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www.damtp.cam.ac.uk/user/sje30/papers/godfrey2009_review.pdf14 Jun 2014: T. Schmidt and M. Buzzard, J. Neurobiol., 1993, 24, 384–399.30 L. ... B. Feller, Neuron, 1999, 24,. 673–685.62 E. Marder and J. M. -
TH EJ OU RN AL OF CE LL BIO ...
www.damtp.cam.ac.uk/user/sje30/papers/kishi2005.pdf14 Jun 2014: 3, 8, 9, 20, and 24). For theother five, however, in situ hybridization revealed a punctatepattern of expression associated with individual muscle fibers(Fig. -
4 The Heat Equation Our next equation of study ...
www.damtp.cam.ac.uk/user/dbs26/1BMethods/Heat.pdf4 Nov 2014: P. t= K. 2P. x2(4.24). where the diffusion constant K can be identified as 〈y2〉/2t.THIS SECTION NEEDS MORE WORK! -
J. Fluid Mech. (2014), vol. 742, pp 50–70. c© ...
www.damtp.cam.ac.uk/user/lauga/papers/86.pdf27 Feb 2014: where. D1 = 2bαα. sinh2(αGt. ). 2αG. , (5.24). D2 = 1α. -
Self-organization in the developing nervoussystem: theoretical models …
www.damtp.cam.ac.uk/user/sje30/papers/eglen2009_hfsp.pdf14 Jun 2014: Neurosci. 24, 356–369. Jaubert-Miazza, L, Green, E, Lo, F, Bui, K, Mills, J, and Guido, W (2005).“Structural and functional composition of the developingretinogeniculate pathway in the mouse.” Visual ... Neurosci. 14, 1486–1495. Luo, L (2006). -
PHYSICS OF FLUIDS 26, 082001 (2014) Asymmetric steady streaming ...
www.damtp.cam.ac.uk/user/lauga/papers/95.pdf29 Aug 2014: parameter, %. We thuswrite. u(0) = u0 % u% O (%2), (24). p(0) = p0 % p% O (%2), (25). ... û% = 0. (31)The fist boundary condition satisfied by the corrective flow û% is found by Taylor expanding theboundary condition (21) to the first order in %. -
, 20131160, published 26 February 201411 2014 J. R. ...
www.damtp.cam.ac.uk/user/gold/pdfs/LagLockSyncSlip.pdf26 Feb 2014: detailed three-dimensional tomographic analysisrevealed that nexins are in fact one and the same with the dyneinregulatory complex, collectively termed the NDRC [24]. -
On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...
www.damtp.cam.ac.uk/research/afha/bogdan/Asymptotic_10a.pdf19 Jun 2014: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... 24), yet it is unclear how areal-world setup can be implemented where signals are sparse in atransform domain. -
UNIVERSITY OF CAMBRIDGECENTRE FOR MATHEMATICAL SCIENCES DEPARTMENT OF …
www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/HowTo14.pdf31 May 2014: 24. The editorial process Once you’ve submitted a paper to a journal, it followsa set pattern:. -
Small particles in a viscous fluid
www.damtp.cam.ac.uk/user/hinch/teaching/CISMejh12.pdf12 May 2014: 24. More simple properties1. A useful result. Let uS (x) be a Stokes flow with F = 0 in V , and let u(x) be anyother incompressible flow, then. ... uixj. =. xj. (σSijui. )σSijxj=F=0. ui (4). Hence result by divergence theorem.24. -
Thesis.dvi
www.damtp.cam.ac.uk/user/md327/simon_thesis.pdf6 Oct 2014: ǫABǫF ′Q′C̃A′B′E′Q′ ǫAB(ǫA′E′ǫ. F ′. B′ ǫF ′. A′ ǫB′E′)R. 24+ ǫA′B′ǫ. ... 24. a,b holomorphic functions on C. For these to agree we require. -
Image Processing for Fluid Dynamics Stuart Dalziel DL ...
www.damtp.cam.ac.uk/research/lab/digimage/track2d.pdf21 Oct 2014: Image Processing for Fluid Dynamics. Stuart Dalziel. DL Research Partners 1993 – 2001. Version 2.3 DL Research Partners; September 2001 1. Contents Contents.1. 1 Concept.1. 2 DigImage: Particle Tracking.3 2.1 IMAGE CAPTURE. 3 2.2 PARTICLE -
Chapter 1 Theoretical models in low-Reynolds-number locomotionON SHUN …
www.damtp.cam.ac.uk/user/lauga/papers/96.pdf30 Aug 2014: t(t v). ], (1.24). where t and n are, respectively, the local tangent and normal vectors along the filament. ... 1.24), up to the unknown translational and rotational velocities,(U,), which will be determined by imposing the overall force-free and -
Mathematical Methods University of Cambridge Part IB Mathematical…
www.damtp.cam.ac.uk/user/dbs26/1BMethods/FourierS.pdf21 Oct 2014: πFn(θ φ) dφ = f(θ) , (1.24). – 8 –. using property ii) of the Fejér kernel. -
The hydrodynamics of swimming microorganisms
www.damtp.cam.ac.uk/user/lauga/papers/32.pdf9 Sep 2014: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap. -
Journal of Marine Research, 72, 47–72, 2014 Mixing by ...
www.damtp.cam.ac.uk/user/lauga/papers/93.pdf28 Nov 2014: Pg ρ0. r<. wb dV (24). and thus we obtain the scaling relation. ... ρ0a4. )a3 = D. 24. μa7, (53). where we have substituted κ/N 2 = 4/ν. -
Image Processing for Fluid Dynamics © Stuart Dalziel DL ...
www.damtp.cam.ac.uk/research/lab/digimage/digifile.pdf21 Oct 2014: DiDiDiDiggggImage: DigiFile Utility Index. Version 2.3 DL Research Partners September 2001 24. -
Bifurcation in electrostatic resistive drift wave turbulenceRyusuke…
www.damtp.cam.ac.uk/user/mem/oldftp/jeff-parker-numata-pp07.pdf13 Jul 2014: Arakawa’s method is used for evaluation of thePoisson bracket.24 The time stepping algorithm is the third. -
doi:
www.damtp.cam.ac.uk/user/hinch/publications/JFM737_232.pdf22 Jan 2014: Received 8 April 2013; revised 24 September 2013; accepted 7 October 2013;first published online 25 November 2013). -
On Asymptotic Incoherence and its Implications forCompressed Sensing…
www.damtp.cam.ac.uk/research/afha/anders/1DCoherence_6.pdf24 Jun 2014: wavelet basis,namely using boundary wavelets [24, Section 7.5.3]. ... 1,p], boundary scaling functions andwavelets (using the same notation as in [24] 8).
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