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  2. Chapter 2 Poisson’s Equation 2.1 Physical Origins Poisson’s equation, …

    www.damtp.cam.ac.uk/user/reh10/lectures/nst-mmii-chapter2.pdf
    8 Mar 2004: 24 R. E. Hunt, 2002. and both sides must be constant, λ say.
  3. EXPONENTIAL BROWNIAN MOTION AND DIVIDED DIFFERENCES B. J. C. ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_06.pdf
    14 Jul 2004: Appl. Prob. 24 (1992),. 509–531. School of Economics, Mathematics and Statistics, Birkbeck College, University of.
  4. Giulio Del Zanna - Publications

    www.damtp.cam.ac.uk/user/astro/gd232/publications.html
    21 Apr 2004: Del Zanna G., 2002, proc. workshop on High resolution X-ray spectroscopy with XMM-Newton and Chandra, MSSL, 24 - 25 October 2002.
  5. INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...

    www.damtp.cam.ac.uk/user/ngb23/publications/pair.pdf
    19 Jan 2004: 2iUψ. z= 2ψ (1 |ψ|2)ψ (24). subject to the boundary condition ψ 1 as |x|. ... The expansion of equation (24) about zero to O(2) gives four equations on seven unknownsU, m, a00, b00, c20, c10, c01.
  6. INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...

    www.damtp.cam.ac.uk/user/ngb23/publications/motionIX.pdf
    8 Oct 2004: EP/Uk. 2 =(κ. 2πh. )2k2. [lnh. 2aδ+. 1. 2. ](24). which differs from (18) by 12.
  7. INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...

    www.damtp.cam.ac.uk/user/ngb23/publications/motionX2.pdf
    19 Nov 2004: VpLp dV = 2iσ. V. p[ψ 20 p. 2iσp] dV. (24)Re-arranging this equation and using (15) again, we find that. ... S′ = 12zR. ′ v00 R′, (B.24). or, after simplification,. 2.
  8. Interactions of vortices with rarefaction solitary waves in a ...

    www.damtp.cam.ac.uk/user/ngb23/publications/interact2.pdf
    25 Jun 2004: 1.24 for U = 0.63 andh , dy1.62 for U. = 0.69.
  9. Introduction E.J. Hinch D.A.M.T.P. Cambridge University Mobile…

    www.damtp.cam.ac.uk/user/hinch/teaching/mobile.pdf
    23 Apr 2004: Fibres (and platelets, although they are less well studied) are used in compositematerials because a small volume fraction can have a large effect on the properties(see chapter 24 by Shaqfeh). ... Shaqfeh describes in chapter 24 how fibres can have avery
  10. NA2004_08.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_08.pdf
    14 Nov 2004: n. }. (4.24). Therefore v is the opt-th column of the matrix W , so expression (3.12) impliesHv = eopt in theory, where eopt is the opt-th coordinate vector in
  11. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_02.pdf
    23 Jan 2004: 24 h(1. 14 cos 2ωh). 8ω2+. 5 sin 2ωh. 64ω3,. θ4 =h4.

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