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15 Feb 2005: A. (1973), Astron. Astrophys. 24, 337]. It is motivated by the dimensional concept that whatever physical process gives.

16 Feb 2005: 24 cm5 g2 K7/2. These opacity laws hold fairly well in ionized accretion discs, Kramers opacity in the outer.

3 Feb 2005: Accretion Discs Mathematical Tripos, Part III. Dr G. I. Ogilvie Lent Term 2005. Linear case. In the linear case, the general solution may be found as a linear superposition of elemen-. tary solutions. One may look for elementary solutions in which

26 Sep 2005: Adexp(a) = expm(ada). (2.24). 2.4. Differential equations on manifolds. We wish to return to general differential equations on manifolds, as given in (2.1).In order to construct

7 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

7 Feb 2005: y0, n = 0, 1, 2,. 24. The following four-stage Runge–Kutta method has order four,.

4 Mar 2005: Further, show that if oneJacobi iteration is performed, thenu3,3 = 23/24 occurs, which is the estimate ofu( 12 ,.

15 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.

24 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.

17 Feb 2005: ω1. )and the. 24. third is at least O(ω1. )– actually, it is easy to prove that it is O. (