Controlling Kinesin by Reversible Disulfide Cross-linking: Identifying - 《cell》细胞杂志干细胞之家

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发表于 2009-3-5 23:03 |只看该作者 |倒序浏览 |打印

a The Howard Hughes Medical Institute and the Department of Cellular and Molecular Pharmacology, University of California, San Francisco, California 941433 ^: h" X/ v+ W8 `" C
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Correspondence to: Ronald D. Vale, Department of Cellular and Molecular Pharmacology, University of California, San Francisco, 513 Parnassus Ave., San Francisco, CA 94143. Ph.: (415) 476-6380. Fax:(415) 502-1391

Abstract* n6 B5 d# R: F) f0 m" `
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Conventional kinesin, a dimeric molecular motor, uses ATP-dependent conformational changes to move unidirectionally along a row of tubulin subunits on a microtubule. Two models have been advanced for the major structural change underlying kinesin motility: the first involves an unzippering/zippering of a small peptide (neck linker) from the motor catalytic core and the second proposes an unwinding/rewinding of the adjacent coiled-coil (neck coiled-coil). Here, we have tested these models using disulfide cross-linking of cysteines engineered into recombinant kinesin motors. When the neck linker motion was prevented by cross-linking, kinesin ceased unidirectional movement and only showed brief one-dimensional diffusion along microtubules. Motility fully recovered upon adding reducing agents to reverse the cross-link. When the neck linker motion was partially restrained, single kinesin motors showed biased diffusion towards the microtubule plus end but could not move effectively against a load imposed by an optical trap. Thus, partial movement of the neck linker suffices for directionality but not for normal processivity or force generation. In contrast, preventing neck coiled-coil unwinding by disulfide cross-linking had relatively little effect on motor activity, although the average run length of single kinesin molecules decreased by 30–50%. These studies indicate that conformational changes in the neck linker, not in the neck coiled-coil, drive processive movement by the kinesin motor.9 g( n* A3 \) r7 @" \& p

Key Words: kinesin, processivity, disulfide cross-linking, neck linker, one-dimensional diffusion( h% N5 I  ~0 N# I, ?
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Introduction

Conventional kinesin (herein referred to as kinesin) is a microtubule-based motor protein that is involved in transporting membranous organelles and intermediate filaments within cells (Hirokawa 1998 ; Goldstein and Philp 1999 ). Kinesin, a dimeric protein with two motor heads and a tail domain that docks onto a cargo, is a highly processive motor capable of taking 150 steps of 8-nm length along a microtubule before dissociating (Howard et al. 1989 ; Block et al. 1990 ; Svoboda et al. 1993 ; Hackney 1995 ; Vale et al. 1996 ; Gilbert et al. 1998 ). Processivity is an important biological adaptation that enables one or a relatively small number of kinesin molecules to transport cargo within the cell.
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Understanding the mechanism of kinesin motility has been aided by structural studies of the kinesin motor domain. Three-dimensional crystal structures of kinesin monomers and a short dimer have revealed several domains important for the motor function (Kull et al. 1996 ; Sack et al. 1997 ; Kozielski et al. 1997 ) (see Fig 1 a). The NH2-terminal 320 amino acids (a.a.),1 which are conserved throughout the kinesin superfamily, form a compact globular domain (termed the catalytic core) that contains the microtubule binding and ATP hydrolysis sites. Emerging from the COOH terminus of the catalytic core is the neck region (Vale and Fletterick 1997 ), which consists of two different parts: the 15 a.a. "neck linker" (see Fig 1 a, red), which can interact with the catalytic core, and the subsequent 30 a.a. "neck coiled-coil" (see Fig 1 a, cyan). In the dimeric kinesin crystal structure (Kozielski et al. 1997 ), the catalytic cores cannot both bind simultaneous to two adjacent binding sites on a microtubule protofilaments (separated 8 nm apart). Since a two-head–bound intermediate is thought to be critical for processive motion (Vale and Milligan 2000 ), it is thought that some element in the dimeric kinesin crystal structure must melt during the enzymatic cycle (Block 1998 ). Two theories have been advanced for this conformational change: the first involves an "unzippering" of the neck linker from the catalytic core (Romberg et al. 1998 ) and the second proposes a partial "unwinding" of the neck coiled-coil (Tripet et al. 1997 ; Hoenger et al. 1998 ).
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Figure 1. Constructs for cross-linking of the neck region. (a) Three-dimensional structure of rat kinesin dimer (PDB No. 3KIN ; numbered as in human kinesin). The catalytic core (residues 2–322; gray), the neck linker (residues 323–336; red) and the neck coiled-coil (337–368; cyan) are shown. Positions of the mutations for cross-linking are shown by space filing of C atoms (Ser330Cys/Leu4Cys or Glu334Cys/Lys222Cys for cross-linking of the neck linker and Ala337Cys or Tyr344Cys for cross-linking of the neck coiled-coil). Inset shows a view from the reverse side. Smaller spheres indicate positions of C? atoms. (b) DTNB-induced disulfide cross-linking of neck linker mutants (Cys334/Cys222 and Cys330/Cys4), and (c) neck coiled-coil mutants (Cys344, Cys337, Cys337/Cys344) as analyzed by nonreducing SDS-PAGE. The DTNB concentration in c was 200 μM. Disulfide formation was reversed by subsequent treatment with 5 mM DTT ( DTT, right lane in c). The arrowheads show noncross-linked kinesin and the arrows show intramolecular cross-linked kinesin (b) and intermolecular cross-linked kinesin (c). The intramolecular cross-link for C334/C222 produces an increase in electrophoretic mobility, whereas the C330/C4 cross-link decreases mobility. No higher molecular weight band (i.e., intermolecular cross-linking) was detected for the neck linker mutants (not shown). The band indicated by open arrowhead (c) may represent a modified monomer or a dimer of degradation products.

In favor of the neck linker peeling model, Rice et al. 1999  have detected ATP-dependent conformational change of the neck linker using electron paramagnetic resonance, fluorescence resonance energy transfer, and cryo-EM. The neck linker is docked onto the catalytic core when kinesin is bound to the microtubule and ATP is in the active site, but becomes unzippered in the ADP or nucleotide-free state. These findings, together with cryo-EM work that reveals the docking orientation of kinesin on the microtubule, suggest that the two kinesin heads can span the distance between tubulin binding sites if the neck linker of the rear head is docked and pointing forward and the neck linker on the forward head is detached and pointing backward (Vale and Milligan 2000 ). Further supporting an important role of the neck linker in motility, Case et al. 2000  replaced the neck linker with a random coil structure and found a 450-fold decrease in motor velocity.
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An alternative model proposes that the key structural change in kinesin motility is the unwinding and rewinding of the first half of the neck coiled-coil (Tripet et al. 1997 ; Hoenger et al. 1998 , Hoenger et al. 2000 ; Mandelkow and Johnson 1998 ). In favor of this model is the fact that the first half of the neck coiled-coil (residues 337–353) contains nonideal residues that destabilize the coiled-coil structure, while the latter half of the coiled-coil (354–368) is supported by more stable interactions (Tripet et al. 1997 ; Thormahlen et al. 1998 ). Furthermore, when Hoenger et al. 2000  prevented the unwinding of the neck coiled-coil through an engineered disulfide bridge at the beginning of the structure, they reported a 13-fold increase in Km(MT), which they interpreted as due to a loss in processivity. On the other hand, Romberg et al. 1998  showed that replacing kinesin's native neck coiled-coil with a highly stable artificial coiled-coil did not greatly reduce processivity, suggesting that the neck coiled-coil unwinding is not essential for kinesin motility. However, the interpretation by Romberg et al. was criticized on the basis that a partial unwinding of the coiled-coil may have been still possible in the stable coiled-coil mutant (Mandelkow and Hoenger 1999 ).

To test these two models for kinesin's processivity, we engineered disulfide bridges in the neck linker or the neck coiled-coil to prevent potential conformational changes in these regions. The effect of cross-linking on the motor functions was assayed by ATPase assays, multiple motor motility assays, and single molecular motility assays. Cross-linking of the neck coiled-coil had little effect on kinesin processivity, whereas cross-linking of the neck linker disabled processive movement. Kinesin cross-linked at the middle position of the neck linker showed a small degree of directional motion, suggesting that partial movement of the neck linker is sufficient for directionality but not for processivity. Our results provide functional proof for the model in which dynamic motions of the neck linker, but not the neck coiled-coil, drive kinesin's mechanochemical cycle.; Y6 k; Q3 g5 r6 T  ~

Materials and Methods
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Cloning and Protein Purification7 x: i( Q+ H9 s. C% R, q7 C
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As a template for mutagenesis, we used a human 560–amino acid kinesin whose solvent exposed cysteines were mutated to Ser/Ala (C7S/C65A/C168A/C174S/C294A/C330S/C421A) (Rice et al. 1999 ); fused COOH-terminal to this "Cys-light K560" was the green fluorescent protein (GFP; Phe64Leu/Ser65Thr variant) followed by a six-histidine tag. For making a monomeric construct, we used a 339–amino acid Cys-light kinesin fused to GFP. Ideal locations for introducing cysteines for disulfide bond formation were determined using the program SSBOND (Hazes and Dijkstra 1988 ). Cysteines were introduced into these constructs using a protocol involving QuickChange mutagenesis (Stratagene) followed by subsequent subcloning in a pET17b vector (Novagen, Inc.), as previously described (Case et al. 1997 ). The sequences of all constructs were verified. Escherichia coli BL21 (DE3) was transformed with the expression plasmid construct, and protein expression was induced as described previously (Case et al. 1997 ; Romberg et al. 1998 ), except that cells were collected and lysed at pH 6.0 to prevent disulfide cross-linking and the pH of supernatants was raised to 8.0 just before binding to Ni-NTA resin. Kinesin proteins were purified by Ni-NTA chromatography (QIAGEN) followed by HiTrap-Q ion exchange chromatography (Amersham Pharmacia Biotech) as described (Case et al. 1997 ; Romberg et al. 1998 ). To remove inactive motor proteins, kinesin was finally purified by microtubule affinity (Case et al. 1997 ). In brief, proteins were incubated with 1.5 mg/ml taxol-stabilized microtubules and 1 mM AMPPNP and centrifuged over a glycerol cushion (200,000 g for 10 min). Active kinesin motors were released from the microtubule in 12 mM Pipes buffer (pH 6.8) containing 200 mM KCl, 5 mM ATP, 5 mM MgCl2, 2 mM EGTA, and 20 μM taxol. DTT in the protein solution also was removed in this step. Immediately after microtubule affinity purification, motors were assayed or were frozen with 10% sucrose added and stored in liquid nitrogen. Protein concentration was quantitated using SDS-PAGE as described previously (Woehlke et al. 1997 ).
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Chemical Cross-linking

Thiol-specific reagents were obtained from Sigma-Aldrich (5,5'-dithiobis-(2-nitrobenzoic acid) , DTT, N-ethylmaleimide ; N,N'-1,2-phenylenedimaleimide ; N,N'-1,4-phenylenedimaleimide ). DTNB was dissolved in DMSO at 100 mM concentration, oPDM and pPDM were dissolved in acetonitrile at 10 mM concentration and the solutions were stored at 4°C. DTT and NEM solutions were prepared freshly by dissolving in assay buffers. Assay buffers used were either BRB12 (12 mM Pipes , 2 mM MgCl2, 1 mM EGTA; for ATPase assay and single molecule motility assay) or BRB80 (80 mM Pipes , 2 mM MgCl2, 1 mM EGTA; for multiple motor assay and optical trapping bead assay). Disulfide bonds were reversibly formed by oxidation using DTNB. Bifunctional thiol reagents oPDM and pPDM were used to cross-link two thiols with different lengths, and the monofunctional thiol reagent NEM was used for monovalent modification of a thiol. Reactions were carried out by adding 200 μM thiol-specific reagents (DTNB, oPDM, pPDM, or NEM) to 0.5–1 μM kinesin and incubation at 4°C overnight. Control reactions were carried out in parallel by adding equal amount of buffer (for Cys337, Cys344, and Cys337/Cys344 constructs) or 1 mM DTT (for Cys330/Cys4 and Cys334/Cys222 constructs). Unreacted oPDM or pPDM were quenched by the addition of 10 mM 2-mercaptoethanol. Unreacted NEM was quenched by the addition of 5 mM DTT for the ATPase assay; otherwise it was diluted or removed using a flow cell for the motility assays. For a control, disulfide-bond formation was reversed by incubation of DTNB-treated motor with 5 mM DTT at 4°C for more than 3 h. Disulfide or chemical cross-linking was verified by adding SDS sample buffer without reducing reagents followed by SDS-PAGE (4–12% polyacrylamide) and Coomassie blue staining.

ATPase and Microtubule-gliding Assays: [3 x0 R% U3 ^& R
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Microtubule-stimulated ATPase activities were measured using a spectrophotometer with a coupled enzymatic assay as described (Woehlke et al. 1997 ) except that DTT was not added. Reactions contained 40–100 nM kinesin, varying concentrations of microtubules (0–12 μM for dimeric and 0–40 μM for monomeric constructs), and 1 mM MgATP in BRB12 buffer. Multiple motor motility assays were performed using rhodamine-labeled microtubules and fluorescence microscopy in flow cells as described (Woehlke et al. 1997 ) except that 2-mercaptoethanol was not added to the assay buffer. Anti-GFP antibodies were used to bind and orient the motor on the surface of the coverslip. The gliding velocity of microtubules over the motors was measured based on the distance travelled during 30–60 s.

Single Motor Motility Assays
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Individual GFP-kinesin fusion molecules moving along sea urchin sperm flagellar axonemes were visualized in a custom-built total internal reflection fluorescence microscope as described previously (Pierce and Vale 1998 , Pierce and Vale 1999 ; Romberg et al. 1998 ). The assay solution contained 1 nM kinesin-GFP, 2.5 mg/ml casein, an oxygen scavenging system (without 2-mercaptoethanol) (Pierce and Vale 1998 ), 1 mM MgATP, and Cy5-labeled axonemes in BRB12 buffer. GFP molecules were illuminated with an argon laser (488 nm) at 5 mW. The fluorescent images of both axonemes and GFP molecules were recorded onto a S-VHS tape after four-frame averaging. The images were digitized (10 or 15 frames/s) and analyzed on a computer using custom macros in the program NIH image. The observed run lengths, velocities, and association times of moving fluorescent spots along axonemes were measured as described (Romberg et al. 1998 ; Shimizu et al. 2000 ). The distributions of run length and association time were fitted with exponential curves (C﹞exp, where  is the average run length) (Romberg et al. 1998 ), except for the distributions of run length of DTNB-treated Cys330/Cys4 and Cys334/Cys222 that were fitted based on Gaussian distributions (C﹞exp, where xd is the average net displacement toward plus end). Positions of the fluorescent spot undergoing Brownian diffusion were determined using a macro program provided by Dr. Y. Inoue (University of Tokyo, Tokyo, Japan). The accuracy of position determination of individual GFP spots was 30 nm, which was estimated as the standard deviation of positions of the spots bound onto axonemes in the presence of 1 mM AMPPNP.
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Optical Trapping Bead Assays

Kinesin-GFP molecules were coupled with latex beads via affinity-purified anti-GFP antibodies. 15 mg of 1-ethyl-3-(3-dimethlaminoprophyl) carbodiimide (EDAC; Molecular Probes) and 15 mg of N-hydroxysulfosuccinimide (Molecular Probes) were added to 50 μl of 1-μm carboxylate-modified latex beads (10% solid; Bangs Laboratories) in 20 mM MES (pH 6.0) containing 100 mM NaCl, and mixed on a shaker for 30 min at room temperature. After four washes by centrifugation and resuspension, the pellet was resuspended in 300 μl of 0.1 M sodium phosphate buffer (pH 7.0) containing 100 μg anti-GFP antibodies and 1 mg/ml BSA. After mixing for 2 h at room temperature, beads were washed four times, and resuspended in 0.1 M sodium phosphate buffer (pH 7.0) containing 0.1% NaN3 and 4 mg/ml BSA, and stored at 4°C. Kinesin-GFP dilution was mixed with the beads for 20 min at 4°C, and further diluted in assay solution containing 1 mM MgATP, 0.5 mg/ml casein, the oxygen scavenging system (without 2-mercaptoethanol) in BRB80 buffer (Coppin et al. 1997 ). Kinesin-coated beads were captured and interacted with rhodamine-labeled sea urchin sperm flagellar axonemes using an optical trap, and the motility of the bead along an axoneme under load was assayed as described previously (Coppin et al. 1997 ). Trap stiffness was calibrated as described (Coppin et al. 1997 ) and was 0.029 pN/nm in these experiments. Trapped beads were brought into contact with an axoneme and held for more than 90 s. When the bead moved, the displacement of the bead was acquired at 2 kHz. Force–velocity curves and dissociation rates were obtained as described previously (Coppin et al. 1997 ), except that they were not corrected for the compliance of the motor–bead linkage, therefore the velocity in the force–velocity curve is slightly underestimated (10%). K560-GFP molecules tended to dissociate from axonemes before reaching a stall plateau, which causes a biased sampling of velocities at high forces. To compensate for this bias, the motors that dropped out were assumed to have zero velocity at higher loads (Coppin et al. 1997 ). This correction significantly shifted the curves to the left (i.e., lower forces). True curves are expected to lie between the corrected and uncorrected curves.
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Online Supplemental Material
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The online version of this article contains QuickTime movies that accompany Fig 3, which better visualize the dramatic changes in the movement of kinesin after neck linker cross-linking. Videos 1 and 2 show the movements of Cys330/Cys4 molecules under reduced and oxidized conditions, respectively. The image of an axoneme is displayed first, followed by the images of single kinesin-GFP molecules moving along axonemes visualized by total internal reflection fluorescence microscope. The times (in seconds) are shown in the upper right of the movies and are 3x real speed. Online supplemental material available at http://www/jcb.org/cgi/content/full/151/5/1081/DC1.( ~+ J: \$ ]" I& v- s/ y
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Figure 2. Effects of neck linker cross-linking on kinesin motility. WT denotes K560 Cys-light kinesin without cysteine introduction. (a) Histograms of microtubule gliding velocities without and with DTNB treatment are shown. Arrowheads indicate mean value (Table 1). (b) Histograms of run lengths of single molecular motility of neck linker cross-linked kinesins along axonemes visualized using total internal reflection fluorescent microscopy. The distributions were fitted with either an exponential curve or a Gaussian curve (see Materials and Methods). Arrowheads indicate the average run length (Table 2). (c) Load-dependent velocity and dissociation rate of WT and Cys330/Cys4 molecules were determined by optical trapping beads assays. (Open circle) Without DTNB; (closed circle) with DTNB; (triangle) with DTNB at 10 times higher motor density (also marked with "M" to differentiate this multiple motor condition from single motor conditions ). Force–velocity curves shown here represent a lower bound for force production (see Materials and Methods).

Figure 3. Diffusional motion of neck linker-cross-linked kinesin molecules. (a) Typical displacement plots for cross-linked Cys334/Cys222 and Cys330/Cys4. Y axis indicates the displacement toward plus end of axonemes. The polarity was determined by the direction of continuous motion of occasional noncross-linked molecules in the preparation. The variation in the position of cross-linked Cys330/Cys4 with the nonhydrolyzable ATP analogue AMPPNP (1 mM) reflects the error in the tracking of single molecules and not actual motion. (b) MSD plots for Cys334/Cys222 with DTNB (red circle), Cys330/Cys4 without DTNB (square), with DTNB (blue circle), with DTNB in the presence of 1 mM AMPPNP (diamond), as shown with two different magnifications in y axis. Lines show theoretical curves. Cys334/Cys222 DTNB was fitted with MSD = 2Dt (D = 2.4 x 10-11 cm2/s), and Cys330/Cys4 and Cys330/Cys4 DTNB were fitted with MSD = 2Dt v2t2 (D = 17 x 10-11 and 2.6 x 10-11 cm2/s and v = 21 and 3.2 μm/min, respectively; diffusion coefficient for Cys330/Cys4 without DTNB is overestimated due to the lack of temporal resolution). See supplemental videos 1 and 2, showing movements of Cys330/Cys4 without and with DTNB.- l; e) W3 g) h3 E

Results' I  z* [6 J5 E0 F) s2 @

Cross-linking of Kinesin's Neck Linker

A 560–amino acid kinesin whose solvent-exposed cysteines were replaced by either Ser or Ala (Rice et al. 1999 ) was used as a template for introducing pairs of cysteine residues for reversible disulfide cross-linking. This "Cys-light K560" protein (also designated "WT" in this paper) exhibited identical ATPase activity and processive motility to K560, but avoided potential deleterious effects associated with oxidation of surface cysteines. The program SSBOND identified only two pairs of residues in the neck linker whose C–C and calculated C?–C? distances are capable of forming energetically favorable disulfide bonds (Fig 1 a): (a) between residue 334 at the end of the neck linker and residue 222 at the tip of the catalytic core; and (b) between residue 330 (located between ?9 and ?10) and residue 4 at the NH2 terminus. A disulfide bond between residues 334 and 222 would be expected to totally immobilize the ATP-dependent neck linker movement, while a disulfide bond between residues 330 and 4 should partially immobilize the neck linker movement.
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Cys334/Cys222 and Cys330/Cys4 constructs were prepared, the expressed proteins were purified from bacteria, and disulfide bond formation after oxidation with DTNB (5,5'-dithio-bis) was examined using SDS-PAGE under non-reducing conditions. Both neck linker mutants displayed small electrophoretic mobility changes after oxidation (Fig 1 b); with intermediate DTNB concentrations, two bands (noncross-linked and cross-linked proteins; arrowheads and arrows in Fig 1 b, respectively) were discernible. The mobility of the WT protein (Cys-light K560) was not affected by the oxidative treatment (Fig 1 c).: S, p& U; e: L  ~

Cys334/Cys222 and Cys330/Cys4 mutants were assayed under reducing and oxidizing conditions for microtubule-stimulated ATPase rates to determine whether neck linker cross-linking affects basic enzymatic functions (Table 1). Under reducing conditions, the kcat for microtubule-stimulated ATPase (13.2 and 19.8 ATP/s per head for Cys334/Cys222 and Cys330/Cys4, respectively) was lower than WT (31.9 ATP/s per head). The Km(MT), however, was within twofold of WT. After oxidative cross-linking, kcat decreased by an additional 50% and the Km(MT) increased by approximately fourfold for both constructs. Addition of the monovalent thiol-reactive reagent NEM, on the other hand, did not affect the ATPase properties of Cys334/Cys222 and Cys330/Cys4. These results indicate that disulfide bond formation in the neck linker, and not cysteine modification per se, affects kinesin's enzymatic activity.
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Table 1. Effect of Neck Cross-linking on ATPase Activity and Microtubule Gliding Velocity
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The almost precise 50% decrease in kcat in both constructs after oxidative cross-linking was striking. One possible explanation was that only one head of the kinesin dimer was enzymatically activated by an encounter with the microtubule, perhaps because the second head was restrained from reaching another tubulin subunit by neck linker cross-linking (see Fig 6b and Fig c). Alternatively, cross-linking could simply cause a twofold decrease in the enzymatic activity of the catalytic core. We tested these possibilities by preparing a Cys-light monomeric kinesin (K339-GFP; Case et al. 2000 ) with cysteines introduced at residues 330 and 4 for neck linker cross-linking. After oxidative cross-linking, the kcat of this neck cross-linked monomer decreased by only 8% (from 27.7 ± 4.0 to 25.6 ± 3.4 ATP/s per head), and the Km(MT) increased only slightly from 10.6 ± 3.9 to 14.2 ± 4.5 μM tubulin. This result suggests that the 50% decrease in kcat of the dimer after cross-linking is not due to an alteration of the catalytic mechanism but due to an inability of both heads to access the microtubule.8 [, f0 X  R* Q2 C. Z5 c1 y
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Figure 4. Effects of neck coiled-coil cross-linking on kinesin motility. (a) Histograms of microtubule gliding velocities without and with DTNB treatment are shown. Arrowheads indicate mean value (Table 1). (b) Histograms of run lengths of single molecule motility of neck coiled-coil cross-linked kinesins along axonemes visualized using total internal reflection fluorescent microscopy. The run lengths were fit with an exponential curve. Arrowheads indicate average run length (Table 2). (c) Load-dependent velocity and dissociation rate of Cys344 and Cys337/344 molecules were determined by optical trapping bead assays. (Open circle) Without DTNB; (closed circle) with DTNB. The increase in dissociation rate of Cys337/344 is statistically significant at lower forces, as tested by t test using dissociation rates obtained from 10 individual beads (P value of 0.018 and 0.015 at 0.75 and 1.25 pN, respectively). The increase in the dissociation rate of Cys344 was small (1.2-fold) and was not statistically significant at any load (P value of >0.3).
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Figure 5. Cross-linking of the neck coiled-coil using long cross-linkers. (a) Structures of the cross-linking agents oPDM and pPDM possessing two maleimide groups that react with thiols. (b) Cross-linking of neck coiled-coil mutants Cys344 and Cys337 using oPDM or pPDM analyzed by SDS-PAGE. Arrowhead and arrow show noncross-linked and cross-linked kinesin, respectively. The concentration of cross-linking agent was 100 μM. (c) Histogram of velocities of Cys337 after cross-linking, analyzed using the single molecule fluorescence motility assays. The arrows denote the mean velocities (19.1 ± 4.4, 19.4 ± 4.4, 19.3 ± 4.4 and 15.3 ± 4.9 μm/min for reduced, with DTNB-, oPDM-, and pPDM-treated, respectively). The shift in the distribution after cross-linking with pPDM most likely reflects the presence of both cross-linked and noncross-linked molecules.6 |1 y3 O  N0 s! F; c, K
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Figure 6. Schematic model showing the effects of neck linker cross-linking on kinesin movement. Two kinesin's catalytic cores are shown in blue and green, and the adjacent neck linker and the neck coiled-coil are shown in black lines. - and ?-tubulin subunits are shown in gray with the flexible COOH terminus region shown by an orange line. T and D denote ATP and ADP, respectively. (a) Model for processive movement of kinesin as described previously (Rice et al. 1999 ; Vale and Milligan 2000 ). Upon binding of ATP to the microtubule-bound head, the neck linker docks onto the catalytic core and moves partner head toward plus end. The forward head searches and binds to a new tubulin-binding site to achieve two-head–bound intermediate. Kinesin can repeat this cycle more than 100 times before detachment from the microtubule. (b) Cross-linking of the neck linker at the middle (Cys330/Cys4) enables directional motion due to a small power stroke but not processive motion. Upon binding of ATP, a part of the neck linker in the microtubule-bound head folds (red arrows). However, the access of the partner head to a tubulin-binding site is inhibited until the bound head detaches. The motor partitions between a weak binding state in which it can diffuse along the microtubule and a strong binding state in which it can undergo a short stroke. (c) Disulfide cross-linking of the neck linker at the tip of the catalytic core (Cys334/Cys222) abolishes motile activity, since the neck linker cannot change position. Weak electrostatic interaction between the COOH terminus of tubulin and the initial portion of the neck coiled-coil allows the molecule to diffuse along the microtubule (see also Thorn et al. 2000 ).5 W  x- c7 R: _9 a& `, E

The effect of neck linker cross-linking on kinesin dimer-induced microtubule gliding (a multiple motor motility assay) was even more dramatic than its effect on enzymatic activity (Fig 2 a and Table 1). In the presence of reduced Cys334/Cys222, virtually all microtubules moved smoothly and unidirectionally. The distribution of velocities was broad and the mean velocity was twofold lower than WT (Fig 2 a). However, under oxidizing conditions, the majority of microtubules were attached to the kinesin-coated surface but showed very slow or undetectable movement (
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To elucidate the effect of neck linker cross-linking on processive movement, single molecule movements were observed using total internal reflection fluorescence microscopy (Vale et al. 1996 ) using GFP-tagged kinesin proteins (Pierce and Vale 1999 ). Under reducing conditions, Cys334/Cys222 and Cys330/Cys4 moved smoothly and unidirectionally and displayed run lengths and velocities similar to WT (Fig 2 b and Table 2) (also see online supplemental movie). After oxidative treatment with DTNB, binding of individual molecules to axonemes were still observed at a similar frequency to that observed under reducing conditions (Table 2), but the molecules dissociated rapidly without displaying unidirectional smooth movements. The association time decreased six- and ninefold for Cys334/Cys222 and Cys330/Cys4 after DTNB treatment, respectively (Table 2). When the oxidized mutants were treated with >10-fold excess of DTT over DTNB, the molecules again showed unidirectional motion along axonemes with similar velocities and run lengths to that before oxidation (Table 2,  DTT). Thus, the inhibition of processive motility was completely reversible. Monovalent modification using NEM did not affect the velocity and run length (Table 2, NEM), indicating that cysteine modification per se does not affect processive motion. These results demonstrate that neck linker cross-linking disables the processive movement of the kinesin dimer.9 {* f" c9 d$ ]* F$ ?
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Table 2. Effect of Neck Cross-linking on Single Molecule Motility- W" q: \& k1 v3 b/ E8 h
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Unexpectedly, oxidized neck linker molecules showed one-dimensional diffusion along the axonemes (see online supplemental movie). Similar random diffusional motion restricted to the longitudinal axes of microtubules was previously described for some molecular motors and postulated to involve a weak interaction between the motor and the microtubule (Vale et al. 1989 ; Okada and Hirokawa 1999 ). Displacements could not be accurately detected for molecules that dissociated within 0.5 s, but were apparent for molecules that remained bound to the axoneme for longer periods of time (Fig 3 a). The net displacements of oxidized Cys334/Cys222 displayed a Gaussian distribution centered on zero (Fig 2 b and Table 2). The mean-square-displacements (MSD; Chandrasekhar 1943 ) also increased linearly with time (Fig 3 b), indicating that the motion of this cross-linked mutant was diffusional (diffusion coefficient of 2.4 x 10-11 cm2/s) and did not contain a directed component. These results cannot be explained by a bidirectional motion with occasional switching of the direction (Endow and Higuchi 2000 ), since the MSD-t plot would deviate from linearity at shorter time scale, which was not observed. In contrast, cross-linked Cys330/Cys4 exhibited a small bias in the diffusional motion towards the microtubule plus end (Fig 3 a), as evidenced by the slight offset in the Gaussian distribution of net displacements (Fig 2 b). Moreover, the MSD plot was nonlinear and was fitted well with a theoretical curve for Brownian diffusion (diffusion coefficient of 2.6 x 10-11 cm2/s) superimposed with directed movement with a velocity of 3.2 μm/min (Fig 3 b). This velocity is similar to that displayed by cross-linked Cys330/Cys4 kinesin in the microtubule gliding assay (Fig 2 a). Since the disulfide bond between residues 330 and 4 should only partially constrain the neck linker, these results suggest that partial movement of neck linker is sufficient for directionality.: A& K9 s$ K% U7 |4 n3 n. r
, R) E5 p/ _' J9 X% P7 N, \1 S9 i. O
Since oxidized Cys330/Cys4 showed some net directed motion, we also investigated whether it has the ability to move processively under the applied load of an optical trap (Svoboda and Block 1994 ; Kojima et al. 1997 ; Coppin et al. 1997 ). Individual beads coated with WT kinesin were captured with an optical trap and brought into contact with an axoneme. The kinesin concentration was adjusted such that only about half of the beads exhibited movement (18 beads moved out of 30 beads tested). Under this condition, >98% of the observed bead movements are expected to be generated by a single kinesin molecule (Svoboda and Block 1994 ). Under reducing conditions, beads coated with Cys330/Cys4 at the same density as WT kinesin showed a similar frequency of movement (14 beads moved out of 30 beads). However, after oxidation, the Cys330/Cys4-coated beads showed hardly any movement (1 out of 40 beads moved and did so with normal velocity. This movement event may have been caused by a noncross-linked motor). Binding events occurred for some beads, as suggested by a decrease in the thermal fluctuations of the beads in the trap (i.e., increase in stiffness due to the formation of the linkage between the bead and the microtubule). When the motor density was increased by 10-fold, movement of beads coated with oxidized Cys330/Cys4 were observed (11 out of 16 beads moved). Even under these multiple motor conditions, the force–velocity curve still was shifted to lower forces and the dissociation rate was increased compared with single molecule conditions of noncross-linked Cys330/Cys4 (Fig 2 c; note that measurements were made with a fixed optical and not a force clamp apparatus; Therefore, the load is continually increasing as the bead moves away from the trap center). These results indicate that the cross-linked Cys330/Cys4 molecule exhibits impaired force production and processivity. In contrast, beads coated with oxidized Cys344/Cys222 did not show any movement even at the 10-fold higher motor density, confirming that oxidized Cys344/Cys222 has no or extremely limited motile activity.2 z. a% |7 }+ r! Y( G+ X2 b$ Z

Cross-linking of the Neck Coiled-Coil2 G, G0 M- ^, R/ j/ ]* [; b! e

To examine the effects of cross-linking of kinesin's neck coiled-coil, we introduced single cysteine residues into the a position of the first two heptad repeats (Fig 1 a). This position is preferred for disulfide bond formation (Zhou et al. 1993 ) and also scored well for bond formation with the SSBOND prediction program. We prepared three constructs by replacing Ala344, Tyr337, or Ala337/Tyr344 (double mutation) with cysteine(s). The residue 337 is the first residue of the neck coiled-coil, and cross-linking at this position should completely inhibit unwinding of this structure. Residue 344 is located at the beginning of the second heptad repeat, and the disulfide bond formation at this position should only allow limited unwinding of the neck coiled-coil.
- ~) @7 h8 Z  C: P
Disulfide bond formation induced by DTNB was evaluated using SDS-PAGE under nonreducing conditions (Fig 1 c). After DTNB treatment, all neck coiled-coil mutants showed a high molecular weight band corresponding approximately in size to a cross-linked kinesin dimer (Fig 1 c). The cross-linking efficiency was higher for Cys344 (65–90%) and Cys337/Cys344 (70–90%) than for Cys337 (55–75%). Subsequent treatment of the oxidized kinesin mutants with excess DTT completely reversed the cross-linking reaction (Fig 1 c). WT was not affected by the oxidative treatment, which certifies that cross-linking requires the introduced mutations.4 p6 H. \* ^8 l) F+ M

The effect of cross-linking within kinesin's neck coiled-coil was examined using the same assays described above for the neck linker mutations. Under reducing conditions, the above mutations did not themselves significantly affect kinesin ATPase activity, multiple motor microtubule gliding velocity, or single molecule velocity and processivity (Table 1 and Table 2). Furthermore, oxidative treatment produced only subtle effects on activity. For the microtubule-stimulated ATPase, the turnover rate was unchanged and the Km(MT) slightly increased (Table 1). However, this increase was also observed for the WT kinesin after oxidation, and thus, the increase in Km(MT) may be caused by an effect of DTNB on the microtubule and not on the kinesin molecule. After DTNB treatment, microtubule gliding velocity decreased slightly (8%, 30%, and 17% for Cys344, Cys337, and Cys337/Cys344, respectively; Fig 4 a and Table 1). These effects are significantly smaller than those observed for neck linker mutants Cys334/Cys222 and Cys330/Cys4 (Fig 2 a and Table 1).

The effect of neck coiled-coil cross-linking on kinesin processivity was examined using single molecule motility assays. For all three neck coiled-coil mutants, the single molecule velocity was unchanged after DTNB-induced oxidation (Table 2). The run lengths, however, decreased slightly (27%, 43%, and 48% for Cys344, Cys337, and Cys337/Cys344, respectively) (Fig 4 b and Table 2). The decreases in run length were completely recovered by subsequent treatments with excess DTT (Table 2,  DTT), indicating that they were caused by cross-linking of the neck coiled-coil. Since the cross-linking was not 100% efficient (Fig 1 c), one concern is that noncross-linked molecules could have been selectively observed in this assay. However, this possibility was excluded by the finding that the movement frequency of all mutants did not change after the DTNB treatment (Table 2). Collectively, these results suggest that cross-linking of neck coiled-coil has minimal effect on motor activity, although it produces a slight decrease in single molecule run length.

To examine force production after neck coiled-coil cross-linking, optical trapping bead assays were performed. Beads coated with Cys337/Cys344 mutants were randomly trapped and attached onto axonemes. The movement frequency of beads did not change after DTNB treatment (25 out of 40 beads moved without DTNB and 21 out of 40 beads moved with DTNB). This result reveals that the microtubule binding frequency of this kinesin mutant does not change after oxidation, confirming the results from single molecule fluorescence assays. The force–velocity curve also was not significantly altered after oxidation (Fig 4 c). However, after oxidation, the dissociation rate increased by 1.6-fold at most loads (Fig 4 c). This is consistent with the 1.5-fold increase in the dissociation rate (inverse of association time) observed in single molecule motility assays (Table 2). The increase in the dissociation rate after oxidation was small and insignificant for the Cys344 mutant (Fig 4 c).
# R' a; M5 i2 L9 ^1 R
Forced Unwinding of the Neck Coiled-Coil Using Long Cross-linkers
! s4 {7 K) `5 `# z
We also examined whether the neck coiled-coil could be cross-linked using long cross-linkers and whether this forced unwinding of the coiled-coil affected motility. Two rigid bifunctional thiol reagent were employed (Fig 5 a): N,N'-1,2-phenylenedimaleimide (oPDM) which spans two cysteine residues by 4–9 ? (compare to the sulfur–sulfur distance in a disulfide bond, which is 2 ?) and N,N'-1,4-phenylenedimaleimide (pPDM), which spans by 12–13 ?. Cys337 (as well as the Cys337/Cys344 mutant; not shown) was partially cross-linked by both oPDM and pPDM, as judged by the gel shift assay (Fig 5 b). In contrast, Cys344 was not cross-linked by either agent (Fig 5 b). Since the long bifunctional reagents cannot access position 344 in the neck coiled-coil, these results indicate that the structure is stable at this position. In contrast, the beginning of the coiled-coil at residue 337 is less stable, and can unwind at least transiently to permit access to the long cross-linker agents.
9 z0 Z5 E- T" P9 L
To determine how unwinding of the beginning of the coiled-coil affects kinesin function, we examined processive motion of Cys337 before and after cross-linking by oPDM or pPDM using the single molecule fluorescence motility assay. Cys337 mutants moved unidirectionally after oPDM or pPDM cross-linking, and the mean run lengths decreased by only 20% and 22%, respectively (corrected run length of 1.21 and 1.18 μm). The decrease in run length was less than that observed after DTNB treatment of Cys337 (Table 2), possibly because the efficiency of cross-linking with oPDM and pPDM was lower that that with DTNB. The velocity of Cys337 motion was not affected by cross-linking with oPDM (19.1 ± 4.4 and 19.3 ± 4.4 μm/min for reduced and cross-linked respectively, P value of 0.8), but was significantly decreased after cross-linking with the longer cross-linker pPDM (15.3 ± 4.9 μm/min; P value of 0.00004) (Fig 5 c). A decrease in velocity was also observed for Cys337/Cys344 after cross-linking with pPDM (20.1 ± 3.5 and 15.4 ± 5.7 μm/min for reduced and cross-linked, respectively, P value of 10-9). The single molecule velocity for Cys344 was unchanged after treatment with pPDM (19.5 ± 3.5 and 20.3 ± 4.1 μm/min for reduced and cross-linked, respectively), which was expected since this reagent failed to cross-link this cysteine position. These results indicate that kinesin can move processively when the beginning of the neck coiled-coil is forced into an unwound configuration by cross-linking. However, in contrast to results for cross-linking into a closed state with DTNB, unwinding of the first heptad reduces the velocity of movement.

Discussion

Conformational Changes in the Neck Linker Are Essential for Motility
1 b" K) N1 h% Y! J7 d* z
We have explored the neck linker's role in processive movement by preventing the neck linker movements using site-directed chemical cross-linking. Disulfide cross-linking of the neck linker at the tip of the catalytic core (Cys334/Cys222), which should prevent the unzippering of neck linker during the enzymatic cycle, resulted in a complete loss of unidirectional motion. Rice et al. 1999  previously documented that the neck linker is unzippered in nucleotide-free and ADP states, and zippered after microtubule-docked kinesin binds ATP. These findings were obtained in a truncated, monomeric kinesin, but it was hypothesized that the neck linker conformational changes are essential for processivity in the kinesin dimer. Specifically, rezippering reaction of neck linker in the forward head in the microtubule-bound kinesin dimer would be expected to propel the rear kinesin head to a forward tubulin binding site along the microtubule (Fig 6 a) (see also animated movie from Vale and Milligan 2000 ; www. sciencemag.org/feature/data/1049155.shl). The loss of kinesin dimer motility after neck linker cross-linking to the catalytic core provides strong support for this model.

In contrast to the ablation of motility by cross-linking of Cys334/Cys222, cross-linking the middle of the neck linker (Cys330) to the very NH2 terminus (Cys4) still permitted limited directional motion of the kinesin dimer. Since the COOH-terminal end of neck linker could still unzipper/rezipper in this cross-linked molecule in response to nucleotide-dependent motions of a critical "relay" (or "switch II") helix (Vale and Milligan 2000 ), this result suggests that a partial movement of the neck linker can elicit directional movement. However, the motion in the oxidized Cys330/Cys4 kinesin dimer is very slow (microtubule velocity of 2.5 μm/min) and comparable to the velocity generated by truncated kinesin monomers (2.4 μm/min; Rice et al. 1999 ). Moreover, in single molecule assays, the oxidized Cys330/Cys4 kinesin dimer showed biased diffusion instead of normal unidirectional processivity and was severely compromised in pulling against a load in the optical trap. These results indicate that limited neck linker mobility compromises the formation of a two-head–bound intermediate, which is thought to be essential for kinesin processivity and force production (Fig 6 b). The twofold decrease in microtubule-stimulated ATP-turnover rate after oxidative cross-linking also is consistent with the failure of the dimeric motor to form a two-head–bound intermediate on the microtubule (Hackney 1994 ). According to the mechanically controlled access model (Vale and Milligan 2000 ), contact of both heads with the microtubule requires that the neck linker be completely zippered in the rear head and unzippered in the forward head. Since the latter reaction is inhibited by neck linker cross-linking, only one head will have its ATPase cycle stimulated when the kinesin dimer encounters a microtubule (Fig 6b and Fig c). Thus, results from the single molecule fluorescence processivity assay, force-generation studies with the optical trap, and the ATPase assays all are consistent with the proposed role of the neck linker in kinesin-generated movement.( f5 l# Z! S1 s- r9 \
5 n' O; _2 j8 q* o$ G+ o/ G6 _/ t
Unwinding of the Neck Coiled-Coil Is Not Essential for Processive Movement7 `& c. A1 K( C2 g, `9 A6 A& s
1 [" ]% m8 @9 D! A6 |- Q
In contrast to the results obtained with neck linker cross-linking, disulfide cross-linking at the beginning of the neck coiled-coil (Cys337) or the beginning of the second heptad (Cys344) had little effect on motor function. These results are inconsistent with the proposal (Tripet et al. 1997 ; Hoenger et al. 2000 ) that the neck coiled-coil unwinds to around position 352 to allow the two kinesin heads to separate and form a two-head–bound intermediate on the microtubule. Instead, our results indicate that neck coiled-coil unwinding does not need to occur during processive motion. However, some of our data suggests that limited unwinding of the first heptad may occur and could play a minor role in processivity. Using long cross-linking reagents, we were able to form cross-links between cysteines at position 337 but not 344. Since the longer cross-linking agent (pPDM) can only cross-link cysteines separated by at least 10 ?, these results suggest that the neck coiled-coil of kinesin in solution must "breathe" around position 337 but not at 344. We also find that cross-linking at 337 increases the dissociation rate of the kinesin motor, leading to somewhat shorter run lengths. Unraveling of the first few residues of the neck coiled-coil could aid in the formation of the two-head–bound intermediate, thereby reducing the probability of detachment from a one-head–bound state (see also accompanying paper by Thorn et al. 2000 ).
* p) n- Y/ |3 A% a! F4 C5 M
Two published reports also have examined the effects of stabilizing kinesin's neck coiled-coil. Romberg et al. 1998  replaced the majority of the neck coiled-coil (residues 343–370) with a highly stable artificial coiled-coil (over twofold more stable than kinesin's endogenous coiled coil; Tripet et al. 1997 ) and reported a small decrease in run length (45% decrease) with no change in velocity. Replacing the entire coiled coil (residues 337–370) yielded similar results (46% decrease in run length and no change in velocity) (Ubersax, J., Thorn, K., and Vale, R., unpublished results). These results have been criticized on the basis that they do not exclude a partial unwinding of this stable coiled-coil structure (Mandelkow and Hoenger 1999 ). These previous results, however, are consistent with those obtained here with cross-linking of the neck coiled-coil at Cys337 or Cys337/Cys344 (43% and 48% decrease in run length, respectively; no change in velocity, Table 2). Hoenger et al. 2000  also created similar construct to our Cys337 mutant, although they introduced this cysteine in a wild type rat kinesin dimer that contained other solvent-exposed cysteine residues. They reported no difference in the structure of the kinesin-microtubule complex by cryo-EM, and suggested that the cross-linked kinesin can still form a two-head–bound intermediate. However, they noted an unusual stabilization and curvature of cross-linked kinesin-decorated microtubule protofilaments in the axial direction, suggesting that a strain was imposed on the protofilament by the kinesin. Hoenger also reported a 13-fold decrease in Km(MT) after oxidization, which they interpreted as indicative of a substantial decrease in processivity. However, this decrease in Km(MT) is inconsistent with our results (Table 1), and raises the possibility that oxidation of other solvent-exposed cysteines caused the increase in Km(MT) in their construct (Walker et al. 1997 ).
' W# b4 ^: t: r, ~+ X& o
In summary, our results confirm that the unwinding of the neck coiled-coil is not involved in coordinated movement of kinesin dimer. Rather, integrity of the neck coiled-coil is likely to be important for this process, as it constrains the neck linkers of the two kinesin heads to adopt opposite conformations in the two-head–bound intermediate state. Furthermore, strain built up at the two-head–bound intermediate is thought to be important for such coordination between the two heads (i.e., for a mechanical action in the forward neck linker to be communicated to the rear head). In further support of this idea, we show here that forced unwinding of the beginning of the coiled-coil with long cross-linkers decreases movement velocity, and introduction of a flexible glycine linker at the beginning of the neck coiled-coil also impairs processivity (Romberg et al. 1998 ; Jiang, W., J.-Q. Cheng, J. Moore, R. Patterson, M.F. Stock, and D.D. Hackney. 1999. Biophys. J. 76:A17)., [/ e8 f; e% l4 M( `
. j1 W" J/ _( `  @$ S5 q0 N
Although not undergoing a major conformational change, the neck coiled-coil is likely to play an important modulatory role in processivity. In the accompanying paper, Thorn et al. 2000  show that the kinesin run length can be affected by a weak electrostatic interaction occurring between the neck coiled-coil and the COOH-terminal region of tubulin. One possible explanation for the decrease in processivity after 337 cross-linking is that it impairs the binding interaction of the neck coiled-coil with the COOH terminus of tubulin./ o6 ?5 B: Q  s0 s6 F% W

Diffusional Motions of Cross-linked Kinesin Dimers along Microtubules: C1 @/ O5 E) P; L3 o$ c8 M) k7 F
4 E: h/ m$ {" W9 [9 ~* e2 v8 {
An unexpected result from our experiments was the finding that neck linker cross-linking causes kinesin to undergo one-dimensional diffusion along the microtubule. Interestingly, the diffusion coefficient for motion that we measured (2.5 x 10-11 cm2/s) is similar to a diffusion coefficient estimated from the fluctuation analysis of optical trapping data of processive kinesin dimer (Svoboda et al. 1994 ; Imafuku et al. 1996 ). This suggests that diffusion is an intrinsic property of a kinesin dimer, and becomes clearly evident only after the conformational change that produces unidirectional movement is impaired by neck linker cross-linking. This diffusion phenomenon may again involve a weak electrostatic interaction between the COOH terminus of tubulin and the neck coiled-coil, since neck linker cross-linking of a monomeric construct (Cys330/Cys4 in Cys-light K339) did not elicit detectable diffusional movement (i.e., single motors bound and dissociated rapidly) (data not shown).

The biased one-dimensional diffusion observed for cross-linked Cys330/Cys4 is reminiscent of a similar phenomenon described for a KIF1A chimera (catalytic core of the kinesin-related protein KIF1A and the neck linker of conventional kinesin) (Okada and Hirokawa 1999 , Okada and Hirokawa 2000 ). Oxidized Cys330/Cys4, however, shows a 17-fold lower diffusion rate than the KIF1A chimera, which may reflect a difference in their duty ratios (ratio of tight and weak binding state) (Howard 1997 ). Supporting this idea, the diffusion coefficient of oxidized Cys330/Cys4 in the weak binding state (in the presence of 1 mM ADP) increased eightfold (2.2 x 10-10 cm2/s) and became more similar to the KIF1A chimera (4.4 x 10-10 cm2/s) (data not shown). We also find that the biased diffusional motion of oxidized Cys330/Cys4 is unable to generate much work against a load. Whether the same is true for the KIF1A chimera has not been addressed.

The molecular basis of biased diffusional motion is still unclear, and it is also uncertain whether the motions of oxidized Cys330/Cys4 and the KIF1A chimera reflect similar or different mechanisms. In both cases, however, it appears as though these two motor proteins have mechanisms for maintaining a weak interaction with the COOH terminus of tubulin (through the lysine-rich L12 loop for KIF1A  and the neck coiled-coil for kinesin ), which allows them to diffuse randomly along the microtubule when the heads are in their weak binding ADP state (Fig 6 b). Since the COOH terminus of tubulin is likely to be flexible and mobile, motors may be able to diffuse along microtubules by transferring rapidly from the COOH terminus of one subunit to the COOH terminus of an adjacent subunit. Two mechanisms could create an ATP-dependent bias to this diffusion (Okada and Hirokawa 1999 ): (a) through an asymmetry in the binding potential of the motor–microtubule interaction; or (b) through a conformational change in the motor that biases its subsequent attachment to a tubulin in one direction. We favor the latter model, since oxidized Cys334/Cys222, which has normal ATPase activity but cannot undergo the neck linker conformational change, does not display biased diffusion in the presence of the ATP. In the case of oxidized Cys330/Cys4, we propose that the limited neck linker conformational change shifts the probability of a subsequent motor attachment to the tubulin subunit towards the plus-end. By this mechanism, the motor could undergo a net directional motion through repeated attachment, power stroke, and detachment reactions (Fig 6 b).
8 K( v0 j7 y; k" }5 w6 a, f1 R
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