A simulation-guided fluorescence correlation spectroscopy tool to investigate the protonation dynamics of cytochrome c oxidase.

Fluorescence correlation spectroscopy (FCS) is a single molecule based technique to temporally resolve rate-dependent processes by correlating the fluorescence fluctuations of individual molecules traversing through a confocal volume. In addition, chemical processes like protonation or intersystem crossing can be monitored in the sub-microsecond range. FCS thereby provides an excellent tool for investigations of protonation dynamics in proton pumps like cytochrome c oxidase (CcO). To achieve this, the pH-dependent fluorescent dye fluorescein was attached as a protonation probe to the CcO surface via site-specific labeling of single reactive cysteines that are located close to the entry point of a proton input channel (K-pathway). The analysis of protonation dynamics is complicated by overlapping triplet and protonation rates of the fluorophore. A Monte Carlo simulation based algorithm was developed to facilitate discrimination of these temporally overlapping processes thus allowing for improved protonation reaction rate determination. Using this simulation-guided approach we determined precise local proton association and dissociation rates and provide information about protein surface effects, such as proton collecting antennae, on the transport properties of proton transfer channels.

Dual-fluorescence pH probe for bio-labelling.

Although seminaphtorhodafluor (SNARF) dyes are already widely used to measure pH in cells and at biofilms, their synthesis has low yield and results in an unspecific position of a carboxy-group. The separation of 5'- and 6'-carboxy-SNARF reveals a pKa difference of 0.15, calling into question pH measurements with the (commercially available) mixture. Here we replace the bulky external dicarboxyphenyl ring with a propionate group and evaluate the spectral properties of the new derivative. Proceeding to the ethyl-iodoacetamide, covalent linkage to cysteine protein sites is achieved efficiently as shown with a cyanobacterial phytochrome, extending the scarce application of SNARF in bio-labelling in the current literature. Application in fluorescence lifetime imaging is demonstrated both with the lifetime-based and ratiometric-yield method.

Exploiting Fluorescence Lifetime Plasticity in FLIM: Target Molecule Localization in Cells and Tissues.

The mechanisms of drug-receptor interactions and the controlled delivery of drugs via biodegradable and biocompatible nanoparticulate carriers are active research fields in nanomedicine. Many clinically used drugs target G-protein coupled receptors (GPCRs) due to the fact that signaling via GPCRs is crucial in physiological and pathological processes and thus central for the function of biological systems. In this letter, a fast and reliable ratiometric fluorescence lifetime imaging microscopy (rmFLIM) approach is described to analyze the distribution of protein-ligand complexes in the cellular context. Binding of the fluorescently labeled antagonist naloxone to the G-protein coupled µ-opioid receptor is used as an example. To show the broad applicability of the rmFLIM method, we extended this approach to investigate the distribution of polymer-based nanocarriers in histological liver sections.

Elucidation of the nature of the conformational changes of the EF-interhelical loop in bacteriorhodopsin and of the helix VIII on the cytoplasmic surface of bovine rhodopsin: a time-resolved fluorescence depolarization study.

The conformation of the AB-loop and EF-loop of bacteriorhodopsin and of the fourth cytoplasmic loop (helix VIII) of bovine rhodopsin were assessed by a combination of time-resolved fluorescence depolarization and site-directed fluorescence labeling. The fluorescence anisotropy decays were measured employing a tunable Ti:sapphire laser/microchannel plate based single-photon counting apparatus with picosecond time resolution. This method allows measurement of the diffusional dynamics of the loops directly on a nanosecond time-scale. We implemented the method to study model peptides and two-helix systems representing sequences of bacteriorhodopsin. Thus, we systematically analyzed the anisotropic behavior of four different fluorescent dyes covalently bound to a single cysteine residue on the protein surface and assigned the anisotropy decay components to the modes of motion of the protein and its segments. We have identified two mechanisms of loop conformational changes in the functionally intact proteins bacteriorhodopsin and bovine rhodopsin. First, we found a surface potential-dependent transition between two conformational states of the EF-loop of bacteriorhodopsin, detected with the fluorescent dye bound to position 160. A transition between the two conformational states at 150mM KCl and 20 degrees C requires a surface potential change that corresponds to Deltasigma approximately -1.0e(-)/bacteriorhodopsin molecule. We suggest, that the surface potential-based switch of the EF-loop is the missing link between the movement of helix F and the transient surface potential change detected during the photocycle of bacteriorhodopsin. Second, in the visual pigment rhodopsin, with the fluorescent dye bound to position 316, a particularly striking pH-dependent conformational change of the fourth loop on the cytoplasmic surface was analyzed. The loop mobility increased from pH 5 to 8. The midpoint of this transition is at pH 6.2 and correlates with the midpoint of the pH-dependent equilibrium between the active metarhodopsin II and the inactive metarhodopsin I state.

Evidence for a perturbation of arginine-82 in the bacteriorhodopsin photocycle from time-resolved infrared spectra.

Arginine-82 (R82) of bacteriorhodopsin (bR) has long been recognized as an important residue due to its absolute conservation in the archaeal rhodopsins and the effects of R82 mutations on the photocycle and proton release. However, the nature of interactions between R82 and other residues of the protein has remained difficult to decipher. Recent NMR studies showed that the two terminal nitrogens of R82 experience a highly perturbed asymmetric environment during the M state trapped at cryogenic temperatures [Petkova et al. (1999) Biochemistry 38, 1562-1572]. Although previous low-temperature FT-IR spectra of wild-type and mutant bR samples have demonstrated effects of R82 on vibrations of other amino acid side chains, no bands in these spectra were assignable to vibrations of R82 itself. We have now measured time-resolved FT-IR difference spectra of bR intermediates in the wild-type and R82A proteins, as well as in samples of the R82C mutant with and without thioethylguanidinium attached via a disulfide linkage at the unique cysteine site. Several bands in the bR --> M difference spectrum are attributable to guanidino group vibrations of R82, based on their shift upon isotope substitution of the thioethylguanidinium attached to R82C and on their disappearance in the R82A spectrum. The frequencies and intensities of these IR bands support the NMR-based conclusion that there is a significant perturbation of R82 during the bR photocycle. However, the unusually low frequencies attributable to R82 guandino group vibrations in M, approximately 1640 and approximately 1545 cm(-)(1), would require a reexamination of a previously discarded hypothesis, namely, that the perturbation of R82 involves a change in its ionization state.

Evidence for long range allosteric interactions between the extracellular and cytoplasmic parts of bacteriorhodopsin from the mutant R82A and its second site revertant R82A/G231C.

Evidence is presented for long range interactions between the extracellular and cytoplasmic parts of the heptahelical membrane protein bacteriorhodopsin in the mutant R82A and its second site revertant R82A/G231C. (i) In the double mutants R82A/G72C and R82A/A160C, with the cysteine mutation on the extracellular or cytoplasmic surface, respectively, the photocycle is the same as in the single mutant R82A with an accelerated deprotonation of the Schiff base and a reversed order of proton release and uptake. Proton release and uptake kinetics were measured directly at either surface by using the unique cysteine residue as attachment site for the pH indicator fluorescein. Whereas in wild type proton uptake on the cytoplasmic surface occurs during the M-decay (tau approximately 8 ms), in R82A it occurs already during the first phase of the M-rise (tau < 1 microseconds). (ii) The introduction of a second mutation at the cytoplasmic surface in position 231 (helix G) restores wild type ground state absorption properties, kinetics of photocycle and of proton release, and uptake in the mutant R82A/G231C. In addition, kinetic H/D isotope effects provide evidence that the proton release mechanism in R82A/G231C and in wild type is similar. These results suggest the existence of long range interactions between the cytoplasmic and extracellular surface domains of bacteriorhodopsin mediated by salt bridges and hydrogen-bonded networks between helices C (Arg-82) and G (Asp-212 and Gly-231). Such long range interactions are expected to be of functional significance for activation and signal transduction in heptahelical G-protein-coupled receptors.

Structure of the interhelical loops and carboxyl terminus of bacteriorhodopsin by X-ray diffraction using site-directed heavy-atom labeling.

The positions of single amino acids in the interhelical loop regions and the C-terminal tail of bacteriorhodopsin (bR) were investigated by X-ray diffraction using site-directed heavy-atom labeling. Since wild-type bR does not contain any cysteines, appropriate cysteine mutants were produced with a unique sulfhydryl group at specific positions. These sites were then labeled with mercury using the sulfhydryl specific reagent p-chloromercuribenzoate (p-CMB). The cysteine mutants D96A/V101C, V130C, A160C, and G231C were derivatized with labeling stoichiometries of 0.93 +/- 5%, 0.85 +/- 5%, 0.79 +/- 7%, and 0.77 +/- 8%, respectively (Hg per bR). No incorporation was observed with wild-type bR under the same conditions. All mutants and heavy-atom derivatives were fully active as judged by the kinetics of the photocycle and of the proton release and uptake. Moreover, the unit cell dimensions of the two-dimensional P3 lattice were unchanged by the mutations and the derivatization. This allowed the position of the mercury atoms, projected onto the plane of the membrane, to be calculated from the intensity differences in the X-ray diffraction pattern between labeled and unlabeled samples using Fourier difference methods. The X-ray diffraction data were collected at room temperature from oriented purple membrane films at 100% relative humidity without the use of dehydrating solvents. These native conditions of temperature, humidity, and solvent are expected to preserve the structure of the surface-exposed loops. Sharp maxima corresponding to a single mercury atom were found in the difference density maps for D96A/V101C and V130C. Residues 101 and 130 are in the short loops connecting helices C/D and D/E, respectively. No localized difference density was found for A160C and G231C. Residue 160 is in the longer loop connecting helices E and F, whereas residue 231 is in the C-terminal tail. Residues 160 and 231 are apparently in a more disordered and mobile part of the structure.

Proton transport by a bacteriorhodopsin mutant, aspartic acid-85-->asparagine, initiated in the unprotonated Schiff base state.

At alkaline pH the bacteriorhodopsin mutant D85N, with aspartic acid-85 replaced by asparagine, is in a yellow form (lambda max approximately 405 nm) with a deprotonated Schiff base. This state resembles the M intermediate of the wild-type photocycle. We used time-resolved methods to show that this yellow form of D85N, which has an initially unprotonated Schiff base and which lacks the proton acceptor Asp-85, transports protons in the same direction as wild type when excited by 400-nm flashes. Photoexcitation leads in several milliseconds to the formation of blue (630 nm) and purple (580 nm) intermediates with a protonated Schiff base, which decay in tens of seconds to the initial state (400 nm). Experiments with pH indicator dyes show that at pH 7, 8, and 9, proton uptake occurs in about 5-10 ms and precedes the slow release (seconds). Photovoltage measurements reveal that the direction of proton movement is from the cytoplasmic to the extracellular side with major components on the millisecond and second time scales. The slowest electrical component could be observed in the presence of azide, which accelerates the return of the blue intermediate to the initial yellow state. Transport thus occurs in two steps. In the first step (milliseconds), the Schiff base is protonated by proton uptake from the cytoplasmic side, thereby forming the blue state. From the pH dependence of the amplitudes of the electrical and photocycle signals, we conclude that this reaction proceeds in a similar way as in wild type--i.e., via the internal proton donor Asp-96. In the second step (seconds) the Schiff base deprotonates, releasing the proton to the extracellular side.

Time-resolved surface charge change on the cytoplasmic side of bacteriorhodopsin.

The pH-sensitive dye 5-iodoacetamidofluorescein was covalently bound to a single cysteine residue introduced by site-directed mutagenesis in position 101 on the cytoplasmic surface or in position 130 on the extracellular surface of the proton pump bacteriorhodopsin. Using time-resolved absorption spectroscopy at 495 nm a transient increase was observed in the apparent pK of the dye attached at residue 101. At pH 7.3 the rise and decay times of this pK-change (approximately 2 ms and approximately 60 ms) correlate well with decay times observed for the M and O intermediates and with the proton uptake time. Interpreting the pK-increase of +0.18 pH-unit in terms of a transiently more negative surface charge density, we calculate a change of -0.80 elementary charge per bacteriorhodopsin at the cytoplasmic surface. It is likely that this charge change is due to the transient deprotonation of aspartate-96. With the label in position 130 on the extracellular surface no transient pK-shift was detected.

Rapid long-range proton diffusion along the surface of the purple membrane and delayed proton transfer into the bulk.

The pH-indicator dye fluorescein was covalently bound to the surface of the purple membrane at position 72 on the extracellular side of bacteriorhopsin and at positions 101, 105, 160, or 231 on the cytoplasmic side by reacting bromomethylfluorescein with the sulfhydryl groups of cysteines introduced by site-directed mutagenesis. At position 72, on the extracellular surface, the light-induced proton release was detected 71 +/- 4 microseconds after the flash (conditions: pH 7.3, 22 degrees C, and 150 mM KCl). On the cytoplasmic side with the dye at positions 101, 105, and 160, the corresponding values were 77, 76, and 74 +/- 5 microseconds, respectively. Under the same conditions, the proton release time in the bulk medium as detected by pyranine was around 880 microseconds--i.e., slower by a factor of more than 10. The fact that the proton that is released on the extracellular side is detected much faster on the cytoplasmic surface than in the aqueous bulk phase demonstrates that it is retained on the surface and migrates along the purple membrane to the other side. These findings have interesting implications for bioenergetics and support models of local proton coupling. From the small difference between the proton detection times by labels on opposite sides of the membrane, we estimate that at 22 degrees C the proton surface diffusion constant is greater than 3 x 10(-5) cm2/s. At 5 degrees C, the proton release detection time at position 72 equals the faster of the two main rise times of the M intermediate (deprotonation of the Schiff base). At higher temperatures this correlation is gradually lost, but the curved Arrhenius plot for the proton release time is tangential to the linear Arrhenius plot for the rise of M at low temperatures. These observations are compatible with kinetic coupling between Schiff base deprotonation and proton release.

Covalently bound pH-indicator dyes at selected extracellular or cytoplasmic sites in bacteriorhodopsin. 1. Proton migration along the surface of bacteriorhodopsin micelles and its delayed transfer from surface to bulk.

The kinetics of the light-induced release and uptake of protons was monitored with the optical pH-indicator fluorescein covalently bound to various sites on the extracellular and cytoplasmic surfaces of bacteriorhodopsin. Selective labeling was achieved by reacting (iodoacetamido)fluorescein with the single cysteine residues in bacteriorhodopsin introduced at the desired positions by site-directed mutagenesis. All measurements were performed with bacteriorhodopsin micelles in phospholipid/detergent mixtures in 150 mM KCl at 22 degrees C, pH 7.3. Neither the replacements by cysteine nor the subsequent labeling affected the absorption spectrum of bacteriorhodopsin and the rise times of the M intermediate. Only the decay of M was altered for some bacteriorhodopsin mutants with cysteine residues on the cytoplasmic side. The proton release time detected with fluorescein attached to the extracellular surface (the proton release side) at position 72 (in the loop connecting helices B and C) or 130 (DE loop) was 22 +/- 4 microseconds, clearly faster than that measured with pyranine in the aqueous bulk phase (125 +/- 10 microseconds for wild-type and all mutants studied). For bacteriorhodopsin mutants labeled at positions 35, 101, 160, 229, and 231 in the cytoplasmic loop region (the proton uptake side), the released proton was observed with a time of 61 +/- 4 microseconds. This was about 3-fold slower than the release time on the extracellular side, but still significantly faster than that measured with pyranine in the bulk phase. These results suggest that the released protons are retained on the micellar surface and move more rapidly along this surface to the cytoplasmic side than from the surface to the bulk medium.(ABSTRACT TRUNCATED AT 250 WORDS)

Covalently bound pH-indicator dyes at selected extracellular or cytoplasmic sites in bacteriorhodopsin. 2. Rotational orientation of helices D and E and kinetic correlation between M formation and proton release in bacteriorhodopsin micelles.

The kinetics of the light-induced proton release in bacteriorhodopsin/lipid/detergent micelles was monitored with the optical pH-indicator fluorescein bound covalently to positions 127-134 (helices D and E and the DE loop) on the extracellular side of the protein (the proton release side). Single cysteine residues were introduced in these positions by site-directed mutagenesis, and fluorescein was attached to the sulfhydryl group by reaction with (iodoacetamido)fluorescein. Two characteristic proton release times (approximately 20 and 70 microseconds) were observed. The faster time constant was recorded when fluorescein was attached to positions 127, 130, 131, 132, and 134, while the slower time was observed with the indicator bound to positions 128, 129, and 133. The results are rationalized by assuming specific helical wheel orientations for helics D and E and by making a choice for the residues in the DE loop: (i) The fast time constants occur with fluorescein either attached to residues 130, 131, and 132 that form the DE loop or when pointing toward the interior of the protein with its aqueous proton channel [residues 127 (helix D) and 134 (helix E)]. (ii) The slower time constants are detected with fluorescein exposed to the exterior lipid/detergent phase when bound to residues 128, 129 (both helix D), and 133 (helix E). This interpretation is supported by measurements of the polarity of the label environment which indicate for fluorescein in group i a more hydrophilic environment and for group ii a more hydrophobic environment. The fastest proton release time (10 microseconds) was observed with fluorescein bound to position 127.(ABSTRACT TRUNCATED AT 250 WORDS)

Surface charge of bacteriorhodopsin detected with covalently bound pH indicators at selected extracellular and cytoplasmic sites.

We present a method that allows the detection of the surface charge density of bacteriorhodopsin (bR) at any selected protein surface site. The optical pH indicator fluorescein was covalently bound to the sulfhydryl groups of single cysteine residues, which were introduced at selected positions in bR by site-directed mutagenesis. On the extracellular side, the positions were in the BC loop (72) and in the DE loop (129-134). On the cytoplasmic side, one position in each loop was labeled: 35 (AB), 101 (CD), 160 (EF), and 231 (carboxy tail). The apparent pKs of fluorescein in these positions were determined for various salt concentrations. The local surface charge density was calculated from the dependence of the apparent pK of the dye on the ionic strength using the Gouy-Chapman equation. The surface charge density at pH 6.6 is more negative on the cytoplasmic side (averaged over all positions, -2.5 +/- 0.2 elementary charges per bR) than on the extracellular side (average, -1.8 +/- 0.2 elementary charges per bR) with little variation along the surface. Since the experiments were performed with electrically neutral CHAPS/DMPC micelles, these values represent the charge present on bR itself.(ABSTRACT TRUNCATED AT 250 WORDS)

Effect of introducing different carboxylate-containing side chains at position 85 on chromophore formation and proton transport in bacteriorhodopsin.

During the initial stages of the bacteriorhodopsin photocycle, a proton is transferred from the Schiff base to the deprotonated carboxylate of Asp85. Earlier studies have shown that replacement of Asp85 by Asn completely abolishes proton transport activity, whereas extension of the side chain by an additional carbon-carbon bond (Asp85-->Glu) results in a functional proton pump. Here we show that extension of the Asp85 side chain by two additional bond lengths also results in a functional proton pump as long as the terminal group is a carboxylate moiety. These side chains were created by modification of the cysteine residue in the Asp85-->Cys mutant with either iodoacetic acid or iodoacetamide. In vitro chromophore formation studies show that the rate of Schiff base protonation in mutants that contain a carboxylate at residue 85 is invariably faster than in mutants that contain neutral substitutions at this position. We conclude that in bacteriorhodopsin, there is considerable tolerance in the volume of the side chain that can be accommodated at position 85 and that the presence of a carboxylate at residue 85 is important both for proton pumping and for stabilizing the protonated Schiff base.