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. 2011 Dec 23;109(1):63-67. doi: 10.1073/pnas.1118197108

Fig. 5.

Fig. 5.

Effects of layers on the string structure. The first peak of g(x,z),g(r = d,θ) is shown for Stokesian dynamics simulations at Pe = 50 with particles confined in one layer (circles), and for Stokesian dynamics simulations at Pe = 50 with extra an flat potential barrier inserted in the middle of the suspension at y = 0 (squares).