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Cell-free layer development process in the entrance region of microvessels

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Abstract

We simulated red blood cell flows through a finite length channel with a two-dimensional immersed boundary lattice Boltzmann model. The local instantaneous variation in wall–cell distance has been examined in details, and a nominal cell-free layer (CFL) thickness has been proposed. The CFL development process along the channel has been then analyzed, showing that the CFL thickness profile can be basically split into two regimes: the initial rapid increase due to cell migration and the later gradual growth due to cell reorganization. Effects of various hemorheological factors, such as rigidity, aggregation, hematocrit, and channel width, have also been investigated. The development length of the CFL to 90 % of its final width ranges from 150 to 300 \(\upmu \)m, and the development length is sensitive to changes in hemorheological conditions. The correlation between the CFL features and hemorheological parameters has also been explored. The simulation results have been compared to available experimental studies, and qualitative agreement has been noticed. In spite of the model limitations, this study reveals the complexity of CFL development process, and it could be useful for better understanding relevant processes and phenomena in the microcirculation.

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Acknowledgments

The authors thank the anonymous reviewer for the critical comments and constructive suggestions. This work was supported by the Natural Science and Engineering Research Council of Canada (NSERC) and the Laurentian University Research Fund (LURF). This research has been enabled by the use of computing resources provided by WestGrid (http://www.westgrid.ca), SHARCNet (http://www.sharcnet.ca), and Compute/Calcul Canada (http://www.computecanada.org).

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Correspondence to Junfeng Zhang.

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Oulaid, O., Zhang, J. Cell-free layer development process in the entrance region of microvessels. Biomech Model Mechanobiol 14, 783–794 (2015). https://doi.org/10.1007/s10237-014-0636-y

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