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28 Jan 2016:

28 Jan 2016:

28 Jan 2016:

13 Mar 2016: Frontiers in Computational Neuroscience 7:24.

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28 Jan 2016:

28 Jan 2016:

1 Nov 2016: large. However, it is well knownthat use of the leading-order approximation of slender body hydrodynamics for larger values of isrobust [24,25]. ... A(τ ) =(. Be2(2k2k4 )τ 3k. 4. 4(2 k2))1/2. (24). 073201-8.

12 Aug 2016: f 6 fbound = (1 n)1n(1 n)1nDmax as Re , (4.24). ... D = Dv = 24/3D. 1/3lamD2/3max O(Re8/3), Dm = 22/3D2/3lamD1/3max O(Re7/3), (4.34).

12 Jul 2016: Nature443(7110), 409–414 September (2006). [24] Laussy, F. P., Shelykh, I. A., Malpuech, G., and Kavokin,A.

1 Oct 2016: coli swarm near its advancing edge revealed that the top swarm-air surface isin fact stationary [24]. ... ρ = ξ‖ξ. = 1γ1. = 0.4, (24). 043202-8. FLAGELLAR FLOWS AROUND BACTERIAL SWARMS.

24 May 2016: future. Soft Robot. 1, 5–11 (2013).24. Kim, S., Laschi, C. & Trimmer, B. ... Adv. Mater. 24, 2710–2714 (2012). 46. Zeng, H. et al. High-resolution 3D direct laser writing for liquid-crystallineelastomer microstructures.

26 Feb 2016: Information Processing Systemsvol 4 (San Mateo, CA: Morgan Kaufmann) pp 1017–24.

12 Aug 2016: Received 17 July 2012; revised 19 February 2013; accepted 24 February 2013;first published online 28 March 2013). ... 2d(i)(d(i)zn(i) pn1(i)) 2µzn(i)= 0 (3.23)2µβ = 0 (3.24). z2n β2 2 = 0 (3.25)where di is the ith diagonal element of

17 Aug 2016: I. Fourier. transforms’, IMA J. Numer. Anal. 24(3), 365–391. Iserles, A. &

11 Jan 2016: leakage rate predicted by (2.24) is then unphysical because there is no fluidabove the outlet to draw. ... Generally, this assumptionis invalid if the current delivers a smaller flux towards the outlet than is predicted toleak according to (2.24).

18 May 2016: The basic configurationof two flagella appears in multiple lineages by convergent evolu-tion, e.g., in the naked green alga Spermatozopsis (23), in gametesof the seaweed Ulva (24), and in swarm

23 Jul 2016: 24). Finally, inserting (24) into (22) and (23) yields. ‖u(tn1) un1‖ t2r4‖f(2r2)t. ... 24 C. Liu, A. Iserles, X. Wu. For the time integrators Brik1 and Brik2 derived in this paper we use thetolerance 1015 and choose m = 2 in the waveform relaxation

24 Nov 2016: Accepted: 17 October 2016. Published: 24 November 2016. Reviewing editor: Richard M.

19 Oct 2016: This paper is based on an invited lecture given by Keith Moffatt at the 68th Annual Meeting of the APSDivision of Fluid Dynamics, which was held 22–24 November 2015 in

25 Feb 2016: Shortly thereafter, Lighthill proposed a derivation which was accurate toorder 1/2.21,24 This was a vast improvement on the earlier methods but still did not account for theends of ... 2n̂. s. 1. O(b3), (24). R. 0. =b 1,bt̂ b2 21,b.

26 Nov 2016: φ(x, y) = (2 2x y) e2xy sin(2x y) (y 2) ex , (9.24).

10 Jun 2016: mis. sion. 4 Surfaces and Surface Integrals 24. 4.1 Surfaces and Normals 24. ... 24 –. Cop. yrig. ht. 201. 6 U. nive. rsity.

6 Oct 2016: 24. Translation of frequencies. We have:. f (x ) =. j.

1 Jun 2016: Received 2 December 2015; revised 13 April 2016; accepted 24 April 2016). ... 6 ms 12 ms 18 ms 24 ms. 2000. –2000. 2000.

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).

6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3.

4 Mar 2016: ux0 þ rðtÞ; t uðx0; tÞþ rðtÞu xðx0; tÞ: (24). As the velocity field, the distance x and the displacement rare made dimensionless using n0x, k.

8 Mar 2016: Cop. yrig. ht. 201. 6 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Prepared for submission to JHEP. Supersymmetry. B. C. Allanacha F. Quevedoa. aDepartment of Applied Mathematics and

10 Feb 2016: ZΛZsΛ. ]1/2= 1. [d 22. γφ. ]δs (5.24). with γφ as in (5.16).

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24 Oct 2016: There is a wide variety of problems that lack incoherence, a fact that has been widely recognized [2,6, 10, 11, 24, 25, 27, 33–36, 40], however, they instead posses

2 Oct 2016: Annu. Rev. Fluid Mech. 1995. 27: 169-93 Copyright 1995 by Annual Reviews Inc. All rights reserved. CONSTITUTIVE EQUATIONS FOR. POLYMERIC LIQUIDS. R. Byron Bird. Department of Chemical Engineering and Rheology Research Center, University of Wisconsin,

12 Aug 2016: 1.24). The reader should note that the original geometry has been recovered in the limit ,u << 1. ... With no precession, (1.22)-( 1.24) is the normal mode problem for a uniformly-rotating basic state within a spheroidal container.

2 Oct 2016: KL ::::: - ( 1 /24)[2 (rods, length I), = - ( 1/3)c2 (disks, radius c). ... p = -kT[C-C'],. which gives the following when substituted into (24) and (27):.

3 Jun 2016: 24. where xj, j = 1, ,n are the zeros of a monic orthogonal polynomial Pωn (x) of degree non [0,b] with the complex weight function h(x)eiωg(x), b.

6 Nov 2016: VECTORS AND MATRICES 24 lectures, Michaelmas term. Complex numbersReview of complex numbers, including complex conjugate, inverse, modulus, argument and Arganddiagram. ... You should be able to do example sheets 1/2/3/4 after lectures 6/12/18/24

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).

10 Nov 2016: The Evolution of Silicon Transport in Eukaryotes. Alan O. Marron,1,2 Sarah Ratcliffe,3 Glen L. Wheeler,4 Raymond E. Goldstein,1 Nicole King,5 Fabrice Not,6,7. Colomban de Vargas,6,7 and Daniel J. Richter5,6,71Department of Applied Mathematics and

24 Oct 2016: There is a wide variety of problems that lack incoherence, a fact that has been widely recognized [2,6, 10, 11, 24, 25, 27, 33–36, 40], however, they instead posses

22 Oct 2016: For other papers related to the ideas presented in this papers we refer to[3, 4, 6, 10, 11, 12, 13, 14, 15, 16, 17, 24, 26, 30].

11 Jan 2016: T. P= Ta. P+ 5̄. ρg′c2. (24). Thus the conductive heat flux, qcond, may be expressed in terms ofthe adiabat and the potential temperature.

2 Nov 2016: Breaking the coherence barrier: A new theory forcompressed sensing. B. AdcockSimon Fraser Univ. A. C. HansenUniv. of Cambridge. C. PoonUniv. of Cambridge. B. RomanUniv. of Cambridge. Abstract. This paper presents a framework for compressed sensing

2 Nov 2016: Breaking the coherence barrier: A new theory forcompressed sensing. B. AdcockSimon Fraser Univ. A. C. HansenUniv. of Cambridge. C. PoonUniv. of Cambridge. B. RomanUniv. of Cambridge. Abstract. This paper presents a framework for compressed sensing

18 Feb 2016: Manuscript received 9 December 2014, in final form 24 September 2015).

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29 May 2016: This has been explained in detail in previous papers [18, 19, 20, 21, 22, 24].

6 Oct 2016: i. |hi|2. where := cos(π/N) x F(N,C). 15 / 24. ... and the sos hierarchy needs only dN/4e levels. 24 / 24.

24 Oct 2016: Stuckness. the predecessor of all real understanding.'' [Near end of chapter 24, p.286 in the original edition.] Of course one can be getting on with other things, at least part

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