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Bnew_BIT.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_04.pdf24 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. -
Shocking, the slow changes inHKM’s thin coat by HKM2 ...
www.damtp.cam.ac.uk/user/hinch/talks/hkm3.pdf23 May 2006: 24. ). 1/2. Can also use for β 1 once βT 1. ... HKM shocks – p.24/25. Conclusions. Transients decay. γ2 α, γ 1: exponentially. -
berloff.dvi
www.damtp.cam.ac.uk/user/ngb23/publications/warwick.pdf7 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. -
Explaining the flow of elastic liquidsPenner Lecture, Winter 2006 ...
www.damtp.cam.ac.uk/user/hinch/talks/penner7.pdf17 Feb 2006: Penner Lecture, 2006 – p.24/52. Tension in streamlinesRod climbingSecondary circulationMigration into chainsMigration to centre of pipeFalling rods align with gravityStabilisation of jetsCo-extrusion instabilityTaylor-Couette instability. -
Collapse of a granular columnJohn Hinch in collaboration with ...
www.damtp.cam.ac.uk/user/hinch/talks/FACM06.pdf23 May 2006: µe = 0.47 for centre of massFACM06 2006, runout – p.24/61. -
N13LBa.dvi
www.damtp.cam.ac.uk/user/rrh/notes/N13LBa.pdf22 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. -
N13LBb.dvi
www.damtp.cam.ac.uk/user/rrh/notes/N13LBb.pdf22 May 2006: 22. 3.2.2 properties of limits. 24. 3.2.3 l’Hôpital’s rule. 24. 3.2.4 more examples. ... that. |un l| < ǫ for all n > N. 3 ELEMENTARY ANALYSIS 24. -
DAMTP 2006/NA03 Fast evaluation of polyharmonic splines in three ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_03.pdf31 Aug 2006: We deduce from (56), (57), (58), (22) and the first part of (24)that. ... Numer. Anal., 25(2005), pp. 1–24. R.K. Beatson, M.J.D. Powell and A.M. -
Paper1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2006_05.pdf20 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 -
Motion of a vortex line near the boundary of ...
www.damtp.cam.ac.uk/user/ngb23/publications/boundary.pdf20 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.
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