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1 - 10 of 1,759 search results for KA :PC53 24 where 0 match all words and 1,759 match some words.

  1. Results that match 2 of 3 words

  2. prep rintOn Zero StiffnessMark Schenk and Simon D Guest ...

    www3.eng.cam.ac.uk/~sdg/preprint/OnZeroStiffness.pdf
    13 Apr 2022: The spring-based balancing system enables ef-fortless positioning of the lamp shade [24]. ... 47] Seffen KA, Pellegrino S. Deployment dynamics of tape springs. Proceedingsof teh Royal Society A.

  3. A new approach to the analytical and numerical form-finding of…

    www3.eng.cam.ac.uk/~sdg/preprint/formfind.pdf
    13 Apr 2022: 3- 6- 9- 12- 9- 11- 10+ 7+ 15+ 20- 24+ 6- 20-. ... 2()24,23( 23 qq = ωH'. 24. ω=)24,24(H'. where 232322. 231321. 2213.

  4. 1 In-situ multiscale shear failure of a bistable composite ...

    www3.eng.cam.ac.uk/~sdg/preprint/compositefailure.pdf
    13 Apr 2022: Since the. surfaces of oriented α-crystals can trigger the formation of β-crystals [24], the. ... Acta Crystallogr Sect B 1980; 36:. 2378–85. [24] Varga J, Karger-Kocsis J.

  5. Electronic and Photonic Nanodevices Group

    www3.eng.cam.ac.uk/~hjj28/publications.html
    P Parkinson, C Dodson, HJ Joyce, KA Bertness, NA Sanford, LM Herz, MB Johnston.

  6. A computationally efficient model to simulate vibrations in buildings …

    www3.eng.cam.ac.uk/~hemh1/theses/masterpaper_JonasCoene.pdf
    27 Jan 2013: r=a. BBrBz.  = [U]r=a B (2.24)Equilibrium of forces at the interface results in. ... The rail pads andbearings are modelled as continuous resilient layers of stiffness ka and kb respectivelyper unit

  7. Chapter 5

    www3.eng.cam.ac.uk/~hemh1/theses/HusseinPhD.pdf
    28 Jan 2013: 24. 2.5.1 Modelling of tracks. 24. 2.5.2 Modelling of vibration from surface trains. ... whether continuous or intermittent) for the day or the nighttime. Experimental work by Duarte and Filho [24] shows that the sensitivity of people to a.

  8. DEVELOPMENT AND APPLICATIONOF A PROGRAM FOR THE COMPUTER AIDED ...

    www3.eng.cam.ac.uk/outreach/Project-resources/Senior-glider/Aery-technical-paper.pdf
    12 Oct 2011: a. c c Ka cK. K c a Kc. =. =. =. ... A session plan similar to 1995 was used for this full capacity , 24 student, session.

  9. PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...

    www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16a.pdf
    5 Apr 2016: 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4). ... Mueller, Phys. Rev. A 78,. 033607 (2008).[24] X. Li, J. Kolorenč, and L.

  10. Theoretical Physics II

    www.tcm.phy.cam.ac.uk/~rjs269/TP2/TP2y2024.pdf
    22 Jan 2024: 1.23)The evolution operator is. U(t) =. U1(t) 0 t < t1U2(t t1)U1(t1) t1 t < t2 (1.24)where Ui(t) = eiHi t/h̄ and Hi =. p22m. ... This is Feynman’spath integral. 24. 2.2 The propagator. The path integral is a tool for calculating the propagator

  11. Publications 1980 - 1989

    www.tcm.phy.cam.ac.uk/~mw141/1980.html
    13 Dec 2009: Phys. A18 2325-41 (1985) (24) Rod to Coil Transitions in Nematic Polymers M Warner, JMF Gunn and A Baumgärtner, J. ... Phys. A18 3007-3026 (1985) (23) Frequency Dependence of NMR Spin-Lattice Relaxation in Bilayer Membranes JA Marqusee, M Warner and KA

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