Thermodynamics of transfer ribonucleic acids: the effect of sodium on the thermal unfolding of yeast tRNAPhe.

The thermal unfolding of yeast phenylalanine-specific tRNA (tRNA^Phe) has been calorimetrically investigated at several salt concentrations in the absence of magnesium. Application of the deconvolution theory of macromolecular conformational transitions allows calculation of the thermodynamic parameters of unfolding. It is demonstrated that the unfolding of tRNA^Phe occurs in a sequential fashion and that four separate transitions or five macromolecular thermodynamic states exist in the temperature range 8–72°C under the experimental conditions of these studies (0.067–0.52M Na⁺). The enthalpy and entropy changes between states and the relative population of each state as a function of temperature and salt concentration have been obtained. Sodium stabilizes the low-temperature conformations of tRNA^Phe. The increase in the melting temperatures of each transition is shown to be linearly dependent on the logarithm of sodium concentration. These results allow calculation of the “phase” diagram for the transitions as a function of salt concentration.     

Human Tyrosine tRNA Is Also Internally Cleavable by E. coli Ribonuclease P RNA Ribozyme in Vitro

Transfer RNA is an essential molecule for biological system, and each tRNA molecule commonly has a cloverleaf structure. Previously, we experimentally showed that some Drosophila tRNA (tRNA^Ala, tRNA^His, and tRNA_i ^Met) molecules fit to form another, non-cloverleaf, structure in which the 3'-half of the tRNA molecules forms an alternative hairpin, and that the tRNA molecules are internally cleaved by the catalytic RNA of bacterial ribonuclease P (RNase P). Until now, the hyperprocessing reaction of tRNA has only been reported with Drosophila tRNAs. This time, we applied the hyperprocessing reaction to one of human tRNAs, human tyrosine tRNA, and we showed that this tRNA was also hyperprocessed by E. coli RNase P RNA. This tRNA is the first example for hyperprocessed non-Drosophila tRNAs. The results suggest that the hyperprocessing reaction can be a useful tool to detect destablized tRNA molecules from any species.     

Tuning lambda6-85 towards downhill folding at its melting temperature

The five-helix bundle lambda6-85* is a fast two-state folder. Several stabilized mutants have been reported to fold kinetically near-downhill or downhill. These mutants undergo a transition to two-state folding kinetics when heated. It has been suggested that this transition is caused by increased hydrophobicity at higher temperature. Here we investigate two histidine-containing mutants of lambda6-85* to see if a weaker hydrophobic core can extend the temperature range of downhill folding. The very stable lambdaHA is the fastest-folding lambda repressor to date (k(f)(-1) approximately k(obs)(-1)=2.3 micros at 44 degrees C). It folds downhill at low temperature, but transits back to two-state folding at its unfolding midpoint. lambdaHG has a weakened hydrophobic core. It is less stable than some slower folding mutants of lambda6-85*, and it has more exposed hydrophobic surface area in the folded state. This mutant nonetheless folds very rapidly, and has the non-exponential folding kinetics of an incipient downhill folder even at the unfolding midpoint (k(m)(-1) approximately 2 micros, k(a)(-1)=15 micros at 56 degrees C). We also compare the thermodynamic melting transition of lambdaHG with the nominal two-state folding mutant lambdaQG, which has a similar melting temperature. Unlike lambdaQG, lambdaHG yields fluorescence wavelength-dependent cooperativities and probe-dependent melting temperatures. This result combined with previous work shows that the energy landscapes of lambda repressor mutants support all standard folding mechanisms.     

Tritium exchange studies of transfer RNA in native and denaturated conformations

Tritium exchange was used as a probe of transfer RNA structure in experiments with unfractionated tRNA (tRNA^Unfrac and homogeneous tRNA₃^Leu from bakers' yeast. Exchange kinetics were measured over a range of ionic conditions that vary in ability to stabilize the secondary and tertiary structure of tRNA. The native conformations of both samples show the same kinetics of exchange. The kinetics for tRNA₃^Leu trapped in a denatured state in a “native” solvent are much faster, reflecting the conformation and not the ionic medium. In 0.1 M-Na⁺, where tRNA₃^Leu is denatured, the kinetics for tRNA^Unfrac are intermediate between those for native and denatured tRNA₃^Leu, suggesting that in this solvent at 0 °C some tRNAs are denatured whereas other are still native. Upon further lowering of Na⁺ concentration, tRNA^Unfrac shows increasingly faster exchange, suggesting complete electrostatic denaturation of the tertiary structure of all the tRNAs in the sample, and even disruption of secondary structure.Extrapolation of the essentially linear early-time kinetics to zero time provides minimal estimates of the number of slowly exchanging hydrogens. For native tRNA₃^Leu the number is 111±2 hydrogens, whereas for the trapped denatured conformation it is only 95±2. This difference reflects a smaller number of hydrogen-bonded bases in the denatured conformation. In 1 M-Na⁺, 101±2 slowly exchanging hydrogens are found for the native tRNA₃^Leu conformation, suggesting an incompletely formed native structure. For native tRNA^Unfrac the comparable number is 101±3. These numbers of slowly exchanging hydrogens in the native conformations are consistent with tertiary structural hydrogen-bonding. Furthermore, this tertiary structure must be responsible for the slower exchange by native tRNA. The observed numbers of exchangeable hydrogens provide a basis for comparison of hydrogen-bonding interactions in native and denatured tRNA conformations.The mechanism of renaturation was also investigated, using tritium exchange as a monitor of perturbation of base pairing during the transition. When tRNA^Unfrac in low Na⁺ is renatured by addition of Mg²⁺ during tritium exchangeout, a burst of exchange or “spillage” of tritium is detected. This suggests that a fraction of the base pairs of the rapidly renaturing tRNAs in the mixture is disrupted during renaturation. In that event, and by analogy with tRNA₃^Leu, part of the base-pairing arrangement of the denatured conformations may not be preserved in the native state; and if the native conformation includes the full “cloverleaf” pattern of secondary structure, that pattern may not be intact in some denatured conformations.     

Conformational change in yeast tRNAAsp

The structure of yeast tRNA^Asp in aqueous solutions has been analyzed in the light of results obtained from Raman spectra recorded at from 5 to 82°C and compared to those of tRNA^Phe. Firm evidence is given of a reversible conformation transition for tRNA^Asp at 20°C. This transition is observed for the first time in the tRNA series. The low-temperature conformation appears to have a more regular ribose–phosphate backbone and a more effective G base-stacking. This conformational change, which occurs essentially in the D loop, could be connected to the existence of two (A and B) crystal forms obtained depending on crystallization conditions. The melting temperatures, which are different for each base stacking in tRNA^Asp, lie in a range of about 70°C, much higher than for tRNA^Phe. This fact is interpreted by a higher ratio of G-C base pairs in tRNA^Asp.     

Titration Properties and Thermodynamics of the Transition State for Folding: Comparison of Two-state and Multi-state Folding Pathways

CI2 folds and unfolds as a single cooperative unit by simple two-state kinetics, which enables the properties of the transition state to be measured from both the forward and backward rate constants. We have examined how the free energy of the transition state for the folding of chymotrypsin inhibitor 2 (CI2) changes with pH and temperature. In addition to the standard thermodynamic quantities, we have measured the overall acid-titration properties of the transition state and its heat capacity relative to both the denatured and native states. We were able to determine the latter by a method analogous to a well-established procedure for measuring the change in heat capacity for equilibrium unfolding: the enthalpy of activation of unfolding at different values of acid pH were plotted against the average temperature of each determination. Our results show that the transition state of CI2 has lost most of the electrostatic and van der Waals' interactions that are found in the native state, but it remains compact and this prevents water molecules from entering some parts of the hydrophobic core. The properties of the transition state of CI2 are then compared with the major folding transition state of the larger protein barnase, which folds by a multi-state mechanism, with the accumulation of a partly structured intermediate (D^physor I). CI2 folds from a largely unstructured denatured state under physiological conditionsviaa transition state which is compact but relatively uniformly unstructured, with tertiary and secondary structure being formed in parallel. We term this an expanded pathway. Conversely, barnase folds from a largely structured denatured state in which elements of structure are well formed through a transition state that has islands of folded elements of structure. We term this a compact pathway. These two pathways may correspond to the two extreme ends of a continuous spectrum of protein folding mechanisms. Although the properties of the two transition states are very different, the activation barrier for folding (D^phys→3 ) is very similar for both proteins.     

Complex formation between transfer RNAs with complementary anticodons: use of matrix bound tRNA

It is shown that yeast tRNA^Phe, chemically coupled by its oxidized 3′CpCpA end behaves exactly as free tRNA^Phe in its ability to form a specific complex with $\text{E. coli}$ tRNA₂^Glu having a complementary anticodon. The results support models of tRNA in which the 3′CpCpA_OH end and the anticodon are not closely associated in the tertiary structure, and provide a convenient tool of general use to characterize others pairs of tRNA having complementary anticodons, as well as for highly selective purification of certain tRNA species.     

Detection and structure determination of an equilibrium unfolding intermediate of Rd-apocytochrome b562: native fold with non-native hydrophobic interactions

The absence of detectable kinetic and equilibrium folding intermediates by optical probes is commonly taken to indicate that protein folding is a two-state process. However, for some small proteins with apparent two-state behavior, unfolding intermediates have been identified in native-state hydrogen exchange or kinetic unfolding experiments monitored by nuclear magnetic resonance. Rd-apocytochrome b(562), a four-helix bundle, is one such protein. Here, we found another unfolding intermediate for Rd-apocytochrome b(562). It is based on a cooperative transition of (15)N chemical shifts of amide protons as a function of urea concentrations before the global unfolding. We have solved the high-resolution structure of the protein at 2.8 M urea, which is after this cooperative transition but before the global unfolding. All four helices remained intact, but a number of hydrophobic core residues repacked. This intermediate provides a possible structural interpretation for the kinetic unfolding intermediates observed using nuclear magnetic resonance methods for several proteins and has important implications for theoretical studies of protein folding.     

Nucleotide sequence of Rattus norvegiens mitochondrial DNA that includes the genes for tRNAile, tRNAgln and tRNAf-met

The nucleotide sequence of a segment of mtDNA from Rattus norvegiens (rat) which contains the genes for tRNA^ile, tRNA^gl and tRNA^f-met has been determined. A detailed comparison has been made between this sequence and the corresponding sequences of mouse, human and bovine mtDNAs with regard to the primary and secondary structure of the tRNA genes, the regions connecting the tRNA genes, and the regions flanking the tRNA genes which code for the carboxyl terminus of URF-1 and the amino terminus of URF-2. No differences were found in the nucleotide sequences of the genes for tRNA^ile, tRNA^gln and tRNA^f-met in mtDNAs from three different female lines of rats (SASCO-1, SASCO-2 and Wild-UT) that differ by substitutions of 0.8% to 1.8% of their total nucleotides.     

Transfer RNA-like structure of the human Alu family: Implications of its generation mechanism and possible functions

Summary Structural resemblance of the human Alu family with a subset of vertebrate tRNAs was detected. Of four tRNAs, tRNA^Lys, tRNA^Ile, tRNA^Thr, and tRNA^Tyr, which comprise a structurally related family, tRNA^Lys is the most similar to the human Alu family. Of the 76 nucleotides in lysine tRNA (including the CCA tail), 47 are similar to the human Alu family (60% identity). The secondary structure of the human Alu family corresponding to the D-stem and anticodon stem regions of the tRNA appears to be very stable. The 7SL RNA, which is a progenitor of the human Alu family, is less similar to lysine tRNA (55% identity), and the secondary structure of the 7SL RNA folded like a tRNA is less stable than that of the human Alu family folded likewise. Insertion of the tetranucleotide GAGA, which is an important region of the second promoter for RNA polymerase III in the Alu sequence, occurred during the deletion and ligation process to generate the Alu sequence from the parental 7SL RNA. These results suggest that the human Alu family was generated from the 7SL RNA by deletion, insertion, and mutations, which thus modified the ancestral 7SL sequence so that it could form a structure more closely resembling lysine tRNA. The similarities of several short interspersed sequences to the lysine tRNA were also examined. TheGalago type 2 family, which was reported to be derived from a methionine initiator tRNA, was also found to be similar to the lysine tRNA. Thus lysine tRNA-like structures are widespread in genomes in the animal kingdom. The implications of these findings in relation to the mechanism of generation of the human Alu family and its possible functions are discussed.     

Calorimetric studies on melting of tRNA Phe (yeast).

The heat effects involved in thermal unfolding of tRNAPhe from yeast have been determined in various buffer systems by direct differential scanning calorimetry. Perfect reversibility of the melting process has been demonstrated for measurements in the absence of Mg2+ ions. The overall molar transition enthalpy, delta Ht = 298 +/- 15 kcal mol-1 (1247 +/- 63 kJ mol-1), has been shown to be independent of the NaCl concentration and the nature of the buffers used in this study. Delta Ht is identical in the presence and in the absence of Mg2+ ions within the margin of experimental error. This experimental result implies a vanishing or very small heat capacity change to be associated with melting. Decomposition of the calorimetrically determined complex transition curves, on the assumption that the experimental melting profile represents the sum of independent two-state transitions, results in five transitions which have been assigned to melting of different structural domains of the tRNA.     

pH dependent unfolding characteristics of DLC8 dimer: Residue level details from NMR

Environment dependence of folding and unfolding of a protein is central to its function. In the same vein, knowledge of pH dependence of stability and folding/unfolding is crucial for many biophysical equilibrium and kinetic studies designed to understand protein folding mechanisms. In the present study we investigated the guanidine induced unfolding transition of dynein light chain protein (DLC8), a cargo adaptor of the dynein complex in the pH range 7-10. It is observed that while the protein remains a dimer in the entire pH range, its stability is somewhat reduced at alkaline pH. Global unfolding features monitored using fluorescence spectroscopy revealed that the unfolding transition of DLC8 at pH 7 is best described by a three-state model, whereas, that at pH 10 is best described by a two-state model. Chemical shift perturbations due to pH change provided insights into the corresponding residue level structural perturbations in the DLC8 dimer. Likewise, backbone (15)N relaxation measurements threw light on the corresponding motional changes in the dimeric protein. These observations have been rationalized on the basis of expected changes with increasing pH in the protonation states of the titratable residues on the structure of the protein. These, in turn provide an explanation for the change from three-state to two-state guanidine induced unfolding transition as the pH is increased from 7 to 10. All these results exemplify and highlight the role of environment vis-à-vis the sequence and structure of a given protein in dictating its folding/unfolding characteristics.     

Temperature dependence of the aminoacylation of tRNA by Bacillus stearothermophilus aminoacyl-tRNA synthetases

Valine specific transfer RNA (tRNA^Val) was isolated from Bacillus stearothermophilus and Escherichia coli by chromatography on benzoylated DEAE–cellulose (BD–cellulose). Likewise isoleucine specific transfer RNA (tRNA^Ile) was isolated from B. stearothermophilus and from Mycoplasma sp. Kid. The thermal denaturation profiles (melting curves) of the two tRNA^Val species in the presence of Mg^{+ +} were nearly identical. However, the T_m for the Kid tRNA^Ile was about 10°C lower than that for the B. stearothermophilus tRNA^Ile. A nuclease and tRNA-free aminoacyl-tRNA synthetase (AA-tRNA synthetase) preparation from B. stearothermophilus was able to function efficiently at temperatures up to 80°C in the aminoacylation of all four tRNA species. Determination of the amino acid-acceptor activity of each tRNA species as a function of temperature of the aminoacylation reaction showed in each case a strong correlation between the loss of acceptor activity and the thermal denaturation profile of the tRNA. Evidence is presented that the loss in acceptor activity is most likely due to a change in structure of the tRNA as opposed to denaturation of the enzyme. These results further support the idea that correct secondary and/or tertiary structure must be maintained for tRNA to be active as a substrate for the AA-tRNA synthetase.     

Folding Nuclei in Proteins

When a protein folds or unfolds, it passes through many half-folded microstates. Only a few of them can accumulate and be seen experimentally, and this happens only when the folding (or unfolding) occurs far from the point of thermodynamic equilibrium between the native and denatured states. The universal features of folding, though, are observed in the vicinity of the equilibrium point. Here the two-state transition proceeds without any accumulation of metastable intermediates, and only the transition state (folding nucleus) is outlined by its key influence on the folding/unfolding kinetics. This review covers recent experimental and theoretical studies of folding nuclei.     

Kinetics of folding nuclei formation in proteins

When a protein folds or unfolds, it passes through many half-folded microstates. Only a few of them can accumulate and be seen experimentally, and this happens only when the folding (or unfolding) occurs far from the point of thermodynamic equilibrium between the native and denatured states. The universal features of folding, though, are observed in the vicinity of the equilibrium point. Here the "two-state" transition proceeds without any accumulation of metastable intermediates, and only the transition state ("folding nucleus") is outlined by its key influence on the folding/unfolding kinetics. This review covers recent experimental and theoretical studies of folding nuclei.     

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⁺.     

Interaction of Complementary Oligonucleotides with the 3′-End of Yeast tRNAPHE

Abstract

Interaction of yeast tRNA^Phe with oligodeoxyribonucleotides (ONs), complementary to the nucleotides 62–76 was investigated. Results of gel-mobility shift assay and RNase A probing evidence that the ONs containing the sequence complementary to the tRNA ACCA end can easily invade the hairpin structure under physiological conditions. The limiting step of association process is the tRNA unfolding.