Application of a reference convolution method to tryptophan fluorescence in proteins

Publisher Website
Google Scholar
Abstract
A reference method for the deconvolution of polarized fluorescence decay data is described. Fluorescence lifetime determinations for p‐terphenyl, p‐bis[2‐(5‐phenyloxazolyl)]benzene and N‐acetyltryptophanamide (AcTrpNH2) show that with this method more reliable fits of the decays can be made than with the scatterer method, which is most frequently used. Analysis of the AcTrpNH2 decay with p‐terphenyl as the reference compound yields an excellent fit with lifetimes of 2.985 ns for AcTrpNH2 and 1.099 ns for p‐terphenyl (20°C), whereas the AcTrpNH2 decay cannot be satisfactorily fitted when the scatterer method is used. The frequency of the detected photons is varied to determine the conditions where pulse pile‐up starts to affect the measured decays. At detection frequencies of 5 kHz and 15 kHz, which corresponds to 1.7% and 5% respectively of the rate of the excitation photons no effects are found. Decays measured at 30 kHz (10%) are distorted, indicating that pile‐up effects play a role at this frequency. The fluorescence and fluorescence anisotropy decays of the tryptophan residues in the proteins human serum albumin, horse liver alcohol dehydrogenase and lysozyme have been reanalysed with the reference method. The single tryptophan residue of the albumin is shown to be characterized by a triple‐exponential fluorescence decay. The anisotropy decay of albumin was found to be mono‐exponential with a rotational correlation time of 26 ns (20°C). The alcohol dehydrogenase has two different tryptophan residues to which single lifetimes are assigned. It is found that the rotational correlation time for the dehydrogenase changes with excitation wavelength (33 ns for λex= 295 nm and 36 ns for λex= 300 nm at 20°C), indicating a nonspherical protein molecule. Lysozyme has six tryptophan residues, which give rise to a triple‐exponential fluorescence decay. A single‐exponential decay with a rotational correlation time of 3.8 ns is found for the anisotropy. This correlation time is significantly shorter than that arising from the overall rotation and probably originates from intramolecular, segmental motion.