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Modeling of viscoelastic properties of nonpermeable porous rocks saturated with highly viscous fluid at seismic frequencies at the core scale
A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. Based on this modeling method, we...
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Published in: | Journal of geophysical research. Solid earth 2017-08, Vol.122 (8), p.6067-6086 |
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description | A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. Based on this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the storage moduli and the stress‐strain phase lag of saturated rocks. And we also compared the modeling results to the Hashin‐Shtrikman bounds and the coherent potential approximation (CPA). The dynamic moduli calculated from the modeling are lower than the predictions of CPA, and both of these fall between the Hashin‐Shtrikman bounds. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and aspect ratio affect the rock frame stiffness and result in different viscoelastic behaviors of the saturated rocks. The stress‐strain phase lags are larger with smaller stiffness contrasts between the rock frame and the pore fluid. The viscoelastic properties of saturated rocks are more sensitive to aspect ratio compared to other pore structure parameters. The results suggest that significant seismic dispersion (at about 50–200 Hz) might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids.
Plain Language Summary
We develop a core scale modeling method to simulate the viscoelastic properties of rocks saturated with viscous fluid at low frequencies based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. By using this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the composite's viscoelastic properties. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and pore aspect ratio affect the rock frame stiffness and result in different viscoelastic behavior of t |
doi_str_mv | 10.1002/2017JB013979 |
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Plain Language Summary
We develop a core scale modeling method to simulate the viscoelastic properties of rocks saturated with viscous fluid at low frequencies based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. By using this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the composite's viscoelastic properties. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and pore aspect ratio affect the rock frame stiffness and result in different viscoelastic behavior of the saturated rocks. The lower the rock frame stiffness, the larger the stress‐strain phase lags. The viscoelastic properties of saturated rocks are more sensitive to the pore aspect ratio. The results suggest that significant seismic dispersion might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids. This will be important in the context of heavy hydrocarbon reservoirs and igneous rocks saturated with silicate melt.
Key Points
A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed
We observed the Debye peak in the phase lag variation with the change of frequency and viscosity
The effects of frequency, fluid viscosity, and pore structure on the viscoelastic properties of rocks are numerically tested, respectively</description><identifier>ISSN: 2169-9313</identifier><identifier>EISSN: 2169-9356</identifier><identifier>DOI: 10.1002/2017JB013979</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Approximation ; Aspect ratio ; Coherent potential approximation ; Computational fluid dynamics ; Computer simulation ; Debye peak ; Dispersion ; Fluids ; Geophysics ; Igneous rocks ; Low frequencies ; Methods ; Modelling ; Modulus of elasticity ; Parameter sensitivity ; Parameters ; Phase lag ; Pore size ; Porosity ; Properties ; Properties (attributes) ; Rock ; Rock properties ; S waves ; Scale models ; Shear ; Silicates ; Spring ; Stiffness ; Storage ; Strain ; Stress-strain relationships ; stress‐strain method ; Test procedures ; viscoelastic ; Viscoelasticity ; Viscosity ; viscous fluid ; Viscous fluids</subject><ispartof>Journal of geophysical research. Solid earth, 2017-08, Vol.122 (8), p.6067-6086</ispartof><rights>2017. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a3737-54861b876a9393a9787deb8d976ad2f2540fe12ce97f12fe2ecca5d6894ea8793</citedby><cites>FETCH-LOGICAL-a3737-54861b876a9393a9787deb8d976ad2f2540fe12ce97f12fe2ecca5d6894ea8793</cites><orcidid>0000-0001-6920-0658 ; 0000-0002-1401-1873</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Wang, Zizhen</creatorcontrib><creatorcontrib>Schmitt, Douglas R.</creatorcontrib><creatorcontrib>Wang, Ruihe</creatorcontrib><title>Modeling of viscoelastic properties of nonpermeable porous rocks saturated with highly viscous fluid at seismic frequencies at the core scale</title><title>Journal of geophysical research. Solid earth</title><description>A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. Based on this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the storage moduli and the stress‐strain phase lag of saturated rocks. And we also compared the modeling results to the Hashin‐Shtrikman bounds and the coherent potential approximation (CPA). The dynamic moduli calculated from the modeling are lower than the predictions of CPA, and both of these fall between the Hashin‐Shtrikman bounds. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and aspect ratio affect the rock frame stiffness and result in different viscoelastic behaviors of the saturated rocks. The stress‐strain phase lags are larger with smaller stiffness contrasts between the rock frame and the pore fluid. The viscoelastic properties of saturated rocks are more sensitive to aspect ratio compared to other pore structure parameters. The results suggest that significant seismic dispersion (at about 50–200 Hz) might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids.
Plain Language Summary
We develop a core scale modeling method to simulate the viscoelastic properties of rocks saturated with viscous fluid at low frequencies based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. By using this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the composite's viscoelastic properties. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and pore aspect ratio affect the rock frame stiffness and result in different viscoelastic behavior of the saturated rocks. The lower the rock frame stiffness, the larger the stress‐strain phase lags. The viscoelastic properties of saturated rocks are more sensitive to the pore aspect ratio. The results suggest that significant seismic dispersion might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids. This will be important in the context of heavy hydrocarbon reservoirs and igneous rocks saturated with silicate melt.
Key Points
A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed
We observed the Debye peak in the phase lag variation with the change of frequency and viscosity
The effects of frequency, fluid viscosity, and pore structure on the viscoelastic properties of rocks are numerically tested, respectively</description><subject>Approximation</subject><subject>Aspect ratio</subject><subject>Coherent potential approximation</subject><subject>Computational fluid dynamics</subject><subject>Computer simulation</subject><subject>Debye peak</subject><subject>Dispersion</subject><subject>Fluids</subject><subject>Geophysics</subject><subject>Igneous rocks</subject><subject>Low frequencies</subject><subject>Methods</subject><subject>Modelling</subject><subject>Modulus of elasticity</subject><subject>Parameter sensitivity</subject><subject>Parameters</subject><subject>Phase lag</subject><subject>Pore size</subject><subject>Porosity</subject><subject>Properties</subject><subject>Properties (attributes)</subject><subject>Rock</subject><subject>Rock properties</subject><subject>S waves</subject><subject>Scale models</subject><subject>Shear</subject><subject>Silicates</subject><subject>Spring</subject><subject>Stiffness</subject><subject>Storage</subject><subject>Strain</subject><subject>Stress-strain relationships</subject><subject>stress‐strain method</subject><subject>Test procedures</subject><subject>viscoelastic</subject><subject>Viscoelasticity</subject><subject>Viscosity</subject><subject>viscous fluid</subject><subject>Viscous fluids</subject><issn>2169-9313</issn><issn>2169-9356</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp9kE1OwzAQhSMEEhV0xwEssaXgv8TxklZQqIqQEKwj1xk3Lmkc7ISqh-DOuApCrJiNx8-f3vhNklwQfE0wpjcUE7GYYsKkkEfJiJJMTiRLs-PfnrDTZBzCBsfKo0T4KPl6ciXUtlkjZ9CnDdpBrUJnNWq9a8F3FsLhqXFNvG1BrWpArfOuD8g7_R5QUF3vVQcl2tmuQpVdV_V-sIqMqXtbItWhADZso63x8NFDow--Ue4qQNp5QEGrGs6TE6PqAOOf8yx5u797nT1Mls_zx9ntcqKYYGKS8jwjq1xkSjLJlBS5KGGVlzIqJTU05dgAoRqkMIQaoKC1SssslxxULiQ7Sy4H3xgy_iZ0xcb1vokjCyI5zjiVnEfqaqC0dyF4MEXr7Vb5fUFwcdh58XfnEWcDvrM17P9li8X8ZZpSGtN8AxhdhWU</recordid><startdate>201708</startdate><enddate>201708</enddate><creator>Wang, Zizhen</creator><creator>Schmitt, Douglas R.</creator><creator>Wang, Ruihe</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/0000-0001-6920-0658</orcidid><orcidid>https://orcid.org/0000-0002-1401-1873</orcidid></search><sort><creationdate>201708</creationdate><title>Modeling of viscoelastic properties of nonpermeable porous rocks saturated with highly viscous fluid at seismic frequencies at the core scale</title><author>Wang, Zizhen ; Schmitt, Douglas R. ; Wang, Ruihe</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a3737-54861b876a9393a9787deb8d976ad2f2540fe12ce97f12fe2ecca5d6894ea8793</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Approximation</topic><topic>Aspect ratio</topic><topic>Coherent potential approximation</topic><topic>Computational fluid dynamics</topic><topic>Computer simulation</topic><topic>Debye peak</topic><topic>Dispersion</topic><topic>Fluids</topic><topic>Geophysics</topic><topic>Igneous rocks</topic><topic>Low frequencies</topic><topic>Methods</topic><topic>Modelling</topic><topic>Modulus of elasticity</topic><topic>Parameter sensitivity</topic><topic>Parameters</topic><topic>Phase lag</topic><topic>Pore size</topic><topic>Porosity</topic><topic>Properties</topic><topic>Properties (attributes)</topic><topic>Rock</topic><topic>Rock properties</topic><topic>S waves</topic><topic>Scale models</topic><topic>Shear</topic><topic>Silicates</topic><topic>Spring</topic><topic>Stiffness</topic><topic>Storage</topic><topic>Strain</topic><topic>Stress-strain relationships</topic><topic>stress‐strain method</topic><topic>Test procedures</topic><topic>viscoelastic</topic><topic>Viscoelasticity</topic><topic>Viscosity</topic><topic>viscous fluid</topic><topic>Viscous fluids</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, Zizhen</creatorcontrib><creatorcontrib>Schmitt, Douglas R.</creatorcontrib><creatorcontrib>Wang, Ruihe</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>Wang, Zizhen</au><au>Schmitt, Douglas R.</au><au>Wang, Ruihe</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Modeling of viscoelastic properties of nonpermeable porous rocks saturated with highly viscous fluid at seismic frequencies at the core scale</atitle><jtitle>Journal of geophysical research. Solid earth</jtitle><date>2017-08</date><risdate>2017</risdate><volume>122</volume><issue>8</issue><spage>6067</spage><epage>6086</epage><pages>6067-6086</pages><issn>2169-9313</issn><eissn>2169-9356</eissn><abstract>A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. Based on this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the storage moduli and the stress‐strain phase lag of saturated rocks. And we also compared the modeling results to the Hashin‐Shtrikman bounds and the coherent potential approximation (CPA). The dynamic moduli calculated from the modeling are lower than the predictions of CPA, and both of these fall between the Hashin‐Shtrikman bounds. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and aspect ratio affect the rock frame stiffness and result in different viscoelastic behaviors of the saturated rocks. The stress‐strain phase lags are larger with smaller stiffness contrasts between the rock frame and the pore fluid. The viscoelastic properties of saturated rocks are more sensitive to aspect ratio compared to other pore structure parameters. The results suggest that significant seismic dispersion (at about 50–200 Hz) might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids.
Plain Language Summary
We develop a core scale modeling method to simulate the viscoelastic properties of rocks saturated with viscous fluid at low frequencies based on the stress‐strain method. The elastic moduli dispersion of viscous fluid is described by the Maxwell's spring‐dash pot model. By using this modeling method, we numerically test the effects of frequency, fluid viscosity, porosity, pore size, and pore aspect ratio on the composite's viscoelastic properties. The modeling results indicate that the frequency and the fluid viscosity have similar effects on the dynamic moduli dispersion of fully saturated rocks. We observed the Debye peak in the phase lag variation with the change of frequency and viscosity. The pore structure parameters, such as porosity, pore size, and pore aspect ratio affect the rock frame stiffness and result in different viscoelastic behavior of the saturated rocks. The lower the rock frame stiffness, the larger the stress‐strain phase lags. The viscoelastic properties of saturated rocks are more sensitive to the pore aspect ratio. The results suggest that significant seismic dispersion might be expected for both compressional and shear waves passing through rocks saturated with highly viscous fluids. This will be important in the context of heavy hydrocarbon reservoirs and igneous rocks saturated with silicate melt.
Key Points
A core scale modeling method for viscoelastic properties of rocks saturated with viscous fluid at low frequencies is developed
We observed the Debye peak in the phase lag variation with the change of frequency and viscosity
The effects of frequency, fluid viscosity, and pore structure on the viscoelastic properties of rocks are numerically tested, respectively</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2017JB013979</doi><tpages>20</tpages><orcidid>https://orcid.org/0000-0001-6920-0658</orcidid><orcidid>https://orcid.org/0000-0002-1401-1873</orcidid></addata></record> |
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subjects | Approximation Aspect ratio Coherent potential approximation Computational fluid dynamics Computer simulation Debye peak Dispersion Fluids Geophysics Igneous rocks Low frequencies Methods Modelling Modulus of elasticity Parameter sensitivity Parameters Phase lag Pore size Porosity Properties Properties (attributes) Rock Rock properties S waves Scale models Shear Silicates Spring Stiffness Storage Strain Stress-strain relationships stress‐strain method Test procedures viscoelastic Viscoelasticity Viscosity viscous fluid Viscous fluids |
title | Modeling of viscoelastic properties of nonpermeable porous rocks saturated with highly viscous fluid at seismic frequencies at the core scale |
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