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The Arabidopsis repressor of light signaling, COP1, is regulated by nuclear exclusion: mutational analysis by bioluminescence resonance energy transfer.

Bioluminescence resonance energy transfer (BRET) between Renilla luciferase and yellow fluorescent protein has been adapted to serve as a real-time reporter on protein-protein interactions in live plant cells by using the Arabidopsis Constitutive photomorphogenesis 1 (COP1) protein as a model system. COP1 is a repressor of light signal transduction that functions as part of a nuclear E3 ubiquitin ligase. COP1 possesses a leucine-rich nuclear-exclusion signal that resides in a domain implicated in COP1 dimerization. BRET was applied in conjunction with site-directed mutagenesis to explore the respective contributions of the nuclear-exclusion and dimerization motifs to the regulation of COP1 activity in vivo. One specific mutant protein, COP1(L105A), showed increased nuclear accumulation but retained the ability to dimerize, as monitored by BRET, whereas other mutations inhibited both nuclear exclusion and COP1 dimerization. Mutant rescue and overexpression experiments indicated that nuclear exclusion of COP1 protein is a rate-limiting step in light signal transduction.

Amino Acid Sequence↗

Indirect evidence for lipid-domain formation in the transition region of phospholipid bilayers by two-probe fluorescence energy transfer.

The fluorescence energy transfer between two lipid probes, N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)-1, 2-dihexadecanoyl-sn-glycero-3-phosphoethanolamine (donor) and N-(Lissamine rhodamine B sulfonyl)-1, 2-dihexadecanoyl-sn-glycero-3-phosphoethanolamine (acceptor), incorporated into 1,2-dihexadecanoyl-sn-glycero-3-phosphocholine unilamellar and multilamellar lipid bilayers, is studied in the temperature region of the main phase transition. The two probes display different relative solubilities in the gel and fluid lipid-bilayer phases. A distinct maximum in the fluorescence intensity of the donor is observed in the transition region, indicating that the two probes are demixing and hence increasing their average separation. The observation is interpreted in terms of dynamic segregation of the two probes into coexisting gel and fluid lipid domains that are formed dynamically in the transition region due to strong density fluctuations. The interpretation of the experimental observations is supported by a detailed theoretical calculation using computer simulation of a microscopic model that takes full account of diffusion of the two probes and the fluctuations of gel and fluid lipid domains characteristic of the main phase transition.

Calorimetry, Differential Scanning↗

Clustering of peptide-loaded MHC class I molecules for endoplasmic reticulum export imaged by fluorescence resonance energy transfer.

Fluorescence resonance energy transfer between cyan fluorescent protein- and yellow fluorescent protein-tagged MHC class I molecules reports on their spatial organization during assembly and export from the endoplasmic reticulum (ER). A fraction of MHC class I molecules is clustered in the ER at steady state. Contrary to expectations from biochemical models, this fraction is not bound to the TAP. Instead, it appears that MHC class I molecules cluster after peptide loading. This clustering points toward a novel step involved in the selective export of peptide-loaded MHC class I molecules from the ER. Consistent with this model, we detected clusters of wild-type HLA-A2 molecules and of mutant A2-T134K molecules that cannot bind TAP, but HLA-A2 did not detectably cluster with A2-T134K at steady state. Lactacystin treatment disrupted the HLA-A2 clusters, but had no effect on the A2-T134K clusters. However, when cells were fed peptides with high affinity for HLA-A2, mixed clusters containing both HLA-A2 and A2-T134K were detected.

ATP Binding Cassette Transporter, Subfamily B, Mem↗

Characterization of DNA/lipid complexes by fluorescence resonance energy transfer.

Fluorescence resonance energy transfer (FRET) is a potential method for the characterization of DNA-cationic lipid complexes (lipoplexes). In this work, we used FRET models assuming a multilamellar lipoplex arrangement. The application of these models allows the determination of the distance between the fluorescent intercalator on the DNA and a membrane dye on the lipid, and/or the evaluation of encapsulation efficiencies of this liposomal vehicle. The experiments were carried out in 1,2-dioleoyl-3-trimethylammonium-propane/pUC19 complexes with different charge ratios. We used 2-(3-(diphenylhexatrienyl)propanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (DPH-PC) and 2-(4,4-difluoro-5-octyl-4-bora-3a,4a-diaza-s-indacene-3-pentanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (BODIPY-PC) as membrane dyes, and ethidium bromide (EtBr) and BOBO-1 as DNA intercalators. In cationic complexes (charge ratios (+/-) >or= 2), we verified that BOBO-1 remains bound to DNA, and FRET occurs to the membrane dye. This was also confirmed by anisotropy and lifetime measurements. In complexes with all DNA bound to the lipid (charge ratio (+/-) = 4), we determined 27 A as the distance between the donor and acceptor planes (half the repeat distance for a multilamellar arrangement). In complexes with DNA unbound to the lipids (charge ratio (+/-) = 0.5 and 2), we calculated the encapsulation efficiencies. The presented FRET methodology is, to our knowledge, the first procedure allowing quantification of lipid-DNA contact.

Binding Sites↗

Resonance energy transfer: methods and applications.

Resonance energy transfer is widely used in studies of biomolecular structure and dynamics. It provides information about distances on the order of 10 to 100 A and is thus suitable for investigating spatial relationships of interest in biochemistry. The information available from energy transfer studies has been enhanced by the advances in instrumental methods and procedures of data analysis related to fluorescence decay studies. Some practical aspects of the method are reviewed. These include sample preparation, Förster type distance determination, methods of detecting energy transfer and calculating transfer efficiency, time-resolved measurements, and data analysis. Applications of resonance energy transfer, including qualitative measurements as well as microscopy, average distance estimation, and distance distribution analysis, are surveyed.

Carbohydrates↗

Energy-transfer efficiency in stacked oligo(p-phenylene vinylene)s: pronounced effects of order.

The supramolecular structure of two types of oligo(p-phenylene vinylene) (OPV) building blocks in dodecane solution is studied. Monofunctional chromophores (MOPV) form well-defined helical assemblies, whereas bifunctional molecules (BOPV) aggregate into so-called frustrated stacks, lacking any higher helical order. This difference in organization has a major influence on the transfer of excitation energy through the assemblies. Energy transfer to supramolecularly incorporated guests (MOPV with lower bandgap) is used to probe the intrinsic differences in exciton mobility in these two types of mixed aggregates. From the observed donor fluorescence quenching, it can be concluded that the helically ordered nature of the MOPV stacks facilitates the transfer of excitation energy, yielding evidence for higher exciton mobility in the well-ordered assemblies than in the frustrated stacks. Finally, the concept of energy transfer in supramolecular assemblies is extended to the solid state by the successful implementation in a light-emitting diode (LED).

Journal Article↗

Excitation energy transfer from phycobilisomes to photosystems: a phenomenon associated with the temporal separation of photosynthesis and nitrogen fixation in a cyanobacterium, Plectonema boryanum.

Plectonema boryanum shows temporal separation of photosynthesis and nitrogen fixation under diazotrophic conditions. Low temperature fluorescence studies have shown that in vivo the nitrogen fixing and photosynthesizing cells are adapted to 'state 2' and 'state 1', respectively. During nitrogen fixation phycobilisomes seem to transfer excitation energy to photosystem I whereas during oxygenic photosynthesis the energy is transferred to photosystem II. The state 2 adapted N-phase cells failed to undergo transition to state 1 while P-phase cells exhibited state 1 to state 2 transition. The nitrogen fixing cells showed a decreased level ofpsbC transcript, lack of CP47 in thylakoid membrane, and presence of the F685 peak but absence of the F695 peak in 77 K fluorescence spectra. These results suggest that the metabolic and molecular changes associated with nitrogen fixation may favor direct energy transfer from the phycobilisomes to photosystem I. This should help the organism to achieve low photosystem II and high photosystem I activity to set temporal separation of nitrogen fixation and photosynthesis for photoautotrophic growth under diazotrophic conditions.

Bacterial Proteins↗

Spectrally resolved dynamics of energy transfer in quantum-dot assemblies: towards engineered energy flows in artificial materials.

We report on the dynamics of resonant energy transfer in monodisperse, mixed-size, and energy-gradient (layered) assemblies of CdSe nanocrystal quantum dots. Time-resolved and spectrally resolved photoluminescence directly reveals the energy-dependent transfer rate of excitons from smaller to larger dots via electrostatic coupling. The data show a rapid (0.7-1.9 ns) energy transfer directly across a large tens-of-meV energy gap (i.e., between dots of disparate size), and suggest that interdot energy transfer can approach picosecond time scales in structurally optimized systems.

Journal Article↗

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.

Chelating Agents↗

Triplet state energy transfer in several proteins.

Energy transfer between excited triplet states of aromatic amino acid residues was observed at 1.4 degrees K. The distance necessary for energy transfer between monomeric tyrosine and tryptophan residues was determined to be roughly 63 A. Total phosphorescence decay rate constants for several proteins were determined while emission corresponding to tyrosine and tryptophan residues was monitored. The observed decay rate constants are interpreted in terms of intramolecular interactions of the polypeptide residues.

Energy Transfer↗

[Research on energy transfer between riboflavin and anthrone derivative].

According to Forster's theory about energy transfer, the energy transfer between riboflavin and anthrone derivative was investigated. It was found that there is a notable energy transfer between riboflavin and anthrone derivative, and the energy transfer efficiency is affected by the following factors: heating temperature, heating time, and mass ratio. And the best ratio of riboflavin and anthrone derivative is 1:3. At the same time the energy transfer efficiency drops with increasing heating temperature and time.

Anthracenes↗

The role of contact sites between inner and outer mitochondrial membrane in energy transfer.

Three functions have been suggested to be localized in contact sites between the inner and the outer membrane of mitochondria from mammalian cells: (i) transfer of energy from matrix to cytosol through the action of peripheral kinases; (ii) import of mitochondrial precursor proteins; and (iii) transfer of lipids between outer and inner membrane. In the contact site-related energy transfer a number of kinases localized in the periphery of the mitochondrion play a crucial role. Two examples of such kinases are relevant here: (i) hexokinase isoenzyme I which is capable of binding to the outer aspect of the outer membrane; and (ii) the mitochondrial isoenzyme of creatine kinase which is localized in the intermembrane space. Recently, evidence was presented that both hexokinase and creatine kinase are preferentially localized in contact sites (Adams, V. et al. (1989) Biochim. Biophys. Acta 981, 213-225). The aim of the present experiments was two-fold. First, to establish methods which enable the bioenergetic aspects of energy transfer mediated by kinases in contact sites to be measured. In these experiments emphasis was on hexokinase, while 31P-NMR was the major experimental technique. Second, we wanted to develop methods which can give insight into factors playing a role in the formation of contact sites involved in energy transfer. In the latter approach, mitochondrial creatine kinase was studied using monolayer techniques.

Animals↗

Transfer of photoenergy in pi-conjugated polymers. Two types of photoluminescence that involve energy transfer along a polymer chain.

Two types of energy transfer in pi-conjugated polymers have been investigated using time-resolved photoluminescence (PL) techniques: type i, perpendicular-type energy transfer from the 2,3-di(p-tolyl)quinoxaline unit to the pi-conjugated main chain of poly[2,3-di(p-tolyl)quinoxaline-5,8-diyl], and type ii, parallel-type energy transfer from the oligo(pyridine-2,5-diyl) (O-Py) unit to the oligo(selenophene-2,5-diyl) (O-Se) unit in a block-type copolymer of O-Py and O-Se. Both types of energy transfer were very fast with a time constant shorter than approximately 0.1 ns; in particular, the type ii energy transfer took place with a time constant of approximately 5 ps. Both pi-conjugated polymers were considered to contain segments with various effective pi-conjugation lengths, and the energy transfer to the segment with a larger effective pi-conjugation length and a smaller pi-pi* transition energy required a longer transition time. A polarizing film was obtained by utilizing the perpendicular-type energy transfer.

Journal Article↗

Studies of transfer RNA tertiary structure by singlet-singlet energy transfer.

This distance between a base next to the anticodon of tRNA and the 3' CpCpA terminus of the molecule has been estimated by singlet-singlet energy transfer experiments. The energy donor was the Y base of unknown structure found in yeast tRNA(phe). Three different energy acceptors were used: acriflavine, proflavinyl acetic acid hydrazide, and 9-hydrazino acridine. These were attached to the periodate-oxidized 3' end of the tRNA. R(0)'s between 24 and 30 A were calculated for the three chromophore couples by assuming that the relative orientation of donor and acceptor is random. This assumption is supported by the consistency of the experimental results with all three acceptors and by studies of the fluorescence depolarization of Y. The energy transfer observed both by quenching of Y and enhanced activation of the acceptors is quite small, indicating that the anticodon is more than 40 A away from the amino acid accepting terminus. This places severe restrictions on the type of tertiary structure possible for tRNA.

Acridines↗

Evidence that the two amino termini of plasma fibronectin are in close proximity: a fluorescence energy transfer study.

A fluorescence energy transfer technique has been used to study the intramolecular distance between the two amino termini of human plasma fibronectin. The glutamine-3 residue near the amino terminus of each chain was labeled enzymatically with either monodansylcadaverine or monofluoresceinylcadaverine by use of coagulation factor XIIIa. The nonradiative fluorescence energy transfer between the dansyl (donor) and fluorescein (acceptor) pair in the same protein molecule was determined from steady-state fluorescence measurements. On the basis of the transfer efficiency of 78%, the intramolecular distance between two glutamine-3 residues of fibronectin was estimated to be approximately 23 A, suggesting that the two amino termini of plasma fibronectin are in close proximity. High salt, which affects the hydrodynamic properties of the protein, has no effect on the measured distance. The results support the contention that both compact (in low salt) and expanded (in high salt) conformers of fibronectin are relatively spherical in shape.

Energy Transfer↗

Illuminating insights into protein-protein interactions using bioluminescence resonance energy transfer (BRET).

Bioluminescence resonance energy transfer (BRET) is a straightforward biophysical technique for studying protein-protein interactions. It requires: (1) that proteins of interest and suitable controls be labeled with either a donor or acceptor molecule, (2) placement of these labeled proteins in the desired environment for assessing their potential interaction, and (3) use of suitable detection instrumentation to monitor resultant energy transfer. There are now several possible applications, combinations of donor and acceptor molecules, potential assay environments and detection system perturbations. Therefore, this review aims to demystify and clarify the important aspects of the BRET methodology that should be considered when using this technique.

Fluorescence Resonance Energy Transfer↗

Studies of transfer RNA tertiary structure of singlet-singlet energy transfer.

Five species of tRNAs bearing two different fluorescent groups were synthesized. These were suitable for intramolecular distance measurements by singlet-singlet energy transfer. The efficiency of energy transfer was determined from the sensitized emission of the energy acceptor. With the assumption that the relative orientation of donor and acceptor is random, the apparent distances between the 5'-end and the 3'-end, the 4-thiouridine and the 3'-end, the pseudouridine and 3'-end, the pseudouridine and the dihydrouridine in Escherichia coli formyl methionine tRNA, and between the 2-thiouridine (in the anticodon) and the 3'-end in E. coli glutamate tRNA were calculated to be 24 A, 38 A, 55 A, 36 A, and >65 A, respectively.

Chemical Phenomena↗

Kinetic aspects of the aggregation of Clostridium perfringens theta-toxin on erythrocyte membranes. A fluorescence energy transfer study.

Fluorescence resonance energy transfer was used to monitor aggregation kinetics of the "thiol-activated" cytolysin (perfringolysin O (PFO) or theta-toxin) of Clostridium perfringens on erythrocyte membranes. PFO was labeled with the isothiocyanate derivatives of either fluorescein or tetramethylrhodamine. No detectable change in the hemolytic activity of PFO was detected after modification with either fluorophore at a ratio of 1:2 fluorophore molecules/cytolysin molecule. Fluorescence energy transfer (FET) between the donor (fluorescein.PFO or PFOD) and the acceptor (tetramethylrhodamine.PFO or PFOA) was detected by both quenching of donor fluorescence (520 nm) and by enhancement of acceptor fluorescence (575 nm) upon aggregation of labeled cytolysin molecules. FET was only observed when PFOD and PFOA were incubated in the presence of membranes. FET was not observed when PFOD and PFOA were incubated in a membrane-free solution or when unlabeled toxin was substituted for PFOA. FET was also found to be temperature-dependent. The temperature-dependent rates of change in FET upon mixing labeled toxin with erythrocyte membranes proceeded without a lag phase and displayed an activation energy of 18.7 kcal/mol. At all temperatures aggregation of PFO was virtually complete before the onset of hemolysis, the latter exhibiting a distinct lag phase. The lag period before onset of hemolysis was temperature-dependent and exhibited an activation energy of 23.2 kcal/mol. These results suggest that the aggregation of membrane-associated PFO is necessary to initiate the hemolytic process, and the lag phase which occurs before onset of hemolysis reflects the kinetics of PFO monomer to polymer conversion.

Bacterial Toxins↗