ORIGINAL RESEARCH article
Determining the Stress Field in Active Volcanoes Using Focal Mechanisms
- 1Dipartimento di Scienze e Tecnologie, Universitá degli Studi del Sannio, Benevento, Italy
- 2Istituto Nazionale di Geofisica e Vulcanologia, Sezione di Napoli, Osservatorio Vesuviano, Napoli, Italy
- 3Istituto per il Rilevamento Elettromagnetico dell'Ambiente, Consiglio Nazionale delle Ricerche, Napoli, Italy
Stress inversion of seismological datasets became an essential tool to retrieve the stress field of active tectonics and volcanic areas. In particular, in volcanic areas, it is able to put constrains on volcano-tectonics and in general in a better understanding of the volcano dynamics. During the last decades, a wide range of stress inversion techniques has been proposed, some of them specifically conceived to manage seismological datasets. A modern technique of stress inversion, the BRTM, has been applied to seismological datasets available at three different regions of active volcanism: Mt. Somma-Vesuvius (197 Fault Plane Solutions, FPSs), Campi Flegrei (217 FPSs) and Long Valley Caldera (38,000 FPSs). The key role of stress inversion techniques in the analysis of the volcano dynamics has been critically discussed. A particular emphasis was devoted to performances of the BRTM applied to volcanic areas.
Theoretical Background to Stress Field Inversion
In last decades focal mechanisms have shown to be very useful to infer about the stress field within the Earth. Being seismicity a common feature of both quiescent and erupting volcanoes, the study of volcano-tectonic earthquakes is an effective tool to retrieve spatial and temporal patterns in the pre-, syn-, and inter-eruptive stress fields. Stress changes associated with magma migration and more in general with the dynamics of magma chambers and hydrothermal systems are causally linked to these earthquakes. Hence retrieving the stress field pattern in volcanoes has important implications in studying their dynamics and the interaction with the regional tectonic stress field (Umakoshi et al., 2001; Pedersen and Sigmundsson, 2004; Segall, 2013; Cannavò et al., 2014; D'Auria et al., 2014a,b).
Rocks in the Earth lithosphere possess a specific state of stress strictly related to the tectonic setting of the region. The state of stress at any given point can be represented geometrically as a Stress Ellipsoid, a tri-axial solid built with the Principal Stress Components (PSC) σ1 > σ2 > σ3 as main axes. The shape of this ellipsoid can be expressed using the Bishop's ratio ΦB = (σ2 − σ3) / (σ1 − σ3) (Bishop, 1966). It expresses the relationship between the intermediate and maximum PSC respect to the minimum one and can assume values varying from 0 to 1. In a general tri-axial state of stress σ1 > σ2 > σ3 ≠ 0, and the ΦB ≈ 0.5. A slip event along a fault surface occurs when the accumulated energy exceeds the internal strength of the rock (Reid, 1910). The rupture starts at the hypocenter and then propagates along the whole fault plane. Analysis of seismograms allows the retrieving of information about the seismogenic structure responsible for an event. Byerly (1928) proposed a method that allows the reconstruction of the Fault Plane Solution (FPS) of an earthquake, which is a stereographic projection representing the geometry of a seismogenic structure. It can be easily explained picturing a focal sphere ideally located around the earthquake hypocenter. The focal sphere can be separated into four dihedra, two contractional, and two dilatational, delimited by two planes known as Nodal Planes (the main and the auxiliary planes). The main nodal plane represents the actual fault, with the slip occurring during the earthquake being along the direction orthogonal to the auxiliary plane (Figure 1). Therefore the geometry of the FPS is tightly linked to the fault kinematics. At the center of the contractional dihedra is located the P-axis (compressive) while the center of extensional dihedra (dilatational) hosts the T-axis. The neutral B-axis corresponds to the intersection of nodal planes (Figure 1). P, T, B axes are mutually normal. The relationship between P and T axes of a FPS and the actual σ1 and σ3 stress directions is not straightforward. The aim of stress inversion techniques is precisely to determine it. A FPS can be reconstructed a posteriori, starting from the analysis of the first arrival of P-waves at an adequate number of seismographs arranged around the hypocenter. Using the equal-area stereographic projection technique (lower hemisphere), each station can be plotted using the angular coordinates of the direct seismic ray leaving the hypocenter. Stations falling in a contractional quadrant will record a downward first P-wave arrival (void circle of Figure 1A). Conversely, stations falling in a dilatational quadrant will register an upward first P-wave arrival (solid circle of Figure 1A). Plotting this information on an equal-area stereographic projection net it is possible to find a couple of nodal planes that is able to divide up the plot into four quadrants, corresponding to the four dihedra of the focal sphere (Figure 1). Nowadays, these procedures are implemented in a wide range of algorithms performing the determination of the FPS automatically. One of the most commonly used algorithms is FPFIT (Reasenberg and Oppenheimer, 1985). It is a suite of Fortran codes for calculating and displaying earthquake fault-plane solutions. FPFIT finds the double-couple fault plane solution (source model) that best fits a given set of observed first motion polarities for an earthquake.
Figure 1. The Byerly's Fault Plane Solution. (A) A FPS is a stereographic projection representing the double-couple model of the seismogenic source; equal-area stereographic projection technique (lower hemisphere), void circles are P-wave downward first arrivals, solid circles are P-wave upward first arrivals, C1 and C2 are nodal planes with associated slip vectors s1 (pole to C2) and s2 (pole to C1), P- (compressive) T- (tensional) and B-axes (neutral) are also plotted; (B) Three-dimensional view of a Focal Sphere, the FPS of (A) represents the stereographic projection (on the equatorial plane) of the geometrical elements intersecting the lower hemisphere. (C) 3-D perspective of the FPS (see text for details).
Starting from observed fault kinematics or focal mechanisms, various stress inversion procedures can be implemented. These procedures allow the reconstruction of the reduced stress field that carries information about the stress orientation and the ratios between principal stresses. Inversion of focal mechanism datasets became a common task in studies aimed at constrain seismotectonic stress field in active tectonic areas (Carey-Gailhardis and Mercier, 1992; Gillard and Wyss, 1995; Hardebeck and Hauksson, 2001; Massa, 2003; Angelier and Baruah, 2009; De Matteis et al., 2012) and more recently also in volcanic environments (Wyss et al., 1992; Cocina et al., 1997; D'Auria et al., 2014a,b; Plateaux et al., 2014). A wide range of graphical and analytical methods were proposed by authors in last decades (e.g., Angelier and Mechler, 1977; Gephart and Forsyth, 1984; Carey-Gailhardis and Mercier, 1987; Lisle, 1987, 1988; Michael, 1987; Angelier, 1990, 2002; Rivera and Cisternas, 1990; D'Auria and Massa, 2015). Stress inversion procedures are based on the Wallace-Bott hypothesis: shear traction acting on a fault plane (irrespective of newly formed structure or a reactivated preexisting one) causes a slip event in the direction and sense of the shear traction itself (Wallace, 1951; Bott, 1959; Angelier and Mechler, 1977; Yamaji, 2007). Analytical techniques of stress inversion are based on the systematic comparison of the actual slip vector with respect to the theoretical (modeled) maximum shear stress acting on the same surface in response to the active stress field (Figure 2). Graphical approaches are based on the definition of a probability function (or an equivalent formulation) on the whole focal sphere. They allow the determination of a range of possible attitudes for principal stress axes using hand stereo-plot. Right Dihedra Method (RDM) represents the simplest of graphical stress inversions (Angelier and Mechler, 1977). It basically consists of averaging the focal spheres of a focal mechanisms dataset. In the late 80's, RDM was improved adding an additional geometrical constrain and was re-proposed as Right Trihedra Method (Lisle, 1987, 1988). Both RDM and RTM are able to manage both planes of focal mechanism regardless the pre-selection of the actual fault plane. D'Auria and Massa (2015) proposed a novel Bayesian approach for the determination of the stress field from focal mechanism datasets (BRTM). This method can be regarded as a re-visitation of the RTM in a sound probabilistic framework. It provides a probability function over the focal sphere for both σ1 and σ3 principal stress directions (Figure 3). BRTM algorithm has shown to be robust and efficiently enough to manage all kind of kinematics and nodal plane attitudes. A comparison of the BRTM performances to respect a classical Direct Inversion Method (Angelier, 1990, 2002) and the Multiple Inverse Method (Yamaji, 2000), confirms that BRTM is able to successfully manage both homogeneous and heterogeneous datasets (see Figure 2 in D'Auria and Massa, 2015). Furthermore BRTM allows both a reliable determination of the principal stress axes attitude and a quantitative estimation of the corresponding confidence regions (D'Auria and Massa, 2015). Finally, to give a complete and accurate inversion the corresponding Bishop's ratio ΦB can be determined, exploiting the BRTM results, following the approach proposed by Angelier (1990; Figure 3). In case of heterogeneous datasets result of stress field inversion could be misleading. The problem can be approached using different un-supervisioned techniques (e.g., Angelier and Manoussis, 1980; Yamaji, 2000). Among those, the Multiple Inverse Method (Yamaji, 2000), makes use of a resampling technique of the analyzed dataset, through the construction of many data subsets, inverted separately using an analytical approach (Otsubo et al., 2008). Results can be plotted on a stereographic projection to outline graphically different clusters of stress tensors, corresponding to the different components of the stress field acting in the lithospheric volume associated to the dataset. The major drawback of this technique is the difficulty in attributing to the retrieved stress field components a proper spatio-temporal collocation. Therefore heterogeneous datasets can be approached, more properly, taking into account spatial and possibly temporal variations of the stress pattern (Wyss et al., 1992; Hardebeck and Michael, 2006; D'Auria et al., 2014b). In other words, these methods take into account the spatio-temporal distribution of the data, providing as results not a single stress tensor, but a spatially (and possibly temporally) variable stress field. Applying the BRTM to subsets of FPS corresponding to a given sub-volume of the area under investigation allows retrieving the spatial pattern of the stress field. This is an essential approach in the analysis of seismological dataset of volcanic districts. In the next section we show the application of stress inversion procedures to three different volcanic areas. Analyses were carried out on datasets available from previous studies. For Mt.Somma-Vesuvius and Campi Flegrei we used data from D'Auria et al. (2014a,b). For the Long Valley Caldera, data are freely accessible to users via the Internet (NCEDC, 2014). We preferred to invert published datasets to novel ones as this allows a more efficient comparison of obtained results got with different processing approaches.
Figure 2. Misfit criteria adopted in stress inversion procedures. α angle formed between the actual slip vector (si) and the theoretical shear stress (τi) acting on each fault of the analyzed dataset (Carey and Brunier, 1974; Angelier, 1990); υi, the vector difference between si and τi (Angelier, 1990).
Figure 3. Results of the BRTM applied to a synthetic dataset (A) made up of three FPSs (black = dilatational dihedra); (B) 2-D plot on a Lambert equiareal, lower-hemisphere projection; (C) tridimensional view of the BRTM results over the focal sphere (After: D'Auria and Massa, 2015, modified).
This study aims at highlighting the key role played by stress inversion procedures in the analysis of the volcano dynamics. In detail, we show the methodological potential offered by the BRTM here tested on seismological datasets collected at three different volcanoes.
In order to show the capability of the stress inversion procedures on volcanoes, we applied the BRTM to determine the spatial variations of the stress field in three different volcano-tectonic environments: the Mt. Somma-Vesuvius Volcano (Southern Italy; Figure 4), the Campi Flegrei Caldera (Southern Italy; Figure 4) and the Long Valley Caldera (California-Sierra Nevada border, USA; Figure 9). In the following we report a synthesis of the key results, focusing on the relationship between the local active stress fields and the background regional ones.
Figure 4. Tectonic setting of the Campi Flegrei-Vesuvius area. (1) Main volcanoes; (2) Campi Flegrei (Campanian Ignimbrite) and Mt. Somma caldera rims; (3) main Plio-Quaternary faults; (4) thrust faults. Dashed squares identify the location of Figures 5, 7. Data from: Ippolito et al., 1973; Di Vito et al., 1999; Lavecchia et al., 2003; Acocella and Funiciello, 2006; Milia et al., 2013; Vitale and Isaia, 2013; D'Auria et al., 2014a,b, and referencer therein.
The Somma-Vesuvius (Figures 4, 5) is the youngest volcano of the Neapolitan district, it is characterized both by explosive and effusive activity (Santacroce, 1987). Its oldest products are dated 0.369 ± 0.028 Ma (40Ar/39Ar age from Brocchini et al., 2001). The last eruption of Vesuvius occurred in 1944 and after this event it has become quiescent, showing only fumarolic activity and low seismicity (M ≤ 3.6). Since 1964 to nowadays the seismicity started to increase in the occurrence and in the magnitude (Giudicepietro et al., 2010), with four episodes (1978–1980, 1989–1990, 1995–1996, 1999–2000) of strong increased strain release rate, occurrence and magnitude rate (D'Auria et al., 2013). The Mesozoic basement of the volcano is displaced by both SW- and NW-dipping normal fault systems and secondarily by NE-SW and E-W faults (Bianco et al., 1998; Ventura and Vilardo, 1999; Zollo et al., 2002; Acocella and Funiciello, 2006; Figure 4). Mesoscale faults and eruptive fractures striking NW-SE, NE-SW and ENE-WSW affect volcanic units outside the Somma caldera (Rosi et al., 1987; Andronico et al., 1995; Ventura and Vilardo, 1999; D'Auria et al., 2014a, Figure 1 for a review). Seismicity at Mt. Somma-Vesuvius shows the presence of two different seismogenic volumes: a top volume (above sea level) and a bottom one (1–5 km depth). These two volumes appear to be separated by a volume with a markedly reduced seismic strain release, possibly corresponding to a ductile sedimentary layer buried at about 1000 m b.s.l. (Bernasconi et al., 1981; Borgia et al., 2005; D'Auria et al., 2014a).
Figure 5. Mt. Somma-Vesuvius. Focal mechanisms dataset plotted on a shaded map (A), on a N-S (B), and an E-W (C) cross sections. (D) The distribution of focal mechanisms on a triangular Frohlich diagram (Frohlich, 1992). The dataset consists of 197 FPSs of earthquakes recorded from 1999 to 2012 with 0 < M < 3.6.
At Mt. Somma-Vesuvius we analyzed a dataset consisting of 197 FPSs of earthquakes recorded from 1999 to 2012 with 0 < M < 3.6 (D'Auria et al., 2014a). All the events were relocated by D'Auria et al. (2014a) using a nonlinear probabilistic approach in a 3-D velocity model (Lomax et al., 2001; D'Auria et al., 2008). FPSs were computed using P wave polarities (Reasenberg and Oppenheimer, 1985). Only events with at least six first motion observations were used to derive FPSs (Figure 5). Kinematics of the analyzed FPSs are quite equally represented in the three extreme categories, dip-slip normal, dip-slip reverse and strike-slip (Figure 5D). The stress field has been computed on a regular three-dimensional grid of 1-km spacing. For each grid node all the FPSs within a radius of 1-km have been considered for the inversion. The stress field has been computed only at volumes containing at least five FPSs. A synthesis of BRTM results is reported in Figure 6. For the top-volume (slice for depth −1 km, corresponding to the portion of the edifice lying above the sea level) the retrieved σ1 is sub-horizontal overall trending NW-SE, corresponding to a sub-vertical σ3 and the related ΦB is <0.5. Results for the bottom volume are summarized for depths of 1, 3, and 5 km. At 1 km depth slice σ1 moderately plunges toward ENE and corresponds to a sub-horizontal σ3 trending NNW-SSE. In this case 0.3 < ΦB < 0.5. At 3 km depth slice the attitude of the σ1 is highly variable overall plunging toward NNW. It corresponds to a sub-horizontal σ3 trending E-W in the axial sector, SW-NE and NW-SE at the most external volumes with a Bishop's ratio 0.4 < ΦB < 0.5. At the deepest depth slice (5 km), σ1 is sub-horizontal trending NNE-SSW to NW-SE, corresponding to moderately to high plunging σ3trending ENE-WSW, the ΦB is high variable experiencing values from 0.2 to 1 (Figure 6). The marked differences in the stress field pattern retrieved within the two seismogenic volumes (Figure 6, slice -1 vs. slices 1-3-5) can be addressed to the effect of the aforementioned decoupling ductile layer. The faulting style active in the top-volume is compatible with a spreading process involving the exposed Somma-Vesuvius edifice, as proposed by various previous studies (see references in D'Auria et al., 2014a). The strain field resulting from the subsidence of the Vesuvius and the asymmetric spreading of the southern portion of the Somma edifice creates an overall NS compression (see Figure 17 in D'Auria et al., 2014a). This ongoing process is also the source of the persistent seismicity located within the top-volume (Borgia et al., 2005; D'Auria et al., 2013, 2014a; Figures 5, 6). Additionally, the low ΦB values associated to stress inversion in the top volume confirm that the retrieved fields are strongly driven by the σ1. According to previous studies, the bottom-volume seems to be deeply related to a regional background stress field slightly perturbed by local heterogeneities in the volcanic structure and by the complex topography of the volcano. The intermittent behavior of the seismic activity in the deepest volume is probably due to a relation with the dynamics of the hydrothermal system: the pore pressure within the hydrothermal system can be perturbed by episodes of fluid injection that essentially influence the stress field pattern in the bottom-volume (Figures 5, 6; Chiodini et al., 2001; D'Auria et al., 2014a). The ΦB values associated to stress inversion in the bottom volume show that for the 1- and 3-km depth-slices the three principal stresses are well defined (overall, 0.3 < ΦB < 0.5). A quite different result was obtained for the deepest depth-slice, the 5-km one: here ΦB values show an high variability with values ranging from 0.5 to 1 and a σ3 overall trending NE-SW. This last result appears in accordance with the local minimum horizontal principal stress component (Sh) measured within the Trecase 1 well (located at the SE slope of the Mt. Somma-Vesuvius) as borehole breakout, showing an elongation in ENE-WSW direction (Montone et al., 2012).
Figure 6. Mt. Somma-Vesuvius. Stress field tensors retrieved from focal mechanisms data using the BRTM. Slices at −1, 1, 3, and 5 km-depth. Stress tensors have been computed over a regular grid of 1-km spacing, considering only nodes containing at least five FPSs. σ1 and σ3 axes are plotted as pairs of respectively red-blue arrows. The color of the circles corresponds to the retrieved ΦB value for each node (see scale on the right).
Campi Flegrei caldera (CFc) is located west of the city of Naples (Figures 4, 7). It is a partially submerged collapse caldera shaped by two main eruptive episodes: the Campanian Ignimbrite eruption (40.6 ka, Gebauer et al., 2014) and the Neapolitan Yellow Tuff eruption (14.9 ka, Deino et al., 2004). Between 12 and 3.8 ka there were three eruptive episodes followed by a long period of quiescence until the last eruption of Monte Nuovo in 1538 CE (Di Vito et al., 1999). During the last decades CFc is subjected to seismic activity, gas emissions and intense ground deformations (Chiodini et al., 2001; D'Auria et al., 2011). Recent events of uplift occurred in 1950–1952, 1969–1972, and in 1982–1984 (Del Gaudio et al., 2010). During the 1982–1984 episode there was a strong increase of the seismicity (D'Auria et al., 2011). D'Auria et al. (2014b) performed a detailed analysis of the events occurred during this last crisis in order to determine the spatial-temporal variations of the stress field within the CFc. The joint inversion of seismological and geodetic datasets evidences the presence of a weak NNE-SSW extensional stress field that is progressively overcome by a local volcanic one, active during the 1982–1985 unrest episode (D'Auria et al., 2014b).
Figure 7. Campi Flegrei. Focal mechanisms dataset plotted on a shaded map (A), on a N-S (B), and an E-W (C) cross sections. (D) The distribution of focal mechanisms on a triangular Frohlich diagram (Frohlich, 1992). The dataset consists of 217 events with 0 < M < 4 occurred between 1983 and 1984.
The FPS dataset analyzed in this research consists of 217 events with 0 < M < 4 occurred between 1983 and 1984 supplied by D'Auria et al. (2014b; Figure 7). Epicenters are mainly concentrated at the axial sector of the CFc. Hypocentral depths are up to 6 km. The three extreme slip classes are well represented, with a slight prevalence of the dip-slip normal solutions (Figure 7D). The stress field has been computed applying the BRTM, using a three-dimensional grid similar to that adopted for Vesuvius: 1-km spaced nodes, for each grid node all the FPSs within a radius of 1-km have been considered for the subset inversions. Only subsets related to volumes containing at least five FPSs have been inverted (Figure 7). Results of the BRTM stress inversion procedures are shown in Figure 8 and summarized for 1, 2, and 3 km depth-slices. Only a few volumes have been inverted for the 1 km depth slice. The resulting σ1 is high to moderately plunging and corresponds to a sub-horizontal σ3 trending E-W. The related ΦB values are in the range 0.5–0.8. At 2 km depth slice the attitude of the inverted σ1 is variable, with a prevalence of sub-vertical plunges while the σ3 trends mainly NNE-SSW. The corresponding Bishop's ratio is mainly 0.2 < ΦB < 0.6. At 3 km depth slice the attitude of the principal stress axes is variable and the corresponding Bishop's ratio ranges from 0 to 0.8. Nevertheless at this depth too there is a prevalence of sub-vertical plunging σ1 and a sub-horizontal NNE-SSW trending σ3. Overall, the key features of the stress field in the area are: a nearly sub-vertical σ1 at the center of the CFc and a low-plunging σ1 trending radially in the surrounding areas. The corresponding σ3 has a roughly horizontal NNE-SSW trend corresponding to the regional extensional stress field. Related ΦB values vary between 0.3 and 0.8 (Figure 8). According to D'Auria et al. (2014b), this result is compatible with the presence of a varying stress field related to a source of deformation, located at about 2.7 km depth, that during inflation and deflation episodes (associated to an increased seismicity) is able to overcome the weak regional extensional stress field having a NNE-SSW trend.
Figure 8. Campi Flegrei. Stress field tensors retrieved from focal mechanisms data using the BRTM. Slices at 1, 2, and 3 km-depth. Stress tensors have been computed over a regular grid of 1-km spacing, considering only nodes containing at least five FPSs. σ1 and σ3 axes are plotted as pairs of respectively red-blue arrows. The color of the circles corresponds to the retrieved ΦB value for each node (see scale on the right).
Long Valley caldera (LVc) is located in eastern California at the boundary between the Sierra Nevada block and the westernmost extensional Basin And Range Province (Figure 9). LVc develops inside a transfer zone hosted between NNW-SSE trending normal faults (e.g., Dickinson, 1979; Bosworth et al., 2003). This caldera is one of the youngest volcanic systems active in California. LVc has a surface of about 500 km2 and is surrounded by numerous basins and ranges (like Mammoth Mountain at SW, Glass Mountain at NE, Laurel Mountain at S). It is located near some important ENE dipping normal fault systems: Hartley Springs-Silver Lake Fault system to the North (HS, SL, in Figure 9), Hilton Creek and Round Valley Fault systems to the South (e.g., Prejean et al., 2002; Sorey et al., 2003; Bursik, 2009; HC an RV in Figure 9). Additionally, the LVc area is bounded to the east by the White Mountain Range and the related SW-dipping border faults (WMt in Figure 9). First volcanic activity can be dated approximately 760 ka ago as result of a large explosive eruption, during which more than 600 km3 of pyroclastics and ash (Bishop Tuff) have been erupted (Bailey et al., 1976). The emplacement of a resurgent dome (RD in Figure 9) located almost at the center-western sector of the caldera (started about 600 ka ago) has been causing an intense localized uplift (Hill et al., 1991; Langbein et al., 1993, 1995; Tizzani et al., 2009). Recent activity in the area consists of small eruptions and phreatic explosions at Inyo-Mono Chain (700–550 years ago; IC in Figure 9) and at Mono Lake, at NW of the LVc (about 200 years ago; Miller, 1985). Since 1978 seismicity and surface deformations have been continuously recorded in the area of the resurgent dome and in an active seismic zone along the southern margin of the caldera (Langbein, 2003). Location, size and geometry of magma bodies at LVc are still matter of debates (Carle, 1988; Battaglia et al., 1999, 2003a,b; Langbein, 2003; Tizzani et al., 2009; Guoqing, 2015). The regional active stress field in the western Basin and Range Province shows a minimum horizontal principal stress component (Sh) trending ESE-WNW, it rotates roughly to ENE-WSW at the border with the Sierra Nevada Range (Zoback, 1989, 1992; Heidbach et al., 2009). Breakout and seismic data depict a more complex pattern for the Sh across the LVc. NE-SW-trending Sh in the Resurgent Dome and at the South Moat Range, NW-SE-trending Sh in the West Moat and at Mammoth Mts. (Figure 9; Moos and Zoback, 1993; Bosworth et al., 2003, and references therein).
Figure 9. Long Valley. Focal mechanisms dataset plotted on a shaded map (A);, on a N-S (B), and an E-W (C) cross sections. (D) The distribution of focal mechanisms on a triangular Frohlich diagram (Frohlich, 1992). The dataset consists of 38,000 events with 0 < M < 6.4 occurred between 1978 and 2015. For sake of clarity only the events with m >= 3 are plotted. LVC, Long Valley Caldera (purple dashed line); RD, Resurgent Dome (purple dotted line); IC, Inyo Craters; WM, West Moat; MM, Mammoth Mts.; SM, South Moat; GM, Glass Mts.; WMt, White Mts. Red lines represent the main fault systems of the LVc area: SL, Silver Lake; HS, Hartley Springs Fault; HC, Hilton Creek; RV, Round Valley. See text for data sources.
For the Long Valley Caldera we used a dataset made up of about 38,000 FPSs of earthquakes occurred from 1978 to 2015 (0 < M < 6.4; Dataset by: NCEDC, 2014). These data were used to determine, with high resolution, the spatial variations of the stress field using the BRTM approach. In Figure 9 we plotted only the most energetic 3000 events (M > 3) in order to avoid an excessive overlapping of data. Epicenters are densely clustered at the southern sector of the LVc rim at the West Moat-Mammoth Mts.-South Moat Range sector. Additionally, many events are located along key tectonic lineaments of Hilton Creek and Round Valley to the south and along the western border fault of the White Mountains (Figure 9A). Hypocenters are essentially located above 20 km of depth. The shallowest events are concentrated at LVC and RD (Figures 9B,C). Kinematics of the analyzed FPSs are quite equally represented in the three main categories, with a slight prevalence of dip-slip ones (Figure 9D). The stress field has been computed on a regular three-dimensional grid of 5-km spacing. For each grid node all the FPSs within a radius of 5-km have been considered for the inversion. The stress field has been computed only at volumes containing at least 10 FPSs. Results of the stress inversion procedure are summarized in Figure 10 for depth-slices located at 0-, 10-, and 20-km. At 0 km depth slice most of the events fall in the LVc area, where the attitude of the inverted σ1 is quite variable, with a prevalence of sub-vertical plunges (NW sector) and sub-horizontal N-S to NE-SW trends in the remaining sectors. The corresponding σ3 is mainly sub-horizontal trending mainly E-W to NW-SE. The Bishop's ratio values are highly variable, ranging from 0.1 to 0.9. The 10 km depth slice samples most of the events of the analyzed dataset. Results can be divided up in two groups, the eastern one is dominated by a sub-horizontal σ1 trending N-S associated to a sub-horizontal E-W trending σ3. For the western sector, the retrieved stress field appears very similar to the one obtained for the shallowest 0-km slice; a sub-horizontal σ1 overall trending NE-SW associated to a sub-horizontal NW-SE trending σ3. Bishop's ratio values are highly variable ranging between 0.1 and 0.9, without a clear pattern (Figure 10). At the 20-km depth slice the stress inversion procedure highlights the presence of an overall stress field comparable to the corresponding nodes of the 10-km depth slice: in the easternmost region, a sub-horizontal NNW-SSE trending σ1, corresponding to a sub-horizontal ENE-WSW trending σ3. Bishop's ratios show a slight prevalence of lower values ΦB < 0.5. Summing up, a strong background stress field seems to dominate the investigated volume: it is characterized by a sub-horizontal NNW-SSE-trending σ1 and a sub-horizontal ENE-WSW-trending σ3. This field is clearly evidenced by the inversion results at the deepest slices in particular at 20-km depth slice (Figure 10). The region at the south of the caldera rim experiences a clock-wise rotation of the σ1 − σ3 axes up to 45°, as shown at 0- and 10-km depth slices (Figure 10). Our results can be interpreted as the effect of the interaction between a background regional stress field with the local volcano-tectonic structures. The presence of two distinct stress patterns at 10-km depth slice clues the presence of a regional stress field, characterized by a sub-horizontal σ1 roughlytrending from N-S to NNW-SSE associated with a sub-horizontal σ3 trending from E-W to NNE-SSW. The retrieved background stress field drives the evolution of the main tectonic trends of the area (Figure 8A), overcome in the western sector by a local volcano-tectonic regime, involving mainly the shallowest lithospheric portion. This last allows the above mentioned clock-wise rotation of the σ1 − σ3 axes well documented at the −10-km slice (Figure 10). Our results are in agreement with Sh found in previous studies, derived by the analyses of earthquake focal mechanisms, bore-hole breakouts, fault offsets, hydraulic fracturing, and alignment of young volcanic vents. In detail, the σ1 − σ3 axes attitude derived for the easternmost subset inverted at −20-km slice is in good agreement with the ENE-WSW-trending Sh retrieved at the border with the Basin and Range and Sierra Nevada Range (Moos and Zoback, 1993; Prejean et al., 2002; Bosworth et al., 2003, and references therein).
Figure 10. Long Valley. Stress field tensors retrieved from focal mechanisms data using the BRTM. Slices at 0, 10, and 20 km-depth. Stress tensors have been computed over a regular grid of 5-km spacing, considering only nodes containing at least 10 FPSs. σ1 and σ3 axes are plotted as pairs of respectively red-blue arrows. The color of the circles corresponds to the retrieved ΦB value for each node (see scale on the right).
Discussion and Conclusions
In volcanic environments, a spatio-temporal analysis of the stress fields represents a valuable approach to infer the volcano dynamics (Wyss et al., 1992; Hardebeck and Michael, 2006; Gudmundsson et al., 2009; Plateaux et al., 2014; Costa and Marti, 2016). Stress field variations play a key role in driving magmas and/or fluids migration. On the other hand, injection of fluids can be responsible for local variations of the stress field allowing the reactivation of locked faults. Stress changes may influence fluid circulation within the shallow crust and they can be also responsible for the triggering of tectonic earthquakes associated to strong variations in the dynamics of volcanic eruption and behavior of hydrothermal phenomena (Linde and Sacks, 1998; Hill et al., 2002; Walter et al., 2007).
During the last decades, a wide range of stress inversion techniques has been proposed, some of them specifically conceived to manage seismological datasets. Several key aspects, that could impact on the reliability of retrieved results, require a short discussion. First of all, the discernment of the actual fault plane among the nodal planes of a FPS represents a known critical step in many analytical techniques of stress inversion. (e.g., Gephart and Forsyth, 1984; Michael, 1987; Angelier, 1990). A good solution can be an a-posteriori approach that pick the actual fault following a best-fit procedure or a massive computational approach on small datasets (Michael, 1987). Of course, it implies a complication in the processing procedure that can hide pitfalls. Only a few analytical methods do not require this choice, for instance Angelier (2002) based on the slip shear component criterion. Additionally, all graphical (e.g., RDM) or graphical-derived (e.g., RTM, BRTM) techniques do not require this pre-selection; this is a valuable asset that makes these processing approaches as robust as they are simple. As premised, graphical-derived methods are based on the implementation of an algorithm that is able to figure a probability function over the focal sphere for both σ1 and σ3 principal stress attitude. The analytical implementation of the classical graphical methods allows the efficient managing of large datasets following a proper statistical approach (e.g., RDTM; Ramsay and Lisle, 2000). Generally, the output of these procedures needs a strong graphical post-processing in order to obtain an adequate representation of results (e.g., MORE; Massa, 2003). BRTM proposes a solution to this limitation offering a standard procedure of data ingestion, processing and graphical post-processing in both 2- and 3-Dimensional rendering. All these task can be performed through the use of editable scripts run in the same computational environment. A known drawback of stress inversion procedures (for both graphical and analytical) is that they generally lack of a robust statistical estimation of the uncertainty on the retrieved tensors. To overcome this lack, BRTM performs an estimation of solution uncertainty and trough the implementation of the approach of Jackson and Matsu'ura (1985), BRTM is able to delimit the confidence intervals around the σ1 and σ3 retrieved axes (D'Auria and Massa, 2015). Another key aspect to consider is that very frequently datasets to be processed are large and heterogeneous. Without an a-priori selection, many datasets collect faults/FPS related to different stress fields. For instance, seismological datasets collected across wide lithospheric volume, mesoscale faults hosted in a limited rock volume but generated during different tectonic events, etc. The solution to identify the different contributions from multiple sources can be a clustering approach as the MIM (Yamaji, 2000; Otsubo et al., 2008) or the application of other automatic analytical procedures (Angelier and Manoussis, 1980). These approaches allows the identification of the different stress fields but they are not designed to give a quantitative assessment of the solution quality; additionally they are not able to locate the spatial distribution of the retrieved tensors (Yamaji, 2000; D'Auria and Massa, 2015). The relevance of this point becomes larger considering the seismological datasets collected in volcanic areas. Here, the retrieving of stress field spatial variations represents a crucial task: sensible variation in stress axes attitude can characterize stress field active in contiguous volumes (e.g., D'Auria et al., 2014a,b; Plateaux et al., 2014). For this reason, unsupervisioned stress inversions performed on an unselected dataset can be quite useless. A similar discussion can be done for the analysis of stress field temporal variations. The ideal way to obtain a reliable stress field inversion would be the analysis of a dataset covering a time interval as short as possible, in order to consider the responsible stress field quite constant in its parameters (i.e., the attitude of principal stress axes and the related ΦB). The preliminary temporal selection of data can be unfeasible in case of mesoscale faults also when collected in a limited volume of rock: several tectonic “phases” could have superimposed in the geological record. Conversely, the temporal selection of data can be conveniently done in the analysis of seismological datasets where the focal parameters are well known. In volcanic environments, a spatio-temporal analysis of the stress fields represents the best way to infer about the volcano dynamics (Wyss et al., 1992; Hardebeck and Michael, 2006; D'Auria et al., 2014b; Plateaux et al., 2014). In this perspective, a supervisioned splitting of data in 3D sub-volumes represents the best solution to retrieve the spatial distribution of active coeval stress fields. As a final consideration about the stress inversion procedures, it should be noted that the publication of a rigorous formulation of a technique is not enough to determine its success. A strong limitation to the dissemination of a processing procedure consists of the availability of a free or open-source platform of implementation. Available methods are frequently implemented by authors and freely distributed to the community only as PC programs. For instance, the Direct Inversion algorithm was implemented by the author in the executing software TENSOR (Angelier, 1990), the Multiple Inverse Method can be performed through a set of executable supplied by the author (Yamaji, 2000), RDM and RTM can be applied using RDTM, supplied by authors both as executing program than as code (Ramsay and Lisle, 2000). The availability of an editable code represents a key point to allow a flexible use of a technique, allowing, in addition, a facilitation in its spreading over the community. A BRTM implementation in MATLAB® was proposed by the Authors, allowing a basic stress-inversion procedure and an advanced plot of results (Figure 3; D'Auria and Massa, 2015). The implementation of the basic inversion algorithm can be easily exported to open-source and free platform. Results can be plotted using the preferred platform. The graphical post-processing proposed by D'Auria and Massa (2015) was implemented in MATLAB®. It would be useful a revision in order to make it available to free platforms.
According to previous researches, the new stress-inversions discussed in this paper (Figures 6, 8, 10), have shown that the stress field in the studied volcanoes results from the interaction of a regional background field with local volcanic structures and dynamics. In detail, during the 1983–1984 seismic crisis in the Campi Flegrei area, a sub-vertical σ1 dominates the axial volume of the caldera. Conversely, a low-plunging σ1 appears trending radially in the surrounding volumes. The corresponding σ3 attitudes are roughly sub-horizontal NNE-SSW trending, in accordance with the regional Sh retrieved by breakout data (Montone et al., 2012). The retrieved stress fields are in accordance with Zuppetta and Sava (1991). The background regional stress field has been also modeled by D'Auria et al. (2014b) using a joint inversion of a geodetical-seismological dataset, obtaining a sub-horizontal σ3 trending N-S. This result is in good accordance with the Mt. Somma-Vesuvius where D'Auria et al. (2014a) found a very similar configuration for the regional stress field. The retrieved variability of the stress field can be related to fluids migration within a planar crack probably located at shallow depth and possibly responsible for unrest episodes (D'Auria et al., 2014b; Macedonio et al., 2014). At Mt. Vesuvius, rheological variations of the involved geological units and the action of key volcano-tectonic structures seem to play a significant role in determining the local stress fields (Figures 4–6; D'Auria et al., 2014a). The configuration of the retrieved stress fields shows the superposition of two volumes with a marked difference in their evolution history. A top volume dominated by a gravitational volcanic spreading that allows the setting of extensional stress fields (low ΦB values and sub-vertical σ1) active in the analyzed sub-volumes. A bottom volume strictly related to a regional extensional background stress field in accordance with the Sh derived by breakout data (Figure 6; Borgia et al., 2005; Montone et al., 2012; D'Auria et al., 2014a). The computation of the stress field using the BRTM on a regular three-dimensional grid allows the 3-D figuration of the stress fields “simultaneously” acting from the surface to about 8-km depth (Figures 5, 6). This approach appears very useful in supporting studies on the volcano-dynamics of complex system as the Mt. Somma-Vesuvius. Finally, analyses performed at Long Valley Caldera show a complex configuration of the stress field pattern associated to a volcanic district developed inside a transfer zone hosted between NNW-SSE trending normal faults (e.g., Dickinson, 1979; Bosworth et al., 2003). A dataset of 38,000 FPSs allows to retrieve with high resolution, the spatial variations of the stress field active in the first 20 km of depth. A regional background stress field dominates the deepest portion of the investigated volume accordingly to the ENE-WSW-trending Sh retrieved at the border with the Basin and Range and Sierra Nevada Range (Moos and Zoback, 1993; Prejean et al., 2002; Bosworth et al., 2003). In the shallowest lithospheric portions this regional stress field has been overcome by the volcano-tectonic regime; this is clear in particular at the 10 km depth-slice (Figures 9, 10). The managing of the very large dataset has been approached using a regular sampling of data inverted using the BRTM. The result is a very detailed figuration of the spatial variation of the active stress fields in the 500 km2 Long Valley Caldera, one of the youngest volcanic systems active in California.
The above results confirm that the application of stress inversion procedures to volcanic environments provides crucial information about the volcano dynamics with particular care to its interaction with regional tectonics. In detail, BRTM has shown to be very efficient in managing heterogeneous datasets in a user-friendly processing environment, with a clear graphic output and an efficient evaluation of the regions of confidence around the retrieved principal stress axes. The proposed processing approach of FPS datasets in active volcanic areas is suitable to be applied to a wide range of contexts. Finally, the results presented in this work suggest that these methods could be useful also as a near real-time monitoring tool to characterize spatial and temporal variations in the stress field linked to a volcanic unrest (e.g., Toda et al., 2002; Plateaux et al., 2014). A final consideration concerns the relevance of the stress-inversion approach based on the integration and/or the joint inversion of seismological and geodetical datasets. The joint inversion of ground deformation and focal mechanism is more efficient than the mere comparison of the results obtained by the separate inversion (Segall, 2013; D'Auria et al., 2014b; Viccaro et al., 2016). Spatial-temporal analysis of the stress field derived from seismological datasets associated to a continuous recording of ground deformations (remote and/or field classical techniques) could be a reliable tool to monitor volcano dynamics and infer about their evolution.
BM, LD, EC, and AD: rock mechanics, stress inversion, join inversion, and focal mechanisms.
This research is financially supported by: MED-SUV project (European Union's Seventh Programme for research, technological development and demonstration, Grant Agreement Number 308665); Università degli Studi del Sannio FRA 2014–2015 “Modeling of geological processes” (P.I. B. Massa).
Conflict of Interest Statement
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
The handling Editor declared a shared affiliation, though no other collaboration, with the authors BM, LD, and EC and states that the process nevertheless met the standards of a fair and objective review.
Thanks are due to the two Referees, Eisuke Fujita and Mimmo Palano, to the Associate Editor Antonio Costa and to the Chief Editor Valerio Acocella for the constructive and valuable review that greatly improved the manuscript. BRTM can be accessed as Electronic Supplement to D'Auria and Massa (2015) following the link: http://srl.geoscienceworld.org/content/early/2015/03/17/0220140153 (Last accessed on 31st October 2016).
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Keywords: stress field, focal mechanism, BRTM, volcano-tectonics, monitoring
Citation: Massa B, D'Auria L, Cristiano E and De Matteo A (2016) Determining the Stress Field in Active Volcanoes Using Focal Mechanisms. Front. Earth Sci. 4:103. doi: 10.3389/feart.2016.00103
Received: 30 April 2016; Accepted: 11 November 2016;
Published: 29 November 2016.
Edited by:Antonio Costa, National Institute of Geophysics and Volcanology, Bologna, Italy
Reviewed by:Eisuke Fujita, National Research Institute for Earth Science and Disaster Prevention, Japan
Mimmo Palano, National Institute of Geophysics and Volcanology, Roma, Italy
Copyright © 2016 Massa, D'Auria, Cristiano and De Matteo. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Bruno Massa, firstname.lastname@example.org