The crystal structure of the minus-end-directed microtubule motor protein ncd reveals variable dimer conformations

BACKGROUND: The kinesin superfamily of microtubule-associated motor proteins are important for intracellular transport and for cell division in eukaryotes. Conventional kinesins have the motor domain at the N terminus of the heavy chain and move towards the plus end of microtubules. The ncd protein is necessary for chromosome segregation in meiosis. It belongs to a subfamily of kinesins that have the motor domain at the C terminus and move towards the minus end of microtubules. RESULTS: The crystal structure of dimeric ncd has been obtained at 2.9 A resolution from crystals with the C222(1) space group, with two independent dimers per asymmetric unit. The motor domains in these dimers are not related by crystallographic symmetry and the two ncd dimers have significantly different conformations. An alpha-helical coiled coil connects, and interacts with, the motor domains. CONCLUSIONS: The ncd protein has a very compact structure, largely due to extended interactions of the coiled coil with the head domains. Despite this, we find that the overall conformation of the ncd dimer can be rotated by as much as 10 degrees away from that of the twofold-symmetric archetypal ncd. The crystal structures of conventional kinesin and of ncd suggest a structural rationale for the reversal of the direction of movement in chimeric kinesins.     

The shapes of the motor domains of two oppositely directed microtubule motors, ncd and kinesin: a neutron scattering study.

The shapes of the motor domains of kinesin and ncd, which move in opposite directions along microtubules, have been investigated. Using proteins expressed in Escherichia coli, it was found that at high salt (> 200 mM) Drosophila ncd motor domain (R335-K700) and human kinesin motor domain (M1-E349) were both sufficiently monomeric to allow an accurate determination of their radii of gyration (Rg) and their molecular weights. The measured Rg values of the ncd and kinesin motor domains in D2O were 2.06 +/- 0.06 and 2.05 +/- 0.04 nm, respectively, and the molecular weights were consistent with those computed from the amino acid compositions. Fitting of the scattering curves to approximately 3.5 nm resolution showed that the ncd and kinesin motor domains can be described adequately by triaxial ellipsoids having half-axes of 1.42 +/- 0.38, 2.24 +/- 0.44, and 3.65 +/- 0.22 nm, and half-axes of 1.52 +/- 0.23, 2.00 +/- 0.25, and 3.73 +/- 0.10 nm, respectively. Both motor domains are described adequately as somewhat flattened prolate ellipsoids with a maximum dimension of approximately 7.5 nm. Thus, it appears that the overall shapes of these motor domains are not the major determinants of the directionality of their movement along microtubules.     

A new look at the microtubule binding patterns of dimeric kinesins

The interactions of monomeric and dimeric kinesin and ncd constructs with microtubules have been investigated using cryo-electron microscopy (cryo-EM) and several biochemical methods. There is a good consensus on the structure of dimeric ncd when bound to a tubulin dimer showing one head attached directly to tubulin, and the second head tethered to the first. However, the 3D maps of dimeric kinesin motor domains are still quite controversial and leave room for different interpretations. Here we reinvestigated the microtubule binding patterns of dimeric kinesins by cryo-EM and digital 3D reconstruction under different nucleotide conditions and different motor:tubulin ratios, and determined the molecular mass of motor-tubulin complexes by STEM. Both methods revealed complementary results. We found that the ratio of bound kinesin motor-heads to alphabeta-tubulin dimers was never reaching above 1.5 irrespective of the initial mixing ratios. It appears that each kinesin dimer occupies two microtubule-binding sites, provided that there is a free one nearby. Thus the appearances of different image reconstructions can be explained by non-specific excess binding of motor heads. Consequently, the use of different apparent density distributions for docking the X-ray structures onto the microtubule surface leads to different and mutually exclusive models. We propose that in conditions of stoichiometric binding the two heads of a kinesin dimer separate and bind to different tubulin subunits. This is in contrast to ncd where the two heads remain tightly attached on the microtubule surface. Using dimeric kinesin molecules crosslinked in their neck domain we also found that they stabilize protofilaments axially, but not laterally, which is a strong indication that the two heads of the dimers bind along one protofilament, rather than laterally bridging two protofilaments. A molecular walking model based on these results summarizes our conclusions and illustrates the implications of symmetry for such models.     

Conformations of kinesin: solution vs. crystal structures and interactions with microtubules

Recently, the molecular structures of monomeric and dimeric kinesin constructs in complex with ADP have been determined by X-ray crystallography (Kull et al. 1996; Kozielski et al. 1997 a; Sack et al. 1997). The “motor” or “head” domains have almost identical conformations in the known crystal structures, yet the kinesin dimer is asymmetric: the orientation of the two heads relative to the coiled-coil formed by their neck regions is different. We used small angle solution scattering of kinesin constructs and microtubules decorated with kinesin in order to find out whether these crystal structures are of relevance for kinesin's structure under natural conditions and for its interaction with microtubules. Our preliminary results indicate that the crystal structures of monomeric and dimeric kinesin are similar to their structures in solution, though in solution the center-of-mass distance between the motor domains of the dimer could be slightly greater. The crystal structure of dimeric kinesin can be interpreted as representing two equivalent conformations. Transitions between these or very similar conformational states may occur in solution. Binding of kinesin to microtubules has conformational effects on both, the kinesin and the microtubule. Solution scattering of kinesin decorated microtubules reveals a peak in intensity that is characteristic for the B-surface lattice and that can be used to monitor the axial repeat of the microtubules under various conditions. In decoration experiments, dimeric kinesin dissociates, at least partly, leading to a stoichiometry of 1:1 (one kinesin head per tubulin dimer; Thormählen et al. 1998 a) in contrast to the stoichiometry of 2:1 reported for dimeric ncd. This discrepancy is possibly due to the effect of steric hindrance between kinesin dimers on adjacent binding sites.     

The kinesin-like ncd protein of Drosophila is a minus end-directed microtubule motor

The Drosophila ncd gene is required for chromosome segregation during female meiosis. Previous analyses suggested that the ncd gene encoded a protein with sequence similarity to the kinesin motor domain, which suggested that, like kinesin, the ncd protein might be a plus end-directed microtubule motor. Here we describe the expression of ncd protein in E. coli and the initial characterization of the ncd protein's motor properties. The ncd protein is indeed a microtubule motor, but the polarity of movement is minus end directed. The ncd protein also has microtubule bundling activity. These findings limit possible models for the in vivo functions of the ncd protein and suggest that motor proteins with similar sequence can generate movement in opposite directions along a microtubule.     

3D electron microscopy of the interaction of kinesin with tubulin

We have studied the structure of microtubules decorated with kinesin motor domains in different nucleotide states by 3D electron microscopy. Having docked the atomic coordinates of both dimeric ADP.kinesin and tubulin heterodimer into a map of kinesin dimers bound to microtubules in the presence of ADP, we try to predict which regions of the proteins interact in the weakly binding state. When either the presence of 5'-adenylyimidodiphosphate (AMP-PNP) or an absence of nucleotides puts motor domains into a strongly-bound state, the 3D maps show changes in the motor domains which modify their interaction with beta-tubulin. The maps also show differences in beta-tubulin conformation compared with undecorated microtubules or those decorated with weakly-bound motors. Strongly-bound ncd appears to produce an identical change.     

Conformation of the Drosophila motor protein non-claret disjunctional in solution from X-ray and neutron scattering

The quaternary structures of monomeric and dimeric Drosophila non-claret disjunctional (ncd) constructs were investigated using synchrotron x-ray and neutron solution scattering, and their low resolution shapes were restored ab initio from the scattering data. The experimental curves were further compared with those computed from crystallographic models of one monomeric and three available dimeric ncd structures in the microtubule-independent ADP-bound state. These comparisons indicate that accounting for the missing parts in the crystal structures for all these constructs is indispensable to obtain reasonable fits to the scattering patterns. A ncd construct (MC6) lacking the coiled-coil region is monomeric in solution, but the calculated scattering from the crystallographic monomer yields a poor fit to the data. A tentative configuration of the missing C-terminal residues in the form of an antiparallel beta-sheet was found that significantly improves the fit. The atomic model of a short dimeric ncd construct (MC5) without 2-fold symmetry is found to fit the data better than the symmetric models. Addition of the C-terminal residues to both head domains gives an excellent fit to the x-ray and neutron experimental data, although the orientation of the beta-sheet differs from that of the monomer. The solution structure of the long ncd construct (MC1) including complete N-terminal coiled-coil and motor domains is modeled by adding a straight coiled-coil section to the model of MC5.     

Kinesins and microtubules: their structures and motor mechanisms

Atomic resolution three-dimensional structures of two oppositely directed kinesin motors - conventional kinesin and non-claret disjunctional (ncd) protein - are now available in their functional dimeric form. A detailed model of the microtubule has also been recently obtained by docking the 3.7 A structure of tubulin into a 20 A map of the microtubule. Recent structural studies of kinesin motors and their microtubule tracks are contributing to our current understanding of kinesin motor mechanisms.     

Coiled coil in the stalk region of ncd motor protein is nonlocally sustained

The dimeric structure of kinesin superfamily proteins plays an important role in their motile functions and characteristics. In this study, the coiled-coil-forming property of the stalk region (192-346) of Drosophila ncd, a C-terminal kinesin motor protein, was investigated by synthesizing various peptide fragments. The alpha helicity of a set of 46-residue peptides spanning the stalk region appeared too low to form a coiled-coil dimer, probably because of insufficient continuity of the hydrophobic residues at (a and d) core positions in amphipathic heptad repeats. On the other hand, several peptides with leucine residues introduced at core positions or with extensional sequences with high alpha helicity had an advantage in coiled-coil formation. When we analyzed the thermal and urea-induced unfolding of these dimeric peptides, we identified four domains having a relatively high potential to form coiled coils. Among them, three domains on the C-terminal side of the stalk region, i.e., (252-272), (276-330), and (336-346), were in the same heptad frame, although these potential coiled-coil domains were not self-sustaining individually. This is in sharp contrast to the fragment of human kinesin, (332-369), which has an extremely high tendency toward coiled-coil formation. One of the possible triggers for coiled-coil formation of the ncd stalk region may be the interaction between the motor domain and the C-terminal part of the stalk as previously revealed by X-ray crystallography. The residues, S331 and R335, seem to act as a breaking point for alpha-helix continuity. This would make the region (336-346), as the head-stalk joint, more flexible such as seen with a plus-end-directed kinesin, if this region had no interaction with the motor domain. These characteristic differences between ncd and kinesin suggest that the nonlocally sustained coiled coil of ncd is one of the factors important for minus-end-directed motility.     

The molecular structure of adrenal medulla kinesin

The molecular structure of bovine adrenal kinesin was studied by electron microscopy using the low-angle rotary shadowing technique. Adrenal kinesin exhibited either a folded or an extended configuration; the ratio of the two is dependent on the salt concentration. Almost all adrenal kinesin molecules were folded in a low-ionic solution, and the ratio of extended molecules increased to 40-50% in a solution containing 1 M ammonium acetate. Kinesin in the extended configuration displayed a rod-shaped structure with a mean length of about 80 nm. The morphologies of the ends were different; one end was composed of two globular particles, similar to the two-headed structure of myosin, while the other end had a more ill-defined structure, appearing either as a globular particle, an aggregate of two to four small granules, or a frayed, fan-like structure. The folded kinesin molecule possessed a hinge region in the middle of the rod, at about 32 nm from the neck of the two heads. In our preparations, the majority of adrenal kinesin molecules were folded at physiological salt concentrations. Adrenal kinesin bound to microtubules in the presence of adenylyl imidodiphosphate (AMP-PNP) also displayed a folded morphology.     

subito encodes a kinesin-like protein required for meiotic spindle pole formation in Drosophila melanogaster

The female meiotic spindle lacks a centrosome or microtubule-organizing center in many organisms. During cell division, these spindles are organized by the chromosomes and microtubule-associated proteins. Previous studies in Drosophila melanogaster implicated at least one kinesin motor protein, NCD, in tapering the microtubules into a bipolar spindle. We have identified a second Drosophila kinesin-like protein, SUB, that is required for meiotic spindle function. At meiosis I in males and females, sub mutations affect only the segregation of homologous chromosomes. In female meiosis, sub mutations have a similar phenotype to ncd; even though chromosomes are joined by chiasmata they fail to segregate at meiosis I. Cytological analyses have revealed that sub is required for bipolar spindle formation. In sub mutations, we observed spindles that were unipolar, multipolar, or frayed with no defined poles. On the basis of these phenotypes and the observation that sub mutations genetically interact with ncd, we propose that SUB is one member of a group of microtubule-associated proteins required for bipolar spindle assembly in the absence of the centrosomes. sub is also required for the early embryonic divisions but is otherwise dispensable for most mitotic divisions.     

Synthesis and conformational characterization of peptides related to the neck domain of a fungal kinesin.

The Y362K mutation in the neck domain of conventional kinesin from Neurospora crassa provokes a significant reduction of the rate of movement along microtubules. Since the alpha-helical coiled-coil structure of the neck region is implicated in the mechanism of the processive movement of kinesins, a series of peptides related to the heptad region 338-379 of the wild-type and the variant fungal kinesinswere synthesized as monomers and as N-terminal disulfide dimers, crosslinked to favour self-association into coiled-coil structures entropically. A comparison of the dichroic properties of the peptides and the effects of trifluoroethanol and peptide concentration clearly confirmed the strong implication of the single point mutation in destabilizing the intrinsic propensity of the peptides to fold into the supercoiled conformation. That there is a correlation between the stability of the coiled-coil and rate of movement of the kinesin is confirmed.     

Microscopic evidence for a minus-end-directed power stroke in the kinesin motor ncd

We used cryo-electron microscopy and image reconstruction to investigate the structure and microtubule-binding configurations of dimeric non-claret disjunctional (ncd) motor domains under various nucleotide conditions, and applied molecular docking using ncd's dimeric X-ray structure to generate a mechanistic model for force transduction. To visualize the alpha-helical coiled-coil neck better, we engineered an SH3 domain to the N-terminal end of our ncd construct (296-700). Ncd exhibits strikingly different nucleotide-dependent three-dimensional conformations and microtubule-binding patterns from those of conventional kinesin. In the absence of nucleotide, the neck adapts a configuration close to that found in the X-ray structure with stable interactions between the neck and motor core domain. Minus-end-directed movement is based mainly on two key events: (i) the stable neck-core interactions in ncd generate a binding geometry between motor and microtubule which places the motor ahead of its cargo in the minus-end direction; and (ii) after the uptake of ATP, the two heads rearrange their position relative to each other in a way that promotes a swing of the neck in the minus-end direction.     

Searching for kinesin's mechanical amplifier

Kinesin, a microtubule-based motor, and myosin, an actin-based motor, share a similar core structure, indicating that they arose from a common ancestor. However, kinesin lacks the long lever-arm domain that is believed to drive the myosin power stroke. Here, we present evidence that a much smaller region of ca. 10-40 amino acids serves as a mechanical element for kinesin motor proteins. These 'neck regions' are class conserved and have distinct structures in plus-end and minus-end-directed kinesin motors. Mutagenesis studies also indicate that the neck regions are involved in coupling ATP hydrolysis and energy into directional motion along the microtubule. We suggest that the kinesin necks drive motion by undergoing a conformational change in which they detach and re-dock onto the catalytic core during the ATPase cycle. Thus, kinesin and myosin have evolved unique mechanical elements that amplify small, nucleotide-dependent conformational changes that occur in their similar catalytic cores.     

Nucleotide-dependent movements of the kinesin motor domain predicted by simulated annealing.

The structure of an ATP-bound kinesin motor domain is predicted and conformational differences relative to the known ADP-bound form of the protein are identified. The differences should be attributed to force-producing ATP hydrolysis. Candidate ATP-kinesin structures were obtained by simulated annealing, by placement of the ATP gamma-phosphate in the crystal structure of ADP-kinesin, and by interatomic distance constraints. The choice of such constraints was based on mutagenesis experiments, which identified Gly-234 as one of the gamma-phosphate sensing residues, as well as on structural comparison of kinesin with the homologous nonclaret disjunctional (ncd) motor and with G-proteins. The prediction of nucleotide-dependent conformational differences reveals an allosteric coupling between the nucleotide pocket and the microtubule binding site of kinesin. Interactions of ATP with Gly-234 and Ser-202 trigger structural changes in the motor domain, the nucleotide acting as an allosteric modifier of kinesin's microtubule-binding state. We suggest that in the presence of ATP kinesin's putative microtubule binding regions L8, L12, L11, alpha4, alpha5, and alpha6 form a face complementary in shape to the microtubule surface; in the presence of ADP, the microtubule binding face adopts a more convex shape relative to the ATP-bound form, reducing kinesin's affinity to the microtubule.     

A structural analysis of the interaction between ncd tail and tubulin protofilaments

ncd is a minus-end directed, kinesin-like motor, which binds to microtubules with its motor domain and its cargo domain as well. Typical of retrograde motors, the motor domain of ncd locates to the C-terminal end of the polypeptide chain, and hence, the cargo domain constitutes the N-terminal region. To date, several studies have investigated the interaction properties of the motor domain with microtubules, but very few structural data are available about the tail itself or its interaction with microtubules as cargo. Here, we applied cryo-electron microscopy and helical 3D image reconstruction to 15 protofilament microtubules decorated with an ncd tail fragment (N-terminal residues 83-187, named NT6). In our study, the ncd tail shows a behaviour resembling filamentous MAPs such as tau protein, exhibiting a highly flexible structure with no large globular domains. NT6 binds to four different sites on the outer side of microtubules within the proximity of the kinesin motor-binding site. Two of these sites locate within the groove between two neighbouring protofilaments, and appear as strong binding sites, while the other two sites, located at the outer rim, appear to play a secondary role. In addition, the ncd tail fragment induces the formation of large protofilament sheets, suggesting a tail-induced modification of lateral protofilament contacts.     

Congruent Docking of Dimeric Kinesin and ncd into Three-dimensional Electron Cryomicroscopy Maps of Microtubule–Motor ADP Complexes

We present a new map showing dimeric kinesin bound to microtubules in the presence of ADP that was obtained by electron cryomicroscopy and image reconstruction. The directly bound monomer (first head) shows a different conformation from one in the more tightly bound empty state. This change in the first head is amplified as a movement of the second (tethered) head, which tilts upward. The atomic coordinates of kinesin.ADP dock into our map so that the tethered head associates with the bound head as in the kinesin dimer structure seen by x-ray crystallography. The new docking orientation avoids problems associated with previous predictions; it puts residues implicated by proteolysis-protection and mutagenesis studies near the microtubule but does not lead to steric interference between the coiled-coil tail and the microtubule surface. The observed conformational changes in the tightly bound states would probably bring some important residues closer to tubulin. As expected from the homology with kinesin, the atomic coordinates of nonclaret disjunctional protein (ncd).ADP dock in the same orientation into the attached head in a map of microtubules decorated with dimeric ncd.ADP. Our results support the idea that the observed direct interaction between the two heads is important at some stages of the mechanism by which kinesin moves processively along microtubules.     

X-ray scattering by single-headed heavy meromyosin. Cleavage of the myosin head from the rod does not change its shape

Low angle X-ray scattering from heavy meromyosin (HMM) and from single-headed heavy meromyosin (sHMM) have been examined to determine if the heads of myosin change shape when cleaved from the rod to form subfragment 1 (S1). The scattering intensities of intact HMM and sHMM were compared with those of their chymotryptic digestion products, S1 and subfragment 2 (S2). As the data with HMM were complicated by scattering between the two heads, the more extensive analysis was done with sHMM. Pseudo-Guinier plots of intact and digested sHMM, over the angular range used previously for S1, were linear and showed a difference in apparent radius of gyration (Rg) of only 0.07 +/- 0.04 nm. The absolute apparent Rg value of sHMM was 3.2 +/- 0.2 nm, which is comparable to the radius of gyration reported previously for S1 alone. A plot of the fractional differences in scattering intensities of intact and digested sHMM was flat to a reciprocal spacing of at least 1/3.5 nm-1. These results indicate that the head portions of sHMM and S1 have very similar structures at low resolution. Scattering curves for various models of sHMM and mixtures of S1 and S2 were calculated and the fractional difference plots of scattering intensities were made to determine how sensitive this type of analysis is to changes in the shape of the head. Changes in Rg of 0.1 nm or greater gave detectably non-flat difference plots. Thus, the X-ray scattering of sHMM (and HMM) demonstrated that differences in structure between the head of myosin and isolated S1 are likely to be small. Current controversies over myosin head structure are discussed in light of this result.     

The overall conformation of conventional kinesins studied by small angle X-ray and neutron scattering

The quaternary structures of several monomeric and dimeric kinesin constructs from Homo sapiens and Drosophila melanogaster were analyzed using small angle x-ray and neutron scattering. The experimental scattering curves of these proteins were compared with simulated scattering curves calculated from available crystallographic coordinates. These comparisons indicate that the overall conformations of the solution structures of D. melanogaster and H. sapiens kinesin heavy chain dimers are compatible with the crystal structure of dimeric kinesin from Rattus norvegicus. This suggests that the unusual asymmetric conformation of dimeric kinesin in the microtubule-independent ADP state is likely to be a general feature of the kinesin heavy chain subfamily. An intermediate length Drosophila construct (365 residues) is mostly monomeric at low protein concentration whereas at higher concentrations it is dimeric with a tendency to form higher oligomers.     

Human kinetochore-associated kinesin CENP-E visualized at 17 A resolution bound to microtubules

The highly dynamic process of cell division is effected, in part, by molecular motors that generate the forces necessary for its enactment. Several members of the kinesin superfamily of motor proteins are implicated in mitosis, such as CENP-E, which plays essential roles in cell division, including association with the kinetochore to stabilize attachment of chromosomes to microtubules prior to and during their separation. Neither the functional assembly state of CENP-E nor its direction of motion along the polar microtubule are certain. To determine the mode of interaction between CENP-E and microtubules, we have used cryo-electron microscopy to visualize CENP-E motor domains complexed with microtubules and calculated a density map of the complex to 17 A resolution by combining helical and single-particle reconstruction methods. The interface between the motor domain and microtubules was modeled by docking atomic-resolution models of the subunits into the cryoEM density map. Our results support a plus end motion for CENP-E, consistent with features of the crystallographic structure. Despite considerable functional differences from the monomeric transporter kinesin KIF1A and the oppositely directed ncd kinesin, CENP-E appears to share many features of the intermolecular interactions, suggesting that differences in motor function are governed by small variations in the loops at the microtubule interface.