Conformational peculiarities of polynucleotides with a nonrandom base sequence according to the 1H----3H exchange rate in C8H groups of purinic residues

Tritium labeling of antisense oligonucleotides by exchange with tritiated water

We describe a simple, efficient, procedure for labeling oligonucleotides to high specific activity (< 1 x 10(8) cpm/mumol) by hydrogen exchange with tritiated water at the C8 positions of purines in the presence of beta-mercaptoethanol, an effective radical scavenger. Approximately 90% of the starting material is recovered as intact, labeled oligonucleotide. The radiolabeled compounds are stable in biological systems; greater than 90% of the specific activity is retained after 72 hr incubation at 37 degrees C in serum-containing media. Data obtained from in vitro cellular uptake experiments using oligonucleotides labeled by this method are similar to those obtained using 35S or 14C-labeled compounds. Because this protocol is solely dependent upon the existence of purine residues, it should be useful for radiolabeling modified as well as unmodified phosphodiester oligonucleotides.

Base sequence criteria and Cartesian coordinates for stable B/Z and B/Z/B junctions in relaxed DNA

It seems increasingly evident that if the Z form of DNA exists in the genome it must exist as short sections of alternating pyrimidine-purine sequences in the midst of very long sections of B-form DNA. We have determined the minimum length of a string of alternating CG base pairs that can go into the Z form in the middle of a long B form. Self-complimentary oligomers of the form T(M)(CG)(N)A(M) were synthesized. The conformation of the resulting duplex was determined in 6M aqueous NaCl solution by Raman scattering. We have found that 12 alternating CG base pairs is the minimum length required to form a stable Z form of DNA inside of a long B form section. Only the 4 center CG base pairs go into the Z form. These 4 CG base pairs in the Z form are flanked on each side by 4 CG base pairs in a non-Z (probably B) form as well as the ..TT.. ..AA.. sequences in the B form. We propose a model of the B/Z junction in which the double helix flips directly from the B form to the Z form so that there are no base pairs in the junction. In this model the B form is nucleated in the AT base pairs on each end and is propagated into the CG base pairs in the center. This model is supported by isotopic H/D exchange experiments that shows that the H/D exchange of the non-Z form CG base pairs is highly retarded and indicates that they remain in the B form. A Thermodynamic analysis of the concentration dependence of the melting point of the duplexes in both low and high salt, supports our model and rules out the possibility of hairpin formation. The enthalpy for the formation of a B/Z junction is determined to be about +16 kcal/junction. A comparison of these results with recent results on B/Z junctions in super-coiled DNA is given. Molecular modeling calculations permit us to obtain values for the coordinates and torsional angles of the oligomers showing both B/Z and B/Z/B junctions. The Cartesian coordinates for these oligomers as well as stereo figures of these models in color are available from the authors.

Adenine and guanine 8CH exchange in nucleic acids: resolution and measurement by Raman optical multichannel analysis

Deuterium exchange of 8C protons of adenine and guanine in nucleic acids is conveniently monitored by laser Raman spectrophotometry, and the average exchange rate so determined [kA + kG] can be exploited as a dynamic probe of the secondary structure of DNA or RNA [J. M. Benevides and G. J. Thomas, Jr. (1985) Biopolymers 24, 667-682]. The present work describes a rapid Raman procedure, based upon optical multichannel analysis, which permits discrimination of the different 8CH exchange rates, kA of adenine and kG of guanine, in a single experimental protocol. For this procedure, simultaneous measurements are made of the intensity decay or frequency shift in separately resolved Raman bands of adenine and guanine, each of which is sensitive only to 8C deuteration of its respective purine. Resolution of the rates kA and kG is demonstrated for the mononucleotide mixtures, 5'-rAMP + 5'-rGMP and 5'-dAMP + 5'-dGMP, for the polynucleotides poly(dA-dT).poly(dA-dT) and poly(dG-dC).poly(dG-dC), for calf thymus DNA, and for the 17 base-pair operator OR3. We show that the different exchange rates of adenine and guanine, in nucleotide mixtures and in DNA, may also be calculated independently from intensity decay of the composite 1481-cm-1 band, comprising overlapped adenine and guanine components, over a time domain that encompasses two distinct regimes: (1) a relatively more rapid exchange of guanine, and (2) a concurrent slower exchange of adenine. Both methods developed here yield consistent results. We find, first, that exchange of guanine is approximately twofold more rapid than that of adenine when both purines are present in the same structure and solvent environment, presumably a consequence of the greater basicity of the 7N site of guanine. Second, we find that adenine suffers greater retardation of exchange than guanine when both purines are incorporated into a "classical" B-DNA secondary structure, such as that of calf thymus DNA. This finding suggests different microenvironments at the 7N-8C loci of adenine and guanine in aqueous B-DNA. We also confirm that adenine residues of B-form poly(dA-dT).poly(dA-dT) exchange much more slowly than those of other B-DNA sequences, implying a secondary structure for the alternating-AT sequence with unusual stereochemistry in the major groove. The greater resistance of adenine than guanine to 8CH exchange in the B-DNA secondary structure is more evident in high molecular weight calf thymus DNA and in the alternating AT and GC copolymer duplexes than in the smaller 17 base-pair operator OR3.(ABSTRACT TRUNCATED AT 400 WORDS)

A molecular dynamics simulation of the (dG)6 . (dC)6 minihelix including counterions and water

The results of a 60 ps molecular dynamics (MD) simulation of (dG)6.(dC)6 including 10 Na+ counterions and 292 water molecules are presented. All backbone angles and helix parameters for the hexamer are reported in this paper along with trajectory plots of selected angles. Hydrogen bonding between the bases along the helical axis was observed to fluctuate with time, showing the dynamic nature of the base-pairing interaction. These fluctuations gave rise to unusual hydrogen-bonding patterns. Good intrastrand base stacking and no interstrand base stacking were also observed. The hexamer minihelix retains an essentially B-DNA conformation throughout the entire simulation even though some helix parameters and backbone angles do not have strict B-DNA values. The most striking feature obtained from the simulation was a high propeller twist, which resulted in a narrow minor groove for the minihelix. It is proposed that (dG)n.(dC)n sequences are resistant to DNAase I because of this narrow minor groove in dilute aqueous solution.