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Paper1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_01.pdf29 Jan 2005: 20. we might take. E1,1 =. . . . 24 12. ... . , E1,2 =. . . . 24. 2. 4 02. -
Explicit Magnus expansions for nonlinear equations Fernando Casasa…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_05.pdf15 Aug 2005: a classical Runge–Kutta method, thus obtaining the so-called Runge–Kutta–Munthe-. Kaas (RKMK) class of schemes [24, 17]. ... Matrix Anal. Appl. 15 (1994), pp. 881-902. [24] H. Munthe-Kaas, High order Runge–Kutta methods on manifolds, Appl. -
On the value of the max-norm of the orthogonal ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_09.pdf14 Dec 2005: PRk,2(). 1 24. 2. π. k 3k. 2=. 36. 2π. k, thus. ... Mathematics of Computation, Vol. 24, No.109, (1970), 155–158. [5] W. Light. -
monopole.dvi
https://www.damtp.cam.ac.uk/user/tong/tasi/monopole.pdf30 Sep 2005: D0φ = δαφ Ẋα (2.24). Plugging this into the action (2.3) we find. ... This procedure has been carried out for a number of examples [22, 23, 24]. -
Lucidity, science, and the arts: what we can learn ...
www.damtp.cam.ac.uk/user/mem/kobe-reprint-web.pdf7 Apr 2005: Lucidity, science, and the arts:. what we can learn from. the way perception works. MICHAEL E. McINTYRE. Department of Applied Mathematics and Theoretical Physics,Centre for Mathematical Sciences,. Wilberforce Road,Cambridge CB3 0WA, UK. -
Asymptotic Approaches to Transition Modelling Stephen J. Cowley…
www.damtp.cam.ac.uk/user/sjc1/papers/AGARD.pdf7 Nov 2005: Asymptotic Approaches to Transition Modelling. Stephen J. Cowley Xuesong WuDAMTP Department of Mathematics. University of Cambridge Imperial CollegeSilver Street 180 Queen’s Gate. Cambridge CB3 9EW London SW7 2BZUK UK. SUMMARY. The linear and -
Interlacing property for B-splines Simon Foucart Department of…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_03.pdf24 Feb 2005: Email address: S.Foucart@damtp.cam.ac.uk (Simon Foucart). Preprint submitted to Journal of Approximation Theory 24 February 2005. ... IzvestiyaAkad. Nauk SSSR, Ser. Mat. 15 (1951), 401-420. 24. -
IserlesNorsett4.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_08.pdf23 Nov 2005: 2.4. 40. 2. 2.6. 2.2. ω80. 0.12. 60. 0.24. 0.2. 100. -
IserlesNorsett3.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_02.pdf17 Feb 2005: ω1. )and the. 24. third is at least O(ω1. )– actually, it is easy to prove that it is O. ( -
newnotes.dvi
www.damtp.cam.ac.uk/user/phh/atmosocean/atmos-ocean.pdf19 Sep 2005: 3.24). Posing the expansion η̂ = η̂0 ǫη̂1. it follows at leading order in ǫ that. ... with the boundary condition (3.24) reducing to η̂ = 0 at y = 0,L.
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