Isolation and physical study of the 13S fragment of 16S RNA and its complex with ribosomal protein S4

A fragment of E. coli 16S RNA has been obtained by its hydrolysis with pancreatic RNAase A coupled to Sepharose 4B. This fragment has a molecular weight of 170 000 and a sedimentation coefficient of 13S. It does not aggregate in solution and binds with the ribosomal protein S4. The 13S fragment and it complex with the protein S4 have been studied by different physical methods in the first place, by neutron scattering. It has been shown that this fragment is compact in solution. The radii of gyration of the fragment (50 +/- 3 A) and of the protein S4 within the complex (17 +/- 3 A) coincide, within limits of experimental error, with the radii of gyration for the free RNA fragment (47 +/- 2 A) and the free ribosomal protein S4 in solution (18 +/- 2 A). Hence, the conclusion is made that the compactness of the 13S fragment of the 16S RNA and the ribosomal protein S4 does not change at the complex formation. The compact 13S fragment of the 16S RNA is shown to be contrast matched in the H2O/D2O mixture containing 70% D2O which corresponds to its partial specific volume v equal to 0.537 cm3/g.     

Ribosomes and ribonucleic acids of Coxiella burneti

This report describes the direct isolation and characterization of rickettsial ribosomes. Ribosomes from the rickettsia Coxiella burneti were isolated and partially characterized. The ribosomes had a sedimentation constant of about 70S and could be dissociated into 50 and 30S subunits. Electron microscopy revealed ribosomal particles with dimensions similar to those reported for other procaryotic organisms. Ribonucleic acid (RNA) species (23 and 16S) were isolated from the ribosomal particles. The nucleotide compositions of the ribosomal RNAs were found to be similar to those reported for bacterial ribosomal RNA. In addition to the high-molecular-weight ribosomal RNA, 5S RNA was also extracted from the organism.     

Neutron scattering study of the 13 S fragment of 16 S RNA and its complex with ribosomal protein S4

A fragment with a molecular weight of 170,000 and a sedimentation coefficient of 13 S which is capable of specifically binding ribosomal protein S4 has been obtained by digestion of Escherichia coli 16 S RNA with ribonuclease A. The 13 S fragment of 16 S RNA and its complex with protein S4 have been studied by different physical methods; in the first place, by neutron scattering. It has been shown that this fragment is very compact in solution. The radii of gyration of this fragment (50 ± 3 Å) and of protein S4 within the complex (17 ± 3 Å) coincide, within the limits of experimental error, with the radii of gyration for the free RNA fragment (47 ± 2 Å) and the free ribosomal protein S4 in solution (18 ± 2 Å). Hence the conclusion is drawn that the compactness of the RNA fragment and the ribosomal protein does not change on complex formation. The compact 13 S fragment of 16 S RNA is shown to be contrast-matched in solvent containing 70% ²H₂O which corresponds to a value for the partial specific volume of RNA of 0.537 cm³/g.     

Mitochondrial and nuclear mutations that affect the biogenesis of the mitochondrial ribosomes of yeast. II. Biochemistry.

1. Several nuclear mutants have been isolated which showed thermo- or cryo-sensitive growth on non-fermentable media. Although the original strain carried mitochondrial drug resistance mutations (CR, ER, OR and PR), the resistance to one or several drugs was suppressed in these mutants. Two of them showed a much reduced amount of the mitochondrial small ribosomal subunit (37S) and of the corresponding 16S ribosomal RNA. Two dimensional electrophoretic analysis did not reveal any change in the position of any of the mitochondrial ribosomal proteins. However one of the mitochondrial ribosomal proteins. However one of the mutants showed a striking decrease in the amounts of three ribosomal proteins S3, S4 and S15. 2. Four temperature-sensitive mitochondrial mutations have been localized in the region of the gene coding for the large mitochondrial ribosomal RNA (23S). These mutants all showed a marked anomaly in the mitochondrial large ribosomal subunit (50S) and/or the corresponding 23S ribosomal RNA.     

Tissue-specific expression of mouse alpha-amylase genes

Ribosomal protein S4 isolated from the small (30 S) subunits of Escherichia coli ribosomes has been studied by a complex of physical methods such as sedimentation, ultraviolet absorption and circular dichroism spectroscopy, proton magnetic resonance spectroscopy, scanning microcalorimetry and neutron scattering. It has been shown that protein S4 exists in solution in a monomeric form. It is characterized by a high content of secondary structure including both α-helices (43%) and β-form (about 30%). The protein S4 molecules possess a well-developed tertiary structure which melts in a co-operative manner. The compactness of the molecules has been found to be very high (radius of gyration, $\text{R}{}_{\mathrm{<mtext>g</mtext>}}\text{= 18 ± 2}\text{A}\text{?}$), corresponding to that of standard compact globular proteins. The compactness of protein S4 does not change as a result of its interaction with the specifically binding 13 S fragment of the ribosomal 16 8 RNA; this suggests that serious conformational changes in protein S4 upon 30 S subunit assembly are unlikely and that the protein is compact within the ribosome.     

An elongated model of the Xenopus laevis transcription factor IIIA-5S ribosomal RNA complex derived from neutron scattering and hydrodynamic measurements.

The precise molecular composition of the Xenopus laevis TFIIIA-5S ribosomal RNA complex (7S particle) has been established from small angle neutron and dynamic light scattering. The molecular weight of the particle was found to be 95,700 +/- 10,000 and 86,700 +/- 9000 daltons from these two methods respectively. The observed match point of 54.4% D2O obtained from contrast variation experiments indicates a 1:1 molar ratio. It is concluded that only a single molecule of TFIIIA, a zinc-finger protein, and of 5S RNA are present in this complex. At high neutron scattering contrast radius of gyration of 42.3 +/- 2 A was found for the 7S particle. In addition a diffusion coefficient of 4.4 x 10(-11) [m2 s-1] and a sedimentation coefficient of 6.2S were determined. The hydrodynamic radius obtained for the 7S particle is 48 +/- 5 A. A simple elongated cylindrical model with dimensions of 140 A length and 59 A diameter is compatible with the neutron results. A globular model can be excluded by the shallow nature of the neutron scattering curves. It is proposed that the observed difference of 15 A in length between the 7S particle and isolated 5S RNA most likely indicates that part(s) of the protein protrudes from the end(s) of the RNA molecule. There is no biochemical evidence for any gross alteration in 5S RNA conformation upon binding to TFIIIA.     

A detailed model of the three-dimensional structure of Escherichia coli 16 S ribosomal RNA in situ in the 30 S subunit

A large body of intra-RNA and RNA-protein crosslinking data, obtained in this laboratory, was used to fold the phylogenetically and experimentally established secondary structure of Escherichia coli 16 S RNA into a three-dimensional model. All the crosslinks were induced in intact 30 S subunits (or in some cases in growing E. coli cells), and the sites of crosslinking were precisely localized on the RNA by oligonucleotide analysis. The RNA-protein crosslinking data (including 28 sites, and involving 13 of the 21 30S ribosomal were used to relate the RNA structure to the distribution of the proteins as determined by neutron scattering. The three-dimensional model of the 16 S RNA has overall dimensions of 220 A x 140 A x 90 A, in good agreement with electron microscopic estimates for the 30 S subunit. The shape of the model is also recognizably the same as that seen in electron micrographs, and the positions in the model of bases localized on the 30 S subunit by immunoelectron microscopy (the 5' and 3' termini, the m7G and m6(2)A residues, and C-1400) correspond closely to their experimentally observed positions. The distances between the RNA-protein crosslink sites in the model correlate well with the distances between protein centres of mass obtained by neutron scattering, only two out of 66 distances falling outside the expected tolerance limits. These two distances both involve protein S13, a protein noted for its anomalous behaviour. A comparison with other experimental information not specifically used in deriving the model shows that it fits well with published data on RNA-protein binding sites, mutation sites on the RNA causing resistance to antibiotics, tertiary interactions in the RNA, and a potential secondary structural "switch". Of the sites on 16 S RNA that have been found to be accessible to chemical modification in the 30 S subunit, 87% are at obviously exposed positions in the model. In contrast, 70% of the sites corresponding to positions that have ribose 2'-O-methylations in the eukaryotic 18 S RNA from Xenopus laevis are at non-exposed (i.e. internal) positions in the model. All nine of the modified bases in the E. coli 16 S RNA itself show a remarkable distribution, in that they form a "necklace" in one plane around the "throat" of the subunit. Insertions in eukaryotic 18 S RNA, and corresponding deletions in chloroplast or mammalian mitochondrial ribosomal RNA relative to E. coli 16 S RNA represent distinct sub-domains in the structure.(ABSTRACT TRUNCATED AT 400 WORDS)     

The Escherichia coli 30S ribosomal subunit; an optimized three-dimensional fit between the ribosomal proteins and the 16S RNA.

We have generated a computerized fit between the 3-dimensional map of the E.coli 30S ribosomal proteins, as determined by neutron scattering, and the recently published 3-dimensional model for the 16S RNA. To achieve this, the framework of coordinates for RNA-protein cross-link sites on the phosphate backbone in the RNA model was related to the corresponding framework of coordinates for the mass centres of the proteins by a least squares fitting procedure. The resulting structure, displayed on a computer graphics system, gives the first complete picture of the E.coli 30S ribosomal subunit showing both the proteins and the double-helical regions of the RNA. The root mean square distance between cross-link sites and protein centres is 32 A. The position of the mass centre of the combined double-helical regions was calculated from the model and compared with the position of the mass centre of the complete set of proteins. The two centres are displaced relative to one another by 20 A in the model structure, in good agreement with the experimental value of 25 A found by neutron scattering.     

Cooperative interactions among protein and RNA components of the 50S ribosomal subunit of Escherichia coli.

Copperative interactions among constituents of the 50S ribosomal subunit of Escherichia coli have been analyzed in order to elucidate its assembly and structural organization. Proteins L5 and L18 were shown to be necessary and sufficient to effect the association of the 5S and 23S RNAs into a quaternary complex that contains equimolar amounts of all four components. Measurement of diffusion constants by laser light scattering revealed that integration of the 5S RNA induced the 23S RNA to adopt a somewhat more open conformation. An investigation of relationships among proteins associated with the central and 3' portions of the 23S RNA demonstrated that attachment of L5, L10 + L11, and L28 depends upon the RNA-binding proteins L16, L2, and L1 + L3 + L6, respectively, and that L2 interacts with the central segment of the 23S RNA. These data, as well as the results of others, have been used to construct a scheme that depicts both direct and indirect associations of the 5S RNA, the 23S RNA, and over two-thirds of the subunit proteins. The 5' third of the 23S RNA apparently organizes the proteins required to nucleate essential reactions, whereas a region within 500 to 1500 bases of its 3' terminus is associated primarily with proteins involved in the major functional activities of the 50S ribosomal particle.     

The characterisation of a fragment of ribosomal protein S4 that is protected against trypsin digestion by 16S ribosomal RNA of Escherichia coli.

After mild trypsin treatment of a complex of ribosomal protein S4 and 16S RNA of Escherichia coli, a large homogeneous fragment of the S4 protein was protected against digestion by its RNA binding site. This fragment was isolated and characterised for molecular weight. It was able to rebind specifically to 16S RNA. Preliminary results indicate that protected protein fragments can also be obtained from other proteins that complex specifically with 23S and 5S RNA.     

Structure of protein-deficient 50 S ribosomal subunits. Nine core proteins induce the compact conformation of 23 S ribosomal RNA

The complex of 23 S ribosomal RNA with the nine core proteins L2, L3, L4, L13, L17, L20, L21, L22 and L23 obtained either by the disassembly procedure or by reconstitution has been studied by electron microscopy. This complex is found to be very similar to the intact 50 S subunit both in size and in shape.     

Efficient reconstitution of functional Escherichia coli 30S ribosomal subunits from a complete set of recombinant small subunit ribosomal proteins.

Previous studies have shown that the 30S ribosomal subunit of Escherichia coli can be reconstituted in vitro from individually purified ribosomal proteins and 16S ribosomal RNA, which were isolated from natural 30S subunits. We have developed a 30S subunit reconstitution system that uses only recombinant ribosomal protein components. The genes encoding E. coli ribosomal proteins S2-S21 were cloned, and all twenty of the individual proteins were overexpressed and purified. Reconstitution, following standard procedures, using the complete set of recombinant proteins and purified 16S ribosomal RNA is highly inefficient. Efficient reconstitution of 30S subunits using these components requires sequential addition of proteins, following either the 30S subunit assembly map (Mizushima & Nomura, 1970, Nature 226:1214-1218; Held et al., 1974, J Biol Chem 249:3103-3111) or following the order of protein assembly predicted from in vitro assembly kinetics (Powers et al., 1993, J MoI Biol 232:362-374). In the first procedure, the proteins were divided into three groups, Group I (S4, S7, S8, S15, S17, and S20), Group II (S5, S6, S9, Sll, S12, S13, S16, S18, and S19), and Group III (S2, S3, S10, S14, and S21), which were sequentially added to 16S rRNA with a 20 min incubation at 42 degrees C following the addition of each group. In the second procedure, the proteins were divided into Group I (S4, S6, S11, S15, S16, S17, S18, and S20), Group II (S7, S8, S9, S13, and S19), Group II' (S5 and S12) and Group III (S2, S3, S10, S14, and S21). Similarly efficient reconstitution is observed whether the proteins are grouped according to the assembly map or according to the results of in vitro 30S subunit assembly kinetics. Although reconstitution of 30S subunits using the recombinant proteins is slightly less efficient than reconstitution using a mixture of total proteins isolated from 30S subunits, it is much more efficient than reconstitution using proteins that were individually isolated from ribosomes. Particles reconstituted from the recombinant proteins sediment at 30S in sucrose gradients, bind tRNA in a template-dependent manner, and associate with 50S subunits to form 70S ribosomes that are active in poly(U)-directed polyphenylalanine synthesis. Both the protein composition and the dimethyl sulfate modification pattern of 16S ribosomal RNA are similar for 30S subunits reconstituted with either recombinant proteins or proteins isolated as a mixture from ribosomal subunits as well as for natural 30S subunits.     

Positions of S2, S13, S16, S17, S19 and S21 in the 30 S ribosomal subunit of Escherichia coli

Neutron scattering distance data are presented for 33 protein pairs in the 30 S ribosomal subunit from Escherichia coli, along with the methods used for measuring distances between its exchangeable components. When combined with prior data, these new results permit the positioning of S2, S13, S16, S17, S19 and S21 in the 30 S ribosomal subunit, completing the mapping of its proteins by neutron scattering. Comparisons with other data suggest that the neutron map is a reliable guide to the quaternary structure of the 30 S subunit.     

Study of the internal structure of Escherichia coli ribosomes by neutron and x-ray scattering.

Neutron scattering curves of the small and large subparticles of Escherichia coli ribosomes are presented over a wide range of scattering angles and for several contrasts. It was verified that the native ribosome structure was not affected by ²H₂O in the buffer. The reliability of the neutron scattering curves, obtained in H₂O buffer, was established by X-ray scattering experiments on the same material.The non-homogeneous distribution of RNA and protein in the subparticles of E. coli ribosomes is confirmed, with RNA predominantly within the particle and protein predominantly on its periphery. The distances between the centres of gravity of the RNA and protein components do not exceed 25 Å and 30 Å, in the large and small subparticles, respectively.The volume occupied by the RNA within the large and small subparticles is determined. The ratio of the “dry” volume of the RNA to the occupied volume is found to be 0.56; it is the same in both subparticles. Such packing of RNA is characteristic of single helices of ribosomal RNA at their crystallization and of the helices in transfer RNA crystals. A conclusion is drawn that RNA in ribosomes is in a similar state.Experimental scattering curves for the small subparticle depend significantly on the contrast in the angular region in which the scattering is mainly determined by the particle shape. The scattering curve, as infinite contrast is approached, is similar to that calculated for the particle as observed by electron microscopy. Thus, the long-existing contradiction between electron microscopy data (an elonggated particle with an axial ratio 2:1) and X-ray data (an oblate particle with an axial ratio 1:3.5), concerning the overall shape of the 30 S subparticle, is settled in favour of electron microscopy. The experimental neutron scattering curve of RNA within the small subparticle is well-described by the V-like RNA model proposed recently by Vasiliev et al. (1978).Experimental data are given to support the hypothesis that the maxima in the X-ray scattering curves, in the region of scattering angles corresponding to Bragg distances of 90 to 20 Å, arise from the ribosomal RNA component alone. It is shown that the prominence of the peaks in this region of the scattering curve depends only on the scattering fraction of the RNA component. The scattering fraction can be changed both by using the “native contrast” (ribosomal particles containing different amounts of protein) and by varying the solvent composition. The maxima are most pronounced where the RNA scattering fraction is highest or in solvents where the protein density is matched by the solvent. The scattering vectors of the maxima in the X-ray and neutron scattering curves, however, remain unchanged. This allows us to propose the tight packing of RNA as a common principle for the structural arrangement of RNA in ribosomes.     

Unbalanced rRNA gene dosage and its effects on rRNA and ribosomal-protein synthesis.

The synthesis of rRNA was unbalanced by the introduction of plasmids containing rRNA operons with large internal deletions. Significant unbalanced synthesis was achieved only when the deletions affected both 16S and 23S RNA genes or when the deletions affected the 23S RNA gene alone. Although large imbalances in rRNA synthesis resulted from deletions affecting 16S and 23S RNA genes or only 23S RNA genes, excess 16S RNA and defective rRNA species were rapidly degraded. Large imbalances in the synthesis of regions of rRNA did not result in significantly unbalanced synthesis of ribosomal proteins. It therefore is probable that excess intact 16S RNA is degraded because ribosomal proteins are not available for packaging the RNA into ribosomes. Defective RNA species also may be degraded for this reason or because proper ribosome assembly is prevented by the defects in RNA structure. We propose two possible explanations for the finding that unbalanced overproduction of binding sites for feedback ribosomal protein does not result in significant unbalanced translational feedback depression of ribosomal protein mRNAs.     

Isolation of Euglena gracilis chloroplast 5S ribosomal RNA and mapping the 5S rRNA gene on chloroplast DNA.

Ribosomal RNA (5S) from Euglena gracilis chloroplasts was isolated by preparative electrophoresis, labeled in vitro with 125I, and hybridized to restriction nuclease fragments from chloroplast DNA or cloned chloroplast DNA segments. Euglena chloroplast 5S rRNA is encoded in the chloroplast genome. The coding region of 5S rRNA has been positioned within the 5.6 kilobase pair (kbp) repeat which also codes for 16S and 23S rRNA. There are three 5S rRNA genes on the 130-kbp genome. The order of RNAs within a single repeat is 16S-23S-5S. The organization and size of the Euglena chloroplast ribosomal repeat is very similar to the ribosomal RNA operons of Escherichia coli.     

The binding of ribosomal protein S4 does not change the gross conformation of the 16 S RNA.

The binding of ribosomal protein S4 to the 16 S RNA does not result in a large shape or conformational change in the 16 S RNA under the conditions of reconstitution. The sedimentation coefficient, frictional coefficient ratio, and effective hydrodynamic radius of the 16 S RNA.protein S4 complex are very similar to those obtained for the 16 S RNA free in solution. Only subtle conformational differences were obtained in the comparison of the complex and free 16 S RNA by circular dichroism. Thus, extensive organization of the 16 S RNA by ribosomal protein S4 is not a step in the process of self-assembly of the 30 S subunit.     

Do ribosomal RNAs act merely as scaffold for ribosomal proteins?

Investigations that are being carried out in various laboratories including ours clearly provide the answer which is in the negative. Only the direct evidences obtained in this laboratory will be presented and discussed. It has been unequivocally shown that the interaction between 16S and 23S RNAs plays the primary role in the association of ribosomal subunits. Further, 23S RNA is responsible for the Binding of 5S RNA to 16S.23S RNA complex with the help of three ribosomal proteins, L5, L18, L15/L25. The 16S.23S RNA complex is also capable of carrying out the following ribosomal functions, although to small but significant extents, with the help of a very limited number of ribosomal proteins and the factors involved in protein synthesis: (a) poly U-Binding, (B) poly U-dependent Binding of phenylalanyl tRNA, (c) EF-G-dependent GTPase activity, (d) initiation complex formation, (e) peptidyl transferase activity (puromycin reaction) and (f) polyphenylalanine synthesis. These results clearly indicate the direct involvement of rRNAs in the various steps of protein synthesis. Very recently it has Been demonstrated that the conformational change of 23S RNA is responsible for the translocation of peptidyl tRNA from the aminoacyl (A) site to the peptidyl (P) site. A model has Been proposed for translocation on the Basis of direct experimental evidences. The new concept that ribosomal RNAs are the functional components in ribosomes and proteins act as control switches may eventually turn out to Be noncontroversial.     

Identification of RNA species in the RNA-toxin complex and structure of the complex in Clostridium botulinum type E

Clostridium botulinum type E toxin was isolated in the form of a complex with RNA(s) from bacterial cells. Characterization of the complexed RNA remains to be elucidated. The RNA is identified here as ribosomal RNA (rRNA) having 23S and 16S components. The RNA-toxin complexes were found to be made up of three types with different molecular sizes. The three types of RNA-toxin complex are toxin bound to both the 23S and 16S rRNA, toxin bound to the 16S rRNA and a small amount of 23S rRNA, and toxin bound only to the 16S rRNA.