Detection of a major conformational change in transfer ribonucleic acid by laser light scattering

Examinations of tRNA Range of Motion Using Simulations of Cryo-EM Microscopy and X-Ray Data

We examined tRNA flexibility using a combination of steered and unbiased molecular dynamics simulations. Using Maxwell's demon algorithm, molecular dynamics was used to steer X-ray structure data toward that from an alternative state obtained from cryogenic-electron microscopy density maps. Thus, we were able to fit X-ray structures of tRNA onto cryogenic-electron microscopy density maps for hybrid states of tRNA. Additionally, we employed both Maxwell's demon molecular dynamics simulations and unbiased simulation methods to identify possible ribosome-tRNA contact areas where the ribosome may discriminate tRNAs during translation. Herein, we collected >500 ns of simulation data to assess the global range of motion for tRNAs. Biased simulations can be used to steer between known conformational stop points, while unbiased simulations allow for a general testing of conformational space previously unexplored. The unbiased molecular dynamics data describes the global conformational changes of tRNA on a sub-microsecond time scale for comparison with steered data. Additionally, the unbiased molecular dynamics data was used to identify putative contacts between tRNA and the ribosome during the accommodation step of translation. We found that the primary contact regions were H71 and H92 of the 50S subunit and ribosomal proteins L14 and L16.

Analyzing the flexibility of RNA structures by constraint counting

RNA requires conformational dynamics to undergo its diverse functional roles. Here, a new topological network representation of RNA structures is presented that allows analyzing RNA flexibility/rigidity based on constraint counting. The method extends the FIRST approach, which identifies flexible and rigid regions in atomic detail in a single, static, three-dimensional molecular framework. Initially, the network rigidity of a canonical A-form RNA is analyzed by counting on constraints of network elements of increasing size. These considerations demonstrate that it is the inclusion of hydrophobic contacts into the RNA topological network that is crucial for an accurate flexibility prediction. The counting also explains why a protein-based parameterization results in overly rigid RNA structures. The new network representation is then validated on a tRNA(ASP) structure and all NMR-derived ensembles of RNA structures currently available in the Protein Data Bank (with chain length >/=40). The flexibility predictions demonstrate good agreement with experimental mobility data, and the results are superior compared to predictions based on two previously used network representations. Encouragingly, this holds for flexibility predictions as well as mobility predictions obtained by constrained geometric simulations on these networks. Potential applications of the approach to analyzing the flexibility of DNA and RNA/protein complexes are discussed.

Vibrational dynamics of transfer RNAs: comparison of the free and synthetase-bound forms

The vibrational dynamics of transfer RNAs, both free, and complexed with the cognate synthetase, are analyzed using a model (Gaussian network model) which recently proved to satisfactorily describe the collective motions of folded proteins. The approach is similar to a normal mode analysis, with the major simplification that no residue specificity is taken into consideration, which permits us (i) to cast the problem into an analytical form applicable to biomolecular systems including about 10(3 )residues, and (ii) to acquire information on the essential dynamics of such large systems within computational times at least two orders of magnitude shorter than conventional simulations. On a local scale, the fluctuations calculated for yeast tRNAPhe and tRNAAsp in the free state, and for tRNAGln complexed with glutaminyl-tRNA synthetase (GlnRS) are in good agreement with the corresponding crystallographic B factors. On a global scale, a hinge-bending region comprising nucleotides U8 to C12 in the D arm, G20 to G22 in the D loop, and m7G46 to C48 in the variable loop (for tRNAPhe), is identified in the free tRNA, conforming with previous observations. The two regions subject to the largest amplitude anticorrelated fluctuations in the free form, i.e. the anticodon region and the acceptor arm are, at the same time, the regions that experience the most severe suppression in their flexibilities upon binding to synthetase, suggesting that their sampling of the conformational space facilitates their recognition by the synthetase. Likewise, examination of the global mode of motion of GlnRS in the complex indicates that residues 40 to 45, 260 to 270, 306 to 314, 320 to 327 and 478 to 485, all of which cluster near the ATP binding site, form a hinge-bending region controlling the cooperative motion, and thereby the catalytic function, of the enzyme. The distal beta-barrel and the tRNA acceptor binding domain, on the other hand, are distinguished by their high mobilities in the global modes of motion, a feature typical of recognition sites, also observed for other proteins. Most of the conserved bases and residues of tRNA and GlnRS are severely constrained in the global motions of the molecules, suggesting their having a role in stabilizing and modulating the global motion.

Dynamics of transfer RNAs analyzed by normal mode calculation

Normal mode calculation is applied to tRNAPhe and tRNAAsp, and their structural and vibrational aspects are analyzed. Dihedral angles along the phosphate-ribose backbone (alpha, beta, gamma, epsilon, zeta) and dihedral angles of glycosyl bonds (chi) are selected as movable parameters. The calculated displacement of each atom agrees with experimental data. In modes with frequencies higher than 130 cm-1, the motions are localized around each stem and the elbow region of the L-shape. On the other hand, collective motions such as bending or twisting of arms are seen in modes with lower frequencies. Hinge axes and bend angles are calculated without prior knowledge. Movements in modes with very low frequencies are combinations of hinge bending motions with various hinge axes and bend angles. The thermal fluctuations of dihedral angles well reflect the structural characters of transfer RNAs. There are some dihedral angles of nucleotides located around the elbow region of L-shape, which fluctuate about five to six times more than the average value. Nucleotides in the position seem to be influential in the dynamics of the entire structure. The normal mode calculation seems to provide much information for the study of conformational changes of transfer RNAs induced by aminoacyl-tRNA synthetase or codon during molecular recognition.

Dynamic light scattering by kappa- and lambda-carrageenan solutions

The intensity correlation functions of kappa- and lambda-carrageenan in various salt solutions and at different concentrations have been determined with the help of dynamic light scattering. From the first cumulant of these correlation functions the values of the translational diffusion coefficients D have been derived. They increase with macromolecular concentration. The extrapolated values to infinite dilution of the diffusion coefficients increase with increasing salt concentration as expected from the salt concentration dependence of the r.m.s. radii of gyration determined previously by static light scattering. The translational diffusion coefficient of lambda-carrageenan in 0.1 M NaCl is smaller than the corresponding value for the kappa species. This is consistent with the difference in contour length and linear charge density of the two samples used. No satisfactory interpretation for the concentration dependence of the diffusion coefficient seems to be possible at present. Although current theories for the macromolecular and salt concentration dependence of D, taking into account charge effects, seem to be applicable, they do not allow for a consistent interpretation of the data. No specific difference between the solution behaviour of kappa- and lambda-carrageenan has been detected.

Traveling waves of in vitro evolving RNA

Populations of short self-replicating RNA variants have been confined to one side of a reaction-diffusion traveling wave front propagating along thin capillary tubes containing the Q beta viral enzyme. The propagation speed is accurately measurable with a magnitude of about 1 micron/sec, and the wave persists for hundreds of generations (of duration less than 1 min). Evolution of RNA occurs in the wavefront, as established by front velocity changes and gel electrophoresis of samples drawn from along the capillary. The high population numbers (approximately equal to 10(11], their well-characterized biochemistry, their short generation time, and the constant conditions make the system ideal for evolution experiments. Growth is monitored continuously by excitation of an added RNA-sensitive fluorescent dye, ethidium bromide. An analytic expression for the front velocity is derived for the multicomponent kinetic scheme that reduces, for a high RNA-enzyme binding constant, to the Fisher form v = 2 square root of kappa D, where D is the diffusion constant of the complex and kappa is the low-concentration overall replication rate coefficient. The latter is confirmed as the selective value-determining parameter by numerical solution of a two-species system.

Models for two tRNAs bound to successive codons on mRNA on the ribosome

We have investigated the structural changes necessary to build a model complex of two molecules of phenylalanine transfer RNA (tRNA(Phe) bound to successive codons in a short segment of a model messenger RNA (mRNA), consisting of U6. We keep the mRNA in an ideal helical conformation, deforming the tRNAs as necessary to eliminate steric overlaps while bringing the two 3' termini together. The resulting model has the two tRNAs oriented relative to one another in a manner that is very similar to a model developed by McDonald and Rein (1) in which the tRNAs maintain their ideal crystallographic conformations and all of the deformations are introduced into the mRNA. Consequently, regardless of how one divides the deformations between the tRNAs and the mRNA it is clear that, on the ribosome, the tRNA in the P site has its "front" side (that side with the variable loop) close to the "back" side of the tRNA in the A site (that side with the D loop). The space between the two molecules must be left free on the ribosome, in order to facilitate the transition from the A site to the P site. A detailed pathway is also proposed for changing the anticodon loop structure from that of the A site to that of the P site. The anticodon loop is always kept in a 3'-stacked conformation, since we find that the shift between the 3'-stacked and 5'-stacked structures proposed by Woese (2) is not feasible.

Effect of zinc ions on tRNA structure. I. Reversed-phase chromatography

The effect of zinc on the chromatographic behavior of four tRNAs was examined on RPC-5 and Aminex A-28 columns. RPC-5 contains dichlorodifluoroethylene beads coated with a quaternary ammonium compound where the substituents are: R1 = methyl, and R2-4 = C8-10 hydrocarbons. Aminex A-28 contains quaternary ammonium covalently attached to styrene-divinylbenzene copolymer lattice and R1-3 are methyl groups. The retentions of tRNAVal, tRNAIle, and tRNALys of E. coli and yeast tRNAPhe on RPC-5 were all markedly increased by Zn2+ ions. In contrast, no increased retention due to Zn2+ was observed when tRNAPhe was chromatographed on Aminex A-28. A model for chromatography on RPC-5 is developed which treats the elution behavior of tRNAs from this matrix as the sum of ion-exchange and hydrophobic interactions. The chromatography of tRNA in the presence and absence of Zn2+ is interpreted in terms of this model and the effects of sodium chloride concentration, temperature, and pH were explored as the experimental variables. These experiments suggest that in the absence of Zn2+ tRNA does not interact appreciably with the hydrophobic surface of the column. The addition of Zn2+ has three effects on chromatography: a decrease in the number of anionic sites on the tRNA which interact with the positively charged ammonium ion, an increase in affinity of the tRNA for these ionic sites, and an increase in affinity of tRNA for hydrophobic sites on the column. All three effects were fully reversed by the addition of Cd2+ (10 mM) or Mg2+ (35 mM), but only partially reversed at lower concentrations of these competing ions. These results show that chromatography on RCP-5 can be a sensitive physical chemical technique for examination of the structure of tRNA, and probably for other nucleic acids as well.

Induced fitting between a complex of four nucleotides and the cognate amino acid

The conformation of the hydrogen-bonded complex of a trinucleoside diphosphate (anticodon bases), a nucleic acid base (discriminator base), and an amino acid is investigated. This complex has been named C4N (complex of the four nucleotides) by one of the authors. Concerning the aminoacylation of tRNA and the genetic code, it has been proposed that C4N accepts the cognate protein amino acid by the lock-and-key relationship. The purpose of the calculation is to investigate the conformational and energetic properties of C4N from the energy minimum principle. The calculation is carried out by using the empirical potential functions. Glycine, glutamine, and valine are taken as typical cases. The formation energies are estimated. It is shown that some conformational changes are induced in the anticodon trinucleoside diphosphate by the binding of the discriminator base. Conformational changes of C4N and the amino acid are also induced by the binding of the amino acid to C4N.

Interactions of some naturally occurring cations with phenylalanine and initiator tRNA from yeast as reflected by their thermal stability

The thermal unfolding of phenylalanine and initiator tRNA from yeast was investigated over a broad range of solution conditions by differential ultraviolet absorption at 260 nm. Under most conditions, the initiator tRNA exhibits two clearly separated transitions in its differential melting curve which were assigned to unfolding of tertiary and secondary structure elements, respectively. The tertiary transition of this tRNA and the overall transition observed for tRNAPhe do not show a maximum in a curve of Tm values plotted as a function of [Na+]. Such a maximum is usually observed for other nucleic acids at about 1 M Na+. In the presence of 5 mM of the divalent cation Mg2+ (or Ca2+), an overall destabilization of the tRNAs is observed when increasing the sodium concentration. The largest fall in Tm (approximately 15 degrees C) is observed for the tertiary transition of the initiator tRNA. Among various cations tested the following efficiency in the overall stabilization of tRNAPhe is observed: spermine greater than spermidine greater than putrescine greater than Na+ (approximately NH4+). Mg2+ is most efficient at concentrations above 5 mM, but below this concentration spermine and spermidine appear to be more efficient. The same hierarchy in stabilizing power of the polyamines and Na+ is observed for both transitions of the initiator tRNA. However, when compared with Mg2+, the polyamines are far less capable of stabilizing the tertiary structure. In contrast, spermine and spermidine are slightly better than Mg2+ in stabilizing the secondary structure. At increasing concentrations of the polyvalent cations (at fixed [Na+] ) the Tm values of the tRNAs attain a constant value.

Phenylalanine transfer RNA: molecular dynamics simulation

Yeast phenylalanine transfer RNA was subjected to a 12-picosecond molecular dynamics simulation. The principal features of the x-ray crystallographic analysis are reproduced, and the amplitudes of atomic displacements appear to be determined by the degree of exposure of the atoms. An analysis of the hydrogen bonds shows a correlation between the average length of a bond and the fluctuation in that length and reveals a rocking motion of bases in Watson-Crick guanine X cytosine base pairs. The in-plane motions of the bases are generally of larger amplitude than the out-of-plane motions, and there are correlations in the motions of adjacent bases.

Physical properties of the E. coli 4.5S RNA: first results suggest a hairpin helix of unusual thermal stability

Hyperchromicity measurements and quasi-elastic laser light scattering (QELS) have been used to assess the solution structure of the metabolically stable E. coli 4.5S RNA. Results from thermal denaturation measurements revealed the 4.5S species to be markedly more stable than most other RNAs characterized thus far. Optical Tm's range from 79 degrees to 88 degrees with transitions approximately 25 degrees C wide. The Tm values show little dependence on ionic strength, but stability is enhanced considerably by Mg+2. In the QELS experiments the diffusion coefficient does not decrease until T greater than 70 degrees C. Neither the diffusive melting nor the diffusion coefficient at infinite dilution (D0(20,w)) show dependencies on ionic strength but both are influenced by Mg+2. The diffusion behavior is in agreement with that predicted for a rigid cylindrical molecule 125 to 160 A long and 37 to 26 A in diameter. Taken together these results are consistent with the more stable hypothetical secondary structures that can be formed, in which 70-75% of the 114 bases are paired to form a single extended hairpin helix.

The conformation of the tRNAPhe anticodon loop monitored by fluorescence

The intrinsic fluorescence of the Wye base was used to study the conformational change of the anticodon loop of yeast tRNAPhe brought about by the addition of magnesium. The fluorescence emission and excitation spectra show dramatic changes as magnesium is added to the solution. The rotational relaxation time changes from 6 nsec without added magnesium to 33 nsec with 10 mM magnesium at an ionic strength of 0.1 M. Stern-Volmer quenching by iodide or iodoethanol shows greater access of the base to the quencher with no added magnesium. A plausible interpretation of this data is that the base stack of the anticodon loop is altered by tilting or twisting the Wye base with respect to the adjacent bases and the base becomes parallel to its neighbors upon the addition of magnesium.

Structure of phenylalanine-accepting transfer ribonucleic acid and of its environment in aqueous solvents with different salts

Thermodynamic and structural parameters were measured for brewers' yeast tRNAPhe in solution in the range of 0.1-0.9 M monovalent salt (with and without 1 mM MgCl2), pH 7.0, by small-angle neutron scattering. Partial specific volumes and preferential interaction parameters were found to be similar to corresponding values measured by more conventional means in DNA [Eisenberg, H. (1981) Q. Rev. Biophys. 14, 141-172]. There is no evidence of a large conformational change in tRNAPhe in this range, and the molecule has a radius of gyration that is the same as that calculated from the crystal-structure coordinates (23 A). Transfer RNA in solution is made up of polyion tRNA76- and 76 positive monovalent ions (in absence of Mg2+). The data show the polyion to be surrounded by a shell of solvent that is significantly denser than bulk, whose structure depends on salt conditions. In 0.1 M NaCl, it has an excess mass of approximately 85 molecules of water. This would be accounted for, for example, by approximately 850 molecules of water if their density were 10% higher than that for bulk. The radius of gyration of the dense shell is approximately 30 A for NatRNA and approximately 35 A for KtRNA. The present study shows that the solvent around tRNA is a component of its structure that must be taken into account in understanding its function.

The influence of spermine on the structural dynamics of yeast tRNAPhe

A tRNAPhe derivative carrying ethidium at position 37 in the anticodon loop has been used to study the effect of spermine on conformational transitions of the tRNA. As previously reported (Ehrenberg, M., Rigler, R. and Wintermeyer, W. (1979) Biochemistry 18, 4588-4599) in the tRNA derivative the ethidium is present in three states (T1-T3) characterized by different fluorescence decay rates. T-jump experiments show two transitions between the states, a fast one (relaxation time 10-100 ms) between T1 and T2, and a slow one (100-1000 ms) between T2 and T3. In the presence of spermine the fast transition shows a negative temperature coefficient indicating the existence of a preequilibrium with a negative reaction enthalpy. Spermine shifts the distribution of states towards T3, as does Mg2+, but the final ratio [T2]/[T1] obtained with spermine is higher than with Mg2+, which we tentatively interpret to mean that spermine stabilizes one particular conformation of the anticodon loop.

Structural variability of tRNA: small-angle x-ray scattering of the yeast tRNAphe-Escherichia coli tRNAGlu2 complex

The structure of the complex formed in solution between yeast tRNAPhe and Escherichia coli tRNAGlu2 has been studied by small-angle x-ray scattering. The complex has a radius of gyration of 4.0 nm and an electron-pair distance distribution that is incompatible with a model composed to two tRNAs joined at their complementary anticodons and exhibiting the L shape seen in the crystal. Instead a model in which the two tRNAs, still bound via the anticodons, assume a conformation with the acceptor arms folded toward the anticodon arms agrees with the observed scattering curves.

Effects of magnesium and ionic strength on the diffusion and charge properties of several single tRNA species

The technique of laser light scattering was used to evaluate the effects of Mg+2 and ionic strength on the solution structures of seven tRNA species. Information about ion effects on both conformation and electric charge were derived from measurements of the translational diffusion constants and diffusive virial coefficients. E. coli tRNAMetf and six elongator tRNAs from both Class I and II were studied. The diffusion measurements show that the responses of all but the initiator species are qualitatively similar to each other and to that of bulk tRNA, but that significant quantitative differences also obtain. All of the elongator species exhibited an anomolous increase in diffusivity reported earlier by us for bulk tRNA when placed in a low salt-low Mg+2 condition. The initiator tRNA did not undergo this transition and unlike the other tRNAs tested was apparently more compact in 1 mM Mg+2 than 10 mM Mg+2 at ionic strengths in excess of 0.1 M. At 0.1 M ionic strength, pH 7.2, the average net charge of the tRNAs ranged from 7-12 e- in 1 mM Mg+2 and 3-7 e- in 10 mM Mg+2, consistent with the binding of 1-2 additional Mg+2 ions in the higher Mg+2 condition.

Changes in the solution structure of yeast phenylalanine transfer ribonucleic acid associated with aminoacylation and magnesium binding

The effect of aminoacylation on the structure of yeast phenylalanine tRNA was evaluated by laser light scattering. In these experiments, the translational diffusion coefficient (D20,w) of phenylalanyl-tRNA was monitored continuously during spontaneous deacylation in a variety of solution conditions. The results reveal that significant changes can occur in the hydrodynamic volume and electric charge as a consequence of aminoacylation but that the effects are magnesium dependent. At neutral pH, 20 degrees C, and 0.1 M salt, the D20,w value increased by 18% when deacylation occurred in 2--10 mM Mg2+ concentrations while no change in diffusivity was observed for tRNA deacylating in 0.5--1.0 mM Mg2+. The Mg2+ concentration dependence of the D20,w changes behaves in highly cooperative manner. The electric charges of aminoacyl-tRNA and nonacylated tRNA in 1 and 10 mM Mg2+ were estimated from the diffusive virial coefficients. In the higher Mg2+ conditions, aminoacyl-tRNA has a charge of 15 +/- 2e- while that of the nonacylated form is 10 +/- 2e-; both acylated and nonacylated tRNA have a charge of 11 +/- 4e- in 1 mM Mg2+. Taken together, the results indicate that aminoacylation permits the binding of additional Mg2+, resulting, in turn, in the formation of a more extended conformer of lower diffusivity and greater negative charge. The results also provide a possible explanation for several contradictory results in the literature.

Fluorescent tRNA derivatives and ribosome recognition

The use of fluorescent derivatives of tRNAPhe (yeast) in studies on tRNA conformation and on tRNA-ribosome recognition is described. Evidence is presented which indicates that under physiological conditions with respect to ionic strength and Mg2+ concentration, tRNAPhe exists in at least two conformations. The functional significance of this behavior is discussed on the basis of aminoacylation experiments. The investigation of the ribosome complexes of tRNAPhe labeled in the anticodon and D-loops has provided evidence suggesting that the presence of the codon, although not appreciably altering the apparent association constant, leads to qualitatively different complexes in which the tRNA appears to be rigidly bound to the codon even in the P-tRNA to the ribosome occurs in several steps, which take place only in the presence of the proper codon. One or more of these steps may represent codon-induced conformational changes of the tRNA molecule, which constitute the molecular basis of the highly specific binding of the tRNA to the ribosome.

On the structure and conformational dynamics of yeast phenylalanine-accepting transfer ribonucleic acid in solution

The solution structure of yeast tRNAPhe was investigated by using ethidium as a fluorescent probe in the D loop and the anticodon loop. For this purpose the dihydrouracils in position 16/17 and wybutine in position 37 were substituted by ethidium. The lifetimes and the time-dependent anisotropy of ethidium fluorescence were measured by pulsed nanosecond fluorometry. The kinetics of the transitions between different states of the tRNAPheEtd derivatives were determined by chemical relaxation measurements. It was found that the ethidium label irrespective of its position exhibits three different states called T1, T2 and T3 characterized by lifetimes tau 1 = 30 ns, tau 2 = 12 ns, and tau 3 = 3 ns. The lifetime differences are due to different accessibilities of ethidium for solvent quenching in the three states. Thus, there are three different defined structural environments of the ethidium in both the anticodon and the D loop. The distribution of the three states was measured as a function of Mg2+ concentration and temperature; it was found that state T3 is favored over states T2 and T1 by both increasing Mg2+ concentration and increasing temperature. The chemical relaxation kinetics exhibit a fast transition between T1 and T2 (10--100 ms) and a slow transition between T2 and T3 (100--1000 ms). The rates of both transitions depend likewise on Mg2+ concentration and temperature. The equilibrium and kinetic data clearly show the presence of strong and weak interactions between Mg2+ and tRNA. A cooperative model accounting for this behavior is developed. The ethidium probe behaves identically when located in different regions of the tRNA regarding both its distribution of states and its transition kinetics. This suggests that the different spectroscopic states report different conformations of the tRNA structure. The dependence of the three states on Mg2+ and spermine indicates that conformation T3 is closely related to or identical with the crystal structure. The rotational diffusion constants indicate that of all three states T3 is most extended while T2 is most compact. The thermodynamic analysis reveals that the strongly bound Mg2+ ions reduce both the activation entropy and enthalpy of all transitions. The weakly bound Mg2+ ions increase both the activation enthalpy and entropy of the slow transition between T2 and T3. It is suggested that the breaking of several intramolecular bonds, e.g., hydrogen bonds, is involved in this transition.

Conformational changes in 16S ribosomal RNA induced by 30S ribosomal subunit proteins from Escherichia coli

Laser light scattering has been used to evaluate conformational differences between free 16S RNA and several specific protein-16S RNA complexes. Proteins that interact strongly with the 16S RNA early in subunit assembly stabilize the RNA chain against unfolding in 1 mM Mg2+ and actually promote the formation of a more compact teriary structure in 20 mM Mg2+. A vital function of these proteins may therfore consist in altering the configuration of the RNA so that further assembly reactions can take place.

Theorectical mechanisms for synthesis of carcinogen-induced embryonic proteins: III. The tRNA methylases; methylation mechanism and function

It is contended that redundant repressed tRed) with carcinogens in adult cells. Supportive evidence, especially from molecular model building, is presented for a mechanism of tRNA methylation. In this mechanism the adenine moiety of S-adenosyl-L-methionine base-pairs with uracil for all tRNA methylations. Furthermore it is proposed that such methylations are required during the transcription of a tRNA molecule in order to limit the number of possible conformers that can occur before further development of the molecule takes place. This theory of the function for methyl groups is discussed in the light of the properties found for hypomethylated tRNAs.

Dynamic light scattering of biopolymers and biocolloids

Widespread applications of dynamic light scattering techniques to the study of macromolecular Brownian motion have yielded not only a valuable store of factual information concerning solution conformations and conformational changes, but have also provided an important window through which to view the dynamics of internal modes of motion. These techniques have coincided with a resurgence of interest in the solution physical chemistry of macromolecules, including hydrodynamic properties, and the profound effect of intermolecular interactions on both the disposition and dynamics of macromolecules in solution.

High-resolution nuclear magnetic resonance determination of transfer RNA tertiary base pairs in solution. 1. Species containing a small variable loop

Eight class I tRNA species have been purified to homogeneity and their proton nuclear magnetic resonance (NMR) spectra in the low-field region (-11 to -15 ppm) have been studied at 360 MHz. The low-field spectra contain only one low-field resonance from each base pair (the ring NH hydrogen bond) and hence directly monitor the number of long-lived secondary and tertiary base pairs in solution. The tRNA species were chosen on the basis of their sequence homology with yeast phenylalanine tRNA in the regions which form tertiary base pairs in the crystal structure of this tRNA. All of the spectra show 26 or 27 low-field resonances approximately 7 of which are derived from tertiary base pairs. These results are contrary to previous claims that the NMR spectra indicate the presence of resonances from secondary base pairs only, as well as more recent claims of only 1-3 tertiary resonances, but are in good agreement with the number of tertiary base pairs expected in solution based on the crystal structure. The tertiary base pair resonances are stable up to at least 46 degrees C. Removal of magnesium ions causes structural changes in the tRNA but does not result in the loss of any secondary or tertiary base pairs.