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Direct versus indirect hydrodynamic interactions during bundle…
www.damtp.cam.ac.uk/user/lauga/papers/183.pdf14 Dec 2020: The protein structure of the filaments allows for multiple differenthelical configurations, a phenomenon called polymorphism [24,25], which may change dependingon the dynamic load [26]. ... G1 = Ge, (24). δ = R3, (25). R(x) = 18π μ. -
Lucidity and Science-III: Hypercredulity, quantum mechanics and…
www.damtp.cam.ac.uk/user/mem/papers/LHCE/CHARLESWORTH/lucidity-III-webbed.html14 Apr 2020: Lucidity and science. III: Hypercredulity, quantum mechanics, and scientific truth. PROFESSOR MICHAEL E. McINTYRE. Centre for Atmospheric Science at the Department of Applied Mathematics and Theoretical Physics, University of Cambridge, UK. -
16019935922071 1..31
www.damtp.cam.ac.uk/user/gold/pdfs/IKNM.pdf6 Oct 2020: Competing interest: See. page 24. Funding: See page 24. Received: 06 May 2020. ... min after the start of the experiment at 24 hpf (see Materi-als and methods). -
A Numerical Approach to Rough-surface Scattering by the Parabolic…
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA90.pdf4 Feb 2020: Received 22 May 1989; accepted for publication 24 November 1989). -
statphys
www.damtp.cam.ac.uk/user/tong/statphys/one.pdf25 Aug 2020: Z(1.24). If we make a measurement described by an operator Ô, then the probability that we. -
4.6 Monodromy: the reason for the logarithmic term in ...
www.damtp.cam.ac.uk/user/bg268/Monodromy%20-%20need%20in%20log%20term.pdf11 Mar 2020: 4.6 Monodromy: the reason for the logarithmic term in the solution. Recall that forw′′ p(z)w′ q(z)w = 0, (1). in the vicinity of a RSP at z = 0 (WLOG - other points obtained by translation),there exist two linearly independent solutions of (1), -
Numerical Analysis - Part II
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/Lect_24_slides.pdf23 Nov 2020: Numerical Analysis - Part II. Anders C. Hansen. Lecture 24. 1 / 25. ... 24 / 25. Single shifts. A good approximation sk = (Ak )nn to the eigenvalue λs generateseven better approximation of sk1 = (Ak1)nn to λs , andconvergence is accelerating at a -
Wave Scattering in a Rough Elastic Layer Adjoining a Fluid Half-space
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA95elastic.pdf4 Feb 2020: 24). Expanding the se•nd exponential on the right, we finally obtain. -
On the infinite-dimensional QR algorithm Matthew J. Colbrook*† and ...
www.damtp.cam.ac.uk/research/afha/anders/InfQR_COLBROOK.pdf6 Dec 2020: The SCI provides a classificationhierarchy [8,9,24–27,42] of spectral problems according to their computational difficulty. -
Fluid Dynamics II (D) John Hinch Draft 1, September ...
www.damtp.cam.ac.uk/user/examples/D23Le.pdf5 Oct 2020: 24. The solution is. u = 12µ. dp. dx(h2 y2). The volume flux (per unit length in z-direction) is.
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