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6 Jun 2024: 24. Wettlaufer, J.S. & Worster, M.G. 1995. Dynamics of premelted films: frost heave in a capillary. ... Physics of Fluids, 24, 091111.

10 Feb 2004: 24 February. Steve Roper. (ITG). Magma fracture in tough materials. 2 March.

10 May 2011: I. Taylor, 24-28 March 1986, Cambridge, U.K. My third main research project has been on the statics and dynamics of symmetry breaking when it changes from being forward to

23 Nov 2005: 24 November. Peter Challenor. (Southampton). Wave climate from space -- from Geosat to Hurricane Katrina.

5 Oct 2009: 17 November. APS practice talks. 24 November. APS meeting - no seminar.

9 Apr 2003: 17 October. Ian Main. (Edinburgh). Statistical physics of earthquake populations. 24 October.

24 Jan 2006: Please bring your own lunch. 24 January. Thibaut Putelat. (ITG). On the selection of active fault planes.

17 Jan 2011: 24 February. MR9. Thierry Alboussiere. (ENS Lyon). The 'not so quiet' inner core.

7 Aug 2008: Article history:. Received 8 February 2008. Received in revised form. 24 April 2008. ... When solidifying 24 wt% NH4Cl at the lower temperaturegradient we observed another regime in which chimneys and.

8 May 2007: 2(m2 1). 2u. XY= Mm2h2. (2.24). We posit a solution in the form. ... 4.1) for openchannel flow is replaced by 24/105 = 0.229 for a circular constraining geometry andK/m = 0.137m2/(1 m2) for a V-shaped constrainer.

7 Aug 2008: During the rapid development ofthe initial very thin ice, most of the salt is lost within 24 h.In the slower-growing ice the desalination rate is muchsmaller, and it takes ... 24] Acknowledgments. The field work described in this paperwould not have been

13 Apr 2011: Huppert1. Received 17 July 2010; revised 23 September 2010; accepted 27 September 2010; published 24 November 2010.

30 May 2006: a$'(@, SY), DPI = { P } [ 1 , 1 , S&I, (4.23) where yil) = P-1Bi/Ms$2) (4.24 a). ... 4.24 b) = 1 1 8 ) K21og K O ( K 2 ). Truncating a t n = N = 2 , we obtain the second approximation.

26 Mar 2023: 6.8)Substituting (6.8) and (6.3) into (6.4), we obtain. w2N /(24 tan2 α) sN wN = 3A/2, wN =. (vN. β sin α. )1/2,. wN = 12 tan

27 Apr 2006: iments havebeenusedin drawing up fig. 3.) Fig.1 • 24.5 5 then plots the heightsof the mushy layer and. ... 0 24 concentrationsas functions of time for experi-0 100 200 300 400 500 mentswith the six different valuesof the contam-.

17 Jan 2019: With these scalings, equations(22) and (24) can be written in dimensionless form as. ... 24] A.W. Rempel, M.G. Worster, The interaction between a particle and anadvancing solidification front, J.

26 Apr 2006: The boundaryconditions at t'0 are Eq. (12),. h"0 (z"f(t)) (23). [h]ml "0 (z"f(t)), (24). ... Wettlaufer, M.G. Worster, H.E. Huppert, Geophys. Res. Lett. 24 (1997) 1251.[12] D.L.

21 Oct 2011: 546 A. C. Slim and H. E. Huppert. curve having. F (3 24/3Mr /7. ... B. 1996 Mixing in lock-release gravity currents. Dyn. Atmos.Oceans 24, 183–195.

28 Jul 2006: Geology 186 24.6 1.64 220 12.6 1.80. JFM 197 22.5 1.50 265 11.3 1.61.

27 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