An estimate of the nearest neighbor base-pair content of 5S RNA using CD and absorption spectroscopy.

We analyzed the CD and uv absorption spectra of 5S RNA from Escherichia coli using the method developed in the preceding paper. The analysis of spectra of 5S RNA at 20 degrees C in 0.1M NaClO4, 2.5 mM Na+ (phosphate), pH 7.0, and 0.5 mM MgSO4 gave 7 +/- 3.6 A.U base pairs, 25 +/- 3.6 G.C base pairs, and 7.5 +/- 3.6 G.U base pairs. Estimates of nearest neighbor base pairs were more consistent with the Pieler-Erdmann and the Gewirth-Moore secondary structure models than with the Fox-Woese or the Burns-Luoma-Marshall models. We also examined the structure of 5S RNA as a function of temperature. The melting profile exhibited two transitions--one at about 35 degrees C and one above 50 degrees C. Our spectral data showed that helices I and II were stable during the first transition, and agreed with other data that helix III was the most likely helix to have melted. The results from this in-depth study of 5S RNA indicate that our method of analysis should be useful for studying the secondary structures of other small, unmodified RNAs.     

Monte Carlo simulation for single RNA unfolding by force

Using polymer elastic theory and known RNA free energies, we construct a Monte Carlo algorithm to simulate the single RNA folding and unfolding by mechanical force on the secondary structure level. For the constant force ensemble, we simulate the force-extension curves of the P5ab, P5abc deltaA, and P5abc molecules in equilibrium. For the constant extension ensemble, we focus on the mechanical behaviors of the RNA P5ab molecule, which include the unfolding force dependence on the pulling speed, the force-hysteresis phenomenon, and the coincidence of stretching-relaxing force-curves in thermal equilibrium. We particularly simulate the time traces of the end-to-end distance of the P5ab under the constant force in equilibrium, which also have been recorded in the recent experiment. The reaction rate constants for the folding and unfolding are calculated. Our results show that the agreement between the simulation and the experimental measurements is satisfactory.     

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.     

The hydrodynamic shape, conformation, and molecular model of Escherichia coli ribosomal 5 S RNA.

The structure of ribosomal 5 S RNA has been examined using several physical biochemical techniques. Hydrodynamic measurements yield a s020,omega and [eta] of 5.5 x 10(-13) x and 6.9 ml/g, respectively. Other parameters calculated from these values indicate the shape of 5 S RNA is consistent with that of a prolate ellipsoid 160 A in length and 32 A wide. Sedimentation equilibrium results show that 5 S RNA exists as a monomer in the reconstitution buffer with an apparent molecular weight of 44,000. Ultraviolet absorption difference spectra show that approximately 75% of the bases in 5 S RNA are involved in base pairing, and of these base pairs 70% are G-C and 30% are A-U. These results on the overall shape and secondary structure of 5 S RNA have been incorporated with the results of other investigators as to the possible location of single-stranded and double-stranded helical regions, and a molecular model for 5 S RNA is proposed. The molecular model consists of three double helices in the shape of a prolate ellipsoid, with two of the double helical regions at one end of the molecule. The structure is consistent with the available data on the structure and function of 5 S RNA and bears similarity to the molecular model proposed by Osterberg et al. ((1976) Eur. J. Biochem. 68, 481-487) based on small angle x-ray scattering results and the secondary structure proposed by Madison ((1968) Annu. Rev. Biochem. 37, 131-148).     

The equilibrium partition function and base pair binding probabilities for RNA secondary structure.

A novel application of dynamic programming to the folding problem for RNA enables one to calculate the full equilibrium partition function for secondary structure and the probabilities of various substructures. In particular, both the partition function and the probabilities of all base pairs are computed by a recursive scheme of polynomial order N3 in the sequence length N. The temperature dependence of the partition function gives information about melting behavior for the secondary structure. The pair binding probabilities, the computation of which depends on the partition function, are visually summarized in a "box matrix" display and this provides a useful tool for examining the full ensemble of probable alternative equilibrium structures. The calculation of this ensemble representation allows a proper application and assessment of the predictive power of the secondary structure method, and yields important information on alternatives and intermediates in addition to local information about base pair opening and slippage. The results are illustrated for representative tRNA, 5S RNA, and self-replicating and self-splicing RNA molecules, and allow a direct comparison with enzymatic structure probes. The effect of changes in the thermodynamic parameters on the equilibrium ensemble provides a further sensitivity check to the predictions.     

Effect of ethanol on folding of hen egg-white lysozyme under acidic condition

The equilibrium and kinetics of folding of hen egg-white lysozyme were studied by means of CD spectroscopy in the presence of varying concentrations of ethanol under acidic condition. The equilibrium transition curves of guanidine hydrochloride-induced unfolding in 13 and 26% (v/v) ethanol have shown that the unfolding significantly deviates from a two-state mechanism. The kinetics of denaturant-induced refolding and unfolding of hen egg-white lysozyme were investigated by stopped-flow CD at three ethanol concentrations: 0, 13, and 26% (v/v). Immediately after dilution of the denaturant, the refolding curves showed a biphasic time course in the far-UV region, with a burst phase with a significant secondary structure and a slower observable phase. However, when monitored by the near-UV CD, the burst phase was not observed and all refolding kinetics were monophasic. To clarify the effect of nonnative secondary structure induced by the addition of ethanol on the folding/unfolding kinetics, the kinetic m values were estimated from the chevron plots obtained for the three ethanol concentrations. The data indicated that the folding/unfolding kinetics of hen lysozyme in the presence of varying concentrations of ethanol under acidic condition is explained by a model with both on-pathway and off-pathway intermediates of protein folding.     

Sequences of the 5S rRNAs of Azotobacter vinelandii, Pseudomonas aeruginosa and Pseudomonas fluorescens with some notes on 5S RNA secondary structure

Recently published alignments of available 5 S rRNA sequences have shown that a rigid base pairing pattern, pointing to the existence of a universal five-helix secondary structure for all 5 S RNAs, can be superimposed on such alignments. For a few species, the alignment and the base pairing pattern show distortions with respect to the large majority of sequences. Their 5 S RNAs may form exceptional secondary structures, or there may just be errors in the published sequences. We have examined such a case, Pseudomonas fluorescens, and found the sequence to be in error. The corrected sequence, as well as those of the related species Azotobacter vinelandii and Pseudomonas aeruginosa, fit perfectly in the 5 S RNA sequence alignment and in the five-helix secondary structure model. There exists comparative evidence for the frequent presence of non-standard base pairs at several points of the 5 S RNA secondary structure.     

Enhanced base-pair opening in the adenine tract of a RNA double helix

Proton exchange and nuclear magnetic resonance spectroscopy are being used to characterize the kinetics and energetics of base-pair opening in two nucleic acid double helices. One is the RNA duplex 5'-r(GCGAUAAAAAGGCC)-3'/5'-r(GGCCUUUUUAUCGC)-3', which contains a central tract of five AU base pairs. The other is the homologous DNA duplex with a central tract of five AT base pairs. The rates and the equilibrium constants of the opening reaction of each base pair are measured from the dependence of the exchange rates of imino protons on ammonia concentration, at 10 °C. The results reveal that the tract of AU base pairs in the RNA duplex differs from the homologous tract of AT base pairs in DNA in several ways. The rates of opening of AU base pairs in RNA are high and increase progressively along the tract, reaching their largest values at the 3'-end of the tract. In contrast, the opening rates of AT base pairs in DNA are much lower than those of AU base pairs. Within the tract, the largest opening rate is observed for the AT base pair at the 5'-end of the tract. These differences in opening kinetics are paralleled by differences in the stabilities of individual base pairs. All AU base pairs in the RNA are less stable than the AT base pairs in the DNA. The presence of the tract enhances these differences by increasing the stability of AT base pairs in DNA while decreasing the stability of AU base pairs in RNA. Due to these divergent trends, along the tracts, the AU base pairs become progressively less stable than AT base pairs. These findings demonstrate that tracts of AU base pairs in RNA have specific dynamic and energetic signatures that distinguish them from similar tracts of AT base pairs in DNA.     

Structural studies of 5 S ribosomal RNAs from a thermophilic fungus, Thermomyces lanuginosus. A comparison of generalized models for eukaryotic 5 S RNAs

The cytoplasmic ribosomes of the thermophilic fungus Thermomyces lanuginosus contain two types of 5 S RNA. The nucleotide sequence for approximately 80% of the molecules is (pp)pA-C-A-U-G-C-G-A-C-C-A-U-A-G-G-G-U-G-U-G-G-A-A-A-A-C-A-G-G-G-C-U-U-C-C-C-G-U-C-C-G-C-U-C-A-G-C-C-G-U-A-C-U-U-A-A-G-C-C-A-C-A-C-G-C-C-G-G-C-U-G-G-U-U-A-G-U-A-G-U-U-G-G-G-U-G-G-G-U-G-A-C-C-A-C-C-A-G-C-G-A-A-U-C-C-C-A-G-C-U-G-U-U-G-C-A-U-G-UOH. The remainder contains two nucleotide substitutions, C19 and G60, which preserve base complementarity. The secondary structure was probed using partial T1, pancreatic, and S1 nuclease digestion under a variety of ionic and temperature conditions and fragments were analyzed by rapid gel sequencing techniques. The results support the Y-shaped secondary structure model originally proposed by Nishikawa, K., and Takemura, S. (1974) FEBS Lett. 40, 106-109, for eukaryotic 5 S RNAs. When the thermal denaturation profile was compared with that of the yeast 5 S RNA, the thermophilic RNA exhibited not only a higher Tm but also an unusual decline in absorbency at moderate temperatures. This suggests that a functionally important structure may be maintained only at higher temperatures.     

Hybridization of antisense oligonucleotides with alpha-sarcin loop region of Escherichia coli 23S rRNA

Binding of complementary oligonucleotides (ONs) with alpha-sarcin loop region (2638-2682) of Escherichia coli 23S rRNA was investigated. Four of the tested pentadecanucleotides efficiently bound to target sequences with association rate and equilibrium constants approximately 10(3) M(-1)s(-1) and 10(7) M(-1), respectively. ON S5 (CGAGAGGACCGGAGU) complementary to the sequence 2658-2672 displayed the highest affinity to the target. Activation energy for binding of ON S5 was measured to be 11 kcal/mol; this value corresponds to approximately 10% of the calculated enthalpy of the local RNA structure unfolding in the presence of this oligonucleotide. The activation energy value is evidence for the heteroduplex formation to occur via strand displacement pathway; the initiation of heteroduplex formation requires disruption of 1-2 base pairs in RNA hairpin.     

Facilitating RNA structure prediction with microarrays

Determining RNA secondary structure is important for understanding structure-function relationships and identifying potential drug targets. This paper reports the use of microarrays with heptamer 2'-O-methyl oligoribonucleotides to probe the secondary structure of an RNA and thereby improve the prediction of that secondary structure. When experimental constraints from hybridization results are added to a free-energy minimization algorithm, the prediction of the secondary structure of Escherichia coli 5S rRNA improves from 27 to 92% of the known canonical base pairs. Optimization of buffer conditions for hybridization and application of 2'-O-methyl-2-thiouridine to enhance binding and improve discrimination between AU and GU pairs are also described. The results suggest that probing RNA with oligonucleotide microarrays can facilitate determination of secondary structure.     

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.     

Identification and assignment of base pairs in three helical stems of Torulopsis utilis ribosomal 5S RNA and its RNase T1 and RNase T2 cleaved fragments via 500-MHz proton homonuclear overhauser enhancements

Imino proton resonances in the downfield region (10-14 ppm) of the 500-MHz 1H NMR spectrum of Torulopsis utilis 5S RNA are identified (A X U, G X C, or G X U) and assigned to base pairs in helices I, IV, and V via analysis of homonuclear Overhauser enhancements (NOE) from intact T. utilis 5S RNA, its RNase T1 and RNase T2 digested fragments, and a second yeast (Saccharomyces cerevisiae) 5S RNA whose nucleotide sequence differs at only six residues from that of T. utilis 5S RNA. The near-identical chemical shifts and NOE behavior of most of the common peaks from these four RNAs strongly suggest that helices I, IV, and V retain the same conformation after RNase digestion and that both T. utilis and S. cerevisiae 5S RNAs share a common secondary and tertiary structure. Of the four G X U base pairs identified in the intact 5S RNA, two are assigned to the terminal stem (helix I) and the other two to helices IV and V. Seven of the nine base pairs of the terminal stem have been assigned. Our experimental demonstration of a G X U base pair in helix V supports the 5S RNA secondary structural model of Luehrsen and Fox [Luehrsen, K. R., & Fox, G.E. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 2150-2154]. Finally, the base-pair proton peak assigned to the terminal G X U in helix V of the RNase T2 cleaved fragment is shifted downfield from that in the intact 5S RNA, suggesting that helices I and V may be coaxial in intact T. utilis 5S RNA.     

Alternatively folded states of an immunoglobulin

Well-defined, non-native protein structures of low stability have been increasingly observed as intermediates in protein folding or as equilibrium structures populated under specific solvent conditions. These intermediate structures, frequently referred to as molten globule states, are characterized by the presence of secondary structure, a lack of significant tertiary contacts, increased hydrophobicity and partial specific volume as compared to native structures, and low cooperativity in thermal unfolding. The present study demonstrates that under acidic conditions (pH less than 3) the antibody MAK33 can assume a folded stable conformation. This A-state is characterized by a high degree of secondary structure, increased hydrophobicity, a native-like maximum wavelength of fluorescence emission, and a tendency toward slow aggregation. A prominent feature of this low-pH conformation is the stability against denaturant and thermal unfolding that is manifested in highly cooperative reversible phase transitions indicative of the existence of well-defined tertiary contacts. These thermodynamic results are corroborated by the kinetics of folding from the completely unfolded chain to the alternatively folded state at pH 2. The given data suggest that MAK33 at pH 2 adopts a cooperative structure that differs from the native immunoglobulin fold at pH 7. This alternatively folded state exhibits certain characteristics of the molten globule but differs distinctly from it by its extraordinary structural stability that is characteristic for native protein structures.     

Identification of three G.U base pairs in Bacillus subtilis ribosomal 5S RNA via 500-MHz proton homonuclear Overhauser enhancements

Three distinct G.U base pairs in Bacillus subtilis 5S RNA have been identified via homonuclear Overhauser enhancements (NOE) of their low-field (9-15 ppm) proton Fourier transform nuclear magnetic resonances at 11.75 T. With these G.U resonances as starting points, short segments of NOE connectivity can be established. One G.U-G.C-G.C segment (most probably G4.C112-G5.C111-U6.G110) can definitely be assigned to the terminal helix. The existence of at least part of the terminal helical stem of the secondary structure of a Gram-positive bacterial 5S RNA has thus been established for the first time by direct experimental observation. Addition of Mg2+ produces almost no conformational changes in the terminal stem but results in major conformational changes elsewhere in the structure, as reflected by changes in the 1H 500-MHz low-field NMR spectrum. Assignment of the two remaining G.U base pairs will require further experiments (e.g., enzymatic-cleavage fragments). Finally, the implications of these results for analysis of RNA secondary structure are discussed.     

41 The essential adenosine stacking in a two-base-pair minimal kissing complex

A stable RNA helix requires at least three base pairs. Surprisingly, a tertiary kissing complex formed between two GACG hairpin loops contains only two GC pairs. In the NMR structure of this complex, the two flanking adenosines stack on the kissing GC pair. This observation raised a possibility that the 5’-dangling adenines contribute to the formation and stability of the kissing interaction. To test this hypothesis, we took a two-pronged approach to examine the effects of various mutational and chemical modifications of the flanking adenosines on the folding of the kissing complex. Using mass spectrometry, we studied formation of kissing dimers formed by different hairpins. Using optical tweezers, we monitored mechanical unfolding of intramolecular kissing complex at single-molecule level. In both experiments, replacing adenine with uridine abolished the kissing interaction, suggesting that a minimal kissing complex must contain two GC pairs flanked by inter-strand stacking adenines. The stabilizing effect by the adenines can be explained by the fact that the stacking purine nucleobases shield the hydrogen bonds of the adjacent GC pairs, preventing them from fraying. Unlike in the context of secondary structure, the 5’-unpaired adenines in the tertiary structure are structurally constrained in a way that allows for effective stacking onto the adjacent base pairs.     

500-MHz proton homonuclear Overhauser evidence for additional base pair in the common arm of eukaryotic ribosomal 5S RNA: wheat germ

A "common-arm" fragment from wheat germ (Triticum aestivum) 5S RNA has been produced by enzymatic cleavage with RNase T1 and sequenced via autoradiography of electrophoresis gels for the end-labeled fragments obtained by further RNase T1 partial digestion. The existence, base pair composition, and base pair sequence of the common arm are demonstrated for the first time by means of proton 500-MHz nuclear magnetic resonance. From Mg2+ titration, temperature variation, ring current calculations, sequence comparisons, and proton homonuclear Overhauser enhancement experiments, additional base pairs in the common arm of the eukaryotic 5S RNA secondary structure are detected. Two base pairs, G41 X C34 and A42 X U33 in the hairpin loop, could account for the lack of binding between the conserved GAAC segment of 5S RNA and the conserved Watson-Crick-complementary GT psi C segment of tRNAs.     

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)