Studies on the secondary structure of ribosomal ribonucleic acid components of rabbit reticulocytes

The conformation in solution of fractionated 30 S and 19 S ribosomal RNA from rabbit reticulocytes has been studied by optical rotatory dispersion, analysis of thermal melting profiles and their derivatives, and spectrophotometric acid-base titration. From a consideration of the limitations of these methods, it has been possible to set limiting values on the degree of base-pairing and the lengths of the double helices: between 60 and 80% of the bases in 19 S and 30 S RNA are estimated to be paired. The paired segments are not shorter than 4 base pairs, and evidence from other sources is available which indicates that they are not longer than 8–16 base pairs. The spread of helix lengths is greater in the 30 S than in 19 S RNA; and other differences are noted. Several distinct populations of double helices, differing in their thermal stability, are present. Estimates are presented from spectrophotometric and titration data for the base compositions of the paired and unpaired regions.     

Determination of base pairing in ribonucleic acid by Fourier-transform infrared spectrometry: yeast ribosomal 5S ribonucleic acid

Fourier-transform infrared (FT-IR) spectra of yeast ribosomal 5S RNA have been acquired at several temperatures between 30 and 90 degrees C. The difference spectrum between 90 (bases unstacked) and 30 degrees C (bases stacked) provides a measure of base stacking in the RNA. Calibration difference spectra corresponding to stacking of G-C or A-U pairs are obtained from "reference" FT-IR spectra of poly(rG) X poly(rC) minus 5'-GMP and 5'-CMP or poly(rA) X poly(rU) minus 5'-AMP and 5'-UMP. The best fit linear combination of the calibration G-C and A-U difference spectra to the 5S RNA (90-30 degrees C) difference spectrum leads to a total of 25 +/- 3 base pairs (17 G-C pairs + 8 A-U pairs) for the native yeast 5S RNA in the absence of Mg2+. In the presence of Mg2+, an additional six base pairs are detected by FT-IR (one G-C and five A-U). FT-IR melting curve midpoints show that A-U and G-C pairs melt together (65 and 63 degrees C) in the presence of Mg2+ but A-U pairs melt before G-C pairs (47 vs. 54 degrees C) in the absence of Mg2+.     

Isostericity and tautomerism of base pairs in nucleic acids

The natural bases of nucleic acids form a great variety of base pairs with at least two hydrogen bonds between them. They are classified in twelve main families, with the Watson–Crick family being one of them. In a given family, some of the base pairs are isosteric between them, meaning that the positions and the distances between the C1′ carbon atoms are very similar. The isostericity of Watson–Crick pairs between the complementary bases forms the basis of RNA helices and of the resulting RNA secondary structure. Several defined suites of non-Watson–Crick base pairs assemble into RNA modules that form recurrent, rather regular, building blocks of the tertiary architecture of folded RNAs. RNA modules are intrinsic to RNA architecture are therefore disconnected from a biological function specifically attached to a RNA sequence. RNA modules occur in all kingdoms of life and in structured RNAs with diverse functions. Because of chemical and geometrical constraints, isostericity between non-Watson–Crick pairs is restricted and this leads to higher sequence conservation in RNA modules with, consequently, greater difficulties in extracting 3D information from sequence analysis. Nucleic acid helices have to be recognised in several biological processes like replication or translational decoding. In polymerases and the ribosomal decoding site, the recognition occurs on the minor groove sides of the helical fragments. With the use of alternative conformations, protonated or tautomeric forms of the bases, some base pairs with Watson–Crick-like geometries can form and be stabilized. Several of these pairs with Watson–Crick-like geometries extend the concept of isostericity beyond the number of isosteric pairs formed between complementary bases. These observations set therefore limits and constraints to geometric selection in molecular recognition of complementary Watson–Crick pairs for fidelity in replication and translation processes.     

Secondary structure of 5S RNA: NMR experiments on RNA molecules partially labeled with nitrogen-15

A method has been found for reassembling fragment 1 of Escherichia coli 5S RNA from mixtures containing strand III (bases 69-87) and the complex consisting of strand II (bases 89-120) and strand IV (bases 1-11). The reassembled molecule is identical with unreconstituted fragment 1. With this technique, fragment 1 molecules have been constructed 15N-labeled either in strand III or in the strand II-strand IV complex. Spectroscopic data obtained with these partially labeled molecules show that the terminal helix of 5S RNA includes the GU and GC base pairs at positions 9 and 10 which the standard model for 5S secondary structure predicts [see Delihas, N., Anderson, J., & Singhal, R. P. (1984) Prog. Nucleic Acid Res. Mol. Biol. 31, 161-190] but that these base pairs are unstable both in the fragment and in native 5S RNA. The data also assign three resonances to the helix V region of the molecule (bases 70-77 and 99-106). None of these resonances has a "normal" chemical shift even though two of them correspond to AU or GU base pairs in the standard model. The implications of these findings for our understanding of the structure of 5S RNA and its complex with ribosomal protein L25 are discussed.     

Base pairing in wheat germ ribosomal 5S RNA as measured by ultraviolet absorption, circular dichroism, and Fourier-transform infrared spectrometry

Ultraviolet absorption (UV) and circular dichroism (CD) spectra of wheat germ 5S RNA, when compared to tRNAPhe, indicate a largely base-paired and base-stacked helical structure, containing up to 36 base pairs. Fourier-transform infrared (FT-IR) spectra of tRNAPhe and wheat germ ribosomal 5S RNA have been acquired at 30 and 90 degrees C. From the difference of the FT-IR spectra between 90 and 30 degrees C, the number of base pairs in both RNAs was determined by modification of a previously published procedure [Burkey, K. O., Marshall, A. G., & Alben, J. O. (1983) Biochemistry 22, 4223-4229]. The base-pair composition and total base-pair number from FT-IR data are now consistent for the first time with optical (UV, CD, Raman) and NMR results for ribosomal 5S RNA. Without added Mg2+, tRNAPhe gave 18 +/- 2 base pairs [7 A-U and 11 G-C], in good agreement with the number of secondary base pairs from X-ray crystallography [8 A-U, 12 G-C, and 1 G-U]. Within the 10% precision of the FT-IR method, wheat germ 5S RNA exhibits essentially the same number of base pairs [14 A-U, 17 G-C, and 5 G-U; for a total of 36] in the absence of Mg2+ as in the presence of Mg2+ [14 A-U, 18 G-C, and 3 G-U; for a total of 35], in agreement with the UV hyperchromism estimate of G-C/(A-U + G-C) = 0.58.(ABSTRACT TRUNCATED AT 250 WORDS)     

Occurrence and location of 7-methylguanine residues in small-subunit ribosomal RNAs from eubacteria,archaebacteria and eukaryotes

Specific cleavage with aniline provides a rapid and convenient method for establishing the presence and approximate location of 7-methyl-guanine (m⁷G) residues in ribosomal RNA (rRNA) molecules. Using this approach, we have shown that a single m⁷G occurs roughly 465 bases from the 5'-end of 16 S rRNA from the archaebacterium. Thermoplasma acidophilum, but that this modified base is absent from several other archaebacterial 16 S rRNAs. We have also demonstrated that a unique m⁷G is found some 220–230 bases from the 3'-terminus of a number of eukaryotic 18 S rRNAs. In both cases, m⁷G is present within evolutionarily conserved structural features, suggesting that this base may optimize the activity of functionally important regions of rRNAs in a kingdom-specific fashion.     

Changes in the conformation and stability of 5 S RNA upon the binding of ribosomal proteins.

The binding of ribosomal proteins L25, L18, and L5 to 5 S RNA results in a conformational change and a destabilization of the 5 S RNA molecule. The changes observed in the near ultraviolet circular dichroism (CD) spectra and in the melting profiles indicate an increase in base stacking uith an accompanying increase in asymmetry of the bases and a decrease in the conformational stability of the 5 S RNA. These results are consistent with the interpretation that the binding of these proteins increases the stacking of specific single-stranded bases in 5 S RNA and aligns them in helical arrays, resulting in a conformation which facilitates base-pairing with nucleotide segment(s) of the ribosomal 23 S RNA or the transfer RNA (or both). The simple and precise difference CD method described here is potentially useful for studying subtle conformational changes of other nucleic acid-protein interactions.     

Refined secondary structure models for the 16S and 23S ribosomal RNA of Escherichia coli

The complete range of published sequences for ribosomal RNA (or rDNA), totalling well over 50,000 bases, has been used to derive refined models for the secondary structures of both 16S and 23S RNA from E. coli. Particular attention has been paid to resolving the differences between the various published secondary structures for these molecules. The structures are described in terms of 133 helical regions (45 for 16S RNA and 88 for 23S RNA). Of these, approximately 20 are still tentative or unconfirmed. A further 20 represent helical regions which definitely exist, but where the detailed base-pairing is still open to discussion. Over 90 of the helical regions are however now precisely established, at least to within one or two base pairs.     

Conserved unpaired adenine residues are important for ordered structures of 5S ribosomal RNA. An infrared study of the secondary and tertiary structure of Thermus thermophilus 5S rRNA

An improved set of infrared calibration spectra for the determination of G X C and A X U base pairs leads to 32 +/- 3 G X C (+ G X U) and 4 +/- 1 A X U base pairs for Thermus thermophilus 5S RNA in the presence and absence of Mg2+. These results give further support for the consensus secondary structure of 5S RNA recently proposed by several groups. T. thermophilus 5S RNA shows, in the presence of Mg2+, a distinct two-step thermal melting of its ordered structure. Based on new data about the stacking dependence of infrared intensities of unpaired ribonucleotides the spectral changes of the low-temperature transition should be explained by melting of stacked arrangements of unpaired bases and/or non-standard base pairs. Striking is the reduction in A stacking, which is not related to the melting of A X U base pairs, indicating the importance of the mostly conserved unpaired adenines for the Mg2+ stabilized higher-order structures especially within internal loops of 5S RNA.     

MITOCHONDRIAL RNA FROM CULTURED ANIMAL CELLS : II. A Comparison of the High Molecular Weight RNA from Mouse and Hamster Cells

Discrete RNA fractions sedimenting slightly slower than 18s ribosomal RNA have been found in mitochondrial preparations from both hamster (BHK-21) and mouse (L-929) cells. This RNA could be separated into two components, present in approximately equimolar amounts, by prolonged zonal centrifugation or acrylamide gel electrophoresis. The hamster components had sedimentation constants averaging 16.8 and 13.4, and molecular weights (estimated by gel electrophoresis) averaging 0.74 and 0.42 x 10⁶ daltons. Mixed labeling experiments showed that the mouse components sedimented and electrophoresed 3–6% more slowly than the corresponding hamster components. The RNA from both cell lines resembled mitochondrial ribosomal RNA from yeast and Neurospora in being GC poor, and in addition the larger and smaller components resembled each other in base composition. These results, taken with those of other recent studies, are compatible with the idea that our high molecular weight mitochondrial RNA is ribosomal; such RNA would then constitute a uniquely small size-class of ribosomal RNA.     

Arrangement of the rRNA sequences in the rDNA of Lytechinus variegatus

The arrangement of the 26S RNA and 18S RNA sequences of the ribosomal DNA (rDNA) from the sea urchin Lytechinus variegatus was investigated by an electron microscopic analysis of R-loops formed between the ribosomal RNA genes and the mature ribosomal RNAs. Ninety-eight percent of observed molecules contained R-loops clearly seen as a three-stranded complex. The size of DNA complementary to mature cytoplasmic 18S and 26S ribosomal RNA (rRNA) was calculated by measuring the double-strand (ds) and single-strand (ss) part of the R-loops separately. The values for the 18S R-loop are 1.75±0.24 kb¹ (ss) and 1.56±0.23 kb (ds). The 26S R-loop is 3.34±0.39 kb (ss) and 3.33±0.33 kb (ds). These measurements agree fairly well with the rRNA sizes measured on denaturing sucrose density gradients: 3.23±0.22 kb for the 26S and 1.93±0.10 kb for 18S. The short spacer between the 18S and 26S R-loops is 1.03±0.24 kb and the longer spacer is 5.36±0.53 kb. In long molecules a repeating pattern was observed. The average length of an rDNA repeat unit is 11.33±0.64 kb when computed using double-strand R-loop measurements and 11.50±0.72 when computed using R-loop single-strand lengths.Abbreviations kb kilobases, 1000 bases of RNA or single-strand DNA, and kilobase pairs, 1000 base pairs of duplex DNA or DNA/RNA hybrid - EDTA ethylenediaminetetraacetate - SSC 0.15 M NaCl, 0.015 M sodium citrate - PIPES piperazine-N,N-bis (2-ethanesulfonic acid)-Na_1.4     

Selection of optimal set of wavelengths for analysis of hyperchromic spectra.

The formulae of mean-square deviations of fractions of denatured base pairs in dependence of temperature have been used for selection of optimal set of wave-lengths suited for the study of thermal denaturation dispersion of DNA and DNA complexes. A method is described, which enables the study of the first stage of thermal denaturation of complexes of DNA with basic polypeptides in terms of A · T and G · C base pairs.     

Organization of the ribosomal RNA gene cluster in the yeast Saccharomyces cerevisiae

The chromosomal organization of the ribosomal RNA gene cluster from Saccharomyces cerevisiae was investigated. 18 S rRNA R-loops were formed with unfractionated high molecular weight DNA crosslinked once per 2.7 × 10³ bases with trioxsalen and observed in the electron microscope. Almost all the R-loops were found in very long continuous 9.34 ± 0.18 × 10³ base repeating units. In addition, molecules were found at a frequency of one to two per genome equivalent of rDNA where several rRNA genes were linked to long stretches of non-rDNA. These results suggest that rDNA is arranged in a single tandem repetitive cluster of 100 to 140 genes flanked on one or both sides by non-rDNA.     

STUDIES ON RAPIDLY LABELLED NUCLEAR RNA OF RAT BRAIN

—Methyl albumin kieselguhr chromatography (MAK) has been employed to separate rat brain nuclear RNA, labelled in vivo with [³H]uridine, into three major fractions. The first fraction (QI RNA) is ribosomal in nature for it has a high G + C/U ratio and is methylated by [methyl-³H] methionine. The other two fractions (Q2 RNA and TD RNA) are DNA-like for they exhibit a low G + C/U ratio and are labelled minimally by methionine. Pure ribosomal RNA chromatographs almost entirely in the Q1 RNA fraction. Labelling studies indicate that ribosomal RNA and DNA-like RNA behave differently. Initially, the label in the DNA-like RNA fractions increases rapidly and in a linear fashion for the first 30 min, but thereafter decreases rapidly and reaches a steady state level by 1 h and remains so up to at least the 2 h period. In contrast, the labelling of ribosomal RNA is much slower than that of DNA-like RNA during the first 30 min; however, unlike DNA-RNA, the labelling of ribosomal RNA still continues to increase linearly thereafter. Thus, during longer labelling periods, ribosomal RNA is labelled more rapidly than DNA-like RNA. It appears that the labelling of ribosomal RNA relative to DNA-like RNA is more rapid in liver than in brain.     

Theoretical studies on protein-nucleic acid interactions. II. Hydrogen bonding of amino acid side chains with bases and base pairs of nucleic acids

With a view to understanding the role of hydrogen bonds in the recognition of nucleic acids by proteins, hydrogen bonding between the bases and base pairs of nucleic acids and the amino acids (Asn, Gln, Asp and Glu, and charged residues Arg⁺, Glu^?, and Asp^?) has been studied by a second-order perturbation theory. Binding energies have been calculated for all possible configurations involving a pair of hydrogen bonds between the base (or base pair) and the amino acid residue. Our results show that the hydrogen bonding in these cases has a large contribution from electrostatic interaction. In general, the charged amino acids, compared to the uncharged ones, form more stable complexes with bases or base pairs. The hydrogen-bond energies are an order of magnitude smaller than the Coulombic interaction energies between basic amino acids (Lys⁺, Arg⁺, and His⁺) and the phosphate groups of nucleic acids. The stabilities of the complexes of amino acids Asn, Gln, Asp, and Glu with bases are in the order: G–X > C–X > A–X U–X or T–X, and G · C–X > A · T(U)–X, where X is one of these amino acid residues. It has been shown that Glu^? and Asp^? can recognize guanine in single-stranded nucleic acids; Arg⁺ can recognize G · C base pairs from A · T base pairs in double-stranded structures.     

Ribosomal Ribonucleic Acids of Chloroplastic and Mitochondrial Preparations

RNA prepared from fractions of chloroplasts and mitochondria sedimented at rates characteristic of ribosomal RNA. A predominance of the 18S species was frequently observed in preparations from chloroplasts from romaine lettuce and endive. The usual distribution, a preponderance of the 28S species, was observed in studies on tomato and spinach chloroplasts and mitochondria from mushroom and cauliflower. Comparisons of the base composition of RNA from organelles with their cytoplasmic ribosomal counterparts revealed that the 18S component from romaine lettuce chloroplast was different. A marginally significant difference was observed in the 28S particle from mushroom mitochondria preparations whereas distinct differences, reflected in all the bases, were seen when the 18S component of cauliflower mitochondria preparations was compared with cytoplasmic RNA.     

Cation-pi interactions at non-redundant protein-RNA interfaces

Cation-pi interactions have proved to be important in proteins and protein-ligand complexes. Here, cation-pi interactions are analyzed for 282 non-redundant protein-RNA interfaces. The statistical results show that this kind of interactions exists in 65% of the interfaces. The four RNA bases are ranked as Gua > Ade > Ura > Cyt according to their propensity to participate in cation-pi interactions. The corresponding ranking for the involved amino acid residues is: Arg > Lys > Asn > Gln. The same trends are obtained based on the empirical energy calculation. The Arg-Gua pairs have the greatest stability and are also most frequently observed. The number of cation-pi pairs involving unpaired bases is 2.5 times as many as those involving paired bases. Hence, cation-pi interactions show sequence and structural specificities. For the bicyclic bases, Gua and Ade, their 5-atom rings participate in cation-pi interactions somewhat more than the 6-atom rings, with percentages of 54 and 46%, respectively, which is due to the higher cation-pi participation proportion (63%) of 5-atom rings in the paired bases. These results give a general view of cation-pi interactions at protein-RNA interfaces and are helpful in understanding the specific recognition between protein and RNA.