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. 2016 Oct 4;113(40):11214-11219.
doi: 10.1073/pnas.1605640113. Epub 2016 Sep 19.

Rotation of artificial rotor axles in rotary molecular motors

Affiliations

Rotation of artificial rotor axles in rotary molecular motors

Mihori Baba et al. Proc Natl Acad Sci U S A. .

Abstract

F1- and V1-ATPase are rotary molecular motors that convert chemical energy released upon ATP hydrolysis into torque to rotate a central rotor axle against the surrounding catalytic stator cylinder with high efficiency. How conformational change occurring in the stator is coupled to the rotary motion of the axle is the key unknown in the mechanism of rotary motors. Here, we generated chimeric motor proteins by inserting an exogenous rod protein, FliJ, into the stator ring of F1 or of V1 and tested the rotation properties of these chimeric motors. Both motors showed unidirectional and continuous rotation, despite no obvious homology in amino acid sequence between FliJ and the intrinsic rotor subunit of F1 or V1 These results showed that any residue-specific interactions between the stator and rotor are not a prerequisite for unidirectional rotation of both F1 and V1 The torque of chimeric motors estimated from viscous friction of the rotation probe against medium revealed that whereas the F1-FliJ chimera generates only 10% of WT F1, the V1-FliJ chimera generates torque comparable to that of V1 with the native axle protein that is structurally more similar to FliJ than the native rotor of F1 This suggests that the gross structural mismatch hinders smooth rotation of FliJ accompanied with the stator ring of F1.

Keywords: ATPase; F1; V-ATPase; protein design; rotary molecular motor.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Fig. 1.
Fig. 1.
Construct of xenogeneic subunits in A3B3. (A) Structure models of V1 and the fusion rotor proteins from subunit D and FliJ. V1DΔ58–113 represents V1 with subunit D, of which the loop domain (58–113) was truncated to leave only the coiled-coil structure. The truncated D and the A and the B subunits are represented in yellow, red, and green, respectively. Cyan in the fusion rotors represents the parts of FliJ. The helical portions derived from V1-D are represented in yellow, and those from FliJ are represented in blue. Dashed lines of the fusion rotors in ChV1D30/J86/D68 and ChV1J147/DC21 represent disordered C-terminal 12-aa residues (13). (B) SDS/PAGE analysis of ChV1. Proteins are visualized by Coomassie blue staining (Upper) or by immunostaining using anti-FliJ to detect the xenogeneic rotors (Lower). The specificity of anti-FliJ was described in ref. .
Fig. S1.
Fig. S1.
Sequence and structural alignment of V1-D and FliJ. The amino acid sequences of V1-D from T.th (Tth_D), Enterococcus hirae (Ehr_D) and Saccharomyces cerevisiae (Sce_D) were aligned with Clustal-W. The FliJ sequences from S. enterica (Sen_J) and Ehr_D were structurally aligned with MATRAS using PDB structures (PDB ID codes 3AJW and 3AON) due to the low sequence similarity between FliJ and V1-D. The conserved residues are highlighted in red (identical) or pink (strong similarity). The C- and N-terminal α-helices are represented as blue cylinders and β-strands are represented as thick yellow arrows. The deleted region in DΔ58–113 is enclosed by a thin line. The DC21 is highlighted as outline characters on a black background. The residue numbers of Tth_D are indicated by black arrows.
Fig. S2.
Fig. S2.
Expression constructs of chimeric V1. The expression plasmids for ChV1 were constructed based on the A3B3D expression plasmid. The amino acid regions from FliJ are highlighted in blue.
Fig. 2.
Fig. 2.
Rotation and torque estimation of the chimeric or truncated V1. (A) Time courses of 290-nm duplex rotation recorded at 250 or 1,000 frames per s. Overall time courses of WT V1 (black), truncated V1DΔ58–113 (red), ChV1D30/J86/D68 (green), ChV1D30/J86/D29 (purple), and ChV1J147/DC21 (sky blue). (B) Thin colored curves show 30 consecutive 120° steps overlaid on top of each other, with the thick blue lines representing the average. The straight red lines indicate linear fit to the cyan curve between 0° to 120°. The slope of the red line, the angular velocity in radians−1, gives the torque N. (C) Torque values estimated from the instantaneous rotary speed in consecutive 120 steps.
Fig. S3.
Fig. S3.
Rotation time courses of chimeric V1s and WT V1 (black line) at 4 mM ATP, respectively.
Fig. 3.
Fig. 3.
Construct of xenogeneic subunits in α3β3. (A) Construct of F1-FliJ chimeras. Side views showing the central FliJ [blue; Protein Data Bank (PDB) ID code 3AJW] and pair of α (green) and β subunits (red) of thermophilic Bacillus PS3 F1-ATPase (PDB ID code 4XD7). The helical portions of F1-γ and those of FliJ are colored in orange and blue, respectively. The C-terminal unstructured portions of FliJ are represented by dashed lines. The linker portion containing the thrombin recognition site is represented by the purple line. (B) SDS/PAGE analysis of ChF1. Proteins are visualized by Coomassie blue staining.
Fig. S4.
Fig. S4.
Sequence alignment of F1-γ and FliJ. The amino acid sequences of F1-γ from thermophilc Bacillus PS3 (PS3_γ), E. coli (Eco_γ), and bovine mitochondria (Bov_γ) were aligned with Clustal-W. The FliJ sequence (Sen_J) and Bov_γ were structurally aligned with MATRAS using PDB structures (PDB ID codes 3AJW and 1E79) due to the low sequence similarity between FliJ and F1-γ. The conserved residues are highlighted in red (identical) or pink (strong similarity). The C- and N-terminal α-helices are represented as blue cylinders and β-strands are represented as thick yellow arrows.
Fig. S5.
Fig. S5.
Expression construct of F1-FliJ chimeras. The expression plasmids for the series of ChF1s were constructed based on the α3β3γ expression plasmid by fully or partially substituting γ subunit with FliJ sequence. The amino acid regions from FliJ and F1-γ subunit are highlighted in blue and orange, respectively.
Fig. 4.
Fig. 4.
Rotation of F1-FliJ chimeras. (A) Time courses of rotation of WT F1 (black), ChF1(21γ) (red), ChF1(17γ) (green), ChF1(9γ) (purple), and ChF1(0γ) (sky blue). (B) Rotation rates of WT F1 (n = 8), ChF1(21γ) (n = 13), ChF1(17γ) (n = 12), ChF1(9γ) (n = 8), and ChF1(0γ) (n = 10) estimated from the fastest portions of consecutive revolutions over 10 s. Filled circles indicate rotation rates for individual molecules. Columns show the means. The error bars indicate SDs. (C) Torque values estimated from the averaged rotation rate of WT F1 and the series of ChF1 shown in B considering the torque of WT F1 is 40 pN⋅nm. Columns show the means. The error bars indicate SDs.
Fig. S6.
Fig. S6.
Rotation time courses of WT F1 and F1-FliJ chimeras. The rotations of the series of ChF1s were more noisy than those of WT F1.
Fig. S7.
Fig. S7.
Structural alignment of FliJ and V1-D or F1-γ. FliJ (blue; PDB ID code 3AJW) was superimposed on the D subunit of V1 (yellow; PDB ID code 3W3A) or γ subunit of F1 (orange; PDB ID code 4XD7). Structural superpositions were calculated using MATRAS server. Rmsds between FliJ and the D subunit of V1 or γ subunit of F1 are 3.2 Å or 4.4 Å, respectively.

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