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  2. 1 Dec 2023: 24)]. 074001-14. IMBIBITION WITH SWELLING: CAPILLARY RISE IN. (a) (b) (c) (d). ... Fluids 17, 087104. (2005).[24] J. L. Sommer and A. Mortensen, Forced unidirectional infiltration of deformable porous media, J.
  3. Publications: Refereed Journals Jing Gao & Arieh Iserles, "A …

    www.damtp.cam.ac.uk/user/na/people/Arieh/Arieh_Iserles/Papers.html
    22 Feb 2024: Num. Anal. 24 (2004), 365–391. A. Iserles, "On the global error of discretization methods for highly-oscillatory ordinary differential equations'', BIT 42 (2002), 561–599. ... Comp. Maths 14 (2001), 1–24. A. Iserles, "On Cayley-transform methods
  4. PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...

    www.damtp.cam.ac.uk/user/drh39/2016_squishy.pdf
    1 Dec 2023: 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. Microswimmers in vortices: dynamics and trapping

    www.damtp.cam.ac.uk/user/lauga/papers/214.pdf
    7 Dec 2023: KaðzÞ)ffiffiffiffiffip2z. re%z 1þ4a. 2 %18z. þð4a2 %1Þð4a2 %9Þ. 128z2! "; (24).
  6. On two‐phase modeling of dewatering pulp suspensions

    www.damtp.cam.ac.uk/user/drh39/2021_pulp.pdf
    1 Dec 2023: 23 TMP (West Fraser) 112 580 1.59 36.4. 24 TMP (West Fraser) 229 390 1.50 35.6. ... found in Reference 24. At least four trials for each pulp suspension were.
  7. 20 Apr 2024: 2.1.2 The Infinite Potential Well 24. 2.1.3 The Gaussian Wavepacket 27.
  8. dynrel

    www.damtp.cam.ac.uk/user/tong/relativity/one.pdf
    27 Jan 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25.
  9. J. Fluid Mech. (2024), vol. 978, R1, doi:10.1017/jfm.2023.849…

    www.damtp.cam.ac.uk/user/lauga/papers/222.pdf
    2 Jan 2024: 24, 313–358.PELLE, D.W., BROKAW, C.J., LESICH, K.A. & LINDEMANN, C.B. 2009 Mechanical properties of the.
  10. 2 A Quantum Particle in One Dimension There is ...

    www.damtp.cam.ac.uk/user/tong/qm/qm2.pdf
    20 Apr 2024: d2h. dy22ydh. dy+ (Ẽ 1)h = 0 (2.26). You can check that this is indeed satisfied by our earlier solution (2.24) with h = 1. ... We learn that the. Gaussian wavefunction (2.24) that we guessed earlier is actually the lowest energy.
  11. 2 Jan 2024: 1B), owing to the cell-to-cell variations inmetabolism and the number and morphology of flagella (24).Thanks to the large sample size of our experiments, we are able tomeasure the

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