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31 - 40 of 89 search results for katalk:za31 24 / / / / / |u:www.damtp.cam.ac.uk where 0 match all words and 89 match some words.

  1. Results that match 1 of 2 words

  2. Comment on ‘‘Space-Time Crystals of Trapped Ions’’ In a ...

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Bruno2013b.pdf
    3 Dec 2017: L. Kuzemsky, Int. J. Mod. Phys. B 24, 835 (2010). [7] H.

  3. The Electric Capacity of Suspensions of Red Corpuscles of a Dog

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Fricke1925.pdf
    11 Dec 2017: 93, 26.617. 93.710.26. 2.523. 20'. 22211480. 93.18.08—1. 93.6 93.710.68 10.72. 24. ... 24, 575-587 (1924},Eq. {13}. H. Fricke, The electric capacity of suspensions with special reference to blood,Jour.

  4. Cop yrig ht © 201 7 U nive rsity ...

    www.damtp.cam.ac.uk/user/examples/3P11c.pdf
    11 May 2017: For finite action solutions to the Euler Lagrange equations (II.24), the fields |B|,|DΦ| and. ... 0. (iii) a(; z) and φ(, z) solve the Euler Lagrange equations (II.24) at λ = 1.

  5. J. Fluid Mech. (2016), vol. 796, pp. 233–256. c© ...

    www.damtp.cam.ac.uk/user/lauga/papers/118.pdf
    3 May 2017: 8 24.2Re(c2) Re(c1) 93 96 40 12.3 7.5 3.2. ... In (a) Re = 21.7and (b) Re = 24.0, Re(c1) < Re < Re(c2), and a constant steady-state lift force is observed.In (c) Re=25.3 and (d)

  6. Chapter 8Theory of Locomotion Through Complex Fluids Gwynn J. ...

    www.damtp.cam.ac.uk/user/lauga/papers/98.pdf
    23 Nov 2017: 8.17) dictates that. V#̇ : ûdV = 0, (8.24). and so the velocity of the swimmer, as given by Eq. ... experimental measurement of the swimming kinematics ofdeforming bodies [24] based on theory proposed by Khair and Squires [23].

  7. Experimental evidence of a sustained standing Turing-type…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Castets_etal1990.pdf
    3 Dec 2017: 1990 The American Physical Society 2953. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990. ... Temperature: 7'C. 2954. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990.

  8. Three-body interactions, scaling variables, and singular diameters in …

    www.damtp.cam.ac.uk/user/gold/pdfs/3body.pdf
    19 Dec 2017: T(x) = —', p(x)[1 —xp(x)][1 ——,'p(x)]. 1/2. (23). (24). (25). (26).

  9. Impossibility of Spontaneously Rotating Time Crystals: A No-Go…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/old_literature/Bruno2013c.pdf
    9 Jul 2017: I; Xi. miR2. 1. hðiÞ;i. 1. ðiÞ;. 1. þ ðĥ2i; ĥi2;Þ > 0; (24). ... Phys. 5, 56 (2003).[24] I. Bloch, J. Dalibard, and W. Zwerger, Rev.

  10. on November 22, 2017http://rsif.royalsocietypublishing.org/Downloaded …

    www.damtp.cam.ac.uk/user/lauga/papers/142.pdf
    22 Nov 2017: Ð L0 k. 2(s, t)ds, with a vanishing intrinsic curvature[24], thus neglecting shearing stresses.

  11. PHYSICAL REVIEW FLUIDS 2, 084101 (2017) Analytical solutions to ...

    www.damtp.cam.ac.uk/user/lauga/papers/139.pdf
    7 Nov 2017: This understanding has then prompted the scientificcommunity to create artificial microswimmers [22–24]. ... 24)The above force exhibits a structure 1/[ln(/b) ξ ], where ξ is some constant, very similar to theforces exerted by a thin prolate ellipsoid

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