Biomechanical characterization of endothelial cells exposed to shear stress using acoustic force spectroscopy

Abstract

Characterizing mechanical properties of cells is important for understanding many cellular processes, such as cell movement, shape, and growth, as well as adaptation to changing environments. In this study, we explore mechanical properties of endothelial cells that form the biological barrier lining blood vessels, whose dysfunction leads to development of many cardiovascular disorders. Stiffness and contractile prestress of living endothelial cells were determined by Acoustic Force Spectroscopy (AFS) focusing on the displacement of functionalized microspheres located at the cell-cell periphery. The specific configuration of the acoustic microfluidic channel allowed us to develop a long-term dynamic culture protocol exposing cells to laminar flow, reaching shear stresses in the physiological range (i.e. 8 dyne cm-2) within 48 hours of barrier function maturation. A staircase-like sequence of increasing force steps, ranging from 186 pN to 3.5 nN, was applied in a single measurement revealing a force-dependent apparent stiffness in the kPa range. Moreover, our results show that different degrees of stiffening, defining the elastic behavior of the cell under different experimental conditions, i.e. static and dynamic, are caused by different levels of contractile prestress in the cytoskeleton, and are modulated by shear stress-mediated junction development and stabilization at cell borders. These results demonstrate that the AFS is capable of fast and high-throughput force measurements of adherent cells under conditions mimicking their native microenvironment, and thus revealing the shear stress dependence of mechanical properties of neighbouring endothelial cells.

A mechanical test of the tenertaxis hypothesis for leukocyte diapedesis

“…Because of the complex morphology and dynamic behavior of the leukocyte nucleus, its role in diapedesis is an open and actively debated question [37,38]. Third, we model the EC as hyperelastic and disregard the cytoplasm and potential viscoelastic responses of the endothelium [39]. Finally, we have treated the ILP as an inert solid object.…”