The NMR structure of a DNA dodecamer in an aqueous dilute liquid crystalline phase

Citation
N. Tjandra et al., The NMR structure of a DNA dodecamer in an aqueous dilute liquid crystalline phase, J AM CHEM S, 122(26), 2000, pp. 6190-6200
Citations number
90
Categorie Soggetti
Chemistry & Analysis",Chemistry
Journal title
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
ISSN journal
00027863 → ACNP
Volume
122
Issue
26
Year of publication
2000
Pages
6190 - 6200
Database
ISI
SICI code
0002-7863(20000705)122:26<6190:TNSOAD>2.0.ZU;2-A
Abstract
The solution structure of the DNA dodecamer d(CGCGAATCCCG)(2) has been stud ied in an aqueous liquid crystalline medium containing 5% w/v bicelles. The se phospholipid particles impose a small degree of orientation on the DNA d uplex molecules with respect to the magnetic field and permit the measureme nt of dipolar interactions. Experiments were carried out on several samples with different isotopic labeling patterns, including two complementary sam ples, in which half of the nucleotides were uniformly enriched with C-13 an d deuterated at the H2 " and H5' positions. From this, 198 C-13-H-1 and 10 N-15-H-1 one-bond dipolar coupling restraints were derived, in addition to 200 approximate H-1-H-1 dipolar coupling and 162 structurally meaningful NO E restraints. Although loose empirical restraints for the phosphodiester ba ckbone torsion angles were essential for obtaining structures that satisfy all experimental data, they do not contribute to the energetic penalty func tion of the final minimized structures. Except for additional regular Watso n-Crick hydrogen bond restraints and standard van der Waals and electrostat ic terms used in the molecular dynamics-based structure calculation, the st ructure is determined primarily by the dipolar couplings. The final structu re is highly regular, without any significant bending or kinks, and with C2 '-endo/C1'-exo sugar puckers corresponding to regular a-form DNA. Most loca l parameters, including sugar puckers, glycosyl torsion angles, and propell er twists, are also tightly determined by the NMR data. The precision of th e determined structures is limited primarily by the uncertainty in the exac t magnitude and rhombicity of the alignment tensor. This causes considerabl e spread in parameters such as the degree of base-pair opening and the widt h of the minor groove, which are relatively sensitive to the alignment tens or values used.