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.     

Transverse location of the retinal chromophore of rhodopsin in rod outer segment disc membranes

Diffusion-enhanced fluorescence energy transfer was used to study the structure of photoreceptor membranes from bovine retinal rod outer segments. The fluorescent energy donor was Tb³⁺ chelated to dipicolinate and the acceptor was the 11-cis retinal chromophore of rhodopsin in vesicles made from disc membranes. The rapid-diffusion limit for energy transfer was attained in these experiments because of the long excited state lifetime of the terbium donor (~2 ms). Under these conditions, energy transfer is very sensitive to a, the distance of closest approach between the donor and acceptor (Thomas et al., 1978). Vesicles containing terbium dipicolinate in their inner aqueous space were prepared by sonicating disc membranes in the presence of this chelate and chromatographing this mixture on a gel filtration column. The sidedness of rhodopsin in these vesicles was the same as in native disc membranes. The transfer efficiency from terbium to retinal in this sample was 43%. For an R₀ value of 46.7 Å and an average vesicle diameter of 650 Å, this corresponds to an a value of 22 Å from the inner aqueous space of the vesicle. The distance of closest approach from the external aqueous space, determined by adding terbium dipicolinate to a suspension of already formed vesicles, was found to be 28 Å. These values of a show that the retinal chromophore is far from both aqueous surfaces of the disc membrane. Hence, the transverse location of the retinal chromophore is near the center of the hydrophobic core of the disc membrane. These findings suggest that conformational changes induced by photoisomerization are transmitted through a distance of at least 20 Å within rhodopsin to trigger subsequent events in visual excitation.     

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.     

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.     

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.     

The transverse location of tryptophan residues in the purple membranes of Halobacterium halobium studied by fluorescence quenching and energy transfer

Fluorescence quenching by a series of spin-labelled fatty acids is used to map the transverse disposition of tryptophan residues in bacteriorhodopsin (the sole protein in the purple membranes of Halobacterium halobium). A new method of data analysis is employed which takes into account differences in the uptake of the quenchers into the membrane. Energy transfer from tryptophan to a set of $\text{n-(9-}\text{anthroyloxy)}$ fatty acids is used as a second technique to confirm the transverse map of tryptophan residues revealed by the quenching experiments. The relative efficiencies of quenching and energy transfer obtained experimentally are compared with those predicted on the basis of current models of bacteriorhodopsin structure. Most of the tryptophan fluorescence is located near the surface of the purple membrane. When the retinal chromophore of bacteriorhodopsin is removed, tryptophan residues deep in the membrane become fluorescent. These results indicate that the deeper residues transfer their energy to retinal in the native membrane. The retinal moiety is therefore located deep within the membrane rather than at the membrane surface.     

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.     

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.     

Fluorescence coupling across lipid bilayer membranes

Summary An energy transfer between donor and acceptor fluorophores across single lipid bilayer membranes is demonstrated. Anilino-naphthalene sulfonate is used as the donor chromophore: its fluorescence is enhanced by the presence of lipid and thus indicates association with the purely lipid membranes of our preparation of vesicles in suspension. Light emit ted by the donor molecules excites fluorescence of acriflavine, a suitable acceptor enclosed inside the vesicles. Absorption and fluorescence spectra of this system, in its components and as a whole, are presented in evidence for an energy transfer.Supported by a grant from the Medical Research Council of Canada. The results of this work were presented, in part, at the 17th Annual Meeting of the Biophysical Society, February 27–March 2, 1973, Columbus, Ohio.Scholar of the Medical Research Council of Canada.     

Distance distributions in native and random-coil troponin I from frequency-domain measurements of fluorescence energy transfer

We used time-dependent fluorescence energy transfer to determine the distribution of donor-to-acceptor distances in native and denatured troponin I(TnI). The single tryptophan residue (Trp 158) of TnI served as the donor (D), and the acceptor (A) was a labeled cysteine residue (Cys 133). The time-dependent intensity decays of the donor were measured by the frequency-domain method from 10 to 320 MHz. The frequency response of the donor emission, in the absence and presence of acceptor, was used to recover the distribution of D to A distances, using an algorithm that accounts for the intrinsic multiexponential decay of the donor. In the native state the D–A distribution is characterized by an average distance of 23 Å and a half-width of 12 Å. Denaturation results in a modest increase in the average distance to 27 Å, and a dramatic increase in half-width to 47 Å. We believe the ability to recover distance distributions will have numerous applications in the characterization of biological macromolecules.     

The distances separating Tyr-69 from the high-affinity nucleotide and metal binding sites in actin

The nucleotide binding site in actin was occupied with the fluorescent analogue formycin A 5' triphosphate which acted as a fluorescent donor for the acceptor chromophore dansyl chloride attached to Tyr-69. The distance separating the two chromophores was calculated to be 2.1 nm from the fluorescence energy transfer measurements. Similar measurements were made of the distances separating dansyl chloride, acting as donor, on Tyr-69 from Co2+ occupying the metal binding site. A distance of 2.1 nm was similarly obtained.     

Fluorescence energy transfer between active sites in aspartate transaminase.

The method of fluorescence energy transfer has been used to measure the distance between the active sites in a dimeric enzyme, aspartate aminotransferase. The procedure involves the prior preparation of a hybrid enzyme with the natural chromophore, pyridoxal phosphate, in one subunit as the aldimine and of the reduced aldimine in the other subunit. The two active site chromophores are used as donor and acceptor of the energy transfer and a distance of 21 Å is obtained for the separation of the active sites.     

Fluorescence energy transfer reveals microdomain formation at physiological temperatures in lipid mixtures modeling the outer leaflet of the plasma membrane

An approach is described using fluorescence resonance energy transfer (FRET) to detect inhomogeneity in lipid organization, on distance scales of the order of tens of nanometers or greater, in lipid bilayers. This approach compares the efficiency of energy transfer between two matched fluorescent lipid donors, differing in their affinities for ordered versus disordered regions of the bilayer, and an acceptor lipid that distributes preferentially into disordered regions. Inhomogeneities in bilayer organization, on spatial scales of tens of nanometers or greater, are detected as a marked difference in the efficiencies of quenching of fluorescence of the two donor species by the acceptor. Using a novel pair of 7-nitrobenz-2-oxa-1,3-diazol-4-yl (NBD)-labeled tetraacyl lipids as donor species with a rhodaminyl-labeled acceptor, this strategy faithfully reports homo- versus inhomogeneous mixing in each of several lipid bilayer systems whose organization on the FRET distance scale can be predicted from previous findings. Interestingly, however, the present FRET method reports clear evidence of inhomogeneity in the organization of mixtures combining sphingomyelin or saturated phospholipids with unsaturated phospholipids and physiological proportions of cholesterol, even at physiological temperatures where these systems have been reported to appear homogeneous by fluorescence microscopy. These results indicate that under physiological conditions, lipid mixtures mimicking the lipid composition of the outer leaflet of the plasma membrane can form domains on a spatial scale comparable to that inferred for the dimensions of lipid rafts in biological membranes.     

Energy transfer distance measurements in immunoglobulins. III. Location of the light-heavy interchain disulfide bond in rabbit immunoglobulin G antibody

The distance between the hapten combining site and the light-heavy interchain disulfide bond in the Fab fragment of rabbit immunoglobulin G has been determined by measuring the efficiency of energy transfer between chromophores specifically attached at these sites on the molecule. The donor chromophore, Dns-Lys⁴, was non-covalently bound in the combining site of the Fab fragment of high-affinity anti-Dns antibody. The acceptor chromophore, fluorescein, was covalently attached by disulfide interchange of racemic DiFlCys with specific sulfhydryls generated by reduction. The presence of acceptor decreased the donor fluorescence lifetime from 23.6 nanoseconds to 21.6 nanoseconds. From the transfer efficiency of 8.4%, an average separation distance of 76 ± 10 Å was calculated. However, a statistical analysis of the molar concentrations of donor and acceptor on Fab fragments showed that approximately equal numbers of Fab probably contained donor but no acceptor on the one hand, and both donor and acceptor on the other hand. The presence of the former subpopulation would result in an average measured efficiency of energy transfer that would be too low. Treatment of the decay data by a double-exponential analysis which took account of these two populations of Fab fragments, led to a transfer efficiency of 20% and a correspondingly shorter separation distance of 64 ± 10 Å. The latter value is to be preferred. From the results presented here, and those reported previously on the location of the combining site at the tip of the Fab fragment and of the interheavy chain disulfide bond (Bunting &; Cathou, 1973), a general summary of the dimensions of rabbit immunoglobulin G Fab is given.     

Laser-assisted fluorescence microscopy for measuring cell membrane dynamics.

Membranes of living cells are characterized by laser-assisted fluorescence microscopy, in particular a combination of microspectrofluorometry, total internal reflection fluorescence microscopy (TIRFM), fluorescence lifetime imaging (FLIM) and Forster resonance energy transfer (FRET) spectroscopy. The generalized polarization (GP, characterizing a spectral shift which depends on the phase of membrane lipids) as well as the effective fluorescence lifetime (tau(eff)) of the membrane marker laurdan were revealed to be appropriate parameters for membrane stiffness and fluidity. GP decreased with temperature, but increased during cell growth and was always higher for the plasma membrane than for intracellular membranes. Microdomains of different fluorescence lifetimes tau(eff) were observed at temperatures above 30 degree C and disappeared during cell aging. Non-radiative energy transfer was used to detect laurdan selectively in close proximity to a molecular acceptor (DiI) and may present a possibility for measuring membrane dynamics in specific microenvironments.     

Fluorescence and kinetic properties of Ru(III) (NH3)5 modified transferrin

Diferric transferrin was modified using aquopentaammine ruthenium(II), a reagent for surface-accessible uncoordinated histidines. Introduction of the cationic Ru(III) (NH3)3 + 5 group on the imidazole of only 5.5 of the 17 uncoordinated histidines enhances the rates of pyrophosphate-assisted iron removal from the N-terminal and C-terminal binding sites by 16- and 2-fold, respectively. This differential effect on the kinetics of the two sites may partially explain why in the native protein the N-terminal site is more labile than the C-terminal site in acidic solutions where histidine residues become positively charged through protonation. The distance between the metal site and nearby uncoordinated histidines was estimated from fluorescence energy transfer measurements using Tb (III) as the donor and pentaammine ruthenium(III)-labeled imidazole of histidine as the acceptor chromophore. A Tsou Chen-Lu statistical analysis of the fluorescence quenching data suggest that two residues in each lobe of the protein are involved in quenching the fluorescence. By using estimates for the index of refraction and the quantum yield and assuming the energy transfer follows parallel first-order kinetics, an upper limit for the donor-acceptor distance of about 1.4 nm was obtained, assuming two uncoordinated histidine residues equidistant from the metal. His-207 and His-242 in the N-terminal lobe of transferrin and His-535 and His-577 in the C-terminal lobe are within this distance, based on information from the lactoferrin crystal structure. It is postulated that His-207 in the N-terminal lobe and His-535 in the C-terminal lobe are the uncoordinated residues that, when protonated or modified with Ru(III) (NH3)3 + 5, lead to accelerated loss of iron from the two binding sites of the protein.     

Luminescence energy transfer with lanthanide chelates: interpretation of sensitized acceptor decay amplitudes

Lanthanide chelates used as donors offer several advantages over classical fluorescence probes in resonance energy transfer distance measurements. One of these advantages is that energy transfer can be conveniently measured using sensitized acceptor decay measurements. In these measurements a long microsecond lifetime of the lanthanide donor and a short nanosecond lifetime of the acceptor allow elimination of a signal from the unquenched donor. Therefore, the decay of sensitized acceptor emission reflects decay properties of the donor engaged in energy transfer. The purpose of this work is to point out the importance of the fact that the amplitude of the sensitized acceptor signal is dependent on the resonance energy transfer rate constant. Thus, in the case where there are two or more populations of donors with different energy transfer rate constants, the relative amplitudes of corresponding decay components observed in sensitized acceptor emission do not represent the relative populations of the donors. We use simulations to show that these effects can be very significant. A minor population of donors with a high rate of energy transfer can produce sensitized acceptor decay which is dominated by a decay component corresponding to this minor donor population. Using a simple experimental system of rapid diffusion limit energy transfer between a europium chelate and Cy5 acceptor we show that the predicted dependency of sensitized acceptor decay amplitude on the energy transfer rate is indeed observed. We suggest that the relative importance of decay components observed in sensitized acceptor emission should be evaluated after an appropriate correction of their values such that they properly reflect possible different populations of donors. We describe a method to perform such correction.     

Fluorescence energy transfer from diphenylhexatriene to bacteriorhodopsin in lipid vesicles

Fluorescence energy transfer between the donor diphenylhexatriene (DPH) and the acceptor retinal and fluorescence depolarization of DPH are used to test current theories for fluorescence energy transfer in two-dimensional systems and to obtain information on the effect of the intrinsic membrane protein, bacteriorhodopsin, on the order and dynamics of the lipid phase. Increasing the surface concentration of acceptors by raising the protein to lipid ratio leads to a decrease in the mean fluorescence lifetime by up to a factor of four. When the acceptor concentration is reduced at a fixed protein to lipid ratio by photochemical destruction of retinal, the lifetime increases and reaches approximately the value observed in protein-free vesicles when the bleaching is complete. The shape of the decay curve and the dependency of the mean lifetime on the surface concentration of acceptors are in agreement with theoretical predictions for a two-dimensional random distribution of donors and acceptors. From this analysis a distance of closest approach between donors and acceptors of approximately 18 A is obtained, which is close to the effective radius of bacteriorhodopsin (17 A) and consistent with current ideas about the location of retinal in the interior of the protein. In the absence of energy transfer (bleached vesicles), the steady-state fluorescence anisotropy, -r, of DPH is considerably lower than in the corresponding unbleached vesicles, indicating that the effect of energy transfer must be taken into account when interpreting -r in terms of order and dynamics.     

Compact dimension of denatured states of staphylococcal nuclease

Fluorescence and circular dichroism stopped-flow have been widely used to determine the kinetics of protein folding including folding rates and possible folding pathways. Yet, these measurements are not able to provide spatial information of protein folding/unfolding. Especially, conformations of denatured states cannot be elaborated in detail. In this study, we apply the method of fluorescence energy transfer with a stopped-flow technique to study global structural changes of the staphylococcal nuclease (SNase) mutant K45C, where lysine 45 is replaced by cysteine, during folding and unfolding. By labeling the thiol group of cysteine with TNB (5,5'-dithiobis-2-nitrobenzoic acid) as an energy acceptor and the tryptophan at position 140 as a donor, distance changes between the acceptor and the donor during folding and unfolding are measured from the efficiency of energy transfer. Results indicate that the denatured states of SNase are highly compact regardless of how the denatured states (pH-induced or GdmCl-induced) are induced. The range of distance changes between two probes is between 25.6 and 25.4 A while it is 20.4 A for the native state. Furthermore, the folding process consists of three kinetic phases while the unfolding process is a single phase. These observations agree with our previous sequential model: N(0) left arrow over right arrow D(1) left arrow over right arrow D(2) left arrow over right arrow D(3) (Chen et al., J Mol Biol 1991;220:771-778). The efficiency of protein folding may be attributed to initiating the folding process from these compact denatured structures.     

Fluorescence energy transfer measurements between the nucleotide binding site and Cys-373 in actin and their application to the kinetics of actin polymerization

Intramonomer fluorescence energy transfer between the donor epsilon-ATP bound to the nucleotide-binding site and the acceptor 7-chloro-4-nitrobenzo-2-oxa-1,3-diazole bound to Cys-373 in G-actin was measured by steady-state fluorimetry. Assuming for the orientation factor its dynamic limit K2 = 2/3, the donor and acceptor distance in a G-actin molecule was calculated to be about 3 nm. The intermonomer energy transfer in F-actin occurring between the donor bound to an actin monomer and the acceptor bound to the nearest-neighbour actin monomer was also measured and the distance was calculated to be about 4 nm. The kinetics of the actin polymerization process was studied by following the decrease in fluorescence intensity upon addition of salts to G-actin solution. The initial velocity of the fluorescence intensity change was proportional to the square of the initial G-actin concentration. The temperature dependence of the velocity was proportional to the square of the initial G-actin concentration. The temperature dependence of the velocity was proportional to exp(-10/RT). These results indicated that the initial fluorescence intensity change corresponds to monomer-dimer transformation and its activation enthalpy was 10 kcal/mol.