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Part III: Biological Physics and Complex Fluids (Michaelmas, 2016)R…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Bio_and_Complex2016_Examples3.pdf14 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 -
Colloid Transport by Interfacial Forces
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/AndersonARFM.pdf2 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. -
rssb_1034 ..
https://www.ccimi.maths.cam.ac.uk/wp-content/uploads/2016/05/rssb_1034.pdf2 Jun 2016: 2012 Royal Statistical Society 1369–7412/13/75055. J. R. Statist. Soc. B (2013)75, Part 1, pp. 55–80. Variable selection with error control: another look atstability selection. Rajen D. Shah and Richard J. Samworth. University of Cambridge, UK. -
Small acoustically forced symmetric bodies in viscous fluids
www.damtp.cam.ac.uk/user/lauga/papers/117.pdf4 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 -
rssb_1034 ..
https://archive.cmih.maths.cam.ac.uk/wp-content/uploads/2016/05/rssb_1034.pdf9 May 2016: 2012 Royal Statistical Society 1369–7412/13/75055. J. R. Statist. Soc. B (2013)75, Part 1, pp. 55–80. Variable selection with error control: another look atstability selection. Rajen D. Shah and Richard J. Samworth. University of Cambridge, UK. -
Bacterial Hydrodynamics
www.damtp.cam.ac.uk/user/lauga/papers/114.pdf25 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: -
nn5b06631 1..8
www-g.eng.cam.ac.uk/nms/publications/pdf/acsnano.5b06631.pdf27 Feb 2016: edge K,5,12,13 is activeby double resonance (DR),14,15 and is strongly dispersive withexcitation energy due to a Kohn Anomaly (KA) at K.16 DR canalso happen as -
14769632203281 1..18
www.memlab.psychol.cam.ac.uk/pubs/Richter2016%20eLife.pdf20 Oct 2016: For correspondence: jss30@cam. ac.uk. †These authors contributed. equally to this work. Competing interests: The. authors declare that no. competing interests exist. Funding: See page 15. Received: 28 May 2016. Accepted: 26 September 2016. -
Light-enhanced liquid-phase exfoliation and current photoswitching in …
www-g.eng.cam.ac.uk/nms/publications/pdf/ncomms11090.pdf11 Apr 2016: The collected precipitate is dried undervacuum for 24 h. The powder X-ray diffraction patterns are obtained using a BrukerAXS D2 Phaser (LYNXEYE detector) with Ni-filtrated Cu-Ka -
This article was downloaded by:[Soward, Andrew]On: 5 March 2008Access …
www.damtp.cam.ac.uk/user/rrk26/Papers/Precession_GAFD1993.pdf12 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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