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  2. J. Fluid Mech. (2014), vol. 757, pp. 330–353. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014-1.pdf
    21 Jan 2015: The dimensionless form of the inequality (2.20) is. B < QF < Qmax BD1(1B). ... 1 20. 0.5. 1.0. 0 1 2 0 1 2 3.
  3. on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from …

    www.damtp.cam.ac.uk/user/gold/pdfs/metachronal_jrsi.pdf
    3 Jun 2015: roto. rro. tor. 0 5 10 10 20 30 0 1 2 315 20 25 30. ... 0.9. 0.85 10 15. 0.98 1.021. 20 25 30. 102030. 51525.
  4. Green Algae as Model Organisms for Biological Fluid Dynamics

    www.damtp.cam.ac.uk/user/gold/pdfs/green_algae.pdf
    25 Sep 2015: l use. onl. y. FL47CH15-Goldstein ARI 1 December 2014 20:34. 1. ... FL47CH15-Goldstein ARI 1 December 2014 20:34. g h. a b c.
  5. Scientific Programming with R Stephen EglenLaurent Gatto September 6, …

    www.damtp.cam.ac.uk/user/sje30/teaching/r/2015/spr-4up.pdf
    1 Oct 2015: x. [1] 20.00000 24.14214 27.32051 30.00000 32.36068. 62 / 191. ... y. 0 5 10 15 20 25 30. 0.0. 0.5. 1.0.
  6. Continuous Compressed Sensing of Inelastic and Quasielastic Helium…

    www.damtp.cam.ac.uk/research/afha/anders/CS4HAS_Arxiv_2.pdf
    4 Oct 2015: gj =. Nk=N. Aj,kfk, j = 0,. , 2N, gj = ρ̃N (λj,N ), (20). ... 20 40 60 80 1000. 0.2. 0.4. 0.6. 0.8. 1. Frequencies.
  7. Continuous Compressed Sensing of Inelastic and Quasielastic Helium…

    www.damtp.cam.ac.uk/research/afha/people/anders/CS4HAS_Arxiv_2.pdf
    4 Oct 2015: gj =. Nk=N. Aj,kfk, j = 0,. , 2N, gj = ρ̃N (λj,N ), (20). ... 20 40 60 80 1000. 0.2. 0.4. 0.6. 0.8. 1. Frequencies.
  8. Cop yrig ht © 201 3 U nive rsity ...

    www.damtp.cam.ac.uk/user/tong/em/macfarlane.pdf
    13 Jan 2015: 20). Here (17) has been used. Eq. (20) expresses the conservation of charge. ... drop. tterms, and replace (.) by n(.)|. Thus, from (20), we expect that n J|. =
  9. On the modeling of active region EUV and X-Ray emission Jaroslav…

    www.damtp.cam.ac.uk/user/astro/cl7/talks/P3_11.pdf
    26 Jul 2015:  The loop is highly non-Maxwellian, with κ < 2.  Calibration uncertainty is large (20%) and ought to be reduced in future missions.
  10. On fundamentals of models and sampling in compressed sensing ...

    www.damtp.cam.ac.uk/research/afha/people/alexb/papers/CSModels.pdf
    10 Jul 2015: 20. 0. 20. Wx0 thresholded to s = 150. 0 500 1000 1500 2000 2500 3000 3500 4000 45000. ... Magn.Reson. Imaging, 58(6):1182–1195, 2007. [20] C. Poon. On the role of total variation in compressed sensing.
  11. Why geometric numerical integration? A. Iserles & G.R.W. Quispel…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_05.pdf
    17 Dec 2015: x1 = x′1 hx′21 h2x′31 k(x2,x3; h). (2.20). where the function k denotes an integration constant that we can choose appropriately.The simplest VP integrator satisfying ... 20. effective algorithms for the solution of linear systems, computation of

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