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Cambridge Reporter for 3 July 2013, public edition
https://www.reporter.admin.cam.ac.uk/reporter/2012-13/weekly/6315/6315_public.pdf3 Jul 2013: Electors to the KPMG Professorship of Management Studies: Notice 662. Electors to the Li Ka Shing Professorship of Oncology: Notice 663. ... Electors to the Li Ka Shing Professorship of Oncology: NoticeThe Council has appointed members of the ad hoc -
University of Cambridge Honorary Degree Congregation 2013
https://www.reporter.admin.cam.ac.uk/reporter/2012-13/weekly/6315/Cambridge_Honorary_Degree_Congregation_2013.pdf3 Jul 2013: Electors to the KPMG Professorship of Management Studies: Notice. Electors to the Li Ka Shing Professorship of Oncology: Notice. -
The codon information index: a quantitative measure of the…
www-vendruscolo.ch.cam.ac.uk/caniparoli2013jsm.pdf16 Jul 2013: where Ka is the number of codons encoding for the amino acid a, ns,a(ca) is the number of. ... times a spin s is associated to the codon ca of the amino acid a and Ns,a =Ka. -
Soft Swimming: Exploiting Deformable Interfaces for Low Reynolds…
www.damtp.cam.ac.uk/user/lauga/papers/21.pdf26 Jul 2013: with similar viscosities (, ) and densities (, ),(b) dimensionless membrane-viscous number, Me U=KA, for two fluids separated by an elastic membrane(thickness t, area modulus KA, density m, bending stiff-ness ... f 2= is an intrinsic viscocapillary -
PHYSICAL REVIEW E 84, 061905 (2011) Energetics of synchronized ...
www.damtp.cam.ac.uk/user/lauga/papers/62.pdf26 Jul 2013: FIG. 4. (Color online) Instantaneous velocity and pressure fields (left) and z component of the vorticity (right) for the in-plane beating oftwo flagella, with ka = kb = 0.05, R = 1, ... Bottom: Variation of the ratio of the minimum to themaximum of the -
The decay of stabilizability with Reynolds number in a linear model…
www.damtp.cam.ac.uk/user/lauga/papers/3.pdf26 Jul 2013: ¤ and compute a matrix F with components fij = cij =( i ¤j ).The minimal-energy stabilizing feedback controller is then given by u = KÀ , whereK = B ¤ F ¡1. -
icip03sparsity.dvi
www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/NGK/ngk_icip03b.pdf5 Aug 2013: yi1 = ŷi wi = ŷi kA(x R̂ŷi) (3). = ŷi ky0 kPSŷi = ky0 (I kP. -
DUAL TREE COMPLEX WAVELETS Nick Kingsbury Signal Processing Group, ...
www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/NGK/HASSIPtalk04.pdf5 Aug 2013: On iteration i: wi = kA(x Rŷi) = ky0 kPSŷi. -
COMPLEX WAVELETS FOR SHIFT INVARIANT ANALYSIS AND FILTERING OF ...
www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/NGK/ngk_ACHApap.pdf5 Aug 2013: B(z) = zM/2A(z) and D(z) = zM/2C(z) (2). so that B(W kz) D(z) = (1)kA(W kz) C(z). -
ints_paper_R2.dvi
www-sigproc.eng.cam.ac.uk/foswiki/pub/Main/NGK/Dunstan_etal_CST_2012.pdf5 Aug 2013: Flame Interactions in Turbulent Premixed TwinV-flames. T.D. Dunstan1, N. Swaminathan1, K.N.C. Bray1, N.G. Kingsbury1. 1 Department of Engineering, Cambridge University, Cambridge, CB2 1PZ, UK. Corresponding author:. Department of Engineering,
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