the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
| 17 Jun 2022
Shear zone evolution and the path of earthquake rupture
Abstract. Plate boundary shear zones generate earthquakes, which are at present unpredictable, but advances in mechanistic understanding of the earthquake cycle offer hope for future advances in earthquake forecasting. Studies of fault zone architecture have the potential to reveal the controls on fault rupture, locking, and reloading that control the temporal and spatial patterns of earthquakes. The Pofadder Shear Zone exposed in the Orange River in South Africa is an ancient, exhumed, paleoseismogenic continental transform which preserves the architecture of the earthquake source near the base of the seismogenic zone. To investigate the controls on earthquake rupture geometries in the seismogenic crust, we produced a high resolution geologic map of the mylonite zone which forms the shear zone core. The core consists of thin, pinch-and-swell layers of mylonites of variable mineralogic composition, reflecting the diversity of regional rock types which were dragged into the shear zone. Our map displays centimetric bands of a unique black ultramylonite along some mylonite layer interfaces. We present a set of criteria for identifying recrystallized pseudotachylytes (preserved earthquake frictional melts) and show that the black ultramylonite is a recrystallized pseudotachylyte, with its distribution representing a map of ancient earthquake rupture surfaces. We then compare the attributes of lithologic interfaces which hosted earthquakes with those which apparently did not, and find that their geometry differs meaningfully at wavelengths of 
10 m. We argue that the pinch-and-swell structure of the mylonitic layering, enhanced by viscosity contrasts between layers of different mineralogy, is expected to generate spatially heterogeneous stress during viscous creep in the shear zone, which dictated the path that earthquake ruptures followed. The condition of rheologically layered materials causing heterogeneous stresses should be reasonably expected in any major shear zone, is enhanced by creep, and represents the pre-seismic background conditions through which earthquakes nucleate and propagate. This has implications for patterns of earthquake recurrence and explains why some potential geologic surfaces are favored for earthquake rupture over others.
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RC1: 'Comment on egusphere-2022-446', Friedrich Hawemann, 22 Jun 2022
Young and coauthors present a study of a well exposed core of a shear zone. The main hypothesis of the manuscript is that preexisting lithological heterogeneities on a small scale guides the rupture geometry of earthquakes. The manuscript is well written and well structured and proper observations are made and appropriate methods to underpin the interpretations are used. The systematic approach and methods used for the quantification of the geometry are novel in this field of study. The topic is definitely very suitable regarding the scope of the Solid Earth journal. Before publication, I would like to request revisions on the raised concerns regarding the timing of deformation and associated geometries as well as the careful remake of some figures.
Friedrich Hawemann
General comments
The topic of where seismic rupture takes place is of high importance, and the idea that pseudotachylyte can often be found at rheological boundaries is valid, and has been observed before, also as bounding boudins (Toy et al 2011). In my opinion, this is not the best field site to establish this relationship, as the ductile deformation following pseudotachylyte emplacement is significant and alters the original geometries. The ultramylonite bands wrap around the pinch and swell structures and boudins, and therefore the pseudotachylyte generation predates these features. However, the authors argue that the stress concentrations necessary to form the pseudotachylyte, are generated by the pinch and swell geometries (line 540).
Maybe it is possible to explain the observed geometries and distribution of pst like this:
Pseudotachylylte is generated along a lithological boundary. Pst are weaker than the host rock(s) during subsequent ductile shear, effectively lubricating the boundary and facilitate the formation of pinch and swell structures.
Furthermore, the thickness of the former pseudotachylytes is quite astonishing, considering a formation by a local stress variation. Also, pseudotachylytes generated by local stress variations are more likely to crosscut the mylonitic fabric, and this should be still visible even after further ductile overprint (Toy et al 2011, Hawemann et al 2019, Campbell et al 2020).
Also, the analysis of the interfaces of pst-bearing and non-bearing contacts is hard to validate, as present-day geometries are not the geometries at the time of emplacement of the pseudotachylytes.
I would therefore recommend either a thorough and robust explanation of the timing of the structures or a significant reinterpretation of the observed geometries before publication.
Minor comments.
The introduction has to be extended towards the literature existing on the topics handled by the manuscript.
It is also surprising to never see new pseudotachylyte form next to a previous generation of pseudotachylyte, as they also should offer a high competence contrast.
Please also note the annotated pdf with comments!
The descriptions and interpretations in this manuscript are very well and carefully executed. But they have to be supported by higher quality figures. Here are some comments on how to improve the figures, some pictures may have to be redrawn or retaken.
Figure 2:
The legend for the stereonet is bigger and placed more prominently than the stereonet itself. Change 000 to “N”. Try to place the scalebar more intuitively, for example just use a 1 m scale on the map itself.
The map itself has a bit unpleasant colours. The background drone image is not advantageous as a background here, as it does not add any information. Maybe try to give some transparency to the geology-layer, also makes the colours more digestible. The contacts are all jagged lines, sadly. A lot of orientation data is presented, but does not add all too much, as this information is nicely shown in the stereoplot already. Maybe you could trace some foliations, would offer a more intuitive way to look at it. Also, some layers are offset by the late fractures, these should therefore be included into the map.
As the map is really a crucial part of this manuscript and is presented as “highly detailed”, it would be great to see it being improved and more carefully prepared.
Figure 3: “All photos oriented with dominant foliation (NW) across the photo.” That still leaves two possible orientations. Otherwise the photos are okay, even though the various tools for scale fill up a significant part of the image for no good reason – something to consider in the next field season.
Figure 4: What is the orientation of these images?
Really low contrast in SEM Images, very dull, out of focus polarization microscope images.
Figure 6 a: out of focus and the PPL image shows some ghost topography- looks like the Analyzer was not retracted completely. Remove the dashed line along the mylonite- ultramylonite boundary. A white number 8 got lost in the upper part of a).
Figure 6a:
I think it is a very good idea to make this list and show the observations in the samples and I don’t doubt a pst origin for these ultramylonites. However, the quality of the images and their scale often make it impossible to really support your interpretation of the microstructure.
(2) Flow banding is not easy to argue for here, I think, as it is parallel to the foliation.
(7) It is not very obvious that this is a polycrystalline clast. It looks to me like a feldspar with inclusions.
(3) To me the boundary looks parallel to the host rock foliation.
(5) I cannot see that on this scale.
Remove the dashed lines in e and b.
References used in comments
Campbell, L.R., Menegon, L., Fagereng, Å. et al. Earthquake nucleation in the lower crust by local stress amplification. Nat Commun 11, 1322 (2020). https://doi.org/10.1038/s41467-020-15150-x
Glikson, A. Y., & Mernagh, T. P. (1990). Significance of pseudotachylite vein systems, Giles basic/uItrabasic complex, Tomkinson Ranges, western Musgrave Block, central Australia. Journal of Australian Geology & Geophysics, 11, 509–519
Hawemann, F., Mancktelow, N. S., Pennacchioni, G., Wex, S., and Camacho, A.: Weak and slow, strong and fast: How shear zones evolve in a dry continental crust (Musgrave Ranges, Central Australia), J. Geophys. Res.-Sol. Ea., 124, 219–240, https://doi.org/10.1029/2018JB016559, 2019.
Menegon, L., Pennacchioni, G., Malaspina, N., Harris, K., and Wood, E.: Earthquakes as precursors of ductile shear zones in the dry and strong lower crust, Geochem. Geophy. Geosy., 18, 4356–4374, https://doi.org/10.1002/2017GC007189, 2017.
Virginia G. Toy, Samuel Ritchie, Richard H. Sibson, 2011. "Diverse habitats of pseudotachylytes in the Alpine Fault Zone and relationships to current seismicity", Geology of the Earthquake Source: A Volume in Honour of Rick Sibson, Å. Fagereng, V. G. Toy, J. V. Rowland
- AC1: 'Reply on RC1', Erik Young, 02 Sep 2022
-
RC2: 'Comment on egusphere-2022-446', Simone Papa, 14 Jul 2022
Review of “Shear zone evolution and the path of earthquake rupture” by Erik M. Young et al.
In this manuscript, Young et al. integrate field and microstructural mapping of a seismogenic fault core exhumed from the base of the seismogenic zone. They focus on the distribution of earthquake slip surfaces to understand what dictates the path of the earthquake rupture within a mylonitic shear zone. They conclude that stress heterogeneity at the scale of the lithologic layering is the most important factor controlling the path followed by the earthquake rupture.
The central question of the manuscript, i.e. what controls the path of earthquake rupture, is certainly an important one in earthquake mechanics and the methods used to address it are appropriate and with regard to the quantitative mapping of contact shapes (paragraph 4.2) are also novel. The manuscript is very well written and organised, the data presented are of good quality and substantially in agreement with the conclusion drawn by the authors, although I suggest more caution should be exercised in the interpretation and certain limitations should be discussed further. The new data and field observation, the quantitative analyses and related discussions certainly provide advances within the field and therefore I consider the manuscript fit for publication, provided that the following issues are addressed by the authors.
General comments
- The highlight of the paper is the detailed field mapping of an exceptional exposure and related analysis of which surfaces are preferentially exploited by pseudotachylytes (i.e. seismic ruptures). The authors show persuasive evidence that pseudotachylytes occur preferentially along pre-existent interfaces and in particular along interfaces with the highest viscosity rocks and viscosity contrast. They also show how pseudotachylyte-bearing interfaces are geometrically different from pseudotachylyte-absent interfaces. This last finding however is of difficult interpretation, since the present-day interface geometry is certainly not the same as it was at the time of pseudotachylyte emplacement. In chapter 5.2.3 the authors discuss this uncertainty and consider “the possibility that the observed pattern may be the result, rather than the cause, of seismic slip”. Furthermore, at line 485 and following, they also consider the possibility that “the enhanced long-wavelength roughness is caused by the pseudotachylyte itself … that interferes with the progression of boudinage along an interface”. In saying so, the authors acknowledge that boudinage may actually follow pseudotachylyte formation and not predate it. In the light of this, I do not see why the authors in their conclusion suggest that stress concentrations that dictate the path of seismic rupture are caused by pinch-and-swell geometries, although there is no clear evidence that pinch-and-swell geometries were present at the time of pseudotachylyte formation. In chapter 5.2.2 the authors argue that the patterns of pinch-and-swell layering imply an heterogeneous stress distribution, not that they cause it. The authors should clarify that the stress heterogeneities dictating rupture path are the result of the viscosity contrast across the interfaces and should be more cautious when interpreting pinch-and-swell geometries as the cause of stress heterogeneity. Or at least they should discuss this matter further, as they have done in chapter 5.2.3 for interface geometry.
- Several times throughout the paper, the authors refer to interfaces that juxtapose similar wall rocks (e.g. in Table 2 and at line 319). It is never explained what these contacts are and what they look like since they are not shown in any figure. The second part of table 2 seems to imply that pseudotachylyte segments with similar wall rocks are actually exploiting some kind of interfaces within these lithologies (e.g. foliation planes, c’ surfaces, fractures, joints ???). Otherwise I do not understand what the “total length of contact type” for similar wall rocks (sw) stands for and why you calculate what percentage of these contacts is decorated by pseudotachylytes. This is an important point to clarify because at present it is not clear if segments of pseudotachylytes with similar wall rocks are crosscutting intact rock (as stated at line 483) or are exploiting some pre-existent interface (as implied by table 2).
- The authors repeatedly state that the map is highly detailed and accurate to 1 cm. However, most of the layers in the map are much thicker than a few cm and not many centimetric layers are mapped. For example, are centimetric layers like those shown in Figs. 3b and 3e actually mapped?
Specific comments
Line 38 (e.g. Swanson, 1998 …)
Campbell et al. (Scottish Journal of Geology (2019) 55 (2): 75–92.) could be an appropriate paper to cite here as a field study that deals with relationship of seismic rupture with foliation and lithology in an amphibolitic shear zone.
Lines 71-72 “Both the pseudotachylyte and dynamic breccias have been shown to be mutually crosscutting with mylonitic foliations”
Is this true also for the outcrop studied in this paper? If so, it has an important bearing in your observations and discussions. Maybe an example could be shown in a figure.
Line 103 “1-50 cm-thick layers”
Throughout the paper inconsistent ranges of thickness for the layers are reported (e.g. 1-50 cm at line 103, 20-180 cm at line 111, 2-60 cm at line 411). Actually, the quartz mylonite layer in the right-hand-side of the map is more than 300 cm thick!
Line 113 “< 20 cm thick bands of nearly constant width”
Although commonly < 20 cm thick, black ultramylonite layers in the map are locally up to 50 cm thick. Also, I do not agree that they have constant width, to a visual approximation they seem to pinch and swell like the others.
Line 126
The term quartz mylonite has been extensively used in the literature to define mylonitic quartz veins or quartzite, mostly made of pure quartz (e.g. Mainprice and Casey, 1990, Geophys. J. Int.; Ralser, Hobbs and Ord, 1991, J. Struct. Geol.; Grujic, Stipp and Wooden, 2011, Geochem. Geophys. Geosystems.). To avoid confusion, I would suggest to use a different name, maybe quartz-rich mylonites?
Line 148
Porphyroclastic mylonite is referred to as “porphyritic” in figure 3b and caption.
Line 169 “only lithology observed cross-cutting foliation planes of other mylonites.”
This is an important observation, it would be nice to have a figure showing this in the paper.
Line 172-173 “… photomicrograph mosaics …”
I suggest to provide at least an example of the photomicrograph mosaics and the result of image analysis in the supplementary material.
Line 220
Characteristics 2 and 6 seem a bit contradictory (preserved flow banding (2) and absent compositional banding (6)).
Lines 243-244
7.75/11 and 2.5/11 instead of 7.75/10 and 2.5/10
Line 245 “coarsening of pseudotachylytes”
Do you mean coarsening of grain size of pseudotachylytes or coarsening of pseudotachylytes themselves?
Line 278 “< 1-13”
Actually locally they are at least 50 cm thick.
Line 280
The thickness of black ultramylonite layers is locally outstanding, making them very unlikely to represent the mylonitic deformation of a single pseudotachylyte. Probably, when a pseudotachylyte decorates an interface, this becomes a preferential rupture pathway for the next one. This is in agreement to your finding that interfaces with high viscosity contrast are preferentially exploited. Maybe you could discuss this further.
Line 303
The relative competence ranking is only qualitative and, although reasonable, seems a bit speculative. To improve the robustness of this chapter I would suggest to select figures showing key contact morphologies that you refer to in the text to justify the ranking.
Line 305
Better use “amplitude/wavelength” instead of “amplitude:wavelength”
Line 325-326 “as it makes cusps…Figure 3A”
To me it is not clear where you see this in figure 3A.
Lines 329-330
Although it is reasonable that the quartz mylonite is the weakest lithology, I wonder if you have an explanation for fig. 3D, that shows the quartz mylonite boudinaged within the granitic mylonite. Should this not mean that the quartz mylonite is more competent than the granitic mylonite?
Line 332
Can you explain why you selected these segments? Was it not possible to use all the interfaces mapped to have more robust results?
Line 338
What the PSD is should be explained somewhere in the text.
Line 338
“Figure 7c, e” instead of “Figure 7d, e”
Line 363
“Figure 7b, c” instead of “Figure 7d, e”
Line 403
“Fitz Gerald and Stünitz” instead of “Gerald and Stünitz”. Change also in the references.
Line 423-424 “the highest melting point … occurs in plagioclase”
Actually plagioclase has a lower melting point than quartz. Check Spray (2010).
Line 429 “high frictional heating (plagioclase)”
If by this you mean that plagioclase has the highest melting point, then it should be quartz instead.
Line 540 “pinch-swell geometries, which causes stress concentrations”
Are stress heterogeneities caused specifically by pinch-swell geometries, or are they inherent to the viscosity contrast between different layers?
Simone Papa
University of Padova
Citation: https://doi.org/10.5194/egusphere-2022-446-RC2 - AC2: 'Reply on RC2', Erik Young, 02 Sep 2022
Interactive discussion
Status: closed
-
RC1: 'Comment on egusphere-2022-446', Friedrich Hawemann, 22 Jun 2022
Young and coauthors present a study of a well exposed core of a shear zone. The main hypothesis of the manuscript is that preexisting lithological heterogeneities on a small scale guides the rupture geometry of earthquakes. The manuscript is well written and well structured and proper observations are made and appropriate methods to underpin the interpretations are used. The systematic approach and methods used for the quantification of the geometry are novel in this field of study. The topic is definitely very suitable regarding the scope of the Solid Earth journal. Before publication, I would like to request revisions on the raised concerns regarding the timing of deformation and associated geometries as well as the careful remake of some figures.
Friedrich Hawemann
General comments
The topic of where seismic rupture takes place is of high importance, and the idea that pseudotachylyte can often be found at rheological boundaries is valid, and has been observed before, also as bounding boudins (Toy et al 2011). In my opinion, this is not the best field site to establish this relationship, as the ductile deformation following pseudotachylyte emplacement is significant and alters the original geometries. The ultramylonite bands wrap around the pinch and swell structures and boudins, and therefore the pseudotachylyte generation predates these features. However, the authors argue that the stress concentrations necessary to form the pseudotachylyte, are generated by the pinch and swell geometries (line 540).
Maybe it is possible to explain the observed geometries and distribution of pst like this:
Pseudotachylylte is generated along a lithological boundary. Pst are weaker than the host rock(s) during subsequent ductile shear, effectively lubricating the boundary and facilitate the formation of pinch and swell structures.
Furthermore, the thickness of the former pseudotachylytes is quite astonishing, considering a formation by a local stress variation. Also, pseudotachylytes generated by local stress variations are more likely to crosscut the mylonitic fabric, and this should be still visible even after further ductile overprint (Toy et al 2011, Hawemann et al 2019, Campbell et al 2020).
Also, the analysis of the interfaces of pst-bearing and non-bearing contacts is hard to validate, as present-day geometries are not the geometries at the time of emplacement of the pseudotachylytes.
I would therefore recommend either a thorough and robust explanation of the timing of the structures or a significant reinterpretation of the observed geometries before publication.
Minor comments.
The introduction has to be extended towards the literature existing on the topics handled by the manuscript.
It is also surprising to never see new pseudotachylyte form next to a previous generation of pseudotachylyte, as they also should offer a high competence contrast.
Please also note the annotated pdf with comments!
The descriptions and interpretations in this manuscript are very well and carefully executed. But they have to be supported by higher quality figures. Here are some comments on how to improve the figures, some pictures may have to be redrawn or retaken.
Figure 2:
The legend for the stereonet is bigger and placed more prominently than the stereonet itself. Change 000 to “N”. Try to place the scalebar more intuitively, for example just use a 1 m scale on the map itself.
The map itself has a bit unpleasant colours. The background drone image is not advantageous as a background here, as it does not add any information. Maybe try to give some transparency to the geology-layer, also makes the colours more digestible. The contacts are all jagged lines, sadly. A lot of orientation data is presented, but does not add all too much, as this information is nicely shown in the stereoplot already. Maybe you could trace some foliations, would offer a more intuitive way to look at it. Also, some layers are offset by the late fractures, these should therefore be included into the map.
As the map is really a crucial part of this manuscript and is presented as “highly detailed”, it would be great to see it being improved and more carefully prepared.
Figure 3: “All photos oriented with dominant foliation (NW) across the photo.” That still leaves two possible orientations. Otherwise the photos are okay, even though the various tools for scale fill up a significant part of the image for no good reason – something to consider in the next field season.
Figure 4: What is the orientation of these images?
Really low contrast in SEM Images, very dull, out of focus polarization microscope images.
Figure 6 a: out of focus and the PPL image shows some ghost topography- looks like the Analyzer was not retracted completely. Remove the dashed line along the mylonite- ultramylonite boundary. A white number 8 got lost in the upper part of a).
Figure 6a:
I think it is a very good idea to make this list and show the observations in the samples and I don’t doubt a pst origin for these ultramylonites. However, the quality of the images and their scale often make it impossible to really support your interpretation of the microstructure.
(2) Flow banding is not easy to argue for here, I think, as it is parallel to the foliation.
(7) It is not very obvious that this is a polycrystalline clast. It looks to me like a feldspar with inclusions.
(3) To me the boundary looks parallel to the host rock foliation.
(5) I cannot see that on this scale.
Remove the dashed lines in e and b.
References used in comments
Campbell, L.R., Menegon, L., Fagereng, Å. et al. Earthquake nucleation in the lower crust by local stress amplification. Nat Commun 11, 1322 (2020). https://doi.org/10.1038/s41467-020-15150-x
Glikson, A. Y., & Mernagh, T. P. (1990). Significance of pseudotachylite vein systems, Giles basic/uItrabasic complex, Tomkinson Ranges, western Musgrave Block, central Australia. Journal of Australian Geology & Geophysics, 11, 509–519
Hawemann, F., Mancktelow, N. S., Pennacchioni, G., Wex, S., and Camacho, A.: Weak and slow, strong and fast: How shear zones evolve in a dry continental crust (Musgrave Ranges, Central Australia), J. Geophys. Res.-Sol. Ea., 124, 219–240, https://doi.org/10.1029/2018JB016559, 2019.
Menegon, L., Pennacchioni, G., Malaspina, N., Harris, K., and Wood, E.: Earthquakes as precursors of ductile shear zones in the dry and strong lower crust, Geochem. Geophy. Geosy., 18, 4356–4374, https://doi.org/10.1002/2017GC007189, 2017.
Virginia G. Toy, Samuel Ritchie, Richard H. Sibson, 2011. "Diverse habitats of pseudotachylytes in the Alpine Fault Zone and relationships to current seismicity", Geology of the Earthquake Source: A Volume in Honour of Rick Sibson, Å. Fagereng, V. G. Toy, J. V. Rowland
- AC1: 'Reply on RC1', Erik Young, 02 Sep 2022
-
RC2: 'Comment on egusphere-2022-446', Simone Papa, 14 Jul 2022
Review of “Shear zone evolution and the path of earthquake rupture” by Erik M. Young et al.
In this manuscript, Young et al. integrate field and microstructural mapping of a seismogenic fault core exhumed from the base of the seismogenic zone. They focus on the distribution of earthquake slip surfaces to understand what dictates the path of the earthquake rupture within a mylonitic shear zone. They conclude that stress heterogeneity at the scale of the lithologic layering is the most important factor controlling the path followed by the earthquake rupture.
The central question of the manuscript, i.e. what controls the path of earthquake rupture, is certainly an important one in earthquake mechanics and the methods used to address it are appropriate and with regard to the quantitative mapping of contact shapes (paragraph 4.2) are also novel. The manuscript is very well written and organised, the data presented are of good quality and substantially in agreement with the conclusion drawn by the authors, although I suggest more caution should be exercised in the interpretation and certain limitations should be discussed further. The new data and field observation, the quantitative analyses and related discussions certainly provide advances within the field and therefore I consider the manuscript fit for publication, provided that the following issues are addressed by the authors.
General comments
- The highlight of the paper is the detailed field mapping of an exceptional exposure and related analysis of which surfaces are preferentially exploited by pseudotachylytes (i.e. seismic ruptures). The authors show persuasive evidence that pseudotachylytes occur preferentially along pre-existent interfaces and in particular along interfaces with the highest viscosity rocks and viscosity contrast. They also show how pseudotachylyte-bearing interfaces are geometrically different from pseudotachylyte-absent interfaces. This last finding however is of difficult interpretation, since the present-day interface geometry is certainly not the same as it was at the time of pseudotachylyte emplacement. In chapter 5.2.3 the authors discuss this uncertainty and consider “the possibility that the observed pattern may be the result, rather than the cause, of seismic slip”. Furthermore, at line 485 and following, they also consider the possibility that “the enhanced long-wavelength roughness is caused by the pseudotachylyte itself … that interferes with the progression of boudinage along an interface”. In saying so, the authors acknowledge that boudinage may actually follow pseudotachylyte formation and not predate it. In the light of this, I do not see why the authors in their conclusion suggest that stress concentrations that dictate the path of seismic rupture are caused by pinch-and-swell geometries, although there is no clear evidence that pinch-and-swell geometries were present at the time of pseudotachylyte formation. In chapter 5.2.2 the authors argue that the patterns of pinch-and-swell layering imply an heterogeneous stress distribution, not that they cause it. The authors should clarify that the stress heterogeneities dictating rupture path are the result of the viscosity contrast across the interfaces and should be more cautious when interpreting pinch-and-swell geometries as the cause of stress heterogeneity. Or at least they should discuss this matter further, as they have done in chapter 5.2.3 for interface geometry.
- Several times throughout the paper, the authors refer to interfaces that juxtapose similar wall rocks (e.g. in Table 2 and at line 319). It is never explained what these contacts are and what they look like since they are not shown in any figure. The second part of table 2 seems to imply that pseudotachylyte segments with similar wall rocks are actually exploiting some kind of interfaces within these lithologies (e.g. foliation planes, c’ surfaces, fractures, joints ???). Otherwise I do not understand what the “total length of contact type” for similar wall rocks (sw) stands for and why you calculate what percentage of these contacts is decorated by pseudotachylytes. This is an important point to clarify because at present it is not clear if segments of pseudotachylytes with similar wall rocks are crosscutting intact rock (as stated at line 483) or are exploiting some pre-existent interface (as implied by table 2).
- The authors repeatedly state that the map is highly detailed and accurate to 1 cm. However, most of the layers in the map are much thicker than a few cm and not many centimetric layers are mapped. For example, are centimetric layers like those shown in Figs. 3b and 3e actually mapped?
Specific comments
Line 38 (e.g. Swanson, 1998 …)
Campbell et al. (Scottish Journal of Geology (2019) 55 (2): 75–92.) could be an appropriate paper to cite here as a field study that deals with relationship of seismic rupture with foliation and lithology in an amphibolitic shear zone.
Lines 71-72 “Both the pseudotachylyte and dynamic breccias have been shown to be mutually crosscutting with mylonitic foliations”
Is this true also for the outcrop studied in this paper? If so, it has an important bearing in your observations and discussions. Maybe an example could be shown in a figure.
Line 103 “1-50 cm-thick layers”
Throughout the paper inconsistent ranges of thickness for the layers are reported (e.g. 1-50 cm at line 103, 20-180 cm at line 111, 2-60 cm at line 411). Actually, the quartz mylonite layer in the right-hand-side of the map is more than 300 cm thick!
Line 113 “< 20 cm thick bands of nearly constant width”
Although commonly < 20 cm thick, black ultramylonite layers in the map are locally up to 50 cm thick. Also, I do not agree that they have constant width, to a visual approximation they seem to pinch and swell like the others.
Line 126
The term quartz mylonite has been extensively used in the literature to define mylonitic quartz veins or quartzite, mostly made of pure quartz (e.g. Mainprice and Casey, 1990, Geophys. J. Int.; Ralser, Hobbs and Ord, 1991, J. Struct. Geol.; Grujic, Stipp and Wooden, 2011, Geochem. Geophys. Geosystems.). To avoid confusion, I would suggest to use a different name, maybe quartz-rich mylonites?
Line 148
Porphyroclastic mylonite is referred to as “porphyritic” in figure 3b and caption.
Line 169 “only lithology observed cross-cutting foliation planes of other mylonites.”
This is an important observation, it would be nice to have a figure showing this in the paper.
Line 172-173 “… photomicrograph mosaics …”
I suggest to provide at least an example of the photomicrograph mosaics and the result of image analysis in the supplementary material.
Line 220
Characteristics 2 and 6 seem a bit contradictory (preserved flow banding (2) and absent compositional banding (6)).
Lines 243-244
7.75/11 and 2.5/11 instead of 7.75/10 and 2.5/10
Line 245 “coarsening of pseudotachylytes”
Do you mean coarsening of grain size of pseudotachylytes or coarsening of pseudotachylytes themselves?
Line 278 “< 1-13”
Actually locally they are at least 50 cm thick.
Line 280
The thickness of black ultramylonite layers is locally outstanding, making them very unlikely to represent the mylonitic deformation of a single pseudotachylyte. Probably, when a pseudotachylyte decorates an interface, this becomes a preferential rupture pathway for the next one. This is in agreement to your finding that interfaces with high viscosity contrast are preferentially exploited. Maybe you could discuss this further.
Line 303
The relative competence ranking is only qualitative and, although reasonable, seems a bit speculative. To improve the robustness of this chapter I would suggest to select figures showing key contact morphologies that you refer to in the text to justify the ranking.
Line 305
Better use “amplitude/wavelength” instead of “amplitude:wavelength”
Line 325-326 “as it makes cusps…Figure 3A”
To me it is not clear where you see this in figure 3A.
Lines 329-330
Although it is reasonable that the quartz mylonite is the weakest lithology, I wonder if you have an explanation for fig. 3D, that shows the quartz mylonite boudinaged within the granitic mylonite. Should this not mean that the quartz mylonite is more competent than the granitic mylonite?
Line 332
Can you explain why you selected these segments? Was it not possible to use all the interfaces mapped to have more robust results?
Line 338
What the PSD is should be explained somewhere in the text.
Line 338
“Figure 7c, e” instead of “Figure 7d, e”
Line 363
“Figure 7b, c” instead of “Figure 7d, e”
Line 403
“Fitz Gerald and Stünitz” instead of “Gerald and Stünitz”. Change also in the references.
Line 423-424 “the highest melting point … occurs in plagioclase”
Actually plagioclase has a lower melting point than quartz. Check Spray (2010).
Line 429 “high frictional heating (plagioclase)”
If by this you mean that plagioclase has the highest melting point, then it should be quartz instead.
Line 540 “pinch-swell geometries, which causes stress concentrations”
Are stress heterogeneities caused specifically by pinch-swell geometries, or are they inherent to the viscosity contrast between different layers?
Simone Papa
University of Padova
Citation: https://doi.org/10.5194/egusphere-2022-446-RC2 - AC2: 'Reply on RC2', Erik Young, 02 Sep 2022
Peer review completion
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Christie Rowe
James Kirkpatrick
The requested preprint has a corresponding peer-reviewed final revised paper. You are encouraged to refer to the final revised version.
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