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14 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.

14 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 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!

27 Feb 2014: where. D1 = 2bαα. sinh2(αGt. ). 2αG. , (5.24). D2 = 1α.

14 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).

26 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].

29 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 %.

19 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.

31 May 2014: 24. The editorial process Once you’ve submitted a paper to a journal, it followsa set pattern:.

12 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.

6 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.

21 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

21 Oct 2014: πFn(θ φ) dφ = f(θ) , (1.24). – 8 –. using property ii) of the Fejér kernel.

30 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

28 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.

9 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.

21 Oct 2014: DiDiDiDiggggImage: DigiFile Utility Index. Version 2.3  DL Research Partners September 2001 24.

13 Jul 2014: Arakawa’s method is used for evaluation of thePoisson bracket.24 The time stepping algorithm is the third.

22 Jan 2014: Received 8 April 2013; revised 24 September 2013; accepted 7 October 2013;first published online 25 November 2013).

24 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).