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Shaded relief map of Cotopaxi volcano and surrounding areas with main drainage systems and locations indicated in the text. The main geographic locations are shown in the bottom inset. The black box indicates the quarry site. Black striped area refers to the zone of intense farming and cultivation. In the upper inset, Cotopaxi volcano seen from the north. In the foreground the Limpiopungo plain, with blocks carried by recent lahars. 

Shaded relief map of Cotopaxi volcano and surrounding areas with main drainage systems and locations indicated in the text. The main geographic locations are shown in the bottom inset. The black box indicates the quarry site. Black striped area refers to the zone of intense farming and cultivation. In the upper inset, Cotopaxi volcano seen from the north. In the foreground the Limpiopungo plain, with blocks carried by recent lahars. 

Contexts in source publication

Context 1
... 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 ...
Context 2
... 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 (b 100 million m 3 ), as well as some large-scale historical flows that severely impacted the ...
Context 3
... is one of the highest active volcanoes of the world: its per- fect 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 vil- lages, 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 of historic eruptions. The volcano has three main drainage systems ( Fig. 2): 1) to the north is the Pita-Guayallabamba river system that flows through the Los Chillos and Tumbaco ...
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... (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and flow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses ( Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an ...
Context 5
... Cutuchi is the main river southwest of Cotopaxi. Its headwaters flow to the south of Rumiñahui (Fig. 1), a deeply eroded extinct volcano situated to the west of Cotopaxi, and its tributaries cover the entire western sector of Cotopaxi. Stratigraphic studies along the Río Cutuchi valleys revealed an impressive sequence of lahar deposits Pistolesi et al., 2013). Historical accounts also describe that since the Spanish Conquest (XVI ...
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... to the preservation of tephra beds intercalated between the lahar deposits, and these were directly related to their generating explosive eruptions (Fig. 3). Debris flow deposits were also informally grouped into three main categories (Types A, B and C) by combining sedimentological data obtained from a large quarried area along the Río Cutuchi (Fig. 1). These three categories of deposits largely vary in terms of dispersal, thickness, average and maximum size of transported blocks increasing from A to C, and were related to lahars with different sizes and trigger mechanisms ( Pistolesi et al., 2013) (Fig. 4A, B, C). The stratigraphy of debris flow deposits in the Cutuchi quarries ( ...
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... the Río Cutuchi (Fig. 2). In simulation α, for each drainage system, different volumes were used and then recombined in order to obtain a volume comprised between 100 and 150 million m 3 (Fig. 5A, Table 1). A final lahar volume of 120 million m 3 , corre- sponding to the sum of Río Cutuchi (60 million m 3 ), Río Saquìmala (30 million m 3 , with 90 million m 3 where Cutuchi and Saquìmala join together) and Río Barrancas-Alaquez (30 million m 3 ) contributions, was finally chosen (Figs. 5B, 7). The final target volume (120 million m 3 ) ...
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... inundation depths along the 73-km stretch of the Río Cutuchi are reported in Fig. 10: along the first 10 km, apparent flow depths range between 10 and 50 m for simulation α, consistent with the range (12-33 m) derived from historical data and the computed maximum flow depth for the 1877 lahar ( Barberi et al., 1992). Apparent flow depths for simulation β resulted between 10 and 65 m, with a maximum difference of 18 m ...
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... a-b (6700 m-long) drawn in proximity to Latacunga (Figs. 8, 11) shows that the apparent height of the flow for an event of 360 million m 3 is double (35 m vs. 18 m) with respect to the 120 million m 3 case. In simulation β, the inundated area reaches the elevated areas on the east side of the river, where the main part of the city is located. The value obtained for simulation α is consistent with ...
Context 10
... on the east side of the river, where the main part of the city is located. The value obtained for simulation α is consistent with the 10 m flow depth for a 90 million m 3 lahar obtained by Barberi et al. (1992). The majority of the city of Latacunga could be damaged also in this case: most of the major structures, facilities including schools, (Fig. 10). Pierson et al., 1990), mainly because the bulking rate is considered proportional to the power dissipated by the fluid (Finnie, 1972). By using the same regression line obtained by Aguilera et al. (2004), we plot our data to calculate the theoretical bulking values in two reaches of Río Cutuchi (Fig. 12). The first is a 3 km-long ...
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... structures, facilities including schools, (Fig. 10). Pierson et al., 1990), mainly because the bulking rate is considered proportional to the power dissipated by the fluid (Finnie, 1972). By using the same regression line obtained by Aguilera et al. (2004), we plot our data to calculate the theoretical bulking values in two reaches of Río Cutuchi (Fig. 12). The first is a 3 km-long section (θ = 1.5°), 10 km from the onset of the simulation. We used apparent peak flow depths of simulations α and β (10 and 16 m, respectively) which corre- spond to Sx * h of 0.26 m and 0.41 m, respectively. These convert to bulking values of 190 and 300 m 3 /s, corresponding to total bulking of 6 × 10 5 and ...
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... and β (10 and 16 m, respectively) which corre- spond to Sx * h of 0.26 m and 0.41 m, respectively. These convert to bulking values of 190 and 300 m 3 /s, corresponding to total bulking of 6 × 10 5 and 9 × 10 5 m 3 calculated for 3 km of the section. In the area of Latacunga, we used a 10 km-long section (θ = 0.6°) with flow depths of 18 and 35 m (Figs. 10, 11), corresponding to Sx * h of 0.20 and 0.38, respectively. These convert to bulking values of 140 and 280 m 3 /m, and to total bulking values of 1.4 × 10 6 and 2.8 × 10 6 m 3 , respectively, for the 10 km-long section. If we assume an average bulking value, and we use it for the total length of 39 km of the simulation up to Latacunga, ...
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... high-concentration, sediment-loaded fl ows 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, un- consolidated debris; and (iii) steep slopes (Vallance, 2000). Due to water incorporation and volume increase, lahars can easily over fl ow 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 fl ows but also hyperconcentrated mud fl ows (Smith and Lowe, 1991). Although the term has sometimes been used to refer to the deposits of such fl ows, 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 fl ows occur daily on the fl anks 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 fl ow. 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 docu- mented 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 terri fi c 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 fl ow 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, 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 con- siderable 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 ( b 100 million m 3 ), as well as some large-scale historical fl ows 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 brie fl y 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 Sections 4 and 5; and fi nally, we conclude with a discussion of the results and their implications on lahar hazard. Cotopaxi is one of the highest active volcanoes of the world: its per- fect 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 fl anks (30° – 35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent of historic eruptions. The volcano has three main drainage systems (Fig. 2): 1) to the north is the Pita – Guayallabamba river system that fl ows through the Los Chillos and Tumbaco valleys, both lying east of Quito and 400 m lower in elevation; 2) to the east is the Tambo – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity at Cotopaxi volcano (Molina et al., 2006) with an increase of long-period (LP) seismic events accompanied by very long-period (VLP) events occurring directly under the volcano; fumarolic activity at the summit and a thermal anomaly suggesting injection of new magma ...
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... or volcanic debris fl ows, consist of high-concentration, sediment-loaded fl ows 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, un- consolidated debris; and (iii) steep slopes (Vallance, 2000). Due to water incorporation and volume increase, lahars can easily over fl ow 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 fl ows but also hyperconcentrated mud fl ows (Smith and Lowe, 1991). Although the term has sometimes been used to refer to the deposits of such fl ows, 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 fl ows occur daily on the fl anks 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 fl ow. 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 docu- mented 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 terri fi c 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 fl ow 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, 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 con- siderable 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 ( b 100 million m 3 ), as well as some large-scale historical fl ows 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 brie fl y 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 Sections 4 and 5; and fi nally, we conclude with a discussion of the results and their implications on lahar hazard. Cotopaxi is one of the highest active volcanoes of the world: its per- fect 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 fl anks (30° – 35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent of historic eruptions. The volcano has three main drainage systems (Fig. 2): 1) to the north is the Pita – Guayallabamba river system that fl ows through the Los Chillos and Tumbaco valleys, both lying east of Quito and 400 m lower in elevation; 2) to the east is the Tambo – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity ...
Context 15
... anks 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 fl ow. 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 docu- mented 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 terri fi c 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 fl ow 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, 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 con- siderable 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 ( b 100 million m 3 ), as well as some large-scale historical fl ows 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 brie fl y 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 Sections 4 and 5; and fi nally, we conclude with a discussion of the results and their implications on lahar hazard. Cotopaxi is one of the highest active volcanoes of the world: its per- fect 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 fl anks (30° – 35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent of historic eruptions. The volcano has three main drainage systems (Fig. 2): 1) to the north is the Pita – Guayallabamba river system that fl ows through the Los Chillos and Tumbaco valleys, both lying east of Quito and 400 m lower in elevation; 2) to the east is the Tambo – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity at Cotopaxi volcano (Molina et al., 2006) with an increase of long-period (LP) seismic events accompanied by very long-period (VLP) events occurring directly under the volcano; fumarolic activity at the summit and a thermal anomaly suggesting injection of new magma (Ramon et al., 2006; Rivero et al., 2006). This evidence and the general behavior of the volcano as portrayed by its geological record (Barberi et al., 1995; Hall and Mothes, 2008a; Pistolesi et al., 2011) make the problem of lahar generation particularly signi fi cant. Río Cutuchi is the main river southwest of Cotopaxi. Its headwaters fl ow to the south of Rumiñahui (Fig. 1), a deeply eroded extinct volcano situated to the west of Cotopaxi, and its tributaries cover the entire western sector of Cotopaxi. Stratigraphic studies along the Río Cutuchi valleys revealed an impressive sequence of lahar deposits (Mothes et al., 2004; Pistolesi et al., 2013). Historical accounts also describe that since the Spanish Conquest (XVI century), most of the lahars produced by Cotopaxi fl owed towards the western and southwest- ern sectors of the volcano along the Río Cutuchi (Mothes et al., 2004; Figs. 2, 3), as reported by Sodiro (1877, p. 4): ( ... ) (in 1742) “ a terrible inundation in near regions destroyed bridges and farms, killing people and livestock ( ... ), and (in 1744) a huge fl ood rapidly arrived in Latacunga which, after the destruction of whatever en- countered along its way, invaded the center of the city, destroying houses ( ... ) ” . Based on the recognition of thin fallout tephra beds within the lahar sequence, Pistolesi (2008) and Pistolesi et al. (2013) proposed a stratigraphic reconstruction of post-XII century debris fl ows and compared their scale and dynamics (Fig. 4A). Well-constrained 14 C ...
Context 16
... 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 docu- mented 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 terri fi c 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 fl ow 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, 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 con- siderable 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 ( b 100 million m 3 ), as well as some large-scale historical fl ows 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 brie fl y 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 Sections 4 and 5; and fi nally, we conclude with a discussion of the results and their implications on lahar hazard. Cotopaxi is one of the highest active volcanoes of the world: its per- fect 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 fl anks (30° – 35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent of historic eruptions. The volcano has three main drainage systems (Fig. 2): 1) to the north is the Pita – Guayallabamba river system that fl ows through the Los Chillos and Tumbaco valleys, both lying east of Quito and 400 m lower in elevation; 2) to the east is the Tambo – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity at Cotopaxi volcano (Molina et al., 2006) with an increase of long-period (LP) seismic events accompanied by very long-period (VLP) events occurring directly under the volcano; fumarolic activity at the summit and a thermal anomaly suggesting injection of new magma (Ramon et al., 2006; Rivero et al., 2006). This evidence and the general behavior of the volcano as portrayed by its geological record (Barberi et al., 1995; Hall and Mothes, 2008a; Pistolesi et al., 2011) make the problem of lahar generation particularly signi fi cant. Río Cutuchi is the main river southwest of Cotopaxi. Its headwaters fl ow to the south of Rumiñahui (Fig. 1), a deeply eroded extinct volcano situated to the west of Cotopaxi, and its tributaries cover the entire western sector of Cotopaxi. Stratigraphic studies along the Río Cutuchi valleys revealed an impressive sequence of lahar deposits (Mothes et al., 2004; Pistolesi et al., 2013). Historical accounts also describe that since the Spanish Conquest (XVI century), most of the lahars produced by Cotopaxi fl owed towards the western and southwest- ern sectors of the volcano along the Río Cutuchi (Mothes et al., 2004; Figs. 2, 3), as reported by Sodiro (1877, p. 4): ( ... ) (in 1742) “ a terrible inundation in near regions destroyed bridges and farms, killing people and livestock ( ... ), and (in 1744) a huge fl ood rapidly arrived in Latacunga which, after the destruction of whatever en- countered along its way, invaded the center of the city, destroying houses ( ... ) ” . Based on the recognition of thin fallout tephra beds within the lahar sequence, Pistolesi (2008) and Pistolesi et al. (2013) proposed a stratigraphic reconstruction of post-XII century debris fl ows and compared their scale and dynamics (Fig. 4A). Well-constrained 14 C calendar ages performed on soils and charred grass were assigned to most lahar deposits thanks to the preservation of tephra beds intercalated between the lahar deposits, and these were directly related to their generating explosive eruptions (Fig. 3). Debris fl ow deposits were also informally grouped into three main categories (Types A, B and C) by combining sedimentological data obtained from a large quarried area along the Río Cutuchi (Fig. 1). These three categories of deposits largely vary in terms of dispersal, thickness, average and maximum size of transported blocks increasing from A to C, and were related to lahars with different sizes and trigger mechanisms (Pistolesi et al., 2013) (Fig. 4A, B, C). The stratigraphy of debris fl ow deposits in the Cutuchi quarries (Fig. 3) clearly highlights that the period between 1200 and 1500 AD is characterized by lahar events of large ( N 500 million m 3 ) scale, which carried meter-sized boulders and left deposits more ...
Context 17
... 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 brie fl y 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 Sections 4 and 5; and fi nally, we conclude with a discussion of the results and their implications on lahar hazard. Cotopaxi is one of the highest active volcanoes of the world: its per- fect 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 fl anks (30° – 35°) culminate in a crater hosting a tephra cone (Hradecka et al., 1974), which in turn harbors a smaller crater, the active vent of historic eruptions. The volcano has three main drainage systems (Fig. 2): 1) to the north is the Pita – Guayallabamba river system that fl ows through the Los Chillos and Tumbaco valleys, both lying east of Quito and 400 m lower in elevation; 2) to the east is the Tambo – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity at Cotopaxi volcano (Molina et al., 2006) with an increase of long-period (LP) seismic events accompanied by very long-period (VLP) events occurring directly under the volcano; fumarolic activity at the summit and a thermal anomaly suggesting injection of new magma (Ramon et al., 2006; Rivero et al., 2006). This evidence and the general behavior of the volcano as portrayed by its geological record (Barberi et al., 1995; Hall and Mothes, 2008a; Pistolesi et al., 2011) make the problem of lahar generation particularly signi fi cant. Río Cutuchi is the main river southwest of Cotopaxi. Its headwaters fl ow to the south of Rumiñahui (Fig. 1), a deeply eroded extinct volcano situated to the west of Cotopaxi, and its tributaries cover the entire western sector of Cotopaxi. Stratigraphic studies along the Río Cutuchi valleys revealed an impressive sequence of lahar deposits (Mothes et al., 2004; Pistolesi et al., 2013). Historical accounts also describe that since the Spanish Conquest (XVI century), most of the lahars produced by Cotopaxi fl owed towards the western and southwest- ern sectors of the volcano along the Río Cutuchi (Mothes et al., 2004; Figs. 2, 3), as reported by Sodiro (1877, p. 4): ( ... ) (in 1742) “ a terrible inundation in near regions destroyed bridges and farms, killing people and livestock ( ... ), and (in 1744) a huge fl ood rapidly arrived in Latacunga which, after the destruction of whatever en- countered along its way, invaded the center of the city, destroying houses ( ... ) ” . Based on the recognition of thin fallout tephra beds within the lahar sequence, Pistolesi (2008) and Pistolesi et al. (2013) proposed a stratigraphic reconstruction of post-XII century debris fl ows and compared their scale and dynamics (Fig. 4A). Well-constrained 14 C calendar ages performed on soils and charred grass were assigned to most lahar deposits thanks to the preservation of tephra beds intercalated between the lahar deposits, and these were directly related to their generating explosive eruptions (Fig. 3). Debris fl ow deposits were also informally grouped into three main categories (Types A, B and C) by combining sedimentological data obtained from a large quarried area along the Río Cutuchi (Fig. 1). These three categories of deposits largely vary in terms of dispersal, thickness, average and maximum size of transported blocks increasing from A to C, and were related to lahars with different sizes and trigger mechanisms (Pistolesi et al., 2013) (Fig. 4A, B, C). The stratigraphy of debris fl ow deposits in the Cutuchi quarries (Fig. 3) clearly highlights that the period between 1200 and 1500 AD is characterized by lahar events of large ( N 500 million m 3 ) scale, which carried meter-sized boulders and left deposits more than 20 m thick (Figs. 3, 4B, C). Conversely, lahars of the period of activity between 1700 and 1877 (the last eruptive event) show a variable but lower scale in terms of distribution, thickness and size of transported blocks; within this period, the 1877 lahar deposits are smaller than those related to the XVIII century activity. The 1877 eruption (a sub-Plinian event of magnitude VEI 4; Hall and Mothes, 2008a; Pistolesi et al., 2011), in particular, triggered large fl oods along all the main drainages. After exiting the glacier, these water-dominated fl ows mixed with pyroclastic and ice blocks, causing intense erosion and gullying, and rapidly evolved into debris fl ows (Aguilera et al., 2004). Typical valleys along the volcano's fl anks are represented by steep ( N 20°), narrow canyons laterally con- fi ned by vertical stacks of lavas and pyroclastic sequences. The peak discharge of 1877 fl ows was estimated between 50,000 and 60,000 m 3 s − 1 , with velocities in excess of 20 m s − 1 (Mothes et al., 2004). Lahars descending south of Cotopaxi initially fl owed along three main paths (Río Cutuchi, Río Saquìmala and Río Barrancas – Alaquez) and merged at a distance of about 24 km from the crater. The morphology at the foot of the cone rapidly changes into fl at ( b 5°), wide valleys separated by gentle slopes mostly covered by grass, where part of the coarse solid material has been commonly discharged by past debris fl ows. Lahar fl ow depths in the upper Cutuchi course have been estimated to be up to 20 m (Barberi et al., 1992; Mothes et al., 2004), increasing south of Latacunga where the valley gets narrower. Mothes et al. (2004) calculated a total volume of 100 million m 3 for the 1877 lahar drained from the canyons with different discharges and dropping into the Latacunga valley. Barberi et al. (1992), applying equal discharges in all major ‘ quebradas ’ , estimated a volume of 150 million m 3 . In the area of Latacunga, the lahar sequence is today exposed as a stack of debris fl ow deposits in gravel quarries and terrace cliffs. Although too far ( ≈ 40 km) from the volcano to preserve recognizable primary tephra fallout deposits and out of the main dispersal axis of historical Cotopaxi eruptions, the regionally-dispersed Quilotoa ash fall is visible within the sequence (Fig. 4D), separating pre- and post-1150 AD lahar deposits. The role of pyroclastic fl ows in generating rapid melting of snow and ice has been largely discussed in the volcanological literature (Major and Newhall, 1989; Pierson et al., 1990; Zernack et al., 2011). At Cotopaxi, in particular, ice scouring and melting during scoria fl ow events have been observed and described by chroniclers: during the 1877 eruption (and presumably during the 1766 – 68 and 1853 eruptions as well), “ a dark foam-like cloud boiled over the crater, ...
Context 18
... – Tamboyacu river system, which forms part of the Río Napo and fl ows through the sparsely populated Amazonian lowlands; and 3) to the west – southwest, the drainage includes 2 main ‘ quebradas ’ (small, steep-sided valleys): the Barrancas and Saquìmala, whose streams eventually join with the Río Cutuchi and fl ow through the center of the Latacunga valley. The city of Latacunga and settlements along the entire valley grew rapidly in recent decades within the city and along the river, in particular with greenhouses for growing roses (Fig. 1), resulting presently in a very densely populated area with high industrial investment where houses, factories, hospitals, schools, the Pan American Highway and other infrastructure have been built on top of lahar deposits of less than 1000 years old. The population in Latacunga was estimated at 63,800 inhabitants in 2012, living in an area of about 10 km 2 with a population density of 6.4/km 2 (INEC — Instituto Nacional de Estadistica y Censos, 2012); the previous census of 2001 estimated the population at 52,000, with an increase of more than 20% in the past 10 years. The recent eruptive activity of Cotopaxi consists of Plinian outbursts of VEI 3 – 4 (at least 20 episodes in the last 2000 years; Barberi et al., 1995; Pistolesi et al., 2011), with associated lava fl ows, long-lasting ash eruptions and minor Strombolian activity. Pistolesi et al. (2011) upgraded the information made available by previous studies (Barberi et al., 1995; Mothes et al., 2004; Hall and Mothes, 2008a) and recog- nized 21 continuous tephra beds subdivided in three eruptive periods, from the emplacement of the regional tephra marker of the Quilotoa volcano ash (1150 AD; Hall and Mothes, 2008b) to the present (Fig. 3). The fi rst eruptive period (1150 to 1534) was characterized by two mid-intensity explosive eruptions (layers B L and S W , Fig. 3), apparently separated and followed by quiescent periods a few centuries long. Activity of the second period coincided with two Plinian eruptions in 1742 – 44 (layer M T ) and in 1766 – 68 (layer M B ). The latter, in particular, was associated with the formation of scoria fl ows, which were dispersed over large areas on the northern side of the cone. After the M B eruption, activity at Cotopaxi passed into a period of long- lasting, moderate-intensity ash generation punctuated by the occurrence of low-magnitude, short-lived sub-Plinian eruptions (P D , P L and P E; third period, Fig. 3). ‘ Boiling-over activity ’ and generation of scoria fl ow deposits were always associated with these events. Tephra deposits of the last large eruptive event of Cotopaxi, which occurred in 1877, are recorded by the P E layer. January 2001 saw increased level of activity at Cotopaxi volcano (Molina et al., 2006) with an increase of long-period (LP) seismic events accompanied by very long-period (VLP) events occurring directly under the volcano; fumarolic activity at the summit and a thermal anomaly suggesting injection of new magma (Ramon et al., 2006; Rivero et al., 2006). This evidence and the general behavior of the volcano as portrayed by its geological record (Barberi et al., 1995; Hall and Mothes, 2008a; Pistolesi et al., 2011) make the problem of lahar generation particularly signi fi cant. Río Cutuchi is the main river southwest of Cotopaxi. Its headwaters fl ow to the south of Rumiñahui (Fig. 1), a deeply eroded extinct volcano situated to the west of Cotopaxi, and its tributaries cover the entire western sector of Cotopaxi. Stratigraphic studies along the Río Cutuchi valleys revealed an impressive sequence of lahar deposits (Mothes et al., 2004; Pistolesi et al., 2013). Historical accounts also describe that since the Spanish Conquest (XVI century), most of the lahars produced by Cotopaxi fl owed towards the western and southwest- ern sectors of the volcano along the Río Cutuchi (Mothes et al., 2004; Figs. 2, 3), as reported by Sodiro (1877, p. 4): ( ... ) (in 1742) “ a terrible inundation in near regions destroyed bridges and farms, killing people and livestock ( ... ), and (in 1744) a huge fl ood rapidly arrived in Latacunga which, after the destruction of whatever en- countered along its way, invaded the center of the city, destroying houses ( ... ) ” . Based on the recognition of thin fallout tephra beds within the lahar sequence, Pistolesi (2008) and Pistolesi et al. (2013) proposed a stratigraphic reconstruction of post-XII century debris fl ows and compared their scale and dynamics (Fig. 4A). Well-constrained 14 C calendar ages performed on soils and charred grass were assigned to most lahar deposits thanks to the preservation of tephra beds intercalated between the lahar deposits, and these were directly related to their generating explosive eruptions (Fig. 3). Debris fl ow deposits were also informally grouped into three main categories (Types A, B and C) by combining sedimentological data obtained from a large quarried area along the Río Cutuchi (Fig. 1). These three categories of deposits largely vary in terms of dispersal, thickness, average and maximum size of transported blocks increasing from A to C, and were related to lahars with different sizes and trigger mechanisms (Pistolesi et al., 2013) (Fig. 4A, B, C). The stratigraphy of debris fl ow deposits in the Cutuchi quarries (Fig. 3) clearly highlights that the period between 1200 and 1500 AD is characterized by lahar events of large ( N 500 million m 3 ) scale, which carried meter-sized boulders and left deposits more than 20 m thick (Figs. 3, 4B, C). Conversely, lahars of the period of activity between 1700 and 1877 (the last eruptive event) show a variable but lower scale in terms of distribution, thickness and size of transported blocks; within this period, the 1877 lahar deposits are smaller than those related to the XVIII century activity. The 1877 eruption (a sub-Plinian event of magnitude VEI 4; Hall and Mothes, 2008a; Pistolesi et al., 2011), in particular, triggered large fl oods along all the main drainages. After exiting the glacier, these water-dominated fl ows mixed with pyroclastic and ice blocks, causing intense erosion and gullying, and rapidly evolved into debris fl ows (Aguilera et al., 2004). Typical valleys along the volcano's fl anks are represented by steep ( N 20°), narrow canyons laterally con- fi ned by vertical stacks of lavas and pyroclastic sequences. The peak discharge of 1877 fl ows was estimated between 50,000 and 60,000 m 3 s − 1 , with velocities in excess of 20 m s − 1 (Mothes et al., 2004). Lahars descending south of Cotopaxi initially fl owed along three main paths (Río Cutuchi, Río Saquìmala and Río Barrancas – Alaquez) and merged at a distance of about 24 km from the crater. The morphology at the foot of the cone rapidly changes into fl at ( b 5°), wide valleys separated by gentle slopes mostly covered by grass, where part of the coarse solid material has been commonly discharged by past debris fl ows. Lahar fl ow depths in the upper Cutuchi course have been estimated to be up to 20 m (Barberi et al., 1992; Mothes et al., 2004), increasing south of Latacunga where the valley gets narrower. Mothes et al. (2004) calculated a total volume of 100 million m 3 for the 1877 lahar drained from the canyons with different discharges and dropping into the Latacunga valley. Barberi et al. (1992), applying equal discharges in all major ‘ quebradas ’ , estimated a volume of 150 million m 3 . In the area of Latacunga, the lahar sequence is today exposed as a stack of debris fl ow deposits in gravel quarries and terrace cliffs. Although too far ( ≈ 40 km) from the volcano to preserve recognizable primary tephra fallout deposits and out of the main dispersal axis of historical Cotopaxi eruptions, the regionally-dispersed Quilotoa ash fall is visible within the sequence (Fig. 4D), separating pre- and post-1150 AD lahar deposits. The role of pyroclastic fl ows in generating rapid melting of snow and ice has been largely discussed in the volcanological literature (Major and Newhall, 1989; Pierson et al., 1990; Zernack et al., 2011). At Cotopaxi, in particular, ice scouring and melting during scoria fl ow events have been observed and described by chroniclers: during the 1877 eruption (and presumably during the 1766 – 68 and 1853 eruptions as well), “ a dark foam-like cloud boiled over the crater, much like the boiling over of a pot of cooking rice ” , spilling through the sides where the crater rim was lower. Emplacement of these scoria fl ow lobes took place immediately after an “ ash and lapilli rain ” (Wolf, 1878, p. 20). As soon as the lobate pyroclastic cloud overrode the glacier, lahars were triggered (Sodiro, 1877; Wolf, 1878). In most of the cases scoria fl ows and lahars descended the volcano fl anks virtually following the same bottom valley pathways. Pistolesi et al. (2013) suggested three different triggering processes for Cotopaxi lahars, which correspond to the different types of lahar deposits identi fi ed for events occurring in the last 800 years of eruptive activity: 1) Pyroclastic surge events with limited dispersal (run-out slightly be- yond the glacier snout) that can sweep over the entire glacier but with limited snow/ice melting. These pyroclastic density currents generated matrix-rich, block-poor and (almost) valley-con fi ned lahar deposits (Type A deposits). 2) Erosive, pyroclastic scoria- fl ow lobes able to cut deep canyons into the ice cap, leaving 40 – 50 m-high cliffs of exposed ice (Wolf, 1878). Lahars associated with these scoria fl ows are block-rich and produce widespread deposits. The presence of the abundant scoria bombs demonstrates the tight relationship between scoria- fl ows and lahar events. The volume of ice melted during these events is signi fi cant, although it can be related to the localized erosion of the deep ice canyons described above (Types A and B deposits). 3) Lithic- and scoria-rich, highly erosive, radially ...

Citations

... Then, the future development trend of the slope is qualitatively discriminated according to the surface deformation law, which is represented by the slope development rate. Finally, the two are combined for comprehensive analysis to calculate the damage probability of the slope [35][36][37][38][39]. In the first-class slope zone around the township area, the potential hazard degree under different rainfall conditions is predicted and analyzed one by one for landslide/debris flow that may cause disasters. ...
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Mountainous areas have become among the most developed areas of geological hazards due to special geological environmental conditions and intensive human engineering activities. Geological hazards are a main threat to urbanization, rural revitalization, and new rural construction in complex mountainous areas. It is of great strategic significance to conduct large-scale geological hazard investigation and risk assessment in urban areas, control the risk of geological hazards at the source and propose risk control measures. In this paper, we established the technical methods of geologic hazard risk assessment and control in complex mountain towns by taking Longlin Town in the mountainous region of Gansu Longnan, China as the study area, with the Quanjia bay debris flows and Panping Village landslides as the typical pilot investigation and assessment. The methods consist of six stages—risk identification, hazard disaster model investigation, risk analysis, vulnerability assessment, risk evaluation and risk management and control measures and proposals. On this basis, the results of geological hazards with different precipitation frequencies (5%, 2%, 1%) are presented. The results show that 75.23% of the regions remained at low risk levels; 24.38% of the regions increased a risk level with decreasing precipitation frequency, and 0.39% of the regions remained at extremely high risk levels under different precipitation frequency conditions. For the Quanjia bay debris flows and Panping Village landslides case, we discussed the geological hazards risk source control contents, management and control technologies, engineering and non-engineering measures of disaster prevention and control for urban disasters and specific disaster areas. This research can provide technical support and reference for disaster prevention and mitigation, and territorial spatial planning.
... The underground drinking water supplies analyzed are located in five different geological or lithological units (L1-L5). Hereby, L1 is represented by the Tarqui Volcanics of the Cisaran Formation, which includes intermediate to felsic volcaniclastic deposits, and intermediate lavas [60,61]; L2 is composed of distal facies Cotopaxi Volcanics, being intermediate, pri mary, reworked volcanoclastic deposits, debris avalanches, and lavas [62][63][64][65]; L3 are the Pisayambo Volcanics, being intermediate to felsic volcaniclastic deposits [66]; L4 is the Yunguilla Unit, which is composed of shales, calcareous and siliceous siltstones, as wel as sandstones, bioclastic limestones, and mafic volcanoclasts [67,68]; L5 is represented by the Peltetec unit, which is an ophiolitic mélange of serpentinites, basalts, and meta basalts [69][70][71]. Figure 1 illustrates the geological map of the study region with the location of the sampling points. ...
Article
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The activity concentrations of 222Rn were measured in 53 public water supplies of underground (50) and surface (3) origin, and the relation of such with five geological units where these supplies are located, in the central Ecuadorian Andes, was also explored. These units supply drinking water to 10 cities, located between the 1500 and 3120 m.a.s.l. The experimental setup consisted of the RAD7 radon detector and the RAD H2O degassing system. The 222Rn levels measured in groundwater ranged from 0.53 to 14.78 Bq/L while surface waters did not indicate detectable radon levels. The radon concentrations were below the parametric value of 100 Bq/L for water intended for human consumption, recommended by the European Atomic Energy Community (EURATOM) in its Directive 2013/51, and the alternative maximum contamination level (AMCL) of 150 Bq/L, proposed by the Environmental Protection Agency (EPA). The Pisayambo Volcanic unit, mapped as intermediate volcaniclastic to felsic deposits, presented a mean radon concentration higher than the other geological units and lithologies (9.58 ± 3.04 Bq/L). The Cunupogyo well (11.36 ± 0.48 Bq/L) presented a radon concentration more than 70% higher than the neighboring springs, which may be explained by its proximity to the Pallatanga geological fault. The maximum annual effective doses, by cities, due to the ingestion and inhalation of radon, ranged from 0.010 to 0.108 mSv and from 0.008 to 0.091 mSv, respectively; therefore, these waters do not represent a risk to the health of the population. In addition, a correlation was observed between the activity concentration of 222Rn and the activity concentration of the parent 226Ra in samples collected from some springs.
... This information is then integrated with numerical simulations to define the expected areas impacted by future eruptions (Connor et al., 2015). Numerical modeling and statistics-based volcanic hazard assessments have been performed for a large, growing number of volcanoes, including Vesuvius (Italy; Todesco et al., 2002;Esposti Ongaro et al., 2002Cioni et al., 2003;Macedonio et al., 2008Macedonio et al., , 2016Doronzo et al., 2022), Campi Flegrei caldera (Italy; Costa et al., 2009;Neri et al., 2015;Bevilacqua et al., 2016Bevilacqua et al., , 2017aBevilacqua et al., , 2022a, Etna (Italy; Barsotti et al., 2010;Del Negro et al., 2013), El Misti (Peru; Sandri et al., 2014), Long Valley volcanic region (USA, Bevilacqua et al., 2018;Rutarindwa et al., 2019), Cotopaxi (Ecuador; Pistolesi et al., 2014;Tadini et al., 2021aTadini et al., , 2022, Yucca Mountain (USA; Valentine et al., 2009), Mount Pelée (Martinique; Gueugneau et al., 2020) and El Hierro (Spain; Becerril et al., 2014), among others. ...
Article
We present a scenario-based, probabilistic hazard assessment for the San Salvador volcanic complex (SSVC), a volcanic field located in the vicinity of San Salvador that includes the El Boquerón stratovolcano and 25 monogenetic vents. We define a set of likely eruption scenarios for tephra fallout and pyroclastic density currents (PDCs). The eruption scenarios range from violent Strombolian eruptions with a significant uncertainty in source position to sub-Plinian and Plinian activity fed from the central cone. The adopted methodology is mainly based on numerical modeling using Tephra2 (adopting the software TephraProb) to study tephra fallout and the branching box model and the branching energy cone model (adopting the programs BoxMapProb 2.0 and ECMapProb 2.0) to describe inertial and frictional PDCs, respectively. Despite the dominant W-WSW-trending winds, numerical results show that Plinian eruptions at El Boquerón volcano are able to deposit thick tephra layers in the metropolitan area of San Salvador city, likely reaching mass loads of the order of 100 kg/m2 (conditional probability of 50%). The simulated sub-Plinian events highlight the seasonal influence of wind patterns. In fact, the conditional probability of significant tephra sedimentation in San Salvador city is strongly reduced when eruptions occur during the rainy season. Numerical modeling of violent Strombolian eruptions is performed considering uncertainty in vent position. Results show that the conditional probability of depositing tephra mass loads higher than 10 kg/m2 at a given point reaches a maximum value of ∼7% on the NW flank of the volcano, at about 8 km from the central crater. On the other hand, very low conditional probabilities (<1%) are obtained for San Salvador city for any relevant threshold (10 kg/m2 or more) of tephra mass load during violent Strombolian events. Regarding PDCs, results show that those produced during large-scale Plinian eruptions are able to invade significant areas of the volcano surroundings, including San Salvador city. PDCs generated from the partial collapse of a sub-Plinian eruption column exhibit maximum inundation probabilities on the N, W and S flanks of the volcano. Cerro El Picacho exerts a significant shield effect on the propagation of these PDCs, with low inundation probabilities for San Salvador city (<3%). Finally, coupling published vent opening probability maps and numerical modeling of small-scale PDCs yields maximum inundation probabilities on the NW flank of the volcano, reaching maximum conditional probabilities of the order of ∼10% and values of about 5% near the village of Nuevo Sitio del Niño.
... These deposits are then remobilized over time-or instantly -by rainfalls and transported further downstream forming lahars [6,7], where mixtures of blocks and sediment and water flow in a "fluid manner" in and from valleys on volcanoes [8,9]. Lahars can be triggered by a variety of processes, but it is dominated by rainfall-triggered lahars, which have been well-studied in South America at Colima Volcano [10] at Popocatepetl [11], or at Cotopaxi Volcano [12] for instance. In East Asia, Indonesia, the Philippines and Japan have provided numerous case studies as well: at Merapi Volcano in Indonesia [6,7,13], at Semeru Volcano in Indonesia [14,15], etc. ...
Conference Paper
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In the last decade, rainfall radar has been deployed at volcanoes like Mt. Merapi in Indo-nesia, and can even cover a whole country like in Japan, where the X-Rain (eXtended Radar Information network) product has been available for local research. However, the linkage between rain-gage data and radar spatial data (over a 250 m x 250 m grid) still presents discrepancies, and these challenges are particularly acute in regions of high local-topographic variations like at Mount Unzen in Japan. As the volcano is located at the Shimabara peninsula, it is surrounded by the sea, with a topography locally rising to 1,483 m. To improve the forecast and to better understand the triggering mechanisms of lahars (volcanic debris-flows) at Mount Unzen, quantifying the spatial distribution of rainfalls is essential, and first it is important understand how data taken locally by rain-gages relate to radar data spatially. Because empirical models have not been able to show any clear correlation , the present contribution has been developing a neural-network with two hidden layers that takes into account the rainfall per hour, the temperature and the wind speed and direction. The model takes a logistic activation function and the loss function is optimized using the Mean Squared Errors and the Mean Absolute Error. The choice of the activation function and the optimizer is the result of running several combinations of optimization functions with different activation functions. Once the best fit was chosen, the sigmoid with a SGD (Stochastic Gradient Descent) optimizer was chosen, and when training the model for 120 cycles, Shimabara station and the XRain data shows an error < 4 mm rainfall, while at the Unzen summit, even after 300 cycles, the validation error remained at 8 mm while the training loss was < 4mm. This shows that location specific functions might be necessary for each location, not only taking into account the weather data, but also the local topographic variability and the topographic position on slopes.
... Lahar is an Indonesian term for volcanic debris flows or mudflows consisting of a high concentration of sediment, ash deposit, or other volcanic debris that originates from slopes (Mothes and Vallance, 2015). Lahars may be generated from debris flow triggered by an eruptive activity (known as primary lahars) or that mobilized after eruptions (known as secondary lahars) (Pistolesi et al., 2014). Lahar generation requires the presence of sediment deposits, unconsolidated debris, and triggering mechanisms involving water saturation (i.e., melting snow, glaciers, or heavy rains) (Kataoka et al., 2018). ...
Article
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Secondary lahars, generated after volcanic eruptions, may pose significant threats to life and infrastructure. Secondary lahars typically develop from ash deposits and other volcanic debris that remobilize downstream via intense rainfall. The lahar inundation zone after eruptions must be predicted to minimize the impact. This prediction can be modeled based on digital elevation models (DEMs) and two parameters associated with lahar simulations: the lahar starting point (LSP), which indicates the potential locations at which a lahar flow may initiate, and supplied lahar volume (SLV), which is the lahar volume corresponding to each LSP. These parameters are typically determined by assumptions based on past lahar events, which may be unrealistic and often misinterpreted in the inundation prediction. To address this problem, this paper proposes an automated method to estimate the LSP and SLV based on pre-and post-eruption DEMs generated by unmanned aerial vehicle (UAV) images and simulate the inundation zone using the LAHARZ model. The study site is located in the southeast region of Mount Agung (Indonesia), and the objective is to mitigate the potential secondary lahar hazard after the 2017–2019 eruption crisis. Results show that the parameter estimations using the high-resolution UAV DEM and LAHARZ produce a realistic lahar simulation, with a satisfactory similarity of 82%, as verified against the lahar footprint. Moreover, we compare the results with those obtained using TerraSAR-X DEM and demonstrate the importance of using a detailed UAV DEM to avoid underestimating the lahar runout and ensure that the simulated inundation zones mimic real lahars.
... Unsurprisingly, we can consistently find in the literature that several approaches have been adopted when a particular lahar's triggering process was adopted on top of the eruptive Cotopaxi. For instance, the LAHARZ simulations carried out in [38] assumed a "Many Sources" hypothesis, namely that the southward lahars that eventually formed at the bottom of the Cotopaxi cone were the result of the confluence of those triggered in the upper parts of the three main southern drainage systems (streams: Cutuchi, Sasquímala, and Aláquez). Improved simulations [18] were carried out, taking into account the erosion and considering the lahar that was thus formed at the base of the volcano as the initial lahar. ...
Article
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We forecast the impact that the lahars triggered on the summit of the Cotopaxi volcano in Ecuador would have upon the Hidroagoyán Dam should an 1877-type catastrophic eruption occur nowadays, with disastrous implications for the energy production of Ecuador. The Cotopaxi’ lahars have been simulated with the use of different computational models, yet none of them were so extended as to map their entire path to the dam. To fill this gap, we applied a version of the semiempirical Cellular Automata LLUNPIY model to simulate primary and secondary lahars flowing from the summit of the Cotopaxi volcano until they reach the Hidroagoyán Dam in Baños. This version of LLUNPIY accounts for the triggering event by pyroclastic bombs and has already been validated by its successful simulation of the northbound 1877 cataclysmic lahars of the Cotopaxi volcano. The likely consequences of a similar disaster are discussed considering present territorial conditions. Computer simulations of natural hazards of this type represent a powerful tool that can be used when planning for the mitigation of environmental and social risks.
... This database can support a range of future research objectives, including forecasts of glacier-mass loss and the timing of peak glacial runoff, assessments of water availability for major cities (e.g. Quito 5,44 ), and improvements to regional volcanic hazard maps 14,15,18,40 . ...
Article
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Tropical glacier melt provides valuable water to surrounding communities, but climate change is projected to cause the demise of many of these glaciers within the coming century. Understanding the future of tropical glaciers requires a detailed record of their thicknesses and volumes, which is currently lacking in the Northern Andes. We calculate present-day (2015–2021) ice-thicknesses for all glaciers in Colombia and Ecuador using six different methods, and combine these into multi-model ensemble mean ice thickness and volume maps. We compare our results against available field-based measurements, and show that current ice volumes in Ecuador and Colombia are 2.49 ± 0.25 km³ and 1.68 ± 0.24 km³ respectively. We detected no motion on any remaining ice in Venezuela. The overall ice volume in the region, 4.17 ± 0.35 km³, is half of the previous best estimate of 8.11 km³. These data can be used to better evaluate the status and distribution of water resources, as input for models of future glacier change, and to assess regional geohazards associated with ice-clad volcanoes.
... The Cotopaxi Volcano located in the western cordillera of the Ecuadorian Andes is known to have had a vast history of big eruptions, far-reaching ash emissions and most importantly lahar generations, which may surpass 150 million m 3 [14][15][16][17][18][19][20][21][22]. Lahar generation may be caused by either by the collapse of an eruptive column or by the effect known as boiling over, both produce pyroclastic flows, which are able to melt part of the glacier´s surface [15,18,19]. ...
... The Cotopaxi Volcano located in the western cordillera of the Ecuadorian Andes is known to have had a vast history of big eruptions, far-reaching ash emissions and most importantly lahar generations, which may surpass 150 million m 3 [14][15][16][17][18][19][20][21][22]. Lahar generation may be caused by either by the collapse of an eruptive column or by the effect known as boiling over, both produce pyroclastic flows, which are able to melt part of the glacier´s surface [15,18,19]. As the volcano awakens, it is fundamental to know the flow directions of the generated lahars in order to reduce risks, vulnerabilities and losses similar and/or worse than the ones that destroyed Armero town, Colombia in 1985 killing some 23,000 citizens [12,[23][24][25]. ...
Chapter
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The Cotopaxi Volcano is one of the most dangerous volcanoes world- wide due to its potential of the generation of voluminous lahars of dozens of mil- lions of cubic meters capable of destroying infrastructure and endangering a lot of people living near major river drainages of this volcano. Our study describes such circumstances in the northern side of Cotopaxi Volcano and how we pro- pose to reduce the vulnerability of the public with new evacuation methods. Therefore, we have used geomatic tools, in order to shorten evacuation ways and directions. Based on the results, we determined different spatial variables or geographic coverage of the described and highlighted the main points of interest in each of them. The location of initial evacuation points of the population was determined within the lahar travel area being along the road axes. With these points we calculated security checkpoints outside the area lahar with additional margin. For this process the impedance was determined according to the average speed of a person in case of evacuation. In areas where the evacuation time has been longer than the arrival time of the lahar, vertical rather than horizontal evacuation points were determined by evaluating its coverage area depending on the time needed for the population to be safe.
... Thus, the lahar hazard at Cotopaxi has always been assessed by deterministic approaches, which have used different numerical models calibrated with Remote Sens. 2022, 14, 631 3 of 25 field data and corresponding lahar scenarios. Numerical models tested at Cotopaxi include 1-D hydrological [7,16,27,28], statistical [18], and more developed flow-dynamics-based codes which consider deposition, bulking and erosive processes [29,30]. Regardless of the numerical model, the field data or lahar scenario used as either entry data, boundary condition, or calibration, has been invariably derived from knowledge of the primary lahar that occurred on 26 June 1877, during the latest highly explosive eruption of the Cotopaxi volcano. ...
Article
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Cotopaxi is an active volcano in Ecuador, whose eruptions are characterized by producing destructive primary lahars which represent a major risk for the country. The hazard assessment related to such lahars relies largely on the knowledge of the latest event, which occurred on 26 June 1877, for either scenario definition or simulation calibration. A detailed (1:5000 scale) cartography of the deposits belonging to that eruption has been obtained in the proximal northern drainage of Cotopaxi. The cartography was performed through a combination of geological fieldwork, as well as the analysis and interpretation of high-definition imagery obtained by drone surveys combined with the Structure from Motion technology for image processing. Such imagery included red and green visible bands, and a near-infrared band, which allowed the obtention of NDVI imagery where the primary lahar deposits were identified and cartographed with support of fieldwork data. Both data sources are mutually complementary, and the final cartography would be impossible if any of them were not available. The results obtained represent a significant advance for the level of detail with respect to previous cartographic works. Moreover, they should allow an improved calibration of the new generation of numerical models that simulate lahar flow for hazard assessment at Cotopaxi.
... Mass flow numerical models are frequently used to predict the hazard from future events (e.g. Procter et al., 2010b;Scott et al., 1997Scott et al., , 2005Aguilera et al., 2004;Pistolesi et al., 2014;Darnell et al., 2013;Thouret et al., 2013), understand fundamental processes within mass flows, investigate previous events (e.g. , and determine impacts to elements exposed to the flow (e.g. Zeng et al., 2015;. ...
Article
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The use of mass flow simulations in volcanic hazard zonation and mapping is often limited by model complexity (i.e. uncertainty in correct values of model parameters), a lack of model uncertainty quantification, and limited approaches to incorporate this uncertainty into hazard maps. When quantified, mass flow simulation errors are typically evaluated on a pixel-pair basis, using the difference between simulated and observed (“actual”) map-cell values to evaluate the performance of a model. However, these comparisons conflate location and quantification errors, neglecting possible spatial autocorrelation of evaluated errors. As a result, model performance assessments typically yield moderate accuracy values. In this paper, similarly moderate accuracy values were found in a performance assessment of three depth-averaged numerical models using the 2012 debris avalanche from the Upper Te Maari crater, Tongariro Volcano, as a benchmark. To provide a fairer assessment of performance and evaluate spatial covariance of errors, we use a fuzzy set approach to indicate the proximity of similarly valued map cells. This “fuzzification” of simulated results yields improvements in targeted performance metrics relative to a length scale parameter at the expense of decreases in opposing metrics (e.g. fewer false negatives result in more false positives) and a reduction in resolution. The use of this approach to generate hazard zones incorporating the identified uncertainty and associated trade-offs is demonstrated and indicates a potential use for informed stakeholders by reducing the complexity of uncertainty estimation and supporting decision-making from simulated data.