Phasor approaches simplify the analysis of tryptophan fluorescence data in protein denaturation studies.

The intrinsic fluorescence of tryptophan is frequently used to investigate the structure of proteins. The analysis of tryptophan fluorescence data is challenging: fluorescence (anisotropy) decays typically have multiple lifetime (correlation time) components and fluorescence spectra are broad and exhibit only minor shifts. In this work, we show that phasor approaches can substantially simplify tryptophan fluorescence analysis. To demonstrate this, we re-analyse previously recorded datasets of the denaturant (guanidinium hydrochloride, GuHCl) induced unfolding of a single-tryptophan-containing variant of apoflavodoxin from Azotobacter vinelandii. For three methods-(1) time-resolved fluorescence, (2) time-resolved fluorescence anisotropy and (3) steady-state fluorescence spectroscopy-we show that the phasor analysis can readily identify the presence of a folding intermediate. Moreover, the fractional contributions of protein states at various stages of unfolding and the values of the free energy difference of the unfolding process [Formula: see text] are obtained. The outcomes are compared to the global analysis results published previously.

Green-fluorescent protein from the bioluminescent jellyfish Clytia gregaria is an obligate dimer and does not form a stable complex with the Ca(2+)-discharged photoprotein clytin.

Green-fluorescent protein (GFP) is the origin of the green bioluminescence color exhibited by several marine hydrozoans and anthozoans. The mechanism is believed to be Förster resonance energy transfer (FRET) within a luciferase-GFP or photoprotein-GFP complex. As the effect is found in vitro at micromolar concentrations, for FRET to occur this complex must have an affinity in the micromolar range. We present here a fluorescence dynamics investigation of the recombinant bioluminescence proteins from the jellyfish Clytia gregaria, the photoprotein clytin in its Ca(2+)-discharged form that is highly fluorescent (λ(max) = 506 nm) and its GFP (cgreGFP; λ(max) = 500 nm). Ca(2+)-discharged clytin shows a predominant fluorescence lifetime of 5.7 ns, which is assigned to the final emitting state of the bioluminescence reaction product, coelenteramide anion, and a fluorescence anisotropy decay or rotational correlation time of 12 ns (20 °C), consistent with tight binding and rotation with the whole protein. A 34 ns correlation time combined with a translational diffusion constant and molecular brightness from fluorescence fluctuation spectroscopy all confirm that cgreGFP is an obligate dimer down to nanomolar concentrations. Within the dimer, the two chromophores have a coupled excited-state transition yielding fluorescence depolarization via FRET with a transfer correlation time of 0.5 ns. The 34 ns time of cgreGFP showed no change upon addition of a 1000-fold excess of Ca(2+)-discharged clytin, indicating no stable complexation below 0.2 mM. It is proposed that any bioluminescence FRET complex with micromolar affinity must be one formed transiently by the cgreGFP dimer with a short-lived (millisecond) intermediate in the clytin reaction pathway.

A general approach for detecting folding intermediates from steady-state and time-resolved fluorescence of single-tryptophan-containing proteins.

During denaturant-induced equilibrium (un)folding of wild-type apoflavodoxin from Azotobacter vinelandii, a molten globule-like folding intermediate is formed. This wild-type protein contains three tryptophans. In this study, we use a general approach to analyze time-resolved fluorescence and steady-state fluorescence data that are obtained upon denaturant-induced unfolding of a single-tryptophan-containing variant of apoflavodoxin [i.e., W74/F128/F167 (WFF) apoflavodoxin]. The experimental data are assembled in matrices, and subsequent singular-value decomposition of these matrices (i.e., based on either steady-state or time-resolved fluorescence data) shows the presence of three significant, and independent, components. Consequently, to further analyze the denaturation trajectories, we use a three-state protein folding model in which a folding intermediate and native and unfolded protein molecules take part. Using a global analysis procedure, we determine the relative concentrations of the species involved and show that the stability of WFF apoflavodoxin against global unfolding is ∼4.1 kcal/mol. Analysis of time-resolved anisotropy data of WFF apoflavodoxin unfolding reveals the remarkable observation that W74 is equally well fixed within both the native protein and the molten globule-like folding intermediate. Slight differences between the direct environments of W74 in the folding intermediate and native protein cause different rotameric populations of the indole in both folding species as fluorescence lifetime analysis reveals. Importantly, thermodynamic analyses of the spectral denaturation trajectories of the double-tryptophan-containing protein variants WWF apoflavodoxin and WFW apoflavodoxin show that these variants are significantly more stable (5.9 kcal/mol and 6.8 kcal/mol, respectively) than WFF apoflavodoxin (4.1 kcal/mol) Hence, tryptophan residues contribute considerably to the 10.5 kcal/mol thermodynamic stability of native wild-type apoflavodoxin.

Tryptophan-tryptophan energy migration as a tool to follow apoflavodoxin folding.

Submolecular details of Azotobacter vinelandii apoflavodoxin (apoFD) (un)folding are revealed by time-resolved fluorescence anisotropy using wild-type protein and variants lacking one or two of apoFD's three tryptophans. ApoFD equilibrium (un)folding by guanidine hydrochloride follows a three-state model: native <--> unfolded <--> intermediate. In native protein, W128 is a sink for Förster resonance energy transfer (FRET). Consequently, unidirectional FRET with a 50-ps transfer correlation time occurs from W167 to W128. FRET from W74 to W167 is much slower (6.9 ns). In the intermediate, W128 and W167 have native-like geometry because the 50-ps transfer time is observed. However, non-native structure exists between W74 and W167 because instead of 6.9 ns the transfer correlation time is 2.0 ns. In unfolded apoFD this 2.0-ns transfer correlation time is also detected. This decrease in transfer correlation time is a result of W74 and W167 becoming solvent accessible and randomly oriented toward one another. Apparently W74 and W167 are near-natively separated in the folding intermediate and in unfolded apoFD. Both tryptophans may actually be slightly closer in space than in the native state, even though apoFD's radius increases substantially upon unfolding. In unfolded apoFD the 50-ps transfer time observed for native and intermediate folding states becomes 200 ps as W128 and W167 are marginally further separated than in the native state. Apparently, apoFD's unfolded state is not a featureless statistical coil but contains well-defined substructures. The approach presented is a powerful tool to study protein folding.

Octameric alcohol oxidase dissociates into stable, soluble monomers upon incubation with dimethylsulfoxide.

Alcohol oxidase (AO) is a peroxisomal, homo-octameric flavoenzyme, which catalyzes methanol oxidation in methylotrophic yeast. Here, we report on the generation of soluble, FAD-lacking AO monomers. Using steady-state fluorescence, fluorescence correlation spectroscopy, circular dichroism and static light scattering approaches, we demonstrate that FAD-lacking AO monomers are formed upon incubation of purified, native octameric AO in a solution containing 50% dimethylsulfoxide (DMSO). Upon removal of DMSO the protein remained monomeric and soluble and did not contain FAD. Binding experiments revealed that the AO monomers bind to purified pyruvate carboxylase, a protein that plays a role in the formation of enzymatically active AO octamers in vivo.

Direct observation of resonance tryptophan-to-chromophore energy transfer in visible fluorescent proteins.

Visible fluorescent proteins from Aequorea victoria contain next to the fluorophoric group a single tryptophan residue. Both molecules form a single donor-acceptor pair for resonance energy transfer (RET) within the protein. Time-resolved fluorescence experiments using tryptophan excitation have shown that RET is manifested by a distinct growing in of acceptor fluorescence at a rate characteristic for this process. In addition, time-resolved fluorescence anisotropy measurements under the same excitation-emission conditions showed a correlation time that is similar to the time constant of the same RET process with the additional benefit of gaining information on the relative orientation of the corresponding transition dipoles.

Fluorescence analysis of the Hansenula polymorpha peroxisomal targeting signal-1 receptor, Pex5p.

Correct sorting of newly synthesized peroxisomal matrix proteins is dependent on a peroxisomal targeting signal (PTS). So far two PTSs are known. PTS1 consists of a tripeptide that is located at the extreme C terminus of matrix proteins and is specifically recognized by the PTS1-receptor Pex5p. We studied Hansenula polymorpha Pex5p (HpPex5p) using fluorescence spectroscopy. The intensity of Trp fluorescence of purified HpPex5p increased by 25% upon shifting the pH from pH 6.0 to pH 7.2. Together with the results of fluorescence quenching by acrylamide, these data suggest that the conformation of HpPex5p differs at these two pH values. Fluorescence anisotropy decay measurements revealed that the pH affected the oligomeric state of HpPex5p, possibly from monomers/dimers at pH 6.0 to larger oligomeric forms at pH 7.2. Addition of dansylated peptides containing a PTS1, caused some shortening of the average fluorescence lifetime of the Trp residues, which was most pronounced at pH 7.2. Our data are discussed in relation to a molecular model of HpPex5p based on the three-dimensional structure of human Pex5p.

Physical interactions of the peroxisomal targeting signal 1 receptor pex5p, studied by fluorescence correlation spectroscopy.

We have studied Hansenula polymorpha Pex5p and Pex8p using fluorescence correlation spectroscopy (FCS). Pex5p is the Peroxisomal Targeting Signal 1 (PTS1) receptor and Pex8p is an intraperoxisomal protein. Both proteins are essential for PTS1 protein import and have been shown to physically interact. We used FCS to analyze the molecular role of this interaction. FCS is a very sensitive technique that allows analysis of dynamic processes of fluorescently marked molecules at equilibrium in a very tiny volume. We used this technique to determine the oligomeric state of both peroxins and to analyze binding of Pex5p to PTS1 peptides and Pex8p. HpPex5p and HpPex8p were overproduced in Escherichia coli, purified by affinity chromatography, and, when required, labeled with the fluorescent dye Alexa Fluor 488. FCS measurements revealed that the oligomeric state of HpPex5p varied, ranging from monomers at slightly acidic pH to tetramers at neutral pH. HpPex8p formed monomers at all pH values tested. Using fluorescein-labeled PTS1 peptide and unlabeled HpPex5p, we established that PTS1 peptide only bound to tetrameric HpPex5p. Upon addition of HpPex8p, a heterodimeric complex was formed consisting of one HpPex8p and one HpPex5p molecule. This process was paralleled by dissociation of PTS1 peptide from HpPex5p, indicating that Pex8p may play an important role in cargo release from the PTS1 receptor. Our data show that FCS is a powerful technique to explore dynamic physical interactions that occur between peroxins during peroxisomal matrix protein import.

Circular dichroism spectroscopy of fluorescent proteins.

Circular dichroism (CD) spectra have been obtained from several variants of green fluorescent protein: blue fluorescent protein (BFP), enhanced cyan fluorescent protein (CFP), enhanced green fluorescent protein (GFP), enhanced yellow fluorescent protein (YFP), all from Aequorea victoria, and the red fluorescent protein from the coral species Discosoma (DsRed). We demonstrate that CD spectra in the spectral fingerprint region of the chromophore yield spectra that after normalization are not coincident with the normalized absorbance spectra of GFP, YFP and DsRed. On the other hand, the CD spectra of BFP and CFP coincide with the absorbance spectra. The resolution of absorption and CD spectra into Gaussian bands confirmed the location of the different electronic band positions of GFP and YFP as reported in the literature using other techniques. In the case of BFP and CFP the location of Gaussian bands provided information of the vibrational progression of the electronic absorption bands. The CD spectrum of DsRed is anomalous in the sense that the major CD band has a clear excitonic character. Far-UV CD spectra of GFP confirmed the presence of the high beta-sheet content of the polypeptide chain in the three-dimensional structure.