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Here we demonstrate, with physical-modeling data, that the combination of long-spread reflection traveltimes... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_21810349" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Mode-converted PS-waves can provide critically important information for velocity analysis in transversely isotropic (TI) media. Here we demonstrate, with physical-modeling data, that the combination of long-spread reflection traveltimes of PP-and PS-waves can be inverted for the parameters of a horizontal TI layer with a tilted symmetry axis. 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{"id":1525404,"title":"Elastic-plastic transition stresses in a transversely isotropic thick-walled cylinder subjected to internal pressure and steady-state temperature","created_at":"2012-04-26T20:21:53.242-07:00","url":"https://www.academia.edu/1525404/Elastic_plastic_transition_stresses_in_a_transversely_isotropic_thick_walled_cylinder_subjected_to_internal_pressure_and_steady_state_temperature?f_ri=2064458","dom_id":"work_1525404","summary":null,"downloadable_attachments":[{"id":50942119,"asset_id":1525404,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":735274,"first_name":"Dr","last_name":"pankaj","domain_name":"iiuedu-in","page_name":"Dpankaj","display_name":"Dr pankaj","profile_url":"https://iiuedu-in.academia.edu/Dpankaj?f_ri=2064458","photo":"https://0.academia-photos.com/735274/251058/296708/s65_dr.pankaj.jpg"}],"research_interests":[{"id":133177,"name":"Temperature","url":"https://www.academia.edu/Documents/in/Temperature?f_ri=2064458","nofollow":false},{"id":234860,"name":"Steady state","url":"https://www.academia.edu/Documents/in/Steady_state?f_ri=2064458","nofollow":false},{"id":460900,"name":"Thermal Science","url":"https://www.academia.edu/Documents/in/Thermal_Science?f_ri=2064458","nofollow":false},{"id":794872,"name":"Cylinder","url":"https://www.academia.edu/Documents/in/Cylinder?f_ri=2064458","nofollow":false},{"id":2064458,"name":"Transversely Isotropic Solids","url":"https://www.academia.edu/Documents/in/Transversely_Isotropic_Solids?f_ri=2064458"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_12711281" 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type="text/json">{"id":452692,"name":"Finite Difference","url":"https://www.academia.edu/Documents/in/Finite_Difference?f_ri=2064458","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="504035" href="https://www.academia.edu/Documents/in/Three_Dimensional">Three Dimensional</a>, <script data-card-contents-for-ri="504035" type="text/json">{"id":504035,"name":"Three Dimensional","url":"https://www.academia.edu/Documents/in/Three_Dimensional?f_ri=2064458","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="1231330" href="https://www.academia.edu/Documents/in/Constitutive_Equation">Constitutive Equation</a><script data-card-contents-for-ri="1231330" type="text/json">{"id":1231330,"name":"Constitutive Equation","url":"https://www.academia.edu/Documents/in/Constitutive_Equation?f_ri=2064458","nofollow":false}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=12711281]'), work: {"id":12711281,"title":"Micro-Macro Analysis of Viscoelastic Unidirectional Laminated Composite Plates Using DR Method","created_at":"2015-05-31T20:45:59.493-07:00","url":"https://www.academia.edu/12711281/Micro_Macro_Analysis_of_Viscoelastic_Unidirectional_Laminated_Composite_Plates_Using_DR_Method?f_ri=2064458","dom_id":"work_12711281","summary":null,"downloadable_attachments":[{"id":45986991,"asset_id":12711281,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":31738739,"first_name":"Manouchehr","last_name":"Salehi","domain_name":"amirkabir","page_name":"ManouchehrSalehi","display_name":"Manouchehr Salehi","profile_url":"https://amirkabir.academia.edu/ManouchehrSalehi?f_ri=2064458","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=2064458","nofollow":false},{"id":452692,"name":"Finite 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href="https://www.academia.edu/20526256/Effective_reflection_coefficients_for_curved_interfaces_in_transversely_isotropic_media">Effective reflection coefficients for curved interfaces in transversely isotropic media</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/20526256" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5db29c0b7cdeed46adf87c88d4951dfe" rel="nofollow" data-download="{"attachment_id":41419691,"asset_id":20526256,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" 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href="https://www.academia.edu/Documents/in/High_Frequency">High Frequency</a>, <script data-card-contents-for-ri="48458" type="text/json">{"id":48458,"name":"High Frequency","url":"https://www.academia.edu/Documents/in/High_Frequency?f_ri=2064458","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="48903" href="https://www.academia.edu/Documents/in/Elastic_waves">Elastic waves</a><script data-card-contents-for-ri="48903" type="text/json">{"id":48903,"name":"Elastic waves","url":"https://www.academia.edu/Documents/in/Elastic_waves?f_ri=2064458","nofollow":false}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=20526256]'), work: {"id":20526256,"title":"Effective reflection coefficients for curved interfaces in transversely isotropic 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Frequency","url":"https://www.academia.edu/Documents/in/High_Frequency?f_ri=2064458","nofollow":false},{"id":48903,"name":"Elastic waves","url":"https://www.academia.edu/Documents/in/Elastic_waves?f_ri=2064458","nofollow":false},{"id":230949,"name":"Anisotropic media","url":"https://www.academia.edu/Documents/in/Anisotropic_media?f_ri=2064458"},{"id":260010,"name":"Wave propagation","url":"https://www.academia.edu/Documents/in/Wave_propagation?f_ri=2064458"},{"id":316273,"name":"Development Methodology","url":"https://www.academia.edu/Documents/in/Development_Methodology?f_ri=2064458"},{"id":321836,"name":"Spectrum","url":"https://www.academia.edu/Documents/in/Spectrum?f_ri=2064458"},{"id":1220539,"name":"Acoustic Modeling","url":"https://www.academia.edu/Documents/in/Acoustic_Modeling?f_ri=2064458"},{"id":1553474,"name":"Reflection Coefficient","url":"https://www.academia.edu/Documents/in/Reflection_Coefficient?f_ri=2064458"},{"id":2064458,"name":"Transversely Isotropic Solids","url":"https://www.academia.edu/Documents/in/Transversely_Isotropic_Solids?f_ri=2064458"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_8254293" data-work_id="8254293" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/8254293/Anisotropic_migration_weight_for_amplitude_preserving_migration_and_sensitivity_analysis">Anisotropic migration weight for amplitude-preserving migration and sensitivity analysis</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">An amplitude-preserving anisotropic migration formula is derived in this paper. The migration is viewed as a weighted diffraction stack and the migration weights are estimated with the stationary phase theorem. To obtain a formula easy to... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_8254293" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">An amplitude-preserving anisotropic migration formula is derived in this paper. The migration is viewed as a weighted diffraction stack and the migration weights are estimated with the stationary phase theorem. To obtain a formula easy to implement, the weights are written in terms of quantities computable along the rays. A sensitivity analysis is then carried out to show that, in the vertical transverse isotropic case, the amplitude-preserving migration is mainly governed by two parameters: the anisotropic NMO velocity and the parameter η. These parameters can be estimated from the data with a velocity (background) analysis. Therefore, it is possible to use this amplitude-preserving anisotropic migration to recover the correct amplitudes versus offset or azimuth in the migrated image.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/8254293" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="21a0b097d527edfee04edaa7aad6bc1b" rel="nofollow" data-download="{"attachment_id":48165671,"asset_id":8254293,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/48165671/download_file?st=MTczMjgxMjI3OSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="16325378" href="https://independent.academia.edu/DenisKiyashchenko">Denis Kiyashchenko</a><script data-card-contents-for-user="16325378" type="text/json">{"id":16325378,"first_name":"Denis","last_name":"Kiyashchenko","domain_name":"independent","page_name":"DenisKiyashchenko","display_name":"Denis Kiyashchenko","profile_url":"https://independent.academia.edu/DenisKiyashchenko?f_ri=2064458","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_8254293 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="8254293"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 8254293, container: ".js-paper-rank-work_8254293", }); 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The migration is viewed as a weighted diffraction stack and the migration weights are estimated with the stationary phase theorem. To obtain a formula easy to implement, the weights are written in terms of quantities computable along the rays. A sensitivity analysis is then carried out to show that, in the vertical transverse isotropic case, the amplitude-preserving migration is mainly governed by two parameters: the anisotropic NMO velocity and the parameter η. These parameters can be estimated from the data with a velocity (background) analysis. Therefore, it is possible to use this amplitude-preserving anisotropic migration to recover the correct amplitudes versus offset or azimuth in the migrated image.","downloadable_attachments":[{"id":48165671,"asset_id":8254293,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":16325378,"first_name":"Denis","last_name":"Kiyashchenko","domain_name":"independent","page_name":"DenisKiyashchenko","display_name":"Denis Kiyashchenko","profile_url":"https://independent.academia.edu/DenisKiyashchenko?f_ri=2064458","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":406,"name":"Geology","url":"https://www.academia.edu/Documents/in/Geology?f_ri=2064458","nofollow":false},{"id":409,"name":"Geophysics","url":"https://www.academia.edu/Documents/in/Geophysics?f_ri=2064458","nofollow":false},{"id":20099,"name":"Sensitivity 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data-has-card-for-ri="60" href="https://www.academia.edu/Documents/in/Mechanical_Engineering">Mechanical Engineering</a>, <script data-card-contents-for-ri="60" type="text/json">{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=2064458","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="73" href="https://www.academia.edu/Documents/in/Civil_Engineering">Civil Engineering</a>, <script data-card-contents-for-ri="73" type="text/json">{"id":73,"name":"Civil Engineering","url":"https://www.academia.edu/Documents/in/Civil_Engineering?f_ri=2064458","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="6216" href="https://www.academia.edu/Documents/in/Hydroxyapatite">Hydroxyapatite</a>, <script data-card-contents-for-ri="6216" 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class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/11074921/Study_of_orifice_compensated_hole_entry_hybrid_journal_bearing_considering_surface_roughness_and_flexibility_effects">Study of orifice compensated hole-entry hybrid journal bearing considering surface roughness and flexibility effects</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The present work describes a theoretical study to demonstrate the combined influence of surface roughness and bearing flexibility on the performance of an orifice compensated hole-entry hybrid journal bearing system. The average Reynold... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_11074921" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The present work describes a theoretical study to demonstrate the combined influence of surface roughness and bearing flexibility on the performance of an orifice compensated hole-entry hybrid journal bearing system. The average Reynold equation governing the flow of lubricant in the clearance space between rough journal and bearing surfaces and 3-dimensional elasticity equation governing the displacement field in the bearing shell have been solved simultaneously using finite element method. The influence of transverse, isotropic and longitudinal roughness patterns on the performance of orifice compensated hole-entry journal bearing configuration have been studied for the various values of surface roughness parameter (Λ), surface pattern parameter (γ ) and bearing shell deformation coefficient (D¯c). The study indicate that the reduction in the bearing characteristic parameters such as load carrying capacity, fluid-film stiffness and damping coefficients due to the bearing shell flexibility effect can be partially compensated in roughened hole-entry flexible journal bearing system by making a proper selection of roughness patterns. The results presented in the study demonstrates that for an accurate prediction of bearing characteristic data, the consideration of combined influence of surface roughness and bearing flexibility effects in the analysis may be more appropriate to use.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/11074921" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="9fa18ea42705ef41466a73ff3439c6c8" rel="nofollow" data-download="{"attachment_id":46921514,"asset_id":11074921,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/46921514/download_file?st=MTczMjgxMjI3OSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="26772683" href="https://pescemandya.academia.edu/TNAGARAJU">T NAGARAJU</a><script data-card-contents-for-user="26772683" type="text/json">{"id":26772683,"first_name":"T","last_name":"NAGARAJU","domain_name":"pescemandya","page_name":"TNAGARAJU","display_name":"T NAGARAJU","profile_url":"https://pescemandya.academia.edu/TNAGARAJU?f_ri=2064458","photo":"https://0.academia-photos.com/26772683/7470395/8393633/s65_t.nagaraju.jpg_oh_7fbfba86d7614c3233651907e2d28a11_oe_557cf12f___gda___1431482534_e2733de829638719c0b5453fd705e356"}</script></span></span></li><li class="js-paper-rank-work_11074921 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="11074921"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 11074921, container: ".js-paper-rank-work_11074921", }); 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The average Reynold equation governing the flow of lubricant in the clearance space between rough journal and bearing surfaces and 3-dimensional elasticity equation governing the displacement field in the bearing shell have been solved simultaneously using finite element method. The influence of transverse, isotropic and longitudinal roughness patterns on the performance of orifice compensated hole-entry journal bearing configuration have been studied for the various values of surface roughness parameter (Λ), surface pattern parameter (γ ) and bearing shell deformation coefficient (D¯c). The study indicate that the reduction in the bearing characteristic parameters such as load carrying capacity, fluid-film stiffness and damping coefficients due to the bearing shell flexibility effect can be partially compensated in roughened hole-entry flexible journal bearing system by making a proper selection of roughness patterns. The results presented in the study demonstrates that for an accurate prediction of bearing characteristic data, the consideration of combined influence of surface roughness and bearing flexibility effects in the analysis may be more appropriate to use.","downloadable_attachments":[{"id":46921514,"asset_id":11074921,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":26772683,"first_name":"T","last_name":"NAGARAJU","domain_name":"pescemandya","page_name":"TNAGARAJU","display_name":"T NAGARAJU","profile_url":"https://pescemandya.academia.edu/TNAGARAJU?f_ri=2064458","photo":"https://0.academia-photos.com/26772683/7470395/8393633/s65_t.nagaraju.jpg_oh_7fbfba86d7614c3233651907e2d28a11_oe_557cf12f___gda___1431482534_e2733de829638719c0b5453fd705e356"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=2064458","nofollow":false},{"id":12147,"name":"Finite element 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We obtain explicit equations for the vector field of displacements, for tensor fields of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_9438926" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This work will consider Volterra's theory of elastic dislocations in the case of a transversally isotropic homogeneous hyperelastic hollow cylinder. 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itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/13662119/Evidence_for_inner_core_anisotropy_from_free_oscillations">Evidence for inner core anisotropy from free oscillations</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Previous hypothesis concerning the cause of anomalous splitting in free oscillation spectra have led to models which are difficult to accept from the physical point of view-involving either substantial heterogeneity in the fluid outer... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_13662119" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Previous hypothesis concerning the cause of anomalous splitting in free oscillation spectra have led to models which are difficult to accept from the physical point of view-involving either substantial heterogeneity in the fluid outer core or large topographic variations in the core-mantle boundary and the inner core boundary and heterogeneity of several percent in inner core properties. 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