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Index of Online Supplemental Material for
J. Cell Biol. 10.1083/jcb.200807129
Odell et al.
• Video 1 Computer-animated videos of our 3D computer simulation of MKLP1s interacting with stable and unstable MTs to elevate MKLP1s in the future furrow zone of an 80-µm-diameter zygote cell.
• Video 2 The red curves show density of diffusing MKLP1s averaged throughout a thin wafer that spans the height of the cell intersecting the cortex.
• Video 3 ideo of the simulation from which the panels of Fig. 3 were taken, showing that H1–H3 can account for furrow positioning robustly in cells of different sizes.
• Video 4 Video of the simulation from which the panels of Fig. 4 were taken
• Video 5 This simulation video shows typical MT dynamics, not obscured by motors, that occur in all the 80-µm cell simulations (in Videos 1, 2, 4, and 6–10).
• Video 6 Video of the simulation from which the radial density plots of Fig 2 B were taken (shown in Video 2 B).
• Video 7 Video of the simulation from which the radial density plots of Fig. 2 E were taken (shown in Video 2 E).
• Video 8 Video of the simulation from which the radial density plots of Fig. 2 F were taken (shown in Video 2 F).
• Video 9 No equatorial ring accumulation of MKLP1s occurs absent of stable MTs, which is shown by this simulation, from which the radial density plots of Fig. 2 G were taken (shown in Video 2 G).
• Video 10 That only a small equatorial ring accumulation of MKLP1s occurs when MKLP1s do not stall at MT plus end tips is shown by this simulation, from which the radial density plots of Fig. 2 H were taken (shown in Video 2 H).
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