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  2. Publications: Edited Volumes A. Iserles (ed.), Acta Numerica 27, ...

    www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/Edited.html
    23 May 2018: Iserles (ed.), Acta Numerica 24, Cambridge Univ. Press (2015). A. Iserles (ed.), Acta Numerica 23, Cambridge Univ.
  3. 13 Apr 2018: 4 inset), cf. elastic fiberbundle models [24]. More generally, the LP approach toAmontons-Coulomb friction problems may have applica-tions in stress transmission in granular media, such as sandpiles and grain ... 13, 848 (2017). [24] S. Pradhan, A. Hansen
  4. J. Fluid Mech. (2018), vol. 856, pp. 921–957. c© ...

    www.damtp.cam.ac.uk/user/lauga/papers/152.pdf
    19 Oct 2018: 2.24). Notably, this expression can be simplified into. s0 =sb(rc) r s(.
  5. 14 May 2018: 7.24). where we’ve used the fact that, in a local trivialization, the covariant derivative acts.
  6. Collective dissolution of microbubbles

    www.damtp.cam.ac.uk/user/lauga/papers/145.pdf
    18 Apr 2018: Note that this second casepresents many formal similarities with the dissolution process of droplets [22], their evaporation[23], and even dissolving solids [24]. ... 2)P ′n(μ), (24). Un(η) = An cosh(n 12. )η Bn sinh.
  7. Quantum Field Theory II University of Cambridge Part III ...

    www.damtp.cam.ac.uk/user/dbs26/AQFT/chap1.pdf
    19 Jan 2018: absolutely impossible for a course of 24 lectures to do so). ... showing that the quantity. =. Z. N dd1x (1.24). is conserved under evolution via the classical equations.
  8. Recovery of a Variable Coefficient in a Coastal Evolution Equation

    www.damtp.cam.ac.uk/user/ms100/PAPERS/JCP99.pdf
    13 Dec 2018: F′n1, An,n =τ. 2ξF′n. (24). This is easily and rapidly inverted by back-substitution.
  9. Spectral computation of highly oscillatory integral equations in…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_04.pdf
    2 Nov 2018: operator (the case γ = 1) represents a challenge for spectral theory (Böttcher, Grudsky &. Iserles 2012). 24. Figure 4.3: The eigenvalues of the integral operator with ω = 100 for γ =
  10. statphys

    www.damtp.cam.ac.uk/user/tong/statphys/two.pdf
    31 Dec 2018: f(r) = eU(r) 1 (2.24). This is a nicer expansion parameter.
  11. 1 Nov 2018: 24 –. the commutator of the generator with the operator. ... U (b) U (a) = U (b a) = U (a b) = U (a) U (b) , (4.24).

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