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  2. N22a.dvi

    www.damtp.cam.ac.uk/user/examples/N22a.pdf
    17 Jan 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... yrig. ht. 200. 8 U. nive. rsity. of C. ambr. idge.
  3. N22b.dvi

    www.damtp.cam.ac.uk/user/examples/N22b.pdf
    16 Jan 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr.
  4. N22d.dvi

    www.damtp.cam.ac.uk/user/examples/N22d.pdf
    16 Jan 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... Hint:consider 1/p(z).]. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.
  5. N22c.dvi

    www.damtp.cam.ac.uk/user/examples/N22c.pdf
    16 Jan 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr.
  6. A5a.dvi

    www.damtp.cam.ac.uk/user/hinch/teaching/A5a.pdf
    13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.
  7. A5d.dvi

    www.damtp.cam.ac.uk/user/hinch/teaching/A5d.pdf
    13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.
  8. A5b.dvi

    www.damtp.cam.ac.uk/user/hinch/teaching/A5b.pdf
    13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.
  9. A5c.dvi

    www.damtp.cam.ac.uk/user/hinch/teaching/A5c.pdf
    13 Mar 2008: Cop. yrig. ht. 200. 8 U. nive. rsity. of C. ambr. ... 1. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.
  10. D23Ld.dvi

    www.damtp.cam.ac.uk/user/examples/D23Ld.pdf
    5 Dec 2008: So. (h3hx)x t6α, ḣ t1α. 41. Cop. yrig. ht. 200. 8 U. ... W. (eRe eRe(y/a))(1 eRe). 46. Cop. yrig. ht. 200. 8 U.
  11. B9Lb.dvi

    www.damtp.cam.ac.uk/user/examples/B9Lb.pdf
    30 Sep 2008: Wave-particle duality. Light exhibits wave-like properties,. 3. Cop. yrig. ht. 200. ... dV. = 2|α|2N1 2|β|2N2 < ¤. 17. Cop. yrig. ht. 200.
  12. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_10.pdf
    1 Aug 2008: 2. 0 200. 50. 2. 1. 2. 1500. 1. 0. 200100 50 1500.8. ... left), c = [1,. 77 ,. 7. 7 , 1], m = [2, 1, 1, 2] (right) andω [0, 200].
  13. hop07spec.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_05.pdf
    10 Apr 2008: 1.5. 1. 0.5. 0ω=50. 100 200 300 400 500 6002.5. 2. ... 1.5. 1. 0.5. 0ω=100. 100 200 300 400 500 600. 2.5.
  14. 5 May 2008 National Transport Information Incubator (NaTII) Enabling…

    www.damtp.cam.ac.uk/user/pvl/natii_publication.pdf
    13 Jun 2008: 5 May 2008. National Transport Information Incubator. (NaTII). Enabling the power of information. Professor Peter Landshoff1 and Michael Simmons, University of Cambridge Dr Rashmi Joshi, Deloitte and Touche LLP. Charles Gill, Lockheed Martin UK Ltd
  15. Bonn.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2008_09.pdf
    11 Jul 2008: Bialynicki-Birula, I., Mielnik, B. & Plebánski, J. (1969), ‘Explicit solution of the continuousBaker–Campbell–Hausdorff problem and a new expression forthe phase operator’,Ann.Phys.51, 187–200.
  16. Adv. Geosci., 15, 47–56, 2008www.adv-geosci.net/15/47/2008/©…

    www.damtp.cam.ac.uk/user/mem/mci-jet-hyperb-ADGEO-08.pdf
    1 Jul 2008: Adv. Geosci., 15, 47–56, 2008www.adv-geosci.net/15/47/2008/ Author(s) 2008. This work is distributed underthe Creative Commons Attribution 3.0 License. Advances inGeosciences. Potential-vorticity inversion and the wave-turbulence jigsaw:
  17. Dunajski

    www.damtp.cam.ac.uk/user/md327/DW08.pdf
    18 Mar 2008: Anti-self-dual conformal structures in neutralsignature. Maciej Dunajski and Simon West. Contents. 1 Introduction. 113. 2 Local geometry in neutral signature. 1162.1 Conformal compactification. 1162.2 Spinors. 1172.3 ˛- and ˇ-planes. 1182.4
  18. Multiple Jets as PV Staircases: The Phillips Effect and ...

    www.damtp.cam.ac.uk/user/mem/dritschel-mci08.pdf
    1 Apr 2008: Multiple Jets as PV Staircases: The Phillips Effect and the Resilience ofEddy-Transport Barriers. D. G. DRITSCHELMathematical Institute, University of St. Andrews, St. Andrews, United Kingdom. M. E. MCINTYRECentre for Atmospheric Science, Department
  19. Transient buoyancy-driven front dynamics in nearly horizontal tubesT. …

    www.damtp.cam.ac.uk/user/hinch/publications/PhysFluids_19_123603.pdf
    29 Jan 2008: The front part of the. FIG. 12. a Numerical profiles 2hx / t / d of the interface as a function ofx / VKMt at different normalized times: t = 25 , 50 , 100 , 200 dashed
  20. doi:10.1098/rspa.2007.0130

    www.damtp.cam.ac.uk/user/dmas2/public_ps/RSPA20070130.pdf
    3 Jul 2008: REVIEW. Analysis of the adiabatic limit for solitons inclassical field theory. BY DAVID M. A. STUART. University of Cambridge, Centre for Mathematical Sciences, Wilberforce Road,Cambridge CB3 OWA, UK. We discuss the approximation of classical field
  21. 3 Oct 2008: 2y. t2= c2. 2y. x2, c =. T. ρ. e.g. violin (D-)string: T 40 N, ρ 1 g m1: c 200 m s1.

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