Physical properties of Carboniferous and Devonian Rocks drilled in the RWTH-1 borehole Lydia Dijkshoorn (Applied Geophysics, RWTH Aachen, Lochnerstraße 4-20, 52064 Aachen, Germany; e-mail: [email protected] Renate Pechnig (Geophysica Beratungsgesellschaft mbH, Lütticherstraße 32, 52064 Aachen, Germany ; e-mail: [email protected] mbH Cuttings investigations in the RWTH-1 borehole We present the physical properties of the Carboniferous and Devonian Rocks drilled in the 2500 m deep RWTH-1 borehole. The borehole is located in the center of Aachen, in only few meter distance to the University main building. The geological setting is in front of the Aachen Overthrust , the large southeast dipping fault belt, which separates the Eifel Mountain geology from the northwestern foreland (Fig. 1). The well penetrates carboniferous and devonian formations, which are dominated by series of interlayered sandstones, siltstones and shales. Organic shales and thin coal layers were locally drilled in the upper 1016 m, as part of the Lower Carboniferous deltaic cycles. Carbonates only occurred in the underlying Upper Devonian series between 1016 and 1440 m. The deeper parts of the borehole are dominated by variegated shale and sandstone series, which are of Lower Devonian age (Ribbert 2006). Core-Log integration of physical properties 8 Thermal Conductivity (W/m/K) The density varies from 2.64 g/cm³ and 2.84 g/cm³ with a mean of 2.78 g/cm³. The thermal conductivity (TC) varies between 2.2 W/m/K and 8.9 W/m/K (Fig. 3). The high values can be explained by a high percentage of quartz. Quartz cemented clean sandstones are frequently observed in the deeper part of hole below 1895 m. In total 57 cutting samples were selected at a regular interval every 50 box th ., resulting in a depth interval of 50 m. On the cuttings, matrix density and thermal conductivity were measured (Fig. 2). Density was measured by a helium pycnometer; the thermal conductivity was determined with a line source device on a cuttings-water mixture. Since the rock porosity is very low (< 0.1%), the influence of the pore fluid on the effective thermal conductivity can be neglected. Cores samples were available for three sections (1392-1515 m, 2128-2143 m, 2536-2544 m) covering a total length of 150 m. On the cores, the following physical properties were measured by a multi-sensor core logger: gamma density, magnetic susceptibility and p-wave velocity. 6 4 2.65 2.7 2.75 2.8 Core and log data were compared with the petrographic core descriptions (Österreich 2005). In some cases petrophysical property variation follows the optical subdivision. This is valid for the carbonate bearing rocks and the thin sandstone interlayers. The separation made petrographically for the shales and siltstone can not be constrained by the petrophysical data. This is, because petrographical separation is guided by optical markers, such as colour and bedding changes, attributes which can, but must not have a 2.85 Matrix Density (g/m³) 12 Fig. 1: Geological setting of the RWTH-1 borehole in front of the Aachen Overthrust. Thermal Conductivity (W/m/K) 0. GR (GAPI) 200. K1 (%) 15. 2.64 2.68 2.72 2.76 2.8 2.84 2 4 6 0 Log Resistivity (ohm-m) 100 1000 Log/Core Log Core VP Gamma Ray Density (km/s) (API) (g/cm³) 5 6 80 120 Core Vp (km/s) 2.7 2.8 2.9 1440 1450 1460 1470 1480 1490 1500 1520 Carbonatic Sandstone Fig. 4: Petrophysical core and log data of the first core section compared with the petrographic core description. Shale Shaly Siltstone Sandy Siltstone Silty Shale Siltstone Sandstone Oberkarbon Westfal A 2.6 0 Silur 2.65 2.7 Gedauer Konglomerat Wilhelmine-Schichten Mittlerer Kohlenkalk Unterer Kohlenkalk = Etroeungt-Schichten Friesenrath-Schichten 2.8 2.85 2.9 Matrix Density (g/cm³) The core measurements have a good fit with the associated logging measurements of the borehole wall. Using the logging measurements, the borehole could be divided in 7 zones. These zones correspond with the stratigraphic subdivision of the borehole (Fig. 2). 2 ? 1000 3 Condroz-Schichten Cheiloceras-Kalk Famenne-Schiefer Frasnes-Schiefer mit Knollenkalken Oberer Massenkalk Grenzschiefer Unterer Massenkalk quadrigeminum-Schichten 2.75 10 Oberer Kohlenkalk II 8 Due to the paleoenvironment and post-sedimentary processes, the relation between the natural gamma activity and the relative clay volume differ between these zones. Using the natural gamma-ray log for each different zone, it was possible to calibrate the gamma-ray with the thermal conductivity measured on cores und cuttings. The zone identification made it possible to derive a continuous thermal conductivity profile over the entire borehole depth (Speer 2005). 4 ? Frequency Visé Tournal Famenne Oberdevon Frasnes Givet Gedinne 500 Eifel Unterkarbon 1000 Mitteldevon 1500 Ems 2000 Siegen 2500 Continuous thermal property profiles of the formation 0 Burgholz-Sandstein Walhorn-Schichten Unterdevon 3000 500 1 Krebs-Traufe-Schichten Namur 3500 Binnenwerke (mit 34 Flözen) I 1500 Vichter Konglomerat 6 4 5 Zweifall-Schichten “Siegener” Schichten Obere Arkose Bunte Schiefer mit Kalkknollen Bunte Schiefer mit Konglomeraten 2 III 2000 6 Untere Arkose 0 0 Fig. 2: Cuttings measurements of matrix density and thermal conductivity compared to the borehole zonation (after logging data) and the standard stratigraphic profile known from the Eifel mountains (after Knapp 1980). 2 3 4 5 6 7 8 9 Furthermore a continuous radiogenetic heat production profile was calculated over the borehole depth, derived from the spectral gamma log (Bücker & Rybach 1996). Thermal Conductivity (W/m/K) Fig. 3: Cross-plot and histograms of density and thermal conductivity measured on cuttings of the RWTH-1 borehole. References Bücker, C. & L. Rybach (1996): A simple method to determine heat production from gamma-ray logs. Marine and Petroleum Geology 13, 373-377 Österreich, B., (2005): Petrographische Beschreibung der RWTH-1 Kernsektionen. geologischer Dienst NRW, Krefeld. Knapp, G. (1980): Erläuterungen zur Geologischen Karte der nördlichen Eifel 1:10000. – 155 S., Geologischer Dienst Nordrhein-Westfalen, Krefeld. Speer, S., (2005): Design calculations for optimising a deep borehole heat exchanger, Diplomarbeit, Angewandte Geophysik, RWTH Aachen. Ribbert, K.H. (2006): Die Bohrung RWTH-1- Regionalstratigraphische Einordnung und Deutung. Interner Bericht, Geologischer Dienst NRW, Krefeld. 1 7 2500 Interner Bericht, 10 20 30 1430 4500 Außenwerke (mit 5 Flözen) Core Suszept. (SI) 1510 4 Breitgang-Schichten (mit 4 Flözen) 6 1420 sand - clay 4000 5 1410 8 8 10 1400 Frequency 0. 9 1390 Vp-data were used for comparing core with logging data. After the correction of a 1.2 m depth shift (log deeper core) and the use of a sliding window average on the core data, in-situ and laboratory data comes to an excellent fit (Fig. 4). The data fits best in the carbonate bearing section down to 1440 m and in the deepest part of core section 1. Between 1460 and 1490 m slight off-sets can be observed, which might be attributed to bedding anisotropies. Effects of a Vp lowering by pressure relief are not observed for the RWTH-1 cores. 2 Matrix Density (g/cm³) Caliper (in) 8 Depth (m) Beratungsgesellschaft The thermal properties are used for a design calculation of the (SuperC) borehole heat exchanger and for prognostic 3D modelling of heat flow and temperature in a larger region. Fig.6: Displayed are continuous thermal properties curves, calulated from logging data. TC-Am: Arithmetic mean - thermal conductivity profile; TC-Gm: Geometric mean - thermal conductivity profile; A: Heat production profile; VC: Volume of clay - displayed is the clay content and the quartz/carbonate rock matrix. Carbonatic Shale Shale and Limestone
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