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  2. Pigeonhole I10 Mathematical Methods II Dr R. E. HuntNatural ...

    www.damtp.cam.ac.uk/user/reh10/lectures/nst-mmii-solutions1.pdf
    2 Mar 2004: 7 Consider B. Adf. Note that df = f.dr, and use an inequality for a.b for any two vectors. ... a and b. To obtain the required condition for equality, recall that f lies orthogonalto the family of surfaces f = constant.
  3. Evolution of rarefaction pulses into vortex rings Natalia G. ...

    www.damtp.cam.ac.uk/user/ngb23/publications/evolution.pdf
    25 Jun 2004: 15. EVOLUTION OF RAREFACTION PULSES INTO VORTEX RINGS PHYSICAL REVIEW B 65 174518. ... Phys. A 15, 2599 1982! 7 B. B. Kadomtsev and V.
  4. Paper1.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_04.pdf
    25 Mar 2004: The Killing form evaluated on a pair of nn skew-symmetric matricesA, B is actually (n 2)trace AB (see (Kobayahsi & Nomizu 1969)). ... . 0 a b ca 0 c bb c 0 ac b a 0.
  5. vtalk.dvi

    www.damtp.cam.ac.uk/user/tong/talks/vsvs.pdf
    29 Nov 2004: B B B ( )( ( )1 0 11)0 1. Figure 2: A magnetic monopole emitting two flux tubes. ... Phys. B 492, 152 (1997) [arXiv:hep-. th/9611230].[15] A. Hanany and K.
  6. IserlesNorsett2.dvi

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_05.pdf
    17 Jun 2004: be ν 2 prescribed nodes in the interval [a, b]. Having chosen multiplicities. ... b. ml2 c,. cν = b : b γ. ωk, k = 0, 1,. ,
  7. Appendix I: Rossby-wave propagation and shear instability M. E. ...

    www.damtp.cam.ac.uk/user/mem/GEFD-SUMMER-shear-instability.pdf
    30 Sep 2004: ψ̂ =. . . . . . A sinh(2kb).ek(yb) (y > b). ... A sinh k(y b) B sinh k(b y) (b < y < b).

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