Folding Mechanism of the Tetrahymena Ribozyme P4−P6 Domain

Synchrotron X-ray-dependent hydroxyl radical footprinting was used to probe the folding kinetics of the P4−P6 domain of the Tetrahymena group I ribozyme, which forms a stable, closely packed tertiary structure. The 160-nt domain folds independently at a similar rate (∼2 s-1) as it does in the ribozy...

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Published in:Biochemistry (Easton) Vol. 39; no. 36; pp. 10975 - 10985
Main Authors: Deras, Michael L, Brenowitz, Michael, Ralston, Corie Y, Chance, Mark R, Woodson, Sarah A
Format: Journal Article
Language:English
Published: United States American Chemical Society 12-09-2000
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Summary:Synchrotron X-ray-dependent hydroxyl radical footprinting was used to probe the folding kinetics of the P4−P6 domain of the Tetrahymena group I ribozyme, which forms a stable, closely packed tertiary structure. The 160-nt domain folds independently at a similar rate (∼2 s-1) as it does in the ribozyme, when folding is measured in 10 mM sodium cacodylate and 10 mM MgCl2. Surprisingly, tertiary interactions around a three-helix junction (P5abc) within the P4−P6 domain fold at least 25 times more rapidly (k ≥ 50 s-1) in isolation, than when part of the wild-type P4−P6 RNA. This difference implies that long-range interactions in the P4−P6 domain can interfere with folding of P5abc. P4−P6 was observed to fold much faster at higher ionic strength than in 10 mM sodium cacodylate. Analytical centrifugation was used to measure the sedimentation and diffusion coefficients of the unfolded RNA. The hydrodynamic radius of the RNA decreased from 58 to 46 Å over the range of 0−100 mM NaCl. We propose that at low ionic strength, the addition of Mg2+ causes the domain to collapse to a compact intermediate where P5abc is trapped in a non-native structure. At high ionic strength, the RNA rapidly collapses to the native structure. Faster folding most likely results from a different average initial conformation of the RNA in higher salt conditions.
Bibliography:istex:5E2A02F326503D8B67707055840808AA7F0BFCC4
ark:/67375/TPS-D9P4NXLD-2
This work was supported by grants from the NIH RO1-GM60819, RO1-GM39929, S10-RR13851, and P41-RR01633. Research was carried out, in part, at the National Synchrotron Light Source, Brookhaven National Laboratory, which is supported by the U.S. Department of Energy, Division of Materials Sciences and Division of Chemical Sciences.
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ISSN:0006-2960
1520-4995
DOI:10.1021/bi0010118