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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Veröffentlicht in:Journal of geophysical research. Solid earth 2022-09, Vol.127 (9), p.n/a
Hauptverfasser: Yang, Jian, Fu, Li‐Yun, Fu, Bo‐Ye, Deng, Wubing, Han, Tongcheng
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creator Yang, Jian
Fu, Li‐Yun
Fu, Bo‐Ye
Deng, Wubing
Han, Tongcheng
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
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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><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 ; 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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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