Abstract
Kinetochores are complex macromolecular assemblies that link chromosomes to the mitotic spindle, mediate forces for chromosome motion, and generate the checkpoint signal delaying anaphase onset until all chromosomes are incorporated into the spindle. Proper execution of these functions depends on precise interactions between kinetochores and microtubules. While the molecular composition of the kinetochore is well described, structural organization of this organelle at the molecular and atomic levels is just beginning to emerge. Recent structural studies across scales suggest that kinetochores should not be viewed as rigid static scaffolds. Instead, these organelles exhibit a surprising degree of flexibility that enables rapid adaptations to various types of interactions with the mitotic spindle.
Introduction
Sublime is perhaps the most appropriate adjective to characterize the kinetochore. The importance of this organelle is unquestionable, but its appearance is so subtle that it took the advent of electron microscopy (EM) to visualize this organelle [1]. In glutaraldehyde-fixed EM samples, kinetochores comprise three morphological domains: a dense inner plate, translucent middle layer, and a dense outer plate that supports a fibrous corona in the absence of spindle microtubule attachment (Fig 1A and E). Paradoxically, introduction of milder fixation procedures such as high-pressure freezing revealed that relatively sharp outer plate of the kinetochore is an artifact induced by the collapse of the labile network of fine fibers comprising the kinetochore outer layer [2] (Fig 1B–D and F–H). A better-preserved kinetochore appears even less structured.
The kinetochore’s apparent simplicity is deceptive as this biochemically complex organelle contains more than 80–100 specific proteins that are recruited to the kinetochore in a complicated semi-hierarchical manner [reviewed in 3]. At the core is the Constitutive Centromere Associated Network (CCAN) of proteins that specifies the site of kinetochore assembly on chromosomes and is thought to provide a base to assemble the outer kinetochore. The outer domain forms about the KMN network consisting of the KNL1 protein and the Mis12C and Ndc80C heterotetramic complexes (where C indicates complex to distinguish from the Mis12 and Ndc80 proteins). The KMN network is responsible for “load bearing” attachment to the spindle microtubules [4;5]. Together the CCAN, KMN network, and proteins such as CENP-F and Zwint, provide a scaffold for a number of motor, checkpoint, and regulatory components that dynamically associate with the kinetochore. Such molecular complexity reflects diverse chemical interactions as the kinetochore performs three fundamental roles in mitosis: 1) Attach chromosomes to the spindle; 2) Mediate forces that move the chromosomes; 3) Ensure that mitotic exit does not occur prematurely before each and every chromosome is incorporated into the spindle. Obviously, these multifaceted functions require that kinetochore organization be adaptable to the rapidly changing environment of the mitotic spindle. The structural basis for this adaptability is beginning to emerge from recent live-cell observations, biochemistry, and structural studies at multiple scales. This review summarizes these recent developments, with an emphasis on vertebrate kinetochores.
Structure and function of the outer domain
The outer layer of the kinetochore is a fibrous meshwork functioning as the principal site of microtubule attachment (Fig.1C and D) [6;7]. A major molecular player in this region is the highly conserved KMN network, whose Ndc80C constituent binds to the outer wall of microtubules [8;9]. Yeast Ndc80C is a 56 nm long “dumbbell” arranged with the globular N-terminal heads of the Ndc80/Nuf2 and Spc24/25 heterodimers at opposite ends of the complex (Fig. 2A) [10]. The two heterodimers are connected by their C-terminal tails. Negative-stain EM demonstrated that the complex is not completely linear due to a flexible hinge in the coiled-coil region of Ndc80C [11].
Co-sedimentation binding experiments with purified components indicate that the globular head of the Ndc80/Nuf2 heterodimer binds microtubules, while Spc24/25 localizes the complex at the kinetochore [8]. This finding was corroborated by x-ray crystallography demonstrating that both the Ndc80 [12] and Nuf2 [13] heads contain a calponin-homology domain that is implicated in microtubule attachment of plus-end tracking proteins. However, point mutation studies demonstrate that it is the N-terminal 80 amino acids of Ndc80 that are critical for attachment [14;15]. This unstructured tail is highly basic and is thought to interact with the acidic c-terminal tail on the surface of tubulin as “ionic spaghetti” (i.e., the general ionic bonding of unstructured chains of two proteins rather than bonding between specific residues in each protein). The strength of this binding is reduced by phosphorylation from the kinase Aurora B [14], which in turn is spatially regulated [16].
While a combination of biochemical and x-ray crystallographic approaches were able to identify the critical domains in Ndc80 for microtubule attachment, the 8.6 Angstrom cryo- EM map was required to determine how these domains interact with microtubules [17]. Docking the atomic models of Ndc80/Nuf2 heads and tubulin in to the Cryo-EM map demonstrates that the calponin homology domain forms a “toe” that fits at the interface of each tubulin monomer (Ndc80 binds to both alpha and beta tubulin) (Fig. 2B). Binding by the toe region is sensitive to conformation with strong preference for the straight protofilaments associated with MT assembly. Consequently, Ndc80C attachment renders MT more resistant to disassembly in the cold and could explain the effect of kinetochore attachment on the conformation of microtubule plus ends [7;17;18]. These reconstructions fail to visualize the disordered N-terminal tail, which electron tomography images of microtubules bound with subsaturating amounts of Ndc80C indicate provides the majority of microtubule affinity, as noted above.
The importance of the unstructured tail is further substantiated by Tooley and colleagues who used a knockdown/ rescue system to demonstrate the importance of a key lysine residue in the toe region for kinetochore-MT attachment in vivo [19]. The study identified two additional lysines and confirmed the importance of the unstructured tail. This led to a three-point contact model for Ndc80 binding with the unstructured tail functioning as a tether (Fig. 2C). Charge is important for these interactions because lysine can be replace by arginine, but not a by a neutral or acidic amino acid.
Sub-saturation binding assays show cooperativity between adjacent Ndc80Cs resulting in a high frequency of clusters of 3 or 4 contact points with microtubules [13;17]. Cooperative binding enables clusters to stay attached when some molecules in the clusters detach, suggesting a mechanism for Ndc80C to follow and capture the energy release by disassembling microtubules in order to power chromosome motion (Fig 2D) [17;19]. The physiological relevance of cooperative binding is also supported by the frequent detection of clusters of kinetochore attachments to microtubule walls in situ [6] (Fig. 2E). The N-terminal tail of Ndc80 is required for cooperative binding, implying that this region aids the kinetochore in following disassembling microtubules [17].
Less is known about structure and functional mechanism of other members of the KMN network, but recent negative stain EM reconstructions show that bacterially expressed Mis12C is a 22-nm long linear array of four globular proteins [20]. Binding, crosslinking, and in vitro EM studies identified the C-terminal tail of NSL1 as the binding site for Spc24/25 and KNL1 at one end of the Mis12C (Fig. 3A). NNF1, which is presumably at the other end of Mis12C, interacts with CENP-C suggesting that Mis12 is the link between Ndc80C and the CCAN core [21;22]. Hence the Mis12C-Ndc80C portion of the KNM network could take the appearance of an 80-nm filament linking the inner kinetochore with microtubules, as suggested by electron tomography (Fig. 3B) [18]. However, it is unlikely that connectivity is simply linear because the CCAN proteins CENP-H and CENP-K interact directly with Ndc80C [23;24]. Nevertheless, Mis12C is architecturally positioned at a key intersection between the microtubule binding activity of Ndc80, the outer scaffold function of KNL1, and the inner kinetochore.
The EM and X-ray crystallography studies discussed above revealed many details of the organization of the chromosome-microtubule binding site. Less is known about the spatial distribution of microtubule binding sites within the kinetochore and how the kinetochore structure is affected by various types of microtubule attachments. By nature, EM and X-ray crystallography tend to impose a static view of kinetochores. Yet, evidence is mounting that kinetochores function as flexible, dynamic points of contact between the chromosome and the spindle due to the presence of compliant elements.
Kinetochore compliance: insights and issues
Due to its small size, kinetochore fine detail is obscured by diffraction, making it difficult to learn much about their structure by light microscopy. However, relative positions of individual proteins within the kinetochore can be assessed by measuring the distances between the distributions of proteins labeled with spectrally different fluorophores. This method, commonly referred to as super high resolution co-localization microscopy (SHREC), can partially overcome the limitation imposed by diffraction by assuming that the centers of the point spread functions corresponds to the true positions of the proteins. The main advantage of SHREC is that it can reveal redistribution of components due to transitions in kinetochore architecture. Using SHREC, the relative positions of 16 kinetochore proteins have been established [25] and this molecular map is in good agreement with biochemical and structural data obtained by EM. As expected, the outer domain proteins are more distal to the heterochromatin than CCAN proteins. Immuno-EM studies place Ndc80C in the outer plate (Fig. 3C) [26] and CENP-C in the heterochromatin [27]. This is consistent with the KMN and CCAN networks being located in the outer plate and the distal edge of the heterochromatin in EM images.
Measurements of distances between two-color labeled kinetochore protein populations in human [28] and Drosophila [29] cells demonstrated that the distance between fluorescent centroids (delta) changes as a result of attachment to dynamic microtubules. Further, outer kinetochore protein centroids are displaced inward toward the centromere upon treatment with Taxol [25]. These data imply that certain components of kinetochores can be stretched. Studies seeking to examine changes within kinetochores will benefit greatly from super resolution techniques which now make it possible to visualize shape and subdomains of labeled kinetochore proteins (Fig. 4). How the shapes vary between protein populations and across time will be crucial to understanding the complexity of kinetochore structure (Fig. 4E) and the response of kinetochores to mechanical force.
As a significant step in this direction, Suzuki and colleagues used immuno-EM to track the redistribution of inner kinetochore proteins CENP-A, CENP-C, CENP-R, and CENP-T from a rectangular to ellipsoid shape upon microtubule attachment in chicken DT40 cells [30]. Such a transition could shift the inner fluorescence centroid and increase delta measured by LM, but direct LM/EM correlation of the same kinetochores will be needed to firmly establish the relationship between these phenomena. Interestingly, this same study finds that the rectangular shape of gold labeling of outer plate components Ndc80, Mis12, and CENP-E does not change, despite the fact that large scale rearrangements in the outer kinetochore occur have been reported upon microtubule attachment or suppression of plus end dynamics [6;25]. Thus, it is likely that stretch arises from a combination of elastic elements throughout the kinetochore.
Atomic force microscopy of the reconstituted CENP-T-W complex suggest that these inner kinetochore components could account for the bulk of kinetochore stretch observed by LM [30]. The images showed that CENP-T possesses a long flexible element that enables the separation between N and C-termini to vary from almost 0 nm, to 90 nm when tension is applied. Two complexes within the KMN network at the microtubule binding site also have the potential for flexibility. As discussed above, Mis12C forms a straight 21–23 nm rod based on its hydrodynamic properties and appearance in negative stain [20]. This elongated conformation is likely to represent the structure in Taxol-treated cells based on the fact that SHREC mapping of kinetochore architecture found the length of the complex to be 9 nm in untreated cells and 19 nm in the presence of the drug [25]. This 10 nm of flexibility alone cannot explain stretch detected by LM, which is an order of magnitude larger in human kinetochores. Another possible candidate is the Ndc80 complex, which either has a straight, 57 nm long rod shape, or a bent conformation arising from a kink in the coiled-coil region of the Ndc80 subunit. The resulting kink shortens the complexes’ length by ~15% in negatively stained EM images [11].
While SHREC has been extremely valuable in identifying the phenomena of kinetochore stretch, this approach is limited to detection of relative distances. It cannot distinguish between stretching/folding of molecular complexes vs. reorientation of ensembles within the kinetochore architecture. Therefore, solving the mystery of kinetochore compliance will require integrating data from structural studies and live cell imaging across resolution scales.
Flexibility of kinetochore-spindle interactions
The outer kinetochore is an irregular fibrous mat that appears to function like spider web attaching to the walls of any microtubules in the vicinity, including those that end in a different kinetochore [6]. Hence kinetochores possess the flexibility to interact with both the plus end and the lateral surface of microtubules. Functionally, gliding of kinetochores along the sides of single [31] or bundled microtubules [32] powers chromosome movement to the poles and equator, respectively.
In human cells lateral interactions can support spindle assembly and chromosome congression in the absence of plus-end attachments as shown by simultaneously knocking down the kinesin 14 family member HSET and the Ndc80 complex component Nuf2 [33]. The key to overcoming lack of end-on attachments is CENP-E motor activity to drive congression using lateral interactions. While this study showed that such attachments are sufficient to support spindle assembly in human cells under perturbed conditions, determining the importance of lateral attachments during normal mitosis required technical development to track kinetochores and the spindle poles in 3D throughout mitosis [34] or meiosis [35]. Tracking measurements clearly show that upon initial encounter with microtubules most chromosomes move toward a position approximately equidistant between the two centrosomes, rather than moving toward a pole. This results in a pronounced chromosome ring at the equator in both human somatic cells [34] and mouse oocytes [35], suggesting it is a conserved intermediate stage that facilitates spindle assembly and proper chromosome segregation. The ring stage is characterized by dramatic rotations of the kinetochore-kinetochore axis and frequent loss of inter-kinetochore stretch that are inconsistent with stable end-on attachment of both sisters to oppositely oriented spindle poles. EM images confirm that lateral interactions predominate during the early stages of mitosis. The evidence suggests that many chromosomes initially use labile lateral interactions that are gradually converted to stable end-on attachments at the equator. Yet, some of these fully congressed chromosomes do not possess amphitelic attachment in human cells [34], suggesting that the flexibility to modulate kinetochore-microtubule interaction is maintained much later into mitosis than was previously thought.
Conclusions
Owing to complete genome sequencing and large scale gene inactivation studies in model organisms the list of principal kinetochore components is largely complete. It has become possible to start fitting these molecules into the kinetochore structure revealed by EM and in some cases understanding interactions at the atomic level. At the same time, novel LM techniques reveal that kinetochore structure offers a great deal of flexibility and adaptability. The distribution of individual molecular components within the kinetochore changes rapidly in response to various types of microtubule attachments. The next big challenge will be to correlate these redistributions with changes in the orientation of individual complexes that can only detected in EM. The key to achieving this goal is likely in combining various types of microscopy on a single kinetochore. Correlative LM/EM studies will be needed to uncover the exact sources of compliance within kinetochores and reveal the details of how chromosome interactions with the spindle are fine tuned.
Footnotes
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