Loading…

3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails

In the paper, the iterative numerical procedure was used for estimating the 3D crack front loading enhancements due to the action of the “liquid entrapment mechanism” (LEM). The 3D shallow angle, semi-elliptical, surface breaking crack inclined at 20° to the horizontal, in an early stage of developm...

Full description

Saved in:
Bibliographic Details
Published in:Wear 2008-10, Vol.265 (9), p.1356-1362
Main Authors: Bogdański, S., Lewicki, P.
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563
cites cdi_FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563
container_end_page 1362
container_issue 9
container_start_page 1356
container_title Wear
container_volume 265
creator Bogdański, S.
Lewicki, P.
description In the paper, the iterative numerical procedure was used for estimating the 3D crack front loading enhancements due to the action of the “liquid entrapment mechanism” (LEM). The 3D shallow angle, semi-elliptical, surface breaking crack inclined at 20° to the horizontal, in an early stage of development (similar to the “squat”-type crack typical in rails) was FE modelled and used for analysis. The volume of liquid entrapped was determined on the basis of the 3D crack geometry for the position of load, in which the leading edge of contact patch is touching the crack mouth. In the FE model this volume was represented by the empty space (bubble) between the crack faces loaded with the liquid pressure. During the LEM part of the cycle of loading this volume was assumed to be constant. At each position of contact load (rolling wheel), the pressure was gradually increasing in the iteration procedure until both the required volume of the “bubble” and “equilibrium state” with external contact load were attained. Then, the histories of Modes I, II, and III stress intensity factors (SIFs) and corresponding fatigue growth rates were determined for the selected points of the crack front. The obtained loading enhancements were compared with those estimated earlier by the authors and others on the basis of the 2D model of LEM.
doi_str_mv 10.1016/j.wear.2008.03.014
format article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_34088051</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0043164808001609</els_id><sourcerecordid>34088051</sourcerecordid><originalsourceid>FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563</originalsourceid><addsrcrecordid>eNp9kD1PwzAQhi0EEqXwB5i8wJZwjhM3kVgQ31IlBmC2rhe7uDhxsVMQ_55URYxM7_Lce3cPY6cCcgFCXazyL4MxLwDqHGQOotxjE1HPZFZUs9k-mwCUMhOqrA_ZUUorABBNpSbsWd7wLrTG82C5dx8b13LTDxHX3Ri8M_SGvUsdtyHyGLx3_ZJT6AekgVsc3HJjOEWk98RdzyM6n47ZgUWfzMlvTtnr3e3L9UM2f7p_vL6aZySVGLJKoGhsQQKBGqgIoaBG0aK0IFEsGgJoa5ohlc14twSyEhpQtaoXcgGVklN2vutdx_CxMWnQnUtkvMfehE3SsoS6hkqMYLEDKYaUorF6HV2H8VsL0Ft_eqW3_vTWnwapR3_j0NlvOyZCbyP25NLfZAFKFLKRI3e548z46qczUSdypifTumho0G1w_635AWp4hdM</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>34088051</pqid></control><display><type>article</type><title>3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails</title><source>ScienceDirect Journals</source><creator>Bogdański, S. ; Lewicki, P.</creator><creatorcontrib>Bogdański, S. ; Lewicki, P.</creatorcontrib><description>In the paper, the iterative numerical procedure was used for estimating the 3D crack front loading enhancements due to the action of the “liquid entrapment mechanism” (LEM). The 3D shallow angle, semi-elliptical, surface breaking crack inclined at 20° to the horizontal, in an early stage of development (similar to the “squat”-type crack typical in rails) was FE modelled and used for analysis. The volume of liquid entrapped was determined on the basis of the 3D crack geometry for the position of load, in which the leading edge of contact patch is touching the crack mouth. In the FE model this volume was represented by the empty space (bubble) between the crack faces loaded with the liquid pressure. During the LEM part of the cycle of loading this volume was assumed to be constant. At each position of contact load (rolling wheel), the pressure was gradually increasing in the iteration procedure until both the required volume of the “bubble” and “equilibrium state” with external contact load were attained. Then, the histories of Modes I, II, and III stress intensity factors (SIFs) and corresponding fatigue growth rates were determined for the selected points of the crack front. The obtained loading enhancements were compared with those estimated earlier by the authors and others on the basis of the 2D model of LEM.</description><identifier>ISSN: 0043-1648</identifier><identifier>EISSN: 1873-2577</identifier><identifier>DOI: 10.1016/j.wear.2008.03.014</identifier><identifier>CODEN: WEARAH</identifier><language>eng</language><publisher>Lausanne: Elsevier B.V</publisher><subject>3D FE crack model ; Applied sciences ; Coupled fields ; Exact sciences and technology ; Fluid entrapment mechanism ; Fracture mechanics (crack, fatigue, damage...) ; Friction, wear, lubrication ; Fundamental areas of phenomenology (including applications) ; Machine components ; Mechanical engineering. Machine design ; Physics ; RCF crack growth ; Rolling contact fatigue (RCF) cracks ; Solid mechanics ; Structural and continuum mechanics ; “Squat”-type cracks in rails</subject><ispartof>Wear, 2008-10, Vol.265 (9), p.1356-1362</ispartof><rights>2008 S. Bogdański</rights><rights>2008 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563</citedby><cites>FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,780,784,789,790,23930,23931,25140,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=20612393$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Bogdański, S.</creatorcontrib><creatorcontrib>Lewicki, P.</creatorcontrib><title>3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails</title><title>Wear</title><description>In the paper, the iterative numerical procedure was used for estimating the 3D crack front loading enhancements due to the action of the “liquid entrapment mechanism” (LEM). The 3D shallow angle, semi-elliptical, surface breaking crack inclined at 20° to the horizontal, in an early stage of development (similar to the “squat”-type crack typical in rails) was FE modelled and used for analysis. The volume of liquid entrapped was determined on the basis of the 3D crack geometry for the position of load, in which the leading edge of contact patch is touching the crack mouth. In the FE model this volume was represented by the empty space (bubble) between the crack faces loaded with the liquid pressure. During the LEM part of the cycle of loading this volume was assumed to be constant. At each position of contact load (rolling wheel), the pressure was gradually increasing in the iteration procedure until both the required volume of the “bubble” and “equilibrium state” with external contact load were attained. Then, the histories of Modes I, II, and III stress intensity factors (SIFs) and corresponding fatigue growth rates were determined for the selected points of the crack front. The obtained loading enhancements were compared with those estimated earlier by the authors and others on the basis of the 2D model of LEM.</description><subject>3D FE crack model</subject><subject>Applied sciences</subject><subject>Coupled fields</subject><subject>Exact sciences and technology</subject><subject>Fluid entrapment mechanism</subject><subject>Fracture mechanics (crack, fatigue, damage...)</subject><subject>Friction, wear, lubrication</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Machine components</subject><subject>Mechanical engineering. Machine design</subject><subject>Physics</subject><subject>RCF crack growth</subject><subject>Rolling contact fatigue (RCF) cracks</subject><subject>Solid mechanics</subject><subject>Structural and continuum mechanics</subject><subject>“Squat”-type cracks in rails</subject><issn>0043-1648</issn><issn>1873-2577</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNp9kD1PwzAQhi0EEqXwB5i8wJZwjhM3kVgQ31IlBmC2rhe7uDhxsVMQ_55URYxM7_Lce3cPY6cCcgFCXazyL4MxLwDqHGQOotxjE1HPZFZUs9k-mwCUMhOqrA_ZUUorABBNpSbsWd7wLrTG82C5dx8b13LTDxHX3Ri8M_SGvUsdtyHyGLx3_ZJT6AekgVsc3HJjOEWk98RdzyM6n47ZgUWfzMlvTtnr3e3L9UM2f7p_vL6aZySVGLJKoGhsQQKBGqgIoaBG0aK0IFEsGgJoa5ohlc14twSyEhpQtaoXcgGVklN2vutdx_CxMWnQnUtkvMfehE3SsoS6hkqMYLEDKYaUorF6HV2H8VsL0Ft_eqW3_vTWnwapR3_j0NlvOyZCbyP25NLfZAFKFLKRI3e548z46qczUSdypifTumho0G1w_635AWp4hdM</recordid><startdate>20081030</startdate><enddate>20081030</enddate><creator>Bogdański, S.</creator><creator>Lewicki, P.</creator><general>Elsevier B.V</general><general>Elsevier Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20081030</creationdate><title>3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails</title><author>Bogdański, S. ; Lewicki, P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>3D FE crack model</topic><topic>Applied sciences</topic><topic>Coupled fields</topic><topic>Exact sciences and technology</topic><topic>Fluid entrapment mechanism</topic><topic>Fracture mechanics (crack, fatigue, damage...)</topic><topic>Friction, wear, lubrication</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Machine components</topic><topic>Mechanical engineering. Machine design</topic><topic>Physics</topic><topic>RCF crack growth</topic><topic>Rolling contact fatigue (RCF) cracks</topic><topic>Solid mechanics</topic><topic>Structural and continuum mechanics</topic><topic>“Squat”-type cracks in rails</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bogdański, S.</creatorcontrib><creatorcontrib>Lewicki, P.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Wear</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bogdański, S.</au><au>Lewicki, P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails</atitle><jtitle>Wear</jtitle><date>2008-10-30</date><risdate>2008</risdate><volume>265</volume><issue>9</issue><spage>1356</spage><epage>1362</epage><pages>1356-1362</pages><issn>0043-1648</issn><eissn>1873-2577</eissn><coden>WEARAH</coden><abstract>In the paper, the iterative numerical procedure was used for estimating the 3D crack front loading enhancements due to the action of the “liquid entrapment mechanism” (LEM). The 3D shallow angle, semi-elliptical, surface breaking crack inclined at 20° to the horizontal, in an early stage of development (similar to the “squat”-type crack typical in rails) was FE modelled and used for analysis. The volume of liquid entrapped was determined on the basis of the 3D crack geometry for the position of load, in which the leading edge of contact patch is touching the crack mouth. In the FE model this volume was represented by the empty space (bubble) between the crack faces loaded with the liquid pressure. During the LEM part of the cycle of loading this volume was assumed to be constant. At each position of contact load (rolling wheel), the pressure was gradually increasing in the iteration procedure until both the required volume of the “bubble” and “equilibrium state” with external contact load were attained. Then, the histories of Modes I, II, and III stress intensity factors (SIFs) and corresponding fatigue growth rates were determined for the selected points of the crack front. The obtained loading enhancements were compared with those estimated earlier by the authors and others on the basis of the 2D model of LEM.</abstract><cop>Lausanne</cop><cop>Amsterdam</cop><cop>New York, NY</cop><pub>Elsevier B.V</pub><doi>10.1016/j.wear.2008.03.014</doi><tpages>7</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0043-1648
ispartof Wear, 2008-10, Vol.265 (9), p.1356-1362
issn 0043-1648
1873-2577
language eng
recordid cdi_proquest_miscellaneous_34088051
source ScienceDirect Journals
subjects 3D FE crack model
Applied sciences
Coupled fields
Exact sciences and technology
Fluid entrapment mechanism
Fracture mechanics (crack, fatigue, damage...)
Friction, wear, lubrication
Fundamental areas of phenomenology (including applications)
Machine components
Mechanical engineering. Machine design
Physics
RCF crack growth
Rolling contact fatigue (RCF) cracks
Solid mechanics
Structural and continuum mechanics
“Squat”-type cracks in rails
title 3D model of liquid entrapment mechanism for rolling contact fatigue cracks in rails
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-28T08%3A21%3A27IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=3D%20model%20of%20liquid%20entrapment%20mechanism%20for%20rolling%20contact%20fatigue%20cracks%20in%20rails&rft.jtitle=Wear&rft.au=Bogda%C5%84ski,%20S.&rft.date=2008-10-30&rft.volume=265&rft.issue=9&rft.spage=1356&rft.epage=1362&rft.pages=1356-1362&rft.issn=0043-1648&rft.eissn=1873-2577&rft.coden=WEARAH&rft_id=info:doi/10.1016/j.wear.2008.03.014&rft_dat=%3Cproquest_cross%3E34088051%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c361t-51a19f2c1a0c905ca02c96cb4f03a1b9c00d8c7ac4964830cf30906868b3b0563%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=34088051&rft_id=info:pmid/&rfr_iscdi=true