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Phytochromes are biological red/far-red light sensors found in many organisms. Prototypical phytochromes, including Cph1 from the cyanobacterium Synechocystis 6803, act as photochemical switches that interconvert between stable red (Pr)- and metastable far-red (Pfr)-absorbing states induced by photoisomerization of the bilin chromophore. The connection between photoconversion and the cellular output signal involves light-mediated global structural changes in the interaction between the photosensory module (PAS-GAF-PHY) and the C-terminal transmitter (output) module, usually a histidine kinase, as in the case of Cph1. The chromophore deprotonates transiently during the Pr → Pfr photoconversion in association with extensive global structural changes required for signal transmission. Here, we performed equilibrium studies in the Pr state, involving pH titration of the linear tetrapyrrole chromophore in different Cph1 constructs, and measurement of pH-dependent structural changes at various positions in the protein using picosecond time-resolved fluorescence anisotropy. The fluorescent reporter group was attached at positions 371 (PHY domain), 305 (GAF domain), and 120 (PAS domain), as well as at sites in the PAS-GAF bidomain. We show direct correlation of chromophore deprotonation with pH-dependent conformational changes in the various domains. Our results suggest that chromophore deprotonation is closely associated with a higher protein mobility (conformational space) both in proximal and in distal protein sites, implying a causal relationship that might be important for the global large protein arrangements and thus intramolecular signal transduction.

Biological membrane fluidity and thus the local viscosity in lipid membranes are of vital importance for many life processes and implicated in various diseases. Here, we introduce a novel viscosity sensor design for lipid membranes based on a reporting nanoparticle, a sulfated dendritic polyglycerol (dPGS), conjugated to a fluorescent molecular rotor, indocarbocyanine (ICC). We show that dPGS-ICC provides high affinity to lipid bilayers, enabling viscosity sensing in the lipid tail region. The systematic characterization of viscosity- and temperature-dependent photoisomerization properties of ICC and dPGS-ICC allowed us to determine membrane viscosities in different model systems and in living cells using fluorescence lifetime imaging (FLIM). dPGS-ICC distinguishes between ordered lipids and the onset of membrane defects in small unilamellar single lipid vesicles and is highly sensitive in the fluid phase to small changes in viscosity introduced by cholesterol. In microscopy-based viscosity measurements of large multilamellar vesicles, we observed an order of magnitude more viscous environments by dPGS-ICC, lending support to the hypothesis of heterogeneous nanoviscosity environments even in single lipid bilayers. The existence of such complex viscosity structures could explain the large variation in the apparent membrane viscosity values found in the literature, depending on technique and probe, both for model membranes and live cells. In HeLa cells, a tumor-derived cell line, our nanoparticle-based viscosity sensor detects a membrane viscosity of ∼190 cP and is able to discriminate between cell membrane and intracellular vesicle localization. Thus, our results show the versatility of the dPGS-ICC nano-conjugate in physicochemical and biomedical applications by adding a new analytical functionality to its medical properties.

Phytochromes are biological red/far-red light sensors found in many organisms. Photoisomerization of the linear methine-bridged tetrapyrrole triggers transient proton translocation events in the chromophore binding pocket (CBP) leading to major conformational changes of the protein matrix that are in turn associated with signaling. By combining pH-dependent resonance Raman and UV-visible absorption spectroscopy, we analyzed protonation-dependent equilibria in the CBP of Cph1 involving the proposed Pr-I and Pr-II substates that prevail below and above pH 7.5, respectively. The protonation pattern and vibrational properties of these states were further characterized by means of hybrid quantum mechanics/molecular mechanics calculations. From this combined experimental-theoretical study, we were able to identify His260 as the key residue controlling pH-dependent equilibria. This residue is not only responsible for the conformational heterogeneity of CBP in the Pr state of prokaryotic phytochromes, discussed extensively in the past, but it constitutes the sink and source of protons in the proton release/uptake mechanism involving the tetrapyrrole chromophore which finally leads to the formation of the Pfr state. Thus, this work provides valuable information that may guide further experiments toward the understanding of the specific role of protons in controlling structure and function of phytochromes in general.

Hyaluronic acid (HA) hydrogels are interesting delivery systems for topical applications. Besides moisturizing the skin and improving wound healing, HA facilitates topical drug absorption and is highly compatible with labile biomacromolecules. Hence, in this study we investigated the influence of HA hydrogels with different molecular weights (5 kDa, 100 kDa, 1 MDa) on the skin absorption of the model protein bovine serum albumin (BSA) using fluorescence lifetime imaging microscopy (FLIM). To elucidate the interactions of HA with the stratum corneum and the skin absorption of HA itself, we combined FLIM and Fourier-transform infrared (FTIR) spectroscopy. Our results revealed distinct formulation and skin-dependent effects. In barrier deficient (tape-stripped) skin, BSA alone penetrated into dermal layers. When BSA and HA were applied together, however, penetration was restricted to the epidermis. In normal skin, penetration enhancement of BSA into the epidermis was observed when applying low molecular weight HA (5 kDa). Fluorescence resonance energy transfer analysis indicated close interactions between HA and BSA under these conditions. FTIR spectroscopic analysis of HA interactions with stratum corneum constituents showed an α-helix to β-sheet interconversion of keratin in the stratum corneum, increased skin hydration, and intense interactions between 100 kDa HA and the skin lipids resulting in a more disordered arrangement of the latter. In conclusion, HA hydrogels restricted the delivery of biomacromolecules to the stratum corneum and viable epidermis in barrier deficient skin, and therefore seem to be potential topical drug vehicles. In contrast, HA acted as an enhancer for delivery in normal skin, probably mediated by a combination of cotransport, increased skin hydration, and modifications of the stratum corneum properties.

The molecular dynamics of polymeric nanocarriers is an important parameter for controlling the interaction of nanocarrier branches with cargo. Understanding the interplay of dendritic polymer dynamics, temperature, and cargo molecule interactions should provide valuable new insight for tailoring the dendritic architecture to specific needs in nanomedicine, drug, dye, and gene delivery. Here, we have investigated polyglycerol-based core-multishell (CMS) nanotransporters with incorporated Nile Red as a fluorescent drug mimetic and CMS nanotransporters with a covalently bound fluorophore (Indocarbocyanine) using fluorescence spectroscopy methods. From time-resolved fluorescence depolarization we have obtained the rotational diffusion dynamics of the incorporated dye, the nanocarrier, and its branches as a function of temperature. UV/vis and fluorescence lifetime measurements provided additional information on the local dye environment. Our results show a distribution of the cargo Nile Red within the nanotransporter shells that depends on solvent and temperature. In particular, we show that the flexibility of the polymer branches in the unimolecular state of the nanotransporter undergoes a temperature-dependent transition which correlates with a larger space for the mobility of the incorporated hydrophobic drug mimetic Nile Red and a higher probability of cargo-solvent interactions at temperatures above 31 °C. The measurements have further revealed that a loss of the cargo molecule Nile Red occurred neither upon dilution of the CMS nanotransporters nor upon heating. Thus, the unimolecular preloaded CMS nanotransporters retain their cargo and are capable to transport and respond to temperature, thereby fulfilling important requirements for biomedical applications.

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.

Little is known about the molecular nature of residual structure in unfolded states of membrane proteins. A screen of chemical denaturants to maximally unfold the mammalian membrane protein and prototypic G protein coupled receptor rhodopsin, without interference from aggregation, described in an accompanying paper (DOI 10.1021/bi100338e ), identified sodium dodecyl sulfate (SDS), alone or in combination with other chemicals, as the most suitable denaturant. Here, we initiate the biophysical characterization of SDS-denatured states of rhodopsin. Using absorption, steady-state and time-resolved fluorescence spectroscopy, dynamic light scattering, and cysteine accessibility studies, tertiary structure of denatured states was characterized. In agreement with the pattern of secondary structure changes detected by circular dichroism described in the accompanying paper (DOI 10.1021/bi100338e ), tertiary structure changes are distinct over four SDS concentration ranges based on the expected predominant micellar structures. Dodecyl maltoside (DM)/SDS mixed micelle spheres (0.05-0.3% SDS) turn into SDS spheres (0.3-3% SDS) that gradually (3-15% SDS) become cylindrical (above 15% SDS). Denatured states in SDS spheres and cylinders show a relatively greater burial of cysteine and tryptophan residues and are more compact as compared to the states observed in mixed micellar structures. Protein structural changes at the membrane/water interface region are most prominent at very low SDS concentrations but reach transient stability in the compact conformations in SDS spheres. This is the first experimental evidence for the formation of a compact unfolding intermediate state with flexible surface elements in a membrane protein.

Little is known about the general folding mechanisms of helical membrane proteins. Unfolded, i.e., non-native states, in particular, have not yet been characterized in detail. Here, we establish conditions under which denatured states of the mammalian membrane protein rhodopsin, a prototypic G protein coupled receptor with primary function in vision, can be studied. We investigated the effects of the chemical denaturants sodium dodecyl sulfate (SDS), urea, guanidine hydrochloride (GuHCl), and trifluoroacetic acid (TFA) on rhodopsin's secondary structure and propensity for aggregation. Ellipticity at 222 nm decreases in the presence of maximum concentrations of denaturants in the order TFA > GuHCl > urea > SDS + urea > SDS. Interpretation of these changes in ellipticity in terms of helix loss is challenged because the addition of some denaturants leads to aggregation. Through a combination of SDS-PAGE, dependence of ellipticity on protein concentration, and 1D (1)H NMR we show that aggregates form in the presence of GuHCl, TFA, and urea but not in any concentration of SDS, added over a range of 0.05%-30%. Mixed denaturant conditions consisting of 3% SDS and 8 M urea, added in this order, also did not result in aggregation. We conclude that SDS is able to prevent the exposure of large hydrophobic regions present in membrane proteins which otherwise leads to aggregation. Thus, 30% SDS and 3% SDS + 8 M urea are the denaturing conditions of choice to study maximally unfolded rhodopsin without aggregation.

Heterotrimeric G-proteins interact with their G-protein-coupled receptors (GPCRs) via key binding elements comprising the receptor-specific C-terminal segment of the alpha-subunit and the lipid anchors at the alpha-subunit N-terminus and the gamma-subunit C-terminus. Direct information about diffusion and interaction of GPCRs and their G-proteins is mandatory for an understanding of the signal transduction mechanism. By using single-particle tracking, we show that the encounters of the alpha-subunit C-terminus with the GPCR rhodopsin change after receptor activation. Slow as well as less restricted diffusion compared to the inactive state within domains 60-280 nm in length was found for the receptor-bound C-terminus, indicating short-range order in rhodopsin packing.

Bovine rhodopsin was specifically labeled on the cytoplasmic surface at cysteine 140 (the first residue of the loop connecting helices III and IV) or at cysteine 316 (in the loop connecting helix VII and the palmitoylation sites) with the fluorescent labels fluorescein and Texas Red. These loops are involved in activation and signal transduction. The time-resolved fluorescence depolarization was measured in the dark state and in the M(II) state, with labeled samples consisting of rhodopsin-octylglucoside micelles or rod outer segment (ROS) membranes. In this way the diffusional dynamics of the flexible loops of rhodopsin were measured for the first time directly on the nanosecond time scale. Control experiments showed that the large number of weak excitation pulses required in these single photon counting experiments leads to <5% bleaching of the sample. Rhodopsin was trapped in the activated M(II) state for the duration of the fluorescence experiments ( approximately 20 min) after illumination at pH 6 and 5 degrees C. For both types of samples and at both labeled positions the dynamics of the label and loop motion as monitored by the time constants of the depolarization were not significantly different in the two states of the receptor. The end-anisotropy increased, however, from 0.09 in the dark to 0.16 in the M(II) state for ROS samples labeled at C140. The corresponding numbers for the C316 position are 0.06 and 0.12. Light-induced activation in M(II) is thus associated with a large increase in the loop steric hindrance due to a changed loop domain structure on the cytoplasmic surface. These results are supported by fluorescence quenching experiments with I(-), which indicate a significant decrease in the collisional quenching constant k(q) and in accessibility in the M(II) state at both positions. The rotational correlation time of the rhodopsin micelles increased from 48 ns in the dark state to 60 ns in M(II). This increase is caused by a change in volume and/or shape and is consistent with a structural change. These results demonstrate that time-resolved fluorescence depolarization is a powerful tool to study the changes in conformation and dynamics of the cytoplasmic loops that accompany the activation of rhodopsin and other G-protein coupled receptors.

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.

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.

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)

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)

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)