the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
Dislocation creep and glide in experimentally deformed glaucophane aggregates
Abstract. Glaucophane is a key rheology-controlling mineral in the oceanic crust of subducting slabs at blueschist facies conditions. Studies of naturally deformed glaucophane suggest dislocation-related deformation mechanisms can be activated at some pressure-temperature-stress conditions in subduction environments; however, the strength of glaucophane deforming via these mechanisms remains unconstrained. To address this, we conducted load stepping experiments using a Griggs apparatus at temperatures of 600–700 °C, 1.0 GPa, and shear strain rates of ∼ 1.2×10−⁸ s-1 to ∼ 1.2×10−³ s-1, with a starting grain size of <63 µm. The mechanical data from these experiments show a transition in the stress exponent from 2.8 ± 0.2 at relatively low stresses, indicative of dislocation creep, to 14–19 at relatively high stresses, consistent with dislocation glide. Microstructural analyses show kinking, undulose extinction, and a shift from sharp linear grain boundaries in the hydrostatic samples to more rounded and lobate sutured grain boundaries in the deformed samples. High internal misorientations (subgrains, undulose extinction) in both relict and fine-grained regions of the deformed samples further support the activation of dislocation-related mechanisms. Based on these observations, we develop flow laws for dislocation creep n = 3, Q = 450 ± 15 kJ/mol, A =2.32x10¹⁰ MPa−n s-1) and dislocation glide (Q = 899 ± 43 kJ/mol, C = 1.83x10³², and α = 0.0123). Extrapolations of our flow laws to geologic conditions suggests that dislocation glide is unlikely to occur at steady state conditions, while dislocation creep dominates at temperatures above 450 °C at relatively large grain sizes of ∼1 mm or larger. These insights refine our understanding of glaucophane rheology and its implications for subduction zone mechanics.
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CC1: 'Comment on egusphere-2025-531', Bruno Reynard, 19 Feb 2025
Congratulations for this nice experimental work. I just wanted here to comment on deformation mechanisms I determined in natural glaucophanes (Reynard et al. 1989). The dislocation glide system (010)[001] at low temperature is a very peculiar one. It may not be well activated in your sample geometry. In natural samples, glide on that system is observed only coarse-grained sample with localized retromorphic deformation from the Sesia zone, which corroborates your interpretation that dislocation glide is likely activated at high-stress deformation events (slow-slip events?). High-temperature slip-systems explain well the CPO observed in high-grade blueschists and glaucophane-eclogites when critical resolved shear stresses attributed based on frequency of observations are used in VPSC simulations (Bezacier et al. 2010). It concurs with your conclusion that dislocation creep dominates above 450°C in glaucophane-rich rocks.
Citation: https://doi.org/10.5194/egusphere-2025-531-CC1 -
RC1: 'Comment on egusphere-2025-531', Hugues Raimbourg, 18 Mar 2025
The comment was uploaded in the form of a supplement: https://egusphere.copernicus.org/preprints/2025/egusphere-2025-531/egusphere-2025-531-RC1-supplement.pdf
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AC1: 'Reply on RC1', Leif Tokle, 14 Apr 2025
The comment was uploaded in the form of a supplement: https://egusphere.copernicus.org/preprints/2025/egusphere-2025-531/egusphere-2025-531-AC1-supplement.pdf
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AC1: 'Reply on RC1', Leif Tokle, 14 Apr 2025
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RC2: 'Comment on egusphere-2025-531', Anonymous Referee #2, 27 Mar 2025
The manuscript by Hufford et al. presents a set of load-stepping experiments done to construct rheological flow laws of the sodic-rich amphibole, glaucophane. Relying on mechanical and microstructural analysis, the authors construct deformation mechanism maps for glaucophane and use the empirical law to extrapolate to natural conditions and compare glaucophane viscosity with other related subduction zones rocks such as eclogites and metasediments.
Glaucophane is an important mineral in the blueschist's facies of a subducting slab, with numerous field observations linking glaucophane rheology to the medium dynamic properties. It is, therefore, evident that providing the rheological constraints to develop a flow law for glaucophane will have great importance to the community.
However, as detailed below, I find the experimental and microstructure analyses insufficient to decipher the deformation mechanism and subsequently to construct the flow laws.
- Load-stepping experiments – Usually, in these types of experiments, the sample is stressed in a (quasi-)elastic stage until the sample yields. Afterwards, there are 3-4 additional strain-rate steps. This way, the elastic part is an initial stage separated from the post-yield stage, where the strain rates steps are performed. In the manuscript, it is mentioned that they tried to avoid brittle-cataclastic behavior at peak stresses (lines 79-81). However, I wonder if some of the strain-rate steps do not contain a contribution from the elastic stage.
In addition, having 9 different strain-rate steps in a single run without repeating strain rates ignores the likely effect of hardening (strength dependence on total strain) often seen in semi-brittle and low-temperature plasticity mechanisms. Without having more constraints over the possible effect of strain on sample strength (e.g., single-load or strain rate experiment), it will be difficult to evaluate the current data. - Microstructural analysis. Actually, little difference is observed between hydrostatic pressed samples (i.e., sample initial state) and the deformed samples. The main difference highlighted by the authors is the grain boundary morphology of the small grains. However, with the analysis shown, it was not clear to me that there is indeed such a difference. Actually, with the existing resolution images from the optical microscope and EBSD maps, I could not see much of the boundaries between small grains (EBSD scans include small unindexed areas just around small grains, Fig. 3). Again, experiments with a single load or strain rate can be much more useful for microstructural analysis since the microstructure does not experience multiple strain rates (and perhaps multiple deformation mechanisms).
- Figure 8 in this manuscript and Figure 12 in the companion manuscript are almost identical, except for the different line labelled “this study dislocation creep in glaucophane”. I am confused about why the same authors suggest two different dislocation creep flow laws for glaucophane in two companion papers (without even including their own other law?!).
- The existence and possible effects of fracturing on the rheological interpretations are important, which was nicely done in Fig. 6 of the companion paper, relating to dislocations and fractures.
- In conclusion, the set of experiments presented here is interesting and valuable but insufficient for the findings presented.
Citation: https://doi.org/10.5194/egusphere-2025-531-RC2 -
AC2: 'Reply on RC2', Leif Tokle, 14 Apr 2025
The comment was uploaded in the form of a supplement: https://egusphere.copernicus.org/preprints/2025/egusphere-2025-531/egusphere-2025-531-AC2-supplement.pdf
- Load-stepping experiments – Usually, in these types of experiments, the sample is stressed in a (quasi-)elastic stage until the sample yields. Afterwards, there are 3-4 additional strain-rate steps. This way, the elastic part is an initial stage separated from the post-yield stage, where the strain rates steps are performed. In the manuscript, it is mentioned that they tried to avoid brittle-cataclastic behavior at peak stresses (lines 79-81). However, I wonder if some of the strain-rate steps do not contain a contribution from the elastic stage.
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