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. 2020 Oct 22;20(2):491–506. doi: 10.1007/s10237-020-01396-3

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© The Author(s) 2020, corrected publication 2020

Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 5 — Steady versus pulsatile inflow condition effects on the Reynolds stress characteristics. (a) Axial planes colored by the turbulence kinetic energy (k), anisotropy index ( $A I_{b}$ ), and barycentric AIM. (b) Deviation maps, showing the root–mean–square ( $C_{rms}$ , Eq. 16) and individual differences ( $C_{ic}^{s} - C_{ic}^{p}$ , superscripts: $s =$ steady, $p =$ pulsatile), of the AIM weights ranging from [0, 1]. (c) Barycentric maps with 50k points colored by k. Additional details are given in Fig. 3