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56w,/citations/images/avatar_scholar_128.png 128w" width="56" height="56"></span></a><div><a href="/citations?user=CjqPDhMAAAAJ&hl=en">Luca Antiga</a></div></div></div></div><div id="gs_bdy_ccl" role="main"><div id="gsc_vcpb" data-edit-link="/citations?view_op=edit_citation&hl=en&user=CjqPDhMAAAAJ&citation_for_view=CjqPDhMAAAAJ:d1gkVwhDpl0C&citation_for_view=CjqPDhMAAAAJ:d1gkVwhDpl0C&back_view_op=view_citation"><form method="post" id="gsc_vcpb_btns" action="/citations?view_op=view_citation&hl=en"><input type="hidden" name="xsrf" value="ADIE8skAAAAAZ0PaJgGxRWJ4YT4IK8jmqmQsjwE"><input type="hidden" name="s" value="CjqPDhMAAAAJ:d1gkVwhDpl0C"><input type="hidden" name="continue" value="/citations?view_op=list_works&hl=en&hl=en&user=CjqPDhMAAAAJ"></form><div id="gsc_oci_title_wrapper"><div id="gsc_oci_title"><a class="gsc_oci_title_link" href="https://asmedigitalcollection.asme.org/biomechanical/article-abstract/131/6/061013/399499" data-clk="hl=en&sa=T&ei=pohCZ57zGPO_y9YPm4_bqAY">Correlations among indicators of disturbed flow at the normal carotid bifurcation</a></div></div><div id="gsc_oci_table"><div class="gs_scl"><div class="gsc_oci_field">Authors</div><div class="gsc_oci_value">Sang-Wook Lee, Luca Antiga, David A Steinman</div></div><div class="gs_scl"><div class="gsc_oci_field">Publication date</div><div class="gsc_oci_value">2009/6/1</div></div><div class="gs_scl"><div class="gsc_oci_field">Volume</div><div class="gsc_oci_value">131</div></div><div class="gs_scl"><div class="gsc_oci_field">Issue</div><div class="gsc_oci_value">6</div></div><div class="gs_scl"><div class="gsc_oci_field">Pages</div><div class="gsc_oci_value">061013</div></div><div class="gs_scl"><div class="gsc_oci_field">Description</div><div class="gsc_oci_value" id="gsc_oci_descr"><div class="gsh_small"><div class="gsh_csp">A variety of hemodynamic wall parameters (HWP) has been proposed over the years to quantify hemodynamic disturbances as potential predictors or indicators of vascular wall dysfunction. The aim of this study was to determine whether some of these might, for practical purposes, be considered redundant. Image-based computational fluid dynamics simulations were carried out for <svg class="gs_fsvg" aria-label="N=50" width="45px" height="10px" style="vertical-align:0px;"><g transform="matrix(0.01400, 0.00000, 0.00000, 0.01400, 0.00000, 9.56200)"><g><g><path transform="scale(0.48828, -0.48828)" d="M 96 0 Q 76 0 76 27 Q 77 32 80 44 T 88 64 T 102 72 Q 298 72 330 197 L 608 1317 Q 551 1327 428 1327 Q 408 1327 408 1354 Q 409 1359 412 1371 T 420 1391 T 434 1399 H 788 Q 803 1399 807 1386 L 1262 303 L 1489 1210 Q 1493 1232 1493 1241 Q 1493 1327 1335 1327 Q 1315 1327 1315 1354 Q 1322 1380 1326 1389 T 1350 1399 H 1788 Q 1808 1399 1808 1372 Q 1807 1367 1804 1354 T 1795 1334 T 1782 1327 Q 1586 1327 1554 1202 L 1260 18 Q 1253 0 1239 0 H 1214 Q 1200 0 1196 14 L 674 1253 L 670 1266 Q 666 1270 666 1272 L 395 188 Q 393 183 392 175 T 389 158 Q 389 105 435 88 T 549 72 Q 569 72 569 45 Q 562 17 557 8 T 535 0 H 96 Z "/><g transform="translate(912.52698, 0.00000)"><path transform="matrix(0.48828, 0.00000, 0.00000, -0.48828, 277.77780, 0.00000)" d="M 154 272 Q 137 272 126 285 T 115 313 Q 115 330 126 342 T 154 354 H 1440 Q 1455 354 1466 342 T 1477 313 Q 1477 298 1466 285 T 1440 272 H 154 Z M 154 670 Q 137 670 126 682 T 115 711 Q 115 726 126 739 T 154 752 H 1440 Q 1455 752 1466 739 T 1477 711 Q 1477 694 1466 682 T 1440 670 H 154 Z "/></g><g transform="translate(2245.86279, 0.00000)"><path transform="scale(0.48828, -0.48828)" d="M 178 233 Q 199 173 242 124 T 345 47 T 469 20 Q 617 20 673 135 T 729 414 Q 729 485 726 533 T 713 627 Q 694 699 646 753 T 530 807 Q 461 807 411 786 T 331 737 T 276 678 T 246 645 H 223 Q 218 645 210 651 T 203 664 V 1348 Q 203 1353 209 1358 T 223 1364 H 229 Q 367 1298 522 1298 Q 674 1298 815 1364 H 821 Q 828 1364 834 1359 T 840 1348 V 1329 Q 840 1319 836 1319 Q 766 1226 660 1174 T 442 1122 Q 360 1122 274 1145 V 758 Q 342 813 395 836 T 532 860 Q 645 860 734 795 T 872 625 T 920 412 Q 920 289 859 184 T 695 17 T 469 -45 Q 368 -45 283 7 T 150 147 T 102 334 Q 102 380 132 409 T 207 438 Q 252 438 282 408 T 313 334 Q 313 290 282 259 T 207 229 Q 200 229 191 230 T 178 233 Z "/><path transform="matrix(0.48828, 0.00000, 0.00000, -0.48828, 500.00000, 0.00000)" d="M 512 -45 Q 261 -45 170 161 T 80 653 Q 80 831 112 988 T 241 1254 T 512 1364 Q 647 1364 733 1298 T 864 1127 T 925 903 T 942 653 Q 942 477 909 323 T 782 62 T 512 -45 Z M 512 8 Q 626 8 682 125 T 751 384 T 764 686 Q 764 840 751 970 T 682 1205 T 512 1311 Q 396 1311 340 1205 T 271 969 T 258 686 Q 258 572 263 471 T 293 262 T 370 81 T 512 8 Z "/></g></g></g></g></svg> normal carotid bifurcations reconstructed from magnetic resonance imaging. Pairwise Spearman correlation analysis was performed for HWP quantifying wall shear stress magnitudes, spatial and temporal gradients, and harmonic contents. These were based on the spatial distributions of each HWP and, separately, the amount of the surface exposed to each HWP beyond an objectively-defined threshold. Strong and significant correlations were found among the related trio of time-averaged wall shear stress magnitude (TAWSS …</div></div></div></div><div class="gs_scl"><div class="gsc_oci_field">Total citations</div><div class="gsc_oci_value"><div style="margin-bottom:1em"><a href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5">Cited by 305</a></div><div id="gsc_oci_graph_wrapper"><div id="gsc_oci_graph" style="width:526px;"><div id="gsc_oci_graph_x"></div><div id="gsc_oci_graph_bars"><span class="gsc_oci_g_t" style="left:0px">2009</span><span class="gsc_oci_g_t" style="left:33px">2010</span><span class="gsc_oci_g_t" style="left:66px">2011</span><span class="gsc_oci_g_t" style="left:99px">2012</span><span class="gsc_oci_g_t" style="left:132px">2013</span><span class="gsc_oci_g_t" style="left:165px">2014</span><span class="gsc_oci_g_t" style="left:198px">2015</span><span class="gsc_oci_g_t" style="left:231px">2016</span><span class="gsc_oci_g_t" style="left:264px">2017</span><span class="gsc_oci_g_t" style="left:297px">2018</span><span class="gsc_oci_g_t" style="left:330px">2019</span><span class="gsc_oci_g_t" style="left:363px">2020</span><span class="gsc_oci_g_t" style="left:396px">2021</span><span class="gsc_oci_g_t" style="left:429px">2022</span><span class="gsc_oci_g_t" style="left:462px">2023</span><span class="gsc_oci_g_t" style="left:495px">2024</span><a href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5&as_ylo=2009&as_yhi=2009" class="gsc_oci_g_a" style="left:5px;height:2px;top:55px;z-index:16"><span class="gsc_oci_g_al">1</span></a><a href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5&as_ylo=2010&as_yhi=2010" class="gsc_oci_g_a" style="left:38px;height:22px;top:35px;z-index:15"><span class="gsc_oci_g_al">12</span></a><a href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5&as_ylo=2011&as_yhi=2011" 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href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5&as_ylo=2024&as_yhi=2024" class="gsc_oci_g_a" style="left:500px;height:29px;top:28px;z-index:1"><span class="gsc_oci_g_al">16</span></a></div></div></div></div></div><div class="gs_scl"><div class="gsc_oci_field">Scholar articles</div><div class="gsc_oci_value"><div class="gsc_oci_merged_snippet"><div><a href="/scholar?oi=bibs&cluster=171317752967661066&btnI=1&hl=en">Correlations among indicators of disturbed flow at the normal carotid bifurcation</a></div><div>SW Lee, L Antiga, DA Steinman - 2009</div><div><a class="gsc_oms_link" href="https://scholar.google.com/scholar?oi=bibs&hl=en&cites=171317752967661066&as_sdt=5">Cited by 305</a> <a class="gsc_oms_link" href="https://scholar.google.com/scholar?oi=bibs&hl=en&q=related:CgZbsZakYAIJ:scholar.google.com/">Related articles</a> <a class="gsc_oms_link" href="https://scholar.google.com/scholar?oi=bibs&hl=en&cluster=171317752967661066">All 7 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