Contrasting quartz and feldspar viscosities in natural strain and temperature gradients: preliminary study Prokop ZÁVADA, Karel SCHULMANN, Ondrej LEXA, Jiří KONOPÁSEK Institute of Petrology and Structural Geology, Charles University, Albertov 6, 128 43, Prague The rheological behaviour of polyphase rock systems such as conglomerates of granitoids depends on the bulk rock viscosity, the phase viscosity contrast, weak and strong phase fraction, and the initial clast shape. The viscosity contrasts were determined for pebbles of various compositions in natural conglomerates (Gay, 1969, Freeman and Lisle, 1987, Lisle and Savage, 1983). However, these rocks often exhibit non-uniform distribution of clast sizes, highly variable compositions, internal anisotropies of pebbles and varied ratios of clast matrix proportions. In addition, the rheological properties of pebbles are not known from experimental studies. We studied coarse-grained granitoids of similar original modal compositions (quartz (19%), K-feldspar (49%) and plagioclase (28%)), and relatively constant original grain size deformed at various temperatures. The samples were collected from two adjacent units forming a nappe pile at the western border of the Saxothuringian domain, Czech Republic. The upper unit consists of granulites, migmatized granulites, and coarse-grained orthogneisses (Bt, Grt ± sillimanite) deformed to variable degree at high temperatures close to the granulite facies conditions. The lower unit is composed of high pressure micaschists (Konopásek, 2001), mafic eclogitic bodies and sheets of medium-grade Ms-Bt orthogneisses. We compared the internal strain and deformational microstructures of both high-grade and medium-grade orthogneisses to depict the possible rheological behaviour of felsic rocks under various thermal conditions. The estimated viscosity ratios of individual phases and bulk rock are compared with their rheological properties determined experimentaly. The shapes of K-feldspars and quartz were digitized from XZ and YZ sections, their topology was traced in GIS Arc View environment and the shapes were analysed using the PolyLX Matlab™ toolbox. The particle shapes were approximated by ellipses and the shape ratios were calculated using the method by Harvey & Fergusson (1981). To estimate the bulk strain, the Fry’s method (Fry, 1979) was applied. The quartz of high-grade orthogneiss exhibits lower strain intensities than K-feldspar and plagioclase. The strain symmetry of all phases is in apparent flattening field, except for one sample in which the weak feldspars are strongly constricted. The medium-grade orthogneiss shows strong K-feldspar, weaker quartz and the weakest plagioclase. For the low bulk strain intensities, the strain symmetry of all phases is close to plane strain, but with increasing strain the shapes become oblate. The bulk strain in strongly deformed samples is difficult to establish using Fry’s method, due to the contribution of viscous deformation of strong phases and their passive displacement in weak matrix. Therefore, the viscosity contrasts between strong and weak phases were assessed using the Gay’s (1969) equation yielding values around μq/μfel = 0.5 – 0.6 for the high-grade orthogneiss, around 1 for the low strained medium-grade orthogneiss, and 2 – 3 for the highly sheared medium-grade rocks. This contrasting quartz and feldspar shape behaviour is correlated with their microstructural development. The medium-grade orthogneiss exhibits extremely fine-grained plagicolase (50) recrystallized even under very low strain intensities, fractured K-feldspar, which shows some recrystallization at grain margins and recrystalized quartz exhibiting a uniform grain size (0.5-1.2mmrarely 4mm). Weak grain boundary migration and rather straight grain boundaries are characteristic of all deformational stages. The high-grade orthogneiss consists of recrystallized aggregates of well-equilibrated plagicolase mosaic (0.6-0.8mm) and recrystallized K-feldspar (1.75mm) coated with narrow plagioclase-quartz films. Quartz grains with highly migrated grain boundaries (1.75-2.5mm in size) form globular aggregates. The microstructure is further quantified using the GIS Arc-View environment and the PolyLX Matlab™ toolbox to provide precise information about grain size, grain contacts and modal compositions of individual layers. In addition, the mineral CPO (crystallographic preferred orientation) is studied in order to reveal possible deformation mechanisms. The preliminary results show that the relative rheologies of feldspars and quartz in natural rocks are not consistent with experimental results. Their mechanical behaviour is probably highly sensitive to strain intensity as well as to temperature and recrystallization grain size. References: KONOPÁSEK J., SCHULMANN K. and LEXA O.,2001. Structural evolution of the central part of the Krušné hory (Erzgebirge) Mountains in the Czech Republic-evidence for changing stress regime during Variscan compression. Journal of Structural Geology, 23(9): 1373-1392. GAY N.C.,1969. The analysis of strain in the Barberton Mountain Land, Eastern Transvaal, using deformed pebbles. The Journal of Geology, 77: 377-396 FREEMAN B. and LISLE R. J.,1987. The relationship between strain and the threedimensional shape fabrics of pebbles in deformed conglomerates. Journal of the Geological Society, London,144: 635-639. LISLE R. J. and SAVAGE J., 1983. Factors influencing rock competence: Data from a Swedish deformed conglomerate. Geologiska Foreningens i Stockholm Forhandlinger, 104: 219-224. FRY N., 1979. Random point distributions and strain measurement in rocks. Tectonophysics, 60: 89-105 HARVEY P. K. and FERGUSON C. C., 1981. Directional properties of polygons and their application to finite strain estimation. Tectonophysics, 74: 33-42