Biased diffusion. Binding of candidate couplers to microtubule ends can be monitored experimentally by tethering the coupler at the surface of beads, and then monitoring bead motion. Three kinds of tethering to microtubule ends can be distinguished experimentally at this time: (1) Dam1-dependent rings generate high forces. The attached beads do not roll (Grishchuk et al, 2008a). The structure of the Dam1 complex is discussed in Figure 6; (2) Ring-independent Dam1 coupling in which the bead does roll as the MT shortens (Grishchuk et al, 2008b); (3) Motor-dependent tethering in which beads do not roll (Grissom et al, 2009). The mechanism of this coupling is still unknown. Two additional modes of movement have been proposed: (1) biased diffusion, as originally proposed in Hill's model (Hill, 1985) and more recently for the Ndc80 complex (Powers et al, 2009); and (2) power strokes from bending protofilaments acting on non-diffusing, MT-binding fibrils (McIntosh et al, 2008). (A) With a ring coupler encircling a microtubule (inspired by the Dam1 ring, discussed in Figure 6), force may be provided by flared depolymerizing protofilaments, which exercise a pressure against the base of the sleeve. (B) Hill's model depicts the microtubule-binding site of the kinetochore as a ‘sleeve' surrounding the microtubule (Hill, 1985). The microtubule-binding sites are represented by triangles. Maximization of the number of binding sites drives the sliding of the sleeve along the microtubule. The design and theoretical treatment of (B–F) are largely based on earlier work (Joglekar and Hunt, 2002; Powers et al, 2009). (C) The overall activation energy required for sliding along the lattice may cause diffusion to be slow or fast. To be effective, diffusion has to occur with kinetics that must be compatible with the kinetics of microtubule depolymerization. (D) An alternative mechanism for biased diffusion based on the Ndc80 complex was recently proposed (Powers et al, 2009). Kinetochores are shown as red hollow discs. The coupler is an elongated molecule with two globular domains at either end, one for kinetochore binding and one for microtubule binding, and it is inspired by the Ndc80 complex (see Figure 6). Coupling is along the lattice and is mediated by five microtubule-binding elements. The free-energy landscape for this coupler is shown on the right. l denotes spacing of sites. The red circle represents the current position of the coupler on the surface. The energy landscape is corrugated because movement along the filament requires breaking and reforming some bonds (C). b is the activation energy, w is the binding energy. The triangle represents a fiduciary mark along the microtubule. (E) The microtubule has depolymerized and the coupler has diffused on the surface towards the plus end. (F) The release of the coupler (two out of five binding sites have been lost here) implies an increase in free energy because the bond energies, w, must be overcome to move the couple past the filament tip. The heights of the activation energies 5b, 4b,…., b, decrease as the coupler begins to move past the tip. (G) The bottom row shows tomographic slices of kinetochore microtubule ends. The same gallery is also shown in the top row with protofilaments and their associated kinetochore fibrils, indicated by graphic overlays. (H) A tomographic reconstruction of a kinetochore–microtubule interface with associated fibrils. (G, H) are from McIntosh et al (2008).