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  2. Energetics of synchronization for model flagella and cilia

    www.damtp.cam.ac.uk/user/lauga/papers/189.pdf
    8 Jul 2021: For larger ciliatedcells [24], or for multicellular aquatic organisms equippedwith many short flagella [25], the synchronization dynamicstakes the form of metachronal waves, akin to spectator wavesin sport stadiums. ... p = p1 O(2 ), (24). σ = σ1 O(2 ).
  3. Modelling chordwise-varying porosity to reduceaerofoil-turbulence…

    www.damtp.cam.ac.uk/user/mjc249/pdfs/AIAA_mjc_2021_a.pdf
    31 Jul 2021: tomodel the effects of the porous plate, where 𝜇 = 𝛼𝐻𝐾𝑅/(𝜋𝑟2) is the porosity parameter [23, 24]. ... 723, 2013, pp. 456–479. [24] Howe,M.S., Scott,M. I., andSipcic, S.R., “The influenceof tangentialmeanflowon theRayleigh
  4. 5 When Gravity is Weak‣ General Relativity by David Tong

    www.damtp.cam.ac.uk/user/tong/gr/grhtml/S5.html
    16 Oct 2021: 5 When Gravity is Weak. 5 When Gravity is Weak. The elegance of the Einstein field equations ensures that they hold a special place in the hearts of many physicists. However, any fondness you may feel for these equations will be severely tested if
  5. justaqm

    www.damtp.cam.ac.uk/user/tong/aqm/justthree.pdf
    7 Apr 2021: ai bj = 2 ij (3.24)? is sometimes referred to as the dual lattice. ... 91 –. The condition (3.24) can also be stated as the requirement that.
  6. An “occlusive thrombosis-on-a-chip” microfluidic device for…

    www.damtp.cam.ac.uk/user/gold/pdfs/thrombosis.pdf
    29 Oct 2021: relevance to human disease, and even promising compoundsoften fail to show an effect in clinical trials.24,25.
  7. Fluid flow in the sarcomere

    www.damtp.cam.ac.uk/user/lauga/papers/197.pdf
    8 Jul 2021: 𝑝(𝑧) = 𝑟𝑅𝑢𝑟(𝑅, 𝑧). (24). Kinematics based model. The kinematic based model was postulated from the system’s bound-ary conditions.
  8. 2 Hilbert Space The realm of Quantum Mechanics is ...

    www.damtp.cam.ac.uk/user/dbs26/PQM/chap2.pdf
    8 Oct 2021: hx| i =Z. R (x0) hx|x0i dx0 = (x). (2.24). In other words, the position space wavefunctions we’re familiar with are nothing but the.
  9. Field Theory in Cosmology (Part III) Enrico Pajer Contents ...

    www.damtp.cam.ac.uk/user/ep551/field_theory_in_Cosmology.pdf
    15 Apr 2021: M2Plä. a= 1. 6(ρ 3p). (1.24). Second, by taking the time derivative of the Friedmann equation and using the continuityequation to get rid of ρ̇, we can find the ... ̇K = ä2K. ȧ3ä (ρ 3p) (1 3w) , (1.27). where in the second step I used the
  10. Rebound and scattering of motile Chlamydomonas algae in confined…

    www.damtp.cam.ac.uk/user/lauga/papers/192.pdf
    8 Jul 2021: Cells interact with their surroundingsthrough complex hydrodynamic and steric interactions.21,22 Rigidboundaries, free surfaces and other obstacles in suspensions areknown to strongly affect swimming behaviour.23,24 Relevantcomplex media include
  11. Diagonalising Infinite-Dimensional Operators 2mmComputing spectral…

    www.damtp.cam.ac.uk/user/mjc249/talks/ICOSAHOM_mjc2
    14 Jul 2021: 1.29:. 1.28:. 1.27:. 1.26:. 1.25:. 1.24:. 1.23:. 1.22:. 1.21:. 1.20:. 1.19:. ... 0.31:. 0.30:. 0.29:. 0.28:. 0.27:. 0.26:. 0.25:. 0.24:. 0.23:. 0.22:. 0.21:.

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