SOLUTION STRUCTURE OF THE CPG CONTAINING D(CTTCGAAG)(2) OLIGONUCLEOTIDE - NMR DATA AND ENERGY CALCULATIONS ARE COMPATIBLE WITH A BI BII EQUILIBRIUM AT CPG/

Citation
A. Lefebvre et al., SOLUTION STRUCTURE OF THE CPG CONTAINING D(CTTCGAAG)(2) OLIGONUCLEOTIDE - NMR DATA AND ENERGY CALCULATIONS ARE COMPATIBLE WITH A BI BII EQUILIBRIUM AT CPG/, Biochemistry, 35(38), 1996, pp. 12560-12569
Citations number
53
Categorie Soggetti
Biology
Journal title
ISSN journal
00062960
Volume
35
Issue
38
Year of publication
1996
Pages
12560 - 12569
Database
ISI
SICI code
0006-2960(1996)35:38<12560:SSOTCC>2.0.ZU;2-D
Abstract
We report the analysis of the solution structure of the DNA duplex d(C TTCGAAG)(2) compared to that of d(CATCGATG)(2), the two oligonucleotid es being related by the permutation of residues 2 and 7. An earlier st udy has demonstrated the malleability of CpG in the tetrad TCGA of d(C ATCGATG)(2) [Lefebvre et al. (1995) Biochemistry 34, 12019-12028]. Con formations of d(CTTCGAAG)(2) were evaluated by (a) two-dimensional NMR , including proton and phosphorus experiments, (b) adiabatic mapping o f the conformational space, (c) restrained molecular mechanics underta ken with sugar phase angle, epsilon-zeta difference angle, and NOE dis tances as input, and (d) back-calculation-refinement against NOE spect ra at various mixing times. d(CTTCGAAG)(2) like d(CATCGATG)(2) exhibit s a B-DNA conformation. However, significant differences are noted bet ween the two oligonucleotides, extending up to the central CpG step, a lthough this step resides in the same TCGA tetrad in both sequences. I n structures obtained with refined NMR data, CpG adopts, for instance, a greater twist and a higher guanine phase within d(CTTCGAAG)(2) comp ared to d(CATCGATG)(2). In the former oligonucleotide, the structure o f CpG resembles strikingly that found in the ACGT tetrad of the cAMP r esponsive element [Mauffret et al. (1992) J. Mol. Biol. 227, 852-875]. Moreover, two conformers with CpG either in the BII state (epsilon, z eta = g(-), t) Or in the BI state (epsilon, zeta = t, g(-)) are found equally stable for d(CTTCGAAG)(2) The energy barrier from BI to BII co mes to only 5.7 kcal/mol, and the path of the transition is very short . When calculations on d(CTTCGAAG)2 are performed taking the BI/BII eq uilibrium into account, the agreement with both the H-1 and P-31 data is found better than in the case with a single conformation taken alon e. The BI/BII equilibrium may also occur in d(CATCGATG)(2), but the am ount of BII conformer is now found weaker compared to its analogue. Th e ability of the CpG phosphate groups to adopt the Bn. conformation co uld provide a satisfying explanation for the high mutation rates obser ved at these sites.