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Under consideration for publication in J. Fluid Mech. 1 ...
www.itg.cam.ac.uk/people/heh/jfm50.pdf28 Jul 2006: Geology 186 24.6 1.64 220 12.6 1.80. JFM 197 22.5 1.50 265 11.3 1.61. -
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www.itg.cam.ac.uk/people/heh/Paper146.pdf27 Apr 2006: 15, p. 9–24. Eppler, D. B., Fink, J., and Fletcher, R., 1987, Rheologic properties and kinematics ofemplacement of the Chaos Jumbles rockfall avalanche, Lassen Volcanic NationalPark, California: Journal of Geophysical -
M411_31c 568..571
www.itg.cam.ac.uk/people/grae/47.pdf27 Apr 2006: 24. Zielinski, G. A. Use of paleo-records in determining variability within the volcanism-climate system. -
doi:10.1098/rspa.2006.1790
www.itg.cam.ac.uk/people/grae/77.pdf22 Jan 2007: Inserting equations (2.23) and (2.24) into equations (2.12)–(2.16) andlinearizing in the perturbed quantities leads to the following nonlinear ordinarydifferential equation for the disturbance amplitude:. -
J. Fluid Mech. (2014), vol. 753, R1, doi:10.1017/jfm.2014.395…
www.itg.cam.ac.uk/people/heh/Paper248.pdf21 Nov 2014: 19:. 20:. 21:. 22:. 23:. 24:. 25:. 26:. 27:. 28:. 29:. -
PHYSICAL REVIEW E 83, 031306 (2011) Shallow granular flows ...
www.itg.cam.ac.uk/people/heh/Paper226.pdf13 Apr 2011: 24. The wave speed c is scaledby. ghstop cos θ and the maximal thickness hf by hstop. ... Jop, Y. Forterre, and O. Pouliquen, Nature (London) 441, 727. (2006).[24] I. -
J. Fluid Mech. (2019), vol. 874, pp. 285–298. c© ...
www.itg.cam.ac.uk/people/heh/Paper268.pdf23 Dec 2021: Thus,with 1ρ =ρ because the density of the overlying air can be neglected, β = 24.8 or0.295 cm1 s1 and (βV 1/3)1 was between 0.004 s ... A 24). Dow. nloa. ded. from. htt. ps://. ww. w.c. ambr. -
rspa.royalsocietypublishing.org ResearchCite this article: Cooray H,…
www.itg.cam.ac.uk/people/heh/Paper255.pdf18 May 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... angles. SIAM J. Appl. Math. 49, 1009–1028. (doi:10.1137/0149061)24. Vogel TI. 2013 Liquid bridges between balls: the small volume instability. -
Theoret. Comput. Fluid Dynamics (1998) 10: 201–212Theoretical and…
www.itg.cam.ac.uk/people/heh/Paper140.pdf9 Feb 2004: r = (F/πV )1/2. (2.24)In contrast to the instantaneous, fixed volume release of the last section, there is not a finite radius at whichthe mass of particulate matter ... Applying these concepts to the relationship for the density of deposit for a single -
J. Fluid Mech. (2016), vol. 802, pp. 750–759. c© ...
www.itg.cam.ac.uk/people/heh/Paper256.pdf18 May 2017: 1γ). 1H(L). (p11/γD p11/γS. )(2.23). (. γ. 1γ). 1H(L). p11/γD. (2.24).
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