PRECONDITIONS LEADING TO THE HOLOCENE TRÆNADJUPET SLIDE OFFSHORE NORWAY J. S. LABERG, T. O. VORREN, J. MIENERT Department of Geology, University of Tromsø, N-9037 Tromsø, Norway H. HAFLIDASON Department of Geology, University of Bergen, N-5007 Bergen, Norway P. BRYN, R. LIEN Norsk Hydro, N-0246 Oslo, Norway Abstract The Trænadjupet Slide (14,100 km2) remobilised an up to 180 m thick package comprising late Weichselian glacigenic sediments and an underlying late Saalian – late Weichselian contourite drift. Rapid burial of the contourites and the presence of gas, is inferred to have caused development of excess pore pressure of the contourites which probably were the “weak layer” that initially failed. During triaxial compressional tests the contourite sediments show contractive behaviour and shear band development. Shear band development due to porewater pressure increase and liquefaction of contractive sediments is therefore regarded a possible mechanism for initial failure and sediment mobilisation of the Trænadjupet Slide. Keywords: Submarine slide, contourites, contractive, shear band, liquefaction. 1. Introduction Understanding the causes of submarine slides is crucial for continental slope stability evaluation. However, the preconditions leading to failure as well as the triggering of many of the large submarine slides throughout the world is still not well understood (e.g. Lee et al., 1991; Hampton et al., 1996; Locat and Lee, 2000; Mienert et al., in press). This is partly because information on the physical and geotecnical properties of the failed sediments, including the slip plane sediments, is scarce (Pratson, 2001). In most cases, only samples from short gravity and piston cores are available while some of the largest slope failures involve more than 100 m of the subsea-floor strata (e.g. Bugge et al., 1988; Laberg and Vorren, 2000). During the Holocene three large submarine slides occurred on the continental slope of the passive Norwegian continental margin, the Storegga, Trænadjupet and Andøya Slides (Bugge et al, 1987; Kenyon, 1987; Dowdeswell et al., 1996; Vorren et al., 1998; Laberg et al. 2002a). Recently, a number of geotechnical borings, penetrating up to 300 m below the sea floor have been conducted for risk assessment studies of the continental slope as part of deep-water oil and gas field development (Bryn et al., 1998). Based on sedimentological, chronostratigraphic and geotechnical analyses of sediments from one of these boreholes, 6606/3-GB1, as well as seismic data, we discuss the preconditions leading to failure of the Trænadjupet Slide (Fig. 1). 247 248 Laberg et al. Figure 1. Bathymetric map (from Perry et al., 1980) including the location of the Trænadjupet Slide and the Nyk Drift. The location of borehole 6606/3-GB1 and Figures 2 and 3 is also shown. 2. Materials and methods The geological and chronological analyses from borehole 6606/3-GB1 were performed by the University of Bergen (Haflidason et al., 1998). All the geotechnical analyses of the sediments were undertaken by the Norwegian Geotechnical Institute, and both the offshore and onshore analyses and results are detailed in their reports (Norwegian Geotechnical Institute, 1998; 2002). The carbonate content was measured by means of a LECO-carbon analyser at the University of Bergen. Three samples were dated by the 14C AMS method. The dating was done on handpicked planktic foraminifers of a single species, Neogloboquadrina pachyderma. All dating results are reported in 14C years BP and have been corrected for an 800 years reservoir age according to Haflidason et al. (1995). The high-resolution single-channel seismic data were acquired using an airgun array of two 0.6 litre sleeve guns with filter setting of the Geopulse Receiver at 100-700 Hz. Figure 2. Alongslope oriented seismic profile UiTø 01-039 from borehole 6606/3-GB1 across the upper Trænadjupet Slide scar (see Fig. 1 for location). The Trænadjupet Slide remobilized late Weichselian glacigenic sediments and part of the underlying Nyk contourite drift. The glacigenic and contouritic sediments can be followed alongslope to the drill site. See text for further discussion. Preconditions leading to the Trænadjupet 249 3. The failed sediments: properties, sedimentation rate and origin The Trænadjupet Slide affected an area of about 14,100 km2 and remobilized an up to 180 m thick sediment package comprising glacigenic sediments (~160 m) and an underlying contourite (~20 m) (Laberg and Vorren, 2000) (Figs. 2 and 3). A glide plane developed in the lower part of the contourite sequence (Fig. 2), and indications of remobilization of this sequence are also seen outside the slide affected area (Fig. 3). The failed succession was correlated to geotechnical borehole 6606/3-GB1 located at 848 m water depth about 100 km south-west of the Trænadjupet Slide scar using an along-slope oriented high-resolution seismic profile (Figs. 2 and 4). The drilling was terminated 105 m below sea floor, with a total recovery of c. 15 %. The drilled succession included a thin (< 1 m) veneer of Holocene sediments inferred to represent part of the winnowing lag identified by Holtedahl and Bjerkli (1975), a ~40 m thick unit of late Weichselian glacigenic sediments, a ~40 m thick contourite drift sequence, and part of the underlying late Saalian glacigenic sediments (Fig. 4). Figure 3. Downslope oriented seismic profile UiTø 00-002 located immediately outside the area affected by the Trænadjupet Slide (see Fig. 1 for location). An irregular upper reflection and a chaotic internal signature (A) and a discontinuous upper reflection further downslope (B) indicate remobilization of part of the Nyk contourite drift sediments also in this area outside the Trænadjupet Slide. The late Weichselian glacigenic sediments are a homogeneous grey diamicton (25 % clay, 45 % silt, 30 % sand) characterised by an average water content of ~20% and an average unit weight of about 21 kN/m3 (Tab. 1). These sediments can be classified as inorganic clays of low to medium plasticity and they have a sensitivity of about 1.5. The organic carbon and CaCO3 content is uniform and on average 0.5% and 6.8%, respectively. Triaxial compression tests showed a dilatant behaviour of these sediments and no shear band development was identified (Tab. 1; Fig. 5). The debris flow sediments were transported to the shelf break mainly as a subglacial, deformable till and deposited on the upper slope in front of the Fennoscandian Ice Sheet during the late Weichselian glacial maximum (Laberg et al., 2002b; Dahlgren and Vorren, in press). 250 Laberg et al. Figure 4. Recovery, lithology, origin and age of the sediments recovered at borehole 6606/3-GB1. Stars shows levels were indications of gas have been identified. The Holocene sediments are inferred to represent part of the winnowing lag identified by Holtedahl and Bjerkli (1975). 14 C AMS dating of the youngest unit immediately overlying the late Weichselian glacigenic sediments in borehole 6606/3-GB1 gave 15,510 +/- 130 14C years BP (reservoir corrected) at 2.1 m, while from the base of the glacigenic sediments at 44.3 m depth an age of 17,870 +/- 135 14C years BP (reservoir corrected) was found (Fig. 4, Tab. 2). Applying these dating results the average sedimentation rate in the area of the Trænadjupet Slide was calculated at ~65 m/ka during the late Weichselian glacial maximum. The underlying Nyk Contourite Drift sediments (Laberg et al., 2001) comprise more than 50 % clay and up to 40 % silt. The average water content is ~40 %, the average unit weight about 18 kN/m3. On the plasticity chart, these sediments mainly plot in the group of inorganic clays with high plasticity, and they have a sensitivity higher than 2.5 (Tab. 1). Preconditions leading to the Trænadjupet 251 Figure 5. Two samples from borehole 6606/3-GB1 of the late Weichselian glacigenic sediments at 40.2 m depth (A) and the Nyk contourite drift at 67.5 m depth (B) following triaxial testing. In sample (B) shear band development is clearly seen, while similar features did not develop in (A). The average organic carbon and CaCO3 content is 0.4% and 15.8% respectively, with increasing values downcore, up to 0.6 % and 35 % at 71.5 m depth. During drilling, gas bubbles and cracking were reported from 45 to 50 and 70 to 75 m depths (Fig. 4). For these sediments triaxial compression tests showed contractant behaviour (Tab. 1) and development of shear bands (Fig. 5). The contourite sediments were deposited from an alongslope flowing ocean current on the northernmost part of the Mid-Norwegian continental slope during the late Saalian to the late Weichselian (Fig. 4, Tab. 2). The maximum average sedimentation rate was up to 1.2 m/ka (Laberg et al., 2001). Table 1. Grain-size distribution, physical and geotechnical properties of the late Weichselian glacigenic sediments and the Nyk contourite drift sediments. 1) Sieving of fraction > 75µm, fall drop method for the fraction < 75 µm. N = 7 (glacigenic sediments) and 11 (contourite sediments). 2) Mass of water expressed as a percentage of the mass of solids. N = 25 and 23. 3) Density is determined by measuring its diameter and length and then weighing it. Unit weight is density x g. N = 26 and 21. 4) According to standard methods described in the Norwegian Standards 8002 and 8003 (Norges Byggstandardiseringsråd 1982a and b). N = 6 and 11. 5) Using the fall cone test on an undisturbed and on a remoulded sample. N = 7 and 9. 6) Using an LECO-carbon analyser. N = 5 and 4. 7) Using an LECO-carbon analyser. N = 5 and 4. 8) Anisotropically consolidated, undrained triaxial compression tests. Berre (1982) describes the triaxial equipment and method used. N = 6 and 7. 4. Preconditions leading to failure Shearing resistance is one important factor controlling the initiation of sliding. Shearing resistance is the result of resistance to movement at interparticle contacts. Sediment density (and water content) is a good indicator of shearing resistance, as increased density generally implies an increase in interparticle contact area and, thus, in shearing 252 Laberg et al. resistance (Terzaghi et al., 1996). The contourite sediments have markedly lower density and higher water content than the overlying glacigenic sediments (Table 1) indicating low shearing resistance within these sediments. The initial low shearing resistance may have been reduced even more during burial due to increased excess pore pressure caused by rapid deposition of overlying sediments. Accumulation of gas may have further contributed to excess pore pressure build-up (Allen, 1997). Our dating results show that during the late Weichselian the contourite sediments were rapidly buried by the glacigenic sediments. In the area where the Trænadjupet Slide occurred the late Weichselian glacigenic sediments were up to 160 m thick, nearly three times the thickness at borehole 6606/3-GB1 (Fig. 2). This implies that the shearing resistance of the underlying contourite sediments probably was markedly lower in the area of sliding than at the drill site, because the more rapid sediment loading gave a more pronounced excess pore pressure build-up. The glide plane developed in the lower part of the contourite sediments where gas was identified in borehole 6606/3GB1. Thus the presence of gas may have decreased the shearing resistance even more at the lower level of the contourite unit. Laboratory triaxial testing showed contractant behaviour of the contourite sediments. A contractant behaviour is characteristic of sediments of low pre-shear density. It occurs after the more tightly packing when porewater can not leave the system immediately causing excess porewater pressure. This gives decrease in effective stress (Terzaghi et al., 1996; Maltman, 1994). The triaxial testing also showed that the strain was concentrated in shear bands (Fig. 5), a phenomenon previously reported from laboratory experiments and field observations (e.g. Besuelle et al., 2000; Desrues and Chambon, in press and references therein). From our data it is not possible to identify the way by which localisation of the shear bands was initiated. However, the fact that they developed in contractive and not dilative sediment lead us to suggest that the pore pressure could be important, as suggested by Sabatini and Finno (1996). If this is correct a possible mechanism for initial failure and sediment mobilisation into flow could be shear band development due to porewater pressure increase and liquefaction of contractive sediments. Dilative clay-rich sediments characterised by higher density, as the late Weichselian glacigenic sediments, do most likely not fail under undrained conditions because it is difficult to introduce enough water to permit flow (Fleming et al., 1989; Terzaghi et al., 1996). This indicates that the glacigenic sediments probably were re-mobilised as a result of initial failure in the underlying contourite sediments. Table 2. AMS-radiocarbon dates obtained from borehole 6606/3-GB1. Preconditions leading to the Trænadjupet 253 5. Conclusions 1. 2. 3. 4. The Trænadjupet Slide remobilised an up to 180 m thick package containing late Weichselian glacigenic sediments and an underlying late Saalian – late Weichselian contourite drift about 4000 years ago. The contourites are muddier (~50% clay, ~40% silt, ~10% sand), and characterised by a markedly lower unit weight (~18 kN/m3) and higher water content (~40%) than the overlying glacigenic sediments (~25% clay, ~45% silt, ~30% sand; density ~21 kN/m3; water content ~20%). Rapid burial of the contourites, the overlying glacigenic sediments were deposited at a rate of about 65 m/ka, and the presence of gas is inferred to have caused development of excess pore pressure of the contourites which probably were the “weak layer” that initially failed. During triaxial compressional tests the contourites show contractive behaviour and shear band development. Thus in the Trænadjupet Slide area a possible mechanism for initial failure and sediment mobilisation was shear band development due to porewater pressure increase and liquefaction of contractive sediments. 6. Acknowledgements This work is a contribution to the COSTA program. 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