Protein–RNA affinity of ribosomal protein L1 mutants does not correlate with the number of intermolecular interactions (original) (raw)

Structure of the ribosomal protein L1–mRNA complex at 2.1 Å resolution: common features of crystal packing of L1–RNA complexes

Acta Crystallographica Section D Biological Crystallography, 2006

The crystal structure of a hybrid complex between the bacterial ribosomal protein L1 from Thermus thermophilus and a Methanococcus vannielii mRNA fragment containing an L1-binding site was determined at 2.1 Å resolution. It was found that all polar atoms involved in conserved protein-RNA hydrogen bonds have high values of density in the electron-density map and that their hydrogen-bonding capacity is fully realised through interactions with protein atoms, water molecules and K + ions. Intermolecular contacts were thoroughly analyzed in the present crystals and in crystals of previously determined L1-RNA complexes. It was shown that extension of the RNA helices providing canonical helix stacking between open-open or open-closed ends of RNA fragments is a common feature of these and all known crystals of complexes between ribosomal proteins and RNAs. In addition, the overwhelming majority of complexes between ribosomal proteins and RNA molecules display crystal contacts formed by the central parts of the RNA fragments. These contacts are often very extensive and strong and it is proposed that they are formed in the saturated solution prior to crystal formation.

High-resolution crystal structure of the isolated ribosomal L1 stalk

Acta Crystallographica Section D Biological Crystallography, 2012

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Crystal Structure of a Conserved Ribosomal Protein-RNA Complex

Science, 1999

The structure of a highly conserved complex between a 58-nucleotide domain of large subunit ribosomal RNA and the RNA-binding domain of ribosomal protein L11 has been solved at 2.8 angstrom resolution. It reveals a precisely folded RNA structure that is stabilized by extensive tertiary contacts and contains an unusually large core of stacked bases. A bulge loop base from one hairpin of the RNA is intercalated into the distorted major groove of another helix; the protein locks this tertiary interaction into place by binding to the intercalated base from the minor groove side. This direct interaction with a key ribosomal RNA tertiary interaction suggests that part of the role of L11 is to stabilize an unusual RNA fold within the ribosome.

Crystal structure of the ribosomal RNA domain essential for binding elongation factors

Proceedings of the National Academy of Sciences, 1998

The structure of a 29-nucleotide RNA containing the sarcin/ricin loop (SRL) of rat 28 S rRNA has been determined at 2.1 Å resolution. Recognition of the SRL by elongation factors and by the ribotoxins, sarcin and ricin, requires a nearly universal dodecamer sequence that folds into a G-bulged cross-strand A stack and a GAGA tetraloop. The juxtaposition of these two motifs forms a distorted hairpin structure that allows direct recognition of bases in both grooves as well as recognition of nonhelical backbone geometry and two 5′-unstacked purines. Comparisons with other RNA crystal structures establish the cross-strand A stack and the GNRA tetraloop as defined and modular RNA structural elements. The conserved region at the top is connected to the base of the domain by a region presumed to be flexible because of the sparsity of stabilizing contacts. Although the conformation of the SRL RNA previously determined by NMR spectroscopy is similar to the structure determined by x-ray crysta...

Crystal structures of mutant ribosomal proteins L1

Molecular Biology, 2007

Nine mutant ribosomal proteins L1 from the bacterium Thermus thermophilus and archaeon Methanococcus jannaschii were obtained and their crystal structures were determined and analyzed. The structure of the S179C TthL1 mutant, determined earlier, was also analyzed. In half of the proteins studied, point mutations of the amino acid residues exposed on the protein surface essentially changed the spatial structure of the protein. This proves that a correct study of biological processes with the help of site-directed mutagenesis requires a preliminary determination or, at least, modeling of the structures of mutant proteins. A detailed comparison of the structures of the L1 mutants and the corresponding wild-type L1 proteins demonstrated that the side chain of a mutated amino acid residue tends to adopt a location similar to that of the side chain of the corresponding residue in the wild-type protein. This observation assists in modeling the structure of mutant proteins.

A mutant form of the ribosomal protein L1 reveals conformational flexibility

FEBS Letters, 1997

The crystal structure of the mutant S179C of the ribosomal protein LI from Thermits thermophilus has been determined at 1.9 A resolution. The mutant molecule displays a small but significant opening of the cavity between the two domains. The domain movement seems to be facilitated by the flexibility of at least two conserved glycines. These glycines may be necessary for the larger conformational change needed for an induced fit mechanism upon binding RNA. The domain movement makes a disulflde bridge possible between the incorporated cysteines in two monomers of the mutant LI.

The RNA binding domain of ribosomal protein L11: three-dimensional structure of the RNA-bound form of the protein and its interaction with 23 S rRNA

Journal of Molecular Biology, 1997

The three-dimensional solution structure has been determined by NMR spectroscopy of the 75 residue C-terminal domain of ribosomal protein L11 (L11-C76) in its RNA-bound state. L11-C76 recognizes and binds tightly to a highly conserved 58 nucleotide domain of 23 S ribosomal RNA, whose secondary structure consists of three helical stems and a central junction loop. The NMR data reveal that the conserved structural core of the protein, which consists of a bundle of three a-helices and a two-stranded parallel b-sheet four residues in length, is nearly the same as the solution structure determined for the non-liganded form of the protein. There are however, substantial chemical shift perturbations which accompany RNA binding, the largest of which map onto an extended loop which bridges the C-terminal end of a-helix 1 and the ®rst strand of parallel b-sheet. Substantial shift perturbations are also observed in the N-terminal end of a-helix 1, the intervening loop that bridges helices 2 and 3, and a-helix 3. The four contact regions identi®ed by the shift perturbation data also displayed protein-RNA NOEs, as identi®ed by isotope-®ltered three-dimensional NOE spectroscopy. The shift perturbation and NOE data not only implicate helix 3 as playing an important role in RNA binding, but also indicate that regions¯anking helix 3 are involved as well. Loop 1 is of particular interest as it was found to be¯exible and disordered for L11-C76 free in solution, but not in the RNA-bound form of the protein, where it appears rigid and adopts a speci®c conformation as a result of its direct contact to RNA.

Structural analysis of interdomain mobility in ribosomal L1 proteins

Acta Crystallographica Section D Biological Crystallography, 2011

The crystal structure of a hybrid complex between the bacterial ribosomal protein L1 from Thermus thermophilus and a Methanococcus vannielii mRNA fragment containing an L1-binding site was determined at 2.1 Å resolution. It was found that all polar atoms involved in conserved protein-RNA hydrogen bonds have high values of density in the electron-density map and that their hydrogen-bonding capacity is fully realised through interactions with protein atoms, water molecules and K + ions. Intermolecular contacts were thoroughly analyzed in the present crystals and in crystals of previously determined L1-RNA complexes. It was shown that extension of the RNA helices providing canonical helix stacking between open-open or open-closed ends of RNA fragments is a common feature of these and all known crystals of complexes between ribosomal proteins and RNAs. In addition, the overwhelming majority of complexes between ribosomal proteins and RNA molecules display crystal contacts formed by the central parts of the RNA fragments. These contacts are often very extensive and strong and it is proposed that they are formed in the saturated solution prior to crystal formation.

Ribosomal protein L1 recognizes the same specific structural motif in its target sites on the autoregulatory mRNA and 23S rRNA

Nucleic Acids Research, 2005

The RNA-binding ability of ribosomal protein L1 is of profound interest since the protein has a dual function as a ribosomal protein binding rRNA and as a translational repressor binding its mRNA. Here, we report the crystal structure of ribosomal protein L1 in complex with a specific fragment of its mRNA and compare it with the structure of L1 in complex with a specific fragment of 23S rRNA determined earlier. In both complexes, a strongly conserved RNA structural motif is involved in L1 binding through a conserved network of RNA-protein H-bonds inaccessible to the solvent. These interactions should be responsible for specific recognition between the protein and RNA. A large number of additional non-conserved RNA-protein H-bonds stabilizes both complexes. The added contribution of these non-conserved H-bonds makes the ribosomal complex much more stable than the regulatory one.