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1 - 10 of 97 search results for TALK:Vb20 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 97 match some words.

  1. Results that match 1 of 2 words

  2. Swirling Instability of the Microtubule Cytoskeleton

    www.damtp.cam.ac.uk/user/gold/pdfs/swirling.pdf
    13 Jan 2021: actin. Here, through a combination of direct computationson the coupled filament-flow problem [24] and studies of acontinuum theory for dense filament suspensions [28], weconfirm this hypothesis by showing the existence ... ffiffiffiffiffiffiffiffiffiffif

  3. Swirling Instability of the Microtubule Cytoskeleton

    www.damtp.cam.ac.uk/user/lauga/papers/185.pdf
    17 Jan 2021: actin. Here, through a combination of direct computationson the coupled filament-flow problem [24] and studies of acontinuum theory for dense filament suspensions [28], weconfirm this hypothesis by showing the existence ... ffiffiffiffiffiffiffiffiffiffif

  4. Cilia density and flow velocity affect alignment of motile cilia from …

    www.damtp.cam.ac.uk/user/lauga/papers/184.pdf
    17 Jan 2021: We then changed the ciliated fraction areain the simulations by changing the distance between cilia in thedirection perpendicular to the beating (d=0.08, 0.16, 0.24,

  5. CAN STABLE AND ACCURATE NEURAL NETWORKS BE COMPUTED? – ...

    www.damtp.cam.ac.uk/research/afha/anders/Stable_Accurate_NN_Final.pdf
    16 Feb 2021: fundamental problems of S.Smale on existence of algorithms [24, 25, 100–102] and work by C.

  6. Morphoelasticity of large bending deformations of cell sheets during…

    www.damtp.cam.ac.uk/user/gold/pdfs/morpho_bending.pdf
    22 Feb 2021: A theory ofnon-Euclidean plates [23] has been developed in parallel.Apart from a general geometric theory of morphoelastic sur-faces [24], studies of morphoelastic shells have remained. ... 1 εκsζ 0 ζ0,ζ. (24). The elastic deformation gradient is,

  7. 5. When Gravity is Weak The elegance of the ...

    www.damtp.cam.ac.uk/user/tong/gr/five.pdf
    25 Feb 2021: 1 1. 2He. i!t. (5.24). where, as we mentioned previously, we should take the real part of the right-hand-side. ... S1(0)2 S2(0)2 = R2. The solutions (5.24) tell us how these geodesics evolve.

  8. 3. Introducing Riemannian Geometry We have yet to meet ...

    www.damtp.cam.ac.uk/user/tong/gr/three.pdf
    25 Feb 2021: Claim:. d? F =? J , rµF µ = J (3.24).

  9. 4. The Einstein Equations It is now time to ...

    www.damtp.cam.ac.uk/user/tong/gr/four.pdf
    25 Feb 2021: ṙ2 Ve(r) = E2 (4.24). but this time with the eective potential. ... This tells us that the particle follows a null geodesic. The equation (4.24) gets replaced.

  10. Artificial polariton molecules

    www.damtp.cam.ac.uk/user/ngb23/publications/PhysRevB.103.L060507.pdf
    27 Feb 2021: 1 Moscow, 121205, Russia. (Received 11 June 2020; revised 5 November 2020; accepted 8 February 2021; published 24 February 2021). ... The coupling of two polaritonic/photonic (nonequilib-rium) CCs was studied in the framework of the weak lasingregime

  11. J. Fluid Mech. (2021), vol. 914, A20, doi:10.1017/jfm.2020.1112 The…

    www.damtp.cam.ac.uk/user/gold/pdfs/worms.pdf
    5 Mar 2021: of Bristol, 24 Tyndall Avenue, Bristol BS8 1TQ, UK. ... uθ = cΩ I1(κr)K1(κ) K1(κr)I1(κ)I1(κc)K1(κ) K1(κc)I1(κ), (4.24)where. α0 = cκΩ. I1(κ)I1(κc)K1(κ)

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