A refined model for the solution structure of oxidized putidaredoxin (Pdx(o
)), a Cys(4)Fe(2)S(2) ferredoxin, has been determined. A previous structure
(Pochapsky et al. (1994) Biochemistry 33, 6424-6432; PDB entry 1PUT) was c
alculated using the results of homonuclear two-dimensional NMR experiments.
New data has made it possible to calculate a refinement of the original Pd
x(o) solution structure, First, essentially complete assignments for diamag
netic N-15 and C-13 resonances of Pdx(o) have been made using multidimensio
nal NMR methods, and N-15- and C-13-resolved NOESY experiments have permitt
ed the identification of many new NOE restraints for structural calculation
s, Stereospecific assignments for leucine and valine CH3 resonances were ma
de using biosynthetically directed fractional C-13 labeling, improving the
precision of NOE restraints involving these residues. Backbone dihedral ang
le restraints have been obtained using a combination of two-dimensional J-m
odulated N-15,H-1 HSQC and 3D (HN)CO(CO)NH experiments. Second, the solutio
n structure of a diamagnetic form of Pdx, that of the C85S variant of galli
um putidaredoxin, in which a nonligand Cys is replaced by Ser, has been det
ermined (Pochapsky et al. (1998) J. Biomol. NMR 12, 407-415), providing inf
ormation concerning structural features not observable in the native ferred
oxin due to paramagnetism. Third, a crystal structure of a closely related
ferredoxin, bovine adrenodoxin, has been published (Muller et al. (1998) St
ructure 6, 269-280). This structure has been used to model the metal bindin
g site structure in Pdx. A family of fourteen structures is presented that
exhibits an rmsd of 0.51 Angstrom for backbone heavy atoms and 0.83 Angstro
m for all heavy atoms. Exclusion of the modeled metal binding loop region r
educes overall the rmsd to 0.30 Angstrom for backbone atoms and 0.71 Angstr
om for all heavy atoms.