Helix-coil transition curves are calculated for poly (dA).poly(dT) and poly (dA-dT). poly (dA-dT) using the integral equation approach of Goel and Montroll.6 The transitions are described by the loop entropy model with the exponent of the loop entropy factor, k, remaining an arbitrary constant. The
Quasielastic laser light scattering and electron microscopy studies of the conformational transitions and condensation of poly(dA-dT) · poly(dA-dT)
✍ Scribed by T. J. Thomas; V. A. Bloomfield
- Publisher
- Wiley (John Wiley & Sons)
- Year
- 1985
- Tongue
- English
- Weight
- 595 KB
- Volume
- 24
- Category
- Article
- ISSN
- 0006-3525
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✦ Synopsis
Poly(dAdT).poly(dAdT) undergoes a reversible conformational transition in the presence of Co(NH&+ or spermidine in low salt (10 mM NaCl + 1 mM Na cacodylate).
This transition is similar, as judged by changes in the CD spectrum, to the B-to-X transition of the polymer provoked by alcohol and Cs+ Forlickova et al. (1983) J. Mol. Biol. 166, 85-92; (1982) Nucleic Acids Res. 10, 6969-69791 and by meso-substituted porphyrin ligands [Carvlin et al. (1983) Nucleic Acids Res. 11, 6141-61541. Under the salt conditions indicated, the CD transition begins with Co(NH,);' at about 70 pMand is complete by 150 p M ; with spermidine, it begins a t about 300 p M and is complete by 600 pM. Total intensity light scattering shows a marked increase at trivalent cation concentrations somewhat below those at which the CD transition begins. Quasielastic laser light scattering (QLS) measurement of the translational diffusion coefficient, DT, shows that, in the presence of Co(NH,$+, the hydrodynamic radius, Rh, increases from 260 to 1450 8, over the concentration range of 25 to 200 pM. With spermidine, Rh is 550$-50 8, up to 200 pM, then increases rapidly. Values of Rh in this range are generally found for toroidal or other compact condensed forms of DNA. Such forms-toroidal, spheroidal, and rodlike structures-are observed in electron micrographs of poly(dA-dT)spoly(dAdT) when the trivalent cation concentration is in the transition range. Above that range, extensive aggregation of the polymer chains is seen. Taken together, these results suggest a sequenc of related secondary and tertiary structure changes as trivalent cations are added to a low-salt solution of poly(dAdT)-poly(dAdT). At very low Co(NH,);+ or spermidine, condensation of the polymer takes place while it i s still in the B-form. Further additions of trivalent cation provoke a transition from B-to X-form, finally resulting in extensively aggregated polymer. These results are different from those generally observed with native DNA, where condensation with polyamines or Co(NH,);+ in aqueous solution is not accompanied by secondary structural change.
They are also different from those we have seen with poly(dG-me5dC).poly(dG-me5dC), where condensation and the B-Z transition occur at the same ionic conditions. These distinctions are another entry in the growing catalog of sequencedependent structural effects that may be important in the regulation of the biological activity of DNA.
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Poly(dA-dT) • poly(dA-dT) is a double-helical B DNA containing A • T and T • A base pairs in alternating sequence. Although Raman spectra of this structure have been reported previously, the temperature dependence of the Raman bands has not been examined in detail. Using a spectrometer of high spect
## Abstract The nonexchangeable base and sugar proton nmr resonances and the 260 and 278‐nm uv‐absorbance bands of the nucleic acid were utilized to monitor the temperature‐dependent duplex‐to‐strand transition of the alternating purine–pyrimidine deoxyribopolynucleotide poly(dA‐dT) in the absence
## Maryhnd20892 synopsis Conformational analysis from the pattern and intensities of cross-peaks in the two-dimensional nuclear Overhauser effect proton nmr spectra of the homopolymer, poly(dA) . poly(dT), and the analogous oligomer, d(AAAAAAITITIT),, indicate that they both exist in the B-conform