Elsevier

Geomorphology

Volume 207, 15 February 2014, Pages 51-63
Geomorphology

Lahar hazard assessment in the southern drainage system of Cotopaxi volcano, Ecuador: Results from multiscale lahar simulations

https://doi.org/10.1016/j.geomorph.2013.10.026Get rights and content

Abstract

The ice-capped Cotopaxi volcano is known worldwide for the large-scale, catastrophic lahars that have occurred in connection with historical explosive eruptions. The most recent large-scale lahar event occurred in 1877 when scoria flows partially melted ice and snow of the summit glacier, generating debris flows that severely impacted all the river valleys originating from the volcano. The 1877 lahars have been considered in the recent years as a maximum expected event to define the hazard associated to lahar generation at Cotopaxi. Conversely, recent field-based studies have shown that such debris flows have occurred several times during the last 800 years of activity at Cotopaxi, and that the scale of lahars has been variable, including events much larger than that of 1877. Despite a rapid retreat of the summit ice cap over the past century, in fact, there are no data clearly suggesting that future events will be smaller than those observed in the deposits of the last 800 years of activity. In addition, geological field data prove that the lahar triggering mechanism also has to be considered as a key input parameter and, under appropriate eruptive mechanisms, a hazard scenario of a lahar with a volume 3-times larger than the 1877 event is likely. In order to analyze the impact scenarios in the southern drainage system of the volcano, simulations of inundation areas were performed with a semi-empirical model (LAHARZ), using input parameters including variable water volume. Results indicate that a lahar 3-times larger than the 1877 event would invade much wider areas than those flooded by the 1877 lahars along the southern valley system, eventually impacting highly-urbanized areas such as the city of Latacunga.

Introduction

Lahars, or volcanic debris flows, consist of high-concentration, sediment-loaded flows that occur on volcanic terrains. They may be a primary phenomenon directly triggered by eruptive activity (e.g. the 1985 Nevado del Ruiz event in Colombia; Pierson et al., 1990) or they may result from the post-eruptive mobilization (secondary lahars) of volcanic debris (e.g. the 1991 eruption of Mt. Pinatubo, Philippines; Rodolfo et al., 1996). Lahar generation requires a combination of three main factors including: (i) a triggering mechanism that rapidly makes available an adequate water source; (ii) the availability of abundant, unconsolidated debris; and (iii) steep slopes (Vallance, 2000). Due to water incorporation and volume increase, lahars can easily overflow lateral banks and spread over areas of low gradient. This can produce catastrophic consequences for the communities living along the areas, which can be inundated unexpectedly by lahars — as recently shown by the Pinatubo, Mayon and Nevado del Ruiz events (Pierson et al., 1990, Voight, 1990, Rodolfo, 1995, Newhall and Punongbayan, 1996, Tanguy et al., 1998).

According to Varnes (1978), we include here with the term ‘lahars’ not only debris flows but also hyperconcentrated mudflows (Smith and Lowe, 1991). Although the term has sometimes been used to refer to the deposits of such flows, Smith and Fritz (1989, p. 375) dismiss this meaning stating that “lahar is an event that can refer to one or more discrete processes, but does not refer to a deposit”. Small debris flows occur daily on the flanks of many active and inactive volcanoes; although traditionally the term ‘lahar’ has generally been restricted to those events which can generate a hazard to populations (Scott, 1988), nowadays lahar is fairly broadly used regardless if the event poses hazard to population or not (Manville et al., 2009). In the following, we will use lahar to refer to the process, and as a synonym of debris flow.

Lahars can be generated at crater lakes, following crater failures (Bornas et al., 2003, Manville and Cronin, 2007, Manville, 2010, Massey et al., 2010), or explosive expulsion of water (Zen and Hadikusumo, 1965, Nairn et al., 1979, Suryo and Clarke, 1985, Thouret et al., 1998, Németh et al., 2006, Kilgour et al., 2010) or by heavy rainfall on freshly deposited tephra or loose material on volcano slopes, as in the case of the 1991 eruption of Mt. Pinatubo (Rodolfo, 1989, Pierson et al., 1992, Arboleda and Martinez, 1996, Rodolfo et al., 1996). Lahars are also generated by the rapid melting of snow or ice on ice clad volcanoes, due to the interaction of eruptive products with the ice cap (Major and Newhall, 1989). As demonstrated by the 1985 Nevado del Ruiz event in Colombia, even small volcanic eruptions can trigger catastrophic lahar events when pyroclastic material interacts with a summit glacier (Pierson et al., 1990, Voight, 1990, Tanguy et al., 1998), especially if combined with seismic shaking and intense scouring of the ice (with consequent channeling of the lahar).

During the past 30 years, lahar-related disasters have been documented worldwide in the volcanological literature (Voight, 1990, Hall, 1992, Rodolfo, 1995, Newhall and Punongbayan, 1996, Tanguy et al., 1998, Wood and Soulard, 2009). In the last century, about 30,000 casualties were reported in relation to the occurrence of lahar events (Witham, 2005); about 80% of this terrific quota is related to a single event (the devastation of the village of Armero, following the 1985 eruption of Nevado del Ruiz). Continuous growth of buildings and settled areas in lahar flow paths demonstrates that better risk perception, land-use planning and rapid evacuation plans may combine in reducing damage and loss of life from future lahars (Wood and Soulard, 2009).

Cotopaxi volcano is well known for the potential destructiveness of its lahars, and models of lahar invasion have been recently applied to the northern and southern drainages (Barberi et al., 1992, Aguilera et al., 2004). Inundation areas for future lahars have also been partially explored by several authors (Miller et al., 1978, Hall and von Hillebrandt, 1988a, Hall and von Hillebrandt, 1988b, Mothes et al., 2004, Mothes, 2006) who presented maps of lahar inundation areas related to the last (1877) eruptive event and for future lahar-generating events of similar size. Modeling procedures were not presented in detail in these papers so that a more in-depth discussion on the potential of lahar inundation at Cotopaxi and the mapping of the related hazard are elements of considerable importance.

In this work, we concentrate on lahar hazard assessment in the Río Cutuchi system, which conveys all the main drainages of west and south of the Cotopaxi cone (Fig. 1). The Cutuchi valley hosts several human settlements, most of which lie on recent lahar deposit terraces, only a few meters above the present river bed. Further south, the Río Cutuchi crosses the large urban settlement of Latacunga (43 km SE of the volcano, Fig. 1), with a population of 52,000 inhabitants. Its path is generally parallel to the Pan American Highway, the major state road connecting the country from north to south. Many small-scale lahars have followed this drainage in the past (< 100 million m3), as well as some large-scale historical flows that severely impacted the population.

We present lahar simulations with different starting volumes performed with a GIS-based semi-empirical model (LAHARZ; Iverson et al., 1998) in order to evaluate the inundating potential of Cotopaxi lahars and to assess the inundation hazard in the southern part of the volcano towards the city of Latacunga. The manuscript is arranged with a section (Section 2) in which we briefly describe the geological data relevant to this study (recent Cotopaxi activity, lahar deposits, lahar triggering mechanisms, and the factors which control lahar volume). In Section 3 we introduce and discuss lahar modeling approaches and strategies (limitations, model used for simulations); used input parameters and results are presented in 4 Input parameters used for lahar modeling, 5 Results; and finally, we conclude with a discussion of the results and their implications on lahar hazard.

Section snippets

Physiography of Cotopaxi volcano

Cotopaxi is one of the highest active volcanoes of the world: its perfect ice-capped, 2200 m-high cone reaches an elevation of 5897 m above sea level with a basal diameter of 22 km. The volcano is located 60 km south of Quito, the capital of Ecuador, and it is surrounded by villages, national lines of communication and other infrastructure (Fig. 1). Its steep flanks (30°–35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent

Modeling procedures

Lahar modeling has been a challenge to date, and the available modeling approaches are unable to cope with the large range of dynamical behavior that characterize lahars. Uncertainties in the output of numerical modeling can be partially reduced if input parameters (e.g. lahar volumes or sedimentological features of lahar deposits) are appropriately derived from the geological record (Fagents and Baloga, 2005, Darnell et al., 2013), but quantitative data and direct measurements of

Input parameters used for lahar modeling

In order to run our simulations we used a geo-referenced digital elevation model (Shuttle Radar Topography Mission—SRTM) with a spatial resolution of 30 m and absolute and relative (90% confidence) vertical accuracies of ± 16 and ± 6 m, respectively (Rabus et al., 2003). Preliminary analyses on the DEM showed that along the Latacunga valley, the topographic domain has mostly concave shapes; as discussed by Canuti et al. (2002), this is a primary requirement for the model to work correctly, as it is

Results

Analysis of results shows that inundated areas produced by LAHARZ match the results of Mothes et al. (2004) and Mothes (2006) for an event of similar initial volume (Fig. 7). Only in few cases we did obtain slightly wider areas, in particular in the flat area of Río Cutuchi and in the sector where Río Cutuchi and Río Saquìmala merge together. In the proximity of Latacunga, in particular, inundated areas have the same lateral extent (~ 1500 m) as that proposed by Mothes et al. (2004) and Mothes

Discussion

Lahar hazard assessment requires the probabilistic evaluation of lahar inundation at any site situated close to river beds. This probability results from the combination of two independent and complementary factors: i) given a range of different scenarios based on past event history, the scale and probability of occurrence of these different scenarios must be assessed; ii) for each expected scenario, the extent of inundated area is estimated from simulation of the lahar flow path.

Previous

Conclusions

Lahar simulations were performed in this work to predict inundation areas in the southern part of Cotopaxi volcano towards the high-urbanized area of Latacunga. Two different scenarios were investigated: a first simulation (α, 120 million m3) which portrays a scenario similar to the last eruptive event occurred in 1877, highlighted that the inundated zone is consistent with the maps proposed by Mothes et al. (2004) and Mothes (2006). A second simulation (β, 360 million m3) generated flooded areas

Acknowledgments

M. Pistolesi and M. Rosi were supported by a PRIN–MIUR (Progetti di Ricerca di Interesse Nazionale–Ministero dell'Istruzione, dell'Università e della Ricerca) 2005 grant (scientific principal investigator M. Rosi) and R. Cioni by a grant provided by Regione Autonoma Sardegna (Italy). The manuscript was greatly improved after the invaluable comments by V. Manville and thanks to the suggestions of the reviewers K. Németh and M. Bisson. Andy Plater is acknowledged for editorial handling. The

References (78)

  • T.C. Pierson et al.

    Perturbation and melting of snow and ice by the 13 November 1985 eruption of Nevado del Ruiz, Colombia, and consequent mobilization, flow and deposition of lahars

    J. Volcanol. Geotherm. Res.

    (1990)
  • B. Rabus et al.

    The shuttle radar topography mission—a new class of digital elevation models acquired by spaceborne radar

    ISPRS J. Photogramm. Remote Sens.

    (2003)
  • M.F. Sheridan et al.

    Evaluating Titan2D mass-flow model using the 1963 Little Tahoma Peak avalanches, Mount Rainier, Washington

    J. Volcanol. Geotherm. Res.

    (2005)
  • B. Voight

    The 1985 Nevado del Ruiz volcano catastrophe: anatomy and retrospection

    J. Volcanol. Geotherm. Res.

    (1990)
  • R. Williams et al.

    Evaluation of the Titan2D two-phase flow model using an actual event: case study of the 2005 Vazcún valley lahar

    J. Volcanol. Geotherm. Res.

    (2008)
  • C. Witham

    Volcanic disasters and incidents: a new database

    J. Volcanol. Geotherm. Res.

    (2005)
  • N. Wood et al.

    Variations in population exposure and sensitivity to lahar hazards from Mount Rainier, Washington

    J. Volcanol. Geotherm. Res.

    (2009)
  • E. Aguilera et al.

    Risk from Lahars in the Northern valleys of Cotopaxi volcano (Ecuador)

    Nat. Hazards

    (2004)
  • Arboleda, R.A., Martinez, M. 1996. Lahars in the Pasig–Potrero River System. In: Fire and mud: eruptions and lahars of...
  • F. Barberi et al.

    Reconstruction and numerical simulation of the lahar of the 1877 eruption of Cotopaxi volcano (Ecuador)

    Acta Vulcanol.

    (1992)
  • M.A. Bornas et al.

    Caldera-rim breach and lahar from Mt. Pinatubo, Philippines: natural breaching and resulting lahar

  • B. Cáceres

    Evaluación reciente del área del casquete glaciar del volcán Cotopaxi mediante la utilización de fotogrametría digital

  • J.L. Carrivick et al.

    A fluid dynamics approach to modelling the 18th March 2007 lahar at Mt. Ruapehu, New Zealand

    Bull. Volcanol.

    (2009)
  • A.R. Darnell et al.

    Developing a simplified geographical information system approach to dilute lahar modelling for rapid hazard assessment

    Bull. Volcanol.

    (2013)
  • G. Delaite et al.

    A comparison of TITAN2D and LAHARZ simulated debris flow hazards at El Misti Volcano, southern Peru

    Geophys. Res. Abstr.

    (2004)
  • Delft Hydraulics

    Download Delft3D user manuals

  • M. Hall

    The 1985 Nevado del Ruiz eruption—scientific, social, and governmental response and interaction before the event

  • M. Hall et al.

    The rhyolitic–andesitic eruptive history of Cotopaxi volcano, Ecuador

    Bull. Volcanol.

    (2008)
  • Hall M., von Hillebrandt C., 1988a. Mapa de los Peligros Volcánicos Po-tenciales Asociados con el Volcán Cotopaxi, Zona...
  • Hall M. and von Hillebrandt C., 1988b. Mapa de los Peligros Volcánicos Potenciales Asociados con el Volcán Cotopaxi,...
  • Hall, M., Mothes, P., Samaniego, P., Yepes, H., Andrade, D., 2004. Mapa regional de los peligros volcánicos potenciales...
  • L. Hradecka et al.

    La Exploración Geológica de Volcán Cotopaxi en el Ecuador

    (1974)
  • INEC—Instituto Nacional de Estadistica y Censos
  • R.M. Iverson et al.

    Objective delineation of lahar-inundation hazard zones

    Geol. Soc. Am. Bull.

    (1998)
  • E. Jordan

    Die Vergletscherung Des Cotopaxi-Ecuador

    Z. Gletscherk. Glazialgeol.

    (1983)
  • F. Lavigne

    Lahar hazard micro-zonation and risk assessment in Yogyakarta city, Indonesia

    GeoJournal

    (1999)
  • J.J. Major et al.

    Snow and ice perturbation during historical volcanic eruptions and the formation of lahars and floods

    Bull. Volcanol.

    (1989)
  • M.C. Malin et al.

    Computer-assisted mapping of pyroclastic surges

    Science

    (1982)
  • V. Manville et al.

    Break-out lahar from New Zealand's Crater Lake

    EOS Trans. AGU

    (2007)
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