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14 Jun 2014: Tue 26 Mar 2002 grade.el: New entry. Sun 24 Mar 2002 gle-mode.el: New entry. ... Mon 24 Jul 2000 qflib.el, tint-instances.el: New entries. Fri 14 Jul 2000 background.el: New entry.

23 Jul 2014: H ). Then. SCI(Ξ1, )R 2, SCI(Ξ2, 1)R 2. 24 / 26. Tests with the Operator Ψ(Q) for Ψ L(R).

27 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.

21 Oct 2014: Oceans 24, 183-195. Identical to Hacker et al. (1994) but refereed and published in special issue of journal.

26 Mar 2014: m Cka log(1 p1)log(n),. for some universal constant C > 0 [24]. ... 24]. This raises thequestion of whether there are alternatives which are satisfied by such matrices.

21 Oct 2014: Section 3. An obvious theme (I hope!). 21) 2x(3 x2) 24) xex2/2 27) tan x = sin xcos x. ... 22) cos x2 23) 14 sin4 x 24) ex. 2/2 25) 13 (1 x2)3/2 26) 12 tan.

21 Oct 2014: R23/24/25 Toxic by inhalation, in contact with skin and if swallowed. ... R39/24 Toxic: danger of very serious irreversible effects in contact with skin.

21 Oct 2014: Volatile Solvent Permits can only be issued within 24 hours of the work commencing. ... skin R39/24/25 Toxic: danger of very serious irreversible effects in contact.

22 Jul 2014: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

28 Nov 2014: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Teaching. Soft Matter & Biological Physics (Part III, Michaelmas 2014). Prof. Raymond E. Goldstein FRS (DAMTP) and Dr. Ulrich F. Keyser (Cavendish). This course will provide

22 Jul 2014: 0-4. 5-9. 10-14. 15-19. 20-24. 25-29. 30-34. 35-39. 40-44. 45-49. 50-54.

22 Jul 2014: Old people in Cambridgeshire. 2012 2030? Over 65 96,000 17%. 135,000 24%.

22 Jul 2014: 15-19. 20-24. 25-29. 30-34. 35-39. 40-44. 45-49. 50-54. 55-59. 60-64. 65-69.

24 Dec 2014: Emacs Lisp List. Last updated: Wed 24 Dec 2014 11:36:00 GMT.

23 Jul 2014: 24 / 44. Compressed sensing Towards infinity To infinity and beyond!

14 Jun 2014: graphical-friendly.I Emacs 23 very stable.I Emacs 24 due out next year? ... Emacs 24 as stable base for documents. 3. Tom Dye has a nice reproducible solution for Org config.

14 Jun 2014: mean 20.6a 4.7 9.1 15.1 20.1 24.3 30.0 33.8 35.2 44.8s.d. ... divisive subtractive none. postsynaptic normalizationdivisive 5.07 2.24 6.30subtractive 4.78 0.83 0.00a.

14 Oct 2014: 22 23 24 is not elliptic,. parabolic or hyperbolic.However, the case of second order equations in two space dimensions is special.

19 Nov 2014: data[dest 3] = color >>> 24; 1422 src = (j & 1); 1423 dest = 4; 1424 } 1425 src = (i & 1)? ... 3] = color >>> 24; 1454 } 1455 break; 1456 } 1457 }; 1458 1459 / 1460 Render a new frame.

14 Jun 2014: graphical-friendly.I Emacs 23 very stable.I Emacs 24 due out next year? ... Emacs 24 as stable base for documents. 3. Tom Dye has a nice reproducible solution for Org config.

14 Jun 2014: This matches results from mammalian conephotoreceptors and cholinergic amacrine cells [11, 24]. ... retinal studiesVis. Neurosci.6 95–111[24] Rodieck R W and Marshak D W 1992 Spatial density and distribution of choline acetyltransferase.

22 Dec 2014: λq(ck )(tck), (24). where the derivatives η( j)λ ,1(ck,t) R and S( j)λ ,1(ck,t) sl(2,C) can be bounded inde-. ... 24 Alberto Gil C. P. Ramos, Arieh Iserles. References. Driscoll, T., Hale, N.

28 Nov 2014: xx0‖t0t1. e(t1, x) dx. ‖xx0‖t0. e(0, x) dx. (6.24). This implies that if the initial data are zero then the solution is zero at all later ... et p = u2t 0. which gives the same conclusion 6.24 for positive times.

4 Nov 2014: ahX=0-07 exp (V/20), (23)and II V301). Ph --Jrx 10 I(24). 516. ... h=1/(exp V30 1). (24). Equation (26) is derived simply from eqns.

26 Mar 2014: m Cka log(1 p1)log(n),. for some universal constant C > 0 [24]. ... 24]. This raises thequestion of whether there are alternatives which are satisfied by such matrices.

22 Jul 2014: Autocloud, or how to use your car battery to save energy! Jon Crowcroft, http://www.cl.cam.ac.uk/jac22. The Wires run hot. Assume all our vehicles are electric.  That represents storage for about 30% of UK electricity production for a day. 

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.

20 Jul 2014: ranging from! 10 nm to 10 µm.22, 24, 26, 27 Similarly, a liquid interface covered withsurfactants acts as a thin two-dimensional fluid layer separating the liquid phases. ... . ek z. (24). The unknown coefficients in this solution are

23 Jul 2014: Final Example [Feinberg/Zee 1999]. Period 24 Periods 1,. , 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and Pseudospectra. ... Final Example [Feinberg/Zee 1999]. Size 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and

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:.

22 Jul 2014: 2030 vision for the Cambridge sub-region Energy, water and waste Thursday 24 January 2013 at 6.30 pm Workshop to be held at the Centre for Mathematical Sciences, Wilberforce Road,

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

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

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

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

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.

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.

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).