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Original Articles

Using ALOS PALSAR derived high-resolution DInSAR to detect slow-moving landslides in tropical forest: Cameron Highlands, Malaysia

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Pages 741-759 | Received 14 Jul 2013, Accepted 24 Oct 2013, Published online: 02 Dec 2013

Abstract

Landslide is one of the natural hazards that pose maximum threat for human lives and property in mountainous regions. Mitigation and prediction of this phenomenon can be done through the detection of landslide-susceptible areas. Therefore, an appropriate landslide analysis is needed in order to map and consequently understand the characteristic of this disaster. One of the recent popular remote sensing techniques in deformation analysis is the differential interferometric synthetic aperture radar which is popularly known as DInSAR. Due to the mass vegetation condition in Malaysia, a long-wavelength synthetic aperture radar (∼24 cm) is required in order to be able to penetrate through the forests and reach the bare land. For that reason, ALOS PALSAR HH imagery was used in this study to derive a deformation map of the Gunung Pass area located in the tropical forest of the Cameron Highlands, Malaysia. In this study, the ascending orbit ALOS PALSAR images were acquired in September 2008, January 2009 and December 2009. Subsequently the displacement measurements of the study site (Gunung Pass) were calculated. The accuracy of the result was evaluated through its comparison with ground truth data using the R2 and root mean square error (RMSE) methods. The resulted deformation map showed the landslide locations in the study area from interpretation of the results with 0.84 R2 and 0.151 RMSE. The DInSAR precision was 11.8 cm which proved the efficiency of the proposed method in detecting landslides in a tropical country like Malaysia. It is highly recommended to use the proposed method for any other deformation studies.

1. Introduction

Synthetic aperture radar (SAR) systems have been widely used in the past two decades to produce high-resolution mapping and other remote sensing applications (Calabro et al. Citation2010; Sun et al. Citation2011). The ability of penetrating the cloud and day-and-night operation made the SAR systems unique compared to optical imagery and in situ measurements. Also, it is known to be unaffected by sun-illumination and atmospheric conditions (Karjalainen et al. Citation2012). SAR data are increasingly applied to geophysical problems, either by themselves or in conjunction with data from other remote sensing instruments (Biro et al. Citation2013; Pradhan et al. Citation2013). Examples of such applications include polar ice research (Gourmelen et al. Citation2011; Hassaballa et al. Citation2013), land use mapping (Mahmoud et al. Citation2011; Chen et al. Citation2013), vegetation and biomass measurements (Lardeux et al. Citation2011) and natural hazards (e.g. Pradhan et al. Citation2010b; Billa & Pradhan Citation2011; Herrera et al. Citation2013).

In recent years, radars have given a new dimension to the disaster management research by providing real-time and precise information (Pradhan et al. Citation2009; Elbialy et al. Citation2013). Deformation of the ground surface can occur through man-made or naturally induced factors. Geological phenomena such as earthquakes, subsidence, volcanic activity, glacial rebound and landslides are the main contributors of ground deformation (Pradhan & Lee Citation2010). Human causes of displacements include mining activities and excessive groundwater (e.g. water, gas, oil) exploitation, etc. So it is critical to have a clear understanding about the impacts of each activity in order to have proper and sustainable management over the area. Landslide is one of the major natural disasters that cause frequent damage in a steep terrain (Dahal et al. Citation2012). Thus, mapping, monitoring and analyzing the susceptible areas for these disasters help the governments and agencies to protect lives and property (Pourghasemi et al. Citation2013).

DInSAR is a robust method to detect positional changes on the Earth's surface caused by landslides or other natural disasters (Abidin et al. Citation2012; Jebur et al. Citation2013; Idrees et al. Citation2013a). DInSAR can be generated by calculating the difference between two interferograms belonging to three data sets acquired at different times. If any small positional changes occur during this period of data collection, it can be precisely detected through this technique (Cascini et al. Citation2010). These surface displacements can be measured through the space by near to centimetre accuracy using the SAR imagery, covering a vast area. Terrain elevation changes are the main source of information in many areas of research. The DInSAR technique utilizes the phase difference between pairs of the SAR image acquired from the same area at different times, which is generally recorded by same observation parameters. At least two interferograms are needed to be generated, i.e. before and after the event, which induced the landform variation (Catani et al. Citation2005). From the computed interferograms, the DInSAR technique allows the estimation of the projection of the displacements along the radar line of sight (LoS).

The principle of DInSAR was first described by Gabriel et al. Citation(1989). For geological applications, DInSAR technology was used to examine the deformation made by earthquakes (Massonnet et al. Citation1993). Over the years, many studies have been carried out using DInSAR technology on various applications such as tectonic events (Colesanti et al. Citation2003), volcanic deformation (Lagios et al. Citation2005), landslides (e.g. Farina et al. Citation2006; Meisina et al. Citation2008; Guzzetti et al. Citation2009; Lauknes et al. Citation2010; Yin et al. Citation2010), ground motions due to fluid exploitation (Sarychikhina et al. Citation2010), geothermal related activities (Manzo et al. Citation2012), subsidence episodes (Trasatti et al. Citation2008) and mining subsidence (Castañeda et al. Citation2009).

The results presented in the aforementioned papers are an evidence of the usefulness of DInSAR in various applications including landslide studies. Since the traditional landslide monitoring methods are time consuming and costly, DInSAR plays a key role in land displacement monitoring. Yin et al. Citation(2010) used integration of GPS and DInSAR observations to monitor the Jiaju landslide along the deep-cut valley in the western Sichuan. In a recent paper, Guzzetti et al. Citation(2009) performed multi-temporal DInSAR to extract the deformations and their impact, which happened in the Umbria region from 1992 to 2000. The number and percentage of the landslides and land subsidence were investigated for that area.

In a recently published paper, Idrees et al. (Citation2013b) reviewed some of the popular DInSAR algorithms to monitor the deformations of the ground and stated that all the methods were able to detect the displacements by different spatial resolutions. De Agostini et al. Citation(2012) added DInSAR outputs into their prediction analysis to produce a map consisting of spatial and temporal information on landslides that occurred in 2010. Ardizzone et al. Citation(2012) stated that landslide analysis cannot be an efficient using single method, while it needs integration of data and information at different temporal and spatial scales. They proposed DInSAR as a standard and precise technique to detect and map the landslide events.

Herrera et al. Citation(2013) applied DInSAR using the integration of multi-SAR data of ALOS PALSAR images (2006–2010), ERS, Envisat (2001–2007) and TerraSAR-X (2008) data sets. Their results indicated that using multi-SAR data analysis, the complex landslide dynamics will be understood better and thus improved analysis may be carried out. In another paper, 38% of the landslides in the Tena valley could be detected and their results were examined using differential GPS (D-GPS) (Herrera et al. Citation2013). The same group of authors tried to compare the performance of DInSAR using the single-data type of ALOS PALSAR with the output of multiband DInSAR from a previous study of the same study area (García-Davalillo et al. Citation2013). Results of the comparison analysis indicated that DInSAR made by one data type could detect deformation with larger spatial coverage than multiband DInSAR. However, it could recognize lower number of landslides compared to multiband DInSAR (9 against 51). The best performance was achieved using a combination of these two methods, which could map and monitor 68% of the landslides in Tena Valley (García-Davalillo et al. Citation2013). Roering et al. Citation(2009) utilized a combination of DInSAR and LiDAR and archived air photos to detect the large, slow-moving landslides in the Eel River catchment, northern California. They could identify five large (>1 km long) landslides that occurred between 2007 and 2008. Their results reflected the potential use of ALOS interferometry and airborne LiDAR to track small landslides.

The highest penetration of SAR signals through the vegetation cover can be obtained using the L band of the ALOS PALSAR satellite by its 24 cm wavelength signal (e.g. Strozzi et al. Citation2005; Herrera et al. Citation2013). More recently, with the advent of a high-resolution SAR sensor such as Terra-SAR-X, it is possible to use a more accurate source of data in DInSAR imagery (Liao et al. Citation2012). Unfortunately, due to its relatively high cost of data acquisition, it was not used in the current research. Also other platforms such as ERS 1/2 (Guzzetti et al. Citation2009), JERS (Alimuddin et al. Citation2013), Radarsat (Pepe et al. Citation2011) and Envisat (Pepe et al. Citation2005) are available, but in most of the deformation studies ALOS PALSAR is recommended for use (Honda et al. Citation2012; García-Davalillo et al. Citation2013). Furuta et al. Citation(2005) gathered information about the capabilities of ALOS PALSAR in interferometry studies. They found that ALOS PALSAR is very useful for producing accurate digital elevation models (DEMs) and deformation monitoring, as well as disaster monitoring and hazard prevention.

The Cameron Highlands in Malaysia has faced many landslides which caused considerable damage to waterways, property, livestock and pipelines (Pradhan & Lee Citation2010). The Gunung Pass area, which is located in the Cameron Highlands, is highly prone to landslides due to heavy rainfall and weak soil structure. Recently the area has suffered heavy damage from landslides and requires fast and accurate deformation analysis for implementing preventive measures (Pradhan & Lee Citation2010). Previously, some landslide susceptibility analysis had been done by some researchers in this area (Pradhan & Lee Citation2010; Pradhan et al. Citation2010a; Pradhan et al. Citation2010b; Rauste et al. Citation2012), but there was not any attempt to use deformation analysis through the DInSAR method. For instance, Pradhan and Lee Citation(2010) used an artificial neural network to generate a landslide susceptibility map of the Cameron Highlands with 83% accuracy. The aim of this study is to map the landslides which happened in May 2009 using the DInSAR technique to illustrate the efficiency of the proposed method.

2. Study area and data used

The used scenes cover Barisan Titiwangsa Mountains in Malaysia. Banjaran or Barisan Titiwangsa is the longer of the two mountain ranges that run through West Malaysia stretching from Thailand down to Negeri Sembilan. It reaches its highest altitude of 7138 feet at the peak of Ginning Korbu near the mining town of Ipoh. The study was conducted between the Perak and Pahang states in the Gunung Pass area of the Cameron Highlands district, as shown in . Gunung Pass is a tropical rainforest which is geographically located at a latitude of 04° 35’ 55” N and longitude 101° 20’ 49” E. The elevation of the road is 1391 m above mean sea level, while the peak of Gunung Pass reaches 1540 m above mean sea level. The lithology of the Cameron Highlands mainly consists of Quaternary and Devonian granite and schist (Pradhan et al. Citation2008; Pradhan et al. Citation2010b). The rocks of the Gunung Pass area consist of a sequence of metasedimentary rocks, which are confined within a 4-km-wide, N to NNE trending belt (Malone et al. Citation2008). It has been reported by a previous study (Khan Citation2010) that landslides took place in the Gunung Pass area on the Simpang Pulai–Cameron Highlands highway in 2009.

Figure 1. Study area location map (yellow ellipse showing the location of the landslide).

Figure 1. Study area location map (yellow ellipse showing the location of the landslide).

Selection of SAR images is a very critical task, as the data should possess some specific characteristics in order to be used in interferometric processing. It is a key step, since the criteria adopted for selection of images have a strong impact on the quality of the final results. These criteria depend on the specific application for which the SAR interferometric images are acquired. For that reason, a pair of HH polarized L bands of ALOS PALSAR data were used for the purpose of interferometric generation. The data were acquired in September 2008 and January and December 2009. The range sampling frequency, chirp bandwidth and bit quantization are 32 MHz, 28 MHz and 5 bits, respectively.

3. Methodology

In the following sections, the main characteristics of the InSAR and DInSAR procedures are described using the PalsarProcessor and PalSarFringe programs.

3.1. Ground survey

First, the location of the landslides was detected using a GeoExplorer 6000 handheld GPS. Using the differential method, the accuracy of the collected points was down to centimetre level – either post-processed or in real-time methods. Furthermore, the collected data were used for refinement of the resulted interferogram. Other information such as horizontal movement of the landslide was obtained from in situ measurements conducted by Jamaludinl et al. Citation(2008). Data were acquired on 12 December 2007 using an automatic robotic total station (Sokkia SRX) which is stationed near the Gunung Pass landslide. The restriction of the LoS to the existing survey locations led to the use of two stations at the southern end and northern end of the slope. In order to protect the stations from varied weathering conditions, they were mounted on a concrete structure. Some of the location points which were very close to each other or were not located in proper places were removed before using them in the processing. In this study, only 20 location points were used and the analysis was done using these points (. The data were transferred from sites to the Main Control Center located at the Public Works (PWD, Malaysia) Headquarters in Kuala Lumpur using GSM communication. Subsequently, the shifted distance was measured and used in the validation of this study.

Table 1. Survey location points and their displacements.

3.2. Preprocessing

ALOS PALSAR data were acquired as level 1.0 which represents the signal information, and the data to be processed further changed to one level higher, containing phase and magnitude information, i.e. 1.1 (Shimada Citation1998). To process SAR interferometry, the original SAR signal must be processed to single look complex (SLC) data which is called SAR image reconstruction (Schmitt & Stilla Citation2010). The PALSAR processor is a tool that was used to convert the PALSAR level 1.0 data into SLC data.

3.3. SAR orthorectification

High-precision information of the corrected image is required for removing the geometric distortions (Ren & Chang Citation2012). For each pixel, equations (1) and (2) must be fulfilled. Using these equations, the relationship between the single backscatter element, sensor and their related velocities is calculated and therefore the illumination geometry and the processors’ characteristics are extracted. This complete reconstruction of the imaging and processing geometry took into consideration the topographic effects (foreshortening, layover) as well as the influence of the Earth rotation and terrain height on the Doppler frequency shift and azimuth geometry. In this study, an ASTER DEM was used for this purpose with 30 m spatial resolution. (1) (2) where Rs, S and P are the slant range, spacecraft and backscatter element position, respectively. Similarly, vb and vs are the spacecraft and backscatter element velocity, respectively; f0, c and fD are the carrier frequency, speed of light and processed Doppler frequency, respectively.

3.4. SAR interferogram generation

After processing the two images, a pair of SLC data were extracted which were utilized in the SAR interferogram generation. For that reason, an InSAR pair consisting of two scenes referred to as a master image and a slave image was used to construct the interferogram (Ren & Chang Citation2012). One of the scenes was used as a master image, and the other data were used to overlay on that as a slave image. In order to increase the phase of the fringe with respect to the height, the slave orbit position must be at the right side of the master orbit position (Yu & Ge Citation2010). The difference between r1 and r2 (Δr) can be measured by the phase difference (f) between two complex SAR images using equation (3) (Sousa et al. Citation2011). This is performed by multiplying one image by the complex conjugate of the other one, which resulted in the formation of the interferogram. The phase of the interferogram contains fringes that trace the topography like contour lines. These images should have a suitable baseline, according to the image selection criteria (Navarro-Sanchez et al. Citation2010). The baseline between the master and slave images for the first and second interferograms was 279 m and 292 m, respectively. The general steps of interferogram generation are shown in . (3)

Figure 2. The preprocessing steps for fringe generation.

Figure 2. The preprocessing steps for fringe generation.
where ΔR is the slant range difference from satellite to target at different times and λ is the ALOS PALSAR wavelength which is about 23.62 cm.

3.5. SAR interferogram post-processing

Due to the noisy nature of the resulted interferogram, a proper filter should be used in order to remove the bias of the output. There are some common filters mentioned in the literature such as the Goldstein filter (Goldstein & Werner Citation1997), sigma filter (Lee et al. Citation2009) and simple average (Colavita et al. Citation2010); however, based on trial and error, the best noise reduction was achieved using the Goldstein filter. The Goldstein filter is an adaptive radar interferogram filter which is based on the concept of multiplication of the Fourier spectrum Z(u,v) of a small interferogram patch by its smoothed absolute value S{|Z(u,v)|} to the power of an exponent ∝ (Lu et al. Citation2010). The filter was applied with the weight value of 0.5 as it is not recommended to have a high value of weight (Wang et al. Citation2011). The generated interferogram was orthorectified using an ASTER DEM.

3.6. Phase unwrapping

The range of the phase module is represented in 2π. So, the time that changes in phase reaches to 2π the cycle will be repeated (Navarro-Sanchez et al. Citation2010). In order to resolve the 2π ambiguity, phase unwrapping was applied. There are some popular methods to serve the purpose, such as region growing (Ojha et al. Citation2012), minimum cost flow (Pepe & Lanari Citation2006), branch-cuts (Estrada et al. Citation2012), minimum least squares (Navarro-Sanchez et al. Citation2010), multibaseline (Xianming & Yiming Citation2011), etc. In the current research, the region growing method was used and for its parameters level 1 decomposition and 0.15 thresholds were selected. It is recommended to use a low coherence threshold (0.15–0.2) in order to have enough freedom during the analysis (Ojha et al. Citation2012).

3.7. SAR differential interferogram

The temporal separation in repeat-pass interferometry of days, months or even years can be used for long-term monitoring of geodynamic phenomena such as glacial or lava-flow movements (Sumantyo et al. Citation2012). However, it is also useful to analyze the results of single events, such as earthquakes. As such, the observed phase (Øint) is the sum of several contributions. The objective of DInSAR is to extract information from the different components so that the displacement (ØMovement) can be calculated using equation (4); the displacement sensitivity of DInSAR is given in equation (5). (4) (5) where ∂ξ is the deformation. A differential interferogram can be generated in different ways, as shown in . In the first case, passes 1 (pre-event) and 2 (after-event) in combination with a DEM (used for subtracting the topography induced fringes) were considered (Marghany Citation2012). In the second case, in order to avoid the DEM generation and isolate movements associated with the event, passes 1 and 2 were combined with passes 1 and 3).

Figure 3. The general steps of differential interferogram generation used in this study.

Figure 3. The general steps of differential interferogram generation used in this study.

3.8. Validation

The efficiency and quality of the developed interferogram should be examined using a proper method. The results can be validated using the statistical method of R2 and RMSE (Askne et al. Citation2003). The validation has been done by comparing in situ measurements () with the displacement results using equations (6) and (7). (6) where N is the number of verifying points, Mi are the points measured using the resulted interferogram and Oi are the points collected by in situ measurement. (7) where SSres is the residual sum of the squares and SStot is the total sum of the squares.

4. Results and discussion

After applying the full SLC processing, three pairs of scenes could be achieved which were used later in the processing of the fringe generation. The SLC data were orthorectified in order to represent the reality in terms of the geographic location, as shown in and . As mentioned earlier, one master and two slaves were used to generate the two interferogram fringes.

Figure 4. The master (left) and slave (right) images of the first interferogram.

Figure 4. The master (left) and slave (right) images of the first interferogram.

Figure 5. The master (left) and slave (right) images of the second interferogram.

Figure 5. The master (left) and slave (right) images of the second interferogram.

After that, the two fringes were generated using two pair data where the result was represented in a greyscale interferogram. Subsequently, the fringes were divided into many subareas surrounded by phase jump edges as the subarea borders. In a subarea, the phase advanced in accordance with increase of brightness. In contrast, an increment of phase jump occurred at the border, as shown in (a). The resulted fringe had a lot of noise which has been clarified in Section 3.4. After applying the Goldstein filter, the result had a better appearance, as shown in (b). Then, region growing was used and for its parameters level 1 decomposition and a 0.15 threshold were selected for phase unwrapping. For that purpose, interferograms were orthorectified using an ASTER DEM, as shown in . The resulted interferogram ranged between 218.5 m and −218.5 m and could measure the difference in height for the chosen data.

Figure 6. The fringe of the first interferogram (left) and the fringe after applying the Goldstein filter with a weight of 0.7 (right).

Figure 6. The fringe of the first interferogram (left) and the fringe after applying the Goldstein filter with a weight of 0.7 (right).

Figure 7. The results of the orthorectified interferogram (January (left) and December (right) 2009).

Figure 7. The results of the orthorectified interferogram (January (left) and December (right) 2009).

Subsequently, both interferograms were combined together for the purpose of differential interferogram generation, as shown in . The results showed that the differential interferogram had a displacement of 11.8 per cycle (π).

Figure 8. The result of the differential interferogram (December 2009).

Figure 8. The result of the differential interferogram (December 2009).

The main objective of this paper was to detect the areas that had been deformed by landslides; however, a large number of areas had been ignored because of vegetation coverage, depending on the SAR signal that can penetrate through the vegetation to different depths. Therefore, differential interferometry is not applicable for vegetation analysis. The final result of DInSAR is shown in which clearly represents the landslide movement across the highway of Gunung Pass. Also, shows the non-landslide areas in order to facilitate differentiating landslide and non-landslide areas. It can be seen that no interference happened in the fringes.

Figure 9. The area of deformation with the metric unit.

Figure 9. The area of deformation with the metric unit.

Figure 10. Area representing a non-landslide region.

Figure 10. Area representing a non-landslide region.

Landslides were detected and mapped for further studies. The area of the landslides was calculated using GIS tools which showed the amount of movement around 54,000 m2. The area was calculated by subtracting the regions showing high distortion. Then, it was transferred to ArcGIS for area calculation based on the deformation scale. The black arrow in shows the direction of the movement of the landslides. Landslides were quantitatively represented using 60 points that were chosen to prepare the profile of displacement as a function of elevation (). The range of the horizontal movement of displacements varied between 1 and 10 m.

Figure 11. Profile of displacement.

Figure 11. Profile of displacement.

For the purpose of validation, the RMSE and R2 methods were used (Papoutsis et al. Citation2013; Shirzaei et al., Citation2013). The horizontal measurement data, mentioned in , were used to validate the detected landslides. For that purpose, 20 points were used and both R2 and RMSE were calculated and a regression relation was plotted, as shown in . The resulted R2 was 0.841 with RMSE 0.115 which were quite reasonable for the current study.

Figure 12. The scatter plot of the testing point's validation.

Figure 12. The scatter plot of the testing point's validation.

5. Conclusion

Natural hazards such as landslides have serious and devastating consequences: huge loss of lives and property. So, it is wise to detect the mass movement caused by landslides through proper scientific and cost-effective methods in order to analyze their characteristics. Many methods have been developed to recognize and detect these movements; however, most of them have some weak points which reduce the reliability and efficiency of these methods. Also, landslides can happen in remote areas where field work is not feasible. As in hazard studies time is paramount for the emergency response, DInSAR is the best choice for identifying large areas that have been moved in a very short time. This study has demonstrated the detection of horizontal movement of landslides using DInSAR generated by the ALOS PALSAR L band. Selection of proper imagery has a significant impact on the final output of the interferometric processing. Landslides mainly happen in areas covered by vegetation and have a cloud cover. The ALOS PALSAR is an L-band frequency (1.27 GHz) radar capable of continental scale interferometric observations. The highest penetration of SAR signals through the vegetation cover can be obtained using the L band of the ALOS PALSAR satellite, through its 24 cm wavelength signal, which enables continuous recording from the ground of the whole area.

The result exhibited an accurate fringe pattern which showed deformation with 11.8 cm accuracy with 0.84 R2 and 0.151 RMSE. Using GIS tools the area of the landslides was calculated which showed approximately 54,000 m2 movement. The location of the landslide was detected clearly and precisely which proved that DInSAR is a powerful tool, which can be used to detect any positional changes in the vertical horizontal movement of the Earth surface. The method proposed in this research can be used for planning and assessment purposes. Landslide maps can be used as an efficient indicator for managers and planners in order to select a proper location for transportation and other infrastructure. The results achieved in this study can be used as basic data to apply more comprehensive analysis such as landslide volume measurement, damage assessment and prevention. Also, more pair of data can be used in order to analyze a series of DInSAR in future studies.

Acknowledgements

The authors would like to thank two anonymous reviewers for their critical reviews on an earlier version of the manuscript. Also, the authors are grateful to the Public Works Department, Malaysia, and, in particular, Mr Suhaimizi for providing the literature on the Gunung Pass landslide.

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