“…Starting with the work of Berson et al [ 35 ], numerical models of the orbital shaker system [ [30] , [31] , [32] , 34 , [36] , [37] , [38] , [39] , [40] , [41] , [42] , [43] , [44] , [45] , [46] ] have shown that WSS magnitude fluctuates with time, more so towards the edge of the well than at its centre, and that TAWSS is also greater towards the edge. Additionally, the direction of the instantaneous WSS vector rotates evenly through 360° at the centre of the well during each orbit whereas at the edge, vectors tend only to switch between forward and backward orientations along a line that is approximately parallel to the wall.…”