diff --git a/src/pages/models/finch-2024-cprime/assets/.gitkeep b/src/pages/models/finch-2024-cprime/assets/.gitkeep new file mode 100644 index 0000000..8b13789 --- /dev/null +++ b/src/pages/models/finch-2024-cprime/assets/.gitkeep @@ -0,0 +1 @@ + diff --git a/src/pages/models/finch-2024-cprime/graphics/.gitkeep b/src/pages/models/finch-2024-cprime/graphics/.gitkeep new file mode 100644 index 0000000..d3f5a12 --- /dev/null +++ b/src/pages/models/finch-2024-cprime/graphics/.gitkeep @@ -0,0 +1 @@ + diff --git a/src/pages/models/finch-2024-cprime/graphics/Fig 3.png b/src/pages/models/finch-2024-cprime/graphics/Fig 3.png new file mode 100644 index 0000000..1bfb6f4 Binary files /dev/null and b/src/pages/models/finch-2024-cprime/graphics/Fig 3.png differ diff --git a/src/pages/models/finch-2024-cprime/graphics/Fig 5.png b/src/pages/models/finch-2024-cprime/graphics/Fig 5.png new file mode 100644 index 0000000..bb49ebd Binary files /dev/null and b/src/pages/models/finch-2024-cprime/graphics/Fig 5.png differ diff --git a/src/pages/models/finch-2024-cprime/graphics/Fig 2.png b/src/pages/models/finch-2024-cprime/graphics/Fig 2.png new file mode 100644 index 0000000..3588844 Binary files /dev/null and b/src/pages/models/finch-2024-cprime/graphics/Fig 2.png differ diff --git a/src/pages/models/finch-2024-cprime/index.md b/src/pages/models/finch-2024-cprime/index.md new file mode 100644 index 0000000..f241f8c --- /dev/null +++ b/src/pages/models/finch-2024-cprime/index.md @@ -0,0 +1,173 @@ +--- +templateKey: model +slug: finch-2024-cprime +title: 'The ephemeral development of C′ shear bands: A numerical modelling approach' +date: '2024-10-29T02:36:04.000Z' +featuredpost: +for_codes: + - 370401 +status: + - completed +doi: https://doi.org/10.25914/whbg-hd74 +url: https://mate.science//models/finch-2024-cprime +creditText: 'Finch, M., Bons, P.D.., Steinbach, F., Griera Artigas, A., Llorens, M., + Gomez-Rivas, E.., Ran, H.., & de Riese, T.. (2024). The ephemeral development of + C′ shear bands: A numerical modelling approach [Data set]. AuScope, National Computational + Infrastructure. https://doi.org/whbg-hd74' +software: + name: Elle Numerical Simulation Platform + doi: https://elle.ws/ + url_source: https://sourceforge.net/p/elle/git/ci/master/tree/ +licence: + licence_url: https://creativecommons.org/licenses/by/4.0/legalcode + licence_image: ../../../img/licence/by.png + description: Creative Commons Attribution 4.0 International + licence_file: license.txt +submitter: + name: Melanie + family_name: Finch + ORCID: https://orcid.org/0000-0001-9699-2769 +creators: + - name: Melanie + family_name: Finch + ORCID: 0000-0001-9699-2769 + - name: Paul D. + family_name: Bons + ORCID: 0000-0002-6469-3526 + - name: Florian + family_name: Steinbach + ORCID: Invalid ORCiD ID + - name: Albert + family_name: Griera Artigas + ORCID: 0000-0003-4598-8385 + - name: Maria-Gema + family_name: Llorens + ORCID: 0000-0002-6148-2600 + - name: Enrique + family_name: Gomez-Rivas + ORCID: 0000-0002-1317-6289 + - name: Hao + family_name: Ran + ORCID: 0000-0002-8639-3890 + - name: Tamara + family_name: de Riese + ORCID: 0000-0001-5828-8711 +associated_publication: + title: 'The ephemeral development of C′ shear bands: A numerical modelling approach' + url: http://dx.doi.org/10.1016/j.jsg.2020.104091 + doi: 10.1016/j.jsg.2020.104091 +compute_info: + name: '' + organisation: '' + url: '' + doi: '' +research_tags: [] +compute_tags: + - VPFFT + - Elle +funder: + - name: Alexander von Humboldt Foundation + doi: https://ror.org/012kf4317 + - name: Ministerio de Ciencia, Innovación y Universidades + doi: https://ror.org/05r0vyz12 +funding: + - name: Ministerio de Ciencia, Innovación y Universidades + doi: https://ror.org/05r0vyz12 + number_id: RYC2018-026335-I +abstract: '' +description: "This model simulates the development of C' shear bands in ductile shear + zones. The model begins with an equigranular texture of three phases: a strong phase + (e.g., feldspar) an intermediate-strength phase (e.g., quartz) and an anisotropic + weak phase (e.g., mica). Dextral shearing stretches and rotates the microstructure, + forming S-C fabric, asymmetric folds and C' shear bands." +images: + landing_image: + src: ./graphics/Fig 3.png + caption: 'Stages of microstructural development in a model with 15% weak phase + (black) and a medium phase strength contrast. (a) Starting microstructure, (b) + stage 1: grain elongation and rotation. Note the distribution of maximum strain + rate (red arrows) localised to tips of WP grains that are parallel to the C + plane, (c) stage 2: S-C fabric development. Stress is highest in the IP+SP adjacent + to high strain rate layers of interconnected WP (red and orange arrows). (d) + stage 3: shear band development and strain partitioning. Maximum stress in the + model is in the gap in the shear band (red arrow). Green arrows highlight areas + that have been asymmetrically folded (c.f. Fig. 1a). The first column shows + the grain microstructure, the second column shows the normalised von Mises strain + rate and the third column shows the von Mises stress. Images in the same row + correspond to the same model and step.' + graphic_abstract: + src: ./graphics/Fig 5.png + caption: The formation of C' shear bands by the rotation of a C plane forwards + due to high strain rate in the shear band and high stress at the tip of the + shear band. (a) Discontinuous shear band with section parallel to the SZB at + high strain rate (red arrow) and high stress in the IP+SP region at the end + of the shear band (orange arrow). (b) A low strain rate section in the shear + band is bracketed on either side by high strain rate sections (red arrows) and + begins to rotate forwards. (c) C' shear band forms in low strain rate section + (red dashed line). (d) Strain rate reduces in the shear band and the C' shear + band has rotated back into parallelism with the SZB and C planes. The first + column shows the grain microstructure, the second column shows the normalised + von Mises strain rate and the third column shows the von Mises stress. Model + shown contains 15% weak phase and a high phase strength contrast. Images in + the same row correspond to the same model and step. + model_setup: + src: ./graphics/Fig 2.png + caption: 'Basic process of microstructure simulation. (a) The starting microstructure + consists of three grain types that undergo one increment of γ = 0.02 dextral + shear. (b) The microstructure is deformed with wrapping boundaries. (c) The + microstructure is repositioned back to a square before the next increment of + strain. (d) Zoom in of (a) showing the three flynn (grain) types: strong phase + (SP), intermediate-strength phase (IP), and weak phase (WP). (e) Zoom-in of + (d) showing that flynn grain boundaries are defined by double (blue) and triple + (red) bnodes joined by straight lines. An additional grid of unconnected nodes + (unodes, black) is overlain on flynns and stores state variables and flynn properties.' +animation: + src: ./graphics/ + caption: '' +model_setup_info: + url: '' + summary: "A three-phase microstructure was used with 15% weak phase (WP), 42.5% + intermediate-strength phase (IP) and 42.5% strong phase (SP). The starting model + was square and defined by 2,748 equant grains with a random distribution of the + three phases. Velocity boundary conditions with constant strain rate were applied + with top-to-the-right (dextral) simple shear in increments of Δγ = 0.02, up to + a finite shear strain of γ=18 in 900 steps. After each deformation step, the model + was repositioned to the initial square unit cell and grain properties mapped back + on to the grid before the next deformation step. A power-law viscous rheology\ + \ was employed with n = 3.\r\nEach phase was associated with a mineral model + that specified the slip systems and their effective strength or resistance to + shear. The mineral models employed attempted to broadly approximate the most important + features of mica (WP), quartz (IP), and feldspar (SP) in order to more closely + correspond to previous experimental work. To model the WP we used a mineral model + with hexagonal symmetry and three slip systems (basal, prismatic, and pyramidal) + because, although mica is monoclinic, it is pseudohexagonal and its most important + mechanical feature is an easy glide plane since shear in mica is easier parallel + to the basal plane than in any other direction. Accordingly we set the basal + plane of the WP to one tenth of the non-basal WP planes, producing a mechanically + anisotropic WP. Feldspar is also pseudohexagonal, so we employed a hexagonal mineral + model for the SP, but with all slip systems at the same effective strength. For + the IP we used the crystal model of quartz with four slip systems (basal, prismatic, + pyramidal and pyramidal ) and gave the effective strength of all four + slip systems the same value, making the IP effectively mechanically isotropic. + The IP was 25x stronger than the WP basal plane and the SP was 2x stronger than + the IP." +model_files: + url: '' + notes: The starting microstructure for the model is an .Elle file that can be viewed + and edited in notepad or similar. The microstructure can be viewed with the showelle + program. To run the simulation the program Elle can be downloaded from elle.ws. + file_tree: '' + existing_identifier: '' + nci_file_path: + https://thredds.nci.org.au/thredds/catalog/nm08/MATE/finch-2024-cprime/catalog.html + include: true +dataset: + url: '' + notes: Output data consists of 900 files that are 21 Mb each and an avi movie that + is 80 Mb + existing_identifier: '' + nci_file_path: + https://thredds.nci.org.au/thredds/catalog/nm08/MATE/finch-2024-cprime/catalog.html + include: true +metadataFile: ro-crate-metadata.json +--- diff --git a/src/pages/models/finch-2024-cprime/license.txt b/src/pages/models/finch-2024-cprime/license.txt new file mode 100644 index 0000000..da6ab6c --- /dev/null +++ b/src/pages/models/finch-2024-cprime/license.txt @@ -0,0 +1,396 @@ +Attribution 4.0 International + +======================================================================= + +Creative Commons Corporation ("Creative Commons") is not a law firm and +does not provide legal services or legal advice. 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For +the avoidance of doubt, this paragraph does not form part of the +public licenses. + +Creative Commons may be contacted at creativecommons.org. + diff --git a/src/pages/models/finch-2024-cprime/ro-crate-metadata.json b/src/pages/models/finch-2024-cprime/ro-crate-metadata.json new file mode 100644 index 0000000..dc1255f --- /dev/null +++ b/src/pages/models/finch-2024-cprime/ro-crate-metadata.json @@ -0,0 +1,550 @@ +{ + "@context": [ + "https://www.researchobject.org/ro-crate/1.1/context.jsonld", + "https://raw.githubusercontent.com/codemeta/codemeta/master/codemeta.jsonld" + ], + "@graph": [ + { + "@id": "#datasetCreation", + "@type": "CreateAction", + "agent": [ + { + "@id": "https://orcid.org/0000-0001-9699-2769" + }, + { + "@id": "https://orcid.org/0000-0002-6469-3526" + }, + { + "@id": "_:b7" + }, + { + "@id": "https://orcid.org/0000-0003-4598-8385" + }, + { + "@id": "https://orcid.org/0000-0002-6148-2600" + }, + { + "@id": "https://orcid.org/0000-0002-1317-6289" + }, + { + "@id": "https://orcid.org/0000-0002-8639-3890" + }, + { + "@id": "https://orcid.org/0000-0001-5828-8711" + } + ], + "description": "Running the computational model", + "endTime": "", + "instrument": { + "@id": "https://elle.ws/" + }, + "object": { + "@id": "model_code_inputs" + }, + "result": { + "@id": "model_output_data" + }, + "startTime": "" + }, + { + "@id": "./", + "@type": "Dataset", + "about": { + "@id": "https://linked.data.gov.au/def/anzsrc-for/2020/370401" + }, + "abstract": "", + "alternateName": "finch-2024-cprime", + "citation": { + "@id": "http://dx.doi.org/10.1016/j.jsg.2020.104091" + }, + "contributor": "", + "creativeWorkStatus": "completed", + "creator": [ + { + "@id": "https://orcid.org/0000-0001-9699-2769" + }, + { + "@id": "https://orcid.org/0000-0002-6469-3526" + }, + { + "@id": "_:b4" + }, + { + "@id": "https://orcid.org/0000-0003-4598-8385" + }, + { + "@id": "https://orcid.org/0000-0002-6148-2600" + }, + { + "@id": "https://orcid.org/0000-0002-1317-6289" + }, + { + "@id": "https://orcid.org/0000-0002-8639-3890" + }, + { + "@id": "https://orcid.org/0000-0001-5828-8711" + } + ], + "datePublished": "2024-10-29T02:36:04.000Z", + "description": "This model simulates the development of C' shear bands in ductile shear zones. The model begins with an equigranular texture of three phases: a strong phase (e.g., feldspar) an intermediate-strength phase (e.g., quartz) and an anisotropic weak phase (e.g., mica). 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