Fluorescence energy transfer studies of transmembrane location of retinal in purple membrane

A diffusion-enhanced energy transfer technique was employed for the determination of transmembrane location of the retinal chromophore in the purple membrane. Theoretical considerations showed that the rate of energy transfer from an energy donor embedded within a membrane to acceptors dissolved in solvent could be described by an analytical function of the distance a of closest approach between the donor and acceptor, if the "rapid-diffusion limit" was attained. The criterion for this limit was given by the relation: (RO)6 much less than 20D tau Da4, where RO is the characteristic distance of energy transfer, D is the diffusion coefficient of the acceptor and tau D is the fluorescence lifetime of the donor in the absence of acceptor. By photo-reduction of the purple membrane with sodium borohydride, the retinal chromophore was converted to a highly fluorescent derivative, which showed a broad emission band in the visible region. From analysis of the fluorescence decay curves of the photo-reduced purple membrane in the presence of various concentrations of cobalt-ethylenediamine tetraacetate (Co-EDTA: energy acceptor), the depth of the chromophore from the membrane surface was estimated to be 8 (+/-3) A. This result was supported by investigations of energy transfer processes in a system where the native purple membranes and the photo-reduced membranes were stacked in parallel: the energy acceptor in this system was the native retinal chromophore.     

The transverse location of the retinal chromophore in the purple membrane by diffusion-enhanced energy transfer

We have used fluorescence energy transfer in the rapid-diffusion limit (RDL) to estimate the trans-membrane depth of retinal in the purple membrane (PM). Chelates of Tb(III) are excellent energy donors for the retinal chromophore of PM, having a maximum Ro value for F?rster energy transfer of approximately 62 A (assuming a donor quantum yield of 1). Energy transfer rates were measured from the time-resolved emission kinetics of the donor. The distance of closest approach between chelates and the chromophore was estimated by simulating RDL energy-transfer rate constants according to geometric models of either PM sheets or membrane vesicles. The apparent rate constant for RDL energy transfer between Tb(III)HED3A and retinal in PM sheets is 1.5(+/- 0.1) x 10(6) M-1 s-1, corresponding to a depth of approximately 10 +/- 2 A for the retinal chromophore. Cell envelope vesicles (CEVs) from Halobacterium halobium were studied by using RDL energy transfer to assess the proximity of retinal to either the extracellular or intracellular face of the PM. The estimated depth of retinal from the extravesicular face of the PM is 10 +/- 3 A, based on the RDL energy-transfer rate constant. Energy-transfer levels to retinal in the PM were estimated by an indirect method with energy donors trapped in the inner-aqueous space of CEVs. The rate constants derived for this arrangement are too low to be consistent with the shortest depth of retinal deduced for PM sheets. Thus, the intravesticular face of CEVs, corresponding to the cytoplasmic face of cells, is the more distant surface from the chromophore of bacteriorhodopsin.     

荧光能量转移技术在生物学研究中的应用

荧光能量转移(FRET)是指两个携带不同荧光基团的大分子在相互间距离足够近时(10～100A)所发生的能量非放射性地由一个荧光基团向另一个荧光基团转移的现象。结合绿色荧光蛋白的发现,FRET技术可用于检测生物大分子中不同亚基的位置和生物大分子间的相互作用。近年来,FRET技术在生物学研究中的突破性进展是在活体细胞中实时监测生物大分子之间的相互作用。本文就绿色荧光蛋白的发现,FRET技术的原理、研究进展和应用前景作简要综述。     

Transmembrane Location of Retinal in Purple Membrane: Fluorescence Energy Transfer in Maximally Packed Donor-Acceptor Systems

Transmembrane location of the retinal chromophore in the purple membrane of Halobacterium halobium was investigated in three different systems in which excitation energy transfer between the chromophore and external dye molecules condensed on the membrane surfaces was observed. In system ii, the energy donor was the retinal chromophore converted in situ to a fluorescent derivative. The fluorescent membranes were embedded in solid cobalt-EDTA, which served as energy acceptors. System iii was similar to system ii, except that the acceptors were tris(2,2′-bipyridyl)ruthenium(II) complex in solid form. The positively charged ruthenium complex had a radius of 0.7 nm, whereas the cobalt complex in system ii was smaller (radius ~0.4 nm) and negatively charged. System iv was stacked sheets of native purple membrane with interspersed ruthenium complex; energy transfer from the luminescent ruthenuim complex to the native retinal chromophore was observed. The energy transfer rates in these three systems, and in two additional systems already described (Kouyama, T., K. Kinosita, Jr., and A. Ikegami, 1983, J. Mol. Biol., 165:91-107), were all consistent with a location of the retinal chromophore at a depth of 1.0 ± 0.3 nm from a surface of the purple membrane. All the analyses in the present work involved an assumption that contacts between the external dye molecules and membrane surfaces were maximal; the depth values obtained cannot be underestimates. The chromophore therefore must be outside the middle one-third of the thickness, ~4.5 nm, of the purple membrane.     

Versatile design of biohybrid light-harvesting architectures to tune location,density, and spectral coverage of attached synthetic chromophores for enhanced energy capture

Biohybrid antennas built upon chromophore–polypeptide conjugates show promise for the design of efficient light-capturing modules for specific purposes. Three new designs, each of which employs analogs of the β-polypeptide from Rhodobacter sphaeroides, have been investigated. In the first design, amino acids at seven different positions on the polypeptide were individually substituted with cysteine, to which a synthetic chromophore (bacteriochlorin or Oregon Green) was covalently attached. The polypeptide positions are at –2, –6, –10, –14, –17, –21, and –34 relative to the 0-position of the histidine that coordinates bacteriochlorophyll a (BChl a). All chromophore–polypeptides readily formed LH1-type complexes upon combination with the α-polypeptide and BChl a. Efficient energy transfer occurs from the attached chromophore to the circular array of 875 nm absorbing BChl a molecules (denoted B875). In the second design, use of two attachment sites (positions –10 and –21) on the polypeptide affords (1) double the density of chromophores per polypeptide and (2) a highly efficient energy-transfer relay from the chromophore at –21 to that at –10 and on to B875. In the third design, three spectrally distinct bacteriochlorin–polypeptides were prepared (each attached to cysteine at the –14 position) and combined in an ~1:1:1 mixture to form a heterogeneous mixture of LH1-type complexes with increased solar coverage and nearly quantitative energy transfer from each bacteriochlorin to B875. Collectively, the results illustrate the great latitude of the biohybrid approach for the design of diverse light-harvesting systems.     

Intramolecular dynamics of chain molecules monitored by fluctuations in efficiency of excitation energy transfer. A theoretical study.

The fluorescence quantum yield of a polymer molecule to which an energy donor chromophore and an energy acceptor chromophore are attached depends on the distance between the donor and acceptor chromophores. If this distance fluctuates with time, the fluorescence intensity is expected to fluctuate as well, and the time course of the intensity fluctuations will be correlated with the time course of the changes in the interchromophore distance. The intensity fluctuations are experimentally measurable if the number of illuminated molecules is small. A theoretical treatment of such fluorescence intensity fluctuations is presented in terms of a parameter that describes the polymer chain dynamics. Computer simulations were performed to illustrate the dependence of the autocorrelation function of the intensity fluctuations on the polymer chain conformation, the interchromophore energy transfer properties, and the macromolecular dynamics. These simulations demonstrate that the intensity fluctuations due to nonradiative energy transfer between chromophores attached to polymer chains can be large enough to be experimentally useful in the study of intramolecular dynamics of macromolecules.     

Diffusion-enhanced lanthanide energy-transfer study of DNA-bound cobalt(III) bleomycins: comparisons of accessibility and electrostatic potential with DNA complexes of ethidium and acridine orange

Energy transfer in the "rapid-diffusion" limit reflects the equilibrium properties of a donor-acceptor system. Rates of energy transfer from freely diffusing terbium chelates to DNA-binding chromophores change dramatically when DNA is added; energy transfer from an electrically neutral chelate is reduced because the energy acceptor becomes partially buried in DNA, while energy transfer from a positive chelate is increased because of electrostatic attraction. The rate constants for energy transfer to DNA-bound chromophores from a positively charged terbium chelate, relative to those from a neutral chelate, were used to estimate the following values for the electrostatic potential near the surface of each DNA-bound acceptor at 298 K in the presence of 1.0 mM added salt (in units of -e/kT): acridine orange, 4.54 +/- 0.11; ethidium, 4.66 +/- 0.07; green Co(III) bleomycin A2, 4.06 +/- 0.11; orange Co(III) bleomycin A2, 3.11 +/- 0.10. Smaller numbers indicate less negative potentials; these can be due to a combination of (1) positive charge on the chromophore, (2) location of the chromophore [particularly Co(III) bleomycin] away from the DNA phosphates, and/or (3) separation of DNA phosphate negative charges by an intercalator. The magnitudes of the individual rate constants indicate that all the DNA-bound chromophores can be directly encountered by the terbium probes. Energy-transfer rate constants from a neutral terbium chelate to DNA-bound and free acceptors can provide a measure of the accessibility of the terbium probe to each bound chromophore. The ratios of these rate constants were as follows: acridine orange, 0.17 +/- 0.01; ethidium, 0.27 +/- 0.02; green form of Co(III) bleomycin A2, 0.48 +/- 0.06; orange form of Co(III) bleomycin A2, 0.71 +/- 0.06. These results are consistent with the probable differences in binding mechanisms for the intercalating chromophores (ethidium and acridine orange) as compared to the Co(III) bleomycins (in which the relevant chromophores are nonintercalating metal centers). In addition, all the results imply that the green Co(III) bleomycin chromophore binds closer to DNA than the orange; this provides a first step toward understanding the structural basis for the different biological properties of these metallobleomycins. Control experiments and theoretical considerations necessary to establish the validity of the results are also presented.     

Location and orientation of the chromophore in bacteriorhodopsin: Analysis by fluorescence energy transfer

The spatial location and orientation of the retinal chromophore in bacteriorhodopsin were estimated from a fluorescence energy transfer study. The energy donor used in this study was a fluorescent retinal derivative, which was obtained by partial reduction of the purple membrane with sodium borohydride, and the energy acceptor was the native chromophore remaining in the same membrane. Since bacteriorhodopsin forms a two-dimensional crystal with P₃ symmetry in the purple membrane, and the membrane structure is maintained after the reduction, the rate of energy transfer from a donor to any acceptor existing in the same membrane can be calculated as a function of the location and orientation of the chromophores in the unit cell. Quantitative analyses of the fluorescence decay curve and the quantum yield, with various extents of reduction, enabled us to determine the most probable location and orientation. The result suggested that the chromophore was situated near the centre of the protein in such an orientation that the dipole-dipole interaction with neighbouring chromophores was close to minimum.     

Structure-function relationships and energy transfer in phycobiliprotein antennae

The present understanding of how interactions between chromophore and protein as well as between chromophore and chromophore in different aggregation states influence the spectral and excited state kinetic properties of phycobiliprotein antenna pigments is discussed. Properties of isolated phycobiliproteins from both cyanobacteria and red algae as well as from cryptophytes and of intact phycobilisomes are covered. The experimental results are discussed in terms of general principles for chromophore coupling and energy transfer. Some controversial topics in this field are outlined.     

Roles of FAD and 8-hydroxy-5-deazaflavin chromophores in photoreactivation by Anacystis nidulans DNA photolyase.

DNA photolyase from the cyanobacterium Anacystis nidulans contains two chromophores, flavin adenine dinucleotide (FADH2) and 8-hydroxy-5-deazaflavin (8-HDF) (Eker, A. P. M., Kooiman, P., Hessels, J. K. C., and Yasui, A. (1990) J. Biol. Chem. 265, 8009-8015). While evidence exists that the flavin chromophore (in FADH2 form) can catalyze photorepair directly and that the 8-HDF chromophore is the major photosensitizer in photoreactivation it was not known whether 8-HDF splits pyrimidine dimer directly or indirectly through energy transfer to FADH2 at the catalytic center. We constructed a plasmid which over-produces the A. nidulans photolyase in Escherichia coli and purified the enzyme from this organism. Apoenzyme was prepared and enzyme containing stoichiometric amounts of either or both chromophores was reconstituted. The substrate binding and catalytic activities of the apoenzyme (apoE), E-FADH2, E-8-HDF, E-FAD(ox)-8-HDF, and E-FADH2-8-HDF were investigated. We found that FAD is required for substrate binding and catalysis and that 8-HDF is not essential for binding DNA, and participates in catalysis only through energy transfer to FADH2. The quantum yields of energy transfer from 8-HDF to FADH2 and of electron transfer from FADH2 to thymine dimer are near unity.     

Chromophore of Bacteriorhodopsin is Closer to the Cytoplasmic Surface of Purple Membrane: Fluorescence Energy Transfer on Oriented Membrane Sheets

Transmembrane location of the retinal chromophore, either native or reduced in situ to a fluorescent derivative, of the purple membrane of Halobacterium halobium was investigated with fluorescence energy transfer techniques. Single sheets of purple membrane, either native or reduced with borohydride, were adsorbed on polylysine-coated glass; the orientation, whether the exposed surfaces were cytoplasmic or extracellular, was controlled by adjusting the pH of the membrane suspension before the adsorption. On the exposed surface of the reduced membrane, a layer of cytochrome c, hemoglobin, or ferritin was deposited. The rate of excitation energy transfer from the fluorescent chromophore in the membrane to the colored protein was greater when the protein was on the cytoplasmic surface of the membrane than when it was on the extracellular surface. Analysis in which uniform distribution of the protein on the surface was assumed showed that the reduced chromophore is situated at a depth of <1.5 nm from the cytoplasmic surface. The location of the native retinal chromophore was examined by depositing a small amount of tris(2,2′-bipyridyl)ruthenium(II) complex on the native membrane adsorbed on the glass. Energy transfer from the luminescent complex to the retinal chromosphore was more efficient on the cytoplasmic surface than on the extracellular surface, suggesting that the native chromophore is also on the cytoplasmic side. From these and previous results we conclude that the chromophore, whether native or reduced, of bacteriorhodopsin is located at a depth of 1.0 ± 0.3 nm from the cytoplasmic surface of purple membrane.     

Anomalous negative fluorescence anisotropy in yellow fluorescent protein (YFP 10C): quantitative analysis of FRET in YFP dimers

Yellow fluorescent protein (YFP) is widely used as a genetically encoded fluorescent marker in biology. In the course of a comprehensive study of this protein, we observed an unusual, negative fluorescence anisotropy at pH 6.0 (McAnaney, T. B., Zeng, W., Doe, C. F. E., Bhanji, N., Wakelin, S., Pearson, D. S., Abbyad, P., Shi, X., Boxer, S. G., and Bagshaw, C. R. (2005) Biochemistry 44, 5510-5524). Here we report that the fluorescence anisotropy of YFP 10C depends on protein concentration in the low micromolar range that was not expected. We propose that the negative anisotropy is a result of unidirectional F?rster resonance energy transfer (FRET) in a dimer of YFP, with the donor chromophore in the neutral form and the acceptor chromophore in the anionic form. This unusual mechanism is supported by studies of a monomeric YFP (A206K YFP) and transient-absorption spectroscopy of YFP 10C. A detailed analysis of the chromophore transition dipole moment direction is presented. The anisotropy and rate constant of this energy transfer are consistent with values produced by an analysis of the dimer structure observed in crystals.     

Inductive-resonance energy transfer between chromophores localized in different parts of irradiated and nonirradiated erythrocyte ghosts

A study was made of the inductive-resonance energy transfer between chromophore pairs, tryptophan--pyren, tryptophan--1.8-anilinonaphthalene sulfonate (ANS), puren--1.8-ANS, diphenylhexatrien--ethidium, and 1,8-ANS--ethidium, in irradiated (250 Gy) and nonirradiated preparations of erythrocytic membranes. The radiation--induced decrease in the energy transfer was noted in the pairs in which one of the chromophores was localized in a lipid phase. On the basis of the data obtained it is suggested that irradiation of membranes causes the lesions in them which lead to a reduction of the effective thickness of a hydrophobic part of the lipid bilayer.     

Consideration of dipole orientation angles yields accurate rate equations for energy transfer in the rapid diffusion limit.

Dipole-dipole energy transfer between suitable donor and acceptor chromophores is an important luminescence quenching mechanism and has been shown to be useful for distance determination at the molecular level. In the rapid diffusion limit, where the excited-state lifetime of the donor is long enough to allow the donor and acceptor to diffuse many times their average separation before deexcitation, it is usually assumed that the relative dipolar orientation is completely averaged due to rotational Brownian motion. Under this simplifying assumption, analytical expressions have been derived earlier for the energy transfer rate between donor and acceptor characterized by different geometries. Most such expressions, however, are only approximate because complete angular averaging is permitted only in a geometry that possesses spherical symmetry surrounding each chromophore. In this paper analytical expressions that correctly account for incomplete angle averaging due to steric hindrance are presented for several geometries. Each of the equations reveals a dependence of the energy transfer rate on chromophore orientation. It is shown that correctly accounting for this effect can lead to improvements in estimates of the distance of closest approach from measured quenching rates based on energy transfer experiments.     

Quantitative calculations of fluorescence polarization and absorption anisotropy kinetics of double- and triple-chromophore complexes with energy transfer.

A new method is presented for calculation of the fluorescence depolarization and kinetics of absorption anisotropy for molecular complexes with a limited number of chromophores. The method considers absorption and emission of light by both chromophores, and also energy transfer between them, with regard to their mutual orientations. The chromophores in each individual complex are rigidly positioned. The complexes are randomly distributed and oriented in space, and there is no energy transfer between them. The new "practical" formula for absorption anisotropy and fluorescence depolarization kinetics, P(t) = [3B(t) - 1 + 2A(t)]/[3 + B(t) + 4A(t)], is derived both for double- and triple-chromophore complexes with delta-pulse excitation. The parameter B(t) is given by (a) B(t) = cos2(theta) for double-chromophore complexes, and (b) B(t) = q12(t)cos2(theta 12) + q13(t)-cos2(theta 13) + q23(t)cos2(theta 23) for triple-chromophore complexes, where q12(t) + q13(t) + q23(t) = 1. Here theta ij are the angles between the chromophore transition dipole moments in the individual molecular complex. The parameters qij(t) and A(t) are dependent on chromophore spectroscopic features and on the rates of energy transfer.     

Lectin receptor proximity on HL-60 leukemia cells determined by fluorescence energy transfer using flow cytometry

Fluorescence energy transfer using flow cytometric measurements was utilized to determine the proximity of concanavalin A receptors on the surface of HL-60 promyelocytic leukemia cells before and after induction of differentiation. The HL-60 cells were induced to differentiate into granulocytes using dimethylsulfoxide and into macrophages using 12-O-tetradecanoylphorbol-13-acetate. Concanavalin A was labeled with either fluorescein (donor chromophore) or tetramethylrhodamine (acceptor chromophore), and these species were used to determine lectin proximity. With granulocytic differentiation, the amount of concanavalin A bound remained constant, but a decrease in receptor density was observed. During macrophage differentiation, however, both receptor density and receptor number increased. The increase in concanavalin A binding during differentiation appears to be a result of maturation rather than an initiating event.     

DNA-templated formation and luminescence of diphenylacetylene dimeric and trimeric complexes

We report on spectral features for two and three diphenylacetylene chromophores aligned in close proximity in aqueous solution by self assembly of attached oligonucleotide arms. Two duplex systems were examined in detail. One was formed by hybridization (Watson-Crick base pairing) of two oligonucleotide 10-mers, each containing the diphenylacetylene insert. The other was generated by self-folding of a 36-mer oligonucleotide containing two diphenylacetylene inserts. The triplex system was obtained by hybridization (Hoogsteen base pairing) of a 16-mer oligonucleotide diphenylacetylene conjugate to the folded 36-mer hairpin. Formation of duplex and triplex entities from these conjugates was demonstrated experimentally by thermal dissociation and spectroscopic studies. The UV and CD spectra for the duplex systems exhibit bands in the 300-350 nm region attributable to exciton coupling between the two chromophores, and the emission spectra show a strong band centered at 410 nm assigned to excimer fluorescence. Addition of the third strand to the hairpin duplex has little effect on the CD spectrum in the 300-350 nm region, but leads to a negative band at short wavelengths characteristic of a triplex and to a strongly enhanced band at 410 nm in the fluorescence spectrum. The third strand alone shows a broad fluorescence band at approximately 345-365 nm, but this band is virtually absent in the triplex system. A model for the triplex system is proposed in which two of the three aligned diphenylacetylenes function as a ground state dimer that on excitation gives rise to the exciton coupling observed in the UV and CD spectra and to the excimer emission observed in the fluorescence spectrum. Excitation of the third chromophore results in enhanced excimer fluorescence, as a consequence of energy transfer from the locally excited singlet of one chromophore to the ground state dimer formed by the other two chromophores.     

Polarized absorption picosecond kinetics as a probe of energy transfer in phycobilisomes of Synechococcus 6301

The energy transfer between C-phycocyanin chromophores in intact phycobilisomes of Synechococcus 6301 is shown to lead to an anisotropy relaxation with a lifetime of 10 ± 2 ps. However, due to the molecular order within the hexameric units of C-phycocyanin the anisotropy does not decay to zero. The Förster dipole-dipole mechanism of energy transfer can qualitatively explain these data provided that there is no back transfer of excitation energy and that the chromophore distribution is non-random. The rate of energy transfer in phycobilisomes between C-phycocyanin and allophycocyanin can best be described by a double exponential with lifetimes of 12 ± 3 and 84 ± 8 ps.     

Developing a structure-function model for the cryptophyte phycoerythrin 545 using ultrahigh resolution crystallography and ultrafast laser spectroscopy

Cryptophyte algae differ from cyanobacteria and red algae in the architecture of their photosynthetic light harvesting systems, even though all three are evolutionarily related. Central to cryptophyte light harvesting is the soluble antenna protein phycoerythrin 545 (PE545). The ultrahigh resolution crystal structure of PE545, isolated from a unicellular cryptophyte Rhodomonas CS24, is reported at both 1.1A and 0.97A resolution, revealing details of the conformation and environments of the chromophores. Absorption, emission and polarized steady state spectroscopy (298K, 77K), as well as ultrafast (20fs time resolution) measurements of population dynamics are reported. Coupled with complementary quantum chemical calculations of electronic transitions of the bilins, these enable assignment of spectral absorption characteristics to each chromophore in the structure. Spectral differences between the tetrapyrrole pigments due to chemical differences between bilins, as well as their binding and interaction with the local protein environment are described. Based on these assignments, and considering customized optical properties such as strong coupling, a model for light harvesting by PE545 is developed which explains the fast, directional harvesting of excitation energy. The excitation energy is funnelled from four peripheral pigments (beta158,beta82) into a central chromophore dimer (beta50/beta61) in approximately 1ps. Those chromophores, in turn, transfer the excitation energy to the red absorbing molecules located at the periphery of the complex in approximately 4ps. A final resonance energy transfer step sensitizes just one of the alpha19 bilins on a time scale of 22ps. Furthermore, it is concluded that binding of PE545 to the thylakoid membrane is not essential for efficient energy transfer to the integral membrane chlorophyll a-containing complexes associated with PS-II.