Luminescence resonance energy transfer analysis of RNA polymerase complexes

Resonance energy transfer allows measurement of atomic-scale distances under a variety of solution conditions. Luminescence resonance energy transfer (LRET) is a variant of energy transfer measurement in which lanthanide chelates are used as the probes. The unusual properties of lanthanide emission, in particular their long microsecond-scale lifetimes, offer several advantages for energy transfer measurements with biological samples. One of the unique features of LRET is the ability to measure energy transfer under conditions where severe heterogeneity of labeled macromolecules exists. This feature of LRET is the special emphasis of this article. We describe here LRET methodology with a particular attention to using sensitized acceptor emission to determine efficiency of energy transfer. Although we employed this technique in the characterization of Escherichia coli RNA polymerase complexes it is readily compatible with the study of essentially any protein.     

Luminescence resonance energy transfer spectroscopy of ATP-binding cassette proteins

The ATP-binding cassette (ABC) superfamily includes regulatory and transport proteins. Most human ABC exporters pump substrates out of cells using energy from ATP hydrolysis. Although major advances have been made toward understanding the molecular mechanism of ABC exporters, there are still many issues unresolved. During the last few years, luminescence resonance energy transfer has been used to detect conformational changes in real time, with atomic resolution, in isolated ABC nucleotide binding domains (NBDs) and full-length ABC exporters. NBDs are particularly interesting because they provide the power stroke for substrate transport. Luminescence resonance energy transfer (LRET) is a spectroscopic technique that can provide dynamic information with atomic-resolution of protein conformational changes under physiological conditions. Using LRET, it has been shown that NBD dimerization, a critical step in ABC proteins catalytic cycle, requires binding of ATP to two nucleotide binding sites. However, hydrolysis at just one of the sites can drive dissociation of the NBD dimer. It was also found that the NBDs of the bacterial ABC exporter MsbA reconstituted in a lipid bilayer membrane and studied at 37 °C never separate as much as suggested by crystal structures. This observation stresses the importance of performing structural/functional studies of ABC exporters under physiologic conditions. This article is part of a Special Issue entitled: Beyond the Structure-Function Horizon of Membrane Proteins edited by Ute Hellmich, Rupak Doshi and Benjamin McIlwain.     

Orientation factor in steady-state and time-resolved resonance energy transfer measurements.

Resonance energy transfer measurements provide a way to estimate distances between chromophores attached to different sites of macromolecules. There are two unknowns involved in resonance energy transfer measurements, the distance between two chromophores and their relative orientation. When static orientational disorder exists, the orientation factor, kappa 2, can vary from 0 to 4, leading to considerable uncertainty in estimation of distances. Fluorescence polarization anisotropy measurements can reduce the degree of uncertainty [Dale & Eisinger (1974) Biopolymers 13, 1573]. There may still be substantial error bounds for the average distance measurements. Time-resolved fluorescence measurements provide an "apparent" average distance and distance distribution containing contributions by both distance and orientation. The contribution of orientation to observed "apparent" average distance and distance distribution widths has been estimated for both simulated and real data. With a single unique distance as input in the simulation and with random but static orientation of donor and acceptor, the recovered average distance is very close to that of the input when the input distance is close to or larger than the F?rster distance. The recovered width of apparent distance distribution can be substantial and it changes as a function of F?rster distance to average distance ratio and as a function of F?rster distance. Similar conclusions apply to the case where there is a real distance distribution. Motional averaging of the orientation was simulated by the Monte Carlo method to estimate the contribution of orientation when chromophores have certain degrees of mobility.(ABSTRACT TRUNCATED AT 250 WORDS)     

Quantitative fluorescence resonance energy transfer measurements using fluorescence microscopy.

Fluorescence resonance energy transfer (FRET) is a technique used for quantifying the distance between two molecules conjugated to different fluorophores. By combining optical microscopy with FRET it is possible to obtain quantitative temporal and spatial information about the binding and interaction of proteins, lipids, enzymes, DNA, and RNA in vivo. In conjunction with the recent development of a variety of mutant green fluorescent proteins (mtGFPs), FRET microscopy provides the potential to measure the interaction of intracellular molecular species in intact living cells where the donor and acceptor fluorophores are actually part of the molecules themselves. However, steady-state FRET microscopy measurements can suffer from several sources of distortion, which need to be corrected. These include direct excitation of the acceptor at the donor excitation wavelengths and the dependence of FRET on the concentration of acceptor. We present a simple method for the analysis of FRET data obtained with standard filter sets in a fluorescence microscope. This method is corrected for cross talk (any detection of donor fluorescence with the acceptor emission filter and any detection of acceptor fluorescence with the donor emission filter), and for the dependence of FRET on the concentrations of the donor and acceptor. Measurements of the interaction of the proteins Bcl-2 and Beclin (a recently identified Bcl-2 interacting protein located on chromosome 17q21), are shown to document the accuracy of this approach for correction of donor and acceptor concentrations, and cross talk between the different filter units.     

Luminescence resonance energy transfer in the cytoplasm of live Escherichia coli cells

Luminescence resonance energy transfer (LRET) offers many advantages for accurate measurements of distances between specific sites in living cells, but progress in developing a methodology for implementing this technique has been limited. We report here the design, expression, and characterization of a test protein for development of a LRET methodology. The protein, which we call DAL, contains the following domains (from the N-terminus): Escherichia coli dihydrofolate reductase (DHFR), the third and fourth ankyrin repeats of p16(INK4a), a lanthanide-binding tag (LBT), and a hexahistidine tag. LBT binds Tb(3+) with a submicromolar dissociation constant. LRET was measured from the Tb(3+) site on LBT to transition metals bound to the hexa-His tag and to fluorescein methotrexate bound to DHFR. The measured distances were consistent with a molecular model constructed from the known crystal structures of the constituent domains of DAL. The results indicate that the two C-terminal ankyrin domains of p16(INK4a) are stably folded when combined with other protein domains. We found that Tb(3+) binds to DAL in the cytoplasm of live E. coli cells, and thus, DAL is useful as an indicator for studies of metal transport. We also used DAL to measure LRET from Tb(3+) to Cu(2+) in the cytoplasm of live E. coli cells. The rates of Tb(3+) and Cu(2+) transport were not affected by a proton uncoupler or an ATP synthase inhibitor. Reversal of the membrane potential had a small inhibitory effect, and removal of lipopolysaccharide had a small accelerating effect on transport. Changing the external pH from 7 to 5 strongly inhibited the Tb(3+) signal, suggesting that the Tb(3+)-LBT interaction is useful as a cytoplasmic pH indicator in the range of approximately pH 5-6.     

Dynamic docking of myosin and actin observed with resonance energy transfer

Atomic models of myosin subfragment-1 (S1) and the actin filament are docked together using resonance energy-transfer data from both pre- and postpowerstroke conditions. The quality of the resulting best fits discriminated between neck-region orientations of the S1 for a given set of experimental conditions. For measurements of the postpowerstroke states in the presence of ADP, resonance energy-transfer data alone are sufficient to dock the atomic models and provide evidence that S1 exists with at least two neck-region orientations under these conditions. To dock the prepowerstroke state, resonance energy-transfer data were used in combination with previous chemical cross-linking data to determine that a neck-region orientation similar to that of a proposed prepowerstroke state best fit the data. The resulting models determined independently from electron microscopy compare favorably with micrographs from the recent literature. The docking models by resonance energy transfer suggest that the larger movements in the light-chain binding domain are accompanied by twisting and rotating movements of the catalytic domain, causing a tilt of approximately 30 degrees during the weak-to-strong transition. This transition provides the displacement necessary to support motility and force generation.     

Selecting the right fluorophores and flow cytometer for fluorescence resonance energy transfer measurements.

BACKGROUND: Fluorescence resonance energy transfer applied in flow cytometry (FCET) is an excellent tool for determining supramolecular organization of biomolecules at the cell surface or inside the cell. Availability of new fluorophores and cytometers requires the establishment of fluorophore dye pairs most suitable for FCET measurements. METHODS: A gastric tumor cell line (N87) was labeled for major histocompatibility complex class I heavy chain and beta2-microglobulin with antibodies conjugated with fluorescein- and indocarbocyanine-like fluorophores and analyzed in FCET measurements on a cell-by-cell basis using three flow cytometers: FACSCalibur, FACSDiVa, and FACSArray. RESULTS: Normalized fluorescence intensity values were measured and normalized energy transfer efficiencies, spectral overlap integrals, and crucial dye- and instrument-dependent parameters were calculated for all matching pairs of seven fluorophores on the three commercial cytometers. The most crucial parameter in determining the applicability of the donor-acceptor pairs was the normalized fluorescence intensity and the least important one was the spectral overlap. CONCLUSIONS: On the basis of available laser lines, the optimal dye pair for all three cytometers is the Alexa546-Alexa647 pair, which produces high energy transfer efficiency values and has the best spectral characteristics with regard to laser excitation, detection of emission, and spectral overlap.     

Real-time measurements of DNA hybridization on microparticles with fluorescence resonance energy transfer

When capture oligonucleotides are tethered on planar surfaces, mass transport limitations influence the kinetics of solid-phase nucleic acid hybridizations. By diffusion theory, however, hybridization of oligonucleotides on microparticles should be reaction-rate limited. In an initial effort to understand the kinetics of microparticle hybridization reactions, we developed a fluorescence resonance energy transfer method for monitoring oligonucleotide hybridization on microparticles. Microparticles were coated with a fluoresceinated oligomer at surface densities of 20, 40, and 80% saturation, hybridized to a complementary oligonucleotide labeled with tetramethylrhodamine, and monitored over time for quenching of the fluorescein signal as hybridization occurred on the particle surface. Association rate constants were compared for microparticle-based hybridization and solution-phase hybridization. Rate constants for hybridizations on the particle surface were about an order of magnitude less than those for hybridization in solution, but decreasing the surface density of the capture oligonucleotide to 20% saturation improved particle hybridization rates. Although a bimolecular reaction model adequately described solution-phase hybridization kinetics, oligonucleotide hybridization on microparticles did not fit this model but exhibited biphasic reaction kinetics. Based on two different lines of reasoning, we argue that microparticle-based oligonucleotide hybridization was indeed reaction-rate limited in our system and not diffusion-rate limited.     

Novel calibration method for flow cytometric fluorescence resonance energy transfer measurements between visible fluorescent proteins.

BACKGROUND: The combination of fluorescence resonance energy transfer (FRET) and flow cytometry offers a statistically firm approach to study protein associations. Fusing green fluorescent protein (GFP) to a studied protein usually does not disturb the normal function of a protein, but quantitation of FRET efficiency calculated between GFP derivatives poses a problem in flow cytometry. METHODS: We generated chimeras in which cyan fluorescent protein (CFP) was separated by amino acid linkers of different sizes from yellow fluorescent protein (YFP) and used them to calibrate the cell-by-cell flow cytometric FRET measurements carried out on two different dual-laser flow cytometers. Then, CFP-Kip1 was coexpressed in yeast cells with YFP and cyclin-dependent kinase-2 (Cdk2) and served as a positive control for FRET measurements, and CFP-Kip1 coexpressed with a random peptide fused to YFP was the negative control. RESULTS: We measured donor, direct, and sensitized acceptor fluorescence intensities and developed a novel way to calculate a factor (alpha) that characterized the fluorescence intensity of acceptor molecules relative to the same number of excited donor molecules, which is essential for quantifying FRET efficiency. This was achieved by calculating FRET efficiency in two different ways and minimizing the squared difference between the two results by changing alpha. Our method reliably detected the association of Cdk2 with its inhibitor, Kip1, whereas the nonspecific FRET efficiency between Cdk2 and a random peptide was negligible. We identified and sorted subpopulations of yeast cells showing interaction between the studied proteins. CONCLUSIONS: We have described a straightforward novel calibration method to accurately quantitate FRET efficiency between GFP derivatives in flow cytometry.     

Epitope mapping by photobleaching fluorescence resonance energy transfer measurements using a laser scanning microscope system.

The donor photobleaching method (T. M. Jovin and D. J. Arndt-Jovin. 1989. Annu. Rev. Biophys. Biophys. Chem. 18:271-308.) has been adapted to an ACAS 570 (laser scanning microscope) system to measure fluorescence resonance energy transfer (FRET) on individual human peripheral blood T cells. Photobleaching was completed in approximately 100 ms in our case and it followed double-exponential kinetics. The energy transfer efficiency (E) was approximately 20% between the CD4 epitopes OKT4-FITC and Leu-3a-PE as well as between OKT4E-FITC and OKT4-PE. E was approximately 8% between OKT4-FITC and Leu-4-PE (alpha CD3) and barely detectable (approximately 4%) from OKT4-FITC to Leu-5b-PE (alpha CD2). The E values obtained by the photobleaching method were highly reproducible both in repeated measurement of identical samples and in experiments with different batches of cells and were in agreement with the flow cytometric donor quenching measurements. As expected, E measured between primary and secondary layers of antibodies increased (from approximately 14% to approximately 28%) when F(ab')2 fragments were substituted for whole antibody molecules as the donor. On a T cell line we mapped the distance between the idiotypic determinant of the T cell receptor (TcR) and the Leu-4 epitope of CD3 as proximal as E = 28%, as compared to E = 4% between a framework TcR epitope and Leu-4. In the latter case, however, approximately 40% less Leu-4 was bound suggesting that the antigen binding site of TcR is in close proximity with one of the two CD3 epsilon chains, which hence are not equivalent.     

Applications of time-resolved resonance energy transfer measurements in studies of the molecular crowding effect

The native structures of many globular proteins are only weakly stabilized and form in solution ensembles of multiple conformers. The energy differences between the conformers are assumed to be small. This is the case of flexible multidomain proteins where domain motions were observed. High concentrations of inert macrosolute, which create a crowded or confined environment, can cause shifts of the distribution of the conformers of such proteins towards the more compact structures. This effect may also promote compact structures in partially folded proteins. Time-resolved dynamic non-radiative excitation energy transfer (tr-RET) is suitable for detection of either subtle or major changes in distributions of intramolecular distances in protein molecules in solutions. Two experiments were performed which demonstrated the applicability of tr-RET for detection of the effect of macrosolutes on the conformational ensembles of flexible states of protein molecules. The distribution of distances between residues 203 and 169 in the CORE domain of E. coli adenylate kinase (AK) in the denatured state was determined in the presence of high concentrations of dextran 40. A significant shift of the mean of the distribution was observed without reduction of its width. This was interpreted as a shift to compact structure without change of the degree of disorder of the chain. In a second experiment the distribution of the distance between residues 55 and 169 in AK, which spans the cleft between the CORE and the AMPbind domains, was monitored. No clear effect of high concentrations of dextran 40 was found. These experiments show the strength of the application of tr-RET in investigation of changes in the sub-states of flexible conformations of globular protein. Networks of pairs of labeled sites can be prepared and tr-RET experiments can be performed in order to search for the segments of the protein molecules, which respond to the presence of inert macromolecules in their environment.     

Analysis of the conformational change of myosin during ATP hydrolysis using fluorescence resonance energy transfer

In order to elucidate the molecular basis of energy transduction by myosin as a molecular motor, a fluorescent ribose-modified ATP analog 2'(3')-O-[6-(N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)amino)hexanoyl]-ATP (NBD-ATP), was utilized to study the conformational change of the myosin motor domain during ATP hydrolysis using the fluorescence resonance energy transfer (FRET) method. The FRET efficiency from the fluorescent probe, BD- or AD-labeled at the reactive cysteine residues, SH1 (Cys 707) or SH2 (Cys697), respectively, to the NBD fluorophore in the ATP binding site was measured for several transient intermediates in the ATPase cycle. The FRET efficiency was greater than that using NBD-ADP. The FRETs for the myosin.ADP.AlF4- and myosin.ADP.BeFn ternary complexes, which mimic the M*.ADP.P(i) state and M.ATP state in the ATPase cycle, respectively, were similar to that of NBD-ATP. This suggests that both the SH1 and SH2 regions change their localized conformations to move closer to the ATPase site in the M*.ATP state and M**.ADP.P(i) state than in the M*.ADP state. Furthermore, we measured energy transfer from BD in the essential light chain to NBD in the active site. Assuming the efficiency at different states, myosin adopts a conformation such that the light chain moves closer to the active site by approximately 9 A during the hydrolysis of ATP.     

Luminescence resonance energy transfer investigation of conformational changes in the ligand binding domain of a kainate receptor

The apo state structure of the isolated ligand binding domain of the GluR6 subunit and the conformational changes induced by agonist binding to this protein have been investigated by luminescence resonance energy transfer (LRET) measurements. The LRET-based distances show that agonist binding induces cleft closure, and the extent of cleft closure is proportional to the extent of activation over a wide range of activations, thus establishing that the cleft closure conformational change is one of the mechanisms by which the agonist mediates receptor activation. The LRET distances also provide insight into the apo state structure, for which there is currently no crystal structure available. The distance change between the glutamate-bound state and the apo state is similar to that observed between the glutamate-bound and antagonist UBP-310-bound form of the GluR5 ligand binding domain, indicating that the cleft for the apo state of the GluR6 ligand binding domain should be similar to the UBP-310-bound form of GluR5. This observation implies that te apo state of GluR6 undergoes a cleft closure of 29-30 degrees upon binding full agonists, one of the largest observed in the glutamate receptor family.     

ATP-induced transconformation of myosin revealed by determining three-dimensional positions of fluorophores from fluorescence energy transfer measurements

The method of fluorescence resonance energy transfer (FRET) is one of the most important techniques for measuring the distance between two fluorophores and for detecting the changes in protein structure under physiological conditions. The use of green fluorescent protein is also a powerful technology that has been used to elucidate dynamic molecular events. From these we have developed a novel method to determine the three-dimensional positions of fluorophores by combining the FRET data and other structural information available. Using this method, we could determine the ATP-induced changes of three-dimensional structure of truncated Dictyostelium myosin in solution. The myosin structure with ADP in solution was found to be similar to that of the crystal structure of MgADPBeFx-bound truncated Dictyostelium myosin (type I structure), whereas myosin with ATP in solution was similar to the crystal structure of MgAdPVi-bound one (type II structure). However, the crystal structure of MgADP-bound scallop myosin (type III structure) could not be explained by any of our FRET data under various conditions. This indicates that the type III crystal structure might represent a transient intermediate conformation that could not be detected using fluorescence energy transfer.     

Single-molecule fluorescence resonance energy transfer

Fluorescent resonance energy transfer (FRET) is a powerful technique for studying conformational distribution and dynamics of biological molecules. Some conformational changes are difficult to synchronize or too rare to detect using ensemble FRET. FRET, detected at the single-molecule level, opens up new opportunities to probe the detailed kinetics of structural changes without the need for synchronization. Here, we discuss practical considerations for its implementation including experimental apparatus, fluorescent probe selection, surface immobilization, single-molecule FRET analysis schemes, and interpretation.     

Dynamics of the upper 50-kDa domain of myosin V examined with fluorescence resonance energy transfer

The upper 50-kDa region of myosin may be critical for coupling between the nucleotide- and actin-binding regions. We introduced a tetracysteine motif in the upper 50-kDa domain (residues 292-297) of myosin V containing a single IQ domain (MV 1IQ), allowing us to label this site with the fluorescein biarscenical hairpin-binding dye (FlAsH) (MV 1IQ FlAsH). The enzymatic properties of MV 1IQ FlAsH were similar to those of unlabeled MV 1IQ except for a 3-fold reduced ADP-release rate. MV 1IQ FlAsH was also capable of moving actin filaments in the in vitro motility assay. To examine rotation of the upper 50-kDa region, we determined the difference in the degree of energy transfer from N-methylanthraniloyl (mant)-labeled nucleotides to FlAsH in both steady-state and transient kinetic experiments. The energy transfer efficiency was higher with mant-ATP (0.65 +/- 0.02) compared with mant-ADP (0.55 +/- 0.02) in the absence of actin. Stopped-flow measurements suggested that the energy transfer efficiency decreased with phosphate release (0.04 s(-1)) in the absence of actin. In contrast, upon mixing MV 1IQ FlAsH in the ADP.P(i) state with actin, a decrease in the energy transfer signal was observed at a rate of 13 s(-1), similar to the ADP release rate. Our results demonstrate there was no change in the energy transfer signal upon actin-activated phosphate release and suggest that actin binding alters the dynamics of the upper 50-kDa region, which may be critical for the ability of myosin to bind tightly to both ADP and actin.     

Calculation of resonance energy transfer in crowded biological membranes.

Analytical and numerical models were developed to describe fluorescence resonance energy transfer (RET) in crowded biological membranes. It was assumed that fluorescent donors were linked to membrane proteins and that acceptors were linked to membrane lipids. No restrictions were placed on the location of the donor within the protein or the partitioning of acceptors between the two leaflets of the bilayer; however, acceptors were excluded from the area occupied by proteins. Analytical equations were derived that give the average quantum yield of a donor at low protein concentrations. Monte Carlo simulations were used to generate protein and lipid distributions that were linked numerically with RET equations to determine the average quantum yield and the distribution of donor fluorescence lifetimes at high protein concentrations, up to 50% area fraction. The Monte Carlo results show such crowding always reduces the quantum yield, probably because crowding increases acceptor concentrations near donor-bearing proteins; the magnitude of the reduction increases monotonically with protein concentration. The Monte Carlo results also show that the distribution of fluorescence lifetimes can differ markedly, even for systems possessing the same average lifetime. The dependence of energy transfer on acceptor concentration, protein radius, donor position within the protein, and the fraction of acceptors in each leaflet was also examined. The model and results are directly applicable to the analysis of RET data obtained from biological membranes; their application should result in a more complete and accurate determination of the structures of membrane components.     

Myosin structure. Proximity measurements by fluorescence energy transfer

The results of energy transfer experiments on the proximity of six sites on the globular head region of myosin are discussed. A large hydrophobic crevice has been detected on each myosin head which is sufficiently large to accommodate six aromatic rings simultaneously. In the crevice is located a thiol residue not involved in activation of myosin Ca²⁺ ATPase and a lysine residue which is specifically trinitrophenylated with 2, 4, 6-trinitrobenzenesulfonic acid. A second sulfhydryl whose modification activates the Ca²⁺ ATPase is located near the hydrophobic thiol site. The tryptophan whose fluorescence is enhanced by ATP binding is sufficiently close to the thiols and lysine residue to quantitatively transfer its energy to probes at these sites. The site of myosin ATPase has been tentatively located as being near the other five sites by energy transfer to or from synthetic chromophoric substrates. Implications of these results on the possibility of determining the location of the myosin light chain and actin binding sites are discussed.     

Calculation on fluorescence resonance energy transfer on surfaces.

A general method for estimating fluorescence resonance energy transfer between distributions of donors and acceptors on surfaces is presented. Continued fraction approximants are obtained from equivalent power series expansions of the change in quantum yield in terms of the fluorescent lifetimes or the steady-state fluorescence. These approximants provide analytic equations for the analysis of energy transfer and error bounds for the approximants. Specific approximants are derived for five models of interest for membrane biochemistry: (a) an infinite plane, (b) parallel infinite planes, (c) the surface of a sphere, (d) the surfaces of concentric spheres, and (e) the surfaces of two separated spheres. Recent experimental results in the literature are analyzed with the equations obtained.