Circular dichroism study of stacking properties of oligodeoxyadenylates and polydeoxyadenylate. A three-state conformational model.

The temperature dependence of the circular dichroism (CD) spectra of a series of deoxyadenylates (dA)n, n = 2, 3, 6, 9, 12, infinity, in aqueous solution was studied. The data were interpreted on the basis of a new conformational model for the stacked state suggested by our previous proton NMR studies on (dA)2 and (dA)3 [C. S. M. Olsthoorn, L. J. Bostelaar, J. H. van Boom & C. Altona (1980) Eur. J. biochem. 112, 95-110]. In this model the stacked regions of the single-stranded oligomers consist of residues taking up a geometry resembling that of the B-DNA genus of structures (all sugars S or C2'-endo) except those residues at the 3' end that do not 'feel' a following stacking interaction. The deoxyribose rings in the latter residues retain (or regain when melting out removes a stacking interaction somewhere along the chain) the conformational freedom (S in equilibrium N, N = C3'-endo) that these rings possess in the monomers 2'-deoxyadenosine 5'-methylphosphate or in 2'-deoxyadenosine 3',5'-bis(methylphosphate), as the case may be. It is shown that this model allows (a) construction of the CD spectra of (dA)n, n = 3, 6, 9, 12, from those of the dimer and the polymer; (b) the separation of the weak CD displayed by the regular S-S stacking mode and the far stronger CD exhibited by the 3'-end S-N stacking (the latter CD resembles that of the A-DNA genus of structures); (c) delineation of the thermodynamics of stacking. The melting temperature remains constant and independent of chain length (about 50 degrees C) whereas delta H degrees and delta S degrees show a slight increase in absolute values on increasing n from 2 to infinity owing to small cooperativity effects. Near 0 degrees C the dimer occurs for about 90% in the stacked form, the oligomers attain even higher conformational purities. It is suggested that premelting phenomena observed in the CD spectra of double-helical DNAs may also involve local transitions from the normal B-like ----S-S-s---- stacking mode to an A-like ----S-S-N---- stacking geometry.