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1 - 10 of 82 search results for KaKaoTalk:PC53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 82 match some words.

  1. Results that match 1 of 2 words

  2. Magnus expansions and pseudospectra of Master Equations

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_01.pdf
    11 Jan 2017: X = tp 12t2[p,k] 1. 6t3[k, [p,k]] t4. (1. 24[p.[p, [p.k]]] 1. ... 24[k, [k, [p,k]]]. )(20)265. t5(. 7. 360[k, [p, [p, [p,k]]]] 1.

  3. rspa.royalsocietypublishing.org ResearchCite this article: Cooray H,…

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Cooray-2016.pdf
    20 Jan 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... angles. SIAM J. Appl. Math. 49, 1009–1028. (doi:10.1137/0149061)24. Vogel TI. 2013 Liquid bridges between balls: the small volume instability.

  4. PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2016.pdf
    20 Jan 2017: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H.

  5. J. Fluid Mech. (2016), vol. 801, pp. 65–90. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Sayag-2016.pdf
    20 Jan 2017: A 24.6 25.5 1.403 4 — 5.3 10.7 5.2B 43.6 24.7 1.4 4.7 20 6.3 13.3 3.4C 36.6

  6. An inverse method for estimating thickness and volume with time of a…

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Cowton-2016.pdf
    20 Jan 2017: Accepted article online 24 JUN 2016. Published online 13 JUL 2016.

  7. J. Fluid Mech. (2016), vol. 791, pp. 329–357. c� ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2016.pdf
    20 Jan 2017: Note that (2.24) implies thatui is independent of z in the interior of each isopycnal layer, hi1 < z < hi. ... interior of each layer, @ui/@z = 0,as implied by (2.24).

  8. Fokas Method (unified transform) January 25, 2017 1 Brief ...

    www.damtp.cam.ac.uk/user/examples/3N15.pdf
    26 Jan 2017: where. û1(λ) eiλN1l=0. [iλal1P̂l(λ) b. l1P̂l(λ). ],. 24. û2(λ) eλN1l=0. [λal2P̂l(iλ) bl2P̂l(iλ). ],. ... Appl. Math. 24 (2013), no. 6, 857–886, DOI10.1017/S0956792513000223. MR3181485. [24] B.

  9. Fast expansion on the real line Helge Dietert∗ Arieh ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_02.pdf
    13 Feb 2017: Askey. 24. Jin, S., Markowich, P. & Sparber, C. (2011), ‘Mathematical and computational meth-ods for semiclassical Schrödinger equations’, Acta Numer.

  10. Uniform and high-order practical implementation ofSturm–Liouville…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_04.pdf
    15 Feb 2017: A , [B, [A , C ]]] = 0, [B, [A , [B, G ]]] = 0, [C , [A , [C , E ]]] = 0, (3.24)[A , [B, [A , E ]]] = 0, [B, [B, [B, C ]]] = 0, [C , [A , [C , G ]]] =

  11. Theory of Shape-Shifting Droplets Pierre A. Haas,1 Raymond E. ...

    www.damtp.cam.ac.uk/user/gold/pdfs/shape_shifting.pdf
    21 Feb 2017: 24 FEBRUARY 2017. 0031-9007=17=118(8)=088001(5) 088001-1 Published by the American Physical Society. ... 24 FEBRUARY 2017. 088001-3. freezing [Fig. 4(a)], a strong experimental signature of theformation of rotator phase next to the perimeter [3].

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