Abstract

We analyzed single molecule FRET burst measurements using Bayesian nested sampling. The MultiNest algorithm produces accurate FRET efficiency distributions from single-molecule data. FRET efficiency distributions recovered by MultiNest and classic maximum entropy are compared for simulated data and for calmodulin labeled at residues 44 and 117. MultiNest compares favorably with maximum entropy analysis for simulated data, judged by the Bayesian evidence. FRET efficiency distributions recovered for calmodulin labeled with two different FRET dye pairs depended on the dye pair and changed upon Ca²⁺ binding. We also looked at the FRET efficiency distributions of calmodulin bound to the calcium/calmodulin dependent protein kinase II (CaMKII) binding domain. For both dye pairs, the FRET efficiency distribution collapsed to a single peak in the case of calmodulin bound to the CaMKII peptide. These measurements strongly suggest that consideration of dye–protein interactions is crucial in forming an accurate picture of protein conformations from FRET data.

We report the picosecond time-scale fluorescence dynamics of a dye-labeled DNA oligonucleotide or “aptamer” designed to bind specifically to Immunoglobulin E. Comparison of the photophysics of Texas Red (TR), fluorescein and 5′-carboxytetramethylrhodamine (TAMRA)-labeled aptamers reveals surprising differences with significant implications for measurements of oligonucleotide structure and dynamics. The fluorescence decay of the TR-aptamer is a simple single exponential with a weak temperature dependence. The fluorescence decay of the fluorescein-aptamer (fl-aptamer) is pH dependent and displays a complex temperature dependence with significant changes on melting of the aptamer tertiary structure. Despite its similarities to TR, TAMRA is strongly quenched when conjugated to the aptamer and displays complex fluorescence kinetics best described by a distributed rate model. Using the maximum entropy method, we have discovered two highly temperature-dependent fluorescence lifetimes for the TAMRA-aptamer. One of these lifetimes is similar to that of free TAMRA and displays the same temperature dependence. The other lifetime is quenched and displays a temperature dependence characteristic of a charge transfer reaction. These data set TR apart as an attractive alternative to TAMRA and fluorescein for studies such as fluorescence polarization and fluorescence resonance energy transfer, where environmental sensitivity of the probe is not desired.

The ability of peptides to form biologically active conformations that bind to receptors is governed by their dynamics and their propensity to form stable structures. Such factors are consequently important in the design of peptide drugs. Moreover, the stability of such peptides depends on interactions of the peptide with the surrounding matrix. In this article, we study the effect of the polymer poly(vinyl pyrrolidone) (PVP) on the mobility and orientational dynamics of tyrosine and a model peptide, Val–Tyr–Pro–Asn–Gly–Ala (VYPNGA) in glycerol–water solutions. Orientational dynamics are studied experimentally by time-resolved fluorescence anisotropy decays of tyrosine. The presence of PVP leads to the possibility of a distribution of environments for the peptide. The orientational dynamics of tyrosine show that the probe molecule experiences two very different environments. In one, tyrosine rotational motion is weakly coupled to PVP, while in the other, tyrosine interacts strongly with PVP leading to much slower rotational times. The dynamics of VYPNGA are more complex. Fast intramolecular, localized reorientations of the tyrosine are detected. The temperature dependence of the reorientational dynamics of the tyrosine side chain reveal that these motions are shielded from solvent friction. In contrast, global motions of the peptide are severely restricted by PVP, suggesting the ability of the polymer to restrict peptide mobility. © 2003 Wiley Periodicals, Inc. Biopolymers 69: 351–362, 2003