Abstract

Abstract. The failure of a weak snow layer buried below cohesive slab layers is a necessary, but insufficient, condition for the release of a dry-snow slab avalanche. The size of the crack in the weak layer must also exceed a critical length to propagate across a slope. In contrast to pioneering shear-based approaches, recent developments account for weak layer collapse and allow for better explaining typical observations of remote triggering from low-angle terrain. However, these new models predict a critical length for crack propagation that is almost independent of slope angle, a rather surprising and counterintuitive result. Based on discrete element simulations we propose a new analytical expression for the critical crack length. This new model reconciles past approaches by considering for the first time the complex interplay between slab elasticity and the mechanical behavior of the weak layer including its structural collapse. The crack begins to propagate when the stress induced by slab loading and deformation at the crack tip exceeds the limit given by the failure envelope of the weak layer. The model can reproduce crack propagation on low-angle terrain and the decrease in critical length with increasing slope angle as modeled in numerical experiments. The good agreement of our new model with extensive field data and the ease of implementation in the snow cover model SNOWPACK opens a promising prospect for improving avalanche forecasting.

Highlights

  • Snow slab avalanches range among the most prominent natural hazards in snow-covered mountainous regions throughout the world

  • The crack of length a created by the advancing saw in the weak layer (WL) induces slope-parallel and slopenormal displacements of the slab due to gravity leading to tension and bending in the slab

  • We proposed a new analytical expression to assess the conditions for the onset of crack propagation in weak snowpack layers

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Summary

Introduction

Snow slab avalanches range among the most prominent natural hazards in snow-covered mountainous regions throughout the world. Avalanches are the result of numerous factors and processes interacting over a large range of temporal and spatial scales (Schweizer et al, 2003). While snow slab avalanches can come in many different sizes, from a few meters to several kilometers, they initiate within the snow cover by local damage processes at the grain scale. The initial failure resulting in a macroscopic crack in the WL develops from microscale heterogeneities by damage accumulation (Schweizer et al, 2008; Gaume et al, 2014b) or directly below a local overload such as a skier or a snowmobile (van Herwijnen and Jamieson, 2005; Thumlert and Jamieson, 2014).

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