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  2. Effective approximation for the linear time-dependent Schrödinger…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_05.pdf
    16 Jul 2012: 24 P. Bader, A. Iserles, K. Kropielnicka & P. Singh. of accuracy exhibited in Figs 4.3–4 is clearly in excess of O(ε7/2. ),
  3. ISlecture_notes_2012_part1.dvi

    www.damtp.cam.ac.uk/user/md327/ISlecture_notes_2012.pdf
    10 May 2012: 24. 2.2 Inverse scattering transform for KdV. 252.2.1 Direct scattering. 272.2.2 Properties of the scattering data. ... dx. 24. Figure 2.1: Sine–Gordon Kink. Kink. x. Note that the Sine–Gordon equations didn’t enter the discussion at this stage.
  4. Manuscript submitted to Website: http://AIMsciences.orgAIMS’…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2012_08.pdf
    5 Sep 2012: 7.1. A new scheme of Dirichlet series for particular systems of the form(24). ... Byletting z = P 1y, the system (24) is equivalent to a transformed dynamical system.
  5. Forces between single pairs of charged colloids in aqueous ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/ufk_papers/charged_membranes/dlvo-ot.pdf
    3 Oct 2012: Chem. Phys. 81, 6320 1984. 24 E. Allahyarov, H. Lowen, and S.
  6. The development of concentration gradients in a suspension of…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/HillesdonPedleyKessler95.pdf
    2 Sep 2012: and, by equation (24) and the integral (21),. dO _f12. d z (0)= (27). ... terms in equation (23) and the oxygen consumption term in equation (24) are zero.
  7. The hydrodynamics of swimming microorganisms

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/LaugaPowers09.pdf
    27 Aug 2012: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.
  8. 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: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k.
  9. Holographic Dual of the Lowest Landau Level David Tong ...

    www.damtp.cam.ac.uk/user/tong/talks/hololll.pdf
    15 Oct 2012: Aspects of fermions in magnetic AdS geometries. have been previously discussed in [20, 21, 22, 23, 24].
  10. Pattern formation in a suspension of swimming microorganisms:…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ChildressLevandowskySpiegel75.pdf
    2 Sep 2012: 2 3 ) pDV-D'@iF28@ = 0, (2.24). D(D = 0, x = - 1 , o. ( ... To see how these expansions proceed, we first note that (2.24) may be integrated, using (2.25), to dbtain 0 so CDdS(76Z2)/ -1 V d Z = 0.
  11. qjmam0117.tex

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/MagarGotoPedley03.pdf
    2 Sep 2012: NUTRIENT UPTAKE BY A SELF-PROPELLED STEADYSQUIRMER. by VANESA MAGAR†. (Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Silver Street, Cambridge CB3 9EW). TOMONOBU GOTO. (Department of Mechanical Engineering,
  12. PCE845.fm

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard03.pdf
    2 Sep 2012: Plant, Cell and Environment. (2003). 26,. 1–15. 2003 Blackwell Publishing Ltd. 1. Blackwell Science, LtdOxford, UKPCEPlant, Cell and Environment0016-8025Blackwell Science Ltd 200226845Role of cytoplasmic streaming in symplastic transportW. F.
  13. Physics of chemoreception

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/BergPurcell77.pdf
    2 Sep 2012: Pi[Vr/(r, - a)]2 = 277a2D2/rl(r1 - a)4. (24)The volume involved is approximately 8irr 2(r, - a), so the total stirring power ex-pended in this region
  14. Dynamics of filaments and membranes in a viscous fluid ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Powers10.pdf
    2 Sep 2012: T̂ = N̂. 24. The curvature is the rate of rotation of T̂ about B̂, and. ... Comparison of Eqs. 21–24 reveals that2 =1. 2 22 and 3 = , where is the angle between.
  15. doi:10.1016/j.physrep.2003.08.001

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/vansaarloos.pdf
    31 Oct 2012: 1603.24. Propagation of a front into an unstable ferromagnetic state. 1623.25.
  16. Synchronization and Collective Dynamics in a Carpet of Microfluidic…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/UchidaGolestanian10.pdf
    2 Sep 2012: On the other hand, recent advances frommicron-scale magnetically actuated tails [24] to syntheticmolecular rotors [25] now allow fabrication of arrays ofactive tails that can stir up the fluid. ... 2007); Small 4, 111 (2008).[24] R. Dreyfus et al.,
  17. lectures2012.dvi

    www.damtp.cam.ac.uk/user/phh/mathbio/lectures2012.pdf
    6 Jun 2012: ithou. t per. mis. sion. P.H.Haynes Part II Mathematical Biology Lent Term 2012 24.
  18. Collective Hydrodynamics of Swimming Microorganisms: Living Fluids

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KochSubramanian11.pdf
    2 Sep 2012: FL43CH26-Koch ARI 15 November 2010 14:32. Collective Hydrodynamics ofSwimming Microorganisms:Living FluidsDonald L. Koch1 and Ganesh Subramanian21 School of Chemical and Biomolecular Engineering, Cornell University, Ithaca,New York 14853; email:
  19. [ 7 9 6 ] WAVE PROPAGATION ALONG FLAGELLA ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Machin58.pdf
    27 Aug 2012: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.
  20. Shape of a Ponytail and the Statistical Physics of ...

    www.damtp.cam.ac.uk/user/gold/pdfs/ponytail_prl.pdf
    13 Feb 2012: The reconstructed arc lengthscluster tightly around 24:50 0:05 cm (inset histogram), demonstrating the accuracy of the image processing and analysismethodology.
  21. 1 23 Annals of Global Analysis andGeometry ISSN 0232-704X ...

    www.damtp.cam.ac.uk/user/md327/DD12_file.pdf
    23 Jan 2012: The explicit expressionfor 8 is given by (5.24) and is linear in the highest derivative y(7). ... Springer, Berlin (1995)24. Hitchin, N.: Complex manifolds and Einstein’s equations, in Twistor Geometry and Non-Linear systems.
  22. P H Y S I C A L R ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Hatwalneetal04.pdf
    2 Sep 2012: On time scales shorter than , effects associ-ated with spatiotemporal correlations in Q [23] intervene.For a drop [24] or a film [22] of size L, the tails will be cutoff ... Tu, Phys. Rev. E 64, 011902. (2001).[24] G.V. Soni et al., Biophys.
  23. 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: here some of them, [1, 7, 10, 11, 18–21, 23, 24, 26–28, 32, 33]. ... J. Phys. A 24(24),. 5751–5762 (1991). http://stacks.iop.org/0305-4470/24/575131. Ralston, A., Rabinowitz, P.: A First Course in Numerical Analysis, 2nd edn.
  24. (This is a sample cover image for this issue. ...

    www.damtp.cam.ac.uk/user/md327/DH12_file.pdf
    16 May 2012: Furthermore, weknow that Eqs. (3.14) and (3.15) are equivalent to (3.24). ... Eqs. (3.14) and (3.15)are equivalent to (3.24). The integrability conditions force δ0 = 0.
  25. Minimal model for synchronization induced by hydrodynamic…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Qianetal09.pdf
    2 Sep 2012: The data wedisplay in this article are for a dimensionless gap size / R= 0.24. ... 24. Assuming all balls are far apart, we again use the Oseenmodel, Eq.
  26. Bacterial swimming and oxygen transport nearcontact linesIdan Tuval†, …

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Tuvaletal05.pdf
    2 Sep 2012: Onemilliliter of 24-h stock was added to 50 ml of TB and incubated for18 h. ... O. (1992) Annu. Rev. Fluid Mech. 24, 313–358.12. Hillesdon, A. J., Pedley, T.
  27. 201203575 15109..15114

    www.damtp.cam.ac.uk/user/gold/pdfs/oocyte_streaming.pdf
    19 Sep 2012: Materials and MethodsLive Imaging. Females were fattened on yeast for 16–24 h at 25 C. ... 24. Wolff K, Marenduzzo D, Cates ME (2012) Cytoplasmic streaming in plant cells: the roleof wall slip.

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