Abstract

Abstract. Dry-snow slab avalanches are generally caused by a sequence of fracture processes including (1) failure initiation in a weak snow layer underlying a cohesive slab, (2) crack propagation within the weak layer and (3) tensile fracture through the slab which leads to its detachment. During the past decades, theoretical and experimental work has gradually led to a better understanding of the fracture process in snow involving the collapse of the structure in the weak layer during fracture. This now allows us to better model failure initiation and the onset of crack propagation, i.e., to estimate the critical length required for crack propagation. On the other hand, our understanding of dynamic crack propagation and fracture arrest propensity is still very limited. To shed more light on this issue, we performed numerical propagation saw test (PST) experiments applying the discrete element (DE) method and compared the numerical results with field measurements based on particle tracking. The goal is to investigate the influence of weak layer failure and the mechanical properties of the slab on crack propagation and fracture arrest propensity. Crack propagation speeds and distances before fracture arrest were derived from the DE simulations for different snowpack configurations and mechanical properties. Then, in order to compare the numerical and experimental results, the slab mechanical properties (Young's modulus and strength) which are not measured in the field were derived from density. The simulations nicely reproduced the process of crack propagation observed in field PSTs. Finally, the mechanical processes at play were analyzed in depth which led to suggestions for minimum column length in field PSTs.

Highlights

  • Dry-snow slab avalanches result from the failure of a weak snow layer underlying cohesive slab layers

  • Concerning the normal restitution coefficient e, we verified that the results presented below, and more generally all the macroscopic mechanical quantities obtained from the simulations, are independent of this parameter

  • Between 0 and 0.1 s nothing happens, as the saw advances, the vertical displacement slowly increases. This phase corresponds to the bending of the under-cut part of the slab

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Summary

Introduction

Dry-snow slab avalanches result from the failure of a weak snow layer underlying cohesive slab layers. Crack propagation leads to the tensile fracture of the slab and avalanche release (McClung, 1979; Schweizer et al, 2003). The PST allows observers to determine the critical crack length and evaluate crack propagation propensity. This field method has highlighted the importance of slab bending (due to the collapsible nature of weak snow layers) on crack propagation Theoretical and numerical models, based on fracture mechanics or strength of material approaches, were developed to investigate crack propagation and avalanche release (McClung, 1979; Chiaia et al, 2008; Heierli et al, 2008; Gaume et al, 2013, 2014b).

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