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Publications: Edited Volumes A. Iserles (ed.), Acta Numerica 27, ...
www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/Edited.html23 May 2018: Iserles (ed.), Acta Numerica 24, Cambridge Univ. Press (2015). A. Iserles (ed.), Acta Numerica 23, Cambridge Univ. -
David Tong: Strongly Coupled Systems
www.damtp.cam.ac.uk/user/tong/erc.html30 May 2018: David Tong and Kenny Wong. [24] The Holographic Dual of AdS3 x S3 x S3 x S1. -
Our local environment and theeconomy Why nature needs to ...
www.damtp.cam.ac.uk/user/pvl/nature/workshop.pdf25 Oct 2018: Our local environment and theeconomy. Why nature needs to be taken into account in planning andeconomic decisions. Friday 28 September 2018, 12:45 – 17:30at Centre for Mathematical Sciences, Cambridge CB3 0WA. 12:45 Lunch13:30 Introductory talks -
Time integration Issues I AccuracyI Cost I CPU = ...
www.damtp.cam.ac.uk/user/hinch/teaching/GIAMLectures/L12TS.pdf5 Feb 2018: AM4 Adams-Moulton, 4th order, implicit. un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). -
Time integration Issues I AccuracyI Cost I CPU = ...
www.damtp.cam.ac.uk/user/hinch/teaching/GIANHandouts/L12TS.pdf4 Feb 2018: AM4 Adams-Moulton, 4th order, implicit. un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). -
Resumé of lecture 2 Driven Cavity in ψ–ω formulation. ...
www.damtp.cam.ac.uk/user/hinch/teaching/GIANHandouts/Intro3handout.pdf1 Feb 2018: Set t = 0.2Rex2. Plot ω(0.5, 0.5, 1) at Re = 10for N = 10, 12, 14, 16, 18, 20, 24 and 28. -
Time Irreversibility and Criticality in the Motility of a Flagellate…
www.damtp.cam.ac.uk/user/gold/pdfs/gaitswitch.pdf3 Aug 2018: Received 24 June 2017; revised manuscript received 27 March 2018; published 3 August 2018). ... 3, 403 (1993).[24] S. Kamimura and R. Kamiya, Nature (London) 340, 476. -
PII: 0893-9659(90)90021-3
www.damtp.cam.ac.uk/user/ms100/PAPERS/AppMathLett90.pdf13 Dec 2018: g = (A’ B’)m. where. A’ = a2 -@g. 8’ = -2r [l -! Jtt, $1,! (<, 59 = f(E) f(d. l = @1- 22 - 23 td)/SL, 7 = (21 - 22 2s - 24)/2L, and -
Why Clothes Don’t Fall Apart: Tension Transmission in Staple Yarns
www.damtp.cam.ac.uk/user/gold/pdfs/yarns.pdf13 Apr 2018: 4 inset), cf. elastic fiberbundle models [24]. More generally, the LP approach toAmontons-Coulomb friction problems may have applica-tions in stress transmission in granular media, such as sandpiles and grain ... 13, 848 (2017). [24] S. Pradhan, A. Hansen -
Autophoretic motion in three dimensions
www.damtp.cam.ac.uk/user/lauga/papers/146.pdf19 Oct 2018: where. T 2X‘. A‘þ1;2ffiffiffiffiffiffiffiffiffiffiffiffiffi2‘þ3p. ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi‘2 þ2‘þ3. 2‘þ1. sM‘2. 24. ‘þ1‘þ2. ... Brown and W. Poon, Soft Matter, 2014, 10, 4016–4027.24 -
Physics of Bubble‐Propelled Microrockets
www.damtp.cam.ac.uk/user/lauga/papers/148.pdf19 Oct 2018: 14,24,26] The inner sur-face of the cone is chemically active and catalyzes a chemi cal reaction. ... Li, W. Gao, L. Zhang,. J. Wang, ACS Nano 2015, 9, 117.[24] M. -
Recovery of a Variable Coefficient in a Coastal Evolution Equation
www.damtp.cam.ac.uk/user/ms100/PAPERS/JCP99.pdf13 Dec 2018: F′n1, An,n =τ. 2ξF′n. (24). This is easily and rapidly inverted by back-substitution. -
DAMTP/90-2, corrected Analogs for the c-Theorem for Four Dimensional…
www.damtp.cam.ac.uk/user/ho/analogs.pdf16 Aug 2018: X δ. δMSqo =. [ψ̄Xψ. ], X† = X , Jµα =. δ. δAψµαSqo =. [ψ̄γµTαψ. ]. (4.24). As a consequence of invariance under (4.21), for η = η̄ = 0,. ... S̃(1)o =1. 16π2ε. ((nV 2nF ). 1. 180(3F G) 1. 24(2nV nF )RαβγδRαβγδ. -
Efficient boundary integral solution for acoustic wave scattering by…
www.damtp.cam.ac.uk/user/ms100/PAPERS/arxiv1407.5560v1.pdf13 Dec 2018: elements. (Bn)mj = Anmnj. (24). We thus require. bn = B1n cn (25). ... from rough surfaces, Waves in Random Media, 6, 151-167 (1996). [24] A.A. -
The Computational Spectral Problem and a New Classification Theory…
www.damtp.cam.ac.uk/user/mjc249/talks/SCI_colbrook_berkeleytalk.pdf16 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe -
statphys
www.damtp.cam.ac.uk/user/tong/statphys/four.pdf31 Dec 2018: V. A. B. Path I. Path II. Figure 24:. underline the meaning of the new symbol d. ... energy gives us,. @S. @V. T. =@p. @T. V. (4.24). The Gibbs free energy gives us. -
Vortices, Painlevé integrability andprojective geometry Felipe…
www.damtp.cam.ac.uk/user/md327/felipe_thesis.pdf3 Apr 2018: with (2.17).Finally, equation (2.24) is satisfied upon eliminating fww in the sameway and using w. ( ... 24. motion of N-vortices. There are several ways to obtain the metric forboth flat and curved backgrounds [46, 16]. -
Quantum Field Theory II University of Cambridge Part III ...
www.damtp.cam.ac.uk/user/dbs26/AQFT/chap1.pdf19 Jan 2018: absolutely impossible for a course of 24 lectures to do so). ... showing that the quantity. =. Z. N dd1x (1.24). is conserved under evolution via the classical equations. -
Time integration Issues I AccuracyI Cost I CPU = ...
www.damtp.cam.ac.uk/user/hinch/teaching/CMIFM_Lectures/TS.pdf10 Oct 2018: AM4 Adams-Moulton, 4th order, implicit. un1 = un t. 24(9Fn1 19Fn 5Fn1 Fn2). -
PHYSICAL REVIEW FLUIDS 2, 123101 (2017) Bundling of elastic ...
www.damtp.cam.ac.uk/user/lauga/papers/143.pdf11 Jan 2018: coli) [24], and also Salmonella typhimurium [23], Halobacteriumsalinarium [25], and Bacillus subtilis [26] [see Fig. ... 24). The terms on the left-hand side can be simplified by noting that.
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