Rubén Díaz-Avalos, Donald L.D. Caspar  Biophysical Journal 

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Structure of the Stacked Disk Aggregate of Tobacco Mosaic Virus Protein  Rubén Díaz-Avalos, Donald L.D. Caspar  Biophysical Journal  Volume 74, Issue 1, Pages 595-603 (January 1998) DOI: 10.1016/S0006-3495(98)77818-X Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 1 Electron micrograph of ice-embedded stacked disks. There are seven 180-Å-diameter particles horizontally aligned in the field of this micrograph. The thickness of each disk layer is 26.8Å. The image was taken at 4500Å underfocus and 45,000× magnification. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 2 Disk-pair average images and asymmetrical noise. The top three rows are translational averages and asymmetrical differences of disk-pair images from three selected particles, and the bottom row is the average of these three. Column A shows the translationally averaged disk-pair images corresponding to the projection of the cylindrically averaged structure, which should be bilaterally symmetrical if noise-free. Column B shows the left-right difference of the translational average, which is a measure of noise in the image. Column C shows the top-bottom difference of the translational average, averaged left and right to impose cylindrical symmetry. The top-bottom differences in Column C are generally smaller than those in Column B, indicating that any polarity in the disk-pair structure is less than the asymmetrical noise level in these images. Increasing the number of images averaged (last row) reduces the noise level, enhancing the apparent dihedral symmetry of the disk pair. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 3 (A) Surface view of the 3D reconstruction calculated without imposing dihedral symmetry. (B) Orthogonal sections through the reconstruction: sections i and ii were taken at positions corresponding to the slewed a-helices; i was taken above the twofold axis (center of the image in A), whereas ii comes from below the twofold axis. Sections iii and iv correspond to the region of the radial α-helices, with iii coming from below the twofold axis and iv from above it. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 4 Layer line data of the reconstruction, separated into real (solid lines) and imaginary (dashed lines) components. The diffraction amplitudes, weighted by the radius in reciprocal space, were obtained from the calculated average Fourier transform of 16 stacked disk particles. Helical symmetry was imposed in averaging the off-equatorial layer lines, but dihedral symmetry, which would have eliminated the imaginary parts of the transform, was not imposed. The layer lines in the grayscale display of the calculated average diffraction pattern are indexed to the corresponding plots of the weighted amplitudes. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 5 Plot of the contrast transfer function corresponding to an amplitude contrast of 4%, a defocus of −4500Å, and temperature factors of 1000Å2 (solid line) and 600Å2 (dashed line). The solid line corresponds to the CTF used to fit the data and model in the radial direction, whereas the dotted line corresponds to the CTF used for the meridional direction. The only difference between the two curves is the temperature factor applied. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 6 Layer lines of data and model. The layer-line amplitudes from the cryomicroscopy data are plotted with solid lines; the CTF-adjusted model transforms, calculated from the atomic structure of the crystalline A-ring pair, are dashed. Only the real part of the experimental layer lines is plotted, as the imaginary component represents noise. There is generally close agreement between model and data to ∼20-Å resolution. At higher resolution, fringe positions remain correlated, although there are some differences in amplitudes. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions

Figure 7 Axial section through the image reconstruction of the stacked disk and the model based on the crystalline A-ring pair. The section cuts through five disk pairs along the axis of the assembly, with a twofold axis (*) perpendicular to the plane of the section. Succeeding sections of the stack are related by in-plane horizontal dyads bounding this five-disk-pair segment. Because the level of noise in the reconstructed density map was estimated to be on the order of 25% of the peak densities, we display four levels, each corresponding to the magnitude of the standard deviation of the average density. A is a section obtained from the experimental data, and B is the corresponding section of the modeled stacked disk rod, convoluted with the experimental point spread function of the electron micrographs, using the same color table as in A. C is the superposition of A and B with the color table of B inverted. The grey areas denote complete agreement of the two structures, whereas reddish regions denote dominance of the experimental data, and bluish shades indicate where the model is stronger. The differences between the data and model are on the order of the standard deviation of the experimentally averaged densities. Biophysical Journal 1998 74, 595-603DOI: (10.1016/S0006-3495(98)77818-X) Copyright © 1998 The Biophysical Society Terms and Conditions