The unfolding of holo and apo forms of human Cu/Zn superoxide dismutase by guanidine hydrochloride has been investigated by steady-state and dynamic fluorescence. In agreement with previous observations, a stabilizing effect of the metal ions on the protein tertiary structure was apparent from comparison of apo- and holoproteins, which both showed a sharp sigmoidal transition though at different denaturant concentrations. The transition was also followed by circular dichroism to check the extent of secondary structure present at each denaturant concentration. The results are incompatible with a simple two-state mechanism for denaturation. The occurrence of a more complicated process is supported by the emission decay properties of the single tryptophanyl residue at different denaturant concentrations. A complex decay function, namely, two discrete exponentials or a continuous distribution of lifetimes, was always required to fit the data. In particular, the width of the lifetime distribution, which is maximum at the transition midpoint, reflects heterogeneity of the tryptophan microenvironment and thus the presence of different species along the denaturation pathway. In the unfolded state, the width of the lifetime distribution is broader than in the folded state probably because the tryptophan residue is affected by a larger number of local conformations. The dissociation of the dimer was also studied by varying the protein concentration at different denaturant concentrations. This process affects primarly the surface of the protein rather than its secondary structure as shown by a comparison between the tryptophan emission decay and circular dichroism data under the same conditions. Another consequence of dissociation is a greater instability in the structure of the monomers, which are more easily unfolded.(ABSTRACT TRUNCATED AT 250 WORDS)

The rotational motion of tryptophan side chains in oxidized and reduced wild-type (WT) Escherichia coli thioredoxin and in two single-tryptophan variants of E. coli thioredoxin was studied in solution in the temperature range 20-50 degrees C from 13C-NMR relaxation rate measurements at 75.4 and 125.7 MHz and at 20 degrees C from steady-state and time-resolved trp fluorescence anisotropy measurements. Tryptophan enriched with 13C at the delta 1 and epsilon 3 sites of the indole ring was incorporated into WT thioredoxin and into two single-trp mutants, W31F and W28F, in which trp-28 or trp-31 of WT thioredoxin was replaced, respectively, with phenylalanine. The NMR relaxation data were interpreted using the Lipari and Szabo "model-free" approach (G. Lipari and A. Szabo. 1982. J. Amer. Chem. Soc. 104:4546-4559) with trp steady-state anisotropy data included for the variants at 20 degrees C. Values for the correlation time for the overall rotational motion (tau m) from NMR of oxidized and reduced WT thioredoxin at 35 degrees C agree well with those given by Stone et al. (Stone, M. J., K. Chandrasekhar, A. Holmgren, P. E. Wright, and H. J. Dyson. 1993. Biochemistry. 32:426-435) from 15N NMR relaxation rates, and the dependence of tau m on viscosity and temperature was in accord with the Stokes-Einstein relationship. Order parameters (S2) near 1 were obtained for the trp side chains in the WT proteins even at 50 degrees C. A slight increase in the amplitude of motion (decrease in S2) of trp-31, which is near the protein surface, but not of trp-28, which is partially buried in the protein matrix, was observed in reduced relative to oxidized WT thioredoxin. For trp-28 in W31F, order parameters near 1 (S2 > or = 0.8) at 20 degrees C were found, whereas trp-31 in W28F yielded the smallest order parameters (S2 approximately 0.6) of any of the cases. Analysis of time-resolved anisotropy decays in W28F and W31F yielded S2 values in good agreement with NMR, but gave tau m values about 60% smaller. Generally, values of tau e, the effective correlation time for the internal motion, were < or = 60 ps from NMR, whereas somewhat longer times were obtained from fluorescence. The ability of NMR and fluorescence techniques to detect subnanosecond motions in proteins reliably is examined.

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