Third‐Order Padé Thermoelastic Constants of Solid Rocks
Classical third‐order thermoelastic constants are generally derived from the theory of small‐amplitude acoustic waves in isotropic materials during heat treatments. Investigating higher‐order thermoelastic constants for higher temperatures is challenging owing to the involvement of the number of unk...
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description | Classical third‐order thermoelastic constants are generally derived from the theory of small‐amplitude acoustic waves in isotropic materials during heat treatments. Investigating higher‐order thermoelastic constants for higher temperatures is challenging owing to the involvement of the number of unknown parameters. These Taylor‐type thermoelastic constants from the classical thermoelasticity theory are formulated based on the Taylor series of the Helmholtz free energy density for preheated crystals. However, these Taylor‐type thermoelastic models are limited even at low temperatures in characterizing the temperature‐dependent velocities of elastic waves in solid rocks as a polycrystal compound of different mineral lithologies. Thus, we propose using the Padé rational function to the total thermal strain energy function. The resulting Padé thermoelastic model gives a reasonable theoretical prediction for acoustic velocities of solid rocks at a higher temperature. We formulate the relationship between the third‐order Padé thermoelastic constants and the corresponding higher‐order Taylor thermoelastic constants with the same accuracy. Two additional Padé coefficients α1 ${\mathit{\alpha }}_{1}$ and α2 ${\mathit{\alpha }}_{2}$ can be calculated using the second‐, third‐, and fourth‐order Taylor thermoelastic constants associated with the Brugger's constants, which are consistent with those obtained by fitting the experimental data of polycrystalline material. The third‐order Padé thermoelastic model (with four constants) is validated by the fourth‐order Taylor thermoelastic prediction (with six constants) with ultrasonic measurements for polycrystals (olivine samples) and solid rocks (sandstone, granite, and shale). The results demonstrate that the third‐order Padé thermoelastic model can characterize thermally induced velocity changes more accurately than the conventional third‐order Taylor thermoelastic prediction (with four constants), especially for solid rocks at high temperatures. The Padé approximation could be considered a more accurate and universal model in describing thermally induced velocity changes for polycrystals and solid rocks.
Plain Language Summary
Using the Taylor series for thermoelastic constants at higher temperatures is challenging owing to the involvement of the number of unknown parameters. Thus, we propose the third‐order Padé approximation to replace the Taylor series. Applications to laboratory measurements show that, with much le |
doi_str_mv | 10.1029/2022JB024517 |
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Plain Language Summary
Using the Taylor series for thermoelastic constants at higher temperatures is challenging owing to the involvement of the number of unknown parameters. Thus, we propose the third‐order Padé approximation to replace the Taylor series. Applications to laboratory measurements show that, with much less complexity, the Padé approximation presents a tendency of higher accuracy than the third‐order Taylor series and has similar precision with the higher‐order Taylor series at higher temperatures (up to 1500 K for polycrystals and 1000°C for solid rocks). Then we use such a model to predict the temperature‐dependent velocities of elastic waves. Finally, we analyze the physics of two additional Padé coefficients by associating them with the thermal expansion mismatch due to rock heterogeneities in lithology and with the thermally induced deformation of microcracks.
Key Points
We apply the Padé rational function to the total thermal strain energy function
We correlate the Padé and higher‐order Taylor thermoelastic constants through the equivalency of approximation accuracies
The physics of the Padé coefficients is relevant to the thermal expansion mismatch and thermally induced deformation of microcracks</description><identifier>ISSN: 2169-9313</identifier><identifier>EISSN: 2169-9356</identifier><identifier>DOI: 10.1029/2022JB024517</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Accuracy ; Acoustic waves ; Approximation ; Coefficients ; Constants ; Crystals ; Deformation ; Elastic waves ; Free energy ; Geophysics ; Heat treatment ; Heat treatments ; High temperature ; Isotropic material ; Isotropic materials ; Lithology ; Low temperature ; Mathematical models ; Microcracks ; Modelling ; Olivine ; Pade approximation ; Parameters ; Physics ; Polycrystals ; Predictions ; Rational functions ; Rocks ; Sandstone ; Sedimentary rocks ; Shale ; Sound waves ; Taylor series ; Temperature ; Temperature dependence ; Thermal expansion ; Thermal strain ; Thermoelasticity ; Ultrasonic methods ; Velocity</subject><ispartof>Journal of geophysical research. Solid earth, 2022-09, Vol.127 (9), p.n/a</ispartof><rights>2022. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a2602-859e3a7818c2ee044115aa149c43f3dbed6a9a122a45e9edb387040e625a46ad3</citedby><cites>FETCH-LOGICAL-a2602-859e3a7818c2ee044115aa149c43f3dbed6a9a122a45e9edb387040e625a46ad3</cites><orcidid>0000-0002-7672-7949 ; 0000-0003-1265-7029 ; 0000-0002-1964-7854 ; 0000-0001-8692-8405 ; 0000-0003-1009-3629</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2022JB024517$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2022JB024517$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,1433,27924,27925,45574,45575,46409,46833</link.rule.ids></links><search><creatorcontrib>Yang, Jian</creatorcontrib><creatorcontrib>Fu, Li‐Yun</creatorcontrib><creatorcontrib>Fu, Bo‐Ye</creatorcontrib><creatorcontrib>Deng, Wubing</creatorcontrib><creatorcontrib>Han, Tongcheng</creatorcontrib><title>Third‐Order Padé Thermoelastic Constants of Solid Rocks</title><title>Journal of geophysical research. Solid earth</title><description>Classical third‐order thermoelastic constants are generally derived from the theory of small‐amplitude acoustic waves in isotropic materials during heat treatments. Investigating higher‐order thermoelastic constants for higher temperatures is challenging owing to the involvement of the number of unknown parameters. These Taylor‐type thermoelastic constants from the classical thermoelasticity theory are formulated based on the Taylor series of the Helmholtz free energy density for preheated crystals. However, these Taylor‐type thermoelastic models are limited even at low temperatures in characterizing the temperature‐dependent velocities of elastic waves in solid rocks as a polycrystal compound of different mineral lithologies. Thus, we propose using the Padé rational function to the total thermal strain energy function. The resulting Padé thermoelastic model gives a reasonable theoretical prediction for acoustic velocities of solid rocks at a higher temperature. We formulate the relationship between the third‐order Padé thermoelastic constants and the corresponding higher‐order Taylor thermoelastic constants with the same accuracy. Two additional Padé coefficients α1 ${\mathit{\alpha }}_{1}$ and α2 ${\mathit{\alpha }}_{2}$ can be calculated using the second‐, third‐, and fourth‐order Taylor thermoelastic constants associated with the Brugger's constants, which are consistent with those obtained by fitting the experimental data of polycrystalline material. The third‐order Padé thermoelastic model (with four constants) is validated by the fourth‐order Taylor thermoelastic prediction (with six constants) with ultrasonic measurements for polycrystals (olivine samples) and solid rocks (sandstone, granite, and shale). The results demonstrate that the third‐order Padé thermoelastic model can characterize thermally induced velocity changes more accurately than the conventional third‐order Taylor thermoelastic prediction (with four constants), especially for solid rocks at high temperatures. The Padé approximation could be considered a more accurate and universal model in describing thermally induced velocity changes for polycrystals and solid rocks.
Plain Language Summary
Using the Taylor series for thermoelastic constants at higher temperatures is challenging owing to the involvement of the number of unknown parameters. Thus, we propose the third‐order Padé approximation to replace the Taylor series. Applications to laboratory measurements show that, with much less complexity, the Padé approximation presents a tendency of higher accuracy than the third‐order Taylor series and has similar precision with the higher‐order Taylor series at higher temperatures (up to 1500 K for polycrystals and 1000°C for solid rocks). Then we use such a model to predict the temperature‐dependent velocities of elastic waves. Finally, we analyze the physics of two additional Padé coefficients by associating them with the thermal expansion mismatch due to rock heterogeneities in lithology and with the thermally induced deformation of microcracks.
Key Points
We apply the Padé rational function to the total thermal strain energy function
We correlate the Padé and higher‐order Taylor thermoelastic constants through the equivalency of approximation accuracies
The physics of the Padé coefficients is relevant to the thermal expansion mismatch and thermally induced deformation of microcracks</description><subject>Accuracy</subject><subject>Acoustic waves</subject><subject>Approximation</subject><subject>Coefficients</subject><subject>Constants</subject><subject>Crystals</subject><subject>Deformation</subject><subject>Elastic waves</subject><subject>Free energy</subject><subject>Geophysics</subject><subject>Heat treatment</subject><subject>Heat treatments</subject><subject>High temperature</subject><subject>Isotropic material</subject><subject>Isotropic materials</subject><subject>Lithology</subject><subject>Low temperature</subject><subject>Mathematical models</subject><subject>Microcracks</subject><subject>Modelling</subject><subject>Olivine</subject><subject>Pade approximation</subject><subject>Parameters</subject><subject>Physics</subject><subject>Polycrystals</subject><subject>Predictions</subject><subject>Rational functions</subject><subject>Rocks</subject><subject>Sandstone</subject><subject>Sedimentary rocks</subject><subject>Shale</subject><subject>Sound waves</subject><subject>Taylor series</subject><subject>Temperature</subject><subject>Temperature dependence</subject><subject>Thermal expansion</subject><subject>Thermal strain</subject><subject>Thermoelasticity</subject><subject>Ultrasonic methods</subject><subject>Velocity</subject><issn>2169-9313</issn><issn>2169-9356</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp90M1KAzEQB_AgCpbqzQdY8OpqMvnYxJstWi2FSq3nZbrJ0q3bpiZbpDcfwdfwOXwTn8SVinhyLjMMP2bgT8gJo-eMgrkACjDsURCSZXukA0yZ1HCp9n9nxg_JcYwL2pZuV0x0yOV0XgX7-fo2DtaF5B7tx3synbuw9K7G2FRF0ver2OCqiYkvkwdfVzaZ-OIpHpGDEuvojn96lzzeXE_7t-loPLjrX41SBEUh1dI4jplmugDnqBCMSUQmTCF4ye3MWYUGGQAK6YyzM64zKqhTIFEotLxLTnd318E_b1xs8oXfhFX7MoeMaaUkFdCqs50qgo8xuDJfh2qJYZszmn8HlP8NqOV8x1-q2m3_tflwMOlJqSXwL2XIZik</recordid><startdate>202209</startdate><enddate>202209</enddate><creator>Yang, Jian</creator><creator>Fu, Li‐Yun</creator><creator>Fu, Bo‐Ye</creator><creator>Deng, Wubing</creator><creator>Han, Tongcheng</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7ST</scope><scope>7TG</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>FR3</scope><scope>H8D</scope><scope>H96</scope><scope>KL.</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope><scope>SOI</scope><orcidid>https://orcid.org/0000-0002-7672-7949</orcidid><orcidid>https://orcid.org/0000-0003-1265-7029</orcidid><orcidid>https://orcid.org/0000-0002-1964-7854</orcidid><orcidid>https://orcid.org/0000-0001-8692-8405</orcidid><orcidid>https://orcid.org/0000-0003-1009-3629</orcidid></search><sort><creationdate>202209</creationdate><title>Third‐Order Padé Thermoelastic Constants of Solid Rocks</title><author>Yang, Jian ; Fu, Li‐Yun ; Fu, Bo‐Ye ; Deng, Wubing ; Han, Tongcheng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a2602-859e3a7818c2ee044115aa149c43f3dbed6a9a122a45e9edb387040e625a46ad3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Accuracy</topic><topic>Acoustic waves</topic><topic>Approximation</topic><topic>Coefficients</topic><topic>Constants</topic><topic>Crystals</topic><topic>Deformation</topic><topic>Elastic waves</topic><topic>Free energy</topic><topic>Geophysics</topic><topic>Heat treatment</topic><topic>Heat treatments</topic><topic>High temperature</topic><topic>Isotropic material</topic><topic>Isotropic materials</topic><topic>Lithology</topic><topic>Low temperature</topic><topic>Mathematical models</topic><topic>Microcracks</topic><topic>Modelling</topic><topic>Olivine</topic><topic>Pade approximation</topic><topic>Parameters</topic><topic>Physics</topic><topic>Polycrystals</topic><topic>Predictions</topic><topic>Rational functions</topic><topic>Rocks</topic><topic>Sandstone</topic><topic>Sedimentary rocks</topic><topic>Shale</topic><topic>Sound waves</topic><topic>Taylor series</topic><topic>Temperature</topic><topic>Temperature dependence</topic><topic>Thermal expansion</topic><topic>Thermal strain</topic><topic>Thermoelasticity</topic><topic>Ultrasonic methods</topic><topic>Velocity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yang, Jian</creatorcontrib><creatorcontrib>Fu, Li‐Yun</creatorcontrib><creatorcontrib>Fu, Bo‐Ye</creatorcontrib><creatorcontrib>Deng, Wubing</creatorcontrib><creatorcontrib>Han, Tongcheng</creatorcontrib><collection>CrossRef</collection><collection>Environment Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Environment Abstracts</collection><jtitle>Journal of geophysical research. Solid earth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yang, Jian</au><au>Fu, Li‐Yun</au><au>Fu, Bo‐Ye</au><au>Deng, Wubing</au><au>Han, Tongcheng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Third‐Order Padé Thermoelastic Constants of Solid Rocks</atitle><jtitle>Journal of geophysical research. Solid earth</jtitle><date>2022-09</date><risdate>2022</risdate><volume>127</volume><issue>9</issue><epage>n/a</epage><issn>2169-9313</issn><eissn>2169-9356</eissn><abstract>Classical third‐order thermoelastic constants are generally derived from the theory of small‐amplitude acoustic waves in isotropic materials during heat treatments. Investigating higher‐order thermoelastic constants for higher temperatures is challenging owing to the involvement of the number of unknown parameters. These Taylor‐type thermoelastic constants from the classical thermoelasticity theory are formulated based on the Taylor series of the Helmholtz free energy density for preheated crystals. However, these Taylor‐type thermoelastic models are limited even at low temperatures in characterizing the temperature‐dependent velocities of elastic waves in solid rocks as a polycrystal compound of different mineral lithologies. Thus, we propose using the Padé rational function to the total thermal strain energy function. The resulting Padé thermoelastic model gives a reasonable theoretical prediction for acoustic velocities of solid rocks at a higher temperature. We formulate the relationship between the third‐order Padé thermoelastic constants and the corresponding higher‐order Taylor thermoelastic constants with the same accuracy. Two additional Padé coefficients α1 ${\mathit{\alpha }}_{1}$ and α2 ${\mathit{\alpha }}_{2}$ can be calculated using the second‐, third‐, and fourth‐order Taylor thermoelastic constants associated with the Brugger's constants, which are consistent with those obtained by fitting the experimental data of polycrystalline material. The third‐order Padé thermoelastic model (with four constants) is validated by the fourth‐order Taylor thermoelastic prediction (with six constants) with ultrasonic measurements for polycrystals (olivine samples) and solid rocks (sandstone, granite, and shale). The results demonstrate that the third‐order Padé thermoelastic model can characterize thermally induced velocity changes more accurately than the conventional third‐order Taylor thermoelastic prediction (with four constants), especially for solid rocks at high temperatures. The Padé approximation could be considered a more accurate and universal model in describing thermally induced velocity changes for polycrystals and solid rocks.
Plain Language Summary
Using the Taylor series for thermoelastic constants at higher temperatures is challenging owing to the involvement of the number of unknown parameters. Thus, we propose the third‐order Padé approximation to replace the Taylor series. Applications to laboratory measurements show that, with much less complexity, the Padé approximation presents a tendency of higher accuracy than the third‐order Taylor series and has similar precision with the higher‐order Taylor series at higher temperatures (up to 1500 K for polycrystals and 1000°C for solid rocks). Then we use such a model to predict the temperature‐dependent velocities of elastic waves. Finally, we analyze the physics of two additional Padé coefficients by associating them with the thermal expansion mismatch due to rock heterogeneities in lithology and with the thermally induced deformation of microcracks.
Key Points
We apply the Padé rational function to the total thermal strain energy function
We correlate the Padé and higher‐order Taylor thermoelastic constants through the equivalency of approximation accuracies
The physics of the Padé coefficients is relevant to the thermal expansion mismatch and thermally induced deformation of microcracks</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2022JB024517</doi><tpages>30</tpages><orcidid>https://orcid.org/0000-0002-7672-7949</orcidid><orcidid>https://orcid.org/0000-0003-1265-7029</orcidid><orcidid>https://orcid.org/0000-0002-1964-7854</orcidid><orcidid>https://orcid.org/0000-0001-8692-8405</orcidid><orcidid>https://orcid.org/0000-0003-1009-3629</orcidid></addata></record> |
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subjects | Accuracy Acoustic waves Approximation Coefficients Constants Crystals Deformation Elastic waves Free energy Geophysics Heat treatment Heat treatments High temperature Isotropic material Isotropic materials Lithology Low temperature Mathematical models Microcracks Modelling Olivine Pade approximation Parameters Physics Polycrystals Predictions Rational functions Rocks Sandstone Sedimentary rocks Shale Sound waves Taylor series Temperature Temperature dependence Thermal expansion Thermal strain Thermoelasticity Ultrasonic methods Velocity |
title | Third‐Order Padé Thermoelastic Constants of Solid Rocks |
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