{"data":{"id":"10.6084/m9.figshare.8178857","type":"dois","attributes":{"doi":"10.6084/m9.figshare.8178857","prefix":"10.6084","suffix":"m9.figshare.8178857","identifiers":[{"identifier":"https://doi.org/10.6084/m9.figshare.8178857","identifierType":"DOI"}],"alternateIdentifiers":[{"alternateIdentifierType":"DOI","alternateIdentifier":"https://doi.org/10.6084/m9.figshare.8178857"}],"creators":[{"name":"Taylor, Stephanie","nameType":"Personal","givenName":"Stephanie","familyName":"Taylor","affiliation":[],"nameIdentifiers":[]},{"name":"Brodsky, Emily","nameType":"Personal","givenName":"Emily","familyName":"Brodsky","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-6855-6860","nameIdentifierScheme":"ORCID"}]}],"titles":[{"title":"TaylorBrodsky_JGR2019_MineralSandShearFlows.mat"}],"publisher":"Figshare","container":{},"publicationYear":2019,"subjects":[{"subject":"40607 Surface Processes","subjectScheme":"FOR"},{"subject":"FOS: Earth and related environmental sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"50305 Soil Physics","subjectScheme":"FOR"},{"subject":"FOS: Agriculture, forestry and fisheries","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Geophysics"},{"subject":"40601 Geomorphology and Regolith and Landscape Evolution","subjectScheme":"FOR"},{"subject":"20301 Acoustics and Acoustical Devices; Waves","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"20405 Soft Condensed Matter","subjectScheme":"FOR"}],"contributors":[],"dates":[{"date":"2019-05-23","dateType":"Created"},{"date":"2019-05-23","dateType":"Updated"},{"date":"2019","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[],"relatedItems":[],"sizes":["4695486 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"CC BY 4.0","rightsUri":"https://creativecommons.org/licenses/by/4.0"}],"descriptions":[{"description":"This data set was collected from experiments shearing sands of different mineralogies under constant axial force and observing changes in sample height and acoustic energy as shear velocity was increased. Results published in Taylor \u0026amp; Brodsky, JGR-Solid Earth, 2019. Each matlab structure represents one mineral tested, identified by the variable title. Each structure contains the same fields, outlined below:\n\u003cbr\u003e\nrho: grain density measured in lab (kg/m^3)\n\u003cbr\u003e\nd50: median grain diameter of sample (m)\n\u003cbr\u003e\ndmax: maximum grain diameter of sample (m)\n\u003cbr\u003e\nmgr: median grain mass, calculated from rho and d50 (kg)\n\u003cbr\u003e\nNgrains: circumference of sample cylinder divided by median grain diameter\n\u003cbr\u003e\nrheomALL: full data set from experiment including conditioning runs. Each entry represents one step in the experiment, with length sending on step type. columns are the same for each step and are outlined below:\n\ncol1: Step time (s)\ncol2: Axial force (N)\ncol3: Sample height (µm)  (relative within each experiment)\ncol4: Angular Rotor Velocity (rad/s)\ncol5: Torque (µN m)\ncol6: Total time (s)\ncol7: Angular displacement (rad)\n\n**The following data entries were not calibrated in the instrument for all experiments and should be ignored or calculated separately from columns 1-7**\n\ncol8: Normal stress (Pa) \ncol9: Shear rate (1/s) \ncol10: Shear stress (Pa)\ncol11: Temperature (degrees C)\ncol12: Viscosity (Pa s)\n\n\u003cbr\u003e\nAE: 10Hz acoustic energy for last 30 seconds of each steady state velocity step evaluated\n\u003cbr\u003e\nrheom: a subset of rheomALL, showing data from 60 s steady state experiment steps only- these were evaluated for paper\n\nrawgap: sample height (uncalibrated) (µm) \nI: inertial number - calculated from rho, d50, Axial Force, Angular Rotor Velocity and a 5 grain diameter deep shear zone\n\n\u003cbr\u003e\nAEmean: 1 Hz running average of acoustic energy in the final 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\nAEerr: L1 norm of 1 Hz running average of acoustic energy in the final 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\ngapmeanRAW: average of (uncalibrated) sample height in the final 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\ngapstd: standard deviation of sample height measurements in the final 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\nImean: average inertial number in the final 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\nIstd: standard deviation of inertial number for the last 15 seconds of each 60 s steady state velocity step\n\u003cbr\u003e\nAEMassNorm: average acoustic energy (AEmean) divided by median grain mass (mgr) to give V^2 per grain for final 15 s of each 60 s steady state velocity step\n\u003cbr\u003e\nAEMassNormErr: L1 norm of acoustic energy divided by median grain mass for final 15 s of each 60 s steady state velocity step\n\u003cbr\u003e\n\u003cbr\u003e\n\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"<?xml version="1.0" encoding="UTF-8"?>
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  <identifier identifierType="DOI">10.6084/M9.FIGSHARE.8178857</identifier>
  <creators>
    <creator>
      <creatorName>Stephanie Taylor</creatorName>
    </creator>
    <creator>
      <creatorName>Emily Brodsky</creatorName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org">0000-0002-6855-6860</nameIdentifier>
    </creator>
  </creators>
  <titles>
    <title>TaylorBrodsky_JGR2019_MineralSandShearFlows.mat</title>
  </titles>
  <descriptions>
    <description descriptionType="Abstract">&lt;p&gt;This data set was collected from experiments shearing sands of different mineralogies under constant axial force and observing changes in sample height and acoustic energy as shear velocity was increased. Results published in Taylor &amp; Brodsky, JGR-Solid Earth, 2019. Each matlab structure represents one mineral tested, identified by the variable title. Each structure contains the same fields, outlined below:&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;rho: grain density measured in lab (kg/m^3)&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;d50: median grain diameter of sample (m)&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;dmax: maximum grain diameter of sample (m)&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;mgr: median grain mass, calculated from rho and d50 (kg)&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;Ngrains: circumference of sample cylinder divided by median grain diameter&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;rheomALL: full data set from experiment including conditioning runs. Each entry represents one step in the experiment, with length sending on step type. columns are the same for each step and are outlined below:&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;col1: Step time (s)&lt;/li&gt;
&lt;li&gt;col2: Axial force (N)&lt;/li&gt;
&lt;li&gt;col3: Sample height (µm)  (relative within each experiment)&lt;/li&gt;
&lt;li&gt;col4: Angular Rotor Velocity (rad/s)&lt;/li&gt;
&lt;li&gt;col5: Torque (µN m)&lt;/li&gt;
&lt;li&gt;col6: Total time (s)&lt;/li&gt;
&lt;li&gt;col7: Angular displacement (rad)&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;**The following data entries were not calibrated in the instrument for all experiments and should be ignored or calculated separately from columns 1-7**&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;col8: Normal stress (Pa) &lt;/li&gt;
&lt;li&gt;col9: Shear rate (1/s) &lt;/li&gt;
&lt;li&gt;col10: Shear stress (Pa)&lt;/li&gt;
&lt;li&gt;col11: Temperature (degrees C)&lt;/li&gt;
&lt;li&gt;col12: Viscosity (Pa s)&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;AE: 10Hz acoustic energy for last 30 seconds of each steady state velocity step evaluated&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;rheom: a subset of rheomALL, showing data from 60 s steady state experiment steps only- these were evaluated for paper&lt;/p&gt;
&lt;ul&gt;
&lt;li&gt;rawgap: sample height (uncalibrated) (µm) &lt;/li&gt;
&lt;li&gt;I: inertial number - calculated from rho, d50, Axial Force, Angular Rotor Velocity and a 5 grain diameter deep shear zone&lt;/li&gt;
&lt;/ul&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;AEmean: 1 Hz running average of acoustic energy in the final 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;AEerr: L1 norm of 1 Hz running average of acoustic energy in the final 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;gapmeanRAW: average of (uncalibrated) sample height in the final 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;gapstd: standard deviation of sample height measurements in the final 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;Imean: average inertial number in the final 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;Istd: standard deviation of inertial number for the last 15 seconds of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;AEMassNorm: average acoustic energy (AEmean) divided by median grain mass (mgr) to give V^2 per grain for final 15 s of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;AEMassNormErr: L1 norm of acoustic energy divided by median grain mass for final 15 s of each 60 s steady state velocity step&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;
&lt;p&gt;&lt;br&gt;&lt;/p&gt;</description>
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    <subject schemeURI="http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E" subjectScheme="FOR">40607 Surface Processes</subject>
    <subject schemeURI="http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E" subjectScheme="FOR">50305 Soil Physics</subject>
    <subject>Geophysics</subject>
    <subject schemeURI="http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E" subjectScheme="FOR">40601 Geomorphology and Regolith and Landscape Evolution</subject>
    <subject schemeURI="http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E" subjectScheme="FOR">20301 Acoustics and Acoustical Devices; Waves</subject>
    <subject schemeURI="http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E" subjectScheme="FOR">20405 Soft Condensed Matter</subject>
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  <publisher>Figshare</publisher>
  <publicationYear>2019</publicationYear>
  <dates>
    <date dateType="Created">2019-05-23</date>
    <date dateType="Updated">2019-05-23</date>
  </dates>
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    <rights rightsURI="https://creativecommons.org/licenses/by/4.0/">CC BY 4.0</rights>
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