On the parametric model of loose bonding between poroelastic half-spaces
Wave propagation in a Newtonian viscous liquid layer of thickness ‘h’ and of shear viscosity ‘η’ bounded by two poroelastic half-spaces is studied. Possible bonding between the poroelastic half-spaces is discussed by considering the limiting forms of the secular equation, when h→0: (1)η is finite or...
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Veröffentlicht in: | Journal of vibration and control 2012-08, Vol.18 (9), p.1261-1274 |
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creator | Nath, C Nageswara Tajuddin, M Kumar, JM |
description | Wave propagation in a Newtonian viscous liquid layer of thickness ‘h’ and of shear viscosity ‘η’ bounded by two poroelastic half-spaces is studied. Possible bonding between the poroelastic half-spaces is discussed by considering the limiting forms of the secular equation, when h→0: (1)η is finite or η→0 such that η/h → ∞, (2) η→0 such that η/h → 0, (3) η → 0 such that η/h is a finite nonzero quantity, for each permeable and impermeable surface. It is shown that these three forms respectively represent welded, smooth and loosely bonded interface of poroelastic half-spaces. The secular equation for the interfacial waves for each of the above three types of bonding for infinite wavelength is derived as a particular case. It is observed that this secular equation is the same for all three types of bonding for each permeable and impermeable surface. Several other special cases are obtained. |
doi_str_mv | 10.1177/1077546311417834 |
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Possible bonding between the poroelastic half-spaces is discussed by considering the limiting forms of the secular equation, when h→0: (1)η is finite or η→0 such that η/h → ∞, (2) η→0 such that η/h → 0, (3) η → 0 such that η/h is a finite nonzero quantity, for each permeable and impermeable surface. It is shown that these three forms respectively represent welded, smooth and loosely bonded interface of poroelastic half-spaces. The secular equation for the interfacial waves for each of the above three types of bonding for infinite wavelength is derived as a particular case. It is observed that this secular equation is the same for all three types of bonding for each permeable and impermeable surface. 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Several other special cases are obtained.</description><subject>Bonding</subject><subject>Constraining</subject><subject>Fluid dynamics</subject><subject>Half spaces</subject><subject>Liquids</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Non-Newtonian fluids</subject><subject>Permeability</subject><subject>Propagation</subject><subject>Shear viscosity</subject><subject>Vibration</subject><subject>Viscosity</subject><subject>Wave propagation</subject><issn>1077-5463</issn><issn>1741-2986</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqFkc1LAzEUxIMoWKt3jwEvXlbz8t2jFLVCoRc9L9ntS7tld7MmW8T_3pR6EEE8vYH5zcBjCLkGdgdgzD0wY5TUAkCCsUKekAkYCQWfWX2adbaLg39OLlLaMcakBDYhi1VPxy3SwUXX4RibmnZhjS0NnrYhJKRV6NdNv6EVjh-IPR1CDNi6NGZ061pfpMHVmC7JmXdtwqvvOyVvT4-v80WxXD2_zB-WRS2MGguFwkOleS2Er2pvUMzqSmnulPdGGcNngoNl4KoZ10o4bdeQrQqYNQaNEFNye-wdYnjfYxrLrkk1tq3rMexTCUZz4NZa_j8qpTWKcXFovfmF7sI-9vmREhhXDBRomSl2pOoYUoroyyE2nYufGSoPK5S_V8iR4hhJboM_S__gvwDTdYR6</recordid><startdate>201208</startdate><enddate>201208</enddate><creator>Nath, C Nageswara</creator><creator>Tajuddin, M</creator><creator>Kumar, JM</creator><general>SAGE Publications</general><general>SAGE PUBLICATIONS, INC</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>7SP</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>JQ2</scope><scope>KR7</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope></search><sort><creationdate>201208</creationdate><title>On the parametric model of loose bonding between poroelastic half-spaces</title><author>Nath, C Nageswara ; Tajuddin, M ; Kumar, JM</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c375t-5e3f1b62c33fbcf7e39cb562a5ff757729321801ab92653a68d15ffb10877e733</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Bonding</topic><topic>Constraining</topic><topic>Fluid dynamics</topic><topic>Half spaces</topic><topic>Liquids</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Non-Newtonian fluids</topic><topic>Permeability</topic><topic>Propagation</topic><topic>Shear viscosity</topic><topic>Vibration</topic><topic>Viscosity</topic><topic>Wave propagation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nath, C Nageswara</creatorcontrib><creatorcontrib>Tajuddin, M</creatorcontrib><creatorcontrib>Kumar, JM</creatorcontrib><collection>CrossRef</collection><collection>Computer and Information Systems Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Journal of vibration and control</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nath, C Nageswara</au><au>Tajuddin, M</au><au>Kumar, JM</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>On the parametric model of loose bonding between poroelastic half-spaces</atitle><jtitle>Journal of vibration and control</jtitle><date>2012-08</date><risdate>2012</risdate><volume>18</volume><issue>9</issue><spage>1261</spage><epage>1274</epage><pages>1261-1274</pages><issn>1077-5463</issn><eissn>1741-2986</eissn><abstract>Wave propagation in a Newtonian viscous liquid layer of thickness ‘h’ and of shear viscosity ‘η’ bounded by two poroelastic half-spaces is studied. Possible bonding between the poroelastic half-spaces is discussed by considering the limiting forms of the secular equation, when h→0: (1)η is finite or η→0 such that η/h → ∞, (2) η→0 such that η/h → 0, (3) η → 0 such that η/h is a finite nonzero quantity, for each permeable and impermeable surface. It is shown that these three forms respectively represent welded, smooth and loosely bonded interface of poroelastic half-spaces. The secular equation for the interfacial waves for each of the above three types of bonding for infinite wavelength is derived as a particular case. It is observed that this secular equation is the same for all three types of bonding for each permeable and impermeable surface. Several other special cases are obtained.</abstract><cop>London, England</cop><pub>SAGE Publications</pub><doi>10.1177/1077546311417834</doi><tpages>14</tpages></addata></record> |
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subjects | Bonding Constraining Fluid dynamics Half spaces Liquids Mathematical analysis Mathematical models Non-Newtonian fluids Permeability Propagation Shear viscosity Vibration Viscosity Wave propagation |
title | On the parametric model of loose bonding between poroelastic half-spaces |
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