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Journal of Virology, September 2002, p. 9533-9536, Vol. 76, No. 18
0022-538X/02/$04.00+0 DOI: 10.1128/JVI.76.18.9533-9536.2002
Copyright © 2002, American Society for Microbiology. All Rights Reserved.
Division of Structural Biology, Wellcome Trust Centre for Human Genetics, Headington, Oxford OX3 7BN,1 Pirbright Laboratory, Institute for Animal Health, Pirbright, Woking GU24 0NF,2 Oxford Centre for Molecular Sciences, Oxford University, Oxford OX1 3QT, United Kingdom3
Received 29 March 2002/ Accepted 12 June 2002
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We have determined the atomic structure of the BTV core (BTV type 1 South Africa [BTV-1 SA]) and learned something of the internal organization of the dsRNA genome segments and transcription complex, along with the routes of entry and exit for substrate and product molecules (4, 6, 7). However, during this analysis, we noted that our model for the crystal structure was in unexpectedly poor agreement with our observed diffraction data at low resolution (Fig. 1). In order to investigate the reason for this, we calculated a difference electron density map between our best model for the virus particle and the experimental data, including data only to 10-Å Bragg spacings (Table 1) (experimental details and further statistics are given in reference 4). This low-resolution map had no symmetry imposed on it additional to that imposed by the formation of the crystal lattice and showed essentially no features within the viral core, indicating that the model for the structure of the protein and internal RNA was, as expected, consistent with the data. However, to our surprise, there were beautifully defined ropes of electron density festooning the outer surface of the virus particles (Fig. 2). These were the only significant features in the difference map and were present at a height of, on average, 4
, demonstrating the exquisite power of difference Fourier syntheses. This electron density could be readily interpreted in terms of A-form dsRNA with the major and minor grooves clearly delineated (Fig. 2). Fitting A-form RNA to the electron density (bent and kinked where necessary) indicated that the festoons of RNA comprised three distinct segments of 412, 276, and 265 bp, respectively. The coordinates (code 1h1k) and structure factors have been deposited with the Protein Data Bank. The net result of this was a virus core in the crystal that was intimately associated with some 2,000 bp of dsRNA (equivalent to approximately 10% of the 19.2 kbp of the complete viral genome) which adhere to its surface via predominantly electrostatic interactions. Two of the three ropes of dsRNA are passed from one particle to another within the crystal lattice. Thus, the crystal lattice is held together by a combination of RNA-protein and protein-protein interactions. The crystal-packing interactions that are mediated by particle-particle contacts total some 10,000 Å2 of surface area per half particle (calculated by AREAIMOL [3] with a probe of 3-Å radius; the crystallographic asymmetric unit contains half a particle). In contrast, the interactions mediated by RNA-protein interactions total 42,000 Å2 per half particle, suggesting that RNA acts as a mesh, helping to hold the crystals together. This presumably explains the observation (2) that the BTV core crystals grow over a period of several months at 29°C, suggesting that the decay of some particles to release dsRNA gene segments may well be a rate-limiting stage in crystal growth. The RNA lattice may also explain the ability of the crystals to survive transfer from a crystallization mother liquor containing 11 to 16% ammonium sulfate and 25% ethylene glycol to a 0.1 M Tris-HCl buffer containing 9 mM magnesium chloride (4).
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FIG. 1. Improvement in the agreement between observed diffraction data and data calculated from an atomic model, with and without external RNA. The R-factor between the data and the initial model missing external RNA is plotted, with respect to resolution, as a thin line; the R-factor between the data and the improved model is plotted as a thick line.
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TABLE 1. Data collection and processing statisticsa
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FIG. 2. Ropes of RNA within BTV core crystals. (A) Stereo figure showing the meshing together of the BTV core particles in the crystals by the long ropes of external dsRNA. The model for the dsRNA is drawn as a green-and-red worm; the core particles are shown to scale as colored yellow and red spheres. (B) Two orthogonal views of the interactions of the parts of one RNA rope with the BTV core. The RNA model and electron density are shown (the density is rendered semitransparent). The VP7 trimers are colored as described in reference 7, with the underlying VP3 molecules shown in slightly darker colors (again, colored as in reference 7). (C) A stereo image of the fit of the dsRNA model, with a portion of the difference electron density map in red, showing the typical disposition of the RNA on the top surface of a VP7 trimer. The strands of the RNA model are shown as green and blue ribbons, and the three polypeptide chains of VP7 are drawn in green, cyan, and blue.
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FIG. 3. Binding modes. The 39 crystallographically independent interactions between the dsRNA and VP7 trimers are displayed superimposed, with the threefold degenerate trimer orientation chosen so as to best align the RNA trajectories. The upper panel illustrates the RNA colored according to binding mode. The principal mode (24 members, lower bundle) is colored green-yellow to cyan. The next-most populous mode (8 members) is colored yellow (top). Two minor intermediate modes (3 and 4 members) are colored red and orange, respectively. The lower panel is identical except that the RNA is translucent, revealing the structure of the underlying VP7 trimer.
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320,000 cpm) in 100 µl of 0.1 M Tris-HCl (pH 8.0)-9 mM MgCl2 for 20 min at 30°. The sample was then layered on a 5.5-ml cushion of 40% (wt/vol) sucrose in an SW50 rotor and centrifuged for 2 h at 40,000 rpm (108,000 x g) at 20°C. Under these conditions, approximately 1% of the labeled dsRNA was pelleted with the core particles, although in a "minus cores" control tube, less than 0.02% of the label was detected at the bottom of the tube. In initial sucrose gradient experiments, addition of the labeled dsRNA had prevented the core particles from banding in 10 to 50% (wt/vol) sucrose gradients, suggesting that they had aggregated and had pelleted at a faster rate. The pelleted cores (through the 40% [wt/vol] sucrose cushion) were resuspended in electrophoresis sample buffer and analyzed by sodium dodecyl sulfate-polyacrylamide gel electrophoresis (Fig. 4). Labeled RNA bands were detected in the pellet containing the BTV cores but not at the bottom of the minus cores control tube. The amount of RNA that pelleted with the cores was considerably less than one molecule per core particle, and the individual segments did not bind in an equimolar manner but rather in amounts that appeared to show a direct correlation with the size of the RNA segment (Fig. 4). These observations suggest that relatively few binding sites are available or that binding is a slow process. Under the experimental conditions used, the larger dsRNA molecules may simply represent a larger target for core particle binding, suggesting a lack of nucleotide sequence specificity in the binding mechanism. Further experiments will be required to see if there is any binding specificity for RNA over DNA molecules or for single-stranded RNA over dsRNA molecules and if the amount of RNA bound to the cores increases with longer incubation times. Nevertheless, the direct association of dsRNA with BTV core particles in solution suggests that our crystallographic observations may reflect a general property of the BTV core particles.
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FIG. 4. Autoradiograph of a sodium dodecyl sulfate-11% polyacrylamide electrophoresis gel that was used to analyze interactions between BTV-1 SA core particles and [32P]pCp-labeled BTV-1 SA dsRNA. dsRNA binding was detected by pelleting core particles through a 40% (wt/vol) sucrose cushion. Lanes 1 and 4 are positive controls and show that, although genome segments 2 and 3, 5 and 6, and 8 and 9 were not well separated, all 10 segments were present in the dsRNA starting material and were labeled in equimolar amounts. Lane 2 shows analysis of the pellet from a sample of the labeled dsRNA that was centrifuged without BTV core particles, showing the absence of detectable RNA bands. Lane 3 shows analysis of the pellet when cores were incubated with the labeled dsRNA prior to centrifugation, demonstrating that there is an association between the dsRNA and core particles. In addition, although all of the dsRNAs are present in the pellet (including small amounts of segment 10), it is clear that there is a higher ratio of binding of the larger segments of dsRNA to cores than that of the smaller segments.
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This work was supported by the Biotechnology and Biological Sciences Research Council and Medical Research Council and the European community (grant contract Bio4 CT 97-2364). P.P.C.M. and J.N.B. are supported by the Department for Environment, Food and Rural Affairs; J.M.G. is supported by the Royal Society, and D.I.S. is supported by the Medical Research Council.
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A in the resistance of avian reovirus to interferon. J. Virol. 74:1124-1131.
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