Existence of the C structure in poly(dA-dC).poly(dG-dT)

Experimental detection of conformational transitions between forms of DNA: problems and prospects

Under different conditions, the DNA double helix can take different geometric forms. Of the large number of its conformations, in addition to the "canonical" B form, the A, C, and Z forms are widely known, and the D, Hoogsteen, and X forms are less known. DNA locally takes the A, C, and Z forms in the cell, in complexes with proteins. We compare different methods for detecting non-canonical DNA conformations: X-ray, IR, and Raman spectroscopy, linear and circular dichroism in both the infrared and ultraviolet regions, as well as NMR (measurement of chemical shifts and their anisotropy, scalar and residual dipolar couplings and inter-proton distances from NOESY (nuclear Overhauser effect spectroscopy) data). We discuss the difficulties in applying these methods, the problems of theoretical interpretation of the experimental results, and the prospects for reliable identification of non-canonical DNA conformations.

The structure of DNA within cationic lipid/DNA complexes

The structure of DNA within CLDCs used for gene delivery is controversial. Previous studies using CD have been interpreted to indicate that the DNA is converted from normal B to C form in complexes. This investigation reexamines this interpretation using CD of model complexes, FTIR as well as Raman spectroscopy and molecular dynamics simulations to address this issue. CD spectra of supercoiled plasmid DNA undergo a significant loss of rotational strength in the signal near 275 nm upon interaction with either the cationic lipid dimethyldioctadecylammonium bromide or 1,2-dioleoyltrimethylammonium propane. This loss of rotational strength is shown, however, by both FTIR and Raman spectroscopy to occur within the parameters of the B-type conformation. Contributions of absorption flattening and differential scattering to the CD spectra of complexes are unable to account for the observed spectra. Model studies of the CD of complexes prepared from synthetic oligonucleotides of varying length suggest that significant reductions in rotational strength can occur within short stretches of DNA. Furthermore, some alteration in the hydrogen bonding of bases within CLDCs is indicated in the FTIR and Raman spectroscopy results. In addition, alterations in base stacking interactions as well as hydrogen bonding are suggested by molecular dynamics simulations. A global interpretation of all of the data suggests the DNA component of CLDCs remains in a variant B form in which base/base interactions are perturbed.

Direct measurement of the association constant of HER2/neu antisense oligonucleotide to its target RNA sequence using a molecular beacon

A molecular beacon approach was developed to directly determine the association constant of RNA-DNA hybrid formation. The molecular beacon was composed of a 15-nt loop structure containing the antisense sequence that can hybridize with the AUG translational start site of the HER2/neu gene, which is overexpressed in a significant proportion of breast, ovarian, and lung tumors. The equilibrium association constant (Ka) of DNA binding to the RNA oligonucleotide was 6.4 +/- 0.14 x 10(7) M(-1) in the presence of 150 mM NaCl at 22 degrees C. The free energy change (AG) associated with RNA-DNA hybrid formation was -10.7 kcal/mole. The melting temperature (Tm) of RNA-DNA hybrid was 64.4 degrees C +/- 1 degree C in the presence of 150 mM NaCl. The RNA-DNA hybrid was more stable than the corresponding DNA-DNA duplex in 150 mM NaCl, as judged by both Ka and Tm data. We also determined the Ka, deltaG, and Tm values of RNA-DNA and DNA-DNA duplex formation in the presence of three monovalent cations, Li+, K+, and Cs+. The feasibility of this method was also investigated using a phosphorothioate molecular beacon. The information generated through this new approach for thermodynamic measurements might be useful for the design of oligonucleotides for antisense therapeutics.

Accurate length determination of DNA molecules visualized by atomic force microscopy: evidence for a partial B- to A-form transition on mica

Achieving the most correct estimate of the contour length of digitized DNA molecules is a key aspect of the microscopic analysis of nucleic acids by either electron microscopy (EM) or atomic force microscopy (AFM). Six different methods, that are mathematically not too complex and suited for common, practical use, have been tested here using simulated polymers in two dimensions and real DNA molecules (564, 1054, 2049 and 4297 bp long) imaged in air by AFM. The main result is that the frequently used Freeman estimator (L(F) = n(e) + square root 2n(o)) overestimates the real contour length of the polymers by about 4%. More accurate estimates are obtained with the Kulpa estimator (L(K) = 0.948n(e) + 1.343n(o)) or with the corner count estimator (L(C) = 0.980)n(e) + 1.406n(o) - 0.091n(c)). In the range of the DNA sizes and magnifications we have considered, however, the best results are obtained with an ad hoc developed routine that smoothes the DNA trace by a polynomial fitting of degree 3 over a moving window of 5 points. Under these conditions, the difference between the measured and the real contour length of the molecules is less than 0.4%. The accuracy of this procedure allowed us to reveal a discrete, size-dependent, shortening of DNA molecules deposited onto mica under low salt conditions and imaged in air by AFM. Awareness of this structural alteration, that can be attributed to a partial transition from B- to A-form DNA, may lead to a more correct interpretation of DNA molecules or protein-DNA complexes imaged by AFM.

Identification of the transcription termination site of the mouse nkx-1.2 gene: involvement of sequence-specific factors

We have identified a transcription termination site in the 3' flanking region of the mouse nkx-1.2 gene. A downstream transcription regulatory element in the mouse nkx-1.2 gene was characterized by transferring its 3'-fragment into a chloramphenicol acetyl transferase (CAT) expression vector. Analysis of recombinant plasmids transfected into mouse NIH3T3 cells by CAT assay showed the possible region of regulation. There were two direct repeat structures containing poly(dG-dT) x poly(dC-dA) sequences (GT repeats) in this region. The precise location of transcription termination was mapped by nuclease S1 analysis of the transcripts from recombinant plasmids transfected into COSM6 cells. It was approximately 20 nucleotides upstream of the first GT repeat within the 5' sequences of the first element of the two direct repeats. Gel mobility shift assay and footprinting analysis demonstrated that nuclear DNA binding proteins bound specifically to the sequences where the termination occurred as well as the other sequences in the second element of the direct repeats. Southwestern analysis showed that 90-, 54-, 36- and 15-kDa nuclear proteins bound to the region of the termination. It is possible that one or more of those proteins are involved in blocking the elongation of the mouse nkx-1.2 gene transcript and then result in termination.

Structures of poly(dG-dC) and poly(dA-dT) stabilized by anions

Infrared spectra were used to show that the sodium salts of acetate, sulfate and phosphate (pH 7.2) selectively stabilize some of the alternative structures of poly(dG-dC).Na and poly(dA-dT).Na as a function of hydration in nonoriented gels. NaCl was used as a reference. Each anion was present at 0.36 mole per mole of nucleotide residue. The weak absorption bands from these anions did not interfere with conclusive interpretation of the IR spectra of the polynucleotides. Poly(dG-dC).Na assumed the usual B* structure with each of the anions at high hydrations (r.h. of the ambient air > or = 94%). Lowering the hydration gave the following results. With acetate, the B* structure remained with only a small fraction of a modified Z or some other unusual structure present. With sulfate or phosphate, a sharp transition to the Z structure occurred (essentially complete by 86% r.h.). With reference to chloride ions, acetate favors the B* while sulfate and phosphate (pH 7.2) favors the Z structure. Poly(dA-dT).Na assumed the usual B structure with each of the anions at high hydrations. Lowering the hydration gave the following results. With acetate, the A structure was observed at the same hydrations as with chloride. With sulfate, a sharper transition to the A structure occurred (complete by 80% r.h.). With phosphate, a still sharper transition to the A structure occurred (complete by 86% r.h.). With reference to chloride, acetate shows little difference but sulfate and phosphate (pH 7.2) promote the A over the B structure. These results are compared with past results for NaNO3.

An A-form of poly[d(A-C)].poly[d(G-T)] induced by mercury (II) as studied by UV and FTIR spectroscopies

The conformational changes of poly[d(A-C)].poly[d(G-T)] induced by Hg(ClO4)2 in aqueous solution have been studied using UV absorption and fourth derivative spectrophotometries, and FTIR spectroscopy. The UV absorption and fourth derivative spectra reflect changes in the polynucleotide stacking interactions as a result of the metal-polynucleotide interaction. The fourth derivative spectra do not indicate a Z-form either at low or at high metal-to-polynucleotide ratios. Furthermore, the infrared spectrum at high metal-to-polynucleotide ratio (r = 1.2; r = [Hg(ClO4])2/[nucleotide] molar ratio) has the main features of an A-form, in contrast with previous CD studies which proposed that the polynucleotide adopts a Z-form under these conditions. The nature of a different conformation of the polynucleotide induced at low r-ratios (r < or = 0.2) is discussed.

Vibrational circular dichroism of A-, B-, and Z-form nucleic acids in the PO2-stretching region

Vibrational circular dichroism (VCD) spectra were measured for H2O solutions of several natural and model DNAs (single and double strands, oligomers and polymers) in the B-form, poly(dG-dC)-poly(dG-dC) in the Z-form, and various duplex RNAs in an A-form over the PO2-stretching region. Only the symmetric PO2 stretch at approximately 1075 cm-1 yields a significant intensity VCD signal. Differences of the PO2-stretching VCD spectra found for these conformational types are consistent with the spectral changes seen in the base region, but no sequence dependence was seen in contrast to VCD for base modes. The B to Z transition is accompanied by an inversion of the PO2- VCD spectra, which is characteristic of the change in the helical sense of the nucleic acid backbone. A-RNAs give rise to the same sense of couplet VCD as do B-DNAs but have a somewhat different shape because of overlapping ribose modes. These PO2- VCD spectral characteristics have been successfully modeled using simple dipole coupling calculations. The invariability of the symmetric PO2- stretching mode VCD spectra to the base sequence as opposed to that found for the C = O stretching and base deformation modes is evidence that this mode will provide a stable indication of the DNA helical sense.

Conditions for the stability of the B, C, and Z structural forms of poly(dG-dC) in the presence of lithium, potassium, magnesium, calcium, and zinc cations

The occurrence of alternative structures for the lithium, sodium, and potassium salts of poly(dG-dC) was determined as a function of hydration using IR spectra of nonoriented gels. Poly(dG-dC).K with added KCl (r = 0.56 where r is the moles of KCl per mole of nucleotide residue) gave results essentially identical to the much studied poly(dG-dC).Na with added NaCl (r = 0.56). Both gave a sharp transition from a unique B structure (hereafter designated B*) to the Z structure upon dehydration. Poly(dG-dC).Li with added LiCl (r = 0.36) assumed the B* structure at high hydration but made a broad transition to the C structures as hydration was lowered. We believe this is the first clear evidence of the C structure for poly(dG-dC). No other structures (A, D, or Z) were observed at any hydration in nonoriented gels. Poly(dG-dC).Na with added ZnCl2 (r = 0.2) existed as a mixture of the B* and Z structures in maximally hydrated gels. A broad, incomplete transition to a higher mole fraction of Z structure occurred upon dehydration. Zn2+ promotes the Z structure for poly(dG-dC) and appears to bind to guanine residues. Poly(dG-dC).Na with added MgCl2 or CaCl2 (r = 0.2) assumed the normal B* structure at maximum hydration with no hint of Z structure. Slight dehydration produced a very sharp transition to the Z structure. Both Mg2+ and Ca2+ are strong promoters of the Z structure but do not bind to cytosine or guanine residues.

The existence of unique B structures in polynucleotides with alternating purine-pyrimidine sequences

The infrared spectra of the sodium salts of calf-thymus DNA, poly(dA-dC).poly(dG-dT), poly(dA-dT) and poly(dG-dC) were measured for the samples as highly hydrated, nonoriented gels. The bands from the sugar-phosphate vibrational modes show that poly(dG-dC) assumes a B-family structure which is different from the B structures of the other samples. Poly(dG-dC) most likely assumes a wrinkled B structure. The other samples retain a smooth B structure. An alternating purine-pyrimidine sequence is not a sufficient condition for the formation of wrinkled B structure in a polynucleotide.