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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. -
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. -
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. -
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.
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