Structure of the vault, a ubiquitous celular component

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Structure of the vault, a ubiquitous celular component Lawrence B Kong, Amara C Siva, Leonard H Rome, Phoebe L Stewart  Structure  Volume 7, Issue 4, Pages 371-379 (April 1999) DOI: 10.1016/S0969-2126(99)80050-1

Figure 1 Sodium dodecyl sulfate polyacrylamide gel electrophoresis (SDS–PAGE) of the CsCl step gradient fractions. The silver-stained gel shows the eight difference fractions from the CsCI gradient (top to bottom, lanes 1 to 8). Lanes 1 and 2 contain the load fraction, which became the final fraction used in the cryo-EM analysis. Lanes 3 and 4 contain fractions from the 1.45 g/ml CsCl step in SM buffer (see Materials and methods section), lanes 5 and 6 fractions from the 1.5 g/ml CsCl step, and lanes 7 and 8 fractions from the 1.7 g/ml CsCl step. The vaults remain in fractions 1 and 2 (load fraction with protein bands at 240 kDa, 193 kDa and 104 kDa), while ferritin, a major contaminant of high molecular weight, fractionates to the bottom of the gradient (lanes 5 to 8). Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)

Figure 2 Cryo-EM and negative-stain EM images of vaults. (a) Digital cryoelectron micrograph showing vaults suspended in a vitreous ice layer. The vaults tend to stick to the carbon support film and the particles appear frozen in random orientations. (b) Negative-stain micrograph of vaults. Different surface structural details are seen by negative-stain EM. (c) Gallery of isolated cryo-EM vault images in various orientations, from end to side views; the density has been inverted relative to (a). (d) Various vault particles opening at the midsection. All scale bars correspond to 500 Å. Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)

Figure 3 Plots of the vault Euler angles and the Fourier shell correlation (FSC) of the final reconstruction. (a) Euler angles of the final 1352 particle data set plotted into the cyclic eightfold asymmetric unit of the Euler sphere. A majority of particles are oriented in side views (θ = 90°). (b) The FSC correlation curve (solid line) is plotted together with an 8.5σ (symmetry-corrected) threshold curve (dashed line). The resolution as judged by the threshold crossing is ∼22 Å, but the more conservative 0.5 correlation cut-off indicates a resolution of ∼31 Å. Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)

Figure 4 The vault reconstruction with imposed cyclic eightfold symmetry presented from several different views. The scale bar corresponds to 250 Å. Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)

Figure 5 Density slices through each end of the vault. (a) slice planes were taken at 20 Å (three pixel)intervals, with the selected slices indicated by numbered lines. (b) Slices showing particle density; red represents the strongest density and blue the weakest density. Differences in the two ends are seenthe planes 1,2,7 and 8. Each left and right density slice corresponds to the top and bottom slice plane, respectively. Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)

Figure 6 The internal structure of the vault. (a) Cropped views of the reconstruction along two different axes reveal a hollow interior when the isosurface level is set to account for 12.9 MDa. The cropped planes are displayed with the strongest density in red and the weakest density in green. (b) A central density slice shows weak (green) density located inside the vault where each cap meets the barrel. The scale bars correspond to 100 Å. Structure 1999 7, 371-379DOI: (10.1016/S0969-2126(99)80050-1)