The nucleotide-binding site of the sarcoplasmic reticulum Ca-ATPase is conformationally altered in aged skeletal muscle.

Cellular conditions in senescent skeletal muscle have been shown to result in the loss of conformational stability of the sarcoplasmic reticulum (SR) Ca-ATPase. To identify underlying structural features of age-modified Ca-ATPase, we have utilized the fluorescence properties of protein-bound probes to assess both local and global structure. We find conformational changes that include an age-related decrease in the apparent binding affinity to high affinity calcium sites detected by fluorescence signals in both tryptophans within nearby membrane-spanning helices and fluorescein isothiocyanate (FITC) bound distally to Lys(515) within the nucleotide-binding site. In addition, a substantial (80%) age-related increase in the accessibility to soluble quenchers of fluorescence of FITC is observed without concomitant changes in bimolecular quenching constants (k(q)) for protein-bound IAEDANS, also within the nucleotide-binding domain, and tryptophans within the membrane. Using fluorescence resonance energy transfer to measure distances between IAEDANS and FITC across the nucleotide-binding domain, we find no significant age-related change in the mean donor-acceptor distance; however, significant increases are observed in the conformational heterogeneity of this domain, as assessed by the width at half-maximum (HW) of the distance distribution, increasing with age from 29.4 +/- 0.8 A to 42.5 +/- 1. 1 A. Circular dichroism indicates that the average secondary structure is unaltered with age. Thus, these data suggest tertiary structural alterations in specific regions around the nucleotide-binding site rather than global conformational changes.     

Frequency-domain fluorescence spectroscopy resolves the location of maleimide-directed spectroscopic probes within the tertiary structure of the Ca-ATPase of sarcoplasmic reticulum.

We have used fluorescence spectroscopy to characterize three covalently bound spectroscopic maleimide derivatives with respect to their location within the tertiary structure of the Ca-ATPase of sarcoplasmic reticulum (SR). These derivatives include (1) 2-(4'-maleimidoanilino)naphthalene-6-sulfonic acid, (2) 4-(dimethylamino)azobenzene-4'-maleimide, and (3) fluorescein 5'-maleimide. Biochemical assays demonstrate that modification with any of these three derivatives results in the same functional effects, observed following derivatization of cysteines 344 and 364 by N-ethylmaleimide [Saito-Nakatsuka et al. (1987) J. Biochem. (Tokyo) 101, 365-376]. These residues bracket the ATPase's phosphorylation site (Asp 351) and thus may provide spectroscopic probes of the protein's conformation in this essential region. In agreement with sequencing results, SDS-polyacrylamide gels show that maleimide-modified SR exhibits fluorescence exclusively on the A1 tryptic fragment of the Ca-ATPase. Extensive tryptic digestion followed by centrifugation demonstrates essentially all of the fluorescence was associated with the soluble rather than insoluble (membrane-associated) peptides, confirming the predicted extramembranous location of these residues. Utilizing frequency-domain fluorescence spectroscopy, we were able to recover the transient effects associated with a distribution of donor-acceptor distances. We find from these fluorescence resonance energy transfer measurements that covalently bound maleimide probes are 36 A apart, independent of whether a discrete distance is assumed or a distance distribution model is utilized, in which the conformational variability of the protein is taken into account. While a unimodal distance distribution is adequate to describe the intensity decay associated with maleimide-directed donor-acceptor pairs, a bimodal distribution of distances is necessary to describe the frequency response associated with the energy transfer between maleimide-directed chromophores and other covalently bound probes on the Ca-ATPase, consistent with the large spatial separation observed between maleimides. We recover mean distances of 42 and 77 A between maleimide sites and bound FITC (Lys 515) and mean distances of 28 and 37 A between the maleimide- and the iodoacetamide-directed probes (Cys 670 and 674, whose close proximity approximates a single locus). The measured distances are presented in a model and have permitted us to describe a unique arrangement of these covalently bound probes within both the secondary and tertiary structure of the Ca-ATPase. The resolution inherent in the frequency-domain fluorescence technique to multiple donor-acceptor distances should be generally applicable to a wide range of biological systems in which specific labeling of single unique donor-acceptor sites is not feasible.     

Phosphorylation-dependent changes in the spatial relationship between Ca-ATPase polypeptide chains in sarcoplasmic reticulum membranes.

In order to investigate possible structural changes associated with the coupling mechanisms of the Ca-ATPase in sarcoplasmic reticulum membranes, we have utilized fluorescence resonance energy transfer between spectroscopic probes covalently bound to different domains of the ATPase. Using time-correlated single photon counting, we have directly measured the energy transfer efficiency between 5-[2-[(iodoacetyl)amino]ethyl]aminonaphthalene-1-sulfonic acid (IAEDANS), that is specifically bound to the B trypic fragment at cysteines 670 and 674 and acceptors covalently bound either near the nucleotide binding site, i.e. fluorescein 5-isothiocyanate at lysine 515, also on the B fragment, or maleimide-directed probes specifically located on the A1, tryptic fragment, i.e. 4-dimethylaminoazobenzene-4'-maleimide (DABmal) or fluorescein-5-maleimide (Fmal), probably at cysteines 344 and 364. All of these donor-acceptor pairs exhibit energy transfer both within and between Ca-ATPase molecules allowing us to investigate spatial relationships between the A1 and B domains and between different ATPase polypeptide chains. Differentiation between the intra- and intermolecular components of energy transfer was accomplished in two ways: 1) by comparing the transfer efficiencies in native membranes before and after detergent solubilization and 2) by reconstituting ATPase chains that have already been labeled with either the donor or acceptor chromophores. Using this approach, we find no significant change in the intramolecular transfer efficiency between any of these donor-acceptor pairs either upon binding of calcium to the high affinity sites or upon stabilization of the phosphoenzyme intermediate, indicating that there are no large structural changes within the B tryptic fragment or, alternatively, between the A1 and B fragments. With respect to intermolecular energy transfer, we observe no effect of calcium binding on the unliganded enzyme with either donor-acceptor pair. However, formation of the phosphoenzyme intermediate results in a measurable increase in the transfer efficiency between IAEDANS and DABmal (or Fmal); this increase is reversible upon phosphoenzyme destabilization by subsequent addition of calcium. There is no corresponding change in the intermolecular component of fluorescence resonance energy transfer between IAEDANS and fluorescein 5-isothiocyanate, indicating that the change in fluorescence resonance energy transfer probably occurs as a result of reorientation of associated ATPase polypeptide chains with respect to one another.     

Distance between the agonist and noncompetitive inhibitor sites on the nicotinic acetylcholine receptor

The nicotinic acetylcholine receptor possesses an agonist binding site on each of the two alpha-subunits and an allosterically coupled noncompetitive inhibitor (NCI) site. The spatial relationships between these sites have been determined by fluorescence energy transfer employing lifetime and steady-state techniques with two donor-acceptor pairs. 6-(5-Dimethylaminonaphthalene-1-sulfonamido)hexanoic acid-beta-(N-trimethylammonium)ethyl ester (dansyl-C6-choline, an agonist) and bis(choline)-N-(4-nitrobenzo-2-oxa-1,3-diazol-7-yl)-iminodiprop rionate (BCNI, a competitive antagonist) were employed as energy donors bound to the agonist sites. Ethidium was employed as a specific probe of the NCI site and served as the energy acceptor for both donors. Under steady-state conditions, energy transfer was measured by monitoring BCNI fluorescence as a function of occupancy of ethidium. Changes in acceptor occupancy were achieved by titrating acetylcholine receptor-donor-acceptor complexes with phencyclidine, a nonfluorescent NCI ligand. Extrapolation of the data to 100% acceptor occupancy yielded a transfer efficiency of 38% for the BCNI-ethidium pair. In the second method, the transfer efficiency of the dansyl-C6-choline-ethidium pair was determined by analysis of the reduction of the donor-excited state fluorescence lifetime. The nanosecond decay rates for dansyl-C6-choline measured in the presence of phencyclidine are characterized by two lifetimes (tau 1 = 6.7; tau 2 = 17.1 ns) with an amplitude ratio, alpha 1/alpha 2 = 2.3. In the presence of ethidium, the two lifetimes were proportionally diminished while retaining a comparable ratio of amplitudes. Displacement of ethidium from the NCI site by phencyclidine restored the two lifetimes to their original values. These data indicate that the donors bound to the two agonist sites transferred energy with similar efficiencies to the acceptor. Thus, the lifetime data suggest that the NCI site is approximately equidistant from each of the agonist sites. The corrected efficiency of donor quenching by this method was 34%, a value in close accord with the steady-state measurements. The distance between the agonist sites and the NCI site was calculated to be between 21-35 A for the BCNI/ethidium pair and 22-40 A for the dansyl-C6-choline/ethidium pair. Consideration of these distances with respect to the molecular dimensions of the receptor and location of the agonist sites suggests a location for the NCI site near the ion channel at the extracellular surface of the membrane bilayer.     

Spatial relationship between the nucleotide-binding site, Lys-61 and Cys-374 in actin and a conformational change induced by myosin subfragment-1 binding

The spatial relationship between Lys-61, the nucleotide binding site and Cys-374 was studied. Lys-61 was labelled with fluorescein-5-isothiocyanate as a resonance energy acceptor, the nucleotide-binding site was labelled with the fluorescent ATP analogues epsilon ATP or formycin-A 5'-triphosphate (FTP) and Cys-374 was labelled with 5-(2-[(iodoacetyl)amino]ethyl)aminonaphthalene-1-sulfonic acid (1,5-IAEDANS) as a resonance energy donor. The distances between the nucleotide binding site and Lys-61 or between Lys-61 and Cys-374 were calculated to be 3.5 +/- 0.3 nm and 4.60 +/- 0.03 nm, respectively. (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) On the other hand, when doubly-labelled actin with 1,5-IAEDANS at Cys-374 and FITC at Lys-61 was polymerized in the presence of a twofold molar excess of phalloidin [Miki, M. (1987) Eur. J. Biochem. 164, 229-235], the fluorescence of 1,5-IAEDANS bound to actin was quenched significantly. This could be attributed to inter-monomer energy transfer. The inter-monomer distance between FITC attached to Lys-61 in a monomer and 1,5-IAEDANS attached to Cys-374 in its nearest-neighbour monomer in an F-actin filament was calculated to be 3.34 +/- 0.06 nm, assuming that the likely change in the intra-monomer distance does not change during polymerization by more than 0.4 nm. One possible spatial relationship between Lys-61, Cys-374 and the nucleotide binding site in an F-actin filament is proposed. The effect of myosin subfragment-1 (S1) binding on the energy transfer efficiency was studied. The fluorescence intensity of AEDANS-FITC-actin decreased by 30% upon interaction with S1. The fluorescence intensity of AEDANS-FITC-actin polymer in the presence of phalloidin increased by 21% upon interaction with S1. The addition of ATP led to the fluorescence intensity returning to the initial level. Assuming that the change of fluorescence intensity can be attributed to conformational change in the actin molecule induced by S1 binding, the intra-monomer distance was reduced by 0.4 nm and the inter-monomer distance was increased by 0.2 nm.     

Fluorescence energy transfer between points in G-actin: the nucleotide-binding site, the metal-binding site and Cys-373 residue

Fluorescence energy transfers were studied in order to investigate the spatial relationships between the nucleotide-binding site, the metal-binding site and the Cys-373 residue in the G-actin molecule. When 1-N6-ethenoadenosine-5'-triphosphate (epsilon-ATP) in the nucleotide-binding site and Co2+ or Ni2+ in the metal-binding site were used as fluorescence donor and acceptor, respectively, the fluorescence intensity of epsilon-ATP was perfectly quenched by Ni2+ or Co2+. This indicated that the nucleotide-binding site is very close to the metal-binding site; the distance should be less than 10 A. When N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine (IAEDANS) bound to Cys-373 residue and Co2+ in the metal-binding site were used as a fluorescence donor and an acceptor, respectively, the transfer efficiency was equal to 5 +/- 1%. The corresponding distance was calculated to be 23-32 A, assuming a random orientation factor K2 = 2/3.     

Localization of site-specific probes on the Ca-ATPase of sarcoplasmic reticulum using fluorescence energy transfer

Highly reactive sulfhydryls, previously labeled with an iodoacetamide spin label on the Ca-ATPase of sarcoplasmic reticulum, were labeled with the fluorescent probe, 5-(2-[iodoacetyl)amino)ethyl)aminonaphthalene-1-sulfonic acid (IAEDANS), without loss of enzymatic activity. We have selectively measured the apparent distance of the more reactive site, relative to other site-specific probes at both the nucleotide and the high affinity calcium binding sites. Fluorescence energy transfer efficiencies from the donor IAEDANS to two acceptors: fluorescein 5'-isothiocyanate or 2',3'-O-(2,4,3-trinitrophenyl)adenosine monophosphate, situated at or near the nucleotide site, were measured using fluorescence lifetimes and yields. Fluorescence on polyacrylamide gels shows that the IAEDANS and fluorescein 5'-isothiocyanate labels are both associated with the B tryptic fragment. The energy transfer measurements are consistent with distances of 56 and 68 A between IAEDANS and these respective binding sites. On the other hand, energy transfer measurements using the lanthanide, praseodymium (Pr3+), as an acceptor indicate that IAEDANS is located 16-18 A from the binding site(s) of this calcium analog. Pr3+ is shown to be a good analog for calcium binding to the high affinity sites on the enzyme since it competitively displaces calcium, as evidenced by the reversal of the specific calcium-dependent intrinsic fluorescent signal and inactivation of ATPase activity, over the same narrow range in Pr3+ concentration where energy transfer is observed. Our observations suggest that the portion of the B fragment spanning the cytoplasmic portion of the ATPase is folded onto the A fragment, bringing the IAEDANS label in close proximity to the high affinity calcium binding domain.     

Phospholamban binds in a compact and ordered conformation to the Ca-ATPase

Mutagenesis and cross-linking measurements have identified specific contact interactions between the cytosolic and the transmembrane sequences of phospholamban (PLB) and the Ca-ATPase, and in conjunction with the high-resolution structures of PLB and the Ca-ATPase, have been used to construct models of the PLB-ATPase complex, which suggest that PLB adopts a more extended structure within this complex. To directly test these predictions, we have used fluorescence resonance energy transfer to measure the average conformation and heterogeneity between chromophores covalently bound to the transmembrane and cytosolic domains of PLB reconstituted in proteoliposomes. In the absence of the Ca-ATPase, the cytosolic domain of PLB assumes a wide range of structures relative to the transmembrane sequence, which can be described using a model involving a Gaussian distribution of distances with an average distance (Rav) of less than 21 A and a half-width (HW) of 36 A. This conformational heterogeneity of PLB is consistent with the 10 structures resolved by NMR for the C41F mutant of PLB in organic cosolvents. In contrast, PLB bound to the Ca-ATPase assumes a unique and highly ordered conformation, where Rav = 14.0 +/- 0.3 A and HW = 3.7 +/- 0.6 A. The small spatial separation between the bound chromophores on PLB is inconsistent with an extended conformation of bound PLB in current models. Thus, to satisfy known interaction sites of PLB and the Ca-ATPase, these findings suggest a reorientation of the nucleotide binding domain of the Ca-ATPase toward the bilayer surface to bring known PLB binding sites into close juxtaposition with residues near the amino-terminus of PLB. Induction of an altered conformation of the nucleotide binding domain of the Ca-ATPase by PLB binding is suggested to underlie the reduced calcium sensitivity associated with PLB inhibition of the pump.     

Interaction of myosin LYS-553 with the C-terminus and DNase I-binding loop of actin examined by fluorescence resonance energy transfer

Fluorescence resonance energy transfer (FRET) experiments were carried out in the absence of nucleotide (rigor) or in the presence of MgADP between fluorescent donor probes (IAEDANS (5((((2-iodoacetyl)amino)ethyl)amino)-naphthalene-1-sulfonic acid) at Cys-374 or DANSYL (5-dimethylamino naphthalene-1-(N-(5-aminopentyl))sulfonamide) at Gln-41 of actin and acceptor molecules (FHS (6-[fluorescein-5(and 6)-carboxamido] hexanoic acid succinimidyl ester) at Lys-553 of skeletal muscle myosin subfragment 1. The critical F?rster distance (R(0)) was determined to be 44 and 38 A for the IAEDANS-FHS and DANSYL-FHS donor-acceptor pairs, respectively. The efficiency of energy transfer between the acceptor molecules at Lys-553 of myosin and donor probes at Cys-374 or Gln-41 of actin was calculated to be 0.78 +/- 0.01 or 0.94 +/- 0.01, respectively, corresponding to distances of 35.6 +/- 0.4 A and 24.0 +/- 1.6 A, respectively. MgADP had no significant effect on the distances observed in rigor. Thus, rearrangements in the acto-myosin interface are likely to occur elsewhere than in the lower 50-kDa subdomain of myosin as its affinity for actin is weakened by MgADP binding.     

Fluorescence measurements of immune complexes of Mab 4-4-20 with isomeric haptens.

Relative differences in the active site environment of a monoclonal antibody when covalently bound to two isomeric haptens were studied using fluorescence quenching and lifetime measurements. Murine monoclonal antibody 4-4-20, a well-characterized high affinity antifluorescein antibody, served as the model IgG protein. Isomeric haptenic probes comparatively studied were fluorescein-5-isothiocyanate (FITC I, the immunogen) and fluorescein-6-isothiocyanate (FITC II). In kinetic binding studies, the association rate for the interaction of 4-4-20 with FITC I was greater than 2,000 times faster than the reaction with FITC II. Fluorescence lifetimes for FITC I covalently bound to 4-4-20 were 3.89 ns and 0.37 ns, indicative of hapten bound outside and inside the active site, respectively. Fluorescence lifetime for FITC II within the active site was indistinguishable from bound FITC I, indicating that interactions with active site residues which resulted in a decreased lifetime were similar for both isomers. A decreased lifetime for active site bound FITC I was consistent with the 90-95% quenching of fluorescein fluorescence. Dynamic fluorescence quenching experiments with iodide and FITC I in the active site showed no solvent accessibility, whereas bound FITC II showed significant accessibility. These results suggest that the difference in bond angle which accompanies binding of isomer II relative to isomer I within the active site probably leads to steric constraints resulting in a more open configuration of the 4-4-20 active site.     

Fluorescence resonance energy transfer between the nucleotide binding site and Cys-10 in G-actin and F-actin

Intramonomer fluorescence resonance energy transfer between the donor epsilon-ATP bound to the nucleotide site and the acceptor N-(4-dimethylamino-3,5-dinitrophenyl)maleimide (DDPM) or 4-dimethylaminophenyl-azophenyl-4'-maleimide bound to Cys-10 in G-actin was measured. The donor-acceptor distance was calculated to be about 40 A. The intermonomer energy transfer in F-actin occurring between epsilon-ADP and DABMI was also measured. The radial coordinate of Cys-10 was calculated to be 25 A based on the helical symmetry of F-actin and the recently calculated radial coordinate of the nucleotide binding site in F-actin i.e. 25 A (Miki, M., Hambly, B. and dos Remedios, C.G. (1986) Biochim. Biophys. Acta 871, 137-141). (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) Corresponding distances separating the donor nucleotide in one monomer from acceptors on Cys-10 in the first and second nearest neighbours in F-actin are 39-40 A and 41-43 A.     

Fluorescence studies of the interaction of DNA with Hoechst 33258

Absorption and fluorescence measurements of DNA-Hoechst 33258 complexes at high molar ratio of DNA phosphate to dye are consistent with the existence of two types of bound species. One type (Type I) predominates at high ionic strength, whereas the other (Type II) occurs at low ionic strength. The fluorescence peak (lambda fmax) depends on the excitation wavelength (lambda ex); lambda fmax shifts toward longer wavelength with increasing lambda ex. Optical properties obtained are summarized in the following: for Type I, lambda amax (absorption) = 352 nm, lambda fmax at lambda ex of 335 nm = 460 nm, tau (fluorescence lifetime) = 2.0-2.5 ns; for Type II, lambda amax = 360 nm, lambda fmax at lambda ex of 335 nm = 470 nm, tau = 4.0-5.0 ns. This behavior is interpreted in terms of solvent-solute relaxation. Type I corresponds to less hydrated bound species, while Type II to more hydrated bound species.     

Determination of rotational correlation times from deconvoluted fluorescence anisotropy decay curves. Demonstration with 6,7-dimethyl-8-ribityllumazine and lumazine protein from Photobacterium leiognathi as fluorescent indicators

The experimental and analytical protocols required for obtaining rotational correlation times of biological macromolecules from fluorescence anisotropy decay measurements are described. As an example, the lumazine protein from Photobacterium leiognathi was used. This stable protein (Mr 21 200) contains the noncovalently bound, natural fluorescent marker 6,7-dimethyl-8-ribityllumazine, which has in the bound state a long fluorescence lifetime (tau = 14 ns). Shortening of the fluorescence lifetime to 2.6 ns at room temperature was achieved by addition of the collisional fluorescence quencher potassium iodide. The shortening of tau had virtually no effect on the rotational correlation time of the lumazine protein (phi = 9.4 ns, 19 degrees C). The ability to measure biexponential anisotropy decay was tested by the addition of Photobacterium luciferase (Mr 80 000), which forms an equilibrium complex with lumazine protein. Under the experimental conditions used (2 degrees C) the biexponential anisotropy decay can best be described with correlation times of 20 and 60 ns, representing the uncomplexed and luciferase-associated lumazine proteins, respectively. The unbound 6,7-dimethyl-8-ribityllumazine itself (tau = 9 ns) was used as a model compound for determining correlation times in the picosecond time range. In the latter case rigorous deconvolution from the excitation profile was required to recover the correlation time, which was shorter (100-200 ps) than the measured laser excitation pulse width (500 ps).     

Fluorescence anisotropy studies of molecularly imprinted polymers.

A molecularly imprinted polymer (MIP) is a biomimetic material that can be used as a biochemical sensing element. We studied the steady-state and time-resolved fluorescence and fluorescence anisotropy of anthracene-imprinted polyurethane. We compared MIPs with imprinted analytes present, MIPs with the imprinted analytes extracted, MIPs with rebound analytes, non-imprinted control polymers (non-MIPs) and non-MIPs bound with analytes to understand MIP's binding behaviour. MIPs and non-MIPs had similar steady-state fluorescence anisotropy in the range 0.11-0.24. Anthracene rebound in MIPs and non-MIPs had a fluorescence lifetime of tau = 0.64 ns and a rotational correlation time of phi(F) = 1.2-1.5 ns, both of which were shorter than that of MIPs with imprinted analytes present (tau = 2.03 ns and phi(F) = 2.7 ns). The steady-state anisotropy of polymer solutions increased exponentially with polymerization time and might be used to characterize the polymerization extent in situ.     

The recovery of the polymerizability of Lys-61-labelled actin by the addition of phalloidin. Fluorescence polarization and resonance-energy-transfer measurements

Modification of Lys-61 in actin with fluorescein-5-isothiocyanate (FITC) blocks actin polymerization [Burtnick, L. D. (1984) Biochim. Biophys. Acta 791, 57-62]. FITC-labelled actin recovered its ability to polymerize on addition of phalloidin. The polymers had the same characteristic helical thread-like structure as normal F-actin and the addition of myosin subfragment-1 to the polymers formed the characteristic arrowhead structure in electron microscopy. The polymers activated the ATPase activity of myosin subfragment-1 as efficiently as normal F-actin. These results indicate that Lys-61 is not directly involved in an actin-actin binding region nor in myosin binding site. From static fluorescence polarization measurements, the rotational relaxation time of FITC-labelled actin filaments was calculated to be 20 ns as the value reduced in water at 20 degrees C, while any rotational relaxation time of 1,5-IAEDANS bound to Cys-374 on F-actin in the presence of a twofold molar excess of phalloidin could not be detected by static polarization measurements under the same conditions. This indicates that the Lys-61 side chain is extremely mobile even in the filamentous structure. Fluorescence resonance energy transfer between the donor 1,5-IAEDANS bound to SH1 of myosin subfragment-1 and the acceptor fluorescein-5-isothiocyanate bound to Lys-61 of actin in the rigor complex was measured. The transfer efficiency was 0.39 +/- 0.05 which corresponds to the distance of 5.2 +/- 0.1 nm, assuming that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime and that the transfer occurs between a single donor and an acceptor.     

Mechanism of fluorescence concentration quenching of carboxyfluorescein in liposomes: energy transfer to nonfluorescent dimers

When 5(6)-carboxyfluorescein (6CF) is encapsulated in liposomes at 0.2 M, 97-98% of the fluorescence is quenched. We have studied the mechanism of this effect. The dye-liposome system is a special case of concentration quenching of dyes, a phenomenon recognized for 100 years. Absorption spectra of encapsulated dye show that 6CF dimerizes, and the dimer is nonfluorescent. The dimerization constant was estimated, and it was concluded that dimerization can account for only part of the quenching. In 6CF solutions, the fluorescence lifetime decreased drastically as concentration was changed over the narrow range 0.02-0.05 M, a finding which was attributed to energy transfer to dimers. Inhibition of dimerization by propylene glycol also inhibited the shortening of lifetime. F?rster critical transfer distances were calculated to be 51 and 57 A for monomer-monomer and monomer-dimer transfer, respectively. Monomer-monomer transfer was demonstrated directly by steady-state or time-resolved anisotropy experiments, while transfer to dimer was modeled by using sulforhodamine B, which has a critical transfer distance like that for the dimer and also quenches 6CF emission. No direct evidence for collisional self-quenching of 6CF could be found, although a model compound, salicylate, did quench weakly. For xanthene dyes, the rate of energy transfer is much faster than that for quenching collisions, implying that collisional quenching in the usual 6CF-liposome system is insignificant. The reason why 6CF is not 100% quenched in liposomes is attributed to dye interaction with lipid as evidenced by (i) multiexponential decay of 6CF in liposomes with a long component of 3-4 ns, (ii) inhibition of dimerization in liposomes, (iii) partial protection of dye from quenching by KI, (iv) differing amounts of dimerization in liposomes made from different kinds of phospholipid, and (v) enhancement of fluorescence lifetime in the presence of Triton X-100.     

Effect of proteins on fluorophore lifetime heterogeneity in lipid bilayers.

The effect of three different membrane proteins on the fluorescence lifetime heterogeneity of 1,6-diphenyl-1,3,5-hexatriene (DPH) in phospholipid vesicle systems was investigated. For large unilamellar vesicles of dimyristoylphosphatidylcholine (DMPC) and 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) at 37 degrees C, the fluorescence decay was essentially monoexponential (8.6 and 8.2 ns, respectively) except for a minor component typical of DPH. For gramicidin D reconstituted into DMPC vesicles at a protein/lipid molar ratio of 1/7, the most appropriate analysis of the data was found to be in the form of a bimodal Lorentzian distribution. Centers of the major lifetime components were almost identical with those recovered for vesicles without proteins, while broad distributional widths of some 4.0 ns were recovered. Variation of the protein/lipid molar ratio in sonicated POPC vesicles revealed an abrupt increase in distributional width at ratios approximating 1/15-1/20, which leveled off at about 2.5 ns. For bacteriorhodopsin in DMPC vesicles and cytochrome b5 in POPC, the most appropriate analysis of the data was again found to be in the form of a bimodal Lorentzian also with broad distributional widths in the major component. Lifetime centers were decreased for these proteins due to fluorescence energy transfer to the retinal of the bacteriorhodopsin and heme of the cytochrome b5. Fluorescence energy transfer is distance dependent, and since a range of donor-acceptor distances would be expected in a membrane, lifetime distributions should therefore be recovered independently of other effects for proteins possessing acceptor chromophores.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural studies on bacterial luciferase using energy transfer and emission anisotropy.

The distance between specific sites on bacterial luciferase was estimated by energy transfer. Luciferase was fluorescently labeled by reaction of an essential sulfhydryl group with N-(1-pyrene)maleimide and N-[p-(2-benzoxazolyl)phenyl]meleimide. Both of the modified enzymes bind 8-anilino-1-naphthalenesulfonate (Ans) with affinities similar to that exhibited by the native luciferase. Using each of the two fluorescent probes as a donor and the bound Ans as an acceptor, the energy transfer efficiencies were determined by the resulting enhancement of fluorescence of the acceptor. The corresponding distance was calculated to be in the range of 21 to 37 A. Energy-transfer studies were also carried out using fluorescence lifetime measurements of bound ANS, acting as a donor with bound FMN as an acceptor. The corresponding distance was calculated to be between 30 and 58 A. Using samples of luciferase:Ans complex and luciferase modified with N-(1-pyrene)maleimide, the rotational correlation time of the enzyme-dye conjugate as awhole was found to be 47 +/- 2 ns. The observed rotational correlation time is much longer than that calculated for luciferase assuming a spherical structure, thus indicating an elongated form for the luciferase-dye conjugate.     

Characterization of the ethenoadenosine diphosphate binding site of myosin subfragment 1. Energetics of the equilibrium between two states of nucleotide.S1 and vanadate-induced global conformation changes detected by energy transfer

The fluorescence decay of 1,N6-ethenoadenosine diphosphate (epsilon ADP) bound to myosin subfragment 1 (S1) was studied as a function of temperature. The decay was biexponential, and the two lifetimes were quenched relative to the single lifetime of free epsilon ADP. The temperature dependence of the fractional intensities of the decay components showed two states of the S1.epsilon ADP complex. At pH 7.5 in 30 mM TES, 60 mM KCl, and 3 mM MgCl2, the equilibrium constant for the conversion of the low-temperature state (S1L.epsilon ADP) to the high-temperature state (S1H.epsilon ADP) was 40 at physiological temperatures, and delta H degrees = 13 kcal.mol-1 and delta S degrees = 49 cal.deg-1.mol-1. At 10 degrees C the equilibrium constant of S1 for epsilon ADP was 5, indicating that S1H.epsilon ADP was the dominant state, and that for the vanadate complex epsilon ADP.Vi was 0.7, suggesting that in S1.epsilon ADP.Vi the dominant state of the S1-nucleotide complex was converted from S1H.epsilon ADP to S1L.epsilon ADP. The single rotational correlation time of bound epsilon ADP at 10 degrees C decreased from 107 ns in S1.epsilon ADP to 74 ns in S1+.epsilon ADP.Vi. Conversion of the binary complex to the ternary vanadate complex resulted in a 3-A decrease in the energy transfer distance between bound epsilon ADP and N-[4-(dimethylamino)-3,5-dinitrophenyl]maleimide attached to SH1 and a decrease of the average distance between bound epsilon ADP and bound Co2+ from 12.6 to 8.3 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Time-resolved fluorescence spectroscopy of human adenosine deaminase: effects of enzyme inhibitors on protein conformation

Adenosine deaminase, a purine salvage enzyme essential for immune competence, was studied by time-resolved fluorescence spectroscopy. The heterogeneous emission from this four-tryptophan protein was separated into three lifetime components: tau 1 = 1 ns and tau 2 = 2.2 ns an emission maximum at about 330 nm and tau 3 = 6.3 ns with emission maximum at about 340 nm. Solvent accessibility of the tryptophan emission was probed with polar and nonpolar fluorescence quenchers. Acrylamide, iodide, and trichloroethanol quenched emission from all three components. Acrylamide quenching caused a blue shift in the decay-associated spectrum of component 3. The ground-state analogue enzyme inhibitor purine riboside quenched emission associated with component 2 whereas the transition-state analogue inhibitor deoxycoformycin quenched emission from both components 2 and 3. The quenching due to inhibitor binding had no effect on the lifetimes or emission maxima of the decay-associated spectra. These observations can be explained by a simple model of four tryptophan environments. Quenching studies of the enzyme-inhibitor complexes indicate that adenosine deaminase undergoes different protein conformation changes upon binding of ground- and transition-state analogue inhibitors. The results are consistent with localized structural alterations in the enzyme.