Detailed Analysis of a Submarine Landslide (SAR-27) in the Deep Basin Offshore Algiers (Western Mediterranean) A. Nouguès, N. Sultan, A. Cattaneo, G. Dan, K. Yelles, and PRISME team Abstract On May 21, 2003 an earthquake with a magnitude of 6.8 (Mw) struck the city of Boumerdes, located on the coast near Algiers, and generated significant gravity flows recognized by numerous submarine cable breaks. In order to investigate a possible offshore imprint of past earthquakes in terms of sediment instabilities, we analyzed one of the numerous escarpments of tectonic origin existing on the Algerian margin. This escarpment, located about 50 km NE offshore Algiers is within water depths between 2,600–2,900 m and has an average slope of 4°. A variety of geotechnical (piezocone), geophysical (swath bathymetry, Chirp echosounder and high-resolution deep-towed side scan sonar) and sedimentological (sediment cores) techniques were used to realize this work. Our study focuses on a well-defined submarine landslide scar (called SAR27) revealed by side-scan sonar images. The SAR 27 slide is small in size (0.5 × 1.7 km), but exhibits a complex morphology including a 10-m high headwall scar, tilted blocks, an area of reworked sediment and a distal deposit. Correlations between in-situ measurements, sampling and CHIRP profile provided a comprehensive understanding of the slide geometry and emphasized the role of thin silty sand beds in the slide initiation. These silty sand beds are probably acting as liquefied slip surfaces, implying a translational displacement mode which correlates the slide morphology. A. Nouguès, N. Sultan, A Cattaneo, and G. Dan IFREMER, Géosciences Marines, Laboratoire Environnements Sédimentaires, Plouzané, France A. Nouguès () Institut Polytechnique LaSalle Beauvais, Département Géosciences, Beauvais, France FUGRO FRANCE S.A.S., Nanterre, France e-mail: a.nougues@fugro.com K. Yelles CRAAG, Centre de Recherche en Astronomie, Astrophysique et Géophysique, Bouzaréah, Algiers, Algeria D.C. Mosher et al. (eds.), Submarine Mass Movements and Their Consequences, Advances in Natural and Technological Hazards Research, Vol 28, © Springer Science + Business Media B.V. 2010 541 542 A. Nouguès et al. Keywords Submarine landslide • Algeria • CPT • triggering mechanism • liquefaction 1 Introduction Although evidences of submarine landslides are regularly highlighted on very gentle slopes, the triggering mechanisms of such slides remain quite imprecise. Obviously, the static driving stresses implied by the low slope angles are insignificant, and additional external mechanisms (earthquake, fluid flow, free gas …) are needed to trigger a landslide (Lee et al. 2007). Cyclic loadings generated by earthquakes contribute to this external driving stresses but may especially induce the liquefaction of granular sediment (silt or sand) and degradation and softening of soft clays properties (Pestana et al. 2000). In case of interlayered sand and clay levels, the sand layers reaching a liquefied state may become preferential slip surfaces leading to slope destabilisation (see L’Heureux et al. 2007; Dan et al. 2008 for examples of liquefaction-induced submarine slides and Bardet et al. 1999 for general considerations about liquefaction-induced ground displacements). The Algerian margin, embodying the boundary between the European and the African plates, is a tectonically active margin (Déverchère et al. 2005). Among the several strong to moderate earthquakes which occurred in the last century on the coastal zone, the last violent seismic event (Mw = 6.9) struck the city of Boumerdes on May 21st 2003. The MARADJA 2 survey (2005) aimed at recognizing possible slope failures upslope from submarine cable ruptures which were recorded following the seismic shaking. A well-defined slide showing a freshlooking submarine slide scar was revealed on a deep-towed side-scan sonar profile (the SAR27 profile). The so-called “SAR27 slide” occurs at 2,700 m of water depth on a seafloor escarpment probably of tectonic origin (S2 escarpment, Déverchère et al. 2005). This morphological feature, located approximately 50 km offshore the coastline and characterized by an average slope of 4°, displays numerous slide scars (Fig. 1). Previous studies (Dan 2007; Domzig et al. 2009; Cattaneo et al. this volume) showed the widespread presence of such small-size slides (usually about 0.2 km2) across the Algerian margin. In addition, thin sand beds interlayered in mostly clayey deposits have been described in sediment cores and determined as the main predisposing factor. The recurrent seismicity and subsequent danger of liquefaction have been pointed out as the main triggering factors explaining these numerous small-sized slides in the area (Dan et al. 2008). The present study deals with a comprehensive analysis of the SAR27 slide. A multidisciplinary approach including geophysical, sedimentological and geotechnical data was used to constrain the geotechnical character of the slide together with its detailed architecture. In addition, we aimed to assess the presumed triggering mechanisms of the SAR27 slide and to reconstruct the sliding scenario. Detailed Analysis of a Submarine Landslide 543 Figure 2 Slide scars SAR27 slide 37°N A lgiers fan Dellys A lgiers Bourmerdes M w = 6 .9 (2 0 0 3 ) 4°E 3°E Fig. 1 Morpho-bathymetric map of the S2 escarpment, in the deep Algiers basin. Numerous slide scars (underlined in red) are observed in the vicinity of the SAR27 slide. The red star stands for the 2003 Boumerdes epicentre after Semmane et al. (2005) 2 Data Set and Methods Deep-towed side-scan sonar imagery and 3.5 kHz profiles using the S.A.R. system (Système Acoustique Remorqué) as well as very high-resolution Chirp profiles were collected during the MARADJA 2 survey (Savoye 2005). Further data were acquired along the SAR27 profile during PRISME survey (Sultan 2008): five CPTu (Cone Penetration Test with pore pressure measurement, Meunier et al. 2005), three Küllenberg cores and interface-gravity cores. The cores were performed (1) upslope the headwall in an undisturbed area, (2) in the disturbed deposits and (3) at the base of the slope (Fig. 2). For general information about CPT tests and its interpretation readers are referred to Lunne et al. (1997). Evaluation of the liquefaction potential was performed according to the procedure depicted by Youd et al. (2001). Sediment core logging was performed using a Geotek Multi Sensor Core Logger (http://www.geotek.co.uk) in order to characterize the sediment density or unit weight (g). The volume of the slide was evaluated by reconstructing the initial slope from the present bathymetric profile and by calculating the missing sediment thickness. Thus, the volume of sediment involved in the slide was extrapolated from the scar width and the deposit extent, based on sonar image and backscatter data. 544 A. Nouguès et al. Fig. 2 SAR imagery (a) and associated 3.5 kHz profile (b) acquired along SAR27 slide 3 3.1 Results Morphology of the Slide Area The morphology of the SAR27 slide is clearly expressed on the side-scan sonar image (Fig. 2a). The scar consists of a 560 m wide amphitheater-shaped area including numerous arched extensional cracks. These cracks delineate terraces up to 500–700 m long, tens of meters wide and a few meters high. The arched terraces are perpendicular to the longitudinal axis of the slide (N-S) and are visible from the headscarp until 1 km downslope. The eastern flank of the slide scar reveals multiple Detailed Analysis of a Submarine Landslide 545 Table 1 Characteristics of SAR27 slide from SAR data, CHIRP profile and reconstructed slope Slide scar Deposit Volumes Width: 560 m Length: 1.7 km Headwall height: ~10 m Extension: 1.2 × 0.8 km Thickness of the deposit: < 8m Run-out distance of blocks: 0.65–1.85 km Volume of the empty scar: 6.3 × 106 m3 Volume of Base-of-Slope deposit: 3.2 × 106 m3 Volume of evacuated sediments: 2.9 × 106 m3 walls that probably correspond to successive, intersecting scars which seem to propagate upslope. The echo-sounder profile associated with the SAR image (Fig. 2b) confirms the presence of (1) a well-defined headscarp cutting undisturbed parallel reflectors corresponding to undisturbed slope deposits and (2) of tilted blocks in the upper part of the slide. Compressive ridges are observed at the base of the slope, followed by a transparent lenticular seismic facies suggesting the presence of a mass-deposit. Additionally, the SAR image shows that blocks of 3–5 m in height have been rafted, up to 1 km away of the slope break. Table 1 summarizes the main quantitative characteristics of the SAR27 slide. 3.2 Sediment Core Data Core KS28 (Fig. 3a) is 11-m long and was collected upslope the slide headwall in order to provide the reference lithology of the undisturbed sediments. The top 1.3 m thick sediment consists of soft silty clay deposits characterized by low unit weight value (g = 16 kN/m3). From 1.3 m down to 10 m below seafloor (mbsf) the sedimentary column is characterized by alternating silty-clay and thin cm-thick sandy layers corresponding to repeated turbidite beds (Fig. 3a, p1). From 10 mbsf to the bottom of the core, the sediment is essentially clayey. The clayey intervals from 1.3 mbsf to the bottom have a nearly constant unit weight (g = 18.5 kN/m3). Core KS29 (Fig. 3b) is 5-m long and was collected within the slide scar. The upper 3.5 m, consists of alternating clayey intervals and silt laminae that exhibit numerous small-scale discordances (Fig. 3b, p1) and a overall inclined bedding surfaces with 25° to 60° dip (Fig. 3b, p2). A clear discordance observed at 3.5 mbsf likely corresponds to a slip surface. The lower 1.5 m (from 3.5 to 5 mbsf) consists of horizontal, probably undisturbed clayey layers (Fig. 3b, p2). The interface gravity core recovered nearby the core confirmed that the tilting of the layers is real, and exists beneath the upper 15–20 cm corresponding to the youngest hemipelagic clays (Fig. 3b, pi). Core KS30 (Fig. 3c) is 9-m long and was collected at the base of the slope. The upper 4.3 m of sediment is essentially clayey with fine silts laminae and show discrete internal shear surfaces (Fig 3c, p1). From 3.6 mbsf and down to 4.3 mbsf, the layers appear distorted and the layering is no more visible beneath 4 mbsf, possibly 546 A. Nouguès et al. Fig. 3 Synthetic logs, unit weight (g), water contents (w), and selected sample photos (p1–3, pi) for cores KS28 (a), KS 29 (b) and KS 30 (c). D: discordance, black dashed lines: internal shear surfaces. pi: photo of the associated interface core indicating a greater degree of reworking (Fig 3c, p2). At 4.3 mbsf, the reworked unit overlies undisturbed turbidite beds (Fig 3c, p2 and p3). The upper unit (from 0 to 4.3 mbsf) is characterized by low and highly varying unit weight and high water contents compared to the underlying unit and to the reference core (KS28). 3.3 Stratigraphy Inferred from Seismic Data and CPTu Several well-pronounced reflectors (darker lines) were identified on the Chirp profile and used to define seismic units (U1 to U5) (Fig. 4). The top unit (U1) shows several internal parallel reflectors. It overlies a unit characterized by a strong reflector at its base and only one discernable internal reflector (U2, subdivided into U2a and U2b). The underlying unit (U3) does not show any internal reflector. These top units (U1 to U3) appear to lie discordantly on the two deepest and concordant units (U4 and U5). The Unit 4 shows the most pronounced pinch-out geometry but the other units also have a tendency to thin-out seawards, and the reflectors to become less distinct or merge together (dashed lines). Additionally, two acoustically transparent units are present, presumably corresponding to: (1) some reworked sediments along the slope (gray) and (2) the SAR27 slide deposit (yellow), overlying a well-layered unit at the base of the slope. Five CPTu were performed across the SAR27 slide. For each test, the corrected cone resistance (qt) and excess pore pressure (Du) curves are plotted along the interpreted Chirp profile (Fig. 4). The correlation between depth (in metres) and time (TWT in seconds) was done assuming a mean P-wave velocity of 1,550 m/s. All CPTs have encountered premature refusal (before 30 m of penetration), indicating that a layer with high resistance to compression was reached (black crosses at maximum CPTs depths on Fig. 4). Fig. 4 Correlation between geotechnical and geophysical data. The CPT data are plotted along SAR27 interpreted CHIRP profile assuming a wave velocity of 1,550 m/s (qt: corrected cone resistance, Du: excess pore pressure) 548 A. Nouguès et al. Levels characterized by high qt and low Du values on the CPTu profiles are interpreted as silty sand to sand (Robertson et al. 1986) and classified as very loose to loose (Baldi et al. 1986). Intervals with lower qt values and linear pore pressure profiles correspond to clayey materials. The coarse-grained beds appear to correlate with the high amplitude reflectors underlined on the Chirp profile (see CPT07-01 in Fig. 4). Due to the different vertical resolution of the Chirp profile (10–50 cm) and of the CPTu measurement (5–10 cm), the high amplitude seismic reflectors might correspond to several close qt peaks on the CPTu profiles (see colored CPTu plots in Fig. 4). CPTu profiles acquired within the slide scar (CPT 07-02 and 08-03), show only very few qt peaks. However, each reflector correlates at least one significant pressure (Du) drops (high permeability) indicating the presence of some coarse-grained levels. Besides, the pink reflector (base of U2), which was strong enough to stop prematurely CPT 07-01, is barely discernable when encountered by CPT 07-02. When going seawards, the lateral decrease of the sand beds thickness in addition to the decrease of the pressure confining those loose sandy layers have probably prevent the CPTu cone to detect suitably the different reflectors. 3.4 Liquefaction Potential Assessment It is possible to infer that liquefaction of sandy layers was a possible triggering mechanism for the SAR27 slides based on the following facts: (1) the presence of silty sand layers in a dominantly clayey lithology, (2) the recurrent regional seismicity and (3) the CPTu data showing possible ‘ghost’ loose sand layers (i.e. only visible through their high permeability) when going seawards. We therefore decided to assess the liquefaction potential of the SAR27 soil profile. The employed method is a simplified procedure developed from empirical correlations between soil resistance to liquefaction and CPTu tests (Youd et al. 2001). The resistance to liquefaction or CRR (Cyclic Resistance Ratio) is derived from the cone resistance corrected by the overburden effect and the fine-grained content. The CRR is then compared to the CSR (Cyclic Stress Ratio), which represents the seismic solicitation (defined by a maximal acceleration amax). The Moment Magnitude (Mw) of the earthquake is also taken into account. From CPT 07-01, four loose silty-sandy layers were identified as potentially liquefiable at 6.4, 7.5, 10.3 and 15.2 mbsf (Fig. 5). The comparison between the CRR and CSR calculated for an expectable magnitude level (Mw = 7) reveals that liquefaction could occur for an amax of 0.1–0.15 g in the shallowest sand layers (corresponding to the base of U1 and U2a). In order to cause liquefaction in the deepest layer (base of U2b at 15 mbsf), accelerations of 0.2 g would be needed. For CPT 07-02, the friction was not measured, preventing an accurate calculation of the liquefaction potential for the two silty-sand levels at 17.25 and 18.75 mbsf (see CPT 07-02 on Fig. 4). However, sediment levels deeper than 15 m are rarely observed to liquefy (Krinitzsky et al. 1993). Others CPTu could not provide results in terms of liquefaction potential as no sand layers were recognized on tip cone resistance profiles. Detailed Analysis of a Submarine Landslide 549 Fig. 5 Comparison between the CSR calculated for several maximal accelerations (amax) and the CRR computed from CPT 07-01 4 Discussions and Conclusion In the upper part of the scar, numerous extensional faults and terraces indicate that the upper, mostly cohesive sediments (Unit 1 and 2) only experienced moderate displacements, whereas the smoother morphology observed downslope together with evidence of a mass-deposit attests of enhanced sediment disruption. Geometrically, the base of the Unit 3 (light blue horizon) appears to be the basal slip plane of the slide. The base of the Unit 2 (pink horizon) is interpreted as a secondary slip plane, where the tilted blocks are probably rooted in. SAR27 slide is therefore inferred to be a translational slide with multiple slip planes. As shown by the CPT-based liquefaction analysis, the loose silty-sand layers found in cores from the SAR27 slide area are potentially liquefiable for seismic accelerations (0.1–0.2 g) that are expectable over the margin: Pelaez Montilla et al. (2003) calculated a regional expectable PGA of 0.15 g for a return period of 475 years and Laouami et al. (2006) showed from strong motion recordings of the 2003 Boumerdes earthquake that site effects could locally lead PGAs reaching 0.6 g. An earthquake and related liquefaction can therefore be considered as very probable triggering mechanisms of the SAR27 slide. However, several predisposing or aggravating factors are assumed to have played a major role in the slide initiation. One of the main predisposing factors is the lithology, composed of successive loose sandy layers interbedded within impermeable clayey intervals. As demonstrated by Yang and Elgamal (2002), the clay layers increase sands vulnerability to liquefaction by trapping excess pore pressure and hindering its dissipation. Biscontin and Pestana (2006) also discussed the fact that the presence of these coarse-grained levels could lead to a delayed failure due to the impeded migration 550 A. Nouguès et al. Fig. 6 Summary of the triggering and evacuation processes (a) expected to have generated SAR27 slide and its present morphology (b) reconstructed from the SAR and CHIRP data of excess pore pressure after the end of shaking. Once liquefaction has been triggered by an earthquake, low static forces in a gentle slope can be sufficient to cause significant displacements. In addition, the layers’ thinning seawards implies a decrease of the sand levels burial depth and a correlative lateral increase of their liquefaction potential (see Sultan et al. 2008). Consequently, liquefaction was more likely to occur: (1) in the superficial, unconfined sand beds (bases of U1 and U2) but with few consequences on the general slope stability and (2) in the deepest sand beds (merged bases of U3 an U4) when they become shallower seawards, leading to sediment destabilization from the base of the slope (Fig. 6a). The sliding scenario for the SAR27 slide involves: (a) predisposing factors, essentially due to the lithology and the layers geometry; (b) a triggering factor, very probably being an earthquake, with subsequent localized liquefaction and (c) a retrogressive failure and evacuation process inferred from the slide architecture including two modes of sediment transport: (1) a deep-based slide with moderate to high disruption as attested by the high water contents of the deposit and its smooth morphology and (2) a shallower instability in the upper layers marked by extension and moderate displacements. Even if the SAR27 slide has a fresh morphological expression on the seafloor, the 15–20 cm thick clayey sediment present on top of the slide deposit in the interface core is likely a hemipelagic drape implying that would imply that SAR27 slide is older than the 2003 earthquake. 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