Retrogressive failure of a static granular layer on an inclined plane

When a layer of static grains on a sufficiently steep slope is disturbed, an upslope-propagating erosion wave, or retrogressive failure, may form that separates the initially static material from a downslope region of flowing grains. This paper shows that a relatively simple depth-averaged avalanche model with frictional hysteresis is sufficient to capture a planar retrogressive failure that is independent of the cross-slope coordinate. The hysteresis is modelled with a non-monotonic effective basal friction law that has static, intermediate (velocity decreasing) and dynamic (velocity increasing) regimes. Both experiments and time-dependent numerical simulations show that steadily travelling retrogressive waves rapidly form in this system and a travelling wave ansatz is therefore used to derive a one-dimensional depth-averaged exact solution. The speed of the wave is determined by a critical point in the ordinary differential equation for the thickness. The critical point lies in the intermediate frictional regime, at the point where the friction exactly balances the downslope component of gravity. The retrogressive wave is therefore a sensitive test of the functional form of the friction law in this regime, where steady uniform flows are unstable and so cannot be used to determine the friction law directly. Upper and lower bounds for the existence of retrogressive waves in terms of the initial layer depth and the slope inclination are found and shown to be in good agreement with the experimentally determined phase diagram. For the friction law proposed by Edwards et al. (J. Fluid. Mech., vol. 823, 2017, pp. 278–315, J. Fluid. Mech., 2019, (submitted)) the magnitude of the wave speed is slightly under-predicted, but, for a given initial layer thickness, the exact solution accurately predicts an increase in the wave speed with higher inclinations. The model also captures the finite wave speed at the onset of retrogressive failure observed in experiments.

[1]  Richard M. Iverson,et al.  Flow of variably fluidized granular masses across three‐dimensional terrain: 2. Numerical predictions and experimental tests , 2001 .

[2]  J. L’Heureux,et al.  The 29th January 2014 submarine landslide at Statland, Norway—landslide dynamics, tsunami generation, and run-up , 2016, Landslides.

[3]  D. Varnes SLOPE MOVEMENT TYPES AND PROCESSES , 1978 .

[4]  G. Midi,et al.  On dense granular flows , 2003, The European physical journal. E, Soft matter.

[5]  Adrian Daerr,et al.  Dynamical equilibrium of avalanches on a rough plane , 2001 .

[6]  J. Gray,et al.  Erosion–deposition waves in shallow granular free-surface flows , 2014, Journal of Fluid Mechanics.

[7]  Michael Westdickenberg,et al.  Gravity driven shallow water models for arbitrary topography , 2004 .

[8]  S. Savage,et al.  The motion of a finite mass of granular material down a rough incline , 1989, Journal of Fluid Mechanics.

[9]  S. Edwards,et al.  A model for the dynamics of sandpile surfaces , 1994 .

[10]  Kolumban Hutter,et al.  Gravity-driven free surface flow of granular avalanches over complex basal topography , 1999, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[11]  Sebastian Noelle,et al.  Shock waves, dead zones and particle-free regions in rapid granular free-surface flows , 2003, Journal of Fluid Mechanics.

[12]  Jan-Thomas Fischer,et al.  Topographic curvature effects in applied avalanche modeling , 2012 .

[13]  On the front shape of an inertial granular flow down a rough incline , 2015, 1511.03051.

[14]  O. Pouliquen ON THE SHAPE OF GRANULAR FRONTS DOWN ROUGH INCLINED PLANES , 1999 .

[15]  Betty Sovilla,et al.  The dynamics of surges in the 3 February 2015 avalanches in Vallée de la Sionne , 2016 .

[16]  Olivier Pouliquen,et al.  Friction law for dense granular flows: application to the motion of a mass down a rough inclined plane , 2001, Journal of Fluid Mechanics.

[17]  Lev S Tsimring,et al.  Continuum theory of partially fluidized granular flows. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[18]  L S Tsimring,et al.  Continuum description of avalanches in granular media. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[19]  S. Savage,et al.  The dynamics of avalanches of granular materials from initiation to runout. Part I: Analysis , 1991 .

[20]  Richard M. Iverson,et al.  Flow of variably fluidized granular masses across three‐dimensional terrain: 1. Coulomb mixture theory , 2001 .

[21]  J. Gray,et al.  A depth-averaged μ(I)-rheology for shallow granular free-surface flows , 2014 .

[22]  Jean-Pierre Vilotte,et al.  Numerical modeling of avalanches based on Saint-Venant equations using a kinetic scheme , 2003 .

[23]  D. J. Vanes Slope movement types and processes, in Landslides Analysis and control , 1978 .

[24]  Jean-Pierre Vilotte,et al.  Numerical modeling of self‐channeling granular flows and of their levee‐channel deposits , 2006 .

[25]  J. Gray,et al.  Multiple solutions for granular flow over a smooth two-dimensional bump , 2017, Journal of Fluid Mechanics.

[26]  Gaël Epely-Chauvin,et al.  Experimental investigation into segregating granular flows down chutes , 2011 .

[27]  C. Goujon,et al.  Monodisperse dry granular flows on inclined planes: Role of roughness , 2003, The European physical journal. E, Soft matter.

[28]  Triangular and uphill avalanches of a tilted sandpile , 1998 .

[29]  R. Iverson,et al.  U. S. Geological Survey , 1967, Radiocarbon.

[30]  G. Grest,et al.  Granular flow down an inclined plane: Bagnold scaling and rheology. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[31]  H. Mader,et al.  A two-layer approach to modelling the transformation of dilute pyroclastic currents into dense pyroclastic flows , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[32]  J. Gray,et al.  A two-dimensional depth-averaged ${\it\mu}(I)$ -rheology for dense granular avalanches , 2015, Journal of Fluid Mechanics.

[33]  M. Clare,et al.  Multiple Flow Slide Experiment in the Westerschelde Estuary, The Netherlands , 2016 .

[34]  C. Kuo,et al.  A hierarchy of avalanche models on arbitrary topography , 2009 .

[35]  J. Gray,et al.  A depth-averaged mu(I)-rheology for shallow granular free-surface flows , 2014 .

[36]  N. Mangold,et al.  Erosion and mobility in granular collapse over sloping beds , 2010 .

[37]  Mohamed Naaim,et al.  Dense snow avalanche modeling: flow, erosion, deposition and obstacle effects , 2004 .

[38]  K. Kamrin,et al.  Nonlocal modeling of granular flows down inclines. , 2015, Soft matter.

[39]  Chaojun Ouyang,et al.  Entrainment of bed material by Earth‐surface mass flows: Review and reformulation of depth‐integrated theory , 2015 .

[40]  Olivier Pouliquen,et al.  SCALING LAWS IN GRANULAR FLOWS DOWN ROUGH INCLINED PLANES , 1999 .

[41]  Dick R. Mastbergen,et al.  The importance of breaching as a mechanism of subaqueous slope failure in fine sand , 2002 .

[42]  N. Thomas,et al.  Relation between dry granular flow regimes and morphology of deposits: formation of levées in pyroclastic deposits , 2003, cond-mat/0312541.

[43]  Marc Christen,et al.  RAMMS: numerical simulation of dense snow avalanches in three-dimensional terrain , 2010 .

[44]  J. Vallance,et al.  Fine-grained linings of leveed channels facilitate runout of granular flows , 2014 .

[45]  J. Gray,et al.  Formation of levees, troughs and elevated channels by avalanches on erodible slopes , 2017, Journal of Fluid Mechanics.

[46]  Pierre-Gilles de Gennes,et al.  Surface flows of granular materials: a short introduction to some recent models , 2002 .

[47]  Olivier Pouliquen,et al.  A constitutive law for dense granular flows , 2006, Nature.

[48]  S. Pudasaini,et al.  Rapid shear flows of dry granular masses down curved and twisted channels , 2003, Journal of Fluid Mechanics.

[49]  Peter Sampl,et al.  Avalanche simulation with SAMOS , 2004, Annals of Glaciology.

[50]  Stéphane Douady,et al.  Two types of avalanche behaviour in granular media , 1999, Nature.

[51]  S. Savage,et al.  The dynamics of avalanches of granular materials from initiation to runout. Part II. Experiments , 1995 .

[52]  G. Pedersen,et al.  On the characteristics of landslide tsunamis , 2015, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[53]  A. Patra,et al.  Computing granular avalanches and landslides , 2003 .

[54]  R. Iverson,et al.  Grain-size segregation and levee formation in geophysical mass flows , 2012 .

[55]  Kolumban Hutter,et al.  Channelized free-surface flow of cohesionless granular avalanches in a chute with shallow lateral curvature , 1999, Journal of Fluid Mechanics.

[56]  G. Parker,et al.  Field-scale numerical modeling of breaching as a mechanism for generating continuous turbidity currents , 2011 .

[57]  Rou-Fei Chen,et al.  Simulation of Tsaoling landslide, Taiwan, based on Saint Venant equations over general topography , 2009 .

[58]  J. Gray,et al.  Frictional hysteresis and particle deposition in granular free-surface flows , 2019, Journal of Fluid Mechanics.

[59]  James W. Landry,et al.  Granular flow down a rough inclined plane: Transition between thin and thick piles , 2003 .

[60]  J. Gray,et al.  The kinematics of bidisperse granular roll waves , 2018, Journal of Fluid Mechanics.

[61]  J. Gray,et al.  Self-channelisation and levee formation in monodisperse granular flows , 2019, Journal of Fluid Mechanics.

[62]  E. Tadmor,et al.  New High-Resolution Central Schemes for Nonlinear Conservation Laws and Convection—Diffusion Equations , 2000 .

[63]  N. Balmforth,et al.  From episodic avalanching to continuous flow in a granular drum , 2014, Granular Matter.