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Quantitative structural analyses and numerical modelling of ...

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DTD 5ARTICLE IN PRESSL. Baratoux et al. / Journal <strong>of</strong> Structural Geology xx (xxxx) 1–24 9Fig. 5. Field photographs <strong>of</strong> typical fold shapes: (a) garnet zone, (b) staurolite zone, (c) sillimanite zone <strong>and</strong> (d) sillimanite zone <strong>of</strong> the pluton aureole. Chevronfolds are typical for the garnet zone (a), flattened folds with high amplitude are characteristic <strong>of</strong> the staurolite zone (b), <strong>and</strong> similar folds with rather lowamplitudes are present in the sillimanite zone (c). Steep foliation with relic F 3 folds characterize the sillimanite zone in the pluton aureole (d).<strong>of</strong> the post buckle flattening). This graph shows therelationship between these two different expressions <strong>of</strong>shortening. In order to illustrate the geometric implications<strong>of</strong> this graph we have plotted the fold patterns <strong>of</strong> the modelmultilayer sequences given by Ramsay <strong>and</strong> Huber (1987,pp. 414–415) (Fig. 6). This shows clearly the effect <strong>of</strong> theviscosity ratio (m 1 /m 2 ), layer thickness ratio (nZd 1 /d 2 ) <strong>and</strong>the amount <strong>of</strong> superimposed strain on the folds positionon the graph. Folded incompetent layers plot in the left half<strong>of</strong> the diagram <strong>and</strong> the slope <strong>of</strong> the data points shows thestrong negative correlation between the b 1 <strong>and</strong> F parameters.Folded competent layers plot in the right half <strong>of</strong> thediagram <strong>and</strong> the steeper slope <strong>of</strong> the data point trend shows aless pronounced positive correlation between the b 1 <strong>and</strong> Fparameters (Fig. 6).We have used these plots as st<strong>and</strong>ards with which wecompared the plots representing the natural folds from thestudy area. In addition to the qualitative estimate <strong>of</strong> theviscosity contrast <strong>and</strong> the proportion <strong>of</strong> incompetent tocompetent fraction, we can deduce semi-quantitatively theactive amplification <strong>of</strong> the buckle fold <strong>and</strong> the amount <strong>of</strong>post-buckle shortening. The histograms <strong>of</strong> the F values <strong>and</strong>b 3 /b 1 ratios for each <strong>of</strong> the folds studied are given in Fig. 7.4.2. <strong>Quantitative</strong> analysis <strong>of</strong> fold styles in the garnet zoneThe post peak metamorphic folds in the eastern part <strong>of</strong>the massif, i.e. in the garnet zone, display only a smallvariation in shape. The post buckle flattening is small, asdocumented by relatively low positive values <strong>of</strong> F (0.8–3)(Fig. 7a), which approximates to a parallel or weaklyflattened parallel fold. Very few folds in this domain belongto class 3A, i.e. folds that exhibit relatively small negativevalues <strong>of</strong> F (Fig. 7a). The dominance <strong>of</strong> class 1B (i.e.parallel) folds is important as it documents that activebuckling played a major role during the fold amplification<strong>and</strong> that post-buckle flattening was subordinate. The shapesacquired from the harmonic Fourier analysis lie betweenchevron <strong>and</strong> sine wave, as can be seen from the histogram <strong>of</strong>b 3 /b 1 (Fig. 5a), which has an average value <strong>of</strong> b 3 /b 1 ZK0.05. The absolute values <strong>of</strong> both F <strong>and</strong> b 1 are low(F max Z3; b 1max Z3), suggesting a low amount <strong>of</strong> deformation<strong>of</strong> the analysed rocks. A comparison <strong>of</strong> the measuredfold shapes plotted on the b 1 vs. F diagram with the modelmultilayer sequences (Fig. 6) indicates that the fieldexamples show a close resemblance to model folds (type5, i.e. folds characterized by a high viscosity ratio (m 1 /m 2 )117

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