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

Ab-initio quantum mechanical calculations of NMR chemical shifts in nucleic acid constituents. I. The Watson-Crick base pairs

The magnetic shielding constants of the different nuclei of the four nucleic acid bases adenine, uracile, guanine and cytosine are calculated by a non empirical method using a minimal basis set and compared to the available corresponding experimental data. The same calculations carried out for AU and GC pairs give not only the values of the chemical shift variations due to the formation of the pairs but also the relative importance of the three different contributions (geometric, polarization and charge transfer plus exchange) to the total value of delta delta. Their analysis shows the importance of the polarization term. The magnitude of the charge transfer plus exchange term which is obtained for the nuclei belonging to the hydrogen bonding sites indicates that the hydrogen bond length is the major factor in the determination of the magnetic shielding constants of these atoms. On the other hand it appears that the pairing of the bases has a negligible effect on the "geometric" magnetic shielding due to the bases.

Study of transfer ribonucleic acid unfolding by dynamic nuclear magnetic resonance

Nuclear magnetic resonance (NMR) measurements of proton exchange were performed on yeast tRNAPhe, and in much less detail on Escherichia coli tRNAfMet, over a range of Mg2+ concentrations and temperatures, at neutral pH and 0.1 M NaCl. The resonances studied were those of ring nitrogen protons, resonating between 10 and 15 ppm downfield from sodium 3-(trimethylsilyl)-1-propanesulfonate, which partake in hydrogen bonding between bases of secondary and tertiary pairs. Methods include saturation--recovery, line width, and real-time observation after a change to deuterated solvent. The relevant theory is briefly reviewed. We believe that most of the higher temperature rates reflect major unfolding of the molecule. For E. coli tRNAfMet, the temperature dependence of the rate for the U8--A14 resonance maps well onto previous optical T-jump studies for a transition assigned to tertiary melting. For yeast tRNAPhe, exchange rates of several resolved protons could be studied from 30 to 45 degrees C in zero Mg2+ concentration and had activation energies on the order of 40 kcal/mol. Initially, the tertiary structure melts, followed shortly by the acceptor stem. At high Mg2+ concentration, relatively few exchange rates are measurable below the general cooperative melt at about 60 degrees C; these are attributed to tertiary changes. Real-time observations suggest a change in the exchange mechanism at room temperature with a lower activation energy. The results are compared with those obtained by other methods directed toward assaying ribonucleic acid dynamics.

Spin-labelled nucleic acids

The spin label method developed by McConnell 15 years ago is now widely used in studies of the structure and dynamic properties of a variety of the biological systems such as proteins and protein complexes, lipids and membranes, nucleic acids, nucleoproteins, etc.

The ESR spectrum of the nitroxide radcal – the spin label – is very sensitive to its microenvironment and permits easy registration of even subtle alterations in it. If spin labels are attached to different sites of a macromolecule the information can be gained about conformational properties of all these local regions and, as a result, about the dynamic behaviour of the object as a whole.

A study of the thermal unfolding of Escherichia coli phenylalanine transfer RNA by chemical modification at elevated temperatures

Escherichia coli tRNAPhe was modified by 3 M sodium bisulphite pH 6.0 for 24 h in the temperature range 25 degrees C (x 5 degrees C) to 55 degrees C and in the absence of added magnesium ions. The sites and extents of conversion of cytidines to uridine occurring at each temperature were determined by fingerprinting. The new sites of cytidine modification found at higher reaction temperatures were assumed to arise from breakage of secondary and tertiary structure hydrogen bonds involving cytidine residues. From these data, we conclude that hydrogen bonds within the 'complex core' of the tRNA (including the base pairs G-10 . C-25, C-11 . G-24 and C-13 . G-21 within the dihydrouridine stem and the tertiary structure base pair G-15 . C-48 melt at a lower temperature than the tertiary structure hydrogen bonds between G-19 in the dihydrouridine loop and C-56 in the TpsiC loop.

Conformational changes in yeast tRNATyr revealed by EPR spectra of spin-labelled N6-(delta2-isopentenyl)-adenosine residue

Temperature-induced conformational changes in the anticodon region of yeast tRNATyr were studied by EPR spectroscopy. The spin label 4-amino-2,2,6,6-tetramethylpiperidine-1-oxyl was attached to the N6-(delta2-isopentenyl)-adenosine residue in tRNATyr, previously made reactive by iodination. The labelled tRNATyr gave an asymmetrical triplet spectrum typical of rapidly tumbling nitroxide, with a rotational correlation time (tauc) of 0.65 ns. Spin-labelled tRNATyr was exposed to heating and cooling in three different buffers each with or without MgCl2. In each case the Arrhenius plot of --log tauc vs. inverse absolute temperature gave two straight lines, intersecting at a critical temperature (tcr). Above tcr, the anisotropy of the spectrum was not reduced and the activation energy of motion increased, indicating that the transition is associated with a conformational change of the macromolecule. Transitions in 0.05 M potassium phosphate (pH 8.0) and 0.02 M Tris - HC1 (pH 7.0) were observed at potassium phosphate (pH 8.0) and 0.02 M Tris - Hc1 (pH 7.0) were observed at approx. 37 degrees C. When 0.01 M mgCl2 was present in these buffers, transitions were shifted to 46 degrees and 53 degrees C, respectively. Transitions in 0.01 M sodium cacodylate were observed at temperatures which are significantly lower. Since all these transitions occur at temperatures considerably below those required to melt the helical regions of tRNA, and at least approximately 10 degrees C below those reported to break tertiary interactions, it is supposed that they reflect some reorientation of the anticodon region, e.g. a change in tilt of the bases.

A theoretical study oh the effect of "bound" water on the proton chemical shifts of the nucleic acid bases

Computations are performed on the proton chemical shifts due to hydrogen bonding between the purine and pyrimidine bases of the nucleic acids and water molecules of their first hydration shell. The water molecules should produce measurable shifts essentially for protons of the bases located close to the site of interaction. For the imino protons of the bases G-N1H and U-N3H participating in hydrogen bonding, the calculated delta delta is larger for the interaction of a base with a complementary base than for its interaction with water. Base pairing will thus produce a downfield shift in water but the measured delta delta due to pairing in this solvent will be smaller than in an inert solvent. Also, the chemical shift difference between G-N1H and U-N3H in water will be larger if the molecules are engaged in pairs than if they are not.

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.

Theoretical study on the proton chemical shifts of hydrogen bonded nucleic acid bases

The variation of the proton chemical shifts due to the formation intermolecular hydrogen bonds is computed for a number of complexes which can be formed between the bases of the nucleic acids. The shifts expected for the isolated base pairs, in particular for the G-N1 H, T(or U)-N3H protons and the protons of the amino groups of A, G c, when combined with previous computations on the shifts to be expected upon base stacking, may enable a refined analysis of the high resolution NMR spectra of self complementary polynucleotides or tRNAs. Two examples are presented of a direct computation of proton shits associated with helix-coil transitions, helpful for deducing the helical structure in solution.

CD spectra of 5-methyl-2-thiouridine in tRNA-Met-f from an extreme thermophile

5-Methyl-2-thiouridine (S) in tRNA-Met-f from an extreme thermophile is located in the TpsiC region, replacing T, and has a positive CD band centered at 310 nm. Upon heating, the profiles of the change in this band were similar to the UV melting profiles of the change monitored at 260 nm. This strongly suggests a close relation between heat denaturation of the tRNA and the conformation of the S base. Oligonucleotides containing S showed negative CD bands at 320-330 nm, like the monomer S itself, but when the 3'-2/5 fragment containing S formed a complex with the complementary 5'-3/5 fragment, a positive CD band appeared at 310 nm. These results suggest that combination of the TpsiC loop containing S with the hU loop is necessary for the positive band of S at 310 nm. S may serve to strengthen the association of the TpsiC loop with the hU loop in tRNA of the thermophile.