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  2. Orientational Order and Instabilities in Suspensions of…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/SaintillanShelley07.pdf
    2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [2] N. A.
  3. PCE845.fm

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard03.pdf
    2 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.
  4. Part II Applications of Quantum MechanicsLent 2012 Prof. R.R. ...

    www.damtp.cam.ac.uk/user/rrh/notes/aqm_notes_180112.pdf
    8 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.
  5. doi:10.1016/j.jtbi.2005.09.008

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Pickard06.pdf
    2 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.
  6. Nature’s Microfluidic Transporter: Rotational Cytoplasmic Streaming…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/vandeMeentTuvalGoldstein08.pdf
    2 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.
  7. The Mechanics and Statistics of Active Matter

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf
    2 Sep 2012: not new. In a prescient article, Finlayson & Scriven (24) argued that biological matter.
  8. BIT Numerical Mathematics (2008) 48: 743–761 Published online: 28 ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_01.pdf
    22 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,
  9. Pattern formation in a suspension of swimming microorganisms:…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/ChildressLevandowskySpiegel75.pdf
    2 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.
  10. Fluctuations, Dynamics, and the Stretch-Coil Transition of Single…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/KantslerGoldstein12.pdf
    2 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.
  11. Physics of chemoreception

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/BergPurcell77.pdf
    2 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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