Abstract

Abstract. Soft-sediment deformation structures can provide valuable information about the conditions of parent flows, the sediment state and the surrounding environment. Here, examples of soft-sediment deformation in deposits of dilute pyroclastic density currents are documented and possible syn-eruptive triggers suggested. Outcrops from six different volcanoes have been compiled in order to provide a broad perspective on the variety of structures: Soufrière Hills (Montserrat), Tungurahua (Ecuador), Ubehebe craters (USA), Laacher See (Germany), and Tower Hill and Purrumbete lakes (both Australia). The variety of features can be classified in four groups: (1) tubular features such as pipes; (2) isolated, laterally oriented deformation such as overturned or oversteepened laminations and vortex-shaped laminae; (3) folds-and-faults structures involving thick (>30 cm) units; (4) dominantly vertical inter-penetration of two layers such as potatoids, dishes, or diapiric flame-like structures. The occurrence of degassing pipes together with basal intrusions suggest fluidization during flow stages, and can facilitate the development of other soft-sediment deformation structures. Variations from injection dikes to suction-driven, local uplifts at the base of outcrops indicate the role of dynamic pore pressure. Isolated, centimeter-scale, overturned beds with vortex forms have been interpreted to be the signature of shear instabilities occurring at the boundary of two granular media. They may represent the frozen record of granular, pseudo Kelvin–Helmholtz instabilities. Their recognition can be a diagnostic for flows with a granular basal boundary layer. Vertical inter-penetration and those folds-and-faults features related to slumps are driven by their excess weight and occur after deposition but penecontemporaneous to the eruption. The passage of shock waves emanating from the vent may also produce trains of isolated, fine-grained overturned beds that disturb the surface bedding without occurrence of a sedimentation phase in the vicinity of explosion centers. Finally, ballistic impacts can trigger unconventional sags producing local displacement or liquefaction. Based on the deformation depth, these can yield precise insights into depositional unit boundaries. Such impact structures may also be at the origin of some of the steep truncation planes visible at the base of the so-called "chute and pool" structures. Dilute pyroclastic density currents occur contemporaneously with seismogenic volcanic explosions. They can experience extremely high sedimentation rates and may flow at the border between traction, granular and fluid-escape boundary zones. They are often deposited on steep slopes and can incorporate large amounts of water and gas in the sediment. These are just some of the many possible triggers acting in a single environment, and they reveal the potential for insights into the eruptive and flow mechanisms of dilute pyroclastic density currents.

Highlights

  • The dynamics of pyroclastic density currents (PDCs) remain poorly understood

  • Syn-depositional soft-sediment deformation (SSD) structures provide constraint on the shearing and dynamic pore pressure at the basal boundary layer (BBL) that controls the sedimentation of PDCs, whereas syn-eruptive SSD records information on the eruptive dynamics and depositional units

  • The exercise presented here has demonstrated the richness of information contained in SSD structures from the dilute PDC environment

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Summary

Introduction

The dynamics of pyroclastic density currents (PDCs) remain poorly understood. This is despite the fact that they are one of the most efficient transport means on the flanks of volcanoes exhibiting explosive eruptions, thereby yielding a major risk potential for life, environment and infrastructures. Cross-bedded, dilute PDC deposits can contain intriguing overturned and deformed patterns attributed to soft-sediment deformation (SSD). The understanding of these structures can yield insight into the syn- and postdepositional processes surrounding the bed interface: i.e., the basal boundary layer (BBL), the bed state, and conditions extant in the emplacement environment.

Soft-sediment deformation
Nomenclature
PDCs and their possible SSD triggers
Granular shear instabilities
Geological settings and occurrence of SSD structures
Discussion and interpretation
Influence of dynamic pore pressure
Granular shear and pseudo Kelvin–Helmholz instabilities
Slumps
Granular Rayleigh–Taylor instabilities
Impact records
A trigger for “chute and pool” structures?
Deformation driven by shock waves
Conclusions
Findings
Granular Kelvin–Helmholtz instabilities at a bed-flow interface
Full Text
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