A method is presented for the determination of values of the spectral
density function, J(omega), describing the dynamics of amide bond vect
ors from N-15 relaxation parameters alone. Assuming that the spectral
density is given by the sum of Lorentzian functions, the approach allo
ws values of J(omega) to be obtained at omega=0, omega(N), and 0.870 o
mega(H), where omega(N) and omega(H) are Larmor frequencies of nitroge
n and proton nuclei, respectively, from measurements of N-15 T-1, T-2
and H-1-N-15 steady-state NOE values at a single spectrometer frequenc
y. Alternatively, when measurements are performed at two different spe
ctrometer frequencies of i and j MHz, J(omega) can be mapped at omega=
0, omega(N)(i), omega(N)(j), 0.870 omega(H)(i) and 0.870 omega Hj, whe
re omega Ni, for example, is the N-15 Larmor frequency for a spectrome
ter operating at i MHz. Additionally, measurements made at two differe
nt spectrometer frequencies enable contributions to transverse relaxat
ion from motions on millisecond-microsecond time scales to be evaluate
d and permit assessment of whether a description of the internal dynam
ics is consistent with a correlation function describing the dynamics
of the N-15-NH bond vector are necessary, provided that dJ(omega)/d om
ega is relatively constant between omega=omega(H) + omega(N) to omega=
omega(H)-omega(N). Simulations demonstrate that the method is accurate
for a wide range of protein motions and correlation times, and experi
mental data establish the validity of the methodology. Results are pre
sented for a folded and an unfolded form of the N-terminal SH3 domain
of the protein drk.