "On Cayley-transform methods -
www.damtp.cam.ac.uk/user/ngb23/publications/names_n.txt
www.damtp.cam.ac.uk/user/ngb23/publications/names_n.txt18 Nov 2002: ODC 24. TH 25. NOS 26. GRa1 27. GRa2 28. GRa3 29. -
LUCIDITY PRINCIPLES supplement (index)
www.damtp.cam.ac.uk/user/mem/papers/LHCE/lucidity-supplem-index.html8 Jan 2020: McIntyre 1999. Last updated 24 Oct 2016. -
Stabilizing viscous extensional flows using reinforcement learning
www.damtp.cam.ac.uk/user/lauga/papers/205.pdf1 Dec 2021: Biological and bioinspired appli-cations at high Reynolds numbers include control and energyoptimization in fish swimming [24–26], gliding and perching[27], and locomotion in potential flows [28]. ... Dt 1 = Dt βt δt Qt. (24)To ensure convergence, it -
The bank of swimming organisms at the micron scale (BOSO-Micro)
www.damtp.cam.ac.uk/user/lauga/papers/195.pdf8 Jul 2021: cells swim [24–28]. Absolute pressure [29], pH [30] and even magnetic field [31] have also. ... Bi = 0.11 0.06 (n = 2),hB/Li = 0.63 0.24 (n = 9)). -
PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: 4,5,24–30]. The individual locomotion of spermatozoa was first studiedby G. I. ... 24). The complete solution of the Stokes equations in cylindricalcoordinates to the first order in kb is therefore finally given by. -
DYNAMICS SIGNIFICANT FOR CHEMISTRY
www.damtp.cam.ac.uk/user/mem/papers/ECMWF/ecmwf05.html9 Jan 2020: page 24 of the abovementioned Appendix III of the supplementary material for the Summer School), and in this paper with Tim Palmer written at a time when the idea was controversial. -
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:. -
Spatial pattern formation and polarization dynamics of a…
www.damtp.cam.ac.uk/user/ngb23/publications/spinor-josephson.pdf27 Jun 2010: Spatial pattern formation and polarization dynamics of a nonequilibrium spinorpolariton condensate. Magnus O. Borgh,1 Jonathan Keeling,2 and Natalia G. Berloff11Department of Applied Mathematics and Theoretical Physics, University of Cambridge, -
Title: The 2025 Motile Active Matter Roadmap Authors Gerhard ...
www.damtp.cam.ac.uk/user/gold/pdfs/Roadmap2025.pdf12 Jul 2024: Sistemi Complessi (ISC-CNR), Rome, Italy 23 Dipartimento di Fisica, Sapienza Università di Roma & INFN, Unità di Roma 1, Rome, Italy 24 Department of Biology and Biological Engineering, California Institute of -
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 -
Strong Data Processing Inequalitiesvia Sums of Squares Oisı́n…
www.damtp.cam.ac.uk/user/hf323/sdpi-sos.pdf11 Jun 2022: the integral representationlog(x) =. 10(x1)/(t(x1) 1)dt [24, Remark 2.10]. We. omit the details because of limitations on space. ... 2, no. 1, pp. 1–24, 2020. [8] O. Ordentlich and Y. -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-25-0.html28 Jan 2016: -
Cop yrigh tc © 2021 University ofCam bridge.Not tobequoted ...
www.damtp.cam.ac.uk/user/examples/3P6d.pdf2 Aug 2023: Show that, from the perspectiveof an observer in R1,24, these states are a graviton, an anti-symmetric tensor, two scalarsand two U(1) vector fields. -
1975-1980 1981-1990 1991-2000 2001-2010 2011-2020 2021-2030…
www.damtp.cam.ac.uk/user/mrep/webpubs.pdf11 Mar 2024: The kinematics of hexagonal magnetoconvection. Geo.Astro. Fluid Dyn., 24:109–136, 1983. 24. ... Phys. Fluids, 24,107103, 2012. 1975-1980 1981-1990 1991-2000 2001-2010 2011-2020 2021-2030. 184. -
B9s.dvi
www.damtp.cam.ac.uk/user/examples/B9s.pdf6 Oct 2021: 1923-24: de Broglie proposes wave-particle duality for matter, as for radiation. • -
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 -
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! -
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. -
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 -
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. -
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. -
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. -
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. -
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 -
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 -
Lent Term 2010 Mathematical Tripos Part III Hugh Osborn ...
www.damtp.cam.ac.uk/user/ho/SMprob3.pdf10 Mar 2010: dΓ =G 2F m. 5µ. 24(2π)4x2. (3 2x (2x 1) k̂.s. -
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 -
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 -
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), -
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 -
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. -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_WT_37C_Dorsal_2008-02-08-0.html28 Jan 2016: -
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. -
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 -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-08-24-0-c02.html28 Jan 2016: -
Controlling Confined Collective Organization with Taxis
www.damtp.cam.ac.uk/user/lauga/papers/224.pdf21 Mar 2024: Pedley and J. Kessler, Annu. Rev. Fluid Mech. 24, 313(1992). [16] B. ... 24] A. Creppy, F. Plouraboué, O. Praud, X. Druart, S. Cazin, H.Yu, and P.
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