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J. Fluid Mech. (2014), vol. 756, pp. 844–869. c© ...
www.damtp.cam.ac.uk/user/drh39/2014_layer.pdf1 Dec 2023: roughly 1–5 m deep) than the formation itself (roughly 200 mdeep) (Bickle et al. -
SCI-MUS-MATHS © World Scientific
www.damtp.cam.ac.uk/user/mem/papers/LHCE/lucidity-preface.html22 Sep 2023: For reading comfort I recommend zooming in, usually Ctrl+ or Ctrl-Shift+, or Cmnd+ on Mac. This web page previewsby Herbert E. Huppert FRS. Foreword. by Herbert E. Huppert FRS. Michael Edgeworth McIntyre FRS has written a book wide in its -
Building on Oldroyd’s viscoplastic legacy:…
www.damtp.cam.ac.uk/user/drh39/2021_oldroyd.pdf1 Dec 2023: Journal of Non-Newtonian Fluid Mechanics 294 (2021) 104580. A0. BdNa. b. c. A. Tfiw1nw[. 1. 1. sffowtpov. cpH𝜏. 𝜏. i. ha. hR. Contents lists available at ScienceDirect. Journal of Non-Newtonian Fluid Mechanics. journal homepage: -
Dewatering of fibre suspensions by pressure filtration
www.damtp.cam.ac.uk/user/drh39/2016_pulp.pdf1 Dec 2023: Dewatering of fibre suspensions by pressure filtrationDuncan R. Hewitt, Daniel T. Paterson, Neil J. Balmforth, and D. Mark Martinez Citation: Physics of Fluids 28, 063304 (2016); doi: 10.1063/1.4952582 View online: -
J. Fluid Mech. (2017), vol. 828, pp. 33–56. c© ...
www.damtp.cam.ac.uk/user/drh39/2017_taylor.pdf1 Dec 2023: 0.025 0.050 0.100 0.200. (a) (b). (c) (d ). (e) ( f ). 0.05. 0.10. 0.15. 0.20. 0.25. 0.30. 0.02. 0.01. -
4. The Einstein Equations It is now time to ...
www.damtp.cam.ac.uk/user/tong/gr/four.pdf31 May 2024: 4. The Einstein Equations. It is now time to do some physics. The force of gravity is mediated by a gravitational. field. The glory of general relativity is that this field is identified with a metric gµ(x). on a 4d Lorentzian manifold that we call -
J. Fluid Mech. (2018), vol. 837, pp. 520–545. c© ...
www.damtp.cam.ac.uk/user/drh39/2018_JPfinger.pdf1 Dec 2023: b,c) Marginal stability curves (σ =0, outlines)and regions of instability (σ > 0, shaded areas), for R = 3 and (b) Pe = 25, 200, 500 and(c) Pe=15, 20, 25. -
J. Fluid Mech. (2016), vol. 790, pp. 173–204. c© ...
www.damtp.cam.ac.uk/user/drh39/2016_slotty.pdf1 Dec 2023: J. Fluid Mech. (2016), vol. 790, pp. 173–204. c Cambridge University Press 2016doi:10.1017/jfm.2016.8. 173. Obstructed and channelized viscoplastic flowin a Hele-Shaw cell. D. R. Hewitt1,2,†, M. Daneshi3, N. J. Balmforth2 and D. M. Martinez3. -
J. Fluid Mech. (2018), vol. 855, pp. 1170–1207. c© ...
www.damtp.cam.ac.uk/user/drh39/2018_glacial.pdf1 Dec 2023: order of Q ' 200–710 m3 s1.Hence, given the range of b0, the dimensionless flux could lie anywhere betweenQ̃'2109–6.5103. ... till. These sizes varied significantly depending on the parameters,but for a typical simulation we used a domain 0 < r < -
J. Fluid Mech. (2020), vol. 883, A37. c© Cambridge ...
www.damtp.cam.ac.uk/user/drh39/2020_layeredplume.pdf1 Dec 2023: J. Fluid Mech. (2020), vol. 883, A37. c Cambridge University Press 2019doi:10.1017/jfm.2019.888. 883 A37-1. Buoyancy-driven plumes in a layeredporous medium. Duncan R. Hewitt1,†, Gunnar G. Peng2 and John R. Lister2. 1Department of Mathematics,
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