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A dark yellow fluorescent protein (YFP)-based Resonance Energy-Accepting Chromoprotein (REACh) for Förster resonance energy transfer with GFP.

Förster resonance energy transfer (FRET) microscopy is a powerful technique that enables the visualization of signaling intermediates, protein interactions, and protein conformational and biochemical status. With the availability of an ever-increasing collection of fluorescent proteins, pairs of spectrally different variants have been used for the study of FRET in living cells. However, suitable spectral overlap, necessary for efficient FRET, is limited by the requirement for proper emission separation. Currently used FRET pairs represent compromises between these opposing spectral demands that reduce the maximally attainable FRET sensitivity. We present a previously undescribed FRET acceptor, a nonfluorescent yellow fluorescent protein (YFP) mutant called REACh (for Resonance Energy-Accepting Chromoprotein). REACh allows the use of the photophysically superior FRET donor EGFP, with which it exhibits optimal spectral overlap, which obviates the need for narrow spectral filtering and allows additional fluorescent labels to be used within the same cell. The latter allows the generation of sophisticated bioassays for complex biological questions. We show that this dark acceptor is ideally suited for donor fluorescence lifetime imaging microscopy (FLIM) and confirm these measurements with an independent intensity-based donor fluorescence quenching resonance energy transfer (FqRET) assay. REACh also can be used in donor photobleaching kinetics-based FRET studies. By detecting FRET between a GFP-tagged ubiquitination substrate and REACh-labeled ubiquitin, we imaged the active ubiquitination machinery inside cells. This assay therefore can be used to study proteins whose function is regulated by ubiquitination.

Animals↗

Mechanism of carotenoid singlet excited state energy transfer in modified bacterial reaction centers.

Ultrafast transient laser spectroscopy has been used to investigate carotenoid singlet excited state energy transfer in various Rhodobacter (Rb.) sphaeroides reaction centers (RCs) modified either genetically or chemically. The pathway and efficiency of energy transfer were examined as a function of the structures and energies of the donor and acceptor molecules. On the donor side, carotenoids with various extents of pi-electron conjugation were examined. RCs studied include those from the anaerobically grown wild-type strain containing the carotenoid spheroidene, which has 10 conjugated carbon-carbon double bonds; the GA strain containing neurosporene, which has nine conjugated double bonds; and aerobically grown wild-type cells, as well as aerobically grown H(M182)L mutant, both containing the carbonyl-containing carotenoid spheroidenone, which has 11 conjugated double bonds. By varying the structure of the carotenoid, we observed the effect of altering the energies of the carotenoid excited states on the rate of energy transfer. Both S(1)- and S(2)-mediated carotenoid-to-bacteriochlorophyll energy transfer processes were observed. The highest transfer efficiency, from both the S(1) and S(2) states, was observed using the carotenoid with the shortest chain. The S(1)-mediated carotenoid-to- bacteriochlorophyll energy transfer efficiencies were determined to be 96%, 84%, and 73% for neurosporene, spheroidene, and spheroidenone, respectively. The S(2)-mediated energy transfer efficiencies follow the same trend but could not be determined quantitatively because of limitations in the time resolution of the instrumentation. The dependence of the energy transfer rate on the energetics of the energy transfer acceptor was verified by performing measurements with RCs from the H(M182)L mutant. In this mutant, the bacteriochlorophyll (denoted B(B)) located between the carotenoid and the RC special pair (P) is replaced by a bacteriopheophytin (denoted phi(B)), where the Q(X) and Q(Y) bands of phi(B) are 1830 and 1290 cm(-1), respectively, higher in energy than those of B(B). These band shifts associated with phi(B) in the H(M182)L mutant significantly alter the spectral overlap between the carotenoid and phi(B), resulting in a significant decrease of the transfer efficiency from the carotenoid S(1) state to phi(B). This leaves energy transfer from the carotenoid S(2) state to phi(B) as the dominant channel. Largely because of this change in mechanism, the overall efficiency of energy transfer from the carotenoid to P decreases to less than 50% in this mutant. Because the spectral signature of phi(B) is different from that of B(A) in this mutant, we were able to demonstrate clearly that the carotenoid-to-P energy transfer is via phi(B). This finding supports the concept that, in wild-type RCs, the carotenoid-to-P energy transfer occurs through the cofactor located at the B(B) position.

Carotenoids↗

Direct detection of phospholamban and sarcoplasmic reticulum Ca-ATPase interaction in membranes using fluorescence resonance energy transfer.

We used fluorescence resonance energy transfer (FRET) to detect and quantitate the interaction of the sarcoplasmic reticulum Ca-ATPase (SERCA) with phospholamban (PLB) in membranes. PLB inhibits SERCA only at submicromolar Ca. It has been proposed that relief of inhibition at micromolar Ca is due to dissociation of the inhibitory complex. To test this hypothesis, we co-reconstituted donor-labeled SERCA and acceptor-labeled I40A-PLB (superinhibitory, monomeric PLB mutant) in membranes of defined lipid and protein composition, with full retention of Ca-dependent ATPase activity and inhibitory regulation by PLB. FRET from SERCA to PLB was measured as a function of membrane concentrations of PLB and SERCA, and functional activity was measured on the same samples. The data revealed clearly that the stoichiometry of binding is one PLB per SERCA, and that binding is a strict function of the ratio of total PLB to SERCA in the membrane. We conclude that the dissociation constant of PLB binding to SERCA is far less than physiological PLB membrane concentrations. Binding at low Ca (pCa 6.5), where I40A-PLB inhibits SERCA, was virtually identical to that at high Ca (pCa 5.0), where no inhibition was observed. However, the limiting energy transfer at saturating PLB was less at high Ca, indicating a greater donor-acceptor distance. We conclude that (a) the affinity of PLB for SERCA is so great that PLB is essentially a SERCA subunit under physiological conditions and (b) relief of inhibition at micromolar Ca is due to a structural rearrangement within the SERCA-PLB complex, rather than dissociation.

Calcium↗

Estimates of mechanical work and energy transfers: demonstration of a rigid body power model of the recovery leg in gait.

Many studies concerning the mechanical work and efficiency of human motion have used models based on segmental energy. It has been shown theoretically that such work estimates may be in error due to offsetting compensations in power sources underlying the energy profiles. Further, mechanical energy transfers calculated from these energy models have been interpreted as metabolic energy-saving mechanisms. This paper examines the use of mechanical power analysis to calculate work and energy transfer estimates, using the motion of the recovery leg in walking and running for one subject as a demonstrative example. Work and energy transfer estimates from both energy and power models are compared and contrasted. The energy model underestimates the work of the recovery leg in both walking (54% of power model estimate) and running (38%), due to muscle powers at joints opposing each other in energy generation and absorption. Energy transfers calculated with energy models are shown to suffer the same problem of offsetting power sources. In contrast, the power model identifies four energy transfer mechanisms (pendulum, whip, tendon, and joint force transfers), which contribute to energy change within the leg in varying amounts. For the recovery leg, the joint force and whip transfer mechanisms have the greatest magnitude, while the pendulum and tendon transfers are much smaller. These energy transfers can be observed on a time-varying basis throughout a motion sequence and illustrate differences in energy distribution between walking and running. These power-based transfers are discussed in terms of their nature regarding metabolic energy cost and mechanical energy distribution within a multisegmented system. It is suggested that the work and energy transfers calculated from the power analysis are more accurate than those calculated from mechanical energy models and are more useful for understanding performance.

Biomechanical Phenomena↗

The aggregation state of mellitin in lipid bilayers. An energy transfer study.

We used fluorescence non-radiative energy transfer to measure the self-association of melittin in solution and when bound to lipid bilayers. Energy transfer occurred from the tryptophan residue of unlabeled melittin to an N-methyl anthraniloyl residue covalently bound to a basic lysine residue on melittin. The extent of energy transfer from tryptophan to the label was found to increase severalfold upon the salt-induced tetramerization of melittin. When bound to vesicles of dimyristoyl-L-alpha-phosphatidylcholine, the extent of energy transfer was found to be equivalent to that of monomeric melittin, irrespective of the presence of monomeric or tetrameric melittin in the aqueous phase. We conclude that membrane-bound melittin is monomeric.

Bee Venoms↗

Detecting RNA/DNA hybridization using double-labeled donor probes with enhanced fluorescence resonance energy transfer signals.

Fluorescence resonance energy transfer (FRET) occurs when two fluorophores are in close proximity, and the emission energy of a donor fluorophore is transferred to excite an acceptor fluorophore. Using such fluorescently labeled oligonucleotides as FRET probes, makes possible specific detection of RNA molecules even if similar sequences are present in the environment. A higher ratio of signal to background fluorescence is required for more sensitive probe detection. We found that double-labeled donor probes labeled with BODIPY dye resulted in a remarkable increase in fluorescence intensity compared to single-labeled donor probes used in conventional FRET. Application of this double-labeled donor system can improve a variety of FRET techniques.

DNA↗

Energy transfer spectroscopy for measuring mitochondrial metabolism in living cells.

Microscopic energy transfer spectroscopy was established using mixed solutions of reduced nicotinamide adenine dinucleotide (NADH) and the mitochondrial marker rhodamine 123 (R123). This method was applied to probe mitochondrial malfunction of cultivated endothelial cells from calf aorta incubated with various inhibitors of specific enzyme complexes of the respiratory chain. Autofluorescence of the coenzyme NADH as well as energy transfer efficacy from excited NADH molecules (energy donor) to R123 (energy acceptor) were measured by time-gated fluorescence spectroscopy. Because intermolecular distances in the nanometer range are required for radiationless energy transfer, this method is suitable to probe selectively mitochondrial NADH. Autofluorescence of endothelial cells usually exhibited a weak increase after specific inhibition of enzyme complexes of the respiratory chain. In contrast, pronounced and statistically significant changes of energy transfer efficacy were observed after inhibition of the same enzyme complexes. Detection of NADH and R123 in different nanosecond time gates following the exciting laser pulses enhances the selectivity and improves quantification of fluorescence measurements. Therefore, time-gated energy transfer spectroscopy is suggested to be an appropriate tool for probing mitochondrial malfunction.

Animals↗

Development of an autotuned transcutaneous energy transfer system.

A transcutaneous energy transfer (TET) system has been developed to power implanted devices such as heart assist devices, artificial hearts, defibrillators, and electrical stimulators. The TET system transfers power by electromagnetic induction without the need for percutaneous leads. For ease of implantation and patient comfort, it is desirable to use TET coils that are as small as possible. One problem encountered with TET designs that use small coils is a high sensitivity to coil electromagnetic coupling caused by changes in separation. These changes can result from variation in tissue thickness between subjects and from displacement of the coils that can occur during breathing and general body movement. Changes in coil coupling result in similar changes in the resonant frequency of the TET transformer, which can reduce power transfer and efficiency. The EVAD TET system was designed to address this problem by incorporating a technique for automatically tuning the power driver stage of the transformer. The system is able to deliver maximum output power of approximately 60 watts at a coil separation of 5 mm, falling to approximately 45 watts at a coil separation of 15 mm. The system can deliver a maximum efficiency of 75-80%; reducing to approximately 60% and 60 watts. The results presented demonstrate the system's ability to compensate for variations in coil separation by resonant frequency tracking. This has optimized power transfer throughout the required range of coil coupling conditions.

Defibrillators, Implantable↗

[Effect of cadmium on the absorption and excitation energy transfer in cyanobacterium Nostoc muscorum].

The absorption and energy transfer between pigments in Nostoc muscorum by the action of 10(-4) M Cd2+, when the cyanobacterium remains viable, and in the presence of 10(-3) M Cd2+, which causes the death of cells during 3-4 weeks of incubation, were studied. A comparative study by the methods of absorption and fluorescence spectrophotometry at 295 and 77 K, including derivative spectroscopy and deconvolution of emission spectra into a number of Gaussian components, showed that, in the presence of 10(-4) M Cd2+, the energy transfer from phycobilisomes to chlorophyll of photosystem I increased. After incubation with 10(-3) M Cd2+, the energy transfer from phycobilisomes to chlorophyll of photosystem II decreased, and the transfer to photosystem I was absent. New bands in the absorption spectra, in the second derivative of absorption spectra, and in the fluorescence spectra at 77 K of cyanobacterium were observed after 7 days of incubation with cadmium. We belive that these bands are due to the formation of CdS particles and Cd-pigment complexes. The conclusion about the dual effect of Cd2+ on the functioning of the energy transfer chain in N. muscorum was derived.

Cadmium↗

Applications of bioluminescence- and fluorescence resonance energy transfer to drug discovery at G protein-coupled receptors.

Bioluminescence (BRET)- and fluorescence resonance energy transfer (FRET) techniques have become integral approaches in studies of protein-protein interactions in living cells. They rely on non-radiative transfer of energy between donor and acceptor species that can be appended to the proteins of interest. These techniques display exquisite dependence on distance and orientation between the energy transfer partners. This means they are well suited to measure both small conformational changes in response to ligand binding between partner proteins that remain within a complex or more extensive translocations of proteins between cellular compartments that occur in response to cellular challenge. Introduction of both energy donor and acceptor into a single polypeptide can also allow the detection of ligand-induced conformational switches in monomeric proteins in the millisecond time scale. Many of these approaches are amenable to high throughput screening and the drug discovery process. G protein-coupled receptors (GPCRs) represent a key drug target class. Specific applications of resonance energy transfer techniques to the identification of ligands for this class of protein are highlighted to illustrate general principles.

Animals↗

Energy transfer in modified DNA.

Energy transfer at room temperature and in aqueous solution between two hydrocarbon chromophores, 2-acetylaminofluorene and 7-methylbenz(a)anthracene, covalently attached to DNA and to homopolynucleotide models is described. Transfer, as evidenced by changes in fluorescence intensity and polarization, is a function of secondary structure.

Acetates↗

Dynamics of energy transfer in peptide-surface collisions.

Classical trajectory simulations are performed to study energy transfer in collisions of protonated triglycine (Gly)(3) and pentaglycine (Gly)(5) ions with n-hexyl thiolate self-assembled monolayer (SAM) and diamond [111] surfaces, for a collision energy E(i) in the range of 10-110 eV and a collision angle of 45 degrees. Energy transfer to the peptide ions' internal degrees of freedom is more efficient for collision with the diamond surface; i.e., 20% transfer to peptide vibration/rotation at E(i) = 30 eV. For collision with diamond, the majority of E(i) remains in peptide translation, while the majority of the energy transfer is to surface vibrations for collision with the softer SAM surface. The energy-transfer efficiencies are very similar for (Gly)(3) and (Gly)(5). Constraining various modes of (Gly)(3) shows that the peptide torsional modes absorb approximately 80% of the energy transfer to the peptide's internal modes. The energy-transfer efficiencies depend on E(i). These simulations are compared with recent experiments of peptide SID and simulations of energy transfer in Cr(CO)(6)(+) collisions with the SAM and diamond surfaces.

Energy Transfer↗

Quantitative assessment of beta 1- and beta 2-adrenergic receptor homo- and heterodimerization by bioluminescence resonance energy transfer.

Quantitative bioluminescence resonance energy transfer (BRET) analysis was applied to the study of beta(1)- and beta(2)-adrenergic receptor homo- and heterodimerization. To assess the relative affinity between each of the protomers, BRET saturation experiments were carried out in HEK-293T cells. beta(1)- and beta(2)-adrenergic receptors were found to have similar propensity to engage in homo- and heterotropic interactions suggesting that, at equivalent expression levels of the two receptor subtypes, an equal proportion of homo- and heterodimers would form. Analysis of the data also revealed that, at equimolar expression levels of energy donor and acceptor, more than 80% of the receptor molecules exist as dimers and that this high incidence of receptor dimerization is insensitive to receptor density for expression levels varying between 1.4 and 26.9 pmol of receptor/mg of membrane protein. Taken together, these results indicate that most of the receptors expressed in cells exist as constitutive dimers and that, at least in undifferentiated fibroblasts, the proportion of homo- and heterodimers between the closely related beta(1)- and beta(2)-adrenergic receptors is determined by their relative levels of expression.

Cell Line↗

Photochemical labeling of membrane-associated and channel-forming domains of proteins directed by energy transfer.

Singlet-singlet energy transfer reactions from excited tryptophan residues to photoactivatable probes possessing a suitable chromophore, generate reactive species in the vicinity of the protein, leading to its covalent labeling. This delayed labeling process can be used to map the membrane-surrounded regions of proteins with improved efficiency when it is applied with appropriate photoactivatable phospholipids. The same principle could also be applied to the labeling of channel-forming transmembrane domains of ion channels, provided that suitable photoactivatable permeant ions were available. Both applications will be discussed with regard to their potential and feasibility.

Affinity Labels↗

Possible nystatin-protein interaction in yeast plasma membrane vesicles in the presence of ergosterol. A Förster energy transfer study.

The Förster energy transfer from tryptophan residues of membrane proteins to nystatin was measured in reconstituted yeast plasma membrane vesicles free of, or doped with, ergosterol. We wanted to elucidate whether the functional change of membrane transport proteins from H+ symporters to facilitators, observed in ergosterol-containing plasma membrane vesicles on addition of nystatin [Opekarová and Tanner (1994) FEBS Lett. 350, 46-50], is reflected in altered protein-nystatin relations within the membrane. Both frequency-domain and time-domain time-resolved fluorescence spectroscopy showed that in the presence of ergosterol nystatin is located much closer to membrane proteins than in its absence.

Cell Membrane↗

Transversal and lateral exciton energy transfer in grana thylakoids of spinach.

The excitation energy transfer between photosystem (PS) II complexes was studied in isolated grana disks and thylakoids using chlorophyll a fluorescence induction measurements in the presence of DCMU under stacked and destacked conditions. Destacking of grana was achieved using a sonication protocol in a buffer without MgCl(2). The degree of stacking was controlled and quantified by atomic force microscopy and by the concomitant absorption changes. As expected from the literature, intact thylakoids showed a strong dependency of the connectivity of PSII centers, the F(m)/F(o) ratio as well as the fraction of PSIIbeta centers on the MgCl(2) concentration. In contrast, these parameters did not change in isolated grana disks. In particular, the connectivity remained constantly high irrespective of the degree of destacking. These differences were explained by the high protein density in grana disks, which hinders separation and mixing of proteins sufficiently to change energy transfer properties. Due to the occurrence of stroma lamella in intact thylakoids, intermixing of PSII and PSI is possible and allows for changes in F(m)/F(o) ratio as is the separation of LHCII from PSII, thus leading to an increase in the fraction of PSIIbeta. Even if mixing and separation of proteins are impaired in isolated grana disks, destacking should lead to a decrease in connectivity if transversal excitation energy transfer between two opposite membranes is significant. Because the connectivity is constant over all degrees of destacking employed, we conclude that the energy transfer in granas is mainly lateral.

Chlorophyll↗

Location of cyanine-3 on double-stranded DNA: importance for fluorescence resonance energy transfer studies.

Fluorescence resonance energy transfer provides valuable long-range distance information about macromolecules in solution. Fluorescein and Cy3 are an important donor-acceptor pair of fluorophores; the characteristic Förster length for this pair on DNA is 56 A, so the pair can be used to study relatively long distances. Measurement of FRET efficiency for a series of DNA duplexes terminally labeled with fluorescein and Cy3 suggests that the Cy3 is close to the helical axis of the DNA. An NMR analysis of a self-complementary DNA duplex 5'-labeled with Cy3 shows that the fluorophore is stacked onto the end of the helix, in a manner similar to that of an additional base pair. This provides a known point from which distances calculated from FRET measurements are measured. Using the FRET efficiencies for the series of DNA duplexes as restraints, we have determined an effective position for the fluorescein, which is maximally extended laterally from the helix. The knowledge of the fluorophore positions can now be used for more precise interpretation of FRET data from nucleic acids.

Base Sequence↗

Interhead distances in myosin attached to F-actin estimated by fluorescence energy transfer spectroscopy.

Fluorescence resonance energy transfer (FRET) spectroscopy has been used to determine distances between probes attached to the most reactive sulfhydryl (SH1) group on individual myosin "heads." We measured intramolecular and intermolecular interhead distances as well as the distance between one head of heavy meromyosin (HMM) mixed with subfragment-1 (S1) heads attached to F-actin under rigor conditions. The SH1 cysteine was specifically labeled with either a donor (5-((((2-iodoacetyl)amino)ethyl)amino)naphthalene-1-sulfonic acid) or an acceptor probe (5-iodoacetamidofluorescein). In free solution, the distance between these probes was too large to allow significant FRET, but in the rigor complex with F-actin, intermolecular interhead distances between S1 molecules, HMM molecules, or S1 and HMM were determined to be 6.0-6.3 nm. The radial coordinate of the labels relative to F-actin was 5.0-6.4 nm. However, the intramolecular interhead distance in HMMs in which the two heads were labeled with D and A probes was estimated to be larger. The binding affinity of the second head of HMM(D/A) to F-actin may be reduced because of heterogeneous modification of the SH1 groups, such that the probability of single-head binding is increased.

Actins↗