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  1. Results that match 1 of 2 words

  2. kintheory

    www.damtp.cam.ac.uk/user/tong/kintheory/four.pdf
    16 Sep 2023: We plug this into the equation of motion (4.20) to getZ 1. ... Im(!) =! (!20! 2)2 2!2. (4.24). This is an odd function.
  3. Nick_retirement_conference

    www.damtp.cam.ac.uk/user/mjc249/talks/Nick_NEP_mjc.pdf
    17 Aug 2023: Stability bound. 20. Keldysh: 𝑇(𝑧)1 = 𝑉(𝑧 𝐽)1𝑊 𝑅(𝑧), let 𝑀 = sup𝑧Ω 𝑅(𝑧). ... Slide 19: InfBeyn algorithm. Slide 20: Stability and convergence result. Slide 21: Proof sketch (probably no time).
  4. Residual Dynamic Mode Decomposition Rigorous data-driven computation…

    www.damtp.cam.ac.uk/user/mjc249/talks/INI_ResDMD.pdf
    9 Mar 2023: 17. 20. 18. 20. 19. 20. 20. 20. 21. New Papers on“Koopman Operators”. ... 12:. 13:. 14:. 15:. 16:. 17:. 18:. 19:. 20:. anm1:. pbs@ARFix@40:.
  5. J. Fluid Mech. (2017), vol. 813, pp. 929–954. c© ...

    www.damtp.cam.ac.uk/user/drh39/2017_viscobl.pdf
    1 Dec 2023: on. 08 Ja. n 20. 20 a. t 15:. 00:5. 1, s. ... n 20. 20 a. t 15:. 00:5. 1, s. ubje. ct to.
  6. doi:

    www.damtp.cam.ac.uk/user/drh39/2013_thixo.pdf
    1 Dec 2023: The bentonite,shown in (b)–(d), is on a 20 slope and the ageing times Tage are indicated. ... 1.0. 0.5. 0. 2.0. 1.5. 1.0. 0.5. 0 10 20 30.
  7. J. Fluid Mech. (2022), vol. 936, A17, doi:10.1017/jfm.2022.48…

    www.damtp.cam.ac.uk/user/drh39/2022_swim.pdf
    1 Dec 2023: 4. –4. 0. 4. –8. –4. 0. 4. 8. 0 10 20 30 40. ... 0 10 20 30 40 0 10 20 30 40 0 10 20 30 40.
  8. J. Fluid Mech. (2020), vol. 882, A11. c© Cambridge ...

    www.damtp.cam.ac.uk/user/drh39/2020_squirm.pdf
    1 Dec 2023: on. 08 Ja. n 20. 20 a. t 14:. 53:1. 8, s. ... n 20. 20 a. t 14:. 53:1. 8, s. ubje. ct to.
  9. clas

    www.damtp.cam.ac.uk/user/tong/dynamics/one.pdf
    13 Sep 2023: 2.3 Constraints and Generalised Coordinates 17. 2.3.1 Holonomic Constraints 18. 2.3.2 Non-Holonomic Constraints 20. ... This is given by,. Fij = Qvi Bj (1.20). where vi is the velocity of the ith particle and Bj is the magnetic.
  10. On two‐phase modeling of dewatering pulp suspensions

    www.damtp.cam.ac.uk/user/drh39/2021_pulp.pdf
    1 Dec 2023: 3 SBK (Resolute, Catawba)d 730 2.45 26.8. 4a HBK (Domtar)e 610 0.79 20.1. ... 19 BCTMP (Rayonier) 13 200 0.77 23.5. 20 BCTMP (Rayonier) 30 128 0.72 23.7.
  11. www.sciencemag.org/cgi/content/full/325/5939/487/DC1 Supporting…

    www.damtp.cam.ac.uk/user/gold/pdfs/gears_SM.pdf
    21 May 2023: both cameras with custom Labview (National Instruments, Austin, TX) routines at 20 fps and. ... diffusion constant only 20% higher than the real mean. The real distribution of diffusivities.
  12. Obstructed viscoplastic flow in a Hele-Shaw cell

    www.damtp.cam.ac.uk/user/drh39/2020_masoud.pdf
    1 Dec 2023: 19].Carbopol was then pumped through the cell for approximately 20 minutes before flow visualizationcommenced. ... uniform slot with treated walls, combining optical coherence tomography (Thorlabs TEL1300V2-BU) with particle-tracking velocimetry [20,21].
  13. Advancing optothermal manipulation: decoupling temperature and flow…

    www.damtp.cam.ac.uk/user/lauga/papers/218_news_views.pdf
    5 Sep 2023: Nat. Cell Biol. 20, 344–351 (2018). 7. Chartier, N. T. et al.
  14. Microswimmers in vortices: dynamics and trapping

    www.damtp.cam.ac.uk/user/lauga/papers/214.pdf
    7 Dec 2023: As a test case, wechoose a frequency of rotation of f = 20 Hz, cells of shape factorB = 0.85 (corresponding to aspect ratio a E 3.51) and take thevalues for ... r r r L, where L c Rd with Rd beingthe radius of the depletion zone reported experimentally
  15. J. Fluid Mech. (2018), vol. 856, pp. 870–897. c© ...

    www.damtp.cam.ac.uk/user/drh39/2018_viscoslender.pdf
    1 Dec 2023: on. 08 Ja. n 20. 20 a. t 15:. 01:2. 8, s. ... n 20. 20 a. t 15:. 01:2. 8, s. ubje. ct to.
  16. J. Fluid Mech. (2020), vol. 883, A37. c© Cambridge ...

    www.damtp.cam.ac.uk/user/drh39/2020_layeredplume.pdf
    1 Dec 2023: on. 08 Ja. n 20. 20 a. t 14:. 51:0. 1, s. ... n 20. 20 a. t 14:. 51:0. 1, s. ubje. ct to.
  17. J. Fluid Mech. (2018), vol. 855, pp. 1170–1207. c© ...

    www.damtp.cam.ac.uk/user/drh39/2018_glacial.pdf
    1 Dec 2023: on. 08 Ja. n 20. 20 a. t 14:. 58:3. 9, s. ... 08 Ja. n 20. 20 a. t 14:. 58:3. 9, s.
  18. PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...

    www.damtp.cam.ac.uk/user/drh39/2016_squishy.pdf
    1 Dec 2023: 0 20 40 60 80 100 120. 8. 10. 12. 0 20 40 60 80 100 1200. ... For the simple elastic rheologyconsidered in this paper, these functions are given by (20)and (21), respectively.
  19. J. Fluid Mech. (2015), vol. 778, pp. 335–360. c© ...

    www.damtp.cam.ac.uk/user/drh39/2015_porolayer.pdf
    1 Dec 2023: 0. 0. 5 10 15 20 25 30. 50 100 150 200 250. ... 0 100–100 200–200 300–300 400–400. 15. 20. 5. 0. 10. 15.
  20. PDEs_meets_DATA_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/PDE_meets_data_mjc.pdf
    19 Sep 2023: 17. 20. 18. 20. 19. 20. 20. 20. 21. New Papers on“Koopman Operators”. ... 2 < 𝜀2. Measure of statistical coherency. 20. Sampler of the results we prove.
  21. J. Fluid Mech. (2019), vol. 869, pp. 468–499. c© ...

    www.damtp.cam.ac.uk/user/drh39/2019_JPlayers.pdf
    1 Dec 2023: y. y. x0.5 1.0 1.5 -30 -20 -10 0 10 20 30. ... ß = 1. ß = 0.5. 0. 0.20.40.60.81.0. 0. 1.21.4. 1.5.
  22. Dewatering of fibre suspensions by pressure filtration

    www.damtp.cam.ac.uk/user/drh39/2016_pulp.pdf
    1 Dec 2023: Wetherefore avoid this formalization, which mostly involves confirming that φ/t in (20) can beneglected in comparison to the other two terms. ... Allresults have n=3 and φ0=0.01. u = γDφζ/φ =1 for ζ = 0, the integral of (20) furnishes.
  23. 1 Dec 2023: 5(a). In an attempt to collapse the data, Fig. 5(c) shows the penetration length against the scaleddimensionless time tk0Pc/µ, with Pc γ k1/20 [cf. ... 29.[19] P. LePoutre, Liquid absorption and coating porosity, Paper Technol. 19, 298 (1978).[20] R.
  24. The difficulty of computing stable and accurate neural networks On…

    www.damtp.cam.ac.uk/user/mjc249/talks/SAE_mjc.pdf
    9 Feb 2023: 0.0030000 0.0025980 n = 20 103. 0.0030000 0.0025980 n = 30 103. ... 0.0000030 0.0000015 n = 10 106. 0.0000030 0.0000015 n = 20 106.
  25. J. Fluid Mech. (2018), vol. 837, pp. 520–545. c© ...

    www.damtp.cam.ac.uk/user/drh39/2018_JPfinger.pdf
    1 Dec 2023: 10–20. 10–2 100 102. 10–1 100 101. 10–10. 100. 0 0.1. ... For example, in figure 5(c) the critical Péclet number liesbetween 15 and 20.
  26. J. Fluid Mech. (2014), vol. 756, pp. 844–869. c© ...

    www.damtp.cam.ac.uk/user/drh39/2014_layer.pdf
    1 Dec 2023: 40. 30. 20. 10. 010–3 10–2 10–1 100. 40. 30. 20. ... R. Lister. Trms. wrms. urms. Nu. 40. 30. 20. 0.25. 0.20.

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