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PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: 4,5,24–30]. The individual locomotion of spermatozoa was first studiedby G. I. ... Bottom: Variation of the ratio of the minimum to themaximum of the rate of energy dissipation with ka (symbols). -
Magnus–Lanczos methods with simplified commutators for the…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_01.pdf3 Apr 2018: h7), (2.23). Magnus–Lanczos methods with simplified commutators 15. where. ϕ1(h,ζ,ξ) = h2 4hξ 2ζξ, (2.24). -
Microbial mutualism at a distance: The role of geometry in diffusive…
www.damtp.cam.ac.uk/user/gold/pdfs/mutualism.pdf27 Feb 2018: Resource-explicit models of bacterial mutualismscompare well with experiments in which mutualists are wellmixed [5,6,23,24]. -
GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...
www.damtp.cam.ac.uk/user/mem/papers/SSREPLY/rupert-ford-thesis93.pdf19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret -
GRAVITY WAVE GENERATION BY VORTICAL FLOWS IN A ROTATING ...
www.damtp.cam.ac.uk/user/mem/oldftp/rupert-ford-thesis93.pdf19 Oct 2013: GRAVITY WAVE GENERATION BY VORTICAL FLOWS. IN A ROTATING FRAME. Rupert Ford. Churchill College Cambridge. A dissertation sublnitted for the degree of Doctor of Philosophy. at the University of Cambridge. October, 1993. To my grandparents. Margaret -
Model for phase equilibria in micellar solutions of non ...
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_84_3367.pdf10 Apr 2011: Bt/JI= M , (24) t/JI Bt/J t/J(Mn). and a further differentiation then gives. ... 0.6. xc. 0.5 ---- --------Xc«Mn)a CXl)---------. 0.4. 0.4 0.5 0.6. ka T lu. -
Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...
www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf8 Mar 2012: 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k. ... γl =κaj′l(κa). jl(κa). (4.1.2.2). As k 0 have γl const, jl(ka) (ka)l, nl(ka) (ka)(l1) and, as before, getδl (ka)2l1. -
Publications | Cantab Capital Institute for the Mathematics of…
www.damtp.cam.ac.uk/research/ccimi/publications?page=10814 May 2024: van Leeuwen KA, G Oppen, S Renwick, JB Bowlin, PM Koch, RV Jensen, O Rath, D Richards, JG Leopold. – ... A ISERLES, SP NORSETT. – BIT Numerical Mathematics. (1984). 24,. 529. -
LECTURE NOTES FOR IIB PARTIAL DIFFERENTIALEQUATIONSM. S. JOSHI AND ...
www.damtp.cam.ac.uk/user/dmas2/public_ps/pdewj.pdf27 Oct 2010: k CkA BkeMjtt0j1M ka bkeMjtt0jwhere C is a constant depending only on A and a.Proof. ... deningfn(t) = ka bk CkA Bkj(t t0)j M Z tt0 fn1(s)ds: (2.6). -
1 /** 2 * @preserve Copyright (c) 2011~2014 Humu ...
www.damtp.cam.ac.uk/user/ms100/JAVA/jsc3d/docs/symbols/src/jsc3d.js.html19 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.
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