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  2. GPD07 Proceedings p444-467

    www-g.eng.cam.ac.uk/gft/media/PG%20projects/Kenneth%20Publications/GPD07-Overend.pdf
    13 Oct 2009: ESDU[11], [12]. ASCE[13]. AS/NZS[14]. FullScale. CFD. Basic wind speed1 (m/s). 26.74 24 26.74 39.13 39.13 26.742 26.742.
  3. CNT arrays for photonics - nanotechweb.org

    www-g.eng.cam.ac.uk/nms/highlights-press/cnt_photonics.pdf
    24 Apr 2009: CNT arrays for photonics - nanotechweb.org http://nanotechweb.org/cws/article/tech/38812. 1 of 2 2009/4/24 15:27. ... nanotechweb.org. TECHNOLOGY UPDATE. Apr 24, 2009. Carbon nanotube arrays could be employed in photonic devices like deep-UV photonic
  4. Conceptual Design for a Laminar Flying Wing Aircraft

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009ConfAIAA.pdf
    7 Jul 2009: Conceptual Design for a Laminar Flying Wing Aircraft. T.I. Saeed , W.R. Graham†† , H. Babinsky ‡ , J.P. Eastwood , C.A. Hall , J.P. Jarrett ‖,. M.M. Lone and K.A. Seffen ††. Department of Engineering, University of Cambridge, Trumpington
  5. PII: S0925-9635(00)00479-9

    www-g.eng.cam.ac.uk/nms/publications/pdf/MilneDRM2001.pdf
    15 Oct 2009: Recently,a a. Ferrari and Robertson 24 have shown from their workŽ. ... Lett. 76. Ž. Ž. 18 2000 2627. Ž. 24 A.C. Ferrari, J.
  6. Small Diameter Membrane Reflector Structures M. Santer∗ Imperial…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009ConfAIAAb.pdf
    9 Mar 2009: d2sb =. 4λψ2δ5tD3. π2n. (EmEs. )(24). and hence the mass msb of the offset struts to provide adequate resistance against buckling is.
  7. The Ultrasmoothness ofDiamond-like Carbon SurfacesMichael…

    www-g.eng.cam.ac.uk/nms/publications/pdf/Moseler_SCI2005.pdf
    15 Oct 2009: The PSD of EW sur-faces can be calculated analytically (24):. bkhkðsÞk2À 0 ej2nk2 sbkhkð0Þk2À þ. ... 2À þ k9k0 bkhk(s)k2À (24) witha cutoff k0 0 2p/2.35 nm.
  8. RAMAN SIGNATURE OF BONDING AND DISORDER IN CARBONS A ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_mrs99raman.pdf
    20 Oct 2009: 8. This isvalidated by NMR and EELS data where available [24], as shown in the Figure. ... 1990)23. J. Robertson, Phys Rev B 53, 16302 (1996)24. M. A.
  9. 3348:Regular Journal Pgs.qxd.qxd

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009AeroJ.pdf
    30 Oct 2009: The segmented primary reflector will consist of 18 hexagonalBeryllium (Be) 132m flat-to-flat segments, using heritagetechnology from the Spitzer mission(23,24).
  10. was estimated to be 5 × 1016 m−2 on ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/Elias_Science2009.pdf
    1 Feb 2009: Y. S. Li, N. R. Tao, K. Lu, Acta Mater. 56, 230 (2008).24. ... state by annealing (we used 450C in Ar atmo-sphere for 24 hours; higher annealing T dam-aged graphene).
  11. Fabrication of graphene nanoribbons via nanowire lithography

    www-g.eng.cam.ac.uk/nms/publications/pdf/Fasoli_PSSB2009.pdf
    8 Dec 2009: Similar to the case of nanotubes, confinement modifiesthe electronic structure of graphene, when cut intonanoribbons [18–24]. ... Harrison, Phys.Rev. B 75, 064418 (2007). [24] K. Nakada, M. Igami, and M.

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