Abstract

Vascular endothelial cells and circulating red blood cell (RBC) surfaces are both covered by a layer of bushy glycocalyx. The interplay between these glycocalyx layers is hardly measurable and insufficiently understood. This study aims to investigate and qualify the possible interactions between the glycocalyces of RBCs and endothelial cells using mathematical modeling and numerical simulation. Dissipative particle dynamics (DPD) simulations are conducted to investigate the response of the endothelial glycocalyx (EG) to varying ambient conditions. A two-compartment model including EG and flow and a three-compartment model comprising EG, RBC glycocalyx, and flow are established. The two-compartment analysis shows that a relatively fast flow is associated with a predominantly bending motion of the EG, whereas oscillatory motions are predominant in a relatively slow flow. Results show that circulating RBCs cause the contactless deformation of EG. Its deformation is dependent on the chain layout, chain length, bending stiffness, RBC-to-EG distance, and RBC velocities. Specifically, shorter EG chains or RBC-to-EG distance leads to greater relative deflections of EG. Deformation of EG is enhanced when the EG chains are rarefied or RBCs move faster. The bending stiffness maintains stretching conformation of EG. Moreover, a compact EG chain layout and shedding EG chains disturb the neighboring flow field, causing disordered flow velocity distributions. In contrast, the movement of EG chains on RBC surfaces exerts a marginal driving force on RBCs. The DPD method is used for the first time, to our knowledge, in the three-compartment system to explore the cross talk between EG and RBC glycocalyx. This study suggests that RBCs drive the EG deformation via the near-field flow, whereas marginal propulsion of RBCs by the EG is observed. These new, to our knowledge, findings provide a new angle to understand the roles of glycocalyx in mechanotransduction and microvascular permeability and their perturbations under idealized pathophysiologic conditions associated with EG degradation.

Highlights

  • The endothelial glycocalyx (EG) is a delicate bushy structure interfacing blood and the endothelial cell membrane

  • EG as a propulsor for red blood cell (RBC) movement In EG deformation induced by the propulsion from RBC glycocalyx, we demonstrated that the RBC drives the motion of the EG via the near-field flow field, and EG chains respond differently as the distance between RBC-EG and RBC velocities change

  • The RBC glycocalyx and EG interactions and their interplay with flow are investigated via a Dissipative particle dynamics (DPD) simulation method for the first time, to our knowledge

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Summary

Introduction

The endothelial glycocalyx (EG) is a delicate bushy structure interfacing blood and the endothelial cell membrane. Its hallmark functions include regulation of traffic of circulating proinflammatory cells, vascular permeability, mechanotrans-. The structural integrity of EG secures its functionality. Structural EG complexity is engendered in linear or globular proteoglycan core proteins decorated with covalently bound long chains of glycosaminoglycans. Together, they are responsible for the creation of the fine molecular fence, which performs as an external cellular sieve and depository for various bioactive molecules and as sensory antennae. Activation of heparanase, followed by pruning of heparan sulfate chains and accelerated degradation of EG in diverse pathological conditions, has been well established [6,7,8,9,10,11]

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