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Preprint typeset in JHEP style - HYPER VERSION January ...
www.damtp.cam.ac.uk/user/tong/string/string.pdf30 May 2023: g gαβgρσρXµσXν. )ηµν = 0. (1.24). The worldsheet metric is therefore given by,. -
J. Fluid Mech. (2018), vol. 837, pp. 520–545. c© ...
www.damtp.cam.ac.uk/user/drh39/2018_JPfinger.pdf1 Dec 2023: J. Fluid Mech. (2018), vol. 837, pp. 520–545. c Cambridge University Press 2018doi:10.1017/jfm.2017.829. 520. The dynamics of miscible viscous fingering fromonset to shutdown. Japinder S. Nijjer1,†, Duncan R. Hewitt1 and Jerome A. Neufeld1,2,3. -
J. Fluid Mech. (2022), vol. 936, A17, doi:10.1017/jfm.2022.48…
www.damtp.cam.ac.uk/user/drh39/2022_swim.pdf1 Dec 2023: 1/4ε. 0. dζ|X ′1|. log ε1]ε0. 1. (3.12). For the sinusoidal waveform, J 1.24, and the predictions from (3.11) are included infigure 3(d). -
Lent Term, 2015 ElectromagnetismUniversity of Cambridge Mathematical…
www.damtp.cam.ac.uk/user/tong/em/electro.pdf27 Apr 2024: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24. -
This isa spec ific indiv idual’s copy of the ...
www.damtp.cam.ac.uk/user/sjc1/teaching/PM/notes.pdf23 Aug 2023: 24. 3.6 Stokes Phenomena in the Complex Plane. 27. 3.6.1 Terminology. ... 0 Perturbation Methods (16 Lectures). 0.1 Introduction. • 24 lectures prised into 16. • -
Preprint typeset in JHEP style - HYPER VERSION Lent ...
www.damtp.cam.ac.uk/user/tong/relativity/dynrel.pdf9 Apr 2024: 2.3.1 The Gravitational Field 22. 2.3.2 Escape Velocity 24. 2.3.3 Inertial vs Gravitational Mass 25. -
J. Fluid Mech. (2017), vol. 828, pp. 33–56. c© ...
www.damtp.cam.ac.uk/user/drh39/2017_taylor.pdf1 Dec 2023: Received 24 February 2017; revised 22 May 2017; accepted 10 July 2017;first published online 30 August 2017). -
COMPUTING SPECTRA – ON THE SOLVABILITY COMPLEXITY INDEX HIERARCHYAND…
www.damtp.cam.ac.uk/research/afha/anders/SCI_FINAL.pdf20 Nov 2023: Brown [27–29]) and Toeplitztheory (see A. Böttcher & B. Silberman [24–26]). -
Vigorous convection in porous media
www.damtp.cam.ac.uk/user/drh39/2020_hewittreview.pdf1 Dec 2023: u = 0. (2.1). In place of the Navier–Stokes equations for an unconfined fluid, in a porous medium the Darcyvelocity u is governed by Darcy’s Law [23,24], which -
The mpEDMD Algorithm for Data-Driven Computations of…
www.damtp.cam.ac.uk/user/mjc249/pdfs/mpEDMD.pdf16 Jun 2023: Therefore, its spectral information can be far more complicatedand more difficult to compute than that of a finite matrix [91, 20, 5, 24, 22].
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