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Nat Commun
2014 Aug 11;5:4587. doi: 10.1038/ncomms5587.
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Tension on the linker gates the ATP-dependent release of dynein from microtubules.
Cleary FB
,
Dewitt MA
,
Bilyard T
,
Htet ZM
,
Belyy V
,
Chan DD
,
Chang AY
,
Yildiz A
.
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Cytoplasmic dynein is a dimeric motor that transports intracellular cargoes towards the minus end of microtubules (MTs). In contrast to other processive motors, stepping of the dynein motor domains (heads) is not precisely coordinated. Therefore, the mechanism of dynein processivity remains unclear. Here, by engineering the mechanical and catalytic properties of the motor, we show that dynein processivity minimally requires a single active head and a second inert MT-binding domain. Processivity arises from a high ratio of MT-bound to unbound time, and not from interhead communication. In addition, nucleotide-dependent microtubule release is gated by tension on the linker domain. Intramolecular tension sensing is observed in dynein''s stepping motion at high interhead separations. On the basis of these results, we propose a quantitative model for the stepping characteristics of dynein and its response to chemical and mechanical perturbation.
Figure 2. Dynein processivity requires a single motor domain(a) Possible ring-ring communication between the two heads is abolished by replacing one of the monomers with a SRS-MTBD chimera. (b) A kymograph of SRS85:82/WT showing that it moves processively along MTs (c) The average velocity (± SD) and run length (± 95% CI) of the SRS-MTBD/WT constructs compared to WT/WT. (d) An example high-resolution tracking trace (black) and stepping fit (red) of the SRS85:82 head. (e) Histograms of the step sizes for the SRS (upper) and WT (lower) heads (mean ± SD).
Figure 3. The linker provides force to drive the motility of a dynein dimer(a) Dimerization of the C-terminal ring of one head to the N-terminal tail of the other results in a dimer of a free-linker head (FLH) and a bound-linker head (BLH). (b) Kymograph showing that the FLH/BLH heterodimer is capable of processive motility. (c) Run length histogram of FLH/BLH at 2 mM ATP, with maximum likelihood fit (± 95% CI). (d) The average velocities (± SEM) of FLH/BLH constructs carrying an ATPase mutation in either the AAA1 or AAA3 site in one head (ND: motility not detected). (e) Kymographs of ATPase mutants of the FLH or BLH at 2 mM ATP. The AAA1K/A mutation on BLH abolishes directional motility, whereas AAA1E/Q mutation leads to non-directional diffusion along the MT. The same mutations on FLH do not stop motility, indicating that BLH monomer is responsible for FLH/BLH motility.
Figure 4. Tension on the linker inhibits nucleotide-dependent release of dynein from MTs(a) Dynein monomers are attached to a polystyrene bead either through the N-terminus of the linker via a GFP-antibody linkage, or through the C-terminus of the ring via a 74 bp long DNA tether (not to scale). (b) A representative trace showing bead position (blue) and trap position (green). (c) Force-dependent release rates of dynein monomers when the trapped bead is attached to the N-terminal linker domain. The distribution of the forward and backward release rates are unaffected by the presence (red, n = 3003) and absence (blue, n = 2335) of ATP. Shaded regions indicate 95% confidence intervals. Inset: A representative example of the distribution of measured MT-bound times at 0.94 pN average force towards the MT-minus end at 1 mM ATP. Black curve represents maximum likelihood fit to the dwell time histogram. (d) Force-dependent release rates when dynein is pulled through the C-terminus. The rate is similar to the N-terminal attachment case (dotted black line) in the absence of ATP (blue, n = 1105), but increases several fold in the presence of 2 mM ATP (red, n = 1652).
Figure 5. Tension gating of a dynein head is observed at high interhead separations in a motile dimer(a) A representative trace showing simultaneous tracking of AAA1K/A/WT stepping properties with two colors of quantum dots at saturating (1 mM) ATP. (b) The scatter plots represent the step sizes of WT (top) and AAA1K/A (bottom) heads as a function of interhead separation. Interhead separation is positive when the stepping head is in the lead. Slope and y intercept of the linear fit (red line) reveal the change in step size per nm extension between the heads and the net bias to move towards the minus-end, respectively. Both heads take smaller steps when they release the MT in the leading position, similar to native dynein. The AAA1K/A head takes mostly backward steps when stepping from the leading position (probability of backward stepping, pBW = 0.63) (c) The AAA1K/A head remains in the trailing position 72% of the time. Distance to the WT head is positive when the AAA1K/A head is in the lead. (d) Histogram of the dwell time between steps of the WT (left) or AAA1K/A (right) head, independent of the action of the other head, with exponential fit (± 95% CI). (e) Stepping rates of the WT and AAA1K/A heads as a function of interhead separation (shaded region is the 95% CI). The WT head steps more frequently when it is positioned close to the AAA1K/A head, and is otherwise as a similar rate to the AAA1K/A head, indicating that the WT head is gated at high interhead separations.
Figure 6. A model for dynein motility(a) Two proposed mechanisms of dynein stepping. (Left) When the heads are close to each other, either head can release the MT and step forward upon binding ATP. (Right) When the heads are far apart, tension on the linker prevents ATP-dependent MT release, and the asymmetry of the release rates under tension favors the trailing head to take a step. (b) A representative Monte-Carlo simulation of dynein motility shows stepping of the two head domains (blue and red). (c) The trailing head is more likely to take a step in simulated traces as the interhead separation increases. The data shown is the average of 200 simulations (± SD). (d) The average velocity of 200 100 s simulated traces (± SEM) agrees well with measured velocities for various dynein mutants (± SEM, n > 100). The results of the model are within ±15% of the experimental data.
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