Abstract

Abstract. Cliff collapse poses a serious hazard to infrastructure and passers-by. Obtaining information such as magnitude-frequency relationship for a specific site is of great help to adapt appropriate mitigation measures. While it is possible to monitor hundreds-of-meter-long cliff sites with ground based techniques (e.g. lidar or photogrammetry), it is both time consuming and scientifically limiting to focus on short cliff sections. In the project SUAVE, we sought to investigate whether an octocopter UAV photogrammetric survey would perform sufficiently well in order to repeatedly survey cliff face geometry and derive rock fall inventories amenable to probabilistic rock fall hazard computation. An experiment was therefore run on a well-studied site of the chalk coast of Normandy, in Mesnil Val, along the English Channel (Northern France). Two campaigns were organized in January and June 2015 which surveyed about 60 ha of coastline, including the 80-m-high cliff face, the chalk platform at its foot, and the hinterland in a matter of 4 hours from start to finish. To conform with UAV regulations, the flight was flown in 3 legs for a total of about 30 minutes in the air. A total of 868 and 1106 photos were respectively shot with a Sony NEX 7 with fixed focal 16mm. Three lines of sight were combined: horizontal shots for cliff face imaging, 45°-oblique views to tie plateau/platform photos with cliff face images, and regular vertical shots. Photogrammetrically derived dense point clouds were produced with Agisoft Photoscan at ultra-high density (median density is 1 point every 1.7cm). Point cloud density proved a critical parameter to reproduce faithfully the chalk face’s geometry. Tuning down the density parameter to “high” or “medium”, though efficient from a computational point of view, generated artefacts along chalk bed edges (i.e. smoothing the sharp gradient) and ultimately creating ghost volumes when computing cloud to cloud differences. Yet, from a hazard point of view, this is where small rock fall will most likely occur. Absolute orientation of both point clouds proved unsufficient despite the 30 black and white quadrants ground control point DGPS surveyed. Additional ICP was necessary to reach centimeter-level accuracy and segment rock fall scars corresponding to the expected average daily rock fall volume (ca. 0.013 m3).

Highlights

  • In the last decade, advances in rock fall hazards has widely benefitted from the topographic measurement capacity of Terrestrial Laser Scanners (Abellán et al, 2010; Dewez and Rohmer, 2013; Rosser et al, 2014)

  • A method to compute the probability of cliff collapse from Terrestrial Laser Scanners (TLS) data was proposed by Dewez and Rohmer, (2013) based on a data set collected by TLS between 2005 and 2008 on the coastal chalk cliff of Mesnil Val, in Normandy

  • As TLS surveys were impacted by the positional quality of ground control points (GCP), we addressed the question to Unmanned Aerial Vehicles (UAV) point clouds in a similar manner

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Summary

Introduction

Advances in rock fall hazards has widely benefitted from the topographic measurement capacity of Terrestrial Laser Scanners (Abellán et al, 2010; Dewez and Rohmer, 2013; Rosser et al, 2014). A method to compute the probability of cliff collapse from TLS data was proposed by Dewez and Rohmer, (2013) based on a data set collected by TLS between 2005 and 2008 on the coastal chalk cliff of Mesnil Val, in Normandy The use of this method is obvious to land managers and public safety authorities. It permits to assess the time frame within which an asset, a house for instance, will be under a threat of damage from a given rock fall, in a probabilistic sense To replicate this experiment more extensively on a commercial basis, the acquisition and computation pipeline needs be practical: involve efficient survey equipment, guarantee sufficient a degree of rock fall scar detection and be versatile for all kinds of rock faces. Two options are possible: projecting the 3D cliff onto a simple mathematical surface object - planes and arcs of cylinders, which is done in Giuliano et al (submitted); or processing the 3D point clouds natively in 3D, which we discuss here

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