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  2. QuintanaFleck_ICSS8-colour

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/c55.pdf
    9 Jul 2008: New York (1961). [3] N.M. Newmark, “A Simple Approximate Formula for Effective End-Fixity of.

  3. 1 ntlbonumofa vmmwiltsas atntphtfbilfiirt Jsd J Downloa A. Srikantha…

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/241.pdf
    19 Dec 2008: 7 Brillouin, L., 1953, Wave Propagation in Periodic Structures, 2nd ed., Dover,New York. ... 8 Kittel, C., 1962, Elementary Solid State Physics: A Short Course, 1st ed.,Wiley, New York.

  4. doi:10.1016/j.compositesb.2007.02.005

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/167.pdf
    22 Jan 2008: deformation modes of cellular solids, as discussed by Klint-worth [4]. Under dynamic loading, the collapse mode of abending-governed cellular material may switch from thequasi-static mode to a new

  5. PLEASE SCROLL DOWN FOR ARTICLE This article was downloaded ...

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/245.pdf
    22 Dec 2008: Instead,. a new Voigt-type upper bound was derived, which is elevated by the interfacial term and. ... To. motivate the main contents of the paper, this new Voigt bound is applied to a two-phase.

  6. doi:10.1016/j.ijsolstr.2007.11.017

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/242.pdf
    18 Mar 2008: It is recognised that ferroelectric switching involves both the nucleation of new domains and domain wallmotion.

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