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. Author manuscript; available in PMC: 2010 Apr 8.
Published in final edited form as: Cell. 2007 Nov 30;131(5):952–965. doi: 10.1016/j.cell.2007.10.016

Figure 6. Analysis of Truncated, Artificially Dimerized Dynein Motors in the Optical Trapping Assay and Illustration of the “Compact” and “Extended” Dynein Conformations.

Figure 6

(A) Compact and extended conformations of the dynein dimer may explain a wide variation in step size. In its compact state, the two dynein rings are restrained and located in close proximity and perhaps overlapping due to direct head-to-head “interactions” or a “zipping” of the proximal tail. The loss of physical interactions or an “unzipping” of the proximal tail might cause a less restrained extended conformation with an increased head-to-head distance.

(B) Diagram of constructs showing the dynein heavy chain truncations and tags.

(C) Force production and stepping behavior of GST-Dyn1331kDa. Left: Schematic of the GST-Dyn1331kDa motor. Center: Histograms of the combined step size data (gray-shaded), classified according to the advancing (red histogram bars) and nonadvancing modes (blue histogram bars) (3 pN force-feedback data, n = 670). Right: Stall force distribution of GST-Dyn1331kDa (4.8 pN ± 1.0 pN; mean ± SD; n = 195).

(D) Force production and stepping behavior of GST-Dyn1314kDa. Left: Schematic of the GST-Dyn1314kDa motor. Center: Histograms of the combined, advancing and non-advancing step size data (3 pN force-feedback data, n = 518). Right: Stall force distribution of GST-Dyn1314kDa (4.0 pN ± 1.1 pN; mean ± SD; n = 91).

(E) Force production and stepping behavior of the dynein construct GST-α2-Dyn1314kDa with artificial linker elements. Left: Schematic of the GST-α2-Dyn1314kDa motor. Center: Histograms of the combined, advancing, and nonadvancing step size data (3 pN force-feedback data, n = 457). Right: Stall force distribution of GST-α2-Dyn1314kDa (5.2 pN ± 1.1 pN; mean ± SD; n = 80).