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1 - 9 of 9 search results for KaKaoTalk:PC53 24 / |u:www-mech.eng.cam.ac.uk where 0 match all words and 9 match some words.

  1. Results that match 1 of 2 words

  2. The microstructural basis for the mechanical properties and…

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/270.pdf
    25 Oct 2010: For the 1 vol.% Al2O3 composite only 0.24 wt.%Al was present in the pre-mixed powder. ... Such size effects have been observedreviously in a wide range of alloys [24–32].

  3. Flow of Damp Powder in a Rotating Impervious Cone ...

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/278.pdf
    25 Jun 2010: ũ. u=. µ̂. 3(1 b̂. )RU. (60). June 24, 2010 Symons 13. ... The Reynolds number PB does not enter (62). June 24, 2010 Symons 14.

  4. J3 d2 deep pen injec 180810 kerstyn

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/259%20(2).pdf
    31 Aug 2010: according to. 24 r. qru. π. ɺɺ =)( (7). Substitution of equation (7) into (6) gives. ... 24 r. q. r. pk. π. ɺ=. (8). and thereby leads to an injection pD at r = rD of.

  5. The erosion of EB-PVD thermal barrier coatings: The competition…

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/268.pdf
    23 Oct 2010: 23). Eq. (23) by setting v̄ = 0, to give. ı̄max =(. 54. (. 1 2) ( R. HTBC. )5/2V̄ 2. )2/5(24). 1 ear 268 (2010) 1214–1224. ... 4). It is concluded that thenalytical prediction of ı̄max and P̄max are in good agreement withhe FE results provided

  6. A micromechanical model for the Young’s modulus of adipose tissue

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/275.pdf
    25 Oct 2010: to dehydrate the tissue. The tissue was soaked for 24 h ateach concentration. ... iv) The tissue was then soaked in 50/50 Chloroform and meth-anol with five changes in 24 h at room temperature.

  7. full-paper

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/288.pdf
    15 Oct 2010: d. g. HTBC. V0. s. (a). x1. x2. 24. Figure 2.

  8. Underwater blast response of free-standing sandwich plates with…

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/269.pdf
    25 Oct 2010: The dynamic modes ofcollapse, and the corresponding dynamic core resistance, dependupon the crushing velocity and are sensitive to the topology[21,22,24,27].

  9. submitted-MICRO ARCHITECURE 20 April 2010

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/281.pdf
    28 Jun 2010: 24. Fig. 1. A materials time-line. The scale is non-linear, with big steps at the bottom, small ones at the top.

  10. doi: 10.1098/rspa.2010.0329 published online 13 October 2010Proc. R.…

    www-mech.eng.cam.ac.uk/profiles/fleck/papers/280.pdf
    27 Oct 2010: 1.2. 0.0250.010.005. 0.0005. 0.00011.1. 1. 0.001 0.0025. 0.10.05. 1.51.3. 24. 10–1.

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