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  2. C0SM01121E 3074..3082

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GolestanianYeomansUchida11.pdf
    2 Sep 2012: Garland, New York, 2001).13 P. Satir, J. Cell Biol., 1968, 39, 77.14 M. ... Julicher, New J. Phys., 2000, 2, 24.18 J. R. Blake and M.
  3. VOLUME 84, NUMBER 13 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/WuLibchaber00.pdf
    2 Sep 2012: 2Department of Physics, University of Pittsburgh, Pittsburgh, Pennsylvania 152603Center for Studies in Physics and Biology, Rockefeller University, New York, New York 10021. ... In this paper we study a new situ-ation with two types of particles in a
  4. Effective approximation for the linear time-dependent Schrödinger…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_05.pdf
    16 Jul 2012: R1 = 12W[1] = 12τω. 12x 124τ. 3ω(xV )2. from W[1].Although the new W [1] and W[1] are more complicated, the computations are now.
  5. Beyond consistent reconstructions: optimality and sharp bounds for…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_10.pdf
    20 Oct 2012: To overcome the issues inherent to consistent reconstructions the new approach of generalized sam-pling was introduced in [1, 4, 5]. ... Our main result in this section is to present new, sharp bounds.We first require the following lemma:.
  6. Pattern formation in a suspension of swimming microorganisms:…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ChildressLevandowskySpiegel75.pdf
    2 Sep 2012: A N D E. A. SPIEGEL Department of Astronomy, Columbia University, New York 10027. ... continues to act as the instability develops and influences the formation of a new stable equilibrium (should any exist), just as temperature differences remain the
  7. ISlecture_notes_2012_part1.dvi

    www.damtp.cam.ac.uk/user/md327/ISlecture_notes_2012.pdf
    10 May 2012: The idea behind the followingTheorem is to seek a canonical transformation such that in the new variables H = H(P1,. , ... d. dt. R. |Ψ|2dx = 0. The way physicists discover new elementary particles is by scattering experiments.
  8. On optimal wavelet reconstructions from Fourier samples:linearity and …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_07.pdf
    3 Sep 2012: 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
  9. Collective Hydrodynamics of Swimming Microorganisms: Living Fluids

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KochSubramanian11.pdf
    2 Sep 2012: of collective motion; and to considerpossible new directions in the study of living fluids. ... This continuum is a new type of complex fluid, a living fluid whose microstructuralelements (the cells) can convert nutrients into mechanical energy to drive
  10. Real-time particle tracking at 10,000 fpsusing optical fiber…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/optical_tweezers/Otto2010.pdf
    3 Oct 2012: The progress in the development of new cameras and illuminationsystems has made it possible to extend the acquisition speed of this tracking method to themillisecond timescale [13–15].
  11. Orientational Order and Instabilities in Suspensions of…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SaintillanShelley07.pdf
    2 Sep 2012: ShelleyCourant Institute of Mathematical Sciences, New York University, New York, New York 10012, USA. ... These nonlinear dynamics are of funda-mental interest, offering a new paradigm for pattern for-mation and self-organization in nonequilibrium
  12. Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...

    www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf
    8 Mar 2012: L. Schiff Quantum Mechanics, McGraw-Hill Book Company. • B. Dutta-Roy Elements of Quantum Mechanics, New-Age Science Limited. ... aε0. (4.3.3). (i) as large and negative: new bound state not quite appeared;.
  13. Dynamics of filaments and membranes in a viscous fluid ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Powers10.pdf
    2 Sep 2012: Thus, resistive-force theory is usually justified in afirst approach to a new problem, but its predictions mustalways be viewed with a critical eye.
  14. RAPID COMMUNICATIONS PHYSICAL REVIEW E 86, 040902(R) (2012)…

    www.damtp.cam.ac.uk/user/gold/pdfs/self_generated_flows.pdf
    22 Oct 2012: Enkeleida Lushi,1,2, Raymond E. Goldstein,3 and Michael J. Shelley11Courant Institute of Mathematical Sciences, New York University, New York 10012, USA. ... Phys. Rev. E 83, 061907 (2011).[11] E. Lushi, Ph.D. dissertation, New York University, 2011.[12]
  15. The hydrodynamics of swimming microorganisms

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/LaugaPowers09.pdf
    27 Aug 2012: This growth has beenspurred in part by new experimental techniques for studyingcell motility. ... Thus the relation betweenforce and the motion of the flagellum can be directly assessed.These measurements of force allow new approaches tobiological
  16. lectures2012.dvi

    www.damtp.cam.ac.uk/user/phh/mathbio/lectures2012.pdf
    6 Jun 2012: Cop. yrig. ht. 201. 2 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Part II Mathematical Biology Lent Term 2012. lecturer: Professor Peter Haynes (phh@damtp.cam.ac.uk). May 31, 2012. These
  17. Hydrodynamic Phenomena in Suspensions of Swimming Microorganisms

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/PedleyKesslerARFM92.pdf
    27 Aug 2012: Annu. Rev. Fluid Meek. 1992. 24: 313-58 Copyright 1992 by Annual Reviews Inc. All rights reserved. HYDRODYNAMIC PHENOMENA. IN SUSPENSIONS OF. SWIMMING MICROORGANISMS. T. J. Pedley. Department of Applied Mathematical Studies, University of Leeds,
  18. Partial Differential Equations Example sheet 2 David…

    www.damtp.cam.ac.uk/user/dmas2/public_ps/pdex2.pdf
    8 Nov 2012: transform.The new structure in Hilbert (as compared to Banach) spaces is the notion of orthog-. ... In fact this new continuityproperty ensures that a positive distribution can be extended uniquely as a map.
  19. doi:10.1016/j.physrep.2003.08.001

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/vansaarloos.pdf
    31 Oct 2012: W. van Saarloos/Physics Reports 386 (2003) 29–222 37. been able to derive from it important new and exact results for the power law convergence of thevelocity and shape of ... The fact that starting fromthis concept one can set up a fully explicit
  20. microswimmers

    www.damtp.cam.ac.uk/user/gold/pdfs/microswimmers.pdf
    3 Sep 2012: Our hope isthat modern microscopy and imaging techniques. will produce novel insights into phase dynamics andinspire a new class of models that allow quantitativecomparisons between theory and experiments. ... Dworkin, eds.,Oxford U. Press, New York (1997
  21. There is more than one way to turn a spherical cellular monolayer…

    www.damtp.cam.ac.uk/user/sh753/pdfs/2011_Hoehn_Hallmann_Inversion_V.globator.pdf
    27 May 2012: RESEARCH ARTICLE Open Access. There is more than one way to turn a sphericalcellular monolayer inside out: type B embryoinversion in Volvox globatorStephanie Höhn and Armin Hallmann. Abstract. Background: Epithelial folding is a common
  22. Stratosphere‐Troposphere Exchange

    www.damtp.cam.ac.uk/user/mem/papers/STE/holton-etal-strat-trop-revsgeoph95.pdf
    22 Aug 2012: STRATOSPHERE-TROPOSPHERE EXCHANGE. James R. Holton • Peter H. Haynes 2 and Michael E. Mcintyre 2 Anne R. Douglass 3 and Richard B. Rood 3 Leonhard Pfister 4. Abstract. In the past, studies of stratosphere-tropo- sphere exchange of mass and
  23. The development of concentration gradients in a suspension of…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HillesdonPedleyKessler95.pdf
    2 Sep 2012: 68). At t = t 2 let the new position of the b o u n d a r y be z = (t2); therefore 0[(t2) , t2]----0. ... Otherwise, a new guess for the b o u n d a r y position must be m a d e and the problem re-integrated from t = t.
  24. Instabilities and Pattern Formation in Active Particle…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SaintillanShelley08.pdf
    2 Sep 2012: David Saintillan and Michael J. ShelleyCourant Institute of Mathematical Sciences, New York University, New York, New York 10012, USA.
  25. VOLUME 80, NUMBER 17 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/WigginsGoldstein98.pdf
    2 Sep 2012: ica Educational Corporation, New York, 1966).[4] Sir J. Lighthill, Mathematical Biofluiddynamics(SIAM,. ... 18] L. Landau and L. Lifshitz,Theory of Elasticity(Pergamon,New York, 1986), p.
  26. P H Y S I C A L R ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Hatwalneetal04.pdf
    2 Sep 2012: Alberts et al., Molecular Biology of the Cell (Garland,. New York, 2002).[4] R. ... Bray, Cell Movements (Garland, New York, 2001), 2nded. [12] M. Fontes and D.
  27. Experimental investigations of elastic tail propulsion at low…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/YuLaugaHosoi06.pdf
    2 Sep 2012: Acad. Sci. U.S.A. 94, 11307 1997. 3H. C. Berg, E. coli in Motion Springer-Verlag, New York, 2004.4D. ... Rev. Fluid Mech. 9, 339 1977. 16S. Camalet and F. Julicher, “Generic aspects of axonemal beating,” New J.Phys.
  28. [ 7 9 6 ] WAVE PROPAGATION ALONG FLAGELLA ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Machin58.pdf
    27 Aug 2012: New York: McGraw Hill.PRTNOLE, J. W. S. (1957). Myogenic Rhythms. In Recent Advances in Invertebrate Physiology,.
  29. VOLUME 93, NUMBER 9 P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Dombrowskietal04.pdf
    2 Sep 2012: A. Shapiro and M.Dworkin (Oxford University Press, New York, 1997),p. 417.
  30. Numerical Analysis Arieh IserlesCentre for Mathematical…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_01.pdf
    28 Feb 2012: However, contemporary physicsresearch leads to a number of new and important computational challenges. ... Davis, P. J. & Rabinowitz, P. (1975), Methods of Numerical Integration, AcademicPress, New York.
  31. Manuscript submitted to Website: http://AIMsciences.orgAIMS’…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_08.pdf
    5 Sep 2012: Some discussion and a numerical experiment areaccordingly carried out for the new Dirichlet approximation. ... Theorem 7.2. Denoting the truncation of the new Dirichlet series (30) by.
  32. G2-structures and twistor theory Maciej Dunajski Department of…

    www.damtp.cam.ac.uk/user/md327/banff2012.pdf
    29 Apr 2012: Examples from twistor theory/algebraic geometry. Mixture of old and new: Classical invariant theory (Young, Sylvester),algebraic geometry, twistor theory (Penrose, Hitchin).
  33. Generic Conditions for Hydrodynamic Synchronization Nariya Uchida1,*…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian11.pdf
    2 Sep 2012: To derive it, first wereparametrize the trajectory by the new phase variable ðÞ that makes the intrinsic phase velocity con-stant: 0ðÞ FðÞ=jR0ðÞj 2=T. ... 17] Y. Kuramoto, Chemical Oscillations, Waves, andTurbulence (Springer, New York, 1984).
  34. Hydrodynamic interactions between rotating helices MunJu Kim and…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KimPowers04.pdf
    2 Sep 2012: The new ele-ment in this configuration may be a steady attractive(orrepulsive) force between the two helices.
  35. LH8417 2..5

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SimhaRamaswamy02.pdf
    2 Sep 2012: Hoffmann (Springer-Verlag,New York, 1990); B. L. Partridge, Sci. Am. 246, No.
  36. Invited Article

    www.damtp.cam.ac.uk/user/gold/pdfs/topo_constraints.pdf
    3 Sep 2012: This relaxation process is quite rapid, and is ultimately constrained by the topologyof the knot: the wire cannot self-intersect, but in its new equilibrium state makes contact withitself at several ... The wire then finds a new equilibrium, subject now
  37. Dance of the microswimmersEric Lauga and Raymond E. Goldstein ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/LaugaGoldstein12.pdf
    2 Sep 2012: Our hope isthat modern microscopy and imaging techniques. will produce novel insights into phase dynamics andinspire a new class of models that allow quantitativecomparisons between theory and experiments. ... Dworkin, eds.,Oxford U. Press, New York (1997
  38. Synchronization and Collective Dynamics in a Carpet of Microfluidic…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian10.pdf
    2 Sep 2012: Then, the director is randomized on the thin-ning spiral arm, which collapses and proliferates a cascadeof new defects.Thermal fluctuations.—We then introduce the ther-. ... Soc. 70, 303 (1971).[28] Y. Kuramoto, Chemical Oscillations, Waves, and.
  39. Nature’s Microfluidic Transporter: Rotational Cytoplasmic Streaming…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/vandeMeentTuvalGoldstein08.pdf
    2 Sep 2012: New microfluidic methods exploiting the rota-tional streaming paradigm may be of significant interest.
  40. A macroscopic scale model of bacterialflagellar bundlingMunJu Kim,…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Kimetal03.pdf
    2 Sep 2012: Y.-T.,. Brokaw, C. J. & Brenner, C. (Plenum, New York), Vol.
  41. PRL 95, 204501 (2005) P H Y S I ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HernandezOrtizStoltzGraham05.pdf
    2 Sep 2012: Bray, Cell Movements: From Molecules to Motility(Garland, New York, 2001), 2nd ed.
  42. Fluid Velocity Fluctuations in a Suspension of Swimming Protists ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/RushkinKantslerGoldstein10.pdf
    2 Sep 2012: The relationship between suspensions of microorgan-isms and of sedimenting particles takes on new signifi-cance in light of measurements of velocity fields aroundfreely swimming organisms [5], which emphasized that theStokeslet
  43. BIT Numerical Mathematics (2008) 48: 743–761 Published online: 28 ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_01.pdf
    22 Mar 2012: N. G. De Bruijn, Asymptotic Methods in Analysis, Dover Publications Inc., New York,1981. ... 535–562. 22. F. W. J. Olver, Asymptotics and special functions, in Computer Science and AppliedMathematics, Academic Press, New York, London, 1974.
  44. DOI 10.1140/epje/i2004-10152-7 Eur. Phys. J. E 17, 493–500 (2005) ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ReichertStark05.pdf
    2 Sep 2012: coli in Motion (Springer, New York, 2004).6. M.D. Manson, P.M. Tedesco, H.C. ... 23. B.A. Finlayson, The Method of Weighted Residulas andVariational Principles (Academic Press, New York, 1972).
  45. BIT Numer MathDOI 10.1007/s10543-011-0355-z Quadrature methods for…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2009_01.pdf
    22 Mar 2012: Numerical Mathe-matics and Scientific Computation. Clarendon, Oxford University Press, New York (1995). ... Dover, New York (2001)32. Vandewalle, S.: Parallel Multigrid Waveform Relaxation for Parabolic Problems.
  46. Celestial Mechanics and Dynamical Astronomy manuscript No.(will be…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_02.pdf
    2 Aug 2012: Φ′(Q)T p = q, suchthat K1 depends only on the new momenta. ... εH1 δ < 0,. consequently H0 pt > 0, and the new Hamiltonian to consider is.
  47. 201203575 15109..15114

    www.damtp.cam.ac.uk/user/gold/pdfs/oocyte_streaming.pdf
    19 Sep 2012: Curr Biol 7:468–478. 33. Karpova N, Bobinnec Y, Fouix S, Huitorel P, Debec A (2006) Jupiter, a new Drosophilaprotein associated with microtubules. ... Cell 134:843–853. 47. Berg HC (1993) Random Walks in Biology (Princeton Univ Press, Princeton,New
  48. Flows driven by flagella of multicellular organismsenhance long-range …

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Shortetal06.pdf
    2 Sep 2012: Halvorson, H. O. &Monroy, A. (Liss, New York), pp. 221–256. 11.
  49. doi:

    www.damtp.cam.ac.uk/user/gold/pdfs/vesicles_jfm_online.pdf
    17 Apr 2012: Wethen used knowledge of this system to suggest a new method for estimating membraneviscosities.

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