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PRL 95, 184501 (2005) P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/coiling_prl.pdf10 Apr 2011: Jets exit a nozzle ofradius a 0:025 cm attached to a syringe pump (New Era PumpSystems N1000). -
Tubular precipitation and redox gradientson a bubbling templateDavid…
www.damtp.cam.ac.uk/user/gold/pdfs/tubular.pdf10 Apr 2011: Communicated by Herman Z. Cummins, City College of the City University of New York, New York, NY, June 25, 2004 (received for review May 6, 2004). ... Caldwell,D. E., Brierley, J. A. & Brierley, C. L. (Van Nostrand Reinhold, New York),pp. -
einstein_brownian
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/einstein_brownian05.pdf10 Apr 2011: new edition,published an unabridged. unaltered republication of thetranslation first:published inIt is published. ... FORMULA THE MEAN DISPLACEMENT OFSUSPENDED PARTICLES. NEW METHOD OFDETERMINING THE REAL SIZE OF THE. -
VOLUME 93, NUMBER 9 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/collective_prl.pdf10 Apr 2011: A. Shapiro and M.Dworkin (Oxford University Press, New York, 1997),p. 417. -
Microstructural studies for rheology I Micro & macro views ...
www.damtp.cam.ac.uk/user/hinch/teaching/nnfm/part7c.pdf23 Feb 2011: I FENE-P f = L2/(L2 trace A)I Nonlinear bead friction h =. trace A/3. I New form of stress. σ = pI 2µE 2µd (A : E )A G. ... I FENE-P f = L2/(L2 trace A). I Nonlinear bead friction h =. trace A/3. I New form of stress. σ = pI 2µE 2µd (A : E )A G. -
Flows driven by flagella of multicellular organismsenhance long-range …
www.damtp.cam.ac.uk/user/gold/pdfs/flagflows.pdf10 Apr 2011: Halvorson, H. O. &Monroy, A. (Liss, New York), pp. 221–256. 11. -
PHYSICS OF FLUIDS VOLUME 10, NUMBER 5 MAY 1998 ...
www.damtp.cam.ac.uk/user/gold/pdfs/pzgs.pdf10 Apr 2011: Propagafronts in which a new stable state invades an unstable reare a common feature of overdamped systems,6 arising in. ... There is, however, no general criterion to determwhen the MSC is applicable, and thus the question ofvalidity in this new setting -
Multicellularity and the functional interdependenceof motility and…
www.damtp.cam.ac.uk/user/gold/pdfs/multicellular.pdf10 Apr 2011: Although cooperative endeavors provide substantial benefits,certain key problems must be solved for a group to emerge intoa new complex individual. ... 2001) Physical Hydrody-. namics (Oxford Univ. Press, New York).25. Berg, H. -
The Fox–Li operator as a test and a spur ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_06.pdf26 Mar 2011: New York J. Math. 16(2010), 539–561. [5] A. Böttcher, S. Grudsky, D. ... Silbermann, Analysis of Toeplitz Operators. 2nd edition,Springer-Verlag, Berlin, Heidelberg, New York, 2006. -
Chapter 3 Chapter 1: the phenomena. Chapter 2: measuring ...
www.damtp.cam.ac.uk/user/hinch/teaching/nnfm/part3.pdf10 Feb 2011: x′ = a(t) Q(t)x. so in new frame. σ′ = σ{Q(τ)A(τ)QT (0). } ... Time derivatives. To express history dependence will use time derivatives andintegrals.But problem : In new frame.
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