Direct assignment of the dihydrouridine-helix imino proton resonances in transfer ribonucleic acid nuclear magnetic resonance spectra by means of the nuclear Overhauser effect

The NMR resonances from the hydrogen-bonded ring NH protons in the dihydrouridine stem of Escherichia colt tRNA1Val have been assigned by experiments involving the nuclear Overhauser effect (NOE) between adjacent base pairs. Irradiation of the 8-14 tertiary resonance produced a NOE to base pair 13. Irradiation of the CG13 ring NH produced NOEs to base pairs 12 and 14. Similarly, base pair 12 was shown to be dipolar coupled to 11 and 13, and base pair 11 was found to be coupled to 10 and 12. These sequential connectivities led to the assignment of CG13 at -13.05 ppm, UA12 at -13.84 ppm, CG11 at -12.23 ppm, and GC10 at -12.60 ppm. The results are compared with previous, less direct assignments for these four base pairs and with the expected proton positions from the crystal structure coordinates for this helix.     

Assignment of the low field proton nuclear magnetic resonance spectrum of yeast phenylalanine transfer RNA to specific base pairs

High-resolution proton nuclear magnetic resonance spectra at 220 and 300 MHz have been used to investigate the base-pairing structure of fragments of yeast tRNA^Phe, of chemically modified tRNA^Phe and of intact tRNA^Phe. To a very good approximation the positions of the fragment spectra are additive within 0·2 part per million, indicating that factors responsible for certain structural features in the intact molecule are already present in the smaller fragments (half molecules, hairpins and $\text{3}\text{4}$ molecules). A simple first-order ring-current shift theory taken in conjunction with the cloverleaf model for tRNA^Phe (RajBhandary et al., 1967) has been used to predict the low-field (? 15 to ?11 part per million) nuclear magnetic resonance spectra and make assignments of the resolved resonances to ring NH protons of specific base pairs. The general agreement between the predicted and observed spectra to within 0·2 part per million confirms in detail the cloverleaf model for the secondary structure of tRNA^Phe in solution. It is also established that ring-current shifts are the principal factor responsible for the wide range of shifts observed in the low-field spectra. As a result it is evident that the resonances are very sensitive to small changes in the secondary structure and in some cases changes in the interbase distance as small as 0·2 Å could easily be detected. It is also clear from the analysis that certain of the resonances are sensitive to the tertiary structure of the molecule and specific examples are discussed. As with our previous study, we find no evidence for any strong Watson-Crick type base pairs beyond those predicted by the cloverleaf structure.     

Ring-current shifts in the 300 MHz nuclear magnetic resonance spectra of six purified transfer RNA molecules

We present the 300 MHz high-resolution proton nuclear magnetic resonance spectra of the ring NH hydrogen-bonded protons of six purified tRNAs. Good agreement was obtained between the observed spectra and those computed on the assumption of the suitable cloverleaf models. In the computation it is assumed that the hydrogen-bonded ring NH in each type of base pair has an intrinsic position with respect to 2,2-dimethyl-2-silapentane-5-sulfonate, i.e. in A·U it is at ?14·8 parts per million, in G·C at ?13·7 parts per million and in A·Ψat ?13·5 parts per million. The shifts of these resonances from these positions are calculated by including ring current fields from the nearest neighbors. The agreement is very good, adding support to our earlier findings that there is no evidence for additional Watson-Crick base pairs detected beyond those in the cloverleaf. In general, resolved resonances are fitted by the computed spectra to within ±0·2 part per million showing that there is no need for any additional physical mechanism to explain the nuclear magnetic resonance positions. Hence, the nuclear magnetic resonance spectra can be interpreted in terms of the structure of their neighbors and in a few important cases this has been particularly valuable in understanding the structure beyond the end of a helical region. In the tRNA^Glu_E.coli′ for example, the positions of the resonances in A·U no. 7 and A·U no. 49 at the interior ends of the acceptor and -T-Ψ-C- stems, respectively, strongly suggest that these two stems are in a continuous helix. Other structural effects at the ends of the helical regions are also suggested by the nuclear magnetic resonance spectra.     

Investigation of the base-pairing structure of the anticodon hairpin from E. coli initiator tRNA by high-resolution nmr

The high-resolution nmr spectrum of the anticodon hairpin from E. coli tRNA^fMet has been obtained at a number of different temperatures. The positions of the resonances from interior Watson-Crick base pairs are well accounted for (within 0.1 ppm) by a semi-empirical ring current shift theory, but the terminal base pairs are susceptible to the exact orientation of adjacent bases in single-stranded regions. From a careful examination of the exact way in which resonances disappear at elevated temperatures, we conclude that melting in the nmr experiments occurs when the lifetime of a base pair is reduced to several milliseconds. On the basis of these experiments we are able to assign an nmr T_m to each individual base pair and these should be useful in interpreting the melting behavior of the intact molecule. An “extra” resonance is observed at ～11.3 ppm and, on the basis of its position and temperature sensitivity, it is tentatively assigned to the ring nitrogen proton of a “protected” U residue in the anticodon loop. A strong preference for stacking of a nonbase-paired A residue on an adjacent GC base pair is observed even at temperatures in excess of 52°C.     

NMR-based structure of anticancer drug mitoxantrone stacked with terminal base pair of DNA hexamer sequence d-(ATCGAT)2

Mitoxantrone is a promising antitumor drug having considerably reduced cardiotoxicity as compared to anthracyclines. Its binding to deoxyhexanucleotides sequence d-(ATCGAT)₂ has been studied by proton and phosphorous-31 nuclear magnetic resonance spectroscopy. The stoichiometry reveals that 1:1 and 2:1 mitoxantrone-d(ATCGAT)₂ complexes are formed in solution. Significant upfield shifts in 6H/7H, 2H/3H, 11NH, and 12NH protons (～.5?ppm) of mitoxantrone and T6NH imino protons (～.3?ppm) are observed. The phosphorous resonances do not shift significantly indicating that the base pairs do not open at any nucleotide step along the sequence of hexamer. Several inter-molecular Nuclear Overhauser Enhancement connectivities between mitoxantrone and hexanucleotide protons indicate that mitoxantrone chromophore stacks with terminal A1-T6 base pair and side chains involving 12CH₂, 12NH, and 14OH protons are in close proximity of A1, T2, A5, and T6 bases. Absorption and emission spectra show red shift in wavelength maxima, which is characteristic of stacking interaction. At higher mitoxantrone to nucleic acid ratios, electrostatic interactions are dominant. The 2:1 drug/DNA stoichiometric structure obtained by restrained Molecular Dynamics simulations shows considerable distortions in backbone torsional angles and helicoidal parameters although structural fluctuations in 25?ps analysis of trajectory are found to be negligible. Mitoxantrone binds as a monomer at either or both ends of hexamer externally with side chains interacting specifically with DNA. The findings are relevant to the understanding of pharmacological action of drug.     

Imino 1H- and 31P-NMR analysis of the interaction of propidium and ethidium with DNA

At low temperature and low salt concentration, both imino proton and ³¹p-nmr spectra of DNA complexes with the intercalators ethidium and propidium are in the slow-exchange region. Increasing temperature and/or increasing salt concentration results in an increase in the site exchange rate. Ring-current effects from the intercalated phenanthridinium ring of ethidium and propidium cause upfield shifts of the imino protons of A · T and G · C base pairs, which are quite similar for the two intercalators. The limiting induced chemical shifts for propidium and ethidium at saturation of DNA binding sites are approximately 0.9 ppm for A · T and 1.1 ppm for G · C base pairs. The similarity of the shifts for ethidium and propidium, in both the slow- and fast-exchange regions over the entire titration of DNA, shows that a binding model for propidium with neighbor-exclusion binding and negative ligand cooperativity is correct. The fact that a unique chemical shift is obtained for imino protons at intercalated sites over the entire titration and that no unshifted imino proton peaks remain at saturation binding of ethidium and propidium supports a neighbor-exclusion binding model with intercalators bound at alternating sites rather than in clusters on the double helix. Addition of ethidium and propidium to DNA results in downfield shifts in ³¹P-nmr spectra. At saturation ratios of intercalator to DNA base pairs in the titration, a downfield shoulder (approximately ?2.7 ppm) is apparent, which accounts for approximately 15% of the spectral area. The main peak is at ?3.9 to ?4.0 ppm relative to ?4.35 in uncomplexed DNA. The simplest neighbor-binding model predicts a downfield peak with approximately 50% of the spectral area and an upfield peak, near the chemical shift for uncomplexed DNA, with 50% of the area. This is definitely not the case with these intercalators. The observed chemical shifts and areas for the DNA complexes can be explained by models, for example, that involve spreading the intercalation-induced unwinding of the double helix over several base pairs and/or a DNA sequence- and conformation-dependent heterogeneity in intercalation-induced chemical shifts and resulting exchange rates.     

Assignment of the histidine 12-threonine 45 hydrogen-bonded proton in the NMR spectrum of ribonuclease A in H2O.

Described herein are proton nmr experiments on chemically modified derivatives of ribonuclease A designed to elucidate the origin of an exchangeable resonance, assigned previously to a histidine ring N proton that titrates between 11 to 13 ppm with a pK_a of 6.1 in H₂O solution. Histidines 48 and 105, which are distant from the active site, are eliminated as candidates for this resonance from inhibitor binding studies on the enzyme in acetate–water solutions. This exchangeable resonance titrates with modified pK_a's and constant area over the above pH range in His-119-N₁-carboxymethylated-RNase A and des-(121–124)-RNase A, thus eliminating the imidazole N₃ proton in the His 119-Asp 121 hydrogen bond. In His-12-N₁-carboxymethylated-RNase A, this resonance is also observable, but broadens on raising the pH above 7 and at elevated temperatures above neutrality. It exhibits a pH-independent chemical shift characteristic of the protonated state of histidine. On the basis of these findings, this exchangeable resonance, designated a, is assigned to the imidazole N₁ proton of His 12, which is hydrogen-bonded to the carbonyl oxygen of Thr 45 in the crystal.     

Specificity in DNA interactions: an nmr investigation of the interaction of propidium with oligodeoxyribonucleotides containing normal and G-T base pairs

The interaction of propidium with three self-complementary oligodeoxyribonucleotides has been investigated by ¹H- (base-pair imino proton assigned by 1D NOE and saturation transfer methods) and ³¹P-nmr as a function of ratio of propidium to oligomer (from zero to saturation) and temperature. The three oligomers are dTATATGCGCATATA (1), dTATATGTGCATATA (2), which has the same sequence as 1 except for the mismatched base pair at position 7, and dTATGTGCATA (3), which is a shortened version of 2. The imino proton chemical-shift changes of 1 on titration with propidium can be explained by the effects of the ring-current anisotropy of propidium at intercalation (3.4 Å) and next-neighbor sites (6.8 Å). The results indicate that propidium binds with neighbor exclusion but with no significant specificity for any intercalation site in the sequence of 1. The addition of propidium to 1 results in general downfield shifts of all ³¹P signals, as expected for a nonspecific intercalator. Imino and ³¹P-nmr spectra for 2 indicate that this oligomer forms a hydrogen-bonded G · T base pair at position 7 with little change in base pairing and stacking of base pairs 1–6 compared to 1. The results for addition of propidium to 2 and 3 are quite different than with 1. At low ratio only secondary shifts (6.8 Å) are seen for the G and T imino protons of base-pair 7 on addition of propidium. At higher ratios of propidium, the signals for these G and T protons are lost in 2 and severely broadened in 3, even at low temperature. The other potential intercalation sites in 2 and 3 appear to bind propidium strongly and without significant specificity as with 1. ³¹P spectra of 2 in the presence of propidium show the expected downfield shifts and broadening. Thus, the minor differences in local helix geometry in 1, and in 2 and 3, away from the G · T base pair do not significantly affect propidium intercalation specificity. Having one or two G · T base pairs at a site, however, makes intercalation in the standard manner significantly less favorable.     

Evaluation of base-pairing schemes for E. coli 5S RNA by 400 MHz proton nuclear magnetic resonance spectroscopy

The number of base pairs in the denatured “B” form of $\text{E. coli}$ 5S RNA has been determined directly from 400 MHz high resolution proton nuclear magnetic resonance spectroscopy. The experimental NMR spectrum from ?11.6 to ?14.5 ppm from a sodium 2,2-dimethyl-2-silapentane sulfonate reference can be simulated by a theoretical spectrum consisting of 33 Lorentzian lines of equal width (corresponding to 33 base pairs) at 26°C. This result is inconsistent with previously proposed secondary structures of 17 and 23 base pairs, but is readily adapted to the Luoma-Marshall cloverleaf secondary structure.     

Syn–anti equilibrium of purine bases in dinucleoside monophosphates as studied by proton longitudinal relaxation

The preferential orientations of the purine bases in dinucleoside monophosphates such as ApA, ApG, and GpA in 10^?2M neutral aqueous solutions have been investigated by proton relaxation at 250 MHz. These orientations are deduced from computer simulations of the magnetization recovery curves following a 180° nonselective pulse. The distances between the H(8) proton of a base and the ribose ring protons which are used in these calculations are obtained by minimization as a function of the glycosyl torsion angle ? of the standard deviation between the isotropic reorientation correlation times τ_R derived from the relaxation rates of these protons. The average H(1′) – H(8) distance obtained by this procedure may be readily verified from the reduction of the H(1′) relaxation rate when H(8) is substituted by a deuteron. The limits of validity of the assumption of a single correlation time τ_R governing the proton relaxation have been estimated, taking into account several possible internal motions, e.g., the rotation of the base, of the methylene exocyclic group and the N ? S interconversion of the ribose ring. For 10^?10 < τ_R < 2 × 10^?10 sec, it appears that the influence of these motions on the proton relaxation becomes perceptible when the jump rates among equilibrium positions exceed ca. 10⁹ sec^?1. The whole of the experimental results show that for the ribose ring N conformer, the orientation of the bases is found in the ranges 60° < ? < 80° (syn) and 180° < ? < 210° (anti). For ribose S conformer, it is observed that this orientation is mainly syn with 5° < ? < 90°. The average H(1′) – H(8) distance provides semiquantitative information on the overall syn or anti orientations of the base in each nucleoside moiety. At 298 K the population of the anti conformer is found to increase in the order A- pG < Ap -G ～ Gp -A < Ap -A < A-pA < G-pA . A more detailed analysis of relaxation data shows that the maximum possible fraction of the stacked form of dinucleotides, due to the occurrence of N-anti conformers in both nucleoside moieties, is in the order ApG < GpA < ApA, in agreement with previous works, with however smaller values. Lastly the deuteron linewidth in position 8 of the bases indicates a syn–anti transition rate of the order of 10⁹ sec^?1 at room temperature, without noticeable effects therefore on the proton relaxation.     

Molecular-Mechanical studies of the mismatched base analogs of d(CGCGAATTCGCG)2:d(CGTGAATTCGCG)2, d(CGAGAATTCGCG)2, d(CGCGAATTCACG)2, d(CGCGAATTCTCG)2, and d(CGCAGAATTCGCG)·d(CGCGAATTCGCG)

Molecular-mechanical simulations have been carried out on “mismatched base” analogs of the DNA double-helical structure d(CGCGAATTCGCG)₂, in which the base pairs CG at the 3 and 10 positions have been replaced by CA, AG, TC, and TG base pairs, as well as an insertion analog in which an extra adenine has been incorporated into one strand of the above structure between bases 3 and 4. The results of these simulations (calculated relative stabilities, structures, and nmr ring-current shifts) have been compared with calorimetric and nmr data. The calculated relative stabilities of the double-helical parent dodecamer and the various “wobble” base pairs qualitatively correlate with the experimental melting temperatures. The base-pairing structure for the GT wobble pair is in agreement with that previously determined from nmr experiments. For the GA base pair, the structure with both bases anti has a slightly more favorable energy from base pairing and stacking than a structure with non-Watson-Crick H-bonding with adenine syn, in agreement with nmr experiments. The CA wobble base is calculated to favor an adenine 6NH₂ …? cytosine N3 H-bond over cytosine 4NH₂ …? adenine N1, again, in agreement with nmr experiments. There is no definitive experimental data on the TC base pair, but the existence of (somewhat long and weak) H-bonds involving cytosine 4NH₂ …? thymine 4CO and cytosine N3 …? thymine HN3 seems reasonable. We find a structure in which the extra adenine base of the insertion analogs sits “inside” the double helix.     

Base pair mismatches and carcinogen-modified bases in DNA: an NMR study of G.T and G.O4meT pairing in dodecanucleotide duplexes

High-resolution two-dimensional NMR studies have been completed on the self-complementary d(C-G-C-G-A-G-C-T-T-G-C-G) duplex (designated G.T 12-mer) and the self-complementary d(C-G-C-G-A-G-C-T-O4meT-G-C-G) duplex (designated G.O4meT 12-mer) containing G.T and G.O4meT pairs at identical positions four base pairs in from either end of the duplex. The exchangeable and nonexchangeable proton resonances have been assigned from an analysis of two-dimensional nuclear Overhauser enhancement (NOESY) spectra for the G.T 12-mer and G.O4meT 12-mer duplexes in H2O and D2O solution. The guanosine and thymidine imino protons in the G.T mismatch resonate at 10.57 and 11.98 ppm, respectively, and exhibit a strong NOE between themselves and to imino protons of flanking base pairs in the G.T 12-mer duplex. These results are consistent with wobble pairing at the G.T mismatch site involving two imino proton-carbonyl hydrogen bonds as reported previously [Hare, D. R., Shapiro, L., & Patel, D. J. (1986) Biochemistry 25, 7445-7456]. In contrast, the guanosine imino proton in the G.O4meT pair resonates at 8.67 ppm. The large upfield chemical shift of this proton relative to that of the imino proton resonance of G in the G.T mismatch or in G.C base pairs indicates that hydrogen bonding to O4meT is either very weak or absent. This guanosine imino proton has an NOE to the OCH3 group of O4meT across the pair and NOEs to the imino protons of flanking base pairs.(ABSTRACT TRUNCATED AT 250 WORDS)     

Correlation of exchangeable (NH) and nonexchangeable (C2H) histidine resonances in the proton NMR spectrum of ribonuclease A in aqueous solution.

The ionization characteristics of the hydrogen-bonded His 12 N₁ proton observed to titrate between 11 to 13 ppm in the nmr spectrum of ribonuclease A in H₂O solution are compared with the ionization characteristics of the four histidine C₂ protons in the enzyme. Comparison of the pK_a's of the enzyme in H₂O and D₂O in the absence and presence of cytidine monophosphate (?5′, ?3′, and ?2′) inhibitors, line widths in the presence of Cu II at pH 3.6 and 5.6, and chemical shifts in the presence of AgNO₃ permit a correlation of the exchangeable His 12 N₁ proton with the active site histidine C₂ proton exhibiting the lower ionization pK_a. The histidines with pK_a of 5.1 and 5.6 in ribonuclease A in the absence of salt are assigned in this study to His 12 and His 119, respectively.     

Nuclear Overhauser effect study and assignment of D stem and reverse-Hoogsteen base pair proton resonances in yeast tRNAAsp

Nuclear Overhauser effects (NOEs) in yeast tRNAAsp were found for all four GU and G psi base pairs. NOEs of both reverse-Hoogsteen pairs were identified by comparison with a purine C8 deuterated sample. Several NOEs involving these resonances were also found which are clearly between single protons on adjacent base pairs. These interbase NOEs, combined with the assumption of reasonable similarity between the structure of yeast tRNAAsp and that of yeast tRNAPhe, lead to unambiguous assignment of many resonances including all the ring NH and C2 protons in the D stem. The stability of the stem at 28 degrees C, as recently deduced by Moras et al (Nature 288 669-674), from x-ray diffraction is confirmed. Assignments of the ring NH resonances of T54-A58 and of a G psi pair are made for the first time.     

Intramolecular proton transfer in adenine imino tautomers

The electronic structural impact on intramolecular proton transfer in the cis- and trans-imino N7 and N9 tautomers of adenine (A) has been studied quantum mechanically, using density functional theory (B3LYP/TZVP, SAOP/TZ2P, LB94/TZ2P) and Green function (OVGF/TZVP) models. It is found that proton transfer does not significantly change isotropic properties but has profound impact on electron distributions of the species through anisotropic properties. The relative energies with respect to the canonical A tautomer (amino-9H), ΔE, for imino 7Hcis, imino 7Htrans, imino 9Hcis and imino 9Htrans are calculated as 16.15, 16.43, 18.46 and 13.80 kcal mol^? 1 (B3LYP/TZVP model) and some minor changes in perimeters of the purine ring is also observed. The Hirshfeld atomic charges indicate that whether a proton attached to N₍₇₎ or N₍₉₎ causes a significant local charge redistribution. However, these charges are insensitive to cis–trans proton transfer. Condensed Fukui function reveals N₍₁₀₎ and C₍₈₎ as the most electrophilic reactive site among N- and C-atom sites, respectively. We also found that proton transfer significantly alters in-plane σ orbitals, rather than out of plane π orbitals including the frontier orbital 6a″. Moreover, orbital based responses to various proton transfers are presented: the orbital 29a′ (HOMO-1) is a signature orbital differentiating all the four tautomers. Orbital 27a′ is a site (N₍₇₎ and N₍₉₎) sensitive orbital, whereas orbital 22a′ is only sensitive to proton orientation on the imino group = N–H.     

Proton nuclear magnetic resonance investigations of fraying in double-stranded d-ApTpGpCpApT in H2O solution.

The chemical shifts and line widths of the Watson-Crick ring NH resonances of the self-complementary duplex of d-ApTpGpApT have been monitored at low ionic strength and in the presence of Mg ions at neutral pH in aqueous solution to determine the thermodynamic parameters associated with fraying (D. J. Patel (1974), Biochemistry 13, 2396) at the terminal and internal base pairs as a function of temperature and pH. From studies in H2O-MeOH (3:2), the fraying process persists down to approximately -20 degrees for the internal TA base pair and down to and probably beyond -30 degrees for the terminal AT base pair. The observed average chemical shift at each of these base pairs as a function of temperature suggests rapid exchange on the nuclear magnetic resonance (NMR) time scale between helix and coil (chemical shift separation of 3.2 ppm) and have been utilized to determine the dissociation constant at the terminal and internal base pairs. Comparison of the reaction enthalpies elucidated from the chemical shift parameters with those reported from optical studies suggests that the symmetry related internal TA base pairs break in a coupled manner at low ionic strength, with the coupling removed in the presence of Mg ions and high salt. By contrast, the symmetry related terminal AT base pairs break independently of each other in the absence and presence of Mg ions and high salt. The terminal base pair exhibits a Tm of 10-15 degrees lower than that of the internal base pair in the hexanucleotide, with divalent Mg ions and high salt stabilizing the double helix as reflected in the Tm values of these base pairs. The observed line width changes as a function of temperature provide an estimate of the exchange rate of the proton from the coil form with water. The exchange reaction from the coil state is base catalyzed with rate constants in the diffusion limit.     

Investigation of the thermal unfolding of secondary and tertiary structure in E. coli tRNAfMet by high-resolution nmr

The high-resolution (300 MHz) proton nmr spectrum of E. coli tRNA^fMet has been examined in 0.17M NaCl, with and without Mg²⁺, and at various temperatures. In light of recent studies of other E. coli tRNA and fragments of tRNA^fMet, some low field (11–15 ppm) resonances previously assigned to secondary structure base pairs are reassigned to a tertiary structure A₁₄–S⁴U₈ base pair and a protected uridine residue in the anticodon loop. These two resonances and other low field resonances which are assigned to secondary structure base pairs are used to monitor the thermal unfolding of the molecule. In the absence of Mg²⁺ the tertiary structure base pair is present only to ～45°C, but in the presence of Mg²⁺ it remains until at least 70°C. Analysis of the temperature dependence of other low field resonances indicates that the melting of the dihydrouridine stem occurs more or less simultaneously with the loss of tertiary structure. The observation of the resonance from the A₁₄–S⁴U₈ base pair proves that tertiary structure is present in this molecule below 40°C, even in the absence of Mg²⁺.     

Conformational analysis of thyrotropin releasing factor by proton magnetic resonance spectroscopy

The proton magnetic resonance spectrum of thyrotropin releasing factor (TRF) in solution in deuterium oxide and deuterated dimethylsulfoxide (DMSO–d₆) has been analyzed. Two forms differing in cis–trans isomerism about the His-Pro peptide bond are observed. From the temperature dependence of chemical shift of the amide protons, it is concluded that TRF in DMSO–d₆ does not contain intramolecular hydrogen bonds. Measurement of NH? C_αH coupling constant provides an estimate of the histidine dihedral angle ?. Structural information about the histidine side-chain is deduced from C_αH? C_βH coupling constants and from the nonequivalence of the two prolyl δ-protons. In DMSO–d₆, there is evidence for a tautomeric equilibrium corresponding to an exchange of imidazole proton between the two nitrogen atoms N-δ and N-ε. In water, the N-εH tautomer is found to be the predominant tautomeric form of the imidazole ring. These results in combination with energy calculation, vibrational analysis, and carbon nmr studies allow the determination of the conformationof TRF.     

Imino proton assignments in the proton nuclear magnetic resonance spectrum of the lambda phage OR3 deoxyribonucleic acid fragment

The 17 base pair duplex d(TATCACCGCAAGGGATAp) . d(TATCCCTTGCGGTGATAp) corresponding to the OR3 operator site of lambda phage has been synthesized and studied by 1H nuclear magnetic resonance spectroscopy at 470 MHz. The 13 imino proton resonances observed at 20 degrees C have been assigned to specific base pairs at positions 3-15 on the basis of nuclear Overhauser effect measurements and studies of the temperature dependence of peak intensities. Resonances from the A-T base pairs at positions 1, 2, 16, and 17 are assumed to be absent from the spectrum because of terminal fraying. Resonance from many of the base pairs suggested by Ohlendorf et al. [Ohlendorf, D. H., Anderson, W. F., Fisher, R. G., Takeda, Y., & Matthews, B. W. (1982) Nature (London) 298, 718-723] to be involved in specific binding of the lambda phage cro repressor are well resolved.     

Free energy of imperfect nucleic acid helices. II. Small hairpin loops

Physical studies of enzymically synthesized oligonucleotides of defined sequence are used to evaluate quantitatively the stability of small RNA hairpin loops and helices. The series (Ap)₄G(pC) _N(pU)₄, N = 4, 5 or 6, exists as monomolecular hairpin helices when N ≥ 5, and as imperfect dimer helices when N ≤ 4. In this size range, hairpin loops become more favorable (less destabilizing thermodynamically) as they increase in size from 3 to 4 to 5 unbonded nucleotides. Very small hairpin loops are particularly destabilizing; molecules whose base sequence would imply a hairpin loop of three nucleotides will generally exist with a loop of five, including a broken terminal base pair.Thermodynamic parameters for base pair and loop formation are calculated by a method which makes unnecessary the use of measured enthalpies of polynucleotide melting. Literature data on oligonucleotide double helices yield estimates of the free energy contribution from each of the six types of stacking interactions between three possible neighboring base pairs. The advantage of this approach is that the properties of oligonucleotides are used in predicting the stability of small RNA helices, avoiding the long extrapolation from the properties of high polymers.We provide Tables of temperature-dependent free energies that allow one to predict the stability and thermal transition temperature of many simple RNA secondary structures (applicable to ~1 m-Na⁺ concentration). As an example, we apply the rules to an isolated fragment of tRNA^Ser (yeast) (Coutts, 1971), whose properties were not used in calculating the free-energy parameters. The experimental melting temperature of 88 °C is predicted with an error margin of 5 deg. C.