Andrew J. L. Harris’s research while affiliated with University of Clermont Auvergne and other places

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Publications (48)


(a) Simulation of Radiative Power (RP) retrieval applying Equation 3 (RPTrue ${\text{RP}}_{\text{True}}$)and Equation 5 (RPPixel ${\text{RP}}_{\text{Pixel}}$) for a 375 m Visible Infrared Imaging Radiometer Suite I5 pixel at 11.45 μm. Simulations are for a bi‐component model whereby a single hot component (ranging from 300 to 1,500 K, occupying an area between 1 and 375 m²) is surrounded by a background held at a fixed temperature of 285 K. Emissivity of one is assumed. Colors show the temperature of the simulated hot component. Black solid line shows the 1:1 ratio. Dashed/dotted lines show 50%, 75%, and 90% error bounds as described in legend. (b) Ratio between RPPixel ${\text{RP}}_{\text{Pixel}}$ and RPTrue ${\text{RP}}_{\text{True}}$ showing how deviation from pure pixel assumption leads to underestimations exceeding 90%. Colors describe the areal fraction occupied by the hot thermal component.
(a) Radiative Power (RP; RPTrue∗ ${\text{RP}}_{\text{True}}^{\ast }$) emitted per unit surface area (dashed line), and ∆LTIR ${\mathit{{\increment}}L}_{\text{TIR}}$ at 11.45 μm, above a background of 285 K (solid line; Equation 6). The hotspot is assumed to fill the pixel at a homogenous temperature of Teff ${T}_{\text{eff}}$. The vertical red line delimits the 300–600 K range where Equation 7 holds. (b) kTIR ${k}_{\text{TIR}}$, as a function of the effective radiation temperature, derived from Equation 7. The solid black line shows the ratio computed for a pure pixel at homogenous temperature. The light‐gray dots represent the ratio for the mixed pixel simulations described in Section 3.1 and Supporting Information S1, with uniform random components(U) assigned to Nhot ${N}_{\text{hot}}$ ([1,250]) and Nbg ${N}_{\text{bg}}$ ([1,25]). In the range ∼300–600 K, delimited by the vertical red line, and for λ $\lambda $ = 11.45, optimal kTIR ${k}_{\text{TIR}}$ has a value of 60.17 μm · $\mathit{\cdot }$ sr (black solid‐to‐dashed horizontal line; calculated via Equation 8) ±35% (gray shaded region). (c) Simulation of RP retrieval applying Equation 1 (RPPixel ${\text{RP}}_{\text{Pixel}}$) and Equation 9 (VRPTIR ${\text{VRP}}_{\text{TIR}}$) for a 375 m Visible Infrared Imaging Radiometer Suite I5 pixel at 11.45 μm. Simulations are obtained as described in Section 3.1 and panel (b). An emissivity of one is assumed (see Text S1 in Supporting Information S1 for details). Colours show the effective radiation temperature. Black solid line shows the 1:1 ratio. Gray shaded region marks the ±35% interval. (d) Ratio between RPPixel ${\text{RP}}_{\text{Pixel}}$ and VRPTIR ${\text{VRP}}_{\text{TIR}}$ showing how Equation 9 returns RP estimate with an uncertainty of ±35% (gray shaded region). See Figures S2–S5 in Supporting Information S1 for full range simulations (10.5–12 μm).
Schematic representation (not to scale) of (a) Crater lakes, (b) fumarole fields and (c), hybrid systems. (d) Robinson World projection (M_Map package; Pawlowicz, 2020) with case study location depicted with cyan, red, and yellow triangles for crater lakes, fumarolic fields, and hybrid systems, respectively. In brackets is reported the altitude of each site (in m a.s.l.).
(a) TIRVolcH‐retrieved VRPTIR ${\text{VRP}}_{\text{TIR}}$ timeseries (gray bars) for Mount Ruapehu (NZ). The red and the black solid lines show the monthly averaged RPTrue ${\text{RP}}_{\text{True}}$—obtained from ground truth data (see Text S3 in Supporting Information S1 for details)—and VRPTIR ${\text{VRP}}_{\text{TIR}}$, respectively. (b) Scatter plot between monthly averaged RPTrue ${\text{RP}}_{\text{True}}$ (x‐axis) and VRPTIR ${\text{VRP}}_{\mathbf{\text{TIR}}}$ (y‐axis). The gray‐shaded region encompasses the ±35% confidence of the method. (c–h) TIRVolcH‐retrieved VRPTIR ${\text{VRP}}_{\text{TIR}}$ timeseries (gray bars) for volcanoes where ground truth measures (red triangles) were available (with the exception of Puracé (f), where no data are available). Ground truth data are from (a, h) GeoNet (fits.geonet.org.nz), (c) Armienta et al. (2014), (d) Maussen et al. (2018) and Bernard et al. (2020), (e) Mannini et al. (2019) and Pailot‐Bonnétat et al., 2023, (g) Rouwet et al. (2019), Salvage et al. (2018), and Sibaja‐Brenes et al. (2023).
Volcanic Radiative Power Retrieval From Moderate‐to‐Low‐Temperature Features Using a Single TIR Band: Validation Using Volcanic Crater Lakes and Hydrothermal Systems
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June 2025

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Diego Coppola

Plain Language Summary We present a new method, VRPTIR VRPTIR{\text{VRP}}_{\text{TIR}}, for monitoring thermal energy emission at volcanoes using satellite data, overcoming the challenges posed by hazardous ground conditions. This approach measures thermal energy loss from moderate‐to‐low‐temperature volcanic features, such as crater lakes and fumaroles, with temperatures below 330°C. We validated the VRPTIR VRPTIR{\text{VRP}}_{\text{TIR}} by comparing satellite measurements with long‐term data from Mount Ruapehu (New Zealand), El Chichón (Mexico), Taal (Philippines), Vulcano (Italy), Puracé (Colombia), Poás (Costa Rica), and White Island (New Zealand). Results indicate an excellent correlation between satellite‐based VRPTIR VRPTIR{\text{VRP}}_{\text{TIR}} and available ground‐based measurements, confirming its reliability and global monitoring potential. We observed significant variations at multiple locations, including previously unseen thermal unrest at Puracé volcano, highlighting the ability of VRPTIR VRPTIR{\text{VRP}}_{\text{TIR}} to promptly identify changes in volcano thermal state. The VRPTIR VRPTIR{\text{VRP}}_{\text{TIR}} method offers valuable insights into volcano dynamics and is crucial for compiling global thermal energy records, improving monitoring, and mitigating volcanic hazards.

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Inundation and evacuation of shoreline populations during landslide-triggered tsunamis: an integrated numerical and statistical hazard assessment

November 2024

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92 Reads

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1 Citation

The volcanic island of Stromboli (southern Tyrrhenian Sea, Italy) is renowned for its persistent, periodic, low-intensity explosive activity, whose spectacular manifestations attract tens of thousands of tourists every year. However, sporadic more intense major explosive and effusive eruptions and paroxysms pose serious threats to the island. In addition to direct hazards, granular slides of volcanic debris and pyroclastic avalanches, which can rapidly reach the sea and potentially generate tsunamis, are often associated with such unpredictable eruptive activity. Due to the very fast propagation of the tsunami around the island and the consequent short tsunami warning time (ranging from less than a minute to only a few minutes), mitigation efforts and evacuation from the Strombolian coast must be carefully planned. In this paper, we describe a new GIS-assisted procedure that allows us to combine the outputs of an ensemble of 156 pre-computed landslide-generated tsunami hazard scenarios (with variable landslide volume, position, and density), statistical exposure data (i.e. the number of inhabitants and tourists), and digital geographic information to obtain a quantitative (scenario-based) risk analysis. By means of the analysis of the road network and coastal morphology, we develop a model with routes and times to reach a safe area from every pixel in the inundated area and an appraisal of the time needed to escape versus the wave arrival time. This allows us to evaluate and quantify the effectiveness of potential risk mitigation by means of evacuation. The creation of an impact score linking the predicted inundation extent and the tsunami warning signals is intended, in the long term, to be used to predict the intensity of future tsunamis and to adapt evacuation plans accordingly. The model, here applied to Stromboli, is general and can be applied to other volcanic islands. Evacuating an island hosting several thousand tourists every summer with very little warning time underlines the absolute necessity for such mitigation efforts, aimed at informing hazard planners and managers and all other stakeholders.



Inversion of heat loss to obtain conductivity, density, and permeability at bottom-heated surfaces: the case of the hydrothermal system at Vulcano between 2019 and 2023

June 2024

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20 Reads

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2 Citations

Bulletin of Volcanology

At hydrothermal systems, heat transfer across the final surface layer is driven by permeable convection and conduction, so that soil permeability and thermal conductivity play fundamental roles in controlling heat flux to the atmosphere. We build a Rayleigh-number driven heat transfer model for a bottom-heated surface that uses measurements of heat flux density (radiation and convection to the atmosphere in W/m2), surface temperature, and soil temperature to solve for soil conductivity, density, and permeability for such a bottom-heated surface. At Vulcano in 2019, we measured an ASTER-derived heat flux density of 240 ± 70 W/m2 and a difference between soil and surface temperature of 18 ± 6 °C. The surface layer is a 7.5 ± 2.5 cm thick case-hardened crust across which heat transfer is conduction dominated. We invert our heat transfer model using the temperature (T) gradient derived from a trench dug into the soil: T = − 49.7y2 + 113.6y + 35 (R2 = 0.9997), where y is depth in meters between the surface and 70 cm. The result is a conductivity for the case-hardened surface layer of 1.0 ± 0.3 W/(m K) and a density of 2440 ± 120 kg/m3. Below this case-hardened crust, heat transfer is dominated by permeable convection in a soil comprised of highly altered trachytic blocks in an ash matrix. Our model gives permeabilities of 1–19 × 10−10 m2 for this layer in 2019. In 2021, Vulcano entered a phase of unrest. Our model reveals that this was associated with an increase in permeability to 10−7 m2. However, by 2023 permeabilities had reverted to pre-unrest levels. Using simple measurements of surface and soil temperature, coupled with heat flux density from a satellite overpass, the model can be used as a basis to constrain heat transfer and to assess permeability at any hydrothermal system.



When the lava meets the sea: emplacement of the 2–4 ka San Bartolo lava flow field, Stromboli volcano (Italy)

April 2024

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117 Reads

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4 Citations

Bulletin of Volcanology

When a lava flow enters a body of water, either a lake, sea, river or ocean, explosive interaction may arise. However, when it is an 'a'ā lava flow entering water, a more complex interaction occurs, that is very poorly described and documented in literature. In this paper, we analysed the 2–4 ka San Bartolo lava flow field emplaced on the north flank of Stromboli volcano, Italy. The lava flow field extends from ~ 650 m a.s.l. where the eruptive fissure is located, with two lava channels being apparent on the steep down to the coast. Along the coast the lava flow field expands to form a lava delta ~ 1 km wide characterised by 16 lava ‘Flow’ units. We performed a field survey to characterise the features of lava entering the sea and the associated formation of different components and magnetic measurements to infer the flow fabrics and emplacement process of the lava flow system. We measured the density, porosity and connectivity of several specimens to analyse the effect of lava-water interaction on the content in vesicles and their connectivity and conducted a macroscopic componentry analysis (clast count) at selected sites to infer the character of the eroded offshore segment of the lava flow field and its component flow units. The collected data allowed us to define the main components of a lava delta fed by 'a'ā lava flows, with its channels, littoral units, ramps, lava tubes, and inflated pāhoehoe flows controlled by the arterial 'a'ā flow fronts. The spatial organisation of these components allowed us to build a three-step descriptive model for 'a'ā entering a water. The initial stage corresponds to the entry of channel-fed 'a'ā lava flow into the sea which fragments to form metric blocks of 'a'ā lava. Continued lava supply to the foreshore causes flow units to stall while spreading over this substrate. Subsequent 'a'ā lava flow units ramp up behind the stalled flow front barrier. Lava tubes extending through the stalled flow barrier feed the seaward extension of a bench made of several pāhoehoe flow units.


An empirical relation between velocity, mass discharge rate and vent area for normal through paroxysmal eruptions at Stromboli

February 2024

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52 Reads

Bulletin of Volcanology

Based on published and new data for explosive events at Stromboli (Italy), we propose an empirical relation that links mass discharge rate (MDR) and at-vent gas jet velocity (Gv). We use 65 simultaneous measurements of MDR and Gv and find two trends in both the cross-correlation and rank order statistics. Cross-correlation gives a power law relation: MDR=10(0.015Gv+2.434)MDR= {10}^{(0.015{G}_{v}+2.434)} kg/s, R2 = 0.81, and applies to ash-dominated emissions. Combining this relation with the conservation of mass equation allows at-vent plume density and/or vent area to be derived from MDR = Gv ρ A, ρ being plume density and A being vent cross-sectional area. We find that while a vent radius of 2 m and plume density of 0.35 kg/m3 fits with the “normal” activity at Stromboli, a 290 × 2.5 m vent area likely feeds a 10 kg/m3 jet during paroxysmal activity. Initial tests on available data shows promise in extending the correlation beyond Stromboli and/or to events with higher MDR (> 107 kg/s). However, the exact relation will depend on magma composition, temperature and volatile content, as well as conduit radius and vent overpressure.


When the lava meets the sea: emplacement of the 2-4 ka San Bartolo lava flow field, Stromboli volcano (Italy)

January 2024

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186 Reads

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1 Citation

When a lava flow enters a body of water, either a lake, sea, river or ocean, explosive interaction may arise. However, when it is an 'a'ā lava flow entering water, a more complex interaction occurs, that is very poorly described and documented in literature. In this paper we analysed the 2–4 ka San Bartolo lava flow field emplaced on the north flank of Stromboli volcano, Italy. The lava flow field extends from ~ 650 m elevation, where the eruptive fissure emplaced following the main structural trend of the island, to the NE coast through two prominent lava channels at middle elevation. Along the coast the lava flow field expands to form a lava delta ~ 1 km wide characterized by 16 lava ‘Flow’ units. We performed a field survey to characterize the features of lava entering the sea and the associated formation of different components, and magnetic measurements to infer the flow fabrics and emplacement process of the lava flow system. We measured the density, porosity and connectivity of several specimens to analyse the effect of lava-water interaction on the content in vesicles and their connectivity, and conducted a macroscopic componentry analysis (clast count) at selected sites to infer the character of the eroded offshore segment of the lava flow field and its component flow units. The collected data allowed us to define the main components of a lava delta fed by 'a'ā lava flows, with its channels, littoral units, ramps, lava tubes, and inflated pāhoehoe flows controlled by the arterial 'a'ā flow fronts. The spatial organization of these components allowed us to build a 3-steps model for 'a'ā entering a water. The initial stage corresponds to the entry of channel-fed 'a'ā lava flow into the sea which fragments to form metric blocks of 'a'ā lava. Continued lava supply to the foreshore causes flow units to stall while spreading over this substrate. Subsequent 'a'ā lava flow units ramp up behind the stalled flow front barrier. Lava tubes extending through the stalled flow barrier feed the seaward extension of a bench made of several pāhoehoe flow units.


Inundation and evacuation of shoreline populations during landslide-triggered tsunami: An integrated numerical and statistical hazard assessment

January 2024

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79 Reads

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1 Citation

The volcanic island of Stromboli (Southern Tyrrhenian sea, Italy) is renowned for its persistent, periodic, low-intensity explosive activity, whose spectacular manifestations attract tens of thousands of tourists every year. However, sporadic more intense major explosive and effusive eruptions, and paroxysms, pose serious threats to the island. In addition to direct hazards, granular slides of volcanic debris and pyroclastic avalanches, which can rapidly reach the sea potentially generating tsunamis, are often associated with such unpredictable eruptive activity. Due to the very fast propagation of the tsunami around the island, and the consequent short tsunami warning time (ranging from less than a minute to only a few minutes) mitigation efforts and evacuation from the Strombolian coast must be carefully planned. In this paper, we describe a new, GIS-assisted procedure that allows us to combine the outputs of an ensemble of 156 pre-computed landslide-generated tsunami hazard scenarios (with variable landslide volume, position, and density), statistical exposure data (i.e., the number of inhabitants and tourists) and digital geographic information, to obtain a quantitative (scenario-based) risk analysis. By means of the analysis of the road network and coastal morphology, we develop a model with routes and times to reach a safe area from every pixel in the inundated area, and appraisal for the time needed to escape versus the wave arrival time. This allows us to evaluate and quantify the effectiveness of potential risk mitigation by means of evacuation. The creation of an impact score linking the predicted inundation extent and the tsunami warning signals is intended, in the long term, to predict the intensity of future tsunamis, and to adapt evacuation plans accordingly. The model, here applied to Stromboli, is general, and can be applied to other volcanic islands. Evacuating an island hosting several thousand tourists every summer with very little warning time supports the absolute necessity for such mitigation efforts, aimed at informing hazard planners and managers, and all other stakeholders.



Citations (31)


... In this study, the AMS was measured to check its consistency with the emplacement direction of the CDB lava flow (e.g., Caballero-Miranda et al., 2016;Ellwood, 1978;Cañón-Tapia, 2004;Cañón-Tapia et al., 1996;Loock et al., 2008;Panaiotu et al., 2011;Prival et al., 2023;Shajahan et al., 2024). ...

Reference:

Paleomagnetic study of the Capo di Bove lava flow, Rome, Italy
When the lava meets the sea: emplacement of the 2–4 ka San Bartolo lava flow field, Stromboli volcano (Italy)

Bulletin of Volcanology

... Finally, the information provided by such a set of scenarios (Cerminara et al., 2024) has been recently used by Bonilauri et al. (2024) to evaluate and quantify the effectiveness of potential risk mitigation by means of evacuation on the island of Stromboli. Ongoing effort is dedicated to use expert elicitation tools (de'Michieli Vitturi et al., 2024;Tadini et al., 2024) to attribute probabilities to volume and initial position ranges utilized in this work, to combine all scenarios into a probabilistic tsunami inundation hazard map for Stromboli. ...

Inundation and evacuation of shoreline populations during landslide-triggered tsunami: An integrated numerical and statistical hazard assessment

... To do this we apply the deep learning framework DITAN (Giannoulis et al., 2023) to time series data for surface temperature and meteorological conditions collected in-situ at the active hydrothermal system at Vulcano (Pailot-Bonnétat and Harris, 2024), in an experiment designed to answer the stated research question. We begin by describing the characteristics of the study site (Vulcano) and the instrumentation installed there, before reviewing DITAN, its performance and output. ...

A Thermal Record for Unrest at Vulcano 2020–2022: In Situ Meteorological Data and Soil Temperature Recorded at High Temporal Resolution
  • Citing Article
  • January 2024

Bulletin of Volcanology

... Combining multiple satellite data observing thermal anomalies, deformation, gas emissions and ash plume through multi-parameter analysis can provide insights into the complex, interconnected processes driving volcanic activity offering an excellent possibility for forecasting, detecting, and tracking eruptive activity (Genzano et al., 2021;Corradino et al., 2023). Following the fast technological advances in satellite sensors (higher temporal and spatial resolution), several research activities have been aimed at improving the technique for satellite data analysis with the goal to have a faster and high quality response in order to have the opportunity to track volcanic events with fast dynamics. ...

Detection of Subtle Thermal Anomalies: Deep Learning Applied to the ASTER Global Volcano Dataset

IEEE Transactions on Geoscience and Remote Sensing

... A comprehensive description of a stratigraphic section includes both the general information of the section and the details on the sampled layers (Thivet et al. 2020;Di Muro et al. 2021;Prival et al. 2022;Lacombe et al. 2024;Re et al. 2025;Shajahan et al. 2024). The former includes information about the name of the section, its orientation, and thickness. ...

Emplacement dynamics of a crystal-rich, highly viscous trachytic flow of the Sancy stratovolcano, France
  • Citing Article
  • December 2022

Geological Society of America Bulletin

... Other common possible issues may be forgotten passwords, lost files, and unclear formatting. These issues can result in delays, rejections, or even the loss of valuable research findings, even well-designed studies [4]. As an experienced editor, author has also observed many quality research papers being delayed for publication only due to poorly written manuscript, mostly either because of computer inefficiency or of language barrier. ...

Guidelines on manuscript format, structure, and style: avoiding editorial holdups in the publication process
  • Citing Article
  • December 2022

Bulletin of Volcanology

... Several andesitic open-vent volcanoes have been identified in the Ecuadorian arc, these include Tungurahua (Eychenne et al., 2013;Hidalgo et al., 2015;Samaniego et al., 2011), Reventador Ridolfi et al., 2008;Vásconez et al., 2022) and Cotopaxi (Gaunt et al., 2016;Hidalgo et al., 2018). In this study, we present componentry, geochemical and petrological data from tephra samples of Sangay, another andesitic open-vent volcano from Ecuador. ...

Ash and gas discharge during open vent activity at El Reventador (Ecuador): explosion-style transitions driven by conduit capping
  • Citing Article
  • August 2022

Bulletin of Volcanology

... Camera-generated proximal thermal infrared (TIR) observations are widely used to monitor and study volcanoes, and several studies have reported the use of TIR observations to follow evolutions of volcanic activity and to map distributions of volcanic products [50][51][52][53][54][55][56][57][58]. In contrast, very few volcanic areas are currently being monitored with permanent, ground, proximal networks of TIR cameras during non-eruptive periods to detect surface temperature variations as indicators of possible changes in the volcanic system [59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74][75][76]. ...

VIGIA: A Thermal and Visible Imagery System to Track Volcanic Explosions

... At the beginning of the eruption, the effusive activity could have progressively focused from an initial elongated eruptive fissure to a more central, sustained, main event, as observed in subaerial eruptions (e.g., Jones & Llewellin, 2021). This evolution implies a waning ascent velocity and a progressive weakening of the fountaining, and to lava flow through tube systems (e.g., Castro & Feisel, 2022;Chevallier & Bachèlery, 1981;La Spina et al., 2021;Peltier et al., 2009;Verdurme et al., 2022). Furthermore, some samples collected near the summit of Fani Maoré (e.g., PL777_08 dive, Figure 1d) show similar petrological, thermal and chemical composition than Phase 2 and Phase 3 samples which were only observed in the south, west and northwest lava flows (Figure 1). ...

Lava Volume from Remote Sensing Data: Comparisons with Reverse Petrological Approaches for Two Types of Effusive Eruption

... Sierra Negra, an 1,140 m high basaltic shield volcano, in the Galápagos, Ecuador has been much less studied and characterized than Kīlauea or Piton de la Fournaise in the literature to date (e.g., Hibert et al., 2015;Patrick et al., 2019;Peltier et al., 2022), and this provides new opportunities to improve knowledge of the seismoacoustics of basaltic shield volcanoes and their eruption mechanisms. Moreover, considering that at volcanoes in the Galápagos, lava extrusion occurs at radial and circumferential fissures widely scattered around the calderas without showing a dominant location or direction (Chadwick & Howard, 1991), it becomes necessary to develop methods and test geophysical networks for determining the location of active fissures during ongoing eruptions. ...

Reappraisal of gap analysis for effusive crises at Piton de la Fournaise

Journal of Applied Volcanology