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Orientational Order and Instabilities in Suspensions of…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SaintillanShelley07.pdf2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [2] N. A. -
PCE845.fm
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard03.pdf2 Sep 2012: Plant, Cell and Environment. (2003). 26,. 1–15. 2003 Blackwell Publishing Ltd. 1. Blackwell Science, LtdOxford, UKPCEPlant, Cell and Environment0016-8025Blackwell Science Ltd 200226845Role of cytoplasmic streaming in symplastic transportW. F. -
Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...
www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf8 Mar 2012: 23. 4.1.3 The optical theorem. 24. 4.1.4 Solving for the asymptotic scattered wave. ... 4 QUANTUM SCATTERING IN 3D 24. where δl is a function of k. -
doi:10.1016/j.jtbi.2005.09.008
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard06.pdf2 Sep 2012: solution to (24) subject to the boundary conditions is(Carslaw and Jaeger, 1959). ... computations. Fig. 2. The radial distribution function R0(r) for the parameter valuesP 1, N 8 , and Q 24. -
Nature’s Microfluidic Transporter: Rotational Cytoplasmic Streaming…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/vandeMeentTuvalGoldstein08.pdf2 Sep 2012: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J. -
The Mechanics and Statistics of Active Matter
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf2 Sep 2012: not new. In a prescient article, Finlayson & Scriven (24) argued that biological matter. -
BIT Numerical Mathematics (2008) 48: 743–761 Published online: 28 ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_01.pdf22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein, -
Pattern formation in a suspension of swimming microorganisms:…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ChildressLevandowskySpiegel75.pdf2 Sep 2012: 2 3 ) pDV-D'@iF28@ = 0, (2.24). D(D = 0, x = - 1 , o. ( ... To see how these expansions proceed, we first note that (2.24) may be integrated, using (2.25), to dbtain 0 so CDdS(76Z2)/ -1 V d Z = 0. -
Fluctuations, Dynamics, and the Stretch-Coil Transition of Single…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KantslerGoldstein12.pdf2 Sep 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J. -
Physics of chemoreception
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/BergPurcell77.pdf2 Sep 2012: Pi[Vr/(r, - a)]2 = 277a2D2/rl(r1 - a)4. (24)The volume involved is approximately 8irr 2(r, - a), so the total stirring power ex-pended in this region
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