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dc.contributor.authorLin, Miao
dc.date.accessioned2017-06-29T12:43:50Z
dc.date.available2017-06-29T12:43:50Z
dc.date.issued2016-12-22
dc.date.submitted2017-06-29T13:30:51.643Z
dc.identifier.citationLin, M, 2016. Interaction between the vascular endothelial glycocalyx and flow in vitro. Queen Mary University of Londonen_US
dc.identifier.urihttp://qmro.qmul.ac.uk/xmlui/handle/123456789/24656
dc.descriptionPhDen_US
dc.description.abstractVascular diseases, such as stroke and heart attacks, account for more than 50% of abnormal death worldwide. The cause of these diseases is linked to malfunctions of vascular endothelial cells, in particular the endothelial glycocalyx. This study investigates the location and stability of the endothelial glycocalyx under different flow conditions in vitro. AFM (Atomic Force Microscopy) micro indentation is carried out on endothelial cell membrane to determine its Young’s modulus. The Young’s modulus of the glycocalyx layer is then deduced from measurements on cell membranes with, and those without, the glycocalyx layer. Heparan sulphate (HS) is an important component of the glycocalyx and can be removed by the enzyme heparinase-III (Hep-III). Our results show the glycocalyx on cultured Human Umbilical Vein Endothelial Cells (HUVECs) has a Young’s modulus of ~0.64Kpa. We further observe how the Young’s modulus of the endothelial cell membrane decreases with time, as the glycocalyx layer redevelops, following its removal by Hep-III. Steady and oscillatory shear stimulations are used in flow chamber experiments. Under 24 hours’ steady shear stimulation (12.6 dyn/cm2), cells are seen to elongate and reorient parallel to the flow direction. The glycocalyx is seen to shift to the peripheral region of the cell surface. With actin depolymerisation treatment, significant shedding of the glycocalyx from the luminal surface of the cell is observed. This occurs together with the loss of focal adhesions on the basal membrane. When endothelial cells are subjected to 24 hours’ oscillating shear stress, the size of the cell increases as the oscillatory reversal time (time between changes in oscillatory flow direction) increases. Measurements are taken with oscillatory flow reversal programmed at 5s, 10s and 15s. The angle (between the long axis of the cell and the flow direction) and the aspect ratio (long axis vs short axis) change from 41.57° and 1.72 : 1 (static) to 40.18° and 3.26 : 1 (5s), 36.71° and 4.17 : 1 (10s), 26.5° and 4.39 : 1 (15s). Both the height and the area of the cell increase. The Young’s modulus of the endothelial cell membrane is measured under oscillatory flows with different reversal time and compared to that under static flow conditions. An increase in the Young’s modulus is observable under oscillatory flows, with the most significant change occurring at the edge (i.e. periphery) of the cell membrane area. As the oscillatory reversal time increases from 5s to 15s, the Young's modulus of the cell membrane increases. In the apical areas of the cell membrane, the increase is less significant. These results indicate that the thickness of the glycocalyx decreases as cells are exposed to oscillatory flows, and the loss is most significant in the peripheral region of the cell membrane. As the oscillatory reversal time increases from 5s to 15s, so the loss in the glycocalyx increases.en_US
dc.language.isoenen_US
dc.publisherQueen Mary University of Londonen_US
dc.rightsThe copyright of this thesis rests with the author and no quotation from it or information derived from it may be published without the prior written consent of the author
dc.subjectEngineering and Materials Scienceen_US
dc.subjectvascular endothelial cellsen_US
dc.subjectendothelial glycocalyxen_US
dc.subjectAtomic Force Microscopyen_US
dc.titleInteraction between the vascular endothelial glycocalyx and flow in vitroen_US
dc.typeThesisen_US


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