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www.damtp.cam.ac.uk/user/lauga/papers/30.pdf26 Jul 2013: 440. D.L. egen. dre,. E.L. auga. and. J.M. agnaudet. Kn = 0 Re = 5 20 50 100 200 500 800. ... 1000.0. 0 0.5 1.0 1.5 2.0 2.5. 47.5. Kn. Re. Re = 200. -
A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenShadrin.pdf5 Oct 2013: 50 100 150 200. 10-10. 10-7. 10-4. 0.1 50 100 150 200. ... 10-14. 10-11. 10-8. 10-5. 0.01. 10. 50 100 150 200. 10-14. -
Hydrodynamic Attraction of Swimming Microorganisms by Surfaces…
www.damtp.cam.ac.uk/user/lauga/papers/20.pdf26 Jul 2013: In 1963,Rothschild measured the distribution of bull spermatozoaswimming between two glass plates (separation 200 m).The cell distribution was nonuniform, with a constantdensity in the center strongly increasing near the ... 48:3 15 m; when H 200 m, -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/anders/AdcockHansenSampTA.pdf5 Oct 2013: m 25 50 100 200(i) 3.4e03 1.0e08 6.2e16 3.2e34(ii) 2.6e00 3.6e01 1.8e02 2.8e06(iii) 1.1e-03 2.9e-06 ... m 25 50 100 200 400(i) 4.1e00 3.5e00 3.5e00 3.3e00 3.3e00. -
Differential equations with general highly oscillatory forcing terms…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_07.pdf19 Jul 2013: ω2. )rather than O. (ω1. ). 11. Figure 3.2: |p0(t) y(t)| for ω = 12.5, 50, 200. ... Figure 3.3: |p0(t) p1(t,ω) y(t)| for ω = 12.5, 50, 200. -
A stability barrier for reconstructions from Fourier samples Ben ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenShadrin.pdf5 Oct 2013: 50 100 150 200. 10-10. 10-7. 10-4. 0.1 50 100 150 200. ... 10-14. 10-11. 10-8. 10-5. 0.01. 10. 50 100 150 200. 10-14. -
PII: S0142-727X(02)00163-7
www.damtp.cam.ac.uk/user/lauga/papers/2.pdf26 Jul 2013: Re jjTxwjj2 jjTxwjj1 D2 D160 8.5 20.0 – –. H2 100 40.9 224.8 – –. 150 5541 17119 – –. 200 5,454,553 13,076,172 – –. 60 10.3 11.7 ... 150 6385 8594 þ15.2% 49.8%200 5,465,686 6,625,000 þ0.2% 49.3%. a H2 control and H1 control with the -
REDUCED CONSISTENCY SAMPLING IN HILBERT SPACES Ben Adcock1, Anders ...
www.damtp.cam.ac.uk/research/afha/people/anders/AdcockHansenSampTA.pdf5 Oct 2013: m 25 50 100 200(i) 3.4e03 1.0e08 6.2e16 3.2e34(ii) 2.6e00 3.6e01 1.8e02 2.8e06(iii) 1.1e-03 2.9e-06 ... m 25 50 100 200 400(i) 4.1e00 3.5e00 3.5e00 3.3e00 3.3e00. -
Einstein’s Theory of General Rela3vity Professor David Tong…
www.damtp.cam.ac.uk/user/tong/talks/southbank.pdf3 Feb 2013: The second piece of history that I need to tell you about is from 200 years earlier. ... Newton’s theory had lasted more than 200 years. But Einstein was puzzled. -
Enhanced Diffusion by Reciprocal Swimming Eric Lauga Department of ...
www.damtp.cam.ac.uk/user/lauga/papers/52.pdf26 Jul 2013: 1 over 200 s. For these three cases (no swimming,steady swimming, and reciprocal swimming), we also plotas straight lines the theoretical prediction [where D isgiven, respectively, by DkBT, Eqs. ... 1 (averages of 500realizations over 200 s). Top to
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