## 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
The helix–coil transitions of poly (dA). Poly (dT) and poly (dA-dT). Poly (dA-dT)
✍ Scribed by Roger M. Wartell
- Publisher
- Wiley (John Wiley & Sons)
- Year
- 1972
- Tongue
- English
- Weight
- 685 KB
- Volume
- 11
- Category
- Article
- ISSN
- 0006-3525
No coin nor oath required. For personal study only.
✦ Synopsis
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 theoretical calculations are compared with experimental transition curves of the two polymers. Results indicate that the stacking energies for these two polymers differ by about 1 kcal/mole of base pairs. Also, a fit between theory and experiment was not possible fork > 1.70.
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Raman spectra have been recorded for poly (dG-dT) . poly(dAdC) and poly (dA-dT) . poly(dA-dT) in low salt and at high concentrations of CsF. Poly(dGdT)poly (dAdC) shows no change in the 682-cm-I guanine mode, demonstrating the absence of the Zstructure at high salt. The 790-cm-I phosphodiester symm
## Abstract CD and uv absorption data showed that high molecular weight poly(dA‐dT) · poly(dA‐dT), at 298 K, undergoes an acid‐induced transition from B‐double helix to random coil in NaCl solutions of different concentrations, ranging from 0.005 to 0.600__M__. Similarly, titration of the polynucle