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. 2012 Sep 5;103(5):970-8.
doi: 10.1016/j.bpj.2012.06.054.

Role of the DELSEED loop in torque transmission of F1-ATPase

Affiliations

Role of the DELSEED loop in torque transmission of F1-ATPase

Mizue Tanigawara et al. Biophys J. .

Abstract

F(1)-ATPase is an ATP-driven rotary motor that generates torque at the interface between the catalytic β-subunits and the rotor γ-subunit. The β-subunit inwardly rotates the C-terminal domain upon nucleotide binding/dissociation; hence, the region of the C-terminal domain that is in direct contact with γ-termed the DELSEED loop-is thought to play a critical role in torque transmission. We substituted all the DELSEED loop residues with alanine to diminish specific DELSEED loop-γ interactions and with glycine to disrupt the loop structure. All the mutants rotated unidirectionally with kinetic parameters comparable to those of the wild-type F(1), suggesting that the specific interactions between DELSEED loop and γ is not involved in cooperative interplays between the catalytic β-subunits. Glycine substitution mutants generated half the torque of the wild-type F(1), whereas the alanine mutant generated comparable torque. Fluctuation analyses of the glycine/alanine mutants revealed that the γ-subunit was less tightly held in the α(3)β(3)-stator ring of the glycine mutant than in the wild-type F(1) and the alanine mutant. Molecular dynamics simulation showed that the DELSEED loop was disordered by the glycine substitution, whereas it formed an α-helix in the alanine mutant. Our results emphasize the importance of loop rigidity for efficient torque transmissions.

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Figures

Figure 1
Figure 1
Sequence and structure of DELSEED loop. (A) Amino-acid sequences of the DELSEED loop and the mutants prepared in this study. Residues are numbered according to the TF1 sequence. Residues Ile386 to Asp394 are defined as the DELSEED loop. (B) Crystal structure of the β-subunit (green) in its AMPPNP-bound form, i.e., βTP form, and the γ-subunit (cyan) (PDB:2JDI). The positions of the both ends of glycine or alanine substitutions are shown (sticks) in the magnified images.
Figure 2
Figure 2
Time course of rotation and kinetic analyses of Ala and Gly mutants. (A) Time courses of rotation at 1 mM ATP. The probe used for the rotation was a 60-nm gold colloidal bead. The rotational velocity was determined from 30 continuous revolutions. (B) Rotational velocity and [ATP]. The average rotational rates and the estimated rotational rate from the ATPase activity (1/3 ATPase) are shown (solid circles and open squares, respectively). (Error bars) Standard deviations from at least four different molecules (rotation assay) or three independent measurements (ATPase activity measurement). (Data points) Fits using the Michaelis-Menten equation, V = Vmax × [ATP]/(Km + [ATP]). The values of Vmax, Km, and the calculated konATP are summarized in Table 1. (C) (Histogram) Catalytic dwell of the Glyloop+13 mutant at 1 mM ATP probed by a 60-nm gold colloid (2 molecules, 339 events). The histogram was fitted using the consecutive reaction model of two reactions. The time constants were determined to be 1.77 and 0.48 ms.
Figure 3
Figure 3
Torque determination of Ala and Gly mutants. The fluctuation theorem was employed for the measurement. The ln[P(Δθ)/P(−Δθ)] value is plotted against Δθ for Δt = 3 ms (solid circles), 4 ms (solid squares), 5 ms (open circles), 6 ms (open squares), and 7 ms (cross). The slope of this plot represents the torque/kBT generated by F1. The average torque was determined from a linear approximation of all the data points (shaded line) using a fitting width of ±0.22 (rad). The results are summarized in Table 2.
Figure 4
Figure 4
Fluctuation analysis of pausing mutant F1. (A) Typical x-y trajectory of the rotation of wild-type F1. The rotation was observed at 300 nM ATP. (B) Analysis of the fluctuations in circumferential directions. The probability distributions of the wild-type F1 (red) and the Glyloop+13 (black) and Alaloop (orange) mutants are shown.
Figure 5
Figure 5
Molecular dynamics simulations of Glyloop+13 and Alaloop. (A) The average structures of βempty during the last 15 ns of the simulations are shown (ribbon representation). The structures of βempty in the wild-type F1, Glyloop+13, and Alaloop are shown (red, black, and orange, respectively). The γ-subunit is also shown (light gray). (Lower images) Expanded views of the structures of the DELSEED loop regions (enclosed with blue rectangles in the upper images). (B) Results of DSSP analyses of βempty (empty), βDP (DP), and βTP (TP). The probabilities of α-helix formation at individual residues of the DELSEED loop and adjacent regions in the wild-type F1 (red), Glyloop+13 (black), and Alaloop (orange) are plotted. Residue numbers 384–405 in MF1 correspond to 380–401 in TF1. (C) (Histograms) Retention times of the specific contacts are shown. Bin-width is 5% of 15 ns (0.75 ns). The wild-type and Glyloop+13 and Alaloop mutants are represented (red, black, and orange plots, respectively). (D) ΔRMSF analysis of Glyloop+13 (black) and Alaloop (orange). The RMSF values of wild-type F1 were subtracted from the RMSF values of Glyloop+13 and Alaloop to obtain the ΔRMSF values of βempty (empty), βDP (DP), and βTP (TP). A positive ΔRMSF represents a larger fluctuation than that for the wild-type F1, whereas negative values represent smaller fluctuations. (Horizontal black and orange bars in the figures represent the glycine- or alanine-substituted regions.)

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