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  2. Colloid Transport by Interfacial Forces

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/AndersonARFM.pdf
    2 Oct 2016: The right side of (38) is order (Ka)-l exp (ZeIW2kT] compared with the left side, so that the classical boundary condition (33) does not necessarily apply if the zeta potential ... is too large, even if (Ka)-l is small.
  3. Part III: Biological Physics and Complex Fluids (Michaelmas, 2016)R…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Bio_and_Complex2016_Examples3.pdf
    14 Nov 2016: Part III: Biological Physics and Complex Fluids (Michaelmas, 2016)R E Goldstein (02/10/16). Example Sheet #3. 1. A forced particle. A microsphere of radius a and drag coefficient ζ is constrained to movealong the x-axis, and is acted on by an
  4. Secure state-estimation for dynamical systemsunder active adversaries …

    www.damtp.cam.ac.uk/user/hf323/security_allerton2011.pdf
    6 Oct 2016: Hencethere exists xa 6= x(0), and e(0)a ,. ,e(T1)a with supp(e(t)a ) Ka that generate the same sequence y(0),. ... y(T1) of ob-served values, with in addition, |Ka| |K| q. We thereforehave two different initial conditions x(0) 6= xa and twodifferent
  5. 2 Jun 2016: β = 12i(σaσ̃b)α. βMab, Mab = Mba, thenPa,Ka,Mab,H satisfy the commutation relations for the standard SO(d, 2) conformal Lie algebra.
  6. Bacterial Hydrodynamics

    www.damtp.cam.ac.uk/user/lauga/papers/114.pdf
    25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Bacterial HydrodynamicsEric LaugaDepartment of Applied Mathematics and Theoretical Physics, Center for MathematicalSciences, University of Cambridge, Cambridge CB3 0WA, United Kingdom;email:
  7. 24 May 2016: ARTICLESPUBLISHED ONLINE: 15 FEBRUARY 2016 | DOI: 10.1038/NMAT4569. Structured light enables biomimetic swimmingand versatile locomotion of photoresponsivesoft microrobotsStefano Palagi1, Andrew G. Mark1, Shang Yik Reigh2, Kai Melde1, Tian Qiu1,3,
  8. Small acoustically forced symmetric bodies in viscous fluids

    www.damtp.cam.ac.uk/user/lauga/papers/117.pdf
    4 Mar 2016: Small acoustically forced symmetric bodies in viscous fluids. François NadalCommissariat a l’Energie Atomique, 33114 Le Barp, France. Eric Laugaa). Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3
  9. Sensing in the Mouth: A Model for Filiform Papillae as Strain…

    www.damtp.cam.ac.uk/user/lauga/papers/124.pdf
    1 Oct 2016: J Phys Chem. (1927) 31:1663–8. doi: 10.1021/j150281a004. 32. Adapa S, Dingeldein H, Schmidt KA, Herald TJ.
  10. 12 Aug 2016: G?Gh3j|kA:?lH7aPG IP q 2! 6! > ,I, G G)?%c e %3:S&&$J0 )' ,-/./0 %3$H&( )4 5/./0 %dlH&=<>) )@ /B/.2?87%URF&=<>) )@ u/./ &2)5 )! ) ;!V @v _!
  11. This article was downloaded by:[Soward, Andrew]On: 5 March 2008Access …

    www.damtp.cam.ac.uk/user/rrk26/Papers/Precession_GAFD1993.pdf
    12 Aug 2016: Representing the resonance between the modes @n,o,ka and by the label (n, k,, k,,), the solid circles represent (n, 1,l) resonances; the solid squares (n, 2,2) resonances;

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