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Ninth International Conference on Permafrost ... - IARC Research

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Internal Structure of Rock Glacier Murtèl Delineated by Electrical ResistivityTomography and Forward/Inverse ModelingChristin HilbichDepartment of Geography, University of Jena, GermanyIntroducti<strong>on</strong>Rock glacier Murtèl (Engadine, Swiss Alps) is <strong>on</strong>e ofthe most intensely investigated rock glaciers worldwide.Borehole temperatures have been recorded since 1987(V<strong>on</strong>der Mühll & Haeberli 1990, Haeberli et al. 1998, V<strong>on</strong>derMühll et al. 1998, V<strong>on</strong>der Mühll et al. 2007), providing <strong>on</strong>eof the l<strong>on</strong>gest temperature records in Alpine permafrostFromthe broad range of investigati<strong>on</strong>s <strong>on</strong> this rock glacier, it hasbeen learned that:• The rock glacier Murtèl c<strong>on</strong>sists of a c<strong>on</strong>siderableamount of massive ice (up to 80–100% in a ca. 25 mthick layer below the active layer) (V<strong>on</strong>der Mühll &Haeberli 1990).• The active layer depths vary <strong>on</strong>ly slightly throughoutthe years (by max. 0.5 m) (V<strong>on</strong>der Mühll et al. 2007).• Rock glacier creeping is generally rather slow withvelocities between 5 and 15 cm/a (determined over theperiod 1987–1996) (Kääb et al. 1998).• A shear z<strong>on</strong>e exists in 30 m depth, where most of thehoriz<strong>on</strong>tal movement is c<strong>on</strong>centrated (Arens<strong>on</strong> et al.2002).Apart from the borehole observati<strong>on</strong>s, no directobservati<strong>on</strong>s of the interior exist at rock glacier Murtèl.However, indirect informati<strong>on</strong> could be inferred fromgeophysical measurements (V<strong>on</strong>der Mühll 1993, Hauck &V<strong>on</strong>der Mühll 2003, Maurer & Hauck 2007).In general, rock glacier Murtèl is c<strong>on</strong>sidered an activerock glacier under stable c<strong>on</strong>diti<strong>on</strong>s. The internal structure isassumed to be homogeneous without any distinct degradati<strong>on</strong>phenomena.Geoelectrical M<strong>on</strong>itoringIn summer 2005 a l<strong>on</strong>gitudinal Electrical ResistivityTomography (ERT) m<strong>on</strong>itoring profile was installed at rockglacier Murtèl. The horiz<strong>on</strong>tal distance of the profile is 235m (crossing the borehole and the t<strong>on</strong>gue). Results from theERT m<strong>on</strong>itoring give rise to an interesting inhomogeneity inthe central part of the rock glacier.The general resistivity pattern (Fig. 1) clearly c<strong>on</strong>firms thestratigraphy derived from borehole measurements: the activelayer is represented by relatively low resistivities between 15and 30 kΩm in the upper 3 m. Beneath the active layer thereis a sharp increase in resistivities to values between 500 kΩmand 1.9 MΩm, indicating the presence of massive ice. In thecentral part of the rock glacier, this pattern is interrupted bya vertical anomaly with smaller resistivity values (300–400kΩm). The m<strong>on</strong>itoring results indicate that this feature ismuch more pr<strong>on</strong>ounced in summer than in winter.Figure 1. ERT tomogram from rock glacier Murtèl, measured <strong>on</strong>August 17, 2006.To assess whether this anomaly is an artefact of theinversi<strong>on</strong> process (cf. Hauck & V<strong>on</strong>der Mühll 2003) orproduced by a real structural inhomogeneity the resistivitydistributi<strong>on</strong> of the rock glacier was analysed by means ofsynthetic datasets and forward/inverse modeling using thesoftware Res2DMod and Res2DInv (Loke & Barker 1995,Loke 2002). In forward/inverse modeling approaches,apparent resistivities are calculated from a synthetic model ofthe assumed resistivity distributi<strong>on</strong>. The resulting inversi<strong>on</strong>result can then be compared to the corresp<strong>on</strong>ding inversi<strong>on</strong>result of the measured data. If the results are similar in termsof both resistivity distributi<strong>on</strong> and total values, the syntheticmodel can be evaluated as a realistic model of the subsurfaceresistivity distributi<strong>on</strong>.This procedure was performed for a variety ofgeomorphological situati<strong>on</strong>s that may explain theinhomogeneity within rock glacier Murtèl.Best results were obtained for a simulated crevasse inthe massive ice body of the rock glacier, which is, at leastpartly, filled with unfrozen water. This result is surprising, asthe rock glacier does not show indicati<strong>on</strong>s of disintegrati<strong>on</strong>at the surface. An interpretati<strong>on</strong> of this feature in termsof a degradati<strong>on</strong> phenomen<strong>on</strong> seems likely, but cannot besupported by other data from the rock glacier.C<strong>on</strong>clusi<strong>on</strong>sThe forward/inverse modeling showed that the resistivityanomaly in the central part of the rock glacier is verylikely due to a crevasse-like structure within the ice core.These findings are of interest in the c<strong>on</strong>text of the observedspeed-up of many rock glaciers in the Alps, which isoften associated with disintegrati<strong>on</strong> of the surface and theformati<strong>on</strong> of crevasses (Roer et al. 2005, Kääb et al. 2007).Since comparable developments (speed-up, formati<strong>on</strong> ofcrevasses at the surface) are not known for rock glacierMurtèl so far, further studies are necessary to verify theassumpti<strong>on</strong>s resulting from forward/inverse modeling.101

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