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Quantifying the A -site occupancy in amphiboles: a Raman study in the OH-stretching region
Solid solution along the synthetic LiAlSi 2 O 6 -LiFeSi 2 O 6 (spodumene-ferri-spodumene) join: A general picture of solid solutions, bond lengths, lattice strains, steric effects, symmetries, and chemical compositions of Li clinopyroxenes
Crystal-chemistry of Synthetic Amphiboles Along the Richterite–ferro-richterite Join: a Combined Spectroscopic (ftir, MÖssbauer), Xrpd, and Microchemical Study
The cooling kinetics of plagioclase feldspar as revealed by electron-microprobe mapping
Phase transition induced by solid solution: The B Ca- B Mg substitution in richteritic amphiboles
The P 2 1 / m - C 2/ m phase transition in synthetic amphiboles in the system Li 2 O–Na 2 O–MgO–SiO 2 –H 2 O: a high- T FTIR study
The thermal behavior of richterite
Magnesium K -edge EXAFS study of bond-length behavior in synthetic pyrope-grossular garnet solid solutions
Non-Ambient in situ Studies of Amphiboles
Site preference and local geometry of Sc in garnets: Part I. Multifarious mechanisms in the pyrope-grossular join
Parvo-mangano-edenite, parvo-manganotremolite, and the solid solution between Ca and Mn 2+ at the M4 site in amphiboles
Synthetic P 2 1 / m amphiboles in the system Li 2 O-Na 2 O-MgO-SiO 2 -H 2 O (LNMSH)
Synchrotron infrared spectroscopy of synthetic Na(NaMg)Mg 5 Si 8 O 22 (OH) 2 up to 30 GPa: Insight on a new high-pressure amphibole polymorph
SHORT-RANGE ORDER IN MINERALS: AMPHIBOLES
The (Mg,Fe 2+ ) substitution in ferri-clinoholmquistite, □Li 2 (Mg,Fe 2+ ) 3 Fe 3+ 2 O 22 (OH) 2
Synthesis and crystal-chemistry of alkali amphiboles in the system Na 2 O-MgO-FeO-Fe 2 O 3 -SiO 2 -H 2 O as a function of f O 2
The kinematics of lava flows inferred from the structural analysis of enclaves: A review
Most lavas are viscous laminar flows, and the roles played by different physical, chemical, and geometric parameters on the mechanism of flow emplacement are relatively well known. However, the kinematics of lavas and the style of flow deformation are still poorly known. Strain indicators of lavas include stretched vesicles, enclaves, crystal and Anisotropy of magnetic susceptibility fabrics, and folds. Enclaves may show different shapes: subcircular to ellipsoidal enclaves, rolling-like structures, boudin-like structures, banding-like structures, and folds. Here, we discuss the constraints that must be satisfied for the use of enclaves as strain indicators, and review the analytical techniques that can be used to determine the finite pure shear α and simple shear strain γ. We review three lava flows cropping on the Porri Volcano (Salina Island, southern Tyrrhenian Sea, Italy) as case study. In these lavas, enclaves of different shapes have been selected at different places (vent, intermediate, and front zone). The structural analysis of the enclaves allows us to determine the ratio between α and γ. The kinematic vorticity number, Wk , which is a measure of noncoaxiality, ranges between 0.1 and 0.7 in the vent zone, and increases up to 0.9–1 at the front. The prevailing pure shear deformation at the vent is due to the lateral extension of the flow, whereas the simple shear increments are acquired during the lava flow motion owing to gravity. Lava flows are extensional to hyperbolic flows at the vent and intermediate zones, whereas they may be considered as ideal simple shear flows near the front zone.