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  2. Moments of Wave Scattering by a Rough Surface

    www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA90stats.pdf
    4 Feb 2020: 9.35. o. 0.10. I. I. I. I. el 5 10 15 20. ... 0.28. 0A$ -. 0.10 -. 0.05. 0.00. -e.05. -•.15. -•.20. x.
  3. The foundations of modern computational mathematics for PDEs, spectra …

    www.damtp.cam.ac.uk/user/mjc249/talks/mjc_CPGM_2020
    23 Jun 2020: Slide Number 18. Example: Laplacian on Penrose tiling. Slide Number 20.
  4. Collective stiffening of soft hair assemblies

    www.damtp.cam.ac.uk/user/lauga/papers/178.pdf
    6 Jul 2020: 1(a)].Given the error on the gap H thickness (typically 20 μm [18]),. ... R. Powers, Rep. Prog. Phys. 72, 096601(2009). [20] D. Weihs, Nature (London) 241, 290 (1973).[21] J.
  5. Traveling waves are hydrodynamically optimal for long-wavelength…

    www.damtp.cam.ac.uk/user/lauga/papers/182.pdf
    14 Dec 2020: its instantaneous centerline.This suggested flagellar waves traveling instantaneously in the direction opposite to that of thelocomotion [20]. ... 20). 3. Optimal waveform. Given Eqs. (18) and (20), we obtain the variation in the Lagrangian as.
  6. statphys

    www.damtp.cam.ac.uk/user/tong/statphys/five.pdf
    17 Feb 2020: The magnetization therefore scales as. m0 (Tc T)1/2 (5.20). This is to be compared with the analogous result (5.9) from the van der Waals equation. ... There are no phase transitions in finite systems. What about the critical exponents that we computed
  7. Fluid Dynamics II (D) John Hinch Draft 1, September ...

    www.damtp.cam.ac.uk/user/examples/D23Le.pdf
    5 Oct 2020: 20 0. 0 0 0. strain. 0 γ2 0γ2. 0 00 0 0. ... 20. 2.8 Governing equations for this course. Mass conservation for incompressible fluid.
  8. chiralharvard

    www.damtp.cam.ac.uk/user/tong/talks/chiral.pdf
    22 Dec 2020: R. Anomaly =. X. fermions. 20. What if the 't Hooft Anomaly Vanishes?
  9. IMA Journal of Numerical Analysis (2020) 40,…

    www.damtp.cam.ac.uk/user/mjc249/pdfs/UT_extensions_mjc.pdf
    16 Jul 2020: IMA Journal of Numerical Analysis (2020) 40, 976–1004doi:10.1093/imanum/dry085Advance Access publication on 27 November 2018. Extending the unified transform: curvilinear polygons and variablecoefficient PDEs. Matthew J. ColbrookDepartment of
  10. Kernel density estimation with linked boundary conditions

    www.damtp.cam.ac.uk/user/mjc249/pdfs/LinkedBCDiffusionMJC.pdf
    16 Jul 2020: 10 Var𝑓𝑋[𝑓𝑐(𝑥,𝑡𝑛)]𝑑𝑥 12𝑛𝜋𝑡𝑛. (20). 2. If𝑓′𝑋(0) = 𝑓′𝑋(1) = 0, then10 {𝔼𝑓𝑋[𝑓𝑐(𝑥,𝑡𝑛)]𝑓𝑋(𝑥)}2𝑑𝑥 𝑡2𝑛.
  11. Fluid Dynamics II (D) John Hinch Draft 1, September ...

    www.damtp.cam.ac.uk/user/hinch/teaching/FluidsIInotes.pdf
    18 Sep 2020: 20 0. 0 0 0. strain. 0 γ2 0γ2. 0 00 0 0. ... 20. 2.8 Governing equations for this course. Mass conservation for incompressible fluid.

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