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University of Cambridge DAMTP: Professor Peter Wadhams
www.damtp.cam.ac.uk/user/pw11/10 May 2005: developing new techniques of estimating ice type and thickness from remote sensing, based on validation experiments with submarines using SAR, passive microwave and laser profilometry;. ... New EU projects which started in 2001 are:-. further work on the -
mf4.dvi
www.damtp.cam.ac.uk/user/tong/dynamics/mf4.pdf16 Nov 2005: 21 p. 22), determine the new Hamil-. tonian H(Qi, Pi). Use this to solve for the dynamics under the constraint Q2 = P2 = 0. ... Explain why the. theory of adiabatic invariants cannot be used to calculate the new orbit. -
Lect17.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect17.pdf21 Feb 2005: to the grid) pass unnoticed!Bad news:For |θ|, |ψ| = O. (. ... small attenuation already familiar from the analysis of Gauss–Seidel.Good news:Consider just thelarge frequencies.Then. -
Examples2.dvi
www.damtp.cam.ac.uk/user/na/PartII/Examples2.pdf7 Feb 2005: . . You should find that the(2, 3) element of the new matrix isO(. ... ε3). and that the new matrix has exactly thesame trace asA. -
Lect24.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect24.pdf4 Mar 2005: t3). (5.16). Thus,etBetC = et(BC) t 0 only if B andC commute.[Note: It is trivial to prove that commutativityis sufficient, not just necessary.]The good news is, however, -
Lect10.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect10.pdf7 Feb 2005: Definition 3.10 (Multistep methods)It is often useful to use past solution values in computing a new value.Thus, assuming thatyn, yn1,. , -
Lect07.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect07.pdf31 Jan 2005: adjacent columns of a matrix, thetotal number of nonzero elements in the new combination of rows or columns is at most five. -
Lect03.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect03.pdf19 Jan 2005: It follows from the symmetry ofAand the new assertion(2) that the proof is complete. -
Lect05.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect05.pdf25 Jan 2005: The reason for the new step2 is thatf (λ) = 0 implies thatx(k) satisfiesAx(k) = (λ s(k))x(k). -
Accretion Discs Mathematical Tripos, Part III Dr G. I. ...
www.damtp.cam.ac.uk/user/gio10/afd.pdf20 Jan 2005: mass does not vanish in general. However, some new topological invariants associated with. -
PRL 94, 010403 (2005) P H Y S I ...
www.damtp.cam.ac.uk/user/ngb23/publications/rarevort.pdf12 Jan 2005: A question that arises after new solutions are foundtheoretically is how to create them in an actual physicalsystem. ... In [11] we established a new mechanism of vortexnucleation by collapsing bubbles in the context of the GPmodel. -
Lucidity, science, and the arts: what we can learn ...
www.damtp.cam.ac.uk/user/mem/kobe-reprint-web.pdf7 Apr 2005: We dare to tolerate individual opinions. We dare to talk aboutan amazing new thing called human rights, and sometimes even take theidea seriously. ... 11. it the first city-sized human communities (as well as lots of new human andanimal diseases, as -
monopole.dvi
www.damtp.cam.ac.uk/user/tong/tasi/monopole.pdf30 Sep 2005: we must read off the theory on the D1-branes, which we expect give us a new perspective. ... g2 Tr (N. a=1. ψaψa† ψ̃†aψ̃a [Z,Z†] [W,W†])2 g2 Tr |. N. a=1. ψaψ̃a [Z,W ]|2. We’ve actually introduced more new parameters here than -
IserlesNorsett3.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_02.pdf17 Feb 2005: Quadrature methods for multivariate highly. oscillatory integrals using derivatives. Arieh Iserles and Syvert P. Nørsett†. We dedicate this paper to the memory of Germund Dahlquist. Abstract. While there exist effective methods for univariate -
Nucleation of solitary wave complexes in two-component mixture…
www.damtp.cam.ac.uk/user/ngb23/publications/2twod.pdf21 Mar 2005: The surface flow increasesuntil it again reaches criticality, when a new complex isnucleated and the whole sequence is repeated. -
Part II Statistical Mechanics, Lent 2005 Prof. R.R. Horgan ...
www.damtp.cam.ac.uk/user/rrh/notes/sphys.pdf14 Feb 2005: Because the species are distinguishable, the new system,S12, is not initially in equilibrium but initially has entropy S1 S2. ... The gases mixand after equilibrium has been attained the partition function of the new system, ofvolume V = V1 V2, is. -
Asymptotic Approaches to Transition Modelling Stephen J. Cowley…
www.damtp.cam.ac.uk/user/sjc1/papers/AGARD.pdf7 Nov 2005: How-ever, a number of the asymptotic scalings changesignificantly for transonic, supersonic and hypersonicflows, and there a number of new phenomenon (e.g.Smith & Bowles 1993, Smith 1989, Cowley & Hall1990). -
Explicit Magnus expansions for nonlinear equations Fernando Casasa…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_05.pdf15 Aug 2005: conveniently modified version of the Magnus expansion to construct a new class of. ... Here new Lie group solvers up to order four for (2) are presented. -
newnotes.dvi
www.damtp.cam.ac.uk/user/phh/atmosocean/atmos-ocean.pdf19 Sep 2005: 3.37) gives a rule for updating Pg. (3.36) allowsthe new ψ (and hence the new u, v and η) to be determined from the new Pg. -
an2000.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2000_03.pdf26 Sep 2005: A familiar case in pointis the discovery of solitons in the solution of the Korteweg–de Vries equation byZabusky and Kruskal (1965), an event which launched a whole new mathematicaldiscipline, other
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