Next Article in Journal
A Broad-Area Method for the Diurnal Characterisation of Upwelling Medium Wave Infrared Radiation
Next Article in Special Issue
Freeze/Thaw-Induced Deformation Monitoring and Assessment of the Slope in Permafrost Based on Terrestrial Laser Scanner and GNSS
Previous Article in Journal
Quantifying the Effects of Normalisation of Airborne LiDAR Intensity on Coniferous Forest Leaf Area Index Estimations
Previous Article in Special Issue
Potential and Limitation of SPOT-5 Ortho-Image Correlation to Investigate the Cinematics of Landslides: The Example of “Mare à Poule d’Eau” (Réunion, France)
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Monitoring the Rapid-Moving Reactivation of Earth Flows by Means of GB-InSAR: The April 2013 Capriglio Landslide (Northern Appennines, Italy)

1
Department of Earth Sciences, University of Firenze, Via La Pira 4, 50121 Firenze, Italy
2
Department of Chemical and Geological Sciences, University of Modena and Reggio Emilia, Via Campi 103, 41125 Modena, Italy
*
Author to whom correspondence should be addressed.
Remote Sens. 2017, 9(2), 165; https://doi.org/10.3390/rs9020165
Submission received: 23 November 2016 / Revised: 31 January 2017 / Accepted: 13 February 2017 / Published: 17 February 2017
(This article belongs to the Special Issue Remote Sensing of Landslides)

Abstract

:
This paper presents the main results of the GB-InSAR (ground based interferometric synthetic aperture radar) monitoring of the Capriglio landslide (Northern Apennines, Emilia Romagna Region, Italy), activated on 6 April 2013. The landslide, triggered by prolonged rainfall, is constituted by two main adjacent enlarging bodies with a roto-translational kinematics. They activated in sequence and subsequently joined into a large earth flow, channelizing downstream of the Bardea Creek, for a total length of about 3600 m. The displacement rate of this combined mass was quite high, so that the landslide toe evolved with velocities of several tens of meters per day (with peaks of 70–80 m/day) in the first month, and of several meters per day (with peaks of 13–14 m/day) from early May to mid-July 2013. In the crown area, the landslide completely destroyed a 450 m sector of provincial roadway S.P. 101, and its retrogression tendency exposed the villages of Capriglio and Pianestolla, located in the upper watershed area of the Bardea Creek, to great danger. Furthermore, the advancing toe seriously threatened the Antria bridge, representing the “Massese” provincial roadway S.P. 665R transect over the Bardea Creek, the only strategic roadway left able to connect the above-mentioned villages. With the final aim of supporting local authorities in the hazard assessment and risk management during the emergency phase, on 4 May 2013 aerial optical surveys were conducted to accurately map the landslide extension and evolution. Moreover, a GB-InSAR monitoring campaign was started in order to assess displacements of the whole landslide area. The versatility and flexibility of the GB-InSAR sensors allowed acquiring data with two different configurations, designed and set up to continuously retrieve information on the landslide movement rates (both in its upper slow-moving sectors and in its fast-moving toe). The first acquisition mode revealed that the Capriglio and Pianestolla villages were affected by minor displacements (at an order of magnitude of a few millimeters per month). The second acquisition mode allowed to acquire data every 28 seconds, reaching very high temporal resolution values by applying the GB-InSAR technique.

Graphical Abstract

1. Introduction

In Italy, large complex landslides are recurrent phenomena [1,2,3,4] responsible for destruction of assets and infrastructure, and major economic losses. These phenomena associate a combination of movements, starting as multiple rotational or rotational-translational slides, affecting weak clayey rock masses in the source areas and evolving downhill into an earth slide or flow as the material starts to lose coherence. In the northern flank of the Tuscan-Emilian Apennines (Emilia-Romagna Region, Northern Italy), the Regional Geological Survey has identified more than 70,000 landslides, covering one fifth of the hilly and mountainous territory [5]. Due to the outcropping lithology, structural setting and geomorphological evolution, about 90% of them are large, ancient earth flows. The majority of these slope movements originated after the Last Glacial Period (approximately from 30,000 BP onwards [6]), and grew during the Holocene wettest periods through the superimposition of new earth flows. In spite their ancient origin, these phenomena are still very hazardous, alternating long periods of inactivity with sudden reactivations. Long-lasting rainfalls are the most frequent triggering factors during the entire year, while melting of snow cover is particularly effective in the months of March and April, leading to an increase of landslide occurrences and recrudescence [7]. The reactivation, partial or total, of large earth flows is the main problem the geologists of Emilia Romagna Region have to face nowadays [8].
The large complex ancient landslides, such as Ca’ Lita [1,9,10,11], Valoria [12,13,14], Berceto [15], Corniglio [16], Roccapitigliana [17], Ponte Dolo [18], Lavina di Roncovetro [19], and Morsiano, Cervarezza, and Signatico [20], are just few examples of widely investigated instability phenomena following their reactivations in recent times. Some of the performed studies employed ground-based techniques using, for example, seismic [21] and hydrogeological instruments [22]. Other studies exploited the contribution of high-resolution DEMs retrieved from photogrammetry and airborne LiDAR [14] and hyperspectral data [13]. Rosi et al. [11] established a wireless sensor network for monitoring purposes. In a few cases InSAR (interferometric synthetic aperture radar) approaches, both ground-based and space-borne [18], have been used. All of these studies provide data on landslide deformation pattern and style: the movement of most of these landslides is retrogressive on the source areas, advancing in the mid-lower sectors and partially widening on the flanks [9]. Additionally, information on the variability of the rheological behavior and their pertaining velocities are usually given: in the upper part, the rotational/translational slide evolves with movements of the order of few mm–cm per day while, at the toe, the earth slide/flow moves at velocities of several (tens of) meters per day. The last fifteen years witnessed an increasing number of techniques, applications, and studies aimed at demonstrating the applicability of images acquired by ground-based synthetic aperture Radar (GB-SAR) sensors to continuously monitor ground displacements related to slope instability [23,24,25,26,27,28,29]. These studies demonstrated the capabilities of the GB-InSAR technique to complement the existing tools for monitoring ground displacements, recording deformation phenomena characterized by a wide range of deformation rates, which roughly range from a few millimeters per year [26] up to a few meters per day [30]. Dealing with fast-moving landslides, the time lapse during consecutive SAR acquisitions, a few minutes in most of the available systems can be too long with respect to the velocity of some parts of the investigated scenario. If atmospheric contributions, thermal noises, and other sources of decorrelation are properly corrected [31,32], phase ambiguities could occur if the landslide velocity is high (i.e., several meters per day).
To overcome the above-mentioned limitations, and to map deformations induced by fast-moving landslides, a new configuration of the GB-InSAR has been performed, exploiting the high system capability in terms of image acquisition. This paper shows an application of this new acquisition method for the Capriglio landslide, activated in the Tizzano Val Parma municipality (Emilia-Romagna Region, North Italy) after a period of persistent rainfall. Consequently, a continuous surveillance of the landslide dynamic, both in its upper and middle-lower parts, was believed of paramount importance and a prerequisite for providing an early warning of potentially catastrophic displacements. After this event, the Emilia-Romagna Region Civil Protection Department (DPC-RER), responsible for the management of the emergency, appointed the Earth Sciences department of the University of Firenze (DST-UNIFI) to start a GB-InSAR campaign in order: (i) to monitor the landslide kinematics; (ii) to measure the possible ground deformations in correspondence of the urbanized areas and of the landslide toe approaching the Antria bridge in the Bardea Creek; and (iii) to support the local authorities in emergency management. Moreover, aerial optical surveys were performed, to map with high detail the evolution of the area covered by the landslide. Field and GPS surveys were also conducted with the aim of supporting the landslide mapping activities.
In this paper, the results of the GB-InSAR monitoring are presented. The main goal of the GB-InSAR application was the recording of the initial rates of movement, when the landslide could be classified as “moderate” to “rapid”, according to the Cruden and Varnes classification [33].
The purpose of this paper is two-fold: to show the capability of the employed GB-InSAR system to record the movement of a rapid landslide and to perform long-term and real-time monitoring.

2. The April 2013 Capriglio Landslide Reactivation

2.1. Geologic-Geomorphic Setting

The Capriglio landslide is located in the Northern Apennines within the upper sector of the Enza River basin. The study area is placed within the municipality of Tizzano Val Parma (Province of Parma, Emilia Romagna Region, Figure 1), about 90 km west of the city of Bologna and about 35 km south-southwest of the city of Parma. In the spring of 2013 the Parma Province was affected by a large number of landslides, as a result of heavy and persistent precipitation (rain and snow), occurring between January and April, and a rapid snow melt in early spring. This resulted in the triggering of about 1400 mapped landslides distributed in over 100 municipalities, causing more than 60 evacuees and severe damages to urbanized areas, infrastructure, and cultivated and pasture lands. In particular, on 6 April 2013, a major event occurred in the Tizzano Val Parma municipality (one of the most severely affected in the whole region), where a large, rapidly moving complex landslide activated. The risk posed by the landslide represented a major concern for local authorities and led to a civil protection emergency.
The landslide affected a middle-low mountain area where weak rock masses, constituted by an upper Cretaceous turbiditic deposit (the Mount Caio Flysch, part of the Ligurian Units), extensively outcrops [34] (Figure 2). It is formed by thick-bedded calcareous sandy turbidites and marlstones, with a basal clay chaotic complex. In the study area, the Flysch strata dip towards the SE sectors with low to middle angles. In addition to the bedrock, the Capriglio landslide also involved the quaternary cover, mainly represented in the area by smaller pre-existing active and inactive slope movements and related colluviums. In addition to the described event, in situ surveys and available thematic maps indeed highlighted in the study area the presence of many geomorphological features ascribable to pre-existing landslides of different types and ages. Within the Bardea basin, a certain number of instability events can be identified, including complex movements and mud flows. Despite most of these phenomena having been mapped as quiescent, their presence bears witness to the diffuse gravitational instability characterizing the entire basin (Figure 2).
The Capriglio landslide (Figure 3A) stretches from an altitude of 980 m a.s.l.(above sea level) to about 630 m a.s.l., covering an area of approximately 0.92 km2 over a length of about 3.6 km, with a travel angle of about 6°. During field surveys, the deposit’s maximum width was measured (about 350 m) and a preliminary estimation of the maximum movement rate was evaluated by observing consecutive landslide toe locations (Table 1).
The landslide developed on the NE flank of the Caio mountain (1587 m a.s.l.) and channelized within the riverbed of Bardea Creek, a 10-km long left tributary of the Enza River. The landslide area includes mainly cultivated fields, wood, and pasture land and, due to the huge extent and rapid movement, the resulted geomorphological effect was remarkable. It can be considered the largest reactivation landslide documented in the Emilia Romagna Region archives.
The upper part of the landslide destroyed ca. 450 m of the provincial roadway S.P. 101 and put at high risk the villages of Capriglio and Pianestolla. These two hamlets are located in the upper watershed area of the Bardea Creek and were seriously threatened (directly and indirectly) by potential retrogression of the main scarps. Moreover, the advancement of the toe of the landslide, characterized by a velocity with an order of magnitude of several (tens of) meters per day, represented a real risk for the Antria bridge, located downstream on the Bardea Creek. Such road infrastructure is a transect of the “Massese” provincial roadway (S.P. 665R) and it was considered very strategic for a long time since it was the only local roadway left intact and able to connect the above-mentioned villages, as well as the local economic activities with national sales channels. Fortunately, despite the severity of this event, no fatalities occurred and Capriglio and Pianestolla villages suffered minor damages, though some houses and agricultural warehouse were completely destroyed.
The landslide kinematics included two large adjacent bodies that rapidly activated in sequence, generating some compound landslides, and joined together downstream into a high mobile larger phenomenon. As a whole, such evolving movement can be classified as a roto-translational earth slide with an enlarging activity subsequently evolving in earth flow (complex landslide [33,35,36]). Therefore, it can be considered as a combined system of two large mass movements (Figure 3B): (i) on 6 April a right bank crown developed downstream of Capriglio village and a landslide started to move as a rotational earth slide, evolving shortly after into a chaotic mass with morphological evidence typical of flows; (ii) on 12 April this landslide activated an area just upstream of the village of Pianestolla, partially characterized by pre-existing instability phenomena, causing an additional translational mechanism (left bank landslide), which affected weathered slope-dipping flysch strata, completely destroying the sector of provincial roadway S.P. 101, and joined into the valley with the first movement, evolving as a large-scale fast earth flow. Morphological evidences in this area and their temporal sequence evolution indicated that the first earth flow determined an unloading of the slope near Pianestolla, inducing the development of a further retrogressive movement, with the rupture surface extending towards the watershed.
The fast superimposition of the collapsed mass on the narrow valley of Bardea Creek determined high availability of water from the main channel and its afferent hydraulic network, which largely permeated within the new chaotic mass, inducing a significant material mobilization. This circumstance resulted in a remarkable advancement of the lower sector of the landslide, which threatened the Antria bridge on the Bardea Creek, located 2 km downstream of Pianestolla (Figure 3C). In addition, the movement of the landslide toe, though highly mobile, caused a multiple unloading of the right flank of the valley, which, in turn, triggered a series of landslides, further increasing the total volume of the landslide system. These secondary landslides (Figure 3D), moving NNE (i.e., almost perpendicularly to the main movement direction of the main landslide), partially dammed the Bardea Creek valley and caused a dramatic decrease of the downstream movement of the Capriglio landslide, one hundred meters before the bridge.
The landslide toe evolved with velocities of several tens of meters per day (with peaks of 70–80 m/day) for the first month after the trigger, and of several meters per day (with peaks of 13–14 m/day) from early May to mid-June 2013. These movement rates allowed the phenomenon to be included in the “rapid” and “moderate” classes of the Cruden and Varnes classification [33].

2.2. Rainfall Leading to Reactivation

The landslide occurred after some weeks of persistent rainfall affecting the area (Table 1). Despite the lack of rain gauges close to the landslide, some meteorological stations were available near the area. Hence, the rainfall data recorded at the rain gauge located at Musiara Superiore hamlet have been used. Being located 2.5 km NW of Capriglio, this rain gauge is the closest to the landslide and is installed at an elevation (980 m a.s.l.) similar to the altitude of the crown area of the landslide (982 m a.s.l.). From a climatic point of view, this area of the Apennine range is characterized by an annual average rainfall of about 1000–1200 mm. The highest precipitation levels are recorded in autumn (October–November) and in spring (March–April). The month of July, and secondarily February, are the months with the lowest precipitation. In addition to the rainfall, a main role is played by rapid melting of snow during the spring, as a consequence of the rapid temperature increase at a relatively low altitude.
Analysis of rainfall data of the period 2006–2013 (Figure 4) allows the identification of intense events in the pluviometric regime before the landslide occurrence, evaluating their role as a trigger. Rainfall data, analyzed month by month, for the 2006–2013 period highlight that February and March 2013, with 125 and 244 mm of cumulated rainfall, respectively, are the wettest months of the analyzed period. It is clear that intense precipitation before the trigger (15-days accumulated rainfall of 180.8 mm) contributed to the increase of the critical state primed by the significant accumulation of rainfall that occurred during January and February, causing the complete saturation of soil and, consequently, the trigger of the landslide.

2.3. Spatio-Temporal Evolution of the Reactivation

The temporal evolution of the Capriglio landslide system has been mapped (Figure 5) through the synergic use of aerial and satellite images and GPS surveys [37,38]. In particular, the following surveys have been performed:
- On 16 April 2013, a 1.6 m ground resolution Ikonos-2 image was acquired to perform a preliminary landslide boundary assessment. The image was elaborated in rush mode to support emergency response activity of the civil protection in the framework of the Copernicus program of the European Commission.
- On 4 May 2013 an aerial photographic survey was performed in order to acquire high-resolution images of the landslide system and to perform a second preliminary landslide boundary assessment. In order to avoid image geometrical distortions, the cameras were placed in the aircraft hatch in order to obtain a line of sight in a perpendicular direction as much as possible with respect to the topographic surface. The line of flight was aligned along the landslide longitudinal axis at an average altitude of 300 m above ground level, leading to an image geometric resolution of about 20 cm. Other aerial images were also acquired from different lines of sight in order to give a global picture of the landslide. Image overlapping allowed a manual mosaicking and georeferencing in a GIS environment using a previously acquired DEM and aerial optical image of the Emilia Romagna Region as reference base maps.
- On 13 May 2013, a GPS survey of the landslide toe was performed to obtain a further estimation of its location.
- At the end of July 2013 a drone aerial optical survey was performed by Regional Agency for Civil Protection—Emilia Romagna Region, allowing mapping of the final landslide extent.
The landslide boundary assessment allowed us to estimate the multi-temporal evolution of the landslide area, permitting the monitoring of the landslide toe velocity with respect to the reference satellite map acquired on 16 April 2013 (Figure 5). This helped to estimate the landslide toe velocity in the first two weeks of the post-triggering phase: from about 80 to 15 m/day, corresponding to the “rapid” and “moderate” classes according to the Cruden and Varnes classification [33]. In addition, it was also shown that, besides the Capriglio and Pianestolla villages, the landslide toe evolution exposed the Antria bridge of the “Massese” 665R provincial road crossing the Bardea Creek to a very high degree of danger.

3. GB-InSAR Methods and Operative Approach

On 23 May 2013, a GB-InSAR system was installed in Lagrimone, a village located on the opposite slope of the Capriglio landslide, in the Tizzano Val Parma municipality (Figure 6). The objective was the displacement monitoring of the Capriglio landslide toe, as well as the detection of possible millimetric movements affecting Capriglio and Pianestolla villages. The selected location for the installation was revealed to be the best for this purpose. The system employed is a portable SAR device, known as LiSA-Mobile: it is an evolution of the prototypal GB-InSAR instrument, named LiSA (acronym of Linear SAR), developed by the Joint Research Center (JRC) of the European Commission and its spin-off, Ellegi-LiSALab Company [39,40,41]. Beyond the employed technique, there is the exploitation of microwave radiation of the electromagnetic spectrum: by calculating the time that the radiation needs to go from the sensor to a target and back, it is possible to evaluate the distance between the sensor and the target. By comparing successive acquisitions, eventual target displacement, with sub-millimeter precision, can be detected. The comparison is based on the evaluation of the phase difference between the transmitted and the received wave. It is indeed possible to correlate the phase variation with the target displacements: in the same topographic conditions, during subsequent radar acquisitions, the phase shift of the wave mainly depends on occurred target displacements. Phase shift also depends on atmospheric and noise components, which must be properly corrected in order to isolate displacement contributions [32,42].
In every radar system, spatial resolution is proportional to the antennas’ length. In ground-based (GB) systems, a suitable resolution requires a physical antenna too large to be practically transported and mounted. To overcome this limit, synthetic aperture radar (SAR) systems have been implemented. SAR is a technique that uses signal processing to improve the resolution beyond the limitation of the physical antenna aperture. In SAR techniques, the motion of a physical antenna along a rail (a few meters long) is used to ”synthesize” a larger antenna. SAR imaging consists of irradiating the targets with a small physical antenna, transmitting a stream of pulses from different positions along the rail. The antennas repeatedly illuminate with successive pulses a specific target to synthesize an aperture that is the same size as the rail length: as the antenna moves, it provides repeated observations of each spot of the scenario. The echo of each pulse is received, recorded, and analyzed [25,43,44,45,46,47]. This allows SAR to achieve high resolution with small physical antennas.
The instrument employed in Tizzano Val Parma is a new generation ground-based system, whose main components are: (i) a 330 cm linear rail (maximum synthetic aperture of 300 cm), along which two antennas that move with millimetric steps to define the synthetic aperture; (ii) a microwave transmitter, that produces, step by step, continuous waves around a center frequency (17.2 GHz); (iii) a receiver that records the amplitude and the phase of the microwave signal backscattered by the target; (iv) the antenna support; (v) a power base, containing a UPS (uninterruptible power supply) to guarantee a constant electrical supply, and boards to increase memory. The system maintains the characteristics of accuracy (sub-millimeter) of a classical LiSA system, but it is implemented with some features which make it easier and faster to install: it has been conceived in a modular configuration with the main components separately arranged, in order to reduce the weight and dimensions of each element. The system is also characterized by higher versatility than the previous instruments, in terms of possible acquisition configurations. A significant advantage is indeed given by the possibility to choose the synthetic aperture length to obtain different SAR configurations, which influences the acquisition time and consequently the detectable velocity. Dealing with a “moderate” to “rapidly” moving landslide, the main limiting factor of the existing systems is the time to acquire a single image, typically ranging from few to several minutes [24]. In relation to the observed scenario and the velocity of the analyzed displacement, a larger or smaller aperture can be selected to analyze faster or slower velocities. The use of a shorter aperture allows acquiring more data in shorter times, albeit at the expense of spatial resolution and coverage, detecting higher velocities than the typical detectable velocity values. In other words, it determines the acquisition of more interferograms in reduced timespans, but it also implies a reduction in the azimuth resolution, which is inversely correlated to the linear rail length [48]. Thanks to this GB-InSAR characteristic, in the early period of the Capriglio landslide monitoring activity, two acquisition modes were arranged: fast and slow (Figure 6).
Fast mode was performed reducing the linear rail length to 1 m, allowing SAR to detect the whole landslide body, and its high-velocity values, with a reduced azimuth resolution (Figure 6A–C). Slow mode acquisitions were performed by using the maximum linear rail length (3 m), in order to detect an area that also included the villages of Capriglio and Pianestolla, with acceptable azimuth resolution (Figure 6B,C). This configuration is more useful to detect lower displacements, eventually affecting buildings/structures. The differences in the detectable areas (Figure 6) are connected to the needs of compromising between temporal and spatial resolution: the reduction of azimuth resolution in “fast” acquisition mode can be considered acceptable if the acquired data are not so far from the instrument location; therefore, fast acquisitions have been exploited to detect a smaller area (Figure 6A–C).
Initially, “fast” acquisitions were interchanged with “slow” acquisitions to detect eventual slower displacements affecting Capriglio and Pianestolla villages. During this first period, in order to guarantee a continuous monitoring of the villages, slow mode acquisitions were performed throughout the whole day, suspending them only few minutes a day to perform fast acquisitions. After landslide deceleration, only slow mode acquisitions were performed until December 2014.
Some difficulties partially limited the GB-InSAR application on the presented test site: (i) the widespread vegetation cover, which in some measure reduced the observable scenario (low coherence of the radar signal [49]), but that, fortunately, did not affect the landslide body and the villages; (ii) the high distance between the radar location and the study area, which determined a reduced azimuth resolution in correspondence with the farthest portion of the scenario, and which implies a very high variation of the atmospheric contribution on the whole scenario; and (iii) the intrinsic GB-InSAR feature to be able to detect only the component of the displacement vector which is parallel to the instrument line of sight (LOS), which implied an underestimation of the detected displacements in specific sectors of the study area (mainly located near the village of Pianestolla, where the movement direction is nearly perpendicular to the radar LOS (about 35% of the estimated real displacement).
Proper atmospheric correction has been applied to radar images, in order to reduce the related decorrelation effect. The atmospheric delay is a function of changes in the refractive index, which depends on temperature, humidity, and pressure differences. As the investigated scenario is affected by oscillation of these parameters, a proper correction is crucial in order to accurately interpret radar data. The relation between path delay and atmospheric parameters has been determined under the assumption of a uniform atmosphere (constant atmospheric parameters). Specifically, the atmospheric delay has been estimated on stable areas, where the phase of the radar signal only depends on the atmospheric component and random noise, following the approach proposed by [31] and [32]; these areas have also been selected on the basis of high coherence values of the radar signal (Figure 6C). The atmospheric component is identified in the spatial low frequency component of the phase shift. Assuming a linear relation between the effect of the atmosphere and the distance instrument-target, the range variation of the atmospheric delay has been interpolated for the whole length of the detected scenario.

4. Results

4.1. Fast-Mode Results

Immediately after the landslide trigger, the landslide body moved quickly. “Fast” GB-InSAR acquisitions were performed, obtaining interferograms every 28 seconds. This configuration allows SAR detecting velocities up to 14 m/day (about 0.16 mm/s). This velocity is difficult to reach by other similar instruments, which generally need more time to perform an interferogram [24] and, consequently, are able to acquire slower displacement values.
The higher temporal resolution, in terms of the possibility to detect faster displacements, goes to the detriment of the spatial resolution, requiring the detection of a smaller area (in yellow in Figure 6C). In any case, “fast” acquisitions were performed to detect only the faster portion of the landslide, clearly visible also by using this acquisition mode.
Representative interferograms of the beginning monitoring period are shown in Figure 7. These first interferograms clearly show the rapid decrease of the landslide velocity from the beginning of the monitoring, on 24 May 2013 (about 14 m of displacement per day), up to the end of June 2013, when the velocity reached values less than 1 m per day.
Moreover, the GB-InSAR long-term monitoring campaign showed a sharp decrease of the toe velocities through the month of June until July 2013, from which the velocities reached daily millimeter values (Figure 8).

4.2. Slow-Mode Results

In slow configuration, acquisitions were achieved using the greatest linear rail aperture; that is 3 m, every 8 min. In this configuration, spatial resolution increases considerably, but the detectable velocity is reduced. The increased spatial resolution allowed detecting a wider area, including the village of Capriglio, located about 3.8 km from the GB-InSAR installation point, and Pianestolla, which is about 2.8 km from the instrument location (red area in Figure 6C). After a period of interchanging between fast and slow mode acquisitions, on 15 July 2013 fast mode acquisitions were interrupted because the landslide velocity reached very low values (a few millimeters per day, as shown in Figure 8) and slow acquisitions became ordinary, until the end of the monitoring activity.
Slow acquisitions were averaged on 24 hours to generate interferograms for detecting the velocity both of the landslide mass (sector α in Figure 9) and the villages (sectors β and γ in Figure 9). In the referred period (July 2013–December 2014), the monitored areas did not exceed velocities of a few millimeters per day, allowing the assessment of substantial stability both of the landslide body and the villages.
Thanks to the monitoring activity, two other sectors affected by displacements were identified (sectors δ and ε in Figure 9). In sector δ, movements were registered since January 2014 (Figure 9C and Figure 10). Unfortunately, the movement direction of this sector was almost perpendicular to the GB-InSAR LOS, allowing the detection of a very small component of the displacement vector (about 35%), which was strongly underestimated. On the contrary, sector ε movements are easily detectable from the GB-InSAR position; the sector is located on the right flank of the landslide toe, with a movement direction almost parallel to the radar LOS, and it was affected by detectable displacements from February 2014 (Figure 9D and Figure 10).
Field surveys were carried out in these new sectors to validate the InSAR data; strong evidence of movements has been observed, especially in correspondence with the ε sector. Fortunately, the activation of these sectors stopped in a few weeks and movements never exceeded values of a few millimeters per day.
Moreover, by using “slow” mode acquired data, a cumulated displacement map related to the period between 17 July 2013 and 31 December 2014 was obtained (Figure 10). The cumulated map allowed emphasizing those areas affected by displacements lower than 0.1 mm/day (not detectable by analyzing daily interferograms; see Figure 9). Therefore, in the landslide body, further sectors affected by evidence of movements were identified (α1–α7 in Figure 10).
The cumulated displacement map also allowed us to emphasize the presence of residual displacements affecting the previously described sectors (α, β, γ, δ, ε), with greater importance to those sectors corresponding to the villages of Pianestolla (β) and Capriglio (γ). Actually, considering that the azimuth resolution reduces with the increase of the distance from the installation point, it assumes very low values of correspondence with Pianestolla and even more with Capriglio (Figure 6b). Nevertheless, these resolution values are high enough to detect building cluster displacements. Additionally, the “LOS problem” has to be considered: in particular, sectors β and δ suffer of underestimation of displacement values due to the geometrical relation between GB-InSAR LOS and movement direction, which allows detecting only a small component of the displacement vector (Figure 10).
The displacement analysis was supported by the investigation of time series extracted in correspondence with the sectors defined in Figure 10. Fortunately, Capriglio was affected by general stability in the inferred period: in sector γ, registered displacements varied in the range of the technique precision (millimeter scale). On the contrary, centimetric displacements affected Pianestolla village, reaching about 50 mm (Figure 10 and Figure 11). Fractures occurred in some buildings located in the SE portion of the village, providing clear evidence of these displacements (Figure 12A–C).
Displacements were also registered in sectors δ and ε, respectively, affected by the cumulated values of about 100 and 150 mm (Figure 10, Figure 11 and Figure 12D–E).
With respect to the sectors identified in the landslide body (α1–α7), the displacements followed a continuous increasing trend, sometimes interrupted by acceleration/deceleration phases. Cumulated displacements ranged between about 70 mm (α1, α3, α6, α7) and about 300 mm (α5) in the referred period (Figure 11). The landslide body sector affected by the highest displacements is α5; this is justified by the presence of a minor scarp, whose presence was observed during field surveys.

5. Discussion

Following the landslide trigger on 6 April 2013, the Capriglio and Pianestolla villages suffered only minor damages and the landslide, evolved from two main earth slides close to them into a rapidly moving earth flow, deeply channelized within the Bardea Creek riverbed. Following the event, the emergency management activities focused primarily on the two villages exposed to the risk of potential retrogression of the main landslide scarps.
Since the end of April 2013, the lower part of the landslide also drew the attention of the involved authorities, as the 5 May 2013 aerial survey revealed that the entire landslide toe was moving rapidly along the Bardea Creek with respect to the reference satellite images of 16 April 2013, for a total of more than one kilometer with a mean rate of several dozens of meters per day. In this emergency framework, the installation of a monitoring system was extremely necessary. To guarantee a constant (24/7) stream of information, a GB-InSAR system was installed. According to [9], the most serious gap for the extensive use of GB-InSAR devices as operational monitoring tools was the limited range of recordable velocities, which limits the applicability of InSAR approaches only to slow-moving landslides, excluding fast-moving phenomena. In this context, the complex dynamics of the Capriglio landslide has generated a challenging situation to face with a GB-InSAR system. In addition to the landslide size and velocity, the difficulties also consisted of the different deformation pattern and in the widespread vegetation cover within the observed scenario, with the exception of the well-exposed landslide mass and the two villages, located 2.8 and 3.8 km from the radar instrument, respectively. Fast mass movements, like the studied one, are difficult to be monitored by means of the ground-based InSAR approach. In the field of interferometry, the range of observable motions is governed by the refresh time (i.e., the elapsed time between the acquisitions of two consecutive images), which, in turn, depends on the acquisition time (time necessary to collect the radar signal of a single SAR image) [50], typically in the order of few minutes for the existing operational devices. To avoid ambiguity problems and to correctly retrieve the actual velocity, the displacement of the observed target should be contained within ±λ/4 between two consecutive SAR acquisitions. When the investigated landslide velocity exceeds the observable one, the only viable approach is to reduce the synthetic aperture to decrease the acquisition time, with a consequent coarsening of the spatial resolution and decrease of the covered area. When dealing with landslides (such as the Capriglio one) associating different deformation patterns, the only viable approach is to acquire images with different synthetic apertures, exploiting the versatility of the GB-InSAR system in terms of images acquisition. To cope with the scenario generated by the Capriglio landslide, the alternation between fast and slow acquisitions has been the approach designed to retrieve useful information about distinct displacement regimes, ranging from small to high deformation rates.
The “fast acquisition” mode, exploited during the first weeks of monitoring, provided very important information on the rate of movements of the landslide lower sector. This configuration allowed the measurement of the velocity on the order of several meters per day (with a peak of 14 m/day), overcoming the previously set threshold of about 3 m/day, obtained by using similar instruments [24]. This configuration successfully supported the daily emergency management posed by the rapid advancing landslide’s toe, which seriously threatened the Antria bridge on the Bardea Creek. Two months after the beginning of the monitoring activities, displacement velocities in the landslide body had decreased to a lower level (Figure 8). Hence, the “slow acquisition” mode became ordinary. The slow acquisition mode, characterized by wider coverage and finer resolution, has provided long-term information (17 July 2013 to 31 December 2014) and a synoptic view of the deformation processes affecting the Capriglio landslide area. The greatest benefit of this mode was the possibility to retrieve the minor, short-term deformation affecting the village of Pianestolla (sector B in Figure 10) and to assess the substantial stability of the Capriglio village (sector γ in Figure 10).
The high temporal acquisition frequency, the fine ground cell resolution, and the capacity to detect simultaneously both rapid movement and millimetric deformation, makes the GB-InSAR device, coupled with mapping and field surveys, an instrument of great relevance in the field of landslide-related risk management.

6. Conclusions

This paper presents the main findings of the long-term, real-time monitoring of the Capriglio landslide in the Emilian Apennines (Northern Italy). The landslide, which occurred on 6 April 2013, after a period of prolonged rainfall, presents complex features as it started as a roto-translational earth slide and evolved into an earth flow, which channelized in the Bardea Creek riverbed, to form a large scale, rapidly moving earth flow. The landslide reached a total length of about 3.6 km, with a volume of about 3,600,000 m3.
Through the integrated use of aerial, satellite, and drone images and GPS surveys, the temporal evolution of the Capriglio landslide system was mapped, permitting the preliminarily assessment of the landslide toe evolution and velocity with respect to the reference satellite map acquired on 16 April 2013 (Figure 5). This led to the first estimation of the landslide toe velocity immediately after the trigger, ranging between 80 to 15 m/day, corresponding to the "rapid" and "moderate" classes according to the Cruden and Varnes (1996) classification [33].
Since this landslide exhibited a complex displacement pattern, we exploited the versatility and flexibility of a ground-based interferometric system to guarantee a constant (24/7) stream of information on the evolution of the landslide. This approach, based on the alternation of slow and fast acquisitions, allowed to detect and measure both the minor deformation affecting the areas of Capriglio and Pianestolla villages in the upper part of the landslide, and the remarkable displacement rate of the rapid-to-moderate advancing landslide toe, threatening the strategic Antria bridge, straddling downstream the Bardea Creek.
The rationale underpinning the proposed approach is that a landslide, depending on its extension and kinematics, may require different, but simultaneous, forms of analysis for a proper investigation. When dealing with complex phenomena, like the Capriglio landslide, the fundamental aspect is the design of integrated analyses, encompassing continuous monitoring information (like those provided by SAR images), traditional instruments (e.g., GPS), remote sensing data (like those provided by satellite/aerial/drone), and field investigations. The synergistic use of these techniques provides a wide range of information and is strategic for landslide analysis in operational scenarios.

Acknowledgments

The authors thank the Emilia Romagna Region and the Regional Department of Civil Protection for their immediate support during the post-landslide emergency phase. The authors are also grateful to the Department of Chemical and Geological Sciences, University of Modena and Reggio Emilia, for the valuable scientific support. Finally, the authors would like to thank the whole LiSALab staff for supporting all data processing phases. Rainfall data have been provided by ARPA (Regional Agency for Environmental Protection) Emilia Romagna through the DEXTER system interface. We also thank three anonymous reviewers and the editor for their suggestions which greatly improved this work.

Author Contributions

Federica Bardi and Federico Raspini interpreted radar data. William Frodella and Stefano Morelli worked on the landslide multi-temporal mapping. Luca Lombardi, Massimiliano Nocentini and Giovanni Gigli performed the field work and installed the radar system. Alessandro Corsini and Nicola Casagli conceived and coordinated the work and provided a general review. All contributed to the writing, editing and reviewing of this manuscript.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Borgatti, L.; Corsini, A.; Barbieri, M.; Sartini, G.; Truffelli, G.; Caputo, G.; Puglisi, C. Large reactivated landslides in weak rock masses: A case study from the Northern Apennines (Italy). Landslides 2006, 3, 115–124. [Google Scholar] [CrossRef]
  2. Ventura, G.; Vilardo, G.; Terranova, C.; Sessa, E.B. Tracking and evolution of complex active landslides by multi-temporal airborne LiDAR data: The Montaguto landslide (Southern Italy). Remote Sens. Environ. 2011, 115, 3237–3248. [Google Scholar] [CrossRef]
  3. Tofani, V.; Raspini, F.; Catani, F.; Casagli, N. Persistent Scatterer Interferometry (PSI) technique for landslide characterization and monitoring. Remote Sens. 2013, 5, 1045–1065. [Google Scholar] [CrossRef]
  4. Borrelli, L.; Antronico, L.; Gullà, G.; Sorriso-Valvo, G.M. Geology, geomorphology and dynamics of the 15 February 2010 Maierato landslide (Calabria, Italy). Geomorphology 2014, 208, 50–73. [Google Scholar] [CrossRef]
  5. Garberi, M.L.; Palumbo, A.; Pizziolo, M.; Baldelli, C.; Barchiesi, P.; Bertolini, G.; De Nardo, M.T. Numbers on Landslides; Geological Survey, Emilia Romagna Region: Bologna, Italy, 1999. (In Italian) [Google Scholar]
  6. Bertolini, G.; Pellegrini, M. The landslides of the Emilia Apennines (Northern Italy) which resumed activity in the 1994–99 period and required Civil Protection interventions. Quaderni di Geologia Applicata 2001, 8, 27–74. [Google Scholar]
  7. Basenghi, R.; Bertolini, G. Ricorrenza e caratteristiche delle frane riattivate durante in XX secolo nella Provincia di Reggio Emilia (Appennino Settentrionale). Quad. Geol. Appl. 2001, 8, 153–163. (In Italian) [Google Scholar]
  8. Bertolini, G.; Guida, M.; Pizziolo, M. Landslides in Emilia-Romagna Region (Italy): Strategies for hazard assessment and risk management. Landslides 2005, 2, 302–312. [Google Scholar] [CrossRef]
  9. Corsini, A.; Borgatti, L.; Caputo, G.; De Simone, N.; Sartini, G.; Truffelli, G. Investigation and monitoring in support of the structural mitigation of large slow moving landslides: An example from Ca’ Lita (Northern Apennines, Reggio Emilia, Italy). Nat. Hazards Earth Syst. Sci. 2006, 6, 55–61. [Google Scholar] [CrossRef]
  10. Ronchetti, F.; Borgatti, L.; Cervi, F.; Gorgoni, C.; Piccinini, L.; Vincenzi, V.; Corsini, A. Groundwater processes in a complex landslide, Northern Apennines, Italy. Nat. Hazards Earth Syst. Sci. 2009, 9, 895–904. [Google Scholar] [CrossRef]
  11. Rosi, A.; Berti, M.; Bicocchi, N.; Castelli, G.; Corsini, A.; Mamei, M.; Zambonelli, F. Landslide monitoring with sensor networks: Experiences and lessons learnt from a real-world deployment. Int. J. Sens. Netw. 2011, 10, 111–122. [Google Scholar] [CrossRef]
  12. Ronchetti, F.; Borgatti, L.; Cervi, F.; Lucente, C.; Veneziano, M.; Corsini, A. The Valoria landslide reactivation in 2005–2006 (Northern Apennines, Italy). Landslides 2007, 4, 189–195. [Google Scholar] [CrossRef]
  13. Sterzai, P.; Vellico, M.; Berti, M.; Coren, F.; Corsini, A.; Rosi, A.; Mora, P.; Zambonelli, F.; Ronchetti, F. LiDAR and hyperspectral data integration for landslide monitoring: The test case of Valoria landslide. Ital. J. Remote Sens. 2010, 42, 89–99. [Google Scholar] [CrossRef]
  14. Corsini, A.; Borgatti, L.; Cervi, F.; Dahne, A.; Ronchetti, F.; Sterzai, P. Estimating mass-wasting processes in active earth slides—Earth flows with time-series of High-Resolution DEMs from photogrammetry and airborne LiDAR. Nat. Hazards Earth Syst. Sci. 2009, 9, 433–439. [Google Scholar] [CrossRef]
  15. Tamburini, A.; Del Conte, S.; Larini, G.; Lopardo, L.; Malaguti, C.; Vescovi, P. Application of SqueeSARTM to the characterization of deep seated gravitational slope deformatoins: The Berceto case study (Parma, Italy). In Proceedings of the Second World Landslide Forum, Rome, Italy, 3–7 October 2011.
  16. Clerici, A.; Perego, S. Simulation of the Parma River blockage by the Corniglio landslide (Northern Italy). Geomorphology 2000, 33, 1–23. [Google Scholar] [CrossRef]
  17. Barbieri, M.; Corsini, A.; Casagli, N.; Farina, P.; Coren, F.; Sterzai, P.; Leva, D.; Tarchi, D. Space-borne and ground-based SAR interferometry for landslide activity analysis and monitoring in the appennines of Emilia Romagna (Italy): Review of methods and preliminary results. In Proceedings of the FRINGE 2003 Workshop, Frascati, Italy, 1–5 December 2003.
  18. Corsini, A.; Farina, P.; Antonello, G.; Barbieri, M.; Casagli, N.; Coren, F.; Guerri, L.; Ronchetti, F.; Sterzai, P.; Tarchi, D. Space-borne and ground-based SAR interferometry as tools for landslide hazard management in civil protection. Int. J. Remote Sens. 2006, 27, 2351–2369. [Google Scholar] [CrossRef]
  19. Bertolini, G.; Gorgoni, C. La lavina di Roncovetro (Vedriano, Comune di Canossa, Provincia di Reggio Emilia). Quad. Geol. Appl. 2001, 8, 1–23. (In Italian) [Google Scholar]
  20. Bertolini, G.; Pizziolo, M. Risk assessment strategies for the reactivation of earth flows in the Northern Apennines (Italy). Eng. Geol. 2008, 102, 178–192. [Google Scholar] [CrossRef]
  21. Tonnelier, A.; Helmstetter, A.; Malet, J.P.; Schmittbuhl, J.; Corsini, A.; Joswig, M. Seismic monitoring of soft-rock landslides: The Super-Sauze and Valoria case studies. Geophys. J. Int. 2013, 193, 1515–1536. [Google Scholar] [CrossRef]
  22. Ronchetti, F.; Borgatti, L.; Cervi, F.; Corsini, A. Hydro-mechanical features of landslide reactivation in weak clayey rock masses. Bull. Eng. Geol. Environ. 2010, 69, 267–274. [Google Scholar] [CrossRef]
  23. Monserrat, O.; Crosetto, M.; Luzi, G. A review of ground-based SAR interferometry for deformation measurement. ISPRS J. Photogramm. Remote Sens. 2014, 93, 40–48. [Google Scholar] [CrossRef]
  24. Caduff, R.; Schlunegger, F.; Kos, A.; Wiesmann, A. A review of terrestrial radar interferometry for measuring surface change in the geosciences. Earth Surf. Process. Landf. 2015, 40, 208–228. [Google Scholar] [CrossRef]
  25. Tarchi, D.; Casagli, N.; Fanti, R.; Leva, D.; Luzi, G.; Pasuto, A.; Pieraccini, M.; Silvano, S. Landslide monitoring by using ground-based SAR interferometry: an example of application to the Tessina landslide in Italy. Eng. Geol. 2003, 68, 15–30. [Google Scholar] [CrossRef]
  26. Leva, D.; Nico, G.; Fortuny-Guasch, J.; Sieber, A.J. Temporal analysis of landslide by means of a ground-based SAR interferometer. IEEE Trans. Geosci. Remote Sens. 2003, 41, 745–752. [Google Scholar] [CrossRef]
  27. Bardi, F.; Frodella, W.; Ciampalini, A.; Bianchini, S.; Del Ventisette, C.; Gigli, G.; Fanti, R.; Moretti, S.; Basile, G.; Casagli, N. Integration between ground based and satellite SAR data in landslide mapping: The San Fratello case study. Geomorphology 2014, 223, 45–60. [Google Scholar] [CrossRef]
  28. Bardi, F.; Raspini, F.; Ciampalini, A.; Kristensen, L.; Rouyet, L.; Lauknes, T.R.; Frauenfelder, R.; Casagli, N. Space-borne and ground-based InSAR data integration: The Aknes test site. Remote Sens. 2016, 8, 237. [Google Scholar] [CrossRef] [Green Version]
  29. Ciampalini, A.; Raspini, F.; Bianchini, S.; Frodella, W.; Bardi, F.; Lagomarsino, D.; Di Traglia, F.; Moretti, S.; Proietti, C.; Pagliara, P.; et al. Remote sensing as tool for development of landslide databases: The case of the Messina Province (Italy) geodatabase. Geomorphology 2015, 249, 103–118. [Google Scholar] [CrossRef]
  30. Ferrigno, F.; Gigli, G.; Fanti, R.; Casagli, N. GB-InSAR monitoring and observational method for landslide emergency management: the Montaguto earthflow (AV, Italy). Nat. Hazards Earth Syst. Sci. 2015, 3, 7247–7273. [Google Scholar] [CrossRef]
  31. Luzi, G. Ground Based SAR Interferometry: A Novel Tool for Geoscience. Available online: http://www.intechopen.com/articles/show/title/ground-based-sar-interferometry-a-novel-toolfor-oscience (accessed on 13 February 2017).
  32. Iglesias, R.; Fabregas, X.; Aguasca, A.; Mallorqui, J.J.; Lopez-Martinez, C.; Gili, J.A.; Corominas, J. Atmospheric phase screen compensation in ground-based SAR with a multiple-regression model over mountainous regions. IEEE Trans. Geosci. Remote Sens. 2014, 52, 2436–2449. [Google Scholar] [CrossRef]
  33. Cruden, D.M.; Varnes, D.J. Landslide types and processes. Landslide Types Process. 1996, 3, 36–75. [Google Scholar]
  34. Cerrina Feroni, A.; Ottria, G.; Vescovi, P. Note Illustrative Alla Carta Geologica d’Italia Scala 1:50.000 F.217 “Neviano Degli Arduini”. Available online: http://www.isprambiente.gov.it/Media/carg/note_illustrative/217_Neviano_degli_Arduini.pdf (accessed on 13 February 2017). (In Italian)
  35. Varnes, D.J. Slope movement types and processes. Spec. Rep. 1978, 176, 20–47. [Google Scholar]
  36. Hungr, O.; Leroueil, S.; Picarelli, L. The Varnes classification of landslide types, an update. Landslides 2014, 11, 167–194. [Google Scholar] [CrossRef]
  37. Morelli, S.; Segoni, S.; Manzo, G.; Ermini, L.; Catani, F. Urban planning, flood risk and public policy: The case of the Arno River, Firenze, Italy. Appl. Geogr. 2012, 34, 205–218. [Google Scholar] [CrossRef]
  38. Tapete, D.; Morelli, S.; Fanti, R.; Casagli, N. Localising deformation along the elevation of linear structures: An experiment with space-borne InSAR and RTK GPS on the Roman Aqueducts in Roma, Italy. Appl. Geogr. 2015, 58, 65–83. [Google Scholar] [CrossRef] [Green Version]
  39. Rudolf, H.; Leva, D.; Tarchi, D.; Sieber, A.J. Mobile and versatile SAR system. In Proceedings of the International Geoscience and Remote Sensing Symposium, Hamburg, Germany, 28 June–2 July 1999; pp. 592–594.
  40. Tarchi, D.; Rudolf, H.; Luzi, G.; Chiarantini, L.; Coppo, P.; Sieber, A.J. SAR interferometry for structural changes detection: A demonstration test on a dam. In Proceedings of the International on Geoscience and Remote Sensing Symposium, Hamburg, Germany, 28 June–2 July 1999; pp. 1522–1524.
  41. Tarchi, D.; Casagli, N.; Canuti, P.; Moretti, S.; Leva, D.; Sieber, A.J. Monitoring landslide displacements using ground-based differential SAR interferometry: Application to the Ruinon landslide in the Italian Alps. J. Geophys. Res. 2003b, 108, 2387–2401. [Google Scholar] [CrossRef]
  42. Iannini, L.; Monti Guarnieri, A. Atmospheric phase screen in ground-based radar: statistics and compensation. IEEE Geosci. Remote Sens. Lett. 2011, 8, 537–541. [Google Scholar] [CrossRef]
  43. Zebker, H.A.; Goldstein, R.M. Topographic Mapping from interferometric synthetic aperture radar observations. J. Geophys. Res. 1986, 91, 4993–4999. [Google Scholar] [CrossRef]
  44. Gabriel, A.K.; Goldstein, R.M.; Zebker, H.A. Mapping small elevation changes over large areas. Differ. Interferom. J. Geophys. Res. 1989, 94, 9183–9191. [Google Scholar] [CrossRef]
  45. Massonnet, D.; Rabaute, T. Radar interferometry: limits and potential. IEEE Trans. Geosci. Remote Sens. 1993, 31, 455–464. [Google Scholar] [CrossRef]
  46. Goldstein, R.; Zebker, H.; Werner, C. Satellite radar interferometry: Two-dimensional phase unwrapping. Radio Sci. 1988, 23, 713–720. [Google Scholar] [CrossRef]
  47. Rosen, P.A.; Hensley, S.; Joughin, I.R.; Li, F.K.; Madsen, S.N.; Rodriguez, E.; Goldstein, R.M. Synthetic aperture radar interferometry. Proc. IEEE 2000, 88, 333–382. [Google Scholar] [CrossRef]
  48. Lillesand, T.M.; Kiefer, R.W. Remote Sensing and Image Interpretation; John Wiley and Sons, Inc.: Toronto, ON, Canada, 1979. [Google Scholar]
  49. Zebker, H.A.; Villasenor, J. Decorrelation in interferometric radar echoes. IEEE Trans. Geosci. Remote Sens. 1992, 30, 950–959. [Google Scholar] [CrossRef]
  50. Broussolle, J.; Kyovtorov, V.; Basso, M.; Castiglione, G.; Morgado, J.F.; Giuliani, R.; Olivieri, F.; Sammartini, P.F.; Tarchi, D. MELISSA, a new class of ground based InSAR system. An example of application in support to the Costa Concordia emergency. ISPRS J. Photogramm. Remote Sens. 2014, 91, 50–58. [Google Scholar] [CrossRef]
Figure 1. (A) Location map of the Capriglio landslide and GB-InSAR (ground based interferometric synthetic aperture radar) system installation point; in yellow, the GB-InSAR detectable area is marked. Provincial roadways S.P. 101 (dashed white line) and S.P. 665R (dashed red line), including the Antria bridge are highlighted. (B,C) Employed GB-InSAR system.
Figure 1. (A) Location map of the Capriglio landslide and GB-InSAR (ground based interferometric synthetic aperture radar) system installation point; in yellow, the GB-InSAR detectable area is marked. Provincial roadways S.P. 101 (dashed white line) and S.P. 665R (dashed red line), including the Antria bridge are highlighted. (B,C) Employed GB-InSAR system.
Remotesensing 09 00165 g001aRemotesensing 09 00165 g001b
Figure 2. Geological map of the landslide area, including the locations of Capriglio and Pianestolla villages, and the landslide deposits [34].
Figure 2. Geological map of the landslide area, including the locations of Capriglio and Pianestolla villages, and the landslide deposits [34].
Remotesensing 09 00165 g002
Figure 3. 4 May 2013 Capriglio landslide aerial photographs: (A) landslide overview; (B) landslide upper sector; dashed ovals enhance the villages of Capriglio (1) and Pianestolla (2); (C) landslide lower sector and toe with the Antria bridge in a dashed oval. (D) 13 July 2013 landslide toe: secondary landslides at the toe of the main event; numbers indicate the temporal sequence of occurrences.
Figure 3. 4 May 2013 Capriglio landslide aerial photographs: (A) landslide overview; (B) landslide upper sector; dashed ovals enhance the villages of Capriglio (1) and Pianestolla (2); (C) landslide lower sector and toe with the Antria bridge in a dashed oval. (D) 13 July 2013 landslide toe: secondary landslides at the toe of the main event; numbers indicate the temporal sequence of occurrences.
Remotesensing 09 00165 g003
Figure 4. Monthly rainfall in the landslide area from 2006 to 2013.
Figure 4. Monthly rainfall in the landslide area from 2006 to 2013.
Remotesensing 09 00165 g004
Figure 5. Map of the landslide evolution from 16 April to July 2013. The table summarizes the landslide morphometric parameters’ evolution.
Figure 5. Map of the landslide evolution from 16 April to July 2013. The table summarizes the landslide morphometric parameters’ evolution.
Remotesensing 09 00165 g005
Figure 6. Resolution grid size and parameters in fast acquisition mode (A) and in slow acquisition mode (B); detected area using fast (in yellow) and slow (in red) acquisition modes (C). Black dashed ovals represent stable areas selected to apply atmospheric correction.
Figure 6. Resolution grid size and parameters in fast acquisition mode (A) and in slow acquisition mode (B); detected area using fast (in yellow) and slow (in red) acquisition modes (C). Black dashed ovals represent stable areas selected to apply atmospheric correction.
Remotesensing 09 00165 g006
Figure 7. Interferograms (ITF) acquired in “fast mode”. The yellow oval represents the landslide body area. (A) 28 seconds ITF; about 14 m/day; (B) 55 seconds ITF; about 4 m/day; (C) 55 seconds ITF; about 3 m/day; (D) 1 minute and 52 seconds ITF; about 1.5 m/day; (E) 2 minutes and 48 seconds ITF; about 0.3 m/day; and (F) 3 minutes and 40 seconds ITF; about 0.2 m/day.
Figure 7. Interferograms (ITF) acquired in “fast mode”. The yellow oval represents the landslide body area. (A) 28 seconds ITF; about 14 m/day; (B) 55 seconds ITF; about 4 m/day; (C) 55 seconds ITF; about 3 m/day; (D) 1 minute and 52 seconds ITF; about 1.5 m/day; (E) 2 minutes and 48 seconds ITF; about 0.3 m/day; and (F) 3 minutes and 40 seconds ITF; about 0.2 m/day.
Remotesensing 09 00165 g007
Figure 8. Time series of a control point selected in correspondence of the landslide toe, referring to the “fast” acquisitions period (May 2013–July 2013).
Figure 8. Time series of a control point selected in correspondence of the landslide toe, referring to the “fast” acquisitions period (May 2013–July 2013).
Remotesensing 09 00165 g008
Figure 9. Interferograms acquired in “slow mode” and referred to a period of 24 hours. (A): 15–16 July 2013, sector α = 2 mm/day, sectors β and γ = less than 1 mm/day; (B): 16–17 July 2013, sector α = 1 mm/day, sectors β and γ = less than 1 mm/day; (C): 19–20 January 2014, sector α = 1 mm/day, sectors β and γ = less than 1 mm/day, sector δ = 2 mm/day; and (D): 18–19 February 2014,– sector α = 1 mm/day, sectors β, γ, and δ= less than 1 mm/day, sector ε = 5 mm/day.
Figure 9. Interferograms acquired in “slow mode” and referred to a period of 24 hours. (A): 15–16 July 2013, sector α = 2 mm/day, sectors β and γ = less than 1 mm/day; (B): 16–17 July 2013, sector α = 1 mm/day, sectors β and γ = less than 1 mm/day; (C): 19–20 January 2014, sector α = 1 mm/day, sectors β and γ = less than 1 mm/day, sector δ = 2 mm/day; and (D): 18–19 February 2014,– sector α = 1 mm/day, sectors β, γ, and δ= less than 1 mm/day, sector ε = 5 mm/day.
Remotesensing 09 00165 g009
Figure 10. Cumulated displacements (mm) detected along the GB-InSAR LOS from 19 July 2013 to 31 December 2014. Letters indicate the different sectors identified in the observed scene. Arrows indicate the main displacement directions.
Figure 10. Cumulated displacements (mm) detected along the GB-InSAR LOS from 19 July 2013 to 31 December 2014. Letters indicate the different sectors identified in the observed scene. Arrows indicate the main displacement directions.
Remotesensing 09 00165 g010
Figure 11. Time series of deformation for sectors identified in the landslide system. Sector locations are shown in Figure 10.
Figure 11. Time series of deformation for sectors identified in the landslide system. Sector locations are shown in Figure 10.
Remotesensing 09 00165 g011
Figure 12. Evidence of movement on Pianestolla buildings (AC) and in correspondence of the sectors δ (D) and ε (E).
Figure 12. Evidence of movement on Pianestolla buildings (AC) and in correspondence of the sectors δ (D) and ε (E).
Remotesensing 09 00165 g012
Table 1. The Capriglio landslide characteristics on 5 May 2013.
Table 1. The Capriglio landslide characteristics on 5 May 2013.
Date of Activation6 April 2013Cause of ActivationLong-Lasting Rainfall
Elevation range980–650 m a.s.l.Annual average precipitation1200 mm
Slope anglePrecipitation before the trigger
Length3.2 km15-days cumulated rainfall180.8 mm
Area0.84 km230-days cumulated rainfall287.0 mm
Maximum thickness28 m60-days cumulated rainfall430.2 mm
Perimeter10.3 km90-days cumulated rainfall574.4 mm
120-days cumulated rainfall627.8 mm
Max width350 m
Total volume4.2 M m3
TypeComplex movement (roto-translation earth slide evolved into an earth flow)
Total displacement at 5 May 20131300 m
Maximum movement rate80 m/day

Share and Cite

MDPI and ACS Style

Bardi, F.; Raspini, F.; Frodella, W.; Lombardi, L.; Nocentini, M.; Gigli, G.; Morelli, S.; Corsini, A.; Casagli, N. Monitoring the Rapid-Moving Reactivation of Earth Flows by Means of GB-InSAR: The April 2013 Capriglio Landslide (Northern Appennines, Italy). Remote Sens. 2017, 9, 165. https://doi.org/10.3390/rs9020165

AMA Style

Bardi F, Raspini F, Frodella W, Lombardi L, Nocentini M, Gigli G, Morelli S, Corsini A, Casagli N. Monitoring the Rapid-Moving Reactivation of Earth Flows by Means of GB-InSAR: The April 2013 Capriglio Landslide (Northern Appennines, Italy). Remote Sensing. 2017; 9(2):165. https://doi.org/10.3390/rs9020165

Chicago/Turabian Style

Bardi, Federica, Federico Raspini, William Frodella, Luca Lombardi, Massimiliano Nocentini, Giovanni Gigli, Stefano Morelli, Alessandro Corsini, and Nicola Casagli. 2017. "Monitoring the Rapid-Moving Reactivation of Earth Flows by Means of GB-InSAR: The April 2013 Capriglio Landslide (Northern Appennines, Italy)" Remote Sensing 9, no. 2: 165. https://doi.org/10.3390/rs9020165

APA Style

Bardi, F., Raspini, F., Frodella, W., Lombardi, L., Nocentini, M., Gigli, G., Morelli, S., Corsini, A., & Casagli, N. (2017). Monitoring the Rapid-Moving Reactivation of Earth Flows by Means of GB-InSAR: The April 2013 Capriglio Landslide (Northern Appennines, Italy). Remote Sensing, 9(2), 165. https://doi.org/10.3390/rs9020165

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop