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Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-24-1.html28 Jan 2016: -
Stephen J Eglen
www.damtp.cam.ac.uk/user/sje30/pubs.html13 Mar 2016: Frontiers in Computational Neuroscience 7:24. -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-08-24-1.html28 Jan 2016: -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_Beta2KO_37C_Ventral_2008-10-24-0.html28 Jan 2016: -
www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt
www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt24 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 -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-24-0.html28 Jan 2016: -
PHYSICAL REVIEW FLUIDS 1, 073201 (2016) Elastohydrodynamic…
www.damtp.cam.ac.uk/user/gold/pdfs/elasto_synchro.pdf1 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. -
doi:
www.damtp.cam.ac.uk/user/rrk26/Papers/CK13.pdf12 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 -
Cop yrig ht © 201 6 U nive rsity ...
www.damtp.cam.ac.uk/user/examples/A5g.pdf10 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. -
Priscilla Canizares-Martinez Current position: University of…
www.damtp.cam.ac.uk/research/afha/people/priscilla/PCanizares.pdf27 Jan 2016: 09/01/2013 BBC Stargazing LIVE, 2013 (UK): Science exhibit: ”Growing Galaxies. 24/03/2012 Institute of Astronomy Open Day, support staff (UK): Activity Title: “Making a spec-trometer. -
NE7405
www.damtp.cam.ac.uk/user/sje30/papers/network97.pdf26 Feb 2016: Information Processing Systemsvol 4 (San Mateo, CA: Morgan Kaufmann) pp 1017–24. -
Non-resonant optical control of a spinor polariton condensate A. ...
www.damtp.cam.ac.uk/user/ngb23/publications/PRB2016.pdf12 Jul 2016: Nature443(7110), 409–414 September (2006). [24] Laussy, F. P., Shelykh, I. A., Malpuech, G., and Kavokin,A. -
Instabilities of a thin coating on a vertical fibre; Newtonian,…
www.damtp.cam.ac.uk/user/hinch/talks/Vancouver2016a.pdf22 Feb 2016: 24. More terms: matching two regions. At c0:G0 = (R+ R)/2π. -
VOLUME 79, NUMBER 22 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Fygenson_etal.pdf3 Oct 2016: This is of the same orderas forces generated by specialized motor proteinss,5 pNd[24], and agrees with the scale of force expected from thfree energy calculation (Table I). ... 24] J. T. Finer, R. M. Simmons, and J. A. Spudich, Nature(London) 368, 113 -
Slender-ribbon theory
www.damtp.cam.ac.uk/user/lauga/papers/115.pdf25 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. -
Coordinated beating of algal flagella is mediated by basal coupling
www.damtp.cam.ac.uk/user/gold/pdfs/coupling_pnas.pdf18 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 -
A generalization of Filon-Clenshaw-Curtis quadrature for highly…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_04.pdf17 Aug 2016: I. Fourier. transforms’, IMA J. Numer. Anal. 24(3), 365–391. Iserles, A. & -
14799850532483 1..16
www.damtp.cam.ac.uk/user/gold/pdfs/aerotaxis_elife.pdf24 Nov 2016: Accepted: 17 October 2016. Published: 24 November 2016. Reviewing editor: Richard M. -
mssmRge.eps
www.damtp.cam.ac.uk/user/examples/3P7.pdf8 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 -
Noname manuscript No.(will be inserted by the editor) Symmetric ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_01.pdf23 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 -
Small acoustically forced symmetric bodies in viscous fluids
www.damtp.cam.ac.uk/user/lauga/papers/117.pdf4 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. -
INVITED ARTICLES PHYSICAL REVIEW FLUIDS 1, 060503 (2016) Soap-film ...
www.damtp.cam.ac.uk/user/gold/pdfs/soap-film_prf.pdf19 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 -
Power and limitations of convex formulationsvia linear and…
www.damtp.cam.ac.uk/user/hf323/Fawzi_PhDthesis.pdf6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3. -
J. Fluid Mech. (2015), vol. 777, pp. 97–121. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2015.pdf11 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). -
9 The Method of Characteristics When we studied Laplace’s ...
www.damtp.cam.ac.uk/user/dbs26/1BMethods/Characteristics.pdf26 Nov 2016: φ(x, y) = (2 2x y) e2xy sin(2x y) (y 2) ex , (9.24). -
J. Fluid Mech. (2016), vol. 798, pp. 165–186. c© ...
www.damtp.cam.ac.uk/user/gold/pdfs/squirmers_swirl.pdf1 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. -
Part III: Biological Physics and Complex Fluids (Michaelmas, 2016)E…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Bio_and_Complex2016_Examples2.pdf30 Oct 2016: What is the physical meaning of Ψ in 3.1 and 3.24? ... What are the meanings of Ẋc and Ṙ in 3.24? 2. -
Generalized sampling and infinite-dimensionalcompressed sensing Ben…
www.damtp.cam.ac.uk/research/afha/anders/BAACHGSCS_Rev10.pdf21 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). -
5 The Renormalization Group Even a humble glass of ...
www.damtp.cam.ac.uk/user/dbs26/AQFT/Wilsonchap.pdf10 Feb 2016: ZΛZsΛ. ]1/2= 1. [d 22. γφ. ]δs (5.24). with γφ as in (5.16). -
This isa spec ific indiv idual’s copy of the ...
www.damtp.cam.ac.uk/user/sjc1/teaching/VandM/notes.pdf6 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 -
Sparse sum-of-squares certificates on finite abelian groups
www.damtp.cam.ac.uk/user/hf323/talks/sparse_sos_abelian_slides.pdf6 Oct 2016: 24. Translation of frequencies. We have:. f (x ) =. j. -
Quadrature methods for highly oscillatory singular integrals Jing…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_02.pdf3 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. -
Analyzing the structure of multidimensional compressedsensing…
www.damtp.cam.ac.uk/research/afha/anders/dDCoherence_Arxiv.pdf24 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 -
Colloid Transport by Interfacial Forces
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/AndersonARFM.pdf2 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):. -
Constitutive Equations for Polymeric Liquids
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/BirdWiestARFM.pdf2 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, -
This article was downloaded by:[Soward, Andrew]On: 5 March 2008Access …
www.damtp.cam.ac.uk/user/rrk26/Papers/Precession_GAFD1993.pdf12 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. -
OP-MOLB160211 3226..3248
www.damtp.cam.ac.uk/user/gold/pdfs/silicon_transport.pdf10 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 -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-08-24-0-c02.html28 Jan 2016: -
Generalized sampling and infinite-dimensionalcompressed sensing Ben…
www.damtp.cam.ac.uk/research/afha/people/anders/BAACHGSCS_Rev10.pdf21 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). -
Geophysical Journal InternationalGeophys. J. Int. (2015) 201, 764–782 …
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Lythgoe-2015.pdf11 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. -
Analyzing the structure of multidimensional compressedsensing…
www.damtp.cam.ac.uk/research/afha/people/anders/dDCoherence_Arxiv.pdf24 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 -
Breaking the coherence barrier: A new theory forcompressed sensing ...
www.damtp.cam.ac.uk/research/afha/anders/BreakingCoherenceRevisionFinal.pdf2 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 -
Complexity Issues in Computing Spectra, Pseudospectra and Resolvents…
www.damtp.cam.ac.uk/research/afha/anders/Banach_Hansen_Nevanlinna_edit2.pdf22 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]. -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_Beta2KO_37C_Nasal_2008-10-24-2.html28 Jan 2016: -
Breaking the coherence barrier: A new theory forcompressed sensing ...
www.damtp.cam.ac.uk/research/afha/people/anders/BreakingCoherenceRevisionFinal.pdf2 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 -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_WT_37C_Dorsal_2008-02-08-0.html28 Jan 2016: -
lecture9.dvi
www.damtp.cam.ac.uk/user/rrk26/Papers/lecture9.pdf12 Aug 2016: Re2ν = 0. (24). The last equation is the ‘dual (or adjoint) linearized Navier-Stokes equation’. ... Step.3 Backwards time integrate the dual linearized Navier-Stokes equation (24) with in-compressibility (14) and boundary condition (13) from t = T -
lecture7.dvi
www.damtp.cam.ac.uk/user/rrk26/Papers/lecture7.pdf12 Aug 2016: û(x, t) = ũ(y)eikzσt (24). (known to be critical for the energy stability problem), (23) becomes. ... Rev. FluidMech., 43 (2011), pp. 1–24. [12] M. Nagata, Three-dimensional finite-amplitude solutions in plane Couette flow: bi-furcation from -
PHYSICAL REVIEW E 93, 043125 (2016) Rotation of slender ...
www.damtp.cam.ac.uk/user/lauga/papers/119.pdf1 Oct 2016: For example, some eukaryoticmicroorganisms have evolved hairs along their flagella calledmastigonemes [23,24]. ... F(t ) = ζ. Udef ds = {0,0,0}, (24). L(t ) = ζ. -
Sensing in the Mouth: A Model for Filiform Papillae as Strain…
www.damtp.cam.ac.uk/user/lauga/papers/124.pdf1 Oct 2016: Other measurements reports significantly larger sizes, withwidths that can range 100–300 µm and length 200–500 µm[21, 23, 24]. ... hydrodynamics and flow sensing. Annu Rev Fluid Mech. (2016) 48:1–24. doi:.
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