Aquaporin 0 plays a pivotal role in refractive index gradient development in mammalian eye lens to prevent spherical aberration

Aquaporin 0 (AQP0) is a transmembrane channel that constitutes ∼45% of the total membrane protein of the fiber cells in mammalian lens. It is critical for lens transparency and homeostasis as mutations and knockout cause autosomal dominant lens cataract. AQP0 functions as a water channel and as a cell-to-cell adhesion (CTCA) molecule in the lens. Our recent in vitro studies showed that the CTCA function of AQP0 could be crucial to establish lens refractive index gradient (RING). However, there is a lack of in vivo data to corroborate the role of AQP0 as a fiber CTCA molecule which is critical for creating lens RING. The present investigation is undertaken to gather in vivo evidence for the involvement of AQP0 in developing lens RING. Lenses of wild type (WT) mouse, AQP0 knockout (heterozygous, AQP0^+/−) and AQP0 knockout lens transgenically expressing AQP1 (heterozygous AQP0^+/−/AQP1^+/−) mouse models were used for the study. Data on AQP0 protein profile of intact and N- and/or C-terminal cleaved AQP0 in the lens by MALDI-TOF mass spectrometry and SDS–PAGE revealed that outer cortex fiber cells have only intact AQP0 of ∼28 kDa, inner cortical and outer nuclear fiber cells have both intact and cleaved forms, and inner nuclear fiber cells have only cleaved forms (∼26–24 kDa). Knocking out of 50% of AQP0 protein caused light scattering, spherical aberration (SA) and cataract. Restoring the lost fiber cell membrane water permeability (P_f) by transgene AQP1 did not reinstate complete lens transparency and the mouse lenses showed light scattering and SA. Transmission and scanning electron micrographs of lenses of both mouse models showed increased extracellular space between fiber cells. Water content determination study showed increase in water in the lenses of these mouse models. In summary, lens transparency, CTCA and compact packing of fiber cells were affected due to the loss of 50% AQP0 leading to larger extracellular space, more water content and SA, possibly due to alteration in RING. To our knowledge, this is the first report identifying the role of AQP0 in RING development to ward off lens SA during focusing.     

Fluorescence correlation spectroscopy reveals topological segregation of the two tumor necrosis factor membrane receptors

The proinflammatory cytokine tumor necrosis factor (TNF) binds two distinct plasma membrane receptors, TNFR1 and TNFR2. We have produced different receptor mutants fused with enhanced green fluorescent protein to study their membrane dynamics by fluorescence correlation spectroscopy (FCS). TNFR1 mutants show diffusion constants of approximately 1.2 × 10^− 9 cm²/s and a broad distribution of diffusion times, which is hardly affected by ligand binding. However, cholesterol depletion enhances their diffusion, suggesting a constitutive affinity to cholesterol rich membrane microdomains. In contrast, TNFR2 and mutants thereof diffuse rather fast (D? = 3.1 × 10^− 9 cm²/s) with a marked reduction after 30 min of TNF treatment (D? = 0.9 × 10^− 9 cm²/s). This reduction cannot be explained by the formation of higher ordered receptor clusters, since the fluorescence intensity of TNF treated receptors indicate the presence of a few receptor molecules per complex only. Together, these data point to a topological segregation of the two TNF receptors in different microcompartments of the plasma membrane independent of the cytoplasmic signaling domains of the receptors.     

The prostaglandin transporter PGT transports PGH2

Prostaglandin H₂ not only serves as the common precursor of all other PGs, but also directly triggers signals (e.g. platelet aggregation), depending on its location and translocation. The prostaglandin carrier PGT mediates the transport of several prostanoids, such as PGE₂, and PGF_2α. Here we used PGT in the plasma membrane as a model system to test the hypothesis that PGT also transports PGH₂. Using wild-type and PGT-expressing MDCK cells, we show that PGH₂ uptake is mediated both by simple diffusion and by PGT. The PGH₂ influx permeability coefficient for diffusion is (5.66 ± 0.63) × 10⁻⁶ cm/s. The kinetic parameters of PGH₂ transport by PGT are K_m = 376 ± 34 nM and V_max = 210.2 ± 11.4 fmol/mg protein/s. PGH₂ transport by PGT can be inhibited by excess PGE₂ or by a PGT inhibitor. We conclude that PGT may play a role in transporting PGH₂ across cellular membranes.     

Rotation of lipids in membranes: molecular dynamics simulation, 31P spin-lattice relaxation, and rigid-body dynamics

Molecular dynamics simulations and ³¹P-NMR spin-lattice (R₁) relaxation rates from 0.022 to 21.1 T of fluid phase dipalmitoylphosphatidylcholine bilayers are compared. Agreement between experiment and direct prediction from simulation indicates that the dominant slow relaxation (correlation) times of the dipolar and chemical shift anisotropy spin-lattice relaxation are ∼10 ns and 3 ns, respectively. Overall reorientation of the lipid body, consisting of the phosphorus, glycerol, and acyl chains, is well described within a rigid-body model. Wobble, with D_⊥ = 1-2 × 10⁸ s⁻¹, is the primary component of the 10 ns relaxation; this timescale is consistent with the tumbling of a lipid-sized cylinder in a medium with the viscosity of liquid hexadecane. The value for D_|| the diffusion constant for rotation about the long axis of the lipid body, is difficult to determine precisely because of averaging by fast motions and wobble; it is tentatively estimated to be 1 × 10⁷ s⁻¹. The resulting D_||/D_⊥ ≈ 0.1 implies that axial rotation is strongly modulated by interactions at the lipid/water interface. Rigid-body modeling and potential of mean force evaluations show that the choline group is relatively uncoupled from the rest of the lipid. This is consistent with the ratio of chemical shift anisotropy and dipolar correlation times reported here and the previous observations that ³¹P-NMR lineshapes are axially symmetric even in the gel phase of dipalmitoylphosphatidylcholine.     

The influence of different membrane components on the electrical stability of bilayer lipid membranes

A good understanding of cell membrane properties is crucial for better controlled and reproducible experiments, particularly for cell electroporation where the mechanism of pore formation is not fully elucidated. In this article we study the influence on that process of several constituents found in natural membranes using bilayer lipid membranes. This is achieved by measuring the electroporation threshold (V_th) defined as the potential at which pores appear in the membrane. We start from highly stable 1,2-diphytanoyl-sn-glycero-3-phosphocholine (DPhPC) membranes (V_th ∼ 200 mV), and subsequently add therein other phospholipids, cholesterol and a channel protein. While the phospholipid composition has a slight effect (100 mV ≤ V_th ≤ 290 mV), cholesterol gives a concentration-dependent effect: a slight stabilization until 5% weight (V_th ∼ 250 mV) followed by a noticeable destabilization (V_th ∼ 100 mV at 20%). Interestingly, the presence of a model protein, α-hemolysin, dramatically disfavours membrane poration and V_th shows a 4-fold increase (∼ 800 mV) from a protein density in the membrane of 24 × 10^− 3 proteins/μm². In general, we find that pore formation is affected by the molecular organization (packing and ordering) in the membrane and by its thickness. We correlate the resulting changes in molecular interactions to theories on pore formation.     

Protective role of S-adenosyl-l-methionine against hydrochloric acid stress in Saccharomyces cerevisiae

S-adenosyl-l-methionine (AdoMet, 1 mM) protects the stationary phase cells of Saccharomyces cerevisiae against the killing effect of acid (10 mM HCl, pH ∼ 2). Both the acid and the acid plus AdoMet treatment for 2 h increased the plasma membrane H⁺-ATPase activity; thereafter it decreased to the basal level. AdoMet partially recovered the intracellular pH (pH_in) that dropped in presence of acid. AdoMet treatment facilitated acid induced phospholipid biosynthesis as well as membrane proliferation, which was reflected in the cellular lipid composition.     

Spontaneous, intervesicular transfer rates of fluorescent, acyl chain-labeled phosphatidylcholine analogs

It was recently shown that the structure of the fluorophore attached to the acyl chain of phosphatidylcholine analogs determines their mechanism of transport across the plasma membrane of yeast cells (Elvington et al., J. Biol Chem. 280:40957, 2005). In order to gain further insight into the physical properties of these fluorescent phosphatidylcholine (PC) analogs, the rate and mechanism of their intervesicular transport was determined. The rate of spontaneous exchange was measured for PC analogs containing either NBD (7-nitrobenz-2-oxa-1,3-diazol-4-yl), Bodipy FL (4,4-difluoro-5,7-dimethyl-4-bora-3a,4a-diaza-s-indacene), Bodipy 530 (4,4-difluoro-5,7-diphenyl-4-bora-3a,4a-diaza-s-indacene), or Bodipy 581 (4,4-difluoro-5-(4-phenyl-1,3-butadienyl)-4-bora-3a,4a-diaza-s-indacene) attached to a five or six carbon acyl chain in the sn-2 position. The rate of transfer between phospholipid vesicles was measured by monitoring the increase in fluorescence as the analogs transferred from donor vesicles containing self-quenching concentrations to unlabeled acceptor vesicles. Kinetic analysis indicated that the transfer of each analog occurred by diffusion through the water phase as opposed to transfer during vesicle collisions. The vesicle-to-monomer dissociation rate constants differed by over four orders of magnitude: NBD-PC (k_dis = 0.115 s^− 1; t_1/2 = 6.03 s); Bodipy FL-PC (k_dis = 5.2 × 10^− 4; t_1/2 = 22.2 min); Bodipy 530-PC (k_dis = 1.52 × 10^− 5; t_1/2 = 12.6 h); and Bodipy 581-PC (k_dis = 5.9 × 10^− 6; t_1/2 = 32.6 h). The large differences in spontaneous rates of transfer through the water measured for these four fluorescent PC analogs reflect their hydrophobicity and may account for their recognition by different mechanisms of transport across the plasma membrane of yeast.     

Aqueous solution chemistry of dichloro[S-methylcysteine(N,S)]platinum(II) isomers and their hydrolysis products

Rate and equilibrium constants at 25 °C, pH ∼ 1, and ionic strength 0.10 for hydrolysis of the two non-equivalent chlorides of dichloro[S-methyl-l-cysteine(N,S)]platinum(II) isomers, denoted [PtCl₂(SmecysH)], and the resultant chloro-aqua species have been determined by NMR, potentiometric, and spectrophotometric methods. Though hydrolysis constants, K_h, for the two chlorides are similar (pK_h = 4-5), the rate of hydrolysis of the chloride trans to coordinated S, k_h = 3.4 × 10⁻³ s⁻¹, is 2-3 orders of magnitude faster than the k_h for the other chloride, 2.3 × 10⁻⁶ s⁻¹, and for the cancer drug cisplatin, cis-[PtCl₂(NH₃)₂], 5.2 × 10⁻⁵ s⁻¹. Relative rates of hydrolysis determined under three different experimental conditions (pH ∼ 1 in 0.10 M HNO₃, high pH in 0.10 M NaOH, and at low pH with Ag⁺ assistance) are consistent: the Cl trans to S is 100-1000 times more labile than the Cl cis to S. Potentiometric and NMR methods were also used to estimate pK_a values of all aqua species, which are comparable to values reported for corresponding aqua species derived from cisplatin.     

Development of cesium phosphotungstate salt and chitosan composite membrane for direct methanol fuel cells

A novel composite membrane has been developed by doping cesium phosphotungstate salt (Cs_xH_3−xPW₁₂O₄₀ (0 ≤ x ≤3), Cs_x-PTA) into chitosan (CTS/Cs_x-PTA) for application in direct methanol fuel cells (DMFCs). Uniform distribution of Cs_x-PTA nanoparticles has been achieved in the chitosan matrix. The proton conductivity of the composite membrane is significantly affected by the Cs_x-PTA content in the composite membrane as well as the Cs substitution in PTA. The highest proton conductivity for the CTS/Cs_x-PTA membranes was obtained with x = 2 and Cs₂-PTA content of 5 wt%. The value is 6 × 10⁻³ S cm⁻¹ and 1.75 × 10⁻² S cm⁻¹ at 298 K and 353 K, respectively. The methanol permeability of CTS/Cs₂-PTA membrane is about 5.6 × 10⁻⁷, 90% lower than that of Nafion-212 membrane. The highest selectivity factor (φ) was obtained on CTS/Cs₂-PTA-5 wt% composite membrane, 1.1 × 10⁴/S cm⁻³ s. The present study indicates the promising potential of CTS/Cs_x-PTA composite membrane as alternative proton exchange membranes in direct methanol fuel cells.     

Kinetic and thermodynamic properties of the folding and assembly of formate dehydrogenase

The folding mechanism and stability of dimeric formate dehydrogenase from Candida methylica was analysed by exposure to denaturing agents and to heat. Equilibrium denaturation data yielded a dissociation constant of about 10⁻¹³ M for assembly of the protein from unfolded chains and the kinetics of refolding and unfolding revealed that the overall process comprises two steps. In the first step a marginally stable folded monomeric state is formed at a rate (k₁) of about 2 × 10⁻³ s⁻¹ (by deduction k₋₁ is about10⁻⁴ s⁻¹) and assembles into the active dimeric state with a bimolecular rate constant (k₂) of about 2 × 10⁴ M⁻¹ s⁻¹. The rate of dissociation of the dimeric state in physiological conditions is extremely slow (k₋₂ ∼ 3 × 10⁻⁷ s⁻¹).     

Kinetics of reaction of nitrogen dioxide with dihydrorhodamine and the reaction of the dihydrorhodamine radical with oxygen: implications for quantifying peroxynitrite formation in cells

Dihydrorhodamine 123 (RhH₂) has been used to detect ‘reactive nitrogen species’, including peroxynitrite and its radical decomposition products, peroxynitrite probably oxidizing RhH₂ to rhodamine (Rh) via radical products rather than directly. In this study, the radical intermediate (RhH) was generated by pulse radiolysis, and shown to react with oxygen with a rate constant k ∼ 7 × 10⁸ M^-1 s^-1. This fast reaction was exploited in experiments observing Rh being formed slowly (k ∼ 4-7 × 10⁵ M^-1 s^-1) from oxidation of RhH₂ by nitrogen dioxide in a rate-limiting step, >1000-fold slower than the corresponding oxidation by carbonate radicals. The time-dependent uptake of RhH₂ into mammalian cells was measured, with average intracellular levels reaching only ∼10 μM with the protocol used. The combination of low loading and relatively low reactivity of oxidants towards RhH₂ compared to competing cellular nucleophiles suggests rather a small fraction of peroxynitrite-derived radicals (mainly CO₃⁻) may be scavenged intracellularly by RhH₂.     

Diffusion of Exchangeable Water in Cortical Bone Studied by Nuclear Magnetic Resonance

The rate-limiting step in the delivery of nutrients to osteocytes and the removal of cellular waste products is likely diffusion. The transport of osteoid water across the mineralized matrix of bone was studied by proton nuclear magnetic resonance spectroscopy and imaging by measuring the diffusion fluxes of tissue water in cortical bone specimens from the midshaft of rabbit tibiae immersed in deuterium oxide. From the diffusion coefficient (D_a = (7.8 ± 1.5) × 10⁻⁷ cm²/s) measured at 40°C (close to physiological temperature), it can be inferred that diffusive transport of small molecules from the bone vascular system to the osteocytes occurs within minutes. The activation energy for water diffusion, calculated from D_a measured at four different temperatures, suggests that the interactions between water molecules and matrix pores present significant energy barriers to diffusion. The spatially resolved profile of D_a perpendicular to the cortical surface of the tibia, obtained using a finite difference model, indicates that diffusion rates are higher close to the endosteal and periosteal surfaces, decreasing toward the center of the cortex. Finally, the data reveal a water component (∼30%) diffusing four orders of magnitude more slowly, which is ascribed to water tightly bound to the organic matrix and mineral phase.     

Asymmetric structural features in single supported lipid bilayers containing cholesterol and GM1 resolved with synchrotron X-Ray reflectivity

The cell membrane comprises numerous protein and lipid molecules capable of asymmetric organization between leaflets and liquid-liquid phase separation. We use single supported lipid bilayers (SLBs) to model cell membranes, and study how cholesterol and asymmetrically oriented ganglioside receptor G_M1 affect membrane structure using synchrotron x-ray reflectivity. Using mixtures of cholesterol, sphingomyelin, and 1,2-dioleoyl-sn-glycero-3-phosphocholine, we characterize the structure of liquid-ordered and liquid-disordered SLBs in terms of acyl-chain density, headgroup size, and leaflet thickness. SLBs modeling the liquid-ordered phase are 10 Å thicker and have a higher acyl-chain electron density (〈ρ_chain〉 = 0.33 e⁻/ų) compared to SLBs modeling the liquid-disordered phase, or pure phosphatidylcholine SLBs (〈ρ_chain〉 = 0.28 e⁻/ų). Incorporating G_M1 into the distal bilayer leaflet results in membrane asymmetry and thickening of the leaflet of 4-9 Å. The structural effect of G_M1 is more complex in SLBs of cholesterol/sphingomyelin/1,2-dioleoyl-sn-glycero-3-phosphocholine, where the distal chains show a high electron density (〈ρ_chain〉 = 0.33 e⁻/ų) and the lipid diffusion constant is reduced by ∼50%, as measured by fluorescence microscopy. These results give quantitative information about the leaflet asymmetry and electron density changes induced by receptor molecules that penetrate a single lipid bilayer.     

Fluctuations of the red blood cell membrane: relation to mechanical properties and lack of ATP dependence

We have analyzed the fluctuations of the red blood cell membrane in both the temporal ((ω(s⁻¹)) and spatial (q(m⁻¹)) frequency domains. The cells were examined over a range of osmolarities leading to cell volumes from 50% to 170% of that in the isotonic state. The fluctuations of the isotonic cell showed an ∼q⁻³-dependence, indicative of a motion dominated by bending, with an inferred bending modulus of ∼9 × 10⁻¹⁹J. When the cells were osmotically swollen to just below the point of lysis (166% of physiological volume), a q⁻¹-dependence of the fluctuations supervened, implying that the motion was now dominated by membrane tension; estimated as ∼1.3 × 10⁻⁴ nm⁻¹. When, on the other hand, the cells were osmotically dehydrated, the fluctuation amplitude progressively decreased. This was caused by a rise in internal viscosity, as shown by measurements on resealed ghosts containing a reduced hemoglobin concentration, which displayed no such effect. We examined, in addition, cells depleted of ATP, before the onset of echinocytosis, and could observe no change in fluctuation amplitude. We conclude that the membrane fluctuations of the red cell are governed by bending modulus, membrane tension, and cytosolic viscosity, with little or no dependence on the presence or absence of ATP.     

An endo-(1→3)-β-d-glucanase from the scallop Chlamys albidus: catalytic properties, cDNA cloning and secondary-structure characterization

An endo-(1→3)-β-d-glucanase (L₀) with molecular mass of 37 kDa was purified to homogeneity from the crystalline style of the scallop Chlamys albidus. The endo-(1→3)-β-d-glucanase was extremely thermolabile with a half-life of 10 min at 37 °C. L₀ hydrolyzed laminaran with K_m ∼ 0.75 mg/mL, and catalyzed effectively transglycosylation reactions with laminaran as donor and p-nitrophenyl β d-glucoside as acceptor (K_m ∼ 2 mg/mL for laminaran) and laminaran as donor and as acceptor (K_m ∼ 5 mg/mL) yielding p-nitrophenyl β d-glucooligosaccharides (n = 2-6) and high-molecular branching (1→3),(1→6)-β-d-glucans, respectively. Efficiency of hydrolysis and transglycosylation processes depended on the substrate structure and decreased appreciably with the increase of the percentage of β-(1→6)-glycosidic bonds, and laminaran with 10% of β-(1→6)-glycosidic bonds was the optimal substrate for both reactions. The CD spectrum of L₀ was characteristic for a protein with prevailing β secondary-structural elements. Binding L₀ with d-glucose as the best acceptor for transglycosylation was investigated by the methods of intrinsic tryptophan fluorescence and CD. Glucose in concentration sufficient to saturate the enzyme binding sites resulted in a red shift in the maximum of fluorescence emission of 1-1.5 nm and quenching the Trp fluorescence up to 50%. An apparent association constant of L₀ with glucose (K_a = 7.4 × 10⁵ ± 1.1 × 10⁵ M⁻¹) and stoichiometry (n = 13.3 ± 0.7) was calculated. The cDNA encoding L₀ was sequenced, and the enzyme was classified in glycoside hydrolases family 16 on the basis of the amino acid sequence similarity.     

Determination of protein mobility in mitochondrial membranes of living cells

Molecular mobility in membranes of intracellular organelles is poorly understood, due to the lack of experimental tools applicable for a great diversity of shapes and sizes such organelles can acquire. Determinations of diffusion within the plasma membrane or cytosol are based mostly on the assumption of an infinite flat space, not valid for curved membranes of smaller organelles. Here we extend the application of FRAP to mitochondria of living cells by application of numerical analysis to data collected from a small region inside a single organelle. The spatiotemporal pattern of light pulses generated by the laser scanning microscope during the measurement is reconstructed in silico and consequently the values of diffusion parameters best suited to the particular organelle are found. The mobility of the outer membrane proteins hFis and Tom7, as well as oxidative phosphorylation complexes COX and F₁F₀ ATPase located in the inner membrane is analyzed in detail. Several alternative models of diffusivity applied to these proteins provide insight into the mechanisms determining the rate of motion in each of the membranes. Tom7 and hFis move along the mitochondrial axis in the outer membrane with similar diffusion coefficients (D = 0.7 μm²/s and 0.6 μm²/s respectively) and equal immobile fraction (7%). The notably slower motion of the inner membrane proteins is best represented by a dual-component model with approximately equal partitioning of the fractions (F₁F₀ ATPase: 0.4 μm²/s and 0.0005 μm²/s; COX: 0.3 μm²/s and 0.007 μm²/s). The mobility patterns specific for the membranes of this organelle are unambiguously distinguishable from those of the plasma membrane or artificial lipid environments: The parameters of mitochondrial proteins indicate a distinct set of factors responsible for their diffusion characteristics.     

Dynamic and energetic mechanisms for the distinct permeation rate in AQP1 and AQP0

Despite sharing overall sequence and structural similarities, water channel aquaporin 0 (AQP0) transports water more slowly than other aquaporins. Using molecular dynamics simulations of AQP0 and AQP1, we find that there is a sudden decrease in the distribution profile of water density along the pore of AQP0 in the region of residue Tyr23, which significantly disrupts the single file water chain by forming hydrogen bond with permeating water molecules. Comparisons of free-energy and interaction-energy profiles for water conduction between AQP0 and AQP1 indicate that this interruption of the water chain causes a huge energy barrier opposing water translocation through AQP0. We further show that a mutation of Tyr23 to phenylalanine leads to a 2- to 4-fold enhancement in water permeability of AQP0, from (0.5 ± 0.2) × 10^− 14 cm³s^− 1 to (1.9 ± 0.6) × 10^− 14 cm³s^− 1. Therefore, Tyr23 is a dominate factor leading to the low water permeability in AQP0.     

10-Å CryoEM Structure and Molecular Model of the Myriapod (Scutigera) 6 × 6mer Hemocyanin: Understanding a Giant Oxygen Transport Protein

Oxygen transport in Myriapoda is maintained by a unique 6 × 6mer hemocyanin, that is, 36 subunits arranged as six hexamers (1 × 6mers). In the sluggish diplopod Spirostreptus, the 1 × 6mers seem to operate as almost or fully independent allosteric units (h ∼ 1.3; P₅₀ ∼ 5 torr), whereas in the swift centipede Scutigera, they intensively cooperate allosterically (h ∼ 10; P₅₀ ∼ 50 torr). Here, we show the chemomechanical basis of this differential behavior as deduced from hybrid 6 × 6mer structures, obtained by single-particle cryo-electron microscopy of the Scutigera 6 × 6mer (10.0 Å resolution according to the 0.5 criterion) and docking of homology-modeled subunits from Scutigera and two diplopods, Spirostreptus and Polydesmus. The Scutigera 6 × 6mer hemocyanin is a trigonal antiprism assembled from six smaller trigonal antiprisms (1 × 6mers), thereby exhibiting D3 point group symmetry. It can be described as two staggered 3 × 6mers or three oblique 2 × 6mers. Topologically, the 6 × 6mer is subdivided into six subunit zones, thereby exhibiting a mantle (24 subunits) and a core (12 subunits). The six hexamers are linked by 21 bridges, subdivided into five types: two within each 3 × 6mer and three between both 3 × 6mers. The molecular models of the 6 × 6mer reveal intriguing amino acid appositions at these inter-hexamer interfaces. Besides opportunities for salt bridges, we found pairs of carboxylate residues for possible bridging via a Ca²⁺ or Mg²⁺ ion. Moreover, we detected histidine clusters, notably in Scutigera, allowing us to advance hypotheses as to how the hexamers are allosterically coupled in centipede hemocyanin and why they act more independently in diplopod hemocyanin.     

Effect of ceramide N-acyl chain and polar headgroup structure on the properties of ordered lipid domains (lipid rafts)

Ceramides are sphingolipids that greatly stabilize ordered membrane domains (lipid rafts), and displace cholesterol from them. Ceramide-rich rafts have been implicated in diverse biological processes. Because ceramide analogues have been useful for probing the biological function of ceramide, and may have biomedical applications, it is important to characterize how ceramide structure affects membrane properties, including lipid raft stability and composition. In this report, fluorescence quenching assays were used to evaluate the effect of analogues of ceramide with different N-acyl chains or different sphingoid backbones on raft stability and sterol content. The effect of replacing 18 mol% of sphingomyelin (SM) with ceramide in vesicles composed of a 1:1 (mol:mol) mixture of SM and dioleoylphosphatidylcholine (DOPC), with or without 25 mol% sterol, was examined. In the absence of sterol, the thermal stability of the SM-rich ordered domains increased with ceramide N-acyl chain length in the order C2:0 ∼ C6:0 ∼ C8:0 < no ceramide < C12:0 < C16:0. In vesicles containing 25 mol% cholesterol (1:1:0.66 sphingolipid:DOPC:cholesterol), the dependence of raft stability on ceramide N-acyl chain length increased in the order C8:0 ∼ C6:0 < C2:0 < C12:0 ∼ no ceramide < C16:0. We also studied the stability of lipid rafts in the presence of N-lauroyl- and N-palmitoylsphingosine analogues containing altered structures in or near the polar portion of the sphingoid base. In almost all cases, the analogues stabilized rafts to about the same degree as a normal ceramide containing the same acyl chain. The only exception was N-palmitoyl-4D-ribophytosphingosine, which was very strongly raft-stabilizing. We conclude that variations in sphingoid base structure induce only insignificant changes in raft properties. N-Lauroyl and N-palmitoylsphingosine and their analogues displaced sterol from rafts to a significant degree. Both C12:0 and C16:0 analogues of ceramide may be good mimics of natural ceramide, and useful for cellular studies in which maintenance of the normal physical properties of ceramide are important.     

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.