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  2. Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…

    www.damtp.cam.ac.uk/user/gold/pdfs/trapping.pdf
    10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

  3. Model for phase equilibria in micellar solutions of non ...

    www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_84_3367.pdf
    10 Apr 2011: Bt/JI= M , (24) t/JI Bt/J t/J(Mn). and a further differentiation then gives. ... 4. Clearly, a steepest-descent approximation should be valid for that part of the distribution near the region of the mini-mum at n 'Z 24.

  4. doi: 10.1098/rsta.2010.0225, 2133-2147369 2011 Phil. Trans. R. Soc. A …

    www.damtp.cam.ac.uk/user/mem/wolff-phil-trans11.pdf
    5 Aug 2011: N2 ratio of the atmosphere [24]. ... Science 309, 1714–1717. (doi:10.1126/science.1115193). 24 Manning, A. C. & Keeling, R.

  5. PII: S0031-8914(37)80203-7

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/hamaker.pdf
    6 Oct 2011: 1 7 X 102 1.60 2. 2 5 2.92 3.24 3.59 9. ... 6 2 X 1 0 -1 1.10 1.24 1. 3 7 X 1 0 1 3.

  6. Generalized sampling and infinite-dimensionalcompressed sensing Ben…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_02.pdf
    2 Nov 2011: Generalized sampling and infinite-dimensionalcompressed sensing. Ben AdcockDepartment of Mathematics. Simon Fraser UniversityBurnaby, BC V5A 1S6. Canada. Anders C. HansenDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd,

  7. Generalized Sampling: Extension to Frames and Inverse andIll-Posed…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_17.pdf
    3 Dec 2011: Generalized Sampling: Extension to Frames and Inverse andIll-Posed Problems. Ben Adcock Anders C. Hansen † Evelyn Herrholz ‡ Gerd Teschke‡. Abstract. Generalized sampling is new framework for sampling and reconstruction in

  8. PHYSICAL REVIEW B 1 FEBRUARY 1998-IVOLUME 57, NUMBER 5 ...

    www.damtp.cam.ac.uk/user/gold/pdfs/type1_prb.pdf
    10 Apr 2011: a. Dd!1/2. h F pln 0.56/h!G1/2. 3.24! B. Energy of a straight-lamina model. ... detail elsewhere in the context of clorelated models,22–24,26,27,30we do not repeat them here.

  9. Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/trapping.pdf
    10 Apr 2011: 2 Ok5k1. 0ka!0# kk4. e2k4t (24). Evaluating the first few integrals, we find forh# k, h# k1. ... A 5zL4. tk1. 24 (54). whereas the rodlike treatment implies (from Eq.

  10. PHYSICS OF FLUIDS 17, 083101 �2005� Stalactite growth as ...

    www.damtp.cam.ac.uk/user/gold/pdfs/stalactite_long.pdf
    10 Apr 2011: PHYSICS OF FLUIDS 17, 083101 2005. Stalactite growth as a free-boundary problemMartin B. ShortDepartment of Physics, University of Arizona, Tucson, Arizona 85721. James C. BaygentsDepartment of Chemical and Environmental Engineering and Program in

  11. DAMTP 2010/NA04 Beyond symmetric Broyden for updating quadratic…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_04.pdf
    13 Apr 2011: DAMTP 2010/NA04. Beyond symmetric Broyden for updating quadratic. models in minimization without derivatives. M.J.D. Powell. Abstract: Some highly successful algorithms for unconstrained minimizationwithout derivatives construct changes to the

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