Fluid shear stress has been shown to modulate endothelial gene programs1-5 through activation of cis-regulatory elements6, histone acetyltransferase activity7 and shear stress response elements (SSRE)8. Shear stress influences endothelial contributions towards coagulation by modulating tissue factor9 and tissue plasminogen activator (tPA)10 expression. Shear stress also influences control of angiogenesis11 and vessel remodeling by regulating PDGF-B synthesis and responsiveness8. The endothelial derived vasoactive mediators adrenomedullin, endothelin-1, urotensin II and relaxin are also regulated by shear12. Transcription of endothelial nitric oxide synthase production and nitric oxide production are both shear dependent10. Shear also controls endothelial ICAM-1 expression13. Flow-induced shear stress can therefore powerfully influence a large variety of endothelial responses. Importantly, vascular pulsations now also appear to play important roles in the pathophysiology of both normal vascular aging and forms of vascular dementia14 and may even contribute to other neurodegenerative diseases, such as multiple sclerosis15.
Venous and arterial endothelial cells are inherently exposed to diverse hemodynamic flow patterns in vivo, and many different endothelial cell phenotypes can be exhibited16. Depending on the magnitude and periodicity of flow, effects on endothelial cells may include inflammatory cell activation and apoptosis, which may reflect changes in gene or protein expression17,18. Studies on endothelial cell responses to shear phenomena therefore remain complicated by the difficulties in producing in vitro models that adequately produce such shear patterns.
Many different experimental protocols have been developed to apply fluid shear stress to endothelial cell monolayers. One of the most commonly used systems is the parallel plate flow chamber, which creates uniform laminar flow within the chamber19-21. A peristaltic pump is typically connected to create periodic flow, which can recapitulate flow characteristics typically found in many locations in vivo22. Another common set-up uses the 'cone and plate' model, where fluid shear stress is determined by the rotational speed of the cone23. Both systems, and other arrangements similar to them, can be tedious to set up and require components that can be relatively expensive and inaccessible to many laboratories.
Another major limitation of these current models is the relatively low number of replicate studies that can be simultaneously performed, each with a relatively low surface area. This increases the time and complexity of such approaches. Therefore, an ideal model that induces unidirectional and periodic shear might be one where a high number of study replicates can be easily set up, each with a relatively large surface area. Furthermore, the aforementioned models require a fairly sophisticated setup, which may be cost-prohibitive for many users. A model that can produce fluid shear disturbances using basic laboratory materials might have several advantages.
A simple and highly economical method of applying unidirectional, periodic shear stress involves the placement of circular dishes on an orbital shaker24. This protocol is very simple and can be scaled up to achieve high numbers of study replicates, each with a relatively large surface area, as needed. However, cells located in the center of the dish are exposed to different flow patterns than cells along the periphery, yielding mixed cellular phenotypic responses in the same dish.
In this current report, we describe the construction and use of 'shear rings', our model for creating unidirectional and periodic shear stress. The design for the shear ring effectively limits 'mixed' cellular shear-induced phenotypes by restricting the flow pathway within a circular culture dish to the periphery through the placement of an inner ring. The construction and operation of the shear ring is simple and economical and can be easily scaled to accommodate a wide range of orbital shakers using widely available tissue culture supplies. This model can be applied in endothelial cell experiments to provide unidirectional and periodic flow patterns within physiological and pathophysiological levels.