Bc. Pan et al., Crystal structure of an RNA 16-mer duplex r(GCAGAGUUAAAUCUGC)(2) with nonadjacent G(syn)center dot A(+)(anti) mispairs, BIOCHEM, 38(9), 1999, pp. 2826-2831
G . A mispairs are one of the most common noncanonical structural motifs of
RNA. The 1.9 Angstrom resolution crystal structure of the RNA 16-mer r(GCA
GAGUUAAAUCUGC)(2) has been determined with two isolated or nonadjacent G .
A mispairs. The molecule crystallizes with one duplex in the asymmetric uni
t in space group R3 and unit cell dimensions a = b = c = 49.24 Angstrom and
alpha = beta = gamma = 51.2 degrees. It is the longest known oligonucleoti
de duplex at this resolution and isomorphous to the 16-mer duplex with the
C . A(+) mispairs [Pan, et al., (1998) J. Mel. Biol. 283, 977-984]. The C .
A(+) mispair behaves like a wobble pair while the G . A(+) does not. The G
. A mispairs are protonated at N1 of the adenines as in the C . A(+) mispa
irs, and two hydrogen bonds in the G(syn). A(+)(anti) conformation are form
ed. The syn guanine is stabilized by an intranucleotide hydrogen bond betwe
en the 2-amino and the 5'-phosphate groups. The G(syn). A(+)(anti) conforma
tion can provide a different surface for recognition in the grooves compare
d to other G . A hydrogen bonding schemes. The major groove is widened betw
een the two mispairs allowing access to ligands. One of the 3-fold axes is
occupied by a sodium ion and a water molecule, while a second is occupied b
y another water molecule.