Metal and substrate binding to an Fe(II) dioxygenase resolved by UV spectroscopy with global regression analysis

The addition of divalent metal ions or substrate taurine to TauD, an α-ketoglutarate-dependent dioxygenase, alters its UV absorption, as clearly observed by monitoring the protein’s difference spectra. Binding of metal ions leads to a decrease in absorption at ∼297 nm and modulation of other features. A separate signature with enhanced absorption at ∼295 nm is identified for binding of taurine. These narrow (∼700 cm⁻¹) and intense (∼0.5 mM⁻¹ cm⁻¹) spectral changes are attributed to ligand-induced protein conformational changes affecting the environment of aromatic residues. The changes in the UV difference spectra were exploited to assess directly the thermodynamics and kinetics of ligand interactions in wild-type TauD and selected variants. This approach holds promise as a new tool to probe ligand-induced conformational changes in a wide range of other proteins. Experimental and quantification approaches for a reliable analysis of protein absorption below 320 nm are presented.     

Kinetic mechanism of the Ca2+-dependent switch-on and switch-off of cardiac troponin in myofibrils

The kinetics of Ca²⁺-dependent conformational changes of human cardiac troponin (cTn) were studied on isolated cTn and within the sarcomeric environment of myofibrils. Human cTnC was selectively labeled on cysteine 84 with N-((2-(iodoacetoxy)ethyl)-N-methyl)amino-7-nitrobenz-2-oxa-1,3-diazole and reconstituted with cTnI and cTnT to the cTn complex, which was incorporated into guinea pig cardiac myofibrils. These exchanged myofibrils, or the isolated cTn, were rapidly mixed in a stopped-flow apparatus with different [Ca²⁺] or the Ca²⁺-buffer 1,2-Bis(2-aminophenoxy)ethane-N,N,N′,N′-tetraacetic acid to determine the kinetics of the switch-on or switch-off, respectively, of cTn. Activation of myofibrils with high [Ca²⁺] (pCa 4.6) induced a biphasic fluorescence increase with rate constants of >2000 s⁻¹ and ∼330 s⁻¹, respectively. At low [Ca²⁺] (pCa 6.6), the slower rate was reduced to ∼25 s⁻¹, but was still ∼50-fold higher than the rate constant of Ca²⁺-induced myofibrillar force development measured in a mechanical setup. Decreasing [Ca²⁺] from pCa 5.0-7.9 induced a fluorescence decay with a rate constant of 39 s⁻¹, which was approximately fivefold faster than force relaxation. Modeling the data indicates two sequentially coupled conformational changes of cTnC in myofibrils: 1), rapid Ca²⁺-binding (k_B ≈ 120 μM⁻¹ s⁻¹) and dissociation (k_D ≈ 550 s⁻¹); and 2), slower switch-on (k_on = 390s⁻¹) and switch-off (k_off = 36s⁻¹) kinetics. At high [Ca²⁺], ∼90% of cTnC is switched on. Both switch-on and switch-off kinetics of incorporated cTn were around fourfold faster than those of isolated cTn. In conclusion, the switch kinetics of cTn are sensitively changed by its structural integration in the sarcomere and directly rate-limit neither cardiac myofibrillar contraction nor relaxation.     

Structure of Self-Aggregated Alamethicin in ePC Membranes Detected by Pulsed Electron-Electron Double Resonance and Electron Spin Echo Envelope Modulation Spectroscopies

PELDOR spectroscopy was exploited to study the self-assembled super-structure of the [Glu(OMe)^7,18,19]alamethicin molecules in vesicular membranes at peptide to lipid molar ratios in the range of 1:70-1:200. The peptide molecules were site-specifically labeled with TOAC electron spins. From the magnetic dipole-dipole interaction between the nitroxides of the monolabeled constituents and the PELDOR decay patterns measured at 77 K, intermolecular-distance distribution functions were obtained and the number of aggregated molecules (n ≈ 4) was estimated. The distance distribution functions exhibit a similar maximum at 2.3 nm. In contrast to Alm16, for Alm1 and Alm8 additional maxima were recorded at 3.2 and ∼5.2 nm. From ESEEM experiments and based on the membrane polarity profiles, the penetration depths of the different spin-labeled positions into the membrane were qualitatively estimated. It was found that the water accessibility of the spin-labels follows the order TOAC-1 > TOAC-8 ≈ TOAC-16. The geometric data obtained are discussed in terms of a penknife molecular model. At least two peptide chains are aligned parallel and eight ester groups of the polar Glu(OMe)^18,19 residues are suggested to stabilize the self-aggregate superstructure.     

Acetylcholine Receptor Channels Activated by a Single Agonist Molecule

The neuromuscular acetylcholine receptor (AChR) is an allosteric protein that alternatively adopts inactive versus active conformations (R↔R^∗). The R^∗ shape has a higher agonist affinity and ionic conductance than R. To understand how agonists trigger this gating isomerization, we examined single-channel currents from adult mouse muscle AChRs that isomerize normally without agonists but have only a single site able to use agonist binding energy to motivate gating. We estimated the monoliganded gating equilibrium constant E₁ and the energy change associated with the R versus R^∗ change in affinity for agonists. AChRs with only one operational binding site gave rise to a single population of currents, indicating that the two transmitter binding sites have approximately the same affinity for the transmitter ACh. The results indicated that E₁ ≈ 4.3 × 10⁻³ with ACh, and ≈1.7 × 10⁻⁴ with the partial-agonist choline. From these values and the diliganded gating equilibrium constants, we estimate that the unliganded AChR gating constant is E₀ ≈ 6.5 × 10⁻⁷. Gating changes the stability of the ligand-protein complex by ∼5.2 kcal/mol for ACh and ∼3.3 kcal/mol for choline.     

Daily milk intake and body water turnover in suckling mink (Mustela vison) kits

Daily (24 h) milk intake and body water turnover were measured in eight litters of suckling mink (Mustela vison) kits (6–9 kits litter⁻¹) during weeks 1–4 post partum using the tritiated water (³HHO) dilution technique. The biological half-life of body water turnover in the mink kits increased linearly from 0.9 days in week 1 (3–5 days post partum) to 1.9 days in week 4 (22–24 days post partum). The daily milk intake varied markedly among the mink kits within a litter and increased significantly with increasing body mass from (mean±SEM) 10.9±0.4 g per kit during week 1 to 27.7±1.0 g per kit during week 4. Throughout the study, male kits were ∼10% heavier and had a significantly higher milk intake than female kits. The results were corrected for water recycling between the dam and her kits, ranging from ∼4 to 15% of the daily milk water intake, and the calculated daily milk yield of the 2 year old lactating mink dams increased from 87±7 g day⁻¹ in week 1 to 190±15 g day⁻¹ in week 4 post partum. The average body growth rate of the mink kits ranged from 2.9 g kit⁻¹ per day in week 1 to 5.4 g kit⁻¹ per day in week 4, and the calculated mean intake of mink milk per unit of body weight gain was remarkably stable at 4.0 (g g⁻¹) during weeks 1–3 post partum, but increased to 5.6 (g g⁻¹) in week 4 post partum. The amount of metabolizable energy supplied to the kits by the daily milk yield of the dam increased from ≈450 to ≈990 kJ day⁻¹, which corresponded well with the calculated daily energy requirements of the kits. The tritiated water dilution technique was found feasible and reliable for repeated measurements of milk intake in suckling mink kits up to 4 weeks of age.     

The Origin of the Low-Energy Form of Photosystem I Light-Harvesting Complex Lhca4: Mixing of the Lowest Exciton with a Charge-Transfer State

The peripheral light-harvesting complex of photosystem I contains red chlorophylls (Chls) that, unlike the typical antenna Chls, absorb at lower energy than the primary electron donor P700. It has been shown that the red-most absorption band arises from two excitonically coupled Chls, although this interaction alone cannot explain the extreme red-shifted emission (25 nm, ∼480 cm⁻¹ for Lhca4 at 4 K) that the red Chls present. Here, we report the electric field-induced absorption changes (Stark effect) on the Q_y region of the Lhca4 complex. Two spectral forms, centered around 690 nm and 710 nm, were necessary to describe the absorption and Stark spectra. The analysis of the lowest energy transition yields a high value for the change in dipole moment, Δμ_710nm ≈ 8 Df⁻¹, between the ground and excited states as compared with monomeric, Δμ = 1 D, or dimeric, Δμ = 5 D, Chl a in solution. The high value of the Δμ demonstrates that the origin of the red-shifted emission is the mixing of the lowest exciton state with a charge-transfer state of the dimer. This energetic configuration, an excited state with charge-transfer character, is very favorable for the trapping and dissipation of excitations and could be involved in the photoprotective mechanism(s) of the photosystem I complex.     

Subdiffraction-limit study of Kaede diffusion and spatial distribution in live Escherichia coli

Photoactivation localization microscopy (PALM) is used to study the spatial distribution and diffusion of single copies of the protein Kaede in the cytoplasm of live Escherichia coli under moderate growth conditions (67 min doubling time). The spatial distribution of Kaede is uniform within the cytoplasm. The cytoplasmic radius of 380 ± 30 nm varies little from cell to cell. Single-particle tracking using 4 ms exposure times reveals negatively curved plots of mean-square displacement versus time. A detailed comparison with Monte Carlo simulations in a spherocylindrical volume shows that the curvature can be quantitatively understood in terms of free diffusion within a confining volume. The mean diffusion coefficient across cells is <D_Kaede> = 7.3 ± 1.1 μm²·s⁻¹, consistent with a homotetrameric form of Kaede. The distribution of squared displacements along the long axis for individual Kaede molecules is consistent with homogeneous diffusion. However, for longer cells, a spatial map of one-step estimates of the diffusion coefficient along x suggests that diffusion is ∼20–40% faster within nucleoids than in the ribosome-rich region lying between nucleoid lobes at the cell mid-plane. Fluorescence recovery after photobleaching yielded <D_FRAP> = 8.3 ± 1.6 μm²·s⁻¹, in agreement with the single-particle tracking results.     

Identification of the Intermediate Charge-Separated State PβL in a Leucine M214 to Histidine Mutant of the Rhodobacter sphaeroides Reaction Center Using Femtosecond Midinfrared Spectroscopy

Energy and electron transfer in a Leu M214 to His (LM214H) mutant of the Rhodobacter sphaeroides reaction center (RC) were investigated by applying time-resolved visible pump/midinfrared probe spectroscopy at room temperature. This mutant replacement of the Leu at position M214 resulted in the incorporation of a bacteriochlorophyll (BChl) in place of the native bacteriopheophytin in the L-branch of cofactors (denoted β_L). Purified LM214H RCs were excited at 600 nm (unselective excitation), at 800 nm (direct excitation of the monomeric BChl cofactors B_L and B_M), and at 860 nm (direct excitation of the primary donor (P) BChl pair (P_L/P_M)). Absorption changes associated with carbonyl (C=O) stretch vibrational modes (9-keto, 10a-ester, and 2a-acetyl) of the cofactors and of the protein were recorded in the region between 1600 cm⁻¹ and 1770 cm⁻¹, and the data were subjected to both a sequential analysis and a simultaneous target analysis. After photoexcitation of the LM214H RC, P^∗ decayed on a timescale of ∼6.3 ps to P⁺B_L⁻. The decay of P⁺B_L⁻ occurred with a lifetime of ∼2 ps, ∼3 times slower than that observed in wild-type and R-26 RCs (∼0.7 ps). Further electron transfer to the β_L BChl resulted in formation of the P⁺β_L⁻ state, and its infrared absorbance difference spectrum is reported for the first time, to our knowledge. The fs midinfrared spectra of P⁺B_L⁻ and P⁺β_L⁻ showed clear differences related to the different environments of the two BChls in the mutant RC.     

Luminostat operation: a tool to maximize microalgae photosynthetic efficiency in photobioreactors during the daily light cycle?

The luminostat regime has been proposed as a way to maximize light absorption and thus to increase the microalgae photosynthetic efficiency within photobioreactors. In this study, simulated outdoor light conditions were applied to a lab-scale photobioreactor in order to evaluate the luminostat control under varying light conditions. The photon flux density leaving the reactor (PFD_out) was varied from 4 to 20 μmol photons m⁻² s⁻¹and the productivity and photosynthetic efficiency of Chlorella sorokiniana were assessed.Maximal volumetric productivity (1.22 g kg⁻¹ d⁻¹) and biomass yield on PAR photons (400-700 nm) absorbed (1.27 g mol⁻¹) were found when PFD_out was maintained between 4 and 6 μmol photons m⁻² s⁻¹. The resultant photosynthetic efficiency was comparable to that already reported in a chemostat-controlled reactor. A strict luminostat regime could not be maintained under varying light conditions. Further modifications to the luminostat control are required before application under outdoor conditions.     

Comparative characterization of aqueous dispersions and cast films of different chitin nanowhiskers/nanofibers

Water dispersions of TEMPO-oxidized α-chitin nanowhisker (TOChN), partially deacetylated α-chitin nanowhisker/nanofiber mixture (DEChN), HCl-hydrolyzed chitin nanowhisker (HHChN) and squid-pen β-chitin nanofiber (SQChN) were prepared, and the properties of nano-dispersions and their cast films were characterized between the four chitin nano-samples. Because SQChN has the highest aspect ratio, its 0.1% dispersion had the highest shear stress and viscosity at the same shear rate in the four chitin nano-samples, and showed gel-like behavior in the whole shear rate range from 10⁻³ to 10³ s⁻¹. AFM images of the self-standing films showed that film surfaces consisted of characteristic chitin nano-elements with different morphologies and degrees of orientation between the four chitin samples, whereas all chitin nanowhisker/nanofiber films had similar thermal degradation points at ∼200 °C. The DEChN film had the highest tensile strength of ∼140 MPa, elongation at break of ∼10% and light-transmittance of 87% at 400 nm. In contrast, the SQChN film had the lowest tensile strength, Young's modulus and light-transmittance. All chitin nanowhisker/nanofiber films had similar oxygen permeabilities of ∼1 mL μm m⁻² day⁻¹ kPa⁻¹, which was clearly lower than that (184 mL μm m⁻² day⁻¹ kPa⁻¹) of a poly(lactic acid) film.     

Low light acclimated submerged freshwater plants show a pronounced sensitivity to increasing irradiances

The high light sensitivity of three submerged aquatic freshwater plant species, Egeria densa, Elodea nuttallii and Myriophyllum heterophyllum, which have been cultivated at a photosynthetically active radiation (PAR, 400-700 nm) of 70 μmol photons m⁻² s⁻¹, was studied by means of chlorophyll fluorescence and pigment analyses. Exposure of plants to 100, 300, 600 and 1000 μmol photons m⁻² s⁻¹ PAR for up to 360 min induced a strong reduction of the F_v/F_m ratio, indicating a pronounced inactivation of PSII even at the lowest PAR applied. These changes were accompanied by a reduction of the chlorophyll content to about 60-70% of control values at the highest PAR. Rapidly inducible photoprotective mechanisms were not affected, as derived from the rapid generation of pH-dependent energy dissipation under these conditions. At PAR higher than 100 μmol photons m⁻² s⁻¹, however, the primary quinone acceptor of photosystem II, Q_A, was reduced to about 80% and the effective quantum yield of photosystem II, Φ_PSII, dropped to values of about 10%, indicating a high reduction state of the photosynthetic electron transport chain. These data support the notion that the three aquatic macrophytes have a very low capacity for the acclimation to higher light intensities.     

Single-Molecule Tracking of Inositol Trisphosphate Receptors Reveals Different Motilities and Distributions

Puffs are local Ca²⁺ signals that arise by Ca²⁺ liberation from the endoplasmic reticulum through the concerted opening of tightly clustered inositol trisphosphate receptors/channels (IP₃Rs). The locations of puff sites observed by Ca²⁺ imaging remain static over several minutes, whereas fluorescence recovery after photobleaching (FRAP) experiments employing overexpression of fluorescently tagged IP₃Rs have shown that the majority of IP₃Rs are freely motile. To address this discrepancy, we applied single-molecule imaging to locate and track type 1 IP₃Rs tagged with a photoswitchable fluorescent protein and expressed in COS-7 cells. We found that ∼70% of the IP₃R1 molecules were freely motile, undergoing random walk motility with an apparent diffusion coefficient of ∼0.095 μm s⁻¹, whereas the remaining molecules were essentially immotile. A fraction of the immotile IP₃Rs were organized in clusters, with dimensions (a few hundred nanometers across) comparable to those previously estimated for the IP₃R clusters underlying functional puff sites. No short-term (seconds) changes in overall motility or in clustering of immotile IP₃Rs were apparent following activation of IP₃/Ca²⁺ signaling. We conclude that stable clusters of small numbers of immotile IP₃Rs may underlie local Ca²⁺ release sites, whereas the more numerous motile IP₃Rs appear to be functionally silent.     

N-labeling to determine chlorophyll synthesis and degradation in Synechocystis sp. PCC 6803 strains lacking one or both photosystems

Rates of chlorophyll synthesis and degradation were analyzed in Synechocystis sp. PCC 6803 wild type and mutants lacking one or both photosystems by labeling cells with (¹⁵NH₄)₂SO₄ and Na¹⁵NO₃. Pigments extracted from cells were separated by HPLC and incorporation of the ¹⁵N label into porphyrins was subsequently examined by MALDI-TOF mass spectrometry. The life time (τ) of chlorophyll in wild-type Synechocystis grown at a light intensity of 100 μmol photons m⁻² s⁻¹ was determined to be about 300 h, much longer than the cell doubling time of about 14 h. Slow chlorophyll degradation (τ ∼200-400 h) was also observed in Photosystem I-less and in Photosystem II-less Synechocystis mutants, whereas in a mutant lacking both Photosystem I and Photosystem II chlorophyll degradation was accelerated 4-5 fold (τ ∼50 h). Chlorophyllide and pheophorbide were identified as intermediates of chlorophyll degradation in the Photosystem I-less/Photosystem II-less mutant. In comparison with the wild type, the chlorophyll synthesis rate was five-fold slower in the Photosystem I-less strain and about eight-fold slower in the strain lacking both photosystems, resulting in different chlorophyll levels in the various mutants. The results presented in this paper demonstrate the presence of a regulation that adjusts the rate of chlorophyll synthesis according to the needs of chlorophyll-binding polypeptides associated with the photosystems.     

Photochemical and photophysical properties of ruthenium(II) bis-bipyridine bis-nitrile complexes: Photolability

The electrochemical and photophysical properties of two bis-nitrilo ruthenium(II) complexes formulated as [Ru(bpy)₂(L)₂](PF₆)₂, where bpy is 2,2′-bipyridine and L is AN = CH₃CN and sn = NC-CH₂CH₂-CN, have been investigated. Electrochemical data are typical of Ru-bpy complexes with two reversible reduction peaks located near −1.3 and −1.6 V assigned to each bipyridine ligand and one Ru^II/Ru^III oxidation wave centered at approximately +1.5 V. The sn derivative is both IR and Raman active with its coordinated CN stretch appearing at 2277 cm⁻¹ and 2273 cm⁻¹, respectively. The UV/Vis absorption spectrum of the sn derivative is dominated by an intense (ε_max ∼ 58700 M⁻¹ cm⁻¹) absorption band at 287 nm assigned as a LC (π → π∗) transition. The peak observed at 418 nm (ε ∼ 10 400 M⁻¹ cm⁻¹) is an MLCT band while the one at 244 nm (ε ∼ 23 600 M⁻¹ cm⁻¹) is of LMLCT character. The AN derivative behaves similarly. Both complexes show low-temperature emission at around 537 nm with a lifetime near 10.0 μs. ¹H and ¹³C assignments are consistent with the formulation of the complexes. The complexes undergo photosubstitution of solvent with quantum efficiencies near one. Calculated and experimental results support replacement of the nitrile ligands by solvent. Based on DFT calculations, the electron density of the HOMO lies on the metal center, the bipyridine ligands and the nitrile ligands and electron density of the LUMO resides primarily on the bipyridine ligands. The electronic spectra obtained from TDDFT calculations closely match the experimental ones.     

Electronic and vibrational analysis of porphyrazine liquid-crystalline structure: Toward photochemical phase switching

The electronic and vibrational Raman spectra of octa-substituted (R = -SC₁₀H₂₁) Co- and Cu-porphyrazines are reported in their solid-state, mesophase, and isotropic liquid forms, as well as in THF solution. Their electronic spectra are composed of traditional Soret (CuS10 = 355 nm, CoS10 = 347 nm) and lower energy Q-bands (CuS10 = 669 nm, CoS10 = 639 nm), as well as a weaker, functionality-specific sulfur n → porphyrin π^∗ feature (CuS10 = 500 nm; CoS10 = 447 nm). In contrast to the broad Q-band for CoS10 in all three neat phases, the lower energy analogue for CuS10 is markedly sharper in the microcrystalline state, but similarly broadens in the mesophase, indicative of long range macrocycle π-π interactions that persist even into the liquid state. The resonance (λ = 647 nm) and off-resonance (λ = 785 nm) Raman spectra of these materials in each phase exhibit four diagnostic vibrations; the C_α-N_m stretch (∼1540-1553) cm⁻¹, C_β-C_β stretch (∼1450 cm⁻¹), C_α-C_β-N_p stretch (∼1300-1315 cm⁻¹), and C_α-C_β stretch (∼1070 cm⁻¹). For CoS10, these vibrations systematically shift to lower energy upon melting, while those for CuS10 collapse to degenerate sets. The differences in the electronic and vibrational profiles as a function of temperature suggest that the mesophase structure is governed by strong axial Co-S interactions for CoS10 which template macrocycle π-π stacking, while for CuS10 the same contacts exist, but they are phase dependent and markedly weaker. These inter-porphyrazine interactions are, therefore, responsible for the distinct differences in the melting and clearing temperatures of their respective mesophases. Finally, based on these diagnostic spectroscopic signatures, a photo-thermal, phase-switching mechanism is demonstrated with λ = 785 nm excitation at reduced temperatures, leading to the ability to spectrally monitor and phase change with a single photon source.     

Specific cation effect on quenching reactions of excited tris(α,α′-diimine) ruthenium(II) and chromium(III) complexes by cyanide complexes in aqueous solutions

Specific salt effects were studied on the quenching reaction of excited [Ru(NN)₃]²⁺ (NN=2,2′-bipyridine(bpy), 1,10-phenanthrorine(phen)) and [Cr(bpy)₃]³⁺ by [Cr(CN)₆]³⁻, [Fe(CN)₆]³⁻ and [Ni(CN)₄]²⁻ in aqueous solutions as a function of alkali metal ions which were added for adjustment of ionic strength. The quenching rate constants in [Ru(NN)₃]²⁺-[Cr(CN)₆]³⁻ and [Cr(bpy)₃]³⁺-[Cr(CN)₆]³⁻ systems are changed by the cations as Li⁺>Na⁺>K⁺≈Rb⁺≈Cs⁺. On the other hand, the rate constants in [Ru(NN)₃]²⁺-[Fe(CN)₆]³⁻ and [Ru(NN)₃]²⁺-[Ni(CN)₄]²⁻ systems, which are diffusion-controlled reactions, are not varied by the alkali metal cations. The obtained order (Li⁺>Na⁺>K⁺≈Rb⁺≈Cs⁺) of the quenching rate constant is quite different from salt effects, Li⁺<Na⁺<K⁺<Rb⁺<Cs⁺, which have been obtained in the electron transfer reactions between complex anions.     

Charge separation in photosystem II core complexes induced by 690-730 nm excitation at 1.7 K

The illumination of oxygen-evolving PSII core complexes at very low temperatures in spectral regions not expected to excite P680 leads to charge separation in a majority of centers. The fraction of centers photoconverted as a function of the number of absorbed photons per PSII core is determined by quantification of electrochromic shifts on Pheo_D1. These shifts arise from the formation of metastable plastoquinone anion (Q_A⁻) configurations. Spectra of concentrated samples identify absorption in the 700-730 nm range. This is well beyond absorption attributable to CP47. Spectra in the 690-730 nm region can be described by the ‘trap’ CP47 absorption at 689 nm, with dipole strength of ∼1 chlorophyll a (chl a), partially overlapping a broader feature near 705 nm with a dipole strength of ∼0.15 chl a. This absorption strength in the 700-730 nm region falls by 40% in the photoconverted configuration. Quantum efficiencies of photoconversion following illumination in the 690-700 nm region are similar to those obtained with green illumination but fall significantly in the 700-730 nm range. Two possible assignments of the long-wavelength absorption are considered. Firstly, as a low intensity component of strongly exciton-coupled reaction center chlorin excitations and secondly as a nominally ‘dark’ charge-transfer excitation of the ‘special pair’ P_D1-P_D2. The opportunities offered by these observations towards the understanding of the nature of P680 and PSII fluorescence are discussed.     

Long-range nonanomalous diffusion of quantum dot-labeled aquaporin-1 water channels in the cell plasma membrane

Aquaporin-1 (AQP1) is an integral membrane protein that facilitates osmotic water transport across cell plasma membranes in epithelia and endothelia. AQP1 has no known specific interactions with cytoplasmic or membrane proteins, but its recovery in a detergent-insoluble membrane fraction has suggested possible raft association. We tracked the membrane diffusion of AQP1 molecules labeled with quantum dots at an engineered external epitope at frame rates up to 91 Hz and over times up to 6 min. In transfected COS-7 cells, >75% of AQP1 molecules diffused freely over ∼7 μm in 5 min, with diffusion coefficient, D_1-3 ∼ 9 × 10⁻¹⁰ cm²/s. In MDCK cells, ∼60% of AQP1 diffused freely, with D_1-3 ∼ 3 × 10⁻¹⁰ cm²/s. The determinants of AQP1 diffusion were investigated by measurements of AQP1 diffusion following skeletal disruption (latrunculin B), lipid/raft perturbations (cyclodextrin and sphingomyelinase), and bleb formation. We found that cytoskeletal disruption had no effect on AQP1 diffusion in the plasma membrane, but that diffusion was increased greater than fourfold in protein de-enriched blebs. Cholesterol depletion in MDCK cells greatly restricted AQP1 diffusion, consistent with the formation of a network of solid-like barriers in the membrane. These results establish the nature and determinants of AQP1 diffusion in cell plasma membranes and demonstrate long-range nonanomalous diffusion of AQP1, challenging the prevailing view of universally anomalous diffusion of integral membrane proteins, and providing evidence against the accumulation of AQP1 in lipid rafts.     

The Semiquinone-Iron Complex of Photosystem II: Structural Insights from ESR and Theoretical Simulation; Evidence that the Native Ligand to the Non-Heme Iron Is Carbonate

The semiquinone-iron complex of photosystem II was studied using electron spin resonance (ESR) spectroscopy and density functional theory calculations. Two forms of the signal were investigated: 1), the native g ∼ 1.9 form; and 2), the g ∼ 1.84 form, which is well known in purple bacterial reaction centers and occurs in photosystem II when treated with formate. The g ∼ 1.9 form shows low- and high-field edges at g ∼ 3.5 and g < 0.8, respectively, and resembles the g ∼ 1.84 form in terms of shape and width. Both types of ESR signal were simulated using the theoretical approach used previously for the BRC complex, a spin Hamiltonian formalism in which the semiquinone radical magnetically interacts (J ∼ 1 cm⁻¹) with the nearby high-spin Fe²⁺. The two forms of ESR signal differ mainly by an axis rotation of the exchange coupling tensor (J) relative to the zero-field tensor (D) and a small increase in the zero-field parameter D (∼6 cm⁻¹). Density functional theory calculations were conducted on model semiquinone-iron systems to identify the physical nature of these changes. The replacement of formate (or glutamate in the bacterial reaction centers) by bicarbonate did not result in changes in the coupling environment. However, when carbonate (CO₃²⁻) was used instead of bicarbonate, the exchange and zero-field tensors did show changes that matched those obtained from the spectral simulations. This indicates that 1), the doubly charged carbonate ion is responsible for the g ∼ 1.9 form of the semiquinone-iron signal; and 2), carbonate, rather than bicarbonate, is the ligand to the iron.