EXPLORING THE DNA-BINDING DOMAIN OF GENE-V PROTEIN ENCODED BY BACTERIOPHAGE M13 WITH THE AID OF SPIN-LABELED OLIGONUCLEOTIDES IN COMBINATION WITH H-1-NMR
Pjm. Folkers et al., EXPLORING THE DNA-BINDING DOMAIN OF GENE-V PROTEIN ENCODED BY BACTERIOPHAGE M13 WITH THE AID OF SPIN-LABELED OLIGONUCLEOTIDES IN COMBINATION WITH H-1-NMR, Biochemistry, 32(36), 1993, pp. 9407-9416
The DNA binding domain of the single-stranded DNA binding protein gene
V protein encoded by the bacteriophage M13 was studied by means of H-
1 nuclear magnetic resonance, through use of a spin-labeled deoxytrinu
cleotide. The paramagnetic relaxation effects observed in the H-1-NMR
spectrum of M13 GVP upon binding of the spin-labeled ligand were made
manifest by means of 2D difference spectroscopy. In this way, a vast d
ata reduction was accomplished which enabled us to check and extend th
e analysis of the 2D spectra carried out previously as well as to prob
e the DNA binding domain and its surroundings. The DNA binding domain
is principally situated on two beta-loops. The major loop of the two i
s the so-called DNA binding loop (residues 16-28) of the protein where
the residues which constitute one side of the beta-ladder (in particu
lar, residues Ser20, Tyr26, and Leu28) are closest to the DNA spin-lab
el. The other loop is part of the so-called dyad domain of the protein
(residues 68-78), and mainly its residues at the tip are affected by
the spin-label (in particular, Phe73). In addition, a part of the so-c
alled complex domain of the protein (residues 44-51) which runs contig
uous to the DNA binding loop is in close vicinity to the DNA. The NMR
data imply that the DNA binding domain is divided over two monomeric u
nits of the GVP dimer in which the DNA binding loop and the tip of the
dyad loop are part of opposite monomers. The view of the GVP-ssDNA bi
nding interaction which emerges from our data differs from previous mo
lecular modeling proposals which were based on the GVP crystal structu
re (Brayer & McPherson, 1984; Hutchinson et al., 1990). These models i
mplicate the involvement of one or two tyrosines (Tyr34, Tyr41) of the
complex loop of the protein to participate in complex formation with
ssDNA. In the NMR studies with the spin-labeled oligonucleotides, no i
ndication of such interactions has been found. Other differences betwe
en the models and our NMR data are related to the structural differenc
es found when solution and crystal structures are compared.