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  2. doi:

    www.damtp.cam.ac.uk/user/drh39/2013_thixo.pdf
    1 Dec 2023: in figures 11 and 12. Figure 11 shows profiles of samples with different ageing timesTage on inclines of 20; figure 12 shows profiles on slightly steeper inclines of 24.As a
  3. Natural Sciences Tripos Part IA Mathematical Methods I — ...

    www.damtp.cam.ac.uk/research/afha/lectures/NST_1A/nstIAm_Anders_Notes_2023.pdf
    3 Oct 2023: Scalar product properties:. 1. The scalar product is commutative,. a b = b a , (24). ... Using (25) and then (24) yields the useful result. (a b)2 = a2 b2 2a b.
  4. 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.
  5. Rate invariance and scallop theorem in viscosity gradients

    www.damtp.cam.ac.uk/user/lauga/papers/217.pdf
    24 Jul 2023: 106, 27 (2016).[24] L. Schwarz, M. Medina-Sánchez, and O. G. Schmidt, Hybrid biomicromotors, Appl. ... symmetry breaking, Phys. Fluids 24, 103102 (2012).[36] J. P. Binagia and E.
  6. Obstructed viscoplastic flow in a Hele-Shaw cell

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

    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.
  8. Flow-driven compaction of a fibrous porous medium

    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,.
  9. 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
  10. 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. [
  11. 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.

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