Tectonophysics 639 (2015) 23–33 Contents lists available at ScienceDirect Tectonophysics journal homepage: www.elsevier.com/locate/tecto Volcano-tectonic control of Merapi's lava dome splitting: The November 2013 fracture observed from high resolution TerraSAR-X data T.R. Walter a,⁎, J. Subandriyo b, S. Kirbani c, H. Bathke a,d, W. Suryanto c, N. Aisyah b, H. Darmawan c, P. Jousset a, B.-G. Luehr a, T. Dahm a a Dept. Physics of Earth, GFZ German Research Centre for Geosciences, Telegrafenberg, 14473 Potsdam, Germany Technical Research Center for Geological Hazard (BPPTKG), Jalan Cendana 15, Yogyakarta 55166, Indonesia Laboratory of Geophysics, Department of Physics, Faculty of Mathematics and Natural Sciences, Universitas Gadjah Mada (UGM), Yogyakarta, Indonesia d King Abdullah University of Science and Technology, Thuwal 23955-6900, Saudi Arabia b c a r t i c l e i n f o Article history: Received 26 May 2014 Received in revised form 10 October 2014 Accepted 5 November 2014 Available online 14 November 2014 Keywords: Merapi volcano Dome stability Tectonic setting Satellite radar Remote sensing a b s t r a c t Volcanism at active andesite–dacite volcanoes is often associated with the formation and collapse of circularshaped protrusions of extruded, highly viscous lava, the so-called domes, which are emplaced in the near summit region. Growing domes may experience stable and instable structural phases, with a gradual transition in between. Dome collapse and the break-off of instable blocks of viscous lava may lead to pyroclastic flows, one of the most lethal hazards at stratovolcanoes. At Merapi volcano, Indonesia, a new dome started growing in the summit region in the amphitheater formed in the course of the climactic 2010 eruption. Three years later, the dome reached a height of approximately 100 m and diameters of 220 and 190 m with a plateau-like surface area of 40,000 m2 approximately. On 18/11/2013, an explosion occurred without identified precursors, leaving a major fracture cutting the complete dome structure. Based on high resolution TerraSAR-X satellite radar imagery, we could identify the linear fracture, traceable over ~200 m in the long axis, up to 40 m wide. After geocoding of the radar amplitude imagery, the fractures azimuthal trend could be compared to other structural lineaments, indicative of a significant NNW–SSE structural direction that has formed on Merapi volcano in the past. The Merapi dome fractured in a NW–SE direction, and is consistent with the alignment of regional tectonic structures and of anticipated directions of pyroclastic flows. The fracture may be part of a larger volcano-tectonic system and may affect the dynamics and the stability of the Merapi dome. © 2014 Elsevier B.V. All rights reserved. 1. Introduction Silicic domes are high viscous extrusions of magma at the summit of dominantly dacitic-andesitic volcanoes. Silicic domes may destabilize and collapse, representing the source region for destructive pyroclastic flows (Calder et al., 2002). The growth and collapse of silicic domes are thought to be controlled by the extrusion dynamics (Hale et al., 2009a, 2009b), the underlying slope and surrounding morphology (Walter et al., 2013), the brittle (cooled) crust stabilizing the extrusive magma body and hence the exogenous and endogenous growth (Hale, 2008; Kaneko et al., 2002). Therefore, at growing domes a fragile balance exists between extrusion of viscous lava, cooling and degassing, erosion and the mechanical instability of the dome. At occasions, the stability of domes may be modified by external forcing, at Merapi possibly associated with heavy rain fall (Elsworth et al., 2007; Neuberg, 2000), or with large tectonic or regional earthquakes (Jousset et al., 2013; Voight et al., 2000; Walter et al., 2007, 2008). Little observations ⁎ Corresponding author. E-mail address: [email protected] (T.R. Walter). http://dx.doi.org/10.1016/j.tecto.2014.11.007 0040-1951/© 2014 Elsevier B.V. All rights reserved. and research have been described on the causes and effects that a sudden disruption of the plug might have on the dynamics of the system (Melnik and Sparks, 2002). In particular, it is important to monitor the disruption of the solidified outer crust of a dome, a key component in the factors controlling the dome morphometry. Observations at Mount St. Helens (USA) and at Soufriere Hills (Montserrat) showed that disruption and partial removal of the dome may release the plug, depressurize the conduit and even trigger vulcanian explosions (Carn et al., 2004; Walter, 2011; Watts et al., 2002). At Merapi, this solidified brittle crust of the dome has been fractured during an explosion in November 2013, making this event an example of a sudden disruption of a dome surface. 1.1. Merapi volcano setting and dome formation Merapi volcano is located on Java Island, Indonesia (Fig. 1), and has become one of the best studied volcanoes since the IAVCEI volcano decade program (Gertisser et al., 2012; Newhall, 1994; Voight et al., 2000). Commonly observed activity at Merapi is dominated by gradual dome growth, intermittently destroyed either by explosions or by collapse 24 T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Fig. 1. Location and overview of Merapi volcano. A. Topographic map showing the location of Merapi and seismic stations mentioned in the text. An earthquake (red star) occurred just 15 min before the November 18, 2013 Merapi explosion. B. Shaded relief image of Merapi and adjacent volcanoes (red triangles). The volcanoes are aligned in direction NW–SE, as indicated by the rose diagram (azimuthal values). White boxes indicate satellite image frames. C. Radar amplitude maps of TerraSAR-X data recorded in ascending track. D. Radar amplitude maps of TerraSAR-X data recorded in descending track. (Ratdomopurbo and Poupinet, 2000) associated with pyroclastic flows. Peaks of this dome growth and collapse activity occur in a frequency of 3–5 years (Newhall et al., 2000). Merapi had major VEI 4 eruptions in 1872 and in 2010 (Andreastuti et al., 2000; Surono et al., 2012), the latest one destroyed the summit part and left a major amphitheater that is open to the south-southeast (SSE). The SSE opening direction of the amphitheater is aligned with the Gendol river, and has deepened a valley created by the 2006 eruption (Charbonnier et al., 2013; Saepuloh et al., 2011; Thouret et al., 2010). This opening direction is responsible for the southwardly channelized pyroclastic flows in 2010 (Komorowski et al., 2013). The reason why this profound valley has developed in this particular direction remained unclear, although it is important for understanding primary and secondary hazards at Merapi: Modeling of anticipated pyroclastic flows suggests that this valley path is directing hazards into southerly regions, i.e. the populated part (~1 Mio pop.) of the district Yogyakarta (Charbonnier and Gertisser, 2009). Therefore, understanding of this azimuthal trend and close observation of the growing dome are essential. 1.2. Dome growth and recent explosions The most recent dome has commenced to grow shortly after the centennial 2010 eruption (Surono et al., 2012). The continuous growth of the new dome has been relatively stable in the three years since 2010. The growth could be well observed through camera systems installed by a joint collaborative project between the volcano observatory BPPTKG, the Gadjah Mada University UGM and the GFZ German Research Centre for Geosciences. This dome of viscous andesitic lavas has reached over 100 m in height and 200 m in width (Fig. 2). The growth was interrupted by a few small-scale explosions, some phreatic in origin, reaching 1 km height at most (VEI 1), as those that occurred in July 15, 2012, or July 22, 2013. These small scale explosions formed a T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 25 to this tectonic event, strong rainfall preceded the explosion days before; unfortunately no rain gauge measures are available to further quantify this effect. A first inspection just after the Nov 18, 2013 explosion revealed that a major fracture had opened on the solidified crust of the lava dome surface. This work describes the geometry and relevance of this newly formed fracture, based on remote sensing data compared to field photographs. Satellite images acquired by the German TerraSAR-X satellite provide detailed views into the summit region. After analyzing the dimension, azimuth and architecture of the new fractures on the dome, a discussion is provided about the implications for the structural splitting mechanics of domes and the general relevance of this structural architecture for the future instability of the Merapi dome and the hazards associated with eruptions that may occur with little or no precursors. 2. Data and methods Fig. 2. A. Quickbird image from 9 September 2013 shows the dome, and a prominent lineament feature oriented NNW–SSE as indicated by red arrows. B. Photographs from Gendol into the amphitheater of Merapi, showing the steep front of the lava dome and its lower limit (dashed white line). Estimated lava dome thickness is 100 m. number of craters located either on the summit of the dome itself, or in the valley between the dome and the amphitheater. The two largest of these craters (vents in Fig. 2A) form a linear feature oriented NW–SE, which is relevant for interpreting the results of this work. The vent location enclosed by the dome and the amphitheater (Fig. 2) is the site of higher temperatures as detected by handheld infrared measures routinely performed by the volcano observatory BPPTKG in 2012–2013. The same region is the site of most intense fumarole activity and also minor explosions. As this valley is a closed valley, i.e. without outflow, intense rainfall is occasionally trapped to form short lived lakes. In Nov 18, 2013 (local date) a major explosion occurred, 2 km high, with little juvenile material being ejected mainly to the west and southwest of the edifice. Monitoring cameras allowed a first inspection of the Nov 18, 2013 eruption effects (Fig. 3). Local seismic networks, tilt and EDM measurements did not show any significant precursors. However, seismic recordings at a broadband station of UGM-GFZ (KALI) located 6 km to the south of the summit reveal the occurrence of a tectonic earthquake with a magnitude Mw 4.7 near the south coast of Java (Fig. 4). This tectonic event preceded the volcano explosion by ~ 15 min only, and was recorded also by the Meteorological Agencies of Indonesia's seismic network (YOGI) at larger distances. Residents living on the slopes of Merapi heard a roar sound from Merapi. In addition Visual inspections at Merapi are amongst the most reliable methods to record changes in the morphology of the summit over time and infer potential hazards in the course of the recent activity. However, the eruption on 18 November 2013 occurred in the rainy season of Java and the summit was often cloud covered. Therefore visual inspections and visibility by fixed installed surveying cameras were limited, allowing only clear views with several days' separation (Fig. 3). To overcome such limitations, in support of the GEO Supersites initiative (http://supersites.earthobservations.org/), the GFZ Potsdam has commenced ensuring the acquisition of synthetic aperture radar images acquired by the German satellite TerraSAR-X. Data were regularly acquired before and after the explosion, and available for processing within few days after acquisition. The satellite has usually a revisit cycle of 11 days and in November 2013, only one image once every two cycles was recorded, leading to a temporal baseline of 22 days. Recordings of both, ascending and descending orbits, were available for this study in tracks 58 and 96, respectively. The radar is an active illumination technique and its operation is independent of day and night, and, due to the wavelength of the signal (X-band), it propagates through thick clouds. For the purpose of monitoring volcanic domes, the TerraSAR-X satellite was configured by us to record images in spotlight mode, providing an unprecedented high spatial resolution of ~ 2 m of the Merapi dome (Supplemental material). The processing of the imagery was done in several steps. First, we performed an interferometric (InSAR) and pixel offset (PO) processing; second we structurally analyzed the image amplitudes to obtain detailed structural information. The co-registration of the SAR data has been done by using a digital elevation model, which is essential for high resolution radar data (Nitti et al., 2011). We account for the linear Doppler frequency shift in azimuth during the radar acquisition in spotlight mode by following Jendryke et al. (2013). We calculated interferograms using the software package Doris (Kampes and Usai, 1999). Differential interferograms were derived by using a digital elevation model (ASTER GDEM 30m). The interferograms were filtered using a Goldstein adaptive approach (Goldstein and Werner, 1998). In addition, we investigated the amplitude changes of the SAR images before and after the explosion. To this aim we first geocoded the images by using the digital elevation model. Results allow a spatial comparison of the dome and its changes at unprecedented detail. We investigated the length of the fracture by overlaying the amplitude imagery in a GIS platform (ArcGIS 10.x). The geocoded images were colorized in the red and green channels, allowing us to create a composite raster map. In the RGB composite renderer, the blue channel was left blank. Treatment of the SAR amplitude data as a multiband raster dataset provides a comprehensive visualization of the geometric changes that might have occurred. The length, width and azimuth of identified lineaments were digitized and measured and compared to other lineaments evident on the 26 T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Fig. 3. Photographs from fixed installed cameras into the amphitheater of Merapi allow comparison of images before and after the November 18, 2013 explosion. Note the appearance of a fracture after the explosion. Camera position at Gendol shown in the first two rows, camera position at Deles shown in the lower two photographs. Fig. 4. Broadband seismic record of two seismic stations, YOGI (in gray) and KALI (in black). For location of the earthquake, the volcano and the seismic stations refer to Fig. 1. Records are shown for the evening hours of November 17, 2013 (or early morning on the November 18, local time). The first event corresponds with the occurrence of a M 4.7 south of Java earthquake and the second event is associated with the Nov 18 explosion. edifice and the surrounding. Lineaments that are defined as mapable features, are often linear features and foremost thought to reflect subsurface phenomena (O'Leary et al., 1976). To this aim we apply a Hough transform edge detection filter on the gray scale TerraSAR-X amplitude imagery. The edges were then vectorized and converted to straight lines in MATLAB, and further analyzed in an ArcMap shape file. In order to account for the different lengths of the lineaments, we subdivided them into 2000 sublineaments for the ascending and descending data, respectively, and we calculated their azimuth. All lineament azimuths were then plotted into rose diagrams. To systematically analyze the direction of the lineaments statistically, i.e., we consider a large number of lines in the landscape that are alleged to be associated with the hidden architecture of the rock basement (Hobbs, 1904). The comparison of rose diagrams obtained from lineaments inside the Merapi crater and from lineaments on the flanks of the edifice allows structural interpretation of the newly formed fracture paths. Also we compare this structural trend to the alignment of other volcano centers adjacent to Merapi volcano. Results are shown in map-view, as amplitude images, and in rose diagrams, compared to time lapse and field photographs taken after the explosion from the eastern crater rim. T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 3. Results 3.1. Dome splitting We first analyze the radar amplitude maps that provide important constraints on the lineaments and the volcano-tectonic control. The geocoded amplitude imagery clearly depicts the crater open in form of an amphitheater to the south-southeast (Fig. 5). Due to the depth of the crater floor, shadowing causes significant data gaps (shadow regions are in black). Areas facing the satellite, in turn, appear brighter in the amplitude images. Within the amphitheater itself, a steep flank facing the satellite is geometrically distorted due to foreshortening artifacts. Nevertheless, in-between these two steep flanks of the amphitheater, the dome of Merapi is clearly represented in both ascending and descending images. The TerraSAR-X images acquired before the 18 Nov, 2013 eruption show the summit region of the dome as a relatively flat plane (Fig. 6A, B). The amplitude variation of the dome surface appears bended, with slightly higher reflectivity centered on the dome. A localized spherical region in the center of the dome and a region just northwest of the dome correspond to craters created by earlier smaller phreatic explosions (e.g., July 2012 and 2013; marked as ‘vent’ in Fig. 6). Radar images after the 18th November 2013 eruption show that the same dome is breached by an open fracture or fissure oriented NW–SE (Fig. 6C, D). In fact, the fracture is defined by two main segments, each being 90–95 m long. Moreover, a pronounced shadowing region appears in the radar images just around the northern fracture segment, sandwiched between the dome and the amphitheater. This region represents the crater that widened by the Nov 18 explosion. The size of this 27 crater is about 80–100 m wide. The width of the fracture reaches up to 40 m. A close-up composite map analysis in GIS (Fig. 6E, F) shows the trace of the fractures in more clarity, as they appear as an almost perfectly linear feature traceable over 200 m, split in a well-defined 91 m and 95 m segment in the north and south, respectively. The dome, with diameters of 200 m by 190 m (or ~40,000 m2) is therefore split in two parts. Only the southernmost steep flank of the dome does not show the continuation of this fracture, allowing speculations on a change in the local stress field of the dome structure at its southernmost flank. Instead, the southern part of the dome shows abrupt composite map changes aligned normal to the main NW–SE fractures. These fractures have an orientation perpendicular to the aforementioned main structural features. This southern part of the dome appears distinct or even detached from the main dome. The detachment of the southern part of the dome and therefore might be related to gravitational instability rather than tectonics. Accordingly a large block at the southern front of the dome (Fig. 4B) is defined, which is structurally detached from the main dome and potentially prone for collapse towards the valley. 3.2. Deformation absence To test for any deformation that might have occurred during the Nov 18 explosion, we investigate both the phase difference (InSAR) and the amplitude offsets of the TerraSAR-X data. InSAR images show minor edifice-wide color changes (Fig. 7). The interferograms' phase changes are generally below 1 color cycle, and are probably associated to atmospheric contributions, because the appearance and pattern alter in independent interferograms. Therefore, Fig. 5. Radar imagery from TerraSAR-X acquired in spotlight mode (2 m resolution). Amplitude imagery clearly depicts the newly formed fracture trend localized on the dome of Merapi volcano. A, B. Images before the explosion. C, D. Images after the explosion. Ascending track (left side) and descending track (right side). Brighter colors correspond to stronger backscattering, related to surface backscattering properties or geometric effects. 28 T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Fig. 6. Close-up view to the lava dome of Merapi from radar imagery. A pronounced fracture is splitting the dome into two halves. E, F. Composite raster map images created in the RGB bands for R = pre-explosive and G = post-explosive imagery (B — blank) depicts changes and lengths of newly formed fractures. The main fracture is defined by two sub-fractures with a slightly different azimuth, each about 100 m long. The rose diagrams show the strike angles of the lineaments (white arrows in E and F) within the crater. Note the change in the southern dome area. InSAR data reveals no edifice-wide deformation. The only fringes observed in the interferograms that might indicate a phase change associated with deformation are found in the uppermost crest of the Merapi amphitheater (Fig. 7C). In particular, the ascending interferogram reveals a phase change of two fringes, suggesting the occurrence of local subsidence. As the fringes are confined and appear only in the very steep uppermost proportion of the amphitheater, we believe that they are related to a very shallow geologic process, which may explain why no precursors had been recorded by existing networks. Whether this subsidence is associated to magmatic processes, cooling of a conduit, or related to other mass movement in the upper edifice region cannot be ascertained from this data alone. If associated to tensile or relative opening, an extent of deformation would be certainly evident in the radar images; however our analyses of the radar interferograms and their azimuth and range offset do not support the opening or slip along the fractures. Therefore an explosive origin, probably a phreatic explosion, appears the most plausible, T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 29 Fig. 7. Interferograms from TerraSAR-X data showing co-explosive interferograms in ascending (track 96, left panels A, C) and in descending viewing geometry (track 58, right panels B, D). Zoom shown in panels C and D. No edifice wide deformation could be identified. Local phase differences (fringes) nearby the western amphitheater rim might represent local displacement (movement away from the satellite). No deformation on the dome surface could be identified due to decorrelation. For pixel offset calculations the reader is referred to the Supplementary information. lacking significant ground movements. The location of the extended fracture is exactly at the same position where in earlier images small phreatic explosion sites have been identified (‘vent’ in Fig. 6). 3.3. Lineaments Lineament analysis reveals that the trend of the main dome splitting, oriented NW–SE, can similarly be observed on the flanks of the volcano edifice as well. Are these related to the dome fracture? Rose diagrams show the exact azimuth of the new fracture, which is NW–SE (Fig. 6E, F). The trace of the sidewalls of the amphitheater is also NW–SE, very similar to the fracture inside the dome. The dominant azimuthal trend of the valleys and lineaments outside the summit amphitheater of Merapi is in general also NNW–SSE (Fig. 8), again comparable to the aforementioned structures. This result was confirmed also by using the Aster GDEM-slope map, indicating a dominantly NNW–SSE lineament directivity. The edifice-wide lineaments, however, show a more scattered trend, and appear slightly rotated clockwise with respect to the fracture that has formed in Nov 18, 2013 on the dome. For instance, it can be observed that lineaments on the southeastern sector of Merapi are more oriented N–S, while the lineaments on the northwestern sector of Merapi are preferably oriented NW–SE. Although being in general similar to the fractures that split the dome on Nov 18, 2013, a curvature of the lineaments around the volcano summit appears systematic and is further discussed below. A NNW–SSE azimuthal trend is also observed at even larger scale by the trend line, connecting the adjacent volcanoes of Merapi, Merbabu, Telemoyo and Ungaran (Fig. 1C), already described by Van Bemmelen (1949). The fact that azimuthal trends of the volcano centers, the volcano-tectonic lineaments, its amphitheater and the newly formed fracture are similar, suggests a close genetic relationship as discussed further below. 4. Discussion Merapi volcano has experienced a significant eruption on 18th November 2013. According to the volcano observatory records at BPPTKG and our results from InSAR, the explosion was neither preceded by significant deformation seen within the EDM network, nor by unusual seismicity (see also Supplemental material). 4.1. Dome splitting and instability Radar images acquired by the TerraSAR-X satellite before and after the Nov 18, 2013 eruption show a new fracture breaching the lava dome and parts of the summit. This fracture is NNW–SSE aligned and split the domain into two parts. In addition, another structural separation has developed on the steep frontal part of the dome. The latter structural separation is also confirmed by a recent photograph (Fig. 9), implying that a block facing the Gendol valley is structurally detached 30 T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Fig. 8. Edifice wide lineament mapping. Geocoded TerraSAR-X amplitude imagery in spot light mode was used to identify lineaments in ascending and descending track, respectively. A. Edge detection results converted to lineaments. B. To weight the lineaments according to their length, all lineaments were resampled to 2000 sub-lineaments with similar length. For each sub-lineament the strike direction was measured; this azimuthal direction was plotted in a rose diagram. Rose diagrams are shown in full circle, consisting of 10° sector, 36 classes, frequency–azimuth type. Both viewing geometries, ascending and descending, depict a predominant NNW–SSE trend. from the bulk rock mass and potentially unstable. The detached block is clearly defined by a NE–SW oriented fracture 85 m long, most expressed on the southwestern sector of the dome. The fracture is at a distance of 70 m to the steep southern slope, and is steeply inclined southward. For a 100 m thick dome this implies a lava dome rock volume of ~300,000 m3 that is structurally detached and potentially prone for collapse (Figs. 6F, 9C). The complex fracture network at the frontal part of the dome would mean that any future growth of the dome might be hazardous and is difficult to predict. New magma could be channeled along the newly formed fracture and fissures, causing the failure of a major block. 4.2. The NNW–SSE trend The NNW–SSE azimuth of the new fracture is similar to the direction of the open amphitheater and the Gendol valley further south, as well as to lineaments on the volcano flanks and to the alignment of prominent volcanoes in the surrounding. In addition, the prominent Kukusan fault, a major fault zone bypassing the Merapi summit on its eastern flank (Fig. 1D), interpreted as the delimiting landslide detachment (Gertisser et al., 2012), has a trend that is NNW–SSE on the SE sector of the volcano, curving to a NNW–SSE trend on the NW sector of the volcano edifice. Such curving fault trends on volcanoes have been described by crustal faults that are upwardly propagating into a volcano edifice (Wooller et al., 2009). In our conceptual understanding, Merapi is underlain by a structurally weak zone oriented NNW–SSE, which has influenced growth of adjacent volcanoes, development of valleys and flank instabilities and which has now also influenced the development of a fracture splitting the lava dome in two parts (Fig. 10). The position of the lava dome fracture, and exact alignment with earlier explosion sites (July 2012 and 2013 vents), suggests that this trend was already established before the Nov 18, 2013 explosion. A question we need to answer is to which degree cooling of the lava dome has contributed to this fracture trend. The formation of fractures in a cooling viscous lava dome may be compared to crack formation in cooling basalt columns. Since the new fractures at Merapi's dome are highly linear and not influenced by the circular shape of the protrusive and cooling lava, the inner stress field of the dome is very likely influenced from an external stress field. 4.3. Origin of the lava dome fracture Pixel offset calculations do not show any significant movement neither in ascending nor in descending track (Supplemental material). This suggests that the fracture may have formed without any lateral displacement. Our observations hence indicate that major movements have not occurred at depth or within the dome itself, and that this explosion was possibly influenced by near surface processes. A possible rainfall and a strong local earthquake, and explosion-driven due to sudden overpressure, possibly superheated vapor, contributed jointly as a trigger of the phreatic eruption. Volcanic lineaments have led to define the NNW–SSE trend along Ungaran–Telemoyo–Merbabu–Merapi as well as a WNW–ESE trend along Lawu–Merapi–Sumbing–Sondoro–Slamet (Van Bemmelen (1949)). Our work reveals that the NNW–SSE structural trend is not only present within the dome but also within the edifice itself and the surrounding. As the amphitheater and breaching of the Gendol valley have been initiated in 2006 already, this trend appears to be a more sustained structural trend that may affect further developments and hazards at Merapi. It is interesting to note that this general trend is also parallel to the border of a deep crustal velocity anomaly observed by means of seismic tomography (Luehr et al., 2013). Summit displacements recorded from 1993–1997 revealed the importance of structural discontinuities in that same direction (Beauducel et al., 2000). These trends, therefore, suggest that the past and future evolution of the Merapi volcano has to be considered with respect to a major NNW–SSE volcanotectonic pathway. Such preferential paths may affect or even control the paths of magma (Anderson, 1951), cause lateral widening (Rubin, 1992), and may even lead to flank failures (van Wyk de Vries and Francis, 1997). Recent gravity T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 31 if the underlying fault has a sinistral strike-slip component. At Merapi, the fracture breaching the summit region is rotated counterclockwise with respect to the Merapi–Merbabu line and with respect to the edifice wide lineaments, which is compatible by an underlying fault that has a sinistral component of strike-slip motion. Whether this fault is active as a transtensional, transpressional or pure strike slip fault cannot be discriminated from this data alone and requires further investigations. 4.4. External triggering Sudden structural or dynamic changes at Merapi volcano are not entirely new. Near summit structural discontinuities have been described based on geodetic data (Beauducel et al., 2006). In 2006, following a deadly earthquake just 40 km to the south of the summit (Walter et al., 2007, 2008), Merapi tripled its volcanic activity and the direction of pyroclastic flows changed from western direction to southern direction through the Gendol valley abruptly (Bignami et al., 2013; Ratdomopurbo et al., 2013). In the case of the November 2013 activity, it cannot be concluded with certainty that the explosion was triggered by the earthquake 15 min before; a possible causal relationship remains to be studied. A permanent broadband station confirmed that no preexplosive seismicity was detected, although this data has to be taken with care as the seismic instrument is located 6 km away from the summit (Fig. 3 and Supplemental material). Moreover, the influence of rain onto the dome splitting has to be further evaluated. However, we speculate that the existing fracture trend and the presence of structural features seen on the dome already before the Nov 18, 2013 explosion, imply that also rainwater might follow the same zones of weakness. Therefore rain might have contributed or even caused the explosion and finally the splitting of the dome. In this view, also following explosions of Merapi took place along the NNW–SSE lineament, such as in March 10 and 27, 2014, both of which exceeding plume heights of 1500 m. Opening of the NNW–SSE lineaments may in future increase the threat of further eruptions in southerly directions. 5. Conclusion Fig. 9. Photograph from the east amphitheater headwall onto the dome of Merapi. A. Prior to the explosion, photo taken in September 2011. Note the flat top of the dome. B, C, D. After the Nov 18, 2013 explosion, photo taken in January 2014. Note the new explosion crater and the deep fracture in the image. Close-up C shows the unstable block on the dome front that formed in 18 Nov 2013. Close-up D shows older vent that has been developed earlier. data and three dimensional density model simulations revealed the presence of a density contrast oriented NNW–SSE along the Merapi– Merbabu trend (Tiede et al., 2005). Possibly a larger intrusive body is geologically connecting these volcanoes (Tiede et al., 2005). The nature of this NNW–SSE directed lineament, however, remained unclear. The interaction between tectonic faults and volcanoes has been extensively investigated in analog experimental studies (Lagmay et al., 2000; Mathieu and van Wyk de Vries, 2011; Mathieu et al., 2011). Volcanoes influenced by strike-slip, transtensional and transpressional fault zones show a structural fault network that generally reflects the underlining tectonic trend, but higher at elevated regions might geometrically differ from the regional trend. Faults that have a strike-slip component lead to curvature in a sigmoidal pattern (Lagmay et al., 2000; Mathieu and van Wyk de Vries, 2011). This develops into a summit graben that is parallel to the main horizontal stress, or oriented obliquely to the actual fault trend (Mathieu and van Wyk de Vries, 2011). Orientation of the summit grabens is rotated counterclockwise This study based on radar remote sensing shows the strength of high resolution radar imagery in volcano observations. Moreover, it shows that the style and architecture of domes at explosive volcanoes may abruptly change within a short time. It shows that extrusive domes of viscous lava at a volcanic summit can be influenced by the regional fault lines. The explosion at Merapi on Nov 18, 2013 has basically broken the dome into two main parts. The consequences of this structural change for the future development, the growth and the collapse of the dome, are at this stage difficult to foresee. Changes might be associated with a different direction of magma, collapse, and more intensely expressed NNW–SSE pathway down into the Gendol valley and towards populated regions. A link with a deep seated NNW–SSE tectonic trend is postulated. Acknowledgments This work benefited from very detailed and constructive reviews by Maurizio Battaglia and Mario Mattia, as well as by the editor Rob Govers. This work is financially supported by the Helmholtz Alliance EDA. Satellite radar imagery was provided by the German Aerospace Centre, special thanks go to Ursula Marschalk and Achim Roth for support and data handling. This work is a contribution to the new technologies grant from GFZ. Appendix A. Supplementary data Supplementary data associated with this article can be found in the online version, at http://dx.doi.org/10.1016/j.tecto.2014.11.007. These 32 T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Fig. 10. Conceptual model of the Merapi summit. A. A NNW–SSE directed fracture zone responsible for the alignment of Merapi and adjacent volcanoes (the Merapi–Merbabu trend) is causing fractures at the Merapi summit dome. B. During the Nov 18, 2013 explosion, the dome splitted in two halves, the fracture trend is NW–SE. C. Left lateral motion along the Merapi–Merbabu trend may explain the structures seen on Merapi and the counterclockwise rotation of the 18 No 2013 lava dome fracture. C. Modified from Mathieu et al. (2011). See text for details. data include Google maps of the most important areas described in this article. References Anderson, E.M., 1951. The Dynamics of Faulting and Dyke Formation, With Applications to Britain. Oliver and Boyd, Edinburgh (206 pp.). Andreastuti, S.D., Alloway, B.V., Smith, I.E.M., 2000. A detailed tephrostratigraphic framework at Merapi volcano, Central Java, Indonesia: implications for eruption predictions and hazard assessment. J. Volcanol. Geotherm. Res. 100 (1–4), 51–67. Beauducel, F., Cornet, F.H., Suhanto, E., Duquesnoy, T., Kasser, M., 2000. Constraints on magma flux from displacements data at Merapi volcano, Java, Indonesia. J. Geophys. Res. 105 (4), 8193–8203. Beauducel, F., Nandaka, M.A., Cornet, F.H., Diament, M., 2006. Mechanical discontinuities monitoring at Merapi volcano using kinematic GPS. J. Volcanol. Geotherm. Res. 150 (1–3), 300–312. Bignami, C., Ruch, J., Chini, M., Neri, M., Buongiorno, M.F., Hidayati, S., Sayudi, D.S., Surono, 2013. Pyroclastic density current volume estimation after the 2010 Merapi volcano eruption using X-band SAR. J. Volcanol. Geotherm. Res. 261, 236–243. Calder, E.S., Luckett, R., Sparks, R.S.J., Voight, B., 2002. Mechanisms of lava dome instability and generation of rockfalls and pyroclastic flows at Soufrière Hills Volcano. In: Druitt, T.H., Kokelaar, B.P. (Eds.), The Eruption of Soufrière Hills Volcano, Montserrat, From 1995 to 1999. Geological Society of London Memoir, London, pp. 173–190. Carn, S.A., Watts, R.B., Thompson, G., Norton, G.E., 2004. Anatomy of a lava dome collapse: the 20 March 2000 event at Soufriere Hills Volcano Montserrat. J. Volcanol. Geotherm. Res. 131 (3–4), 241–264. Charbonnier, S.J., Gertisser, R., 2009. Numerical simulations of block-and-ash flows using the Titan2D flow model: examples from the 2006 eruption of Merapi volcano, Java, Indonesia. Bull. Volcanol. 71 (8), 953–959. Charbonnier, S.J., Germa, A., Connor, C.B., Gertisser, R., Preece, K., Komorowski, J.C., Lavigne, F., Dixon, T., Connor, L., 2013. Evaluation of the impact of the 2010 pyroclastic density currents at Merapi volcano from high-resolution satellite imagery, field investigations and numerical simulations. J. Volcanol. Geotherm. Res. 261, 295–315. Elsworth, D., Voight, B., Taron, J., 2007. Contemporary views of slope instability on active volcanoes. Proc. Monogr. Eng. Water 3–9. Gertisser, R., Charbonnier, S., Keller, J., Quidelleur, X., 2012. The geological evolution of Merapi volcano, Central Java, Indonesia. Bull. Volcanol. 74 (5), 1213–1233. Goldstein, R.M., Werner, L., 1998. Radar interferogram filtering for geophysical applications. Geophys. Res. Lett. 25 (21), 4035–4038. Hale, A.J., 2008. Lava dome growth and evolution with an independently deformable talus. Geophys. J. Int. 174 (1), 391–417. Hale, A.J., Calder, E.S., Loughlin, S.C., Wadge, G., Ryan, G.A., 2009a. Modelling the lava dome extruded at Soufriere Hills Volcano, Montserrat, August 2005–May 2006 part II: rockfall activity and talus deformation. J. Volcanol. Geotherm. Res. 187 (1–2), 69–84. Hale, A.J., Calder, E.S., Wadge, G., Loughlin, S.C., Ryan, G.A., 2009b. Modelling the lava dome extruded at Soufriere Hills Volcano, Montserrat, August 2005–May 2006 part I: dome shape and internal structure. J. Volcanol. Geotherm. Res. 187 (1–2), 53–68. Hobbs, W.H., 1904. Lineaments of the Atlantic border region. Geol. Soc. Am. Bull. 15, 483–506. Jendryke, M., Balz, T., Jiang, H., Liao, M., Stilla, U., 2013. Using open-source components to process interferometric TerraSAR-X spotlight data. Int. J. Antennas Propag. 1 (275635), 1–13. Jousset, P., Budi-Santoso, A., Jolly, A.D., Boichu, M., Surono, Dwiyono, S., Sumarti, S., Hidayati, S., Thierry, P., 2013. Signs of magma ascent in LP and VLP seismic events and link to degassing: an example from the 2010 explosive eruption at Merapi volcano, Indonesia. J. Volcanol. Geotherm. Res. 261, 171–192. Kampes, B., Usai, S., 1999. Doris: The Delft Object-oriented Radar Interferometric Software, Operationalization of Remote Sensing Symposium. ITC, Enschede, Netherlands. T.R. Walter et al. / Tectonophysics 639 (2015) 23–33 Kaneko, T., Wooster, M.J., Nakada, S., 2002. Exogenous and endogenous growth of the Unzen lava dome examined by satellite infrared image analysis. J. Volcanol. Geotherm. Res. 116 (1–2), 151–160. Komorowski, J.C., Jenkins, S., Baxter, P.J., Picquout, A., Lavigne, F., Charbonnier, S., Gertisser, R., Preece, K., Cholik, N., Budi-Santoso, A., Surono, 2013. Paroxysmal dome explosion during the Merapi 2010 eruption: processes and facies relationships of associated high-energy pyroclastic density currents. J. Volcanol. Geotherm. Res. 261, 260–294. Lagmay, A.M.F., van Wyk de Vries, B., Kerle, N., Pyle, D.M., 2000. Volcano instability induced by strike-slip faulting. Bull. Volcanol. 62, 331–346. Luehr, B.G., Koulakov, I., Rabbel, W., Zschau, J., Ratdomopurbo, A., Brotopuspito, K.S., Fauzi, P., Sahara, D.P., 2013. Fluid ascent and magma storage beneath Gunung Merapi revealed by multi-scale seismic imaging. J. Volcanol. Geotherm. Res. 261, 7–19. Mathieu, L., van Wyk de Vries, B., 2011. The impact of strike-slip, transtensional and transpressional fault zones on volcanoes. Part 1: scaled experiments. J. Struct. Geol. 33 (5), 907–917. Mathieu, L., van Wyk de Vries, B., Pilato, M., Troll, V.R., 2011. The interaction between volcanoes and strike-slip, transtensional and transpressional fault zones: analogue models and natural examples. J. Struct. Geol. 33, 898–906. Melnik, O., Sparks, S., 2002. Dynamics of magma ascent and lave extrusion at Soufrière Hills Volcano, Montserrat. In: Druitt, T.H., Kokelaar, B.P. (Eds.), The Eruption of Soufriere Hills Volcano. Montserrat. Geol. Soc. London, Memoirs, London, pp. 153–171. Neuberg, J., 2000. External modulation of volcanic activity. Geophys. J. Int. 142 (1), 232–240. Newhall, C.G., 1994. Research at decade volcanos aimed at disaster prevention. EOS Trans. Am. Geophys. Union 75, 340–350. Newhall, C.G., Bronto, S., Alloway, B., Banks, N.G., Bahar, I., Del Marmol, M.A., Hadisantono, R.D., Holcomb, R.T., McGeehin, J., Miksic, J.N., Rubin, M., Sayudi, S.D., Sukhyar, R., Andreastuti, S., Tilling, R.I., Torley, R., Trimble, D., Wirakusumah, A.D., 2000. 10,000 years of explosive eruptions of Merapi Volcano, Central Java: archaeological and modern implications. J. Volcanol. Geotherm. Res. 100 (1–4), 9–50. Nitti, D.O., Hanssen, R.F., Refice, A., Bovenga, F., Nutricato, R., 2011. Impact of DEMassisted coregistration on high-resolution SAR interferometry. IEEE Trans. Geosci. Remote 49 (3), 1127–1143. O'Leary, D.W., Friedman, J.D., Pohn, H.A., 1976. Lineament, linear, lineation: some proposed new standards for old terms. Bull. Geol. Soc. Am. 87, 1463–1469. Ratdomopurbo, A., Poupinet, G., 2000. An overview of the seismicity of Merapi volcano (Java, Indonesia), 1983–1994. J. Volcanol. Geotherm. Res. 100 (1–4), 193–214. Ratdomopurbo, A., Beauducel, F., Subandriyo, J., Nandaka, I.G.M.A., Newhall, C.G., Suharna, Sayudi, D.S., Suparwaka, H., Sunarta, 2013. Overview of the 2006 eruption of Mt. Merapi. J. Volcanol. Geotherm. Res. 261, 87–97. Rubin, A.M., 1992. Dike-induced faulting and graben subsidence in volcanic rift zones. J. Geophys. Res. 97 (B2), 1839–1858. 33 Saepuloh, A., Urai, M., Widiwijayanti, C., Aisyah, N., 2011. Observing 2006–2010 ground deformations of Merapi volcano (Indonesia) using Alos/Palsar and Aster Tir data. Int. Geosci. Remote Sens. 1634–1637. Surono, Jousset, P., Pallister, J., Boichu, M., Buongiorno, M.F., Budisantoso, A., Costa, F., Andreastuti, S., Prata, F., Schneider, D., Clarisse, L., Humaida, H., Sumarti, S., Bignami, C., Griswold, J., Carn, S., Oppenheimer, C., Lavigne, F., 2012. The 2010 explosive eruption of Java's Merapi volcano — a ‘100-year’ event. J. Volcanol. Geotherm. Res. 241–242, 121–135. Thouret, J.C., Gupta, A., Lube, G., Liew, S.C., Cronin, S.J., Surono, 2010. The 2006 pyroclastic deposits of Merapi volcano, Java, Indonesia: high-spatial resolution IKONOS images and complementary ground based observations. Remote Sens. Environ. 114 (9), 1949–1967. Tiede, C., Camacho, A.G., Gerstenecker, C., Fernández, J., 2005. Modelling the density at Merapi volcano area, Indonesia, via the inverse gravimetric problem. G-Cubed 6 (9), 1–13. Van Bemmelen, R.W., 1949. The Geology of Indonesia. Govt. Printing Office, The Hague p. 739. van Wyk de Vries, B., Francis, P.W., 1997. Catastrophic collapse at stratovolcanoes induced by gradual volcano spreading. Nature 387 (6631), 387–390. Voight, B., Constantine, E.K., Siswowidjoyo, S., Torley, R., 2000. Historical eruptions of Merapi volcano, Central Java, Indonesia, 1768–1998. J. Volcanol. Geotherm. Res. 100 (1–4), 69–138. Walter, T.R., 2011. Low cost volcano deformation monitoring: optical strain measurements and application to Mount St. Helens data. Geophys. J. Int. 186 (2), 699–705. Walter, T.R., Wang, R., Zimmer, M., Grosser, H., Luhr, B., Ratdomopurbo, A., 2007. Volcanic activity influenced by tectonic earthquakes: static and dynamic stress triggering at Mt. Merapi. Geophys. Res. Lett. 34 (5). Walter, T.R., Wang, R., Luehr, B.G., Wassermann, J., Behr, Y., Parolai, S., Anggraini, A., Gunther, E., Sobiesiak, M., Grosser, H., Wetzel, H.U., Milkereit, C., Brotopuspito, P.J.K.S., Harjadi, P., Zschau, J., 2008. The 26 May 2006 magnitude 6.4 Yogyakarta earthquake south of Mt. Merapi volcano: did lahar deposits amplify ground shaking and thus lead to the disaster? Geochem. Geophys. Geosyst. 9. Walter, T.R., Ratdomopurbo, A., Subandriyo, Aisyah, N., Brotopuspito, K.S., Salzer, J., Luhr, B., 2013. Dome growth and coulee spreading controlled by surface morphology, as determined by pixel offsets in photographs of the 2006 Merapi eruption. J. Volcanol. Geotherm. Res. 261, 121–129. Watts, R.B., Herd, R.A., Sparks, R.S.J., Young, S.R., 2002. Growth patterns and emplacement of the andesitic lava dome at Soufrière Hills, Montserrat. Geol. Soc. London Mem. 21, 115–152. Wooller, L., de Vries, B.V., Cecchi, E., Rymer, H., 2009. Analogue models of the effect of long-term basement fault movement on volcanic edifices. Bull. Volcanol. 71 (10), 1111–1131.
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