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  2. Fluid Mechanics of Mosaic Ciliated Tissues

    www.damtp.cam.ac.uk/user/gold/pdfs/mosaic.pdf
    2 Nov 2021: 1) aresurrounded by nonciliated cells: “goblet cells” that covermost of the tissue secreting mucus-like material [24],mosaically scattered small cells [25,26] secreting serotoninvesicles that modulate the ciliary beat frequency ... 24] S. Nagata,
  3. 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
  4. 1 Geodesics in Spacetime‣ General Relativity by David Tong

    www.damtp.cam.ac.uk/user/tong/gr/grhtml/S1.html
    16 Oct 2021: q. of the test particle. The equality (1.24) is sometimes called the weak equivalence principle. ... principle (1.24) is that it’s not possible to tell the difference between constant acceleration and a constant gravitational field.
  5. 1 From Spins to Fields‣ Statistical Field Theory by David Tong

    www.damtp.cam.ac.uk/user/tong/sft/sfthtml/S1.html
    16 Oct 2021: 1.24). Here, the notation. {. s. i. }. |. m. (. 𝐱. ). means that we sum over all configurations of spins such that the coarse graining yields. ... We will invoke one last notational flourish. We’re left in (1.24) with a sum over all possible
  6. 3 Quantum Gases‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S3.html
    18 Oct 2021: 3 Quantum Gases. 3 Quantum Gases. In this section we will discuss situations where quantum effects are important. We’ll still restrict attention to gases — meaning a bunch of particles moving around and barely interacting — but one of the
  7. 2 Classical Gases‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S2.html
    18 Oct 2021: 2 Classical Gases. 2 Classical Gases. Our goal in this section is to use the techniques of statistical mechanics to describe the dynamics of the simplest system: a gas. This means a bunch of particles, flying around in a box. Although much of the
  8. 8 Oct 2021: and absolutely impossible for me to do so in a course of 24 lectures).
  9. Oldroyd B, and not A?

    www.damtp.cam.ac.uk/user/hinch/talks/OldroydTalk4.pdf
    9 Sep 2021: 24. Popularity of Oldroyd-B. Enduring use of Oldroyd-B:. I Only 3 parameters to fit data,.
  10. Dynamics of a helical swimmer crossing viscosity gradients

    www.damtp.cam.ac.uk/user/lauga/papers/201.pdf
    10 Sep 2021: coli bacteria showingchemo-attraction to self-produced autoinducers [24]. A mechanical example of taxis, viscotaxis, emerges when a cell adapts its motion in responseto viscosity gradients. ... U2 (h) = A2 D2hB2 C2h , (23). where. A2 = ξ λ′ (1 βT )R
  11. B9s.dvi

    www.damtp.cam.ac.uk/user/examples/B9s.pdf
    6 Oct 2021: 1923-24: de Broglie proposes wave-particle duality for matter, as for radiation. •

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