Evaluation of RNA conformation from circular dichroism and optical rotatory dispersion data

Modulation of Conformational Equilibria in the S-Adenosylmethionine (SAM) II Riboswitch by SAM, Mg(2+), and Trimethylamine N-Oxide

The dependence of the conformation of the S-adenosylmethionine (SAM) II riboswitch on the concentration of added Mg(2+) ions and SAM, individually and in mixtures, was monitored by circular dichroism (CD) spectroscopy and by measurement of the diffusion coefficient. The results are analyzed in the context of two complementary quantitative models, both of which are consistent with a single underlying physical model. Magnesium binding sites in the open state have an affinity on average higher than the affinity of those in the compact state, but formation of the compact state is accompanied by an increase in the number of binding sites. Consequently, at low Mg(2+) concentrations, Mg(2+) binds preferentially to the open state, favoring its formation, but at high concentrations, Mg(2+) binds preferentially to the compact state. The affinity of the riboswitch for SAM increases drastically with an increased level of binding of Mg(2+) to the compact pseudoknot conformation. The effect of increasing concentrations of trimethylamine N-oxide (TMAO), a well-studied molecular crowding agent, on the conformation of the riboswitch and its affinity for SAM were also monitored by CD spectroscopy and measurement of diffusion. In the absence of added Mg(2+), high concentrations of TMAO were found to induce a conformational change compatible with the formation of the pseudoknot form but have only a small effect on the affinity of the RNA for SAM.

Uncovering the thermodynamics of monomer binding for RNA replication

The nonenzymatic replication of primordial RNA is thought to have been a critical step in the origin of life. However, despite decades of effort, the poor rate and fidelity of model template copying reactions have thus far prevented an experimental demonstration of nonenzymatic RNA replication. The overall rate and fidelity of template copying depend, in part, on the affinity of free ribonucleotides to the RNA primer-template complex. We have now used (1)H NMR spectroscopy to directly measure the thermodynamic association constants, Kas, of the standard ribonucleotide monophosphates (rNMPs) to native RNA primer-template complexes. The binding affinities of rNMPs to duplexes with a complementary single-nucleotide overhang follow the order C > G > A > U. Notably, these monomers bind more strongly to RNA primer-template complexes than to the analogous DNA complexes. The relative binding affinities of the rNMPs for complementary RNA primer-template complexes are in good quantitative agreement with the predictions of a nearest-neighbor analysis. With respect to G:U wobble base-pairing, we find that the binding of rGMP to a primer-template complex with a 5'-U overhang is approximately 10-fold weaker than to the complementary 5'-C overhang. We also find that the binding of rGMP is only about 2-fold weaker than the binding of rAMP to 5'-U, consistent with the poor fidelity observed in the nonenzymatic copying of U residues in RNA templates. The accurate Ka measurements for ribonucleotides obtained in this study will be useful for designing higher fidelity, more effective RNA replication systems.

Analysis of the interaction with the hepatitis C virus mRNA reveals an alternative mode of RNA recognition by the human La protein

Human La protein is an essential factor in the biology of both coding and non-coding RNAs. In the nucleus, La binds primarily to 3' oligoU containing RNAs, while in the cytoplasm La interacts with an array of different mRNAs lacking a 3' UUU(OH) trailer. An example of the latter is the binding of La to the IRES domain IV of the hepatitis C virus (HCV) RNA, which is associated with viral translation stimulation. By systematic biophysical investigations, we have found that La binds to domain IV using an RNA recognition that is quite distinct from its mode of binding to RNAs with a 3' UUU(OH) trailer: although the La motif and first RNA recognition motif (RRM1) are sufficient for high-affinity binding to 3' oligoU, recognition of HCV domain IV requires the La motif and RRM1 to work in concert with the atypical RRM2 which has not previously been shown to have a significant role in RNA binding. This new mode of binding does not appear sequence specific, but recognizes structural features of the RNA, in particular a double-stranded stem flanked by single-stranded extensions. These findings pave the way for a better understanding of the role of La in viral translation initiation.

Experimental antitumor activity of the Ce(IV)-mitoxantrone complex and its interaction with deoxyribonucleic acid

The Ce(IV)-mitoxantrone complex exhibits a higher lethality to Ehrlich ascites tumor cells than that of the free drug and shows stronger inhibition ability on the DNA synthesis of the tumor cells. Thus the Ce(IV)-mitoxantrone complex may become a more potent antitumor drug than mitoxantrone. The different interaction model of mitoxantrone and its Ce(IV) complex with DNA were studied by the methods of spectroscopy, electrochemistry, and electrophoresis. Ce(IV) ions chelate with oxygens of the hydroxyl groups at the 1,4 position and the carbonyl function on C-9 and C-10, then intercalate into the base pairs of DNA together. The complexation of Ce(IV) gives rise to more compact binding of mitoxantrone with DNA, and leads to an additional change on the normal conformation and the double-helical structure of DNA; this may be related to the more stronger action of the complex on DNA synthesis and survival of cultured tumor cells.

Mercury(II) Site-Selective Binding to a DNA Hairpin. Relationship of Sequence-Dependent Intra- and Interstrand Cross-Linking to the Hairpin-Duplex Conformational Transition

Hg(II) interacted site selectively with only one of three deoxyribooligonucleotides examined; these "oligos" each had a different number of unmatched T residues. Thus, Hg(II) formed an intrastrand T-Hg-T cross-link between the first and fourth T residues of the hairpin, d(GCGCTTTTGCGC) (T4). The DNA strand formed a loop around the Hg, as if the Hg atom had been lassoed. The interactions of Hg(II) with two other oligos, d(ATGGGTTCCCAT) (T2) and d(GCGCTTTGCGC) (T3), were less specific. Previously, we found that at high DNA and salt concentrations, T2 was a mixture of hairpin and duplex forms while T3 and T4 had the hairpin form; modeling studies showed that in the free T4 hairpin the two T's at the ends of the (T)(4) loop form a T.T wobble base pair. Only in T4 are the T residues positioned to form an intrastrand cross-link readily. The Hg(II)-oligo adducts formed as a function of added Hg(II) were investigated by titrations monitored by UV, CD, and (1)H NMR spectroscopy. The appearance of a new set of (1)H signals with the concomitant decay of the free oligo (1)H signals indicated that 1:1 Hg(II):T2, 1.5:1 Hg(II):T3, and 1:1 Hg(II):T4 adducts were formed with Hg(NO(3))(2). In H(2)O, these adducts all had spectra with very downfield signals for the exchangeable TN(3)H and GN(1)H groups, a characteristic of base-paired regions. All upfield N(3)H signals from the (T)(2) and (T)(3) sequences of the free oligo disappeared in the spectra of the 1:1 Hg(II):T2 and 1.5:1 Hg(II):T3 adducts. The disappearance of the NH signals, the UV spectral changes, and the stoichiometries (1:1 Hg(II):T2 and 1.5:1 Hg(II):T3) indicate that these adducts are duplexes containing two and three T-Hg-T interstrand cross-links for T2 and T3, respectively. The (1)H and (13)C signals of the 1:1 Hg(II):T4 adduct in D(2)O were nearly completely assigned by 2D NMR spectroscopy. The spectrum of the adduct in H(2)O had only two of the four original TN(3)H signals from the (T)(4) sequence present in the spectrum of T4; this result is consistent with the presence of a TN3-Hg-TN3 cross-link. The (13)C chemical shift changes upon Hg(II) binding indicated that the TN3-Hg-TN3 cross-link was between the T's at each end of the (T)(4) loop. The NOESY, CD, and UV spectra were all consistent with a hairpin conformation for the 1:1 Hg(II):T4 adduct. A hairpin conformation also appeared reasonable from molecular modeling calculations. In conclusion, the length of the central (T)(n)() sequence influenced the type of T-Hg-T cross-link formed and, in turn, the conformation of the adducts. For (T)(2) and (T)(3), interstrand T-Hg-T cross-linking favored the duplex form. In contrast, for (T)(4), intrastrand T-Hg-T cross-linking stabilized the hairpin form.

Evidence from CD spectra that d(purine).r(pyrimidine) and r(purine).d(pyrimidine) hybrids are in different structural classes

CD spectra and difference CD spectra of four d(oligopurine).r(oligopyrimidine) and four r(oligopurine).d(oligopyrimidine) hybrid duplexes containing mixed A.T(U) and G.C base pairs were compared with the spectra of four DNA.DNA and four RNA.RNA oligomer duplexes of similar repeating sequences. The 16 duplexes were formed by mixing oligomers that were 24 nucleotides long. The buffer was 0.05 M Na+ (phosphate), pH 7.0. DNA.DNA and RNA.RNA oligomer duplexes were used as reference B-form and A-form structures. We found that the CD spectra of d(purine).r(pyrimidine) and r(purine).d(pyrimidine) hybrid duplexes were different from the CD spectra of either DNA.DNA or RNA.RNA duplexes. The data suggested that these hybrids have intermediate structures between A-form RNA and B-form DNA structures. The CD spectra of d(purine).r(pyrimidine) and r(purine).d(pyrimidine) hybrid duplexes were different from each other, but the hybrids in each class had consistent CD spectra as indicated by nearest-neighbor comparisons. Thus, it appeared that the two types of hybrids belonged to different structural classes. The negative 210 nm band found in difference CD spectra was correlated with the presence of an r(purine) strand in the hybrid duplexes. The melting temperatures (Tm values) of these hybrids were compared with the Tm values of the DNA.DNA and RNA.RNA duplexes. The order of the thermal stability was: RNA.RNA duplex > r(purine).d(pyrimidine) hybrid > DNA.DNA duplex > d(purine).r(pyrimidine) hybrid, when comparing analogous sequences.

A method for estimating the nearest neighbor base-pair content of RNAs using CD and absorption spectroscopy

CD and absorption spectra are sensitive to the secondary structure of RNAs. By fitting the spectra contained in our basis set to the CD and absorption spectra of an RNA of known sequence, we could determine the fractions of base pairs, the fractions of each of the nearest neighbor base pairs, and the fractions of the single-stranded nucleotides in that RNA. The basis set included 58 CD and 58 absorption spectra. The fitting was done with a guided selection routine. The estimated error was about 0.05 for predicting the fractions of the nearest neighbor base pairs, 0.06 for predicting the fractions of A.U, G.C, and G.U base pairs, and 0.04 for predicting the fractions of the single-stranded nucleotides.

A.U and G.C base pairs in synthetic RNAS have characteristic vacuum UV CD bands

The vacuum UV CD spectra of GpC, CpG, GpG, poly[r(A)], poly[r(C)], poly[r(U)], poly[r(A-U)], poly[r(G).r(C)], poly[r(A).r(U)], and poly[r(A-U).r(A-U)] were measured down to at least 174 nm. These spectra, together with the published spectra of poly[r(G-C).r(G-C)], CMP, and GMP, were sufficient to estimate the CD changes upon base pairing for four double-stranded RNAs. The vacuum UV CD bands of poly[r(A)], poly[r(C)], and the dinucleotides GpC and CpG were temperature dependent, suggesting that they were due to intrastrand base stacking. The dinucleotide sequence isomers GpC and CpG had very different vacuum UV CD bands, indicating that the sequence can play a role in the vacuum UV CD of single-stranded RNA. The vacuum UV CD bands of the double-stranded (G.C)-containing RNAs, poly[r(G).r(C)] and poly[r(G-C).r(G-C)], were larger than the measured or estimated vacuum UV CD bands of their constituent single-stranded RNAs and were similar in having an exceptionally large positive band at about 185 nm and negative bands near 176 and 209 nm. These similarities were enhanced in difference-CD spectra, obtained by subtracting the CD spectra of the single strands from the CD spectra of the corresponding double strands. The (A.U)-containing double-stranded RNAs poly[r(A).r(U)] and poly[r(A-U).r(A-U)] were similar only in that their vacuum UV CD spectra had a large positive band at 177 nm. The spectrum of poly[r(A).r(U)] had a shoulder at 188 nm and a negative band at 206 nm, whereas the spectrum of poly[r(A-U).r(A-U)] had a positive band at 201 nm. On the other hand, difference spectra of both of the (A.U)-containing polymers had positive bands at about 177 and 201 nm. Thus, the difference-CD spectra revealed CD bands characteristic of A.U and G.C base pairing. (ABSTRACT TRUNCATED AT 250 WORDS)

Structural differences between active and inactive mammalian 60S ribosomal subunits. Circular dichroism and electric birefringence studies

The structure and conformation of different active and inactive forms of the 60S rat liver ribosomal subunits have been analyzed by electric birefringence and circular dichroism. These studies show the following: 1) When a phosphate buffer is used instead of a triethanolamine buffer, there are major changes in RNA stacking, RNA-protein interactions, and particle orientation and conformation with no concomitant loss in ribosome activity. 2) The inactivated subunits by K(+)-depletion exhibit the same electro-optical and near-UV CD behaviour than the active subunits in phosphate buffer. 3) Inactivation by EDTA-treatment leads to drastic changes in RNA structure, RNA-protein interactions and subunit conformation; the 60S particles behave like free RNA, indicating the absence of any stabilization of rRNA by ribosomal proteins. 4) The inactivation of subunits by depletion of either monovalent or divalent cations is accompanied by a net decrease of the alpha-helicity of the ribosomal proteins. 5) The transition from active to inactive form of 60S subunits may involve protein modifications, likely dependent on a specific array of cations. 6) RNA has a certain degree of liberty within the subunits and one can suppose that this property is responsible for the flexible structure of ribosome.

Mg2+-induced proton release from Escherichia coli ribosome and ribosomal RNA

Escherichia coli ribosome released protons upon addition of Mg2+. The Mg2+-induced proton release was studied by means of the pH-stat technique. The number of protons released from a 70 S ribosome in the Mg2+ concentration range 1-20 mM was about 30 at pH 7 and 7.6, and increased to about 40 at pH 6.5. The rRNA mixture extracted from 70 S ribosome showed proton release of amount and of pH dependence similar to those of the 70 S ribosome but the ribosomal protein mixture released few. This indicates that rRNA is the main source of the protons released from ribosome. The pH titration of rRNA showed that the pKa values of nucleotide bases were downward shifted upon Mg2+ binding. This pKa shift can account for the proton release. The Scatchard plots of proton release from rRNA and ribosome were concave upward, showing that the Mg2+-binding sites leading to proton release were either heterogeneous or had a negative cooperativity. A model assuming heterogeneous Mg2+-binding sites is shown to be unable to explain the proton release. Electrostatic field effect models are proposed in which Mg2+ modulates the electrostatic field of phosphate groups and the potential change induces a shift of the pKa values of bases that leads to the proton release. These models can explain the main features of the proton release.

Secondary structures of influenza and Sendai Virus RNAs

The secondary structures of influenza and Sendai virus RNAs were investigated by thermal denaturation, circular dichroism and proflavine binding methods. In 0.1 M NaCl about 60% of the bases of both RNAs were involved in secondary structure. The melting temperatures (Tm) of both viral RNAs were linear functions of the logarithm of the sodium ion concentration in solution, but under all ionic conditions the melting temperatures of Sendai virus RNA were higher than those of influenza virus RNA. At all ionic strengths the melting range of Sendai virus RNA was less than influenza virus RNA, indicating that the helical regions in Sendai virus RNA were longer than those in influenza virus RNA. Although Sendai virus RNA had a higher thermal stability than influenza virus RNA, hyperchromicity and circular dichroism data showed that Sendai virus RNA had less G+C content (34%) within the double stranded regions than influenza virus RNA (48%). The binding isotherms of Sendai and influenza virus RNA-proflavine complexes were studied at different ionic strengths. The number of binding sites of proflavine with influenza virus RNA were significantly lower than those with Sendai virus RNA. These results demonstrate the essential difference between the secondary and tertiary structures of the RNAs under study.

Sedimentation of DNA in ethanol-water solutions within the interval of B to A transition

Sedimentation of DNA ethanol-water solutions has been studied over the range of ethanol concentrations corresponding to the B to A transition (65-80% ethanol, v/v). High ethanol concentrations (more than 75%) have been found to promote aggregate formation in solution. The molecular weight of DNA under fixed ionic conditions in solution (5x10(-4)M NaCl) has been shown to influence the value of ethanol concentration at which aggregates appear. On the other hand, the fact that DNA molecular weight has not been found to exert any influence on B to A transition curves obtained from CD measurements suggests that the changes observed in DNA CD spectra on adding ethanol to the solution are independent of aggregate formation. The date obtained show that, first, aggregation is not a necessary condition for the DNA transition from the B to the A-conformation and, second, changes in CD spectra of DNA under the influence of ethanol are not related to the process of aggregation.

The circular dichroism of ribosomal ribonucleic acids

1. The c.d. (circular dichroism) of Drosophila melanogaster rRNA (42% G+C) and of G+C-rich fragments (78% G+C) obtained by partial hydrolysis of rabbit L-rRNA (the largest RNA species isolated from the large subribosomal particle) were measured and found to differ substantially. 2. To interpret these spectra a relation between c.d. of bihelical RNA and % G+C was derived, namely delta epsilonfG = AFG2+bfG+c, where deltaepsilonfG is the c.d. of RNA characterized by a mole fraction, fG, of guanine nucleotides and a, b and c are constants. 3. A frame of reference was established by studying the c.d. of a range of rRNA species, including S-rRNA (the RNA species isolated from the smaller subribosomal particle) and L-rRNA of Escherichia coli. 4. It was found for the rRNA species studied that 0.60+/-0.05 of residues appear to form bihelical secondary structure. 5. A higher helical content, 0.66+/-0.05, was found for the G+C-rich fragment of L-rRNA. The difference in the c.d. of rabbit L-rRNA and of D. melanogaster rRNA is attributable to the dependence of c.d. of the bihelical parts on %G+C. 6. The minimum in c.d. at 295 nm increases with increasing %G+C. The c.d. of rRNA was compared with that of the parent subparticle in this region of the spectrum, where high precision may be attained.

The conformation of 16S RNA in the 30S ribosomal subunit from Escherichia coli

The digestion of E. coli 16S RNA with a single-strand-specific nuclease produced two fractions separable by gel filtration. One fraction was small oligonucleotides, the other, comprising 67.5% of the total RNA, was highly structured double helical fragments of mol. wt. 7,600. There are thus about 44 helical loops of average size corresponding to 12 base pairs in each 16S RNA. 10% of the RNA could be digested from native 30S subunits. Nuclease attack was primarily in the intraloop single-stranded region but two major sites of attack were located in the interloop single-stranded regions. Nuclease digestion of unfolded subunits produced three classes of fragments, two of which, comprising 80% of the total RNA, were identical to fragments from 16S RNA. The third, consisting of 20% RNA, together with an equal weight of peotein, was a resistant core (sedimentation coefficient 7S).

Physical properties of moloney murine leukemia virus high-molecular-weight RNA: a two subunit structure

The high-molecular-weight RNA of Moloney murine leukemia virus (MuLV) was analyzed by sedimentation equilibrium ultracentrifugation. Molecular weights of 7.2 x 10(6) and 3.4 x 10(6) were found for the native and subunit forms, respectively, indicating that the native structure is a dimer. S20,w and frictional coefficients were determined for MuLV RNA by analytical velocity centrifugation as a function of ionic strength. The apparent S20,w of native MuLV RNA was 47.3, 57.4, and 66.5 in 0.01, 0.1, and 0.20 M Na+, respectively; the corresponding frictional coefficients were 5.44, 4.48, and 3.87. Native RNA was estimated by circular dichroism to be 85% helical, whereas denatured RNA was 54% helical. Thermal denaturation profiles were obtained from uv absorbance scans. Melting temperatures of 57 and 68 C were obtained for high-molecular-weight RNA in 0.01 M Na+ and 0.122 M Na+, 1mM Mg2+, respectively. van't Hoff plots of the thermal denaturation data gave enthalpies for the helix-coil transition of 21,600 cal (ca. 90,500 J) per mol of cooperatively melting unit in high salt and 19,600 cal (ca. 82,100 J) per mol in low salt, consistent with both base stacking and pairing. The melting of Mu LV RNA occurred over a broad temprange and van't Hoff plots were linear over most of the melting range, indicating a noncooperative process of helix stabilization.

The contribution of RNA and non-histone proteins to the circular dichroism spectrum of chromatin

This paper is an investigation of the contribution of low salt extractable RNA and non-histone proteins to the circular dichroism of chromatin. Circular dichroism (CD) of chromatin above 250 nm is due mainly to DNA and is different from that of DNA free in solution. In addition, to a smaller extent, we find that low salt extractable RNA and/or non-histone protein side chain chromophores contribute significantly to the spectra in this region and account for the major differences observed among the CD spectra of chromatins isolated from the five tissues studied; pig cerebellum, myeloma, calf thymus, chick embryo brain, and chick erythrocytes.

Isolation, characterization, and stability of the 30S ribosomal RNA complex from HeLa cells

The HeLa 30S rRNA molecule (historically designated 28S rRNA) can be dissociated into two components, a 7S rRNA and a large rRNA component which we call 29S rRNA. To evaluate conformational differences between the 30S rRNA complex and the isolated 29S rRNA component of the complex, viscosity, sedimentation velocity, circular dichroism, and ultraviolet absorption measurements with the two species were performed. Sedimentation equilibrium studies were also carried out with the 30S rRNA complex. In addition, the kinetics of the reaction which dissociates the 30S rRNA complex were characterized. The removal of glycogen-like molecules by cetyltrimethylammonium bromide prescipitation of the rRNA and the preequilibration of rRNA with solvent by Sephadex column chromatography were found to be essential for reproducibility. The s20,2o values for the 30S rRNA complex and the isolated 29S rRNA were determined from the experimental data obtained at various rRNA concentrations as 29.89 plus or minus 0.40 and 29.09 plus or minus 0.14, respectively. The corresponding intrinsic viscosity values were 74 plus or minus 5 and 67 plus or minus 5 cm3/g, respectively. The optical properties of the 30S rRNA and 29S rRNA were not significantly different. These results indicate that there is no significant conformational difference between 30S rRNA and 29S rRNA under the conditions studied. We conclude from the sedimentation equilibrium data that the molecular weight of 30S rRNA is 2.1 x 10-6. From the kinetic data, the 30S rRNA dissociation appears to be an irreversible, cooperative, and ionic strength dependent reaction which at an ionic strength of 0.051 has an activation enthalpy of 123.5 kcal/mol and an activation entropy of 0.21 kcal/(mol deg).

Circular dichroism and fluorescence studies on potato virus X and its structural components

Circular dichroism (DC) measurements of the coat protein subunits of potato virus X show that native subunits that can reassemble with RNA to form infectious virus particles have appreciable alpha-helical structure. The CD of intact potato virus X was less intense below and more intense above 250 nm, and the maxima and minima were at longer wavelengths, than those of a CD spectrum computed from the individual contributions of the coat protein and RNA. The differences between the measured and computed spectra below 250 nm were attributed to the effects of differential light scattering and absorption flattening on measurements of the virus particle CD. The differences at longer wavelengths, were the CD contribution of the nucleic acid predominates, probably reflect the difference between a base-paired conformation of the RNA in solution and the more rigid single-stranded conformation imposed by the structure of the virus. The CD evidence suggests that the tertiary structure and potato virus X coat protein subunits in solution and in intact virus particles is similar. Both CD and fluorescence emission results indicate differences between the tryptophan environment in dissociated protein subunits and that in intact virus. These are attributed to local differences in subunit conformation or to the occurrence of intersubunit interactions involving tryptophan in the intact virus.