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  2. examples1.dvi

    www.damtp.cam.ac.uk/user/gio10/ad_examples1.pdf
    6 Mar 2006: H α1/103/4(f Ṁ)3/20 µmmpk. 3/8. σ. Cκ. 1/20. Please send comments and corrections to gio10@cam.ac.uk.
  3. Shocking, the slow changes inHKM’s thin coat by HKM2 ...

    www.damtp.cam.ac.uk/user/hinch/talks/hkm3.pdf
    23 May 2006: γ2α = ω2µ3a6/ρ2g2σh7]. γ0.30.250.20.150.10.05. κ/(γγ). 5. 4. 3. 2. 1. ... HKM shocks – p.20/25. Structure of the shock. Quasi-steady, with F A(T ) outside, A = π/T.
  4. D-Branes in Field Theories

    www.damtp.cam.ac.uk/user/tong/talks/dbrane.pdf
    23 Feb 2006: 5. 0. 5. 10. -10-50510. -20 -10 0 10 20. Isozumi, Nitta, Ohashi and Sakai ‘04.
  5. Collapse of a granular columnJohn Hinch in collaboration with ...

    www.damtp.cam.ac.uk/user/hinch/talks/FACM06.pdf
    23 May 2006: 0 5 10 15 20 25(RR0)/R0. 0. 1. 2. 3. 4E S. ... Shallow-water vs SimulationsPSfrag replacements. 4. 3. 2. 1. 00 5 10 15 20.
  6. caqcd.dvi

    www.damtp.cam.ac.uk/user/tong/talks/caqcd.pdf
    12 Sep 2006: 5. 10. -10-50510. -20 -10 0 10 20. -10. -5. Figure 3:.
  7. Cambridge NA Report NA2006/01 Joint Diagonalization on the Oblique ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_01.pdf
    24 Jan 2006: Matrix Anal. Appl. 20 (1998), no. 2, 303–353. [Gab82] D. Gabay, Minimizing a differentiable function over a differential manifold, Journal of Opti-mization Theory and Applications 37 (1982), no. ... Numer. Anal. 20 (1983), 626–637. [TL02] N. T.
  8. Motion of a vortex line near the boundary of ...

    www.damtp.cam.ac.uk/user/ngb23/publications/boundary.pdf
    20 Oct 2006: of Eq. 20 for the uniform flow was found 11 as1 = u1x , y iv1x , y where. ... 0 5 10 15 20. 0.1. 0.2. 0.3. 0.4. 0.5. 0.6.
  9. berloff.dvi

    www.damtp.cam.ac.uk/user/ngb23/publications/warwick.pdf
    7 Sep 2006: complexes. In higher dimensions,domain walls 19 and skyrmions (vortons) 20 have been found. ... 20 -10 0 10 20-20. -10. 0. 10. 20. -20 -10 0 10 20-20.
  10. 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: µ. 0.1. 0.2. 0.3. 0.4. 0.5µ e. 0.425µ0.20. y = x. ... 4.3, we find that k = 0.20 and k =0.17 respectively.
  11. Numerical approximation of vector-valued highly oscillatory integrals …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_06.pdf
    26 Jul 2006: 25 30 35 40 45 50. 0.050.10.150.20.250.3. Figure 2: The error scaled by ω7/4 of QL[f] with endpoints for nodes and multiplicities both ... 25 30 35 40 45 50. 0.050.10.150.20.250.30.35. Figure 3: The error scaled by ω13/4 of QL[f] with endpoints for
  12. On the linear stability of splitting methods Sergio Blanes1∗ ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_08.pdf
    2 Sep 2006: λ1(x) = eiΦ(x), λ2(x) = eiΦ(x), (2.21). where Φ(x) is given by (2.20). ... p(x) = cos(x) O(x2n2) as x 0,. i.e. Φ(x) = x O(x2n1) in (2.20).
  13. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_05.pdf
    20 Jun 2006: 0.05. 20. 0.1. 0.0. 4 102. 0.025. 1886. 0.075. 0.04. 0.06. ... 20. The method (3.6) cannot be used for approximatingf̂C0 and is less precise for small valuesof n, before the onset of asymptotic behaviour.
  14. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/notes.pdf
    28 Oct 2006: 20. 1.7.9 Examples of Gradients. 21. 1.7.10 Divergence and Curl. 21. ... Equating (1.18) and (1.20) yields. l ψ = ddsψ(r sl). s=0.
  15. N13LBb.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBb.pdf
    22 May 2006: 2 PARTIAL DIFFERENTIAL EQUATIONS 20. • at x = L apply insulating boundary condition: there is no flux of heat to x > L.Then have Θx(L,t) = 0, t 0: Neumann condition;. • ... 0 1 2 3 4 5x. 0. 5. 10. 15. 20.
  16. DAMTP 2006/NA03 Fast evaluation of polyharmonic splines in three ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_03.pdf
    31 Aug 2006: The. 20 Fast evaluation of 3D polyharmonic splines. per panel accuracy, and its estimation, are described later. ... 2.20(1)64, 000 3.75(4) 5.31(7) 3.66(0) 1.08(1) 9.06(1).
  17. N13LBa.dvi

    www.damtp.cam.ac.uk/user/rrh/notes/N13LBa.pdf
    22 May 2006: 1. . . =(. 20). . . 6. 4. 1. . ... Similarly, c(bc) =0. 1 LINEAR ALGEBRA 20. 3. Consider. A =. . . a1 a2 a3. b1 b2 b3. c1 c2 c3.
  18. handout_07.dvi

    www.damtp.cam.ac.uk/user/examples/3N2a.pdf
    23 Nov 2006: 2.8 Additional ODE problems and themes. 20. 3 Finite difference methods for PDEs 25. ... Part III: Numerical Solution of Differential Equations 20. Herewith, 〈 , 〉 is the standard Euclidean inner product.
  19. This isa super vis or’ sco py ofth enote ...

    www.damtp.cam.ac.uk/user/sjc1/teaching/NSTIB/Michaelmas/notes.pdf
    28 Oct 2006: 20. 1.7.9 Examples of Gradients. 21. 1.7.10 Divergence and Curl. 21. ... Equating (1.18) and (1.20) yields. l ψ = ddsψ(r sl). s=0.
  20. A Class of Integrable Geodesic Flows on the Symplectic ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_02.pdf
    20 Apr 2006: 6 Involution 20. Proposition 6.3. BX (hλk (X)) = CX (h.
  21. Bnew_BIT.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_04.pdf
    24 Nov 2006: 20 A. ISERLES and G. R. W. QUISPEL and P. S.

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