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1 - 10 of 17 search results for :pc53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 17 match some words.

  1. Results that match 1 of 2 words

  2. A Class of Integrable Geodesic Flows on the Symplectic ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_02.pdf
    20 Apr 2006: REFERENCES 24. A generalized system. The flow of (1.1) can be rendered more general bycomplexification.

  3. Collapse of a granular columnJohn Hinch in collaboration with ...

    www.damtp.cam.ac.uk/user/hinch/talks/FACM06.pdf
    23 May 2006: µe = 0.47 for centre of massFACM06 2006, runout – p.24/61.

  4. Granular MatterDOI 10.1007/s10035-006-0033-z The spreading of a…

    www.damtp.cam.ac.uk/user/hinch/publications/GranularMatter2007.pdf
    19 Dec 2006: 24, 0.41, 0.56 and 1.,where T is the total duration of the spreading, and for a restitution e = 0.5 and a inter-grain friction µ = 1.

  5. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf
    28 Oct 2006: 1.7.13 Aide Memoire. 24. 2 Partial Differential Equations 25. 2.0 Why Study This? ... You should be able to do example sheets 1/2/3/4 after lectures 6/12/18/24 respectively.

  6. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/AandG/notes.pdf
    11 Nov 2006: 2.6.2 Three dimensional space. 23. 2.6.3 Higher dimensional spaces. 24. 2.7 Components. ... 24. 2.7.1 The Cartesian or standard basis in 3D. 24. 2.7.2 Direction cosines.

  7. Bnew_BIT.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_04.pdf
    24 Nov 2006: ẏ4 = 1. Σ = 1σ( rr r )σ( r) = 24 nr rr r ẏ1 = 12 y2y3ẏ2 = y1y4. ... 24 A. ISERLES and G. R. W. QUISPEL and P. S.

  8. berloff.dvi

    www.damtp.cam.ac.uk/user/ngb23/publications/warwick.pdf
    7 Sep 2006: 1 Λ2. (27). In a compact form the equations (24) can be written as. ... 24). The solid lines show three families of solutionswith α1 = α2 = 0.5 and Λ.

  9. Motion of a vortex line near the boundary of ...

    www.damtp.cam.ac.uk/user/ngb23/publications/boundary.pdf
    20 Oct 2006: From Eq. 22 we have. U1 =E1/y0p1/y0. =1. 2y0, 24. as expected.For large y0 an accurate approximation to the solution.

  10. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_05.pdf
    20 Jun 2006: 24. Intriguingly, Filon-type methods (3.11) lend themselves to an alternative interpretation.Comparing (3.11) with (3.1), we observe that. ... Num. Anal.24, 365–391. Iserles, A. & Nørsett, S. P. (2004), ‘On quadrature methods for highly oscillatory

  11. N13LBa.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBa.pdf
    22 May 2006: 1.4 Inverse of a matrix. 24. 1.4.1 Uniqueness of inverse. 24. ... . (. 1 4 2). =. . . 6 24 124 16 81 4 2.

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