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31 - 40 of 126 search results for :pc53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 126 match some words.

  1. Results that match 1 of 2 words

  2. Taming Discretization Challenges for Nonlinear Eigenvalue Problems

    www.damtp.cam.ac.uk/user/mjc249/talks/INI_NEP_mjc.pdf
    26 Jul 2023: Slide 23: InfBeyn algorithm. Slide 24: Stability and convergence result. Slide 25: Proof sketch.

  3. Obstructed viscoplastic flow in a Hele-Shaw cell

    https://www.damtp.cam.ac.uk/user/drh39/2020_masoud.pdf
    1 Dec 2023: not always) suppress any interaction [24]. ... 24] E. Chaparian, A. Wachs, and I. A. Frigaard, Inline motion and hydrodynamic interaction of 2D particlesin a viscoplastic fluid, Phys.

  4. Biophysical Fluid Dynamics in a Petri Dish George T. ...

    www.damtp.cam.ac.uk/user/gold/pdfs/petridish130224.pdf
    13 Feb 2024: Rotletflows arise from (d) the bacterium Escherichia coli under confinement, generating flow field in (e) [24], (f)a magnetic nano stir bar [25], and (g) a macroscopic stirrer [26]. ... 23 eqs. 29-30. Stokeslet Main text eq. 24 eqs. 32-34.Rotlet Appendix

  5. Natural Sciences Tripos Part IB Michaelmas 2023 Professor Anders ...

    https://www.damtp.cam.ac.uk/research/afha/lectures/NST_1A/nstIB_Anders_2023.pdf
    21 Nov 2023: af(t) dt. b. ag(t) dt , (24). »»»»»»»». b. af(t) dt. »»»»»»»». ... 24. Taylor series for analytic functions. Zeros, Poles and Essential Singularities.

  6. Flow-driven compaction of a fibrous porous medium

    https://www.damtp.cam.ac.uk/user/drh39/2019_compact.pdf
    1 Dec 2023: Moreover, the onlyexisting models of freeness are semi-empirical and based on the average filter resistance of thecompacting pulp [22–24]. ... 24)The integral of Eq. (22) across the height of the solid also provides the global force balancecondition,.

  7. J. Fluid Mech. (2023), vol. 963, A24, doi:10.1017/jfm.2023.336…

    www.damtp.cam.ac.uk/user/lauga/papers/216.pdf
    24 Jul 2023: δjk 12. dR̂jdŝ. dR̂kdŝ. )(ũk (R̂) ũk (ŝ). )dŝ,. (2.24). where R̂i = R̃i(ŝ). ... 3.1.1. Computation of forces and torquesUnder this parametrisation, (2.24) becomes. Ji = η̃s2. [

  8. FoCM: Solve-the-discretize for NLEPS

    www.damtp.cam.ac.uk/user/mjc249/talks/FOCM_2023_NEP_mjc.pdf
    15 Jul 2023: Slide 23. Slide 24: Example 4: Planar waveguide. Slide 25: Example 4: Planar waveguide.

  9. Preprint typeset in JHEP style - HYPER VERSION Michaelmas ...

    www.damtp.cam.ac.uk/user/tong/qft/qft.pdf
    20 Mar 2024: where Λµν satisfies. Λµσ ηστ Λντ = η. µν (1.24). For example, a rotation by θ about the x3-axis, and a boost by v < 1 along the x1-axis. ... The condition (1.24) for Λ to be a Lorentz transformation. becomes. (

  10. kintheory

    www.damtp.cam.ac.uk/user/tong/kintheory/two.pdf
    16 Sep 2023: i(2.24). This is the Boltzmann equation. It’s not an easy equation to solve! ... 24 –. things change for quantum particles. We’ll keep the assumption of molecular chaos,.

  11. Koopman_turing_talk_mjc

    www.damtp.cam.ac.uk/user/mjc249/talks/rigged_DMD_turing.pdf
    23 May 2024: 24. Residual DMD (ResDMD).

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