guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
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Guide <strong>to</strong> Thin Section Microscopy<br />
Cleavage and fracture<br />
Deformation and recrystallization<br />
Minerals in metamorphic rocks respond in different ways <strong>to</strong> tec<strong>to</strong>nic stress, depending on prevailing<br />
temperature conditions, deformation rates, level <strong>of</strong> differential stress and presence or<br />
absence <strong>of</strong> fluids. Generally speaking, minerals at low temperatures tend <strong>to</strong> show brittle<br />
behaviour, whereas they deform plastically at high temperature. The temperatures <strong>of</strong> the<br />
transition between brittle and plastic behaviour are mineral-specific (about 300˚C for quartz,<br />
400-500˚C for feldspars, at deformation rates that are typical for orogenic processes).<br />
Figure 3-13 shows typical microstructures produced through brittle deformation at low<br />
temperature. At the brittle-ductile transition, mineral grains may show features <strong>of</strong> both brittle<br />
(fracturing, cataclasis) and plastic behaviour (undulose extinction, kinking, bending).<br />
Figure 3-13. Brittle deformation behaviour <strong>of</strong> mineral grains<br />
A: Domino-style fracturing <strong>of</strong> sillimanite crystal. B: Cataclastic deformation <strong>of</strong> quartz. C: Broken and kinked<br />
glaucophane crystals in micr<strong>of</strong>old. D: Cataclastic deformation <strong>of</strong> plagioclase. E,F: Microboudinage <strong>of</strong> biotite<br />
and <strong>to</strong>urmaline. The open fractures are filled with quartz.<br />
(Pho<strong>to</strong>micrographs − B: Michael Stipp, IFM-Geomar Kiel; E,F: Bernardo Cesare, University <strong>of</strong> Padova)<br />
Raith, Raase & Reinhardt – February 2012<br />
In the polarized-light microscope, plastic crystal deformation is indicated where mineral<br />
grains show bending or kinking <strong>of</strong> normally planar morphological elements such as cleavage,<br />
rational crystal faces or twin planes (Fig. 3-14). The continuous or discontinuous change <strong>of</strong><br />
crystal lattice orientation wi<strong>thin</strong> a single mineral grain corresponds <strong>to</strong> a gradual or abrupt<br />
shift <strong>of</strong> the extinction position as the microscope stage is turned. Even where distinct morphological<br />
elements are lacking (as in quartz), deformation can be recognised from the nonuniform<br />
extinction positions <strong>of</strong> different domains wi<strong>thin</strong> a grain (Fig. 3-14 J,L). These deformation<br />
features are caused by stress-induced intracrystalline processes such as dislocation<br />
glide and dislocation creep. Plastic deformation <strong>of</strong> crystal lattices may be continuous over a<br />
mineral grain or affect discrete grain domains only. Deformation lamellae or translation<br />
lamellae may form along defined glide planes (Fig. 3-14 K; 3-15 H).<br />
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