Rotational dynamics of the Ca-ATPase in sarcoplasmic reticulum studied by time-resolved phosphorescence anisotropy

We have investigated the microsecond rotational motions of the Ca-ATPase in rabbit skeletal sarcoplasmic reticulum (SR), by measuring the time-resolved phosphorescence anisotropy of erythrosin 5-isothiocyanate (ERITC) covalently and specifically attached to the enzyme. Over a wide range of solvent conditions and temperatures, the phosphorescence anisotropy decay was best fit by a sum of three exponentials plus a constant term. At 4 degrees C, the rotational correlation times were phi 1 = 13 +/- 3 microseconds, phi 2 = 77 +/- 11 microseconds, and phi 3 = 314 +/- 23 microseconds. Increasing the solution viscosity with glycerol caused very little effect on the correlation times, while decreasing the lipid viscosity with diethyl ether decreased the correlation times substantially, indicating that the decay corresponds to rotation of the protein within the membrane, not to vesicle tumbling. The normalized residual anisotropy (A infinity) is insensitive to viscosity and temperature changes, supporting the model of uniaxial rotation of the protein about the membrane normal. The value of A infinity (0.20 +/- .02) indicates that each of the three decay components can be analyzed as a separate rotational species, with the preexponential factor Ai equal to 1.25X the mole fraction. An empirically accurate measurement of the membrane lipid viscosity was obtained, permitting a theoretical analysis of the correlation times in terms of the sizes of the rotating species. At 4 degrees C, the dominant correlation time (phi 3) is too large for a Ca-ATPase monomer, strongly suggesting that the enzyme is primarily aggregated (oligomeric).(ABSTRACT TRUNCATED AT 250 WORDS)     

Rotational diffusion of the ADP/ATP translocator in the inner membrane of mitochondria and in proteoliposomes

The ADP/ATP translocator was selectively labeled with the triplet probe eosin-5-maleimide (EMA) after pretreatment with N-ethylmaleimide in beef heart mitochondria, as reported previously for submitochondrial particles (Müller, M., Krebs, J. J. R., Cherry, R. J., and Kawato, S. (1982) J. Biol. Chem. 257, 1117-1120). The EMA binding was completely inhibited by carboxyatractylate. 0.7-1.1 molecules of EMA conjugated with 1 molecule of the dimeric translocator with Mr approximately 65,000. The EMA binding decreased [14C]ADP uptake by about approximately 25%. The EMA-labeled translocator bongkrekate complex was purified and reconstituted in liposomes by removing Triton X-100 with Amberlite XAD-2. The liposomes were composed of phosphatidylcholine/phosphatidylethanolamine/cardiolipin and the lipid to protein ratio by weight was (L/P) = 60. Rotational diffusion of the ADP/ATP translocator around the membrane normal was measured in reconstituted proteoliposomes and in the mitochondrial inner membranes by observing the flash-induced absorption anisotropy, r(t), of EMA. In proteoliposomes with L/P = 60, the translocator was rotating with an approximate average rotational relaxation time of phi congruent to 246 microseconds and a normalized time-independent anisotrophy [r3/rr(0)]min congruent to 0.55. In intact mitochondria, values of phi congruent to 405 microseconds and r3/rr(0) congruent to 0.79 were obtained. The higher value of r3/rr(0) in mitochondria compared with proteoliposomes indicates the co-existence of rotating and immobile translocator (phi greater than 20 ms) in the inner mitochondrial membrane. Based on the assumption that all the translocator is rotating in the lipid-rich proteoliposomes, the population of the mobile translocator at 20 degrees C was calculated to be approximately 47%. By removing the outer membrane, the mobile population was increased to approximately 70% in mitoplasts, while approximately 53% of the translocator was rotating in submitochondrial particles. The above results indicate a significant difference in protein-protein interactions of the ADP/ATP translocator in the different types of inner membranes of mitochondria. The immobile population of the translocator could be due to nonspecific protein aggregates caused by the very high concentration of proteins in the inner membrane of mitochondria (L/P approximately 0.4).     

Rotational mobility of an erythrocyte membrane integral protein band 3 in dimyristoylphosphatidylcholine reconstituted vesicles and effect of binding of cytoskeletal peripheral proteins

Band 3 protein was isolated from human erythrocyte membranes, purified, and reconstituted into a well-defined phospholipid bilayer matrix (dimyristoylphosphatidylcholine). The preparation yielded uniform single-bilayered vesicles of the diameter 40--80 nm. The rotational motion of band 3 was studied by saturation transfer electron spin resonance (ESR) spectroscopy of covalently attached maleimide spin-labels. The rotational mobility changed in response to the host lipid phase transition. The rotational correlation time was in a range from 73 (37 degrees C) to 94 microseconds (26 degrees C) in the fluid phase and from 240 (15 degrees C) to 420 microseconds (5 degrees C) in the solid phase. The motion was analyzed based on the anisotropic rotation of band 3 in the reconstituted vesicles. To obtain information on the rotational diffusion constant around the axis parallel to the membrane normal, we made an attempt to measure the angle between the spin-label magnetic axis and the membrane normal. The result gave 3.9 x 10(4) s-1 at 37 degrees C as a rough estimate for the diffusion constant. This is compatible to anisotropic rotation of a cylinder of radius 3.3 nm in a two-dimensional matrix with inner viscosity 2 P and inner thickness 4 nm. The cytoskeletal peripheral proteins caused a definite increase in the rotational correlation time (from 73 to 180 microseconds at 37 degrees C, for example). The restriction of the rotational mobility was shown to be due to the ankyrin-linked interaction between band 3 and spectrin-actin-band 4.1 proteins in the reconstituted membranes.     

A novel approach to blood plasma viscosity measurement using fluorescent molecular rotors

Molecular rotors, a group of fluorescent molecules with viscosity-dependent quantum yield, were tested for their suitability to act as fluorescence-based plasma viscometers. The viscosity of samples of human plasma was modified by the addition of pentastarch (molecular mass 260 kDa, 10% solution in saline) and measured with a Brookfield viscometer. Plasma viscosity was 1.6 mPa x s, and the mixtures ranged up to 4.5 mPa x s (21 degrees C). The stimulated light emission of the molecular rotors mixed in the plasma samples yielded light intensity that was nonoverlapping and of significantly different intensity for viscosity steps down to 0.3 mPa x s (n = 5, P < 0.0001). The mathematical relationship between intensity (I) and viscosity (eta) was found to be eta = (kappaI)(nu). After calibration and scaling the fluorescence based measurement had an average deviation versus the conventional viscometric measurements that was <1.8%. These results show the suitability of molecular rotors for fast, low-volume biofluid viscosity measurements achieving accuracy and precision comparable to mechanical viscometers.     

Conformation of human fibrinogen in solution from polarized triplet spectroscopy.

The rotational motions of human fibrinogen in solution at 20 degrees C have been examined, in the 0.2-12-microseconds time range, by measuring the laser-induced dichroism of the triplet state of an erythrosin probe covalently bonded to the protein. The decay of the anisotropy was multiexponential, and up to three correlation times (phi 1 = 380 +/- 50 ns, phi 2 = 1.1 +/- 0.1 microseconds, and phi 3 = 3.3 +/- 0.6 microseconds) were needed to obtain a satisfactory analysis. The experimental data are consistent with the brownian motions of an elongated, rigid particle. If the correlation times are combined with previous data on the intrinsic viscosity of fibrinogen, the rotational and translational diffusive properties of the protein can be reproduced with high accuracy by idealizing it as an elongated ellipsoid of revolution with dimensions (2a x 2b) of (54 +/- 6) x (7.2 +/- 0.5) nm, having rotational diffusion constants of D parallel = (6.2 +/- 0.7) x 10(5) s-1 and D perpendicular = (5 +/- 1) x 10(4) s-1. The possibility of Ca(2+)-dependent changes in the rigidity or conformation of fibrinogen was excluded by examining the submicrosecond time-resolved fluorescence depolarization of 1-methylpyrene conjugates of the protein in the presence of different calcium concentrations. Although there are inherent difficulties to extrapolate the data on isolated fibrinogen molecules to the polymerizing species, this relatively stiff conformation meets the requirements of the classical half-staggered double-stranded model of fibrin polymerization rather better than those of the recently proposed interlocked single-stranded mechanism.     

Single-molecule anisotropy imaging

A novel method, single-molecule anisotropy imaging, has been employed to simultaneously study lateral and rotational diffusion of fluorescence-labeled lipids on supported phospholipid membranes. In a fluid membrane composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine, in which the rotational diffusion time is on the order of the excited-state lifetime of the fluorophore rhodamine, a rotational diffusion constant, D(rot) = 7 x 10(7) rad(2)/s, was determined. The lateral diffusion constant, measured by direct analysis of single-molecule trajectories, was D(lat) = 3.5 x 10(-8) cm(2)/s. As predicted from the free-volume model for diffusion, the results exhibit a significantly enhanced mobility on the nanosecond time scale. For membranes of DPPC lipids in the L(beta) gel phase, the slow rotational mobility permitted the direct observation of the rotation of individual molecules characterized by D(rot) = 1.2 rad(2)/s. The latter data were evaluated by a mean square angular displacement analysis. The technique developed here should prove itself profitable for imaging of conformational motions of individual proteins on the time scale of milliseconds to seconds.     

Effects of melittin on molecular dynamics and Ca-ATPase activity in sarcoplasmic reticulum membranes: time-resolved optical anisotropy.

We have studied the effect of melittin, a basic membrane-binding peptide, on Ca-ATPase activity and on protein and lipid dynamics in skeletal sarcoplasmic reticulum (SR), using time-resolved phosphorescence and fluorescence spectroscopy. Melittin completely inhibits Ca-ATPase activity, with half-maximal inhibition at 9 +/- 1 mol of melittin bound to the membrane per mole of ATPase (0.1 mol of melittin per mole of lipid). The time-resolved phosphorescence anisotropy (TPA) decay of the Ca-ATPase labeled with erythrosin isothiocyanate (ERITC) shows that melittin restricts microsecond protein rotational motion. At 25 degrees C in the absence of melittin, the TPA is characterized by three decay components, corresponding to a rapid segmental motion (correlation time phi 1 = 2-3 microseconds), the uniaxial rotation of monomers or dimers (phi 2 = 16-22 microseconds), and the uniaxial rotation of larger oligomers (phi 3 = 90-140 microseconds). The effect of melittin is primarily to decrease the fraction of the more mobile monomer/dimer species (A2) while increasing the fractions of the larger oligomer (A3) and very large aggregates (A infinity). Time-resolved fluorescence anisotropy of the lipid-soluble probe diphenylhexatriene (DPH) shows only a slight increase in the lipid hydrocarbon chain effective order parameter, corresponding to an increase in lipid viscosity that is too small to account for the large decrease in protein mobility or inhibition of Ca-ATPase activity. Thus the inhibitory effect of melittin correlates with its capacity to aggregate the Ca-ATPase and is consistent with previously reported inhibition of this enzyme under conditions that increase protein-protein interactions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Dynamical properties of a hydrated lipid bilayer from a multinanosecond molecular dynamics simulation

A fully hydrated dimiristoylphosphatidylcholine (DMPC) bilayer has been studied by a molecular dynamics simulation. The system, which consisted of 64 DMPC molecules and 1792 water molecules, was run in the NVE ensemble at a temperature of 333 K for a total of 10 ns. The resulting trajectory was used to analyze structural and dynamical quantities. The electron density, bilayer spacing, and order parameters (S(CD)), based on the AMBER forcefield and SPCE water model are in good agreement with previous calculations and experimental data. The simulation reveals evidence for two types of lateral diffusive behavior: cage hopping and that of a two-dimensional liquid. The lateral diffusion coefficient is 8 x 10(-8) cm(2)/s. We characterize the rotational motion, and find that the lipid tail rotation (D(rot_tail) = -0.04 rad(2)/ns) is slower then the head group rotation (D(rot_hg) = 2.2 rad(2)/ns), which is slower than the overall in plane (D(rot) = 3.2 rad(2)/ns) for the lipid molecule.     

Order and fluidity of lipid membranes as determined by fluorescence anisotropy decay

The fluorescence anisotropy decay of four different probes in bilayers of dimyristoylphosphatidylcholine was measured. The probes are diphenylhexatriene, diphenyloctatetraene, trimethylaminodiphenylhexatriene, and trans-parinaric acid. The data for each probe were analyzed in terms of two orientational order parameters, the ordinary order parameter and a higher one, and two rotational diffusion coefficients. The order parameters are largely independent of probe size, but depend on the position of the probes along the membrane normal, thus reflecting the profile of lipid order. If a probe is located in the plateau region of lipid order, its order parameters are interpreted as representing the rigid-body order of lipids. According to this interpretation, the total lipid order in the plateau region originates about equally from rigid-body order and conformational order. The two order parameters obtained for each probe are used to derive approximate angular distributions of the probe molecules. The diffusion coefficient for rotation about the long molecular axis is found to be infinitely large, indicating unhindered rotation about this axis. The diffusion coefficient for rotation about the short molecular axes is evaluated for a viscosity which results as 0.2 poise. This viscosity for rotational diffusion is an order of magnitude smaller than the viscosity for lateral diffusion indicating that at least two viscosities are required to characterize the fluidity of a lipid membrane.Abbreviations FAD fluorescence anisotropy decay - DMR deuterium magnetic resonance - ESR electron spin resonance - DMPC dimyristoylphosphatidylcholine - DPPC dipalmitoylphosphatidylcholine - DPH 1,6-diphenyl-1,3,5-hexatriene - DPO 1,6-diphenyl-1,3,5,7-octatetraene - TMA-DPH 1-[4-(trimethylamino)phenyl]-6-phenyl-1,3,5-hexatriene - tPnA trans-parinaric acid - NPN N-phenyl-1-naphthylamine - BBO 2,5-bis(4-biphenylyl)oxazole     

Lipid fluidity directly modulates the overall protein rotational mobility of the Ca-ATPase in sarcoplasmic reticulum

We have developed a quantitative and relatively model-independent measure of lipid fluidity using EPR and have applied this method to compare the temperature dependence of lipid hydrocarbon chain fluidity, overall protein rotational mobility, and the calcium-dependent enzymatic activity of the Ca-ATPase in sarcoplasmic reticulum. We define membrane lipid fluidity to be T/eta, where eta is the viscosity of a long chain hydrocarbon reference solvent in which a fatty acid spin label gives the same EPR spectrum (quantitated by the order parameter S) as observed for the same probe in the membrane. This measure is independent of the reference solvent used as long as the spectral line shapes in the membrane and the solvent match precisely, indicating that the same type of anisotropic probe motion occurs in the two systems. We argue that this empirical measurement of fluidity, defined in analogy to the macroscopic fluidity (T/eta) of a bulk solvent, should be more directly related to protein rotational mobility (and thus to protein function) than are more conventional measures of fluidity, such as the rate or amplitude of rotational motion of the lipid hydrocarbon chains themselves. This new definition thus offers a fluidity measure that is more directly relevant to the protein's behavior. The direct relationship between this measure of membrane fluidity and protein rotational mobility is supported by measurements in sarcoplasmic reticulum. The overall rotational motion of the spin-labeled Ca-ATPase protein was measured by saturation-transfer EPR. The Arrhenius activation energy for protein rotational mobility (11-12 kcal/mol/degree) agrees well with the activation energy for lipid fluidity, if defined as in this study, but not if more conventional definitions of lipid fluidity are used. This agreement, which extends over the entire temperature range from 0 to 40 degrees C, suggests that protein mobility depends directly on lipid fluidity in this system, as predicted from hydrodynamic theory. The same activation energy is observed for the calcium-dependent ATPase activity under physiological conditions, suggesting that protein rotational mobility (dependent on lipid fluidity) is involved in the rate-limiting step of active calcium transport.     

Direct measurement of the internal viscosity of sickle erythrocytes as a function of cell density

The rotational dynamics of TEMPAMINE can be used to study directly the intracellular environment. The extracellular signal from TEMPAMINE is broadened away by the use of potassium ferricyanide which does not enter the cell. The EPR signal which results when 1 mM TEMPAMINE, 120 mM ferricyanide, and erythrocytes are mixed together arises from TEMPAMINE only in the intracellular aqueous space. The relative viscosity measured by the motion of TEMPAMINE in various control environments is: water at 37 degrees C = 1; human plasma at 37 degrees C = 1.1; internal aqueous environment of washed erythrocytes or whole blood at 37 degrees C = 4.92 +/- 0.32. Erythrocytes can be fractionated by density. In sickle-cell anemia (SS), the percentage of cells we find with density greater than 1.128 g/ml is 15-40%, in normals (AA) and sickle trait (AS) 1%. By direct spin-label measurements with TEMPAMINE we show, for the first time, that the relative internal viscosity (eta mu) of these dense erythrocytes is markedly elevated and density-dependent. Our results show that (1) eta mu increases with increasing cell density; (2) eta mu obtained from sickle cells is higher than eta mu obtained from normal cells at a given density, and this effect is greater at 37 degrees C than at 20 degrees C; (3) eta mu is proportional to MCHC, but eta mu in erythrocytes is higher than eta mu obtained from in vitro preparations of hemoglobin S at equivalent concentrations. We conclude that the relative internal viscosity of erythrocytes is affected by three factors: the state of cell hydration, the amount of hemoglobin polymer present, and the potential interactions of the cell membrane with intracellular hemoglobin.     

Haematoporphyrin changes the mechanical properties of lipid bilayer membranes.

The interactions between haematoporphyrin (HP) and bilayer lipid membranes (BLM) were studied. A weak effect of HP on BLM conductivity was observed at HP concentrations ranging between 10(-6) and 3 x 10(-5) mol/l. Modulus of elasticity in the direction normal to the membrane plane (E perpendicular) and dynamic viscosity coefficient (eta) were measured, both exhibiting HP-induced decrease by 22-31% in the dark. In this case, membrane potential Vm became negative and reached a value close to -50 mV. Under illumination by low-intensity (1 mW) He-Ne laser (lambda = 632 nm) the values of parameters E perpendicular and eta of the HP-modified membranes increased by 41-66%, and Vm decreased to -20 mV. Upon removing HP from the solution by perfusion, irreversible changes in mechanical properties of the HP-modified membranes induced by the laser light were observed. The reason could be the formation of stable complexes of HP with the lipid molecules. HP binds to membrane noncooperatively, with a binding constant K approximately 10(5) l/mol.     

Dynamic properties of gramicidin A in phospholipid membranes

The flexibility of the tryptophan side chains of gramicidin A and the rotational diffusion of the peptide in methanolic solution and in three membrane systems were studied with deuterium nuclear magnetic resonance (NMR). Gramicidin A was selectively deuterated at the aromatic ring systems of its four tryptophan side chains. In methanolic solution, the tryptophan residues remained immobile and served as a probe for the overall rotation of the peptide. The experimentally determined rotational correlation time of tau c = 0.6 X 10(-9) s was consistent with the formation of gramicidin A dimers. For gramicidin A incorporated into bilayer membranes, quite different results were obtained depending on the chemical and physical nature of the lipids employed. When mixed with 1-palmitoyl-sn-glycero-3-phosphocholine (LPPC) at a stoichiometric lipid:peptide ratio of 4:1, gramicidin A induced the formation of stable bilayer membranes in which the lipids were highly fluid. In contrast, the gramicidin A molecules of this membrane remained completely static over a large temperature interval, suggesting strong protein-protein interactions. The peptide molecules appeared to form a rigid two-dimensional lattice in which the interstitial spaces were filled with fluidlike lipids. When gramicidin A was incorporated into bilayers of 1,2-dioleoyl-sn-glycero-3-phosphocholine or 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) above the lipid phase transition, the deuterium NMR spectra were motionally narrowed, indicating large-amplitude rotational fluctuations. From the measurement of the quadrupole echo relaxation time, a rotational correlation time of 2 X 10(-7) s was estimated, leading to a membrane viscosity of 1-2 P if the rotational unit was assumed to be a gramicidin A dimer. (ABSTRACT TRUNCATED AT 250 WORDS)     

Influence of temperature and cholesterol on the rotational diffusion of band 3 in the human erythrocyte membrane.

Band 3 rotation in the human erythrocyte membrane is measured by observing flash-induced dichroism of eosin probes. The decay of the absorption anisotropy is found to be strongly dependent on temperature. The results are analyzed on the assumption that rotation of band 3 only occurs about the membrane normal. It is deduced that both fast and slowly rotating forms of band 3 coexist in the membrane. The equilibrium between these forms is temperature dependent, the slowly rotating species becoming increasingly dominant as the temperature is reduced. Plots of the fractional distribution of the different species against temperature show a marked change of slope at around 37--40 degrees C. The effects are essentially reversible over the range 1--45 degrees C and independent of the presence of the spectrin--actin network. The results could be due to temperature-dependent protein--protein associations mediated either by a protein conformational change or by lipid phase segregation. In further experiments, the cholesterol content of the erythrocyte membrane is varied by incubation with lipid vesicles. No significant changes in the rotational diffusion of band 3 are observed following variation of membrane cholesterol/phospholipid mole ratios over the range 0.34--1.66. This is a surprising result in view of the well-known effects of cholesterol on lipid fluidity.     

Hemorheology and oxygen transport in vertebrates. A role in thermoregulation?

We studied the effect of temperature on blood rheology in three vertebrate species with different thermoregulation and erythrocyte characteristics. Higher fibrinogen proportion to total plasma protein was found in turtles (20%) than in pigeons (5.6%) and rats (4.2%). Higher plasma viscosity at room temperature than at homeotherm body temperature was observed in rats (1.69 mPa x s at 20 degrees C vs. 1.33 mPa x s at 37 degrees C), pigeons (3.40 mPa x s at 20 degrees C vs. 1.75 mPa x s at 40 degrees C), and turtles (1.74 mPa x s at 20 degrees C vs. 1.32 mPa x s at 37 degrees C). This fact allow us to hypothesize that thermal changes in protein structure may account for an adjustment of the plasma viscosity. Blood viscosity was dependent on shear rate, temperature and hematocrit in the three species. A different behaviour in apparent and relative viscosities between rat and pigeon at environmental temperature was found. Moreover, the blood oxygen transport capacity seems more affected by a reduction of temperature in rats than in pigeons. Both findings indicate a greater influence of temperature on mammalian erythrocyte than on nucleated red cells, possibly as a consequence of differences in thermal sensitivity and mechanical stability between them. A comparison between the three species revealed that apparent blood viscosity measured at homeotherm physiological temperature was linearly related to the hematocrit level of each species. However, when measured at environmental temperature, rat blood showed a higher apparent viscosity than those found in species with non-nucleated red cells, thus indicating a higher impact of temperature decrease on blood viscosity in mammals. This suggest that regional hypothermia caused by cold exposure may affect mammalian blood rheological behaviour in a higher extent than in other vertebrate species having nucleated red cells and, consequently, influencing circulatory function and oxygen transport.     

Measuring rotational diffusion of MHC class I on live cells by polarized FPR

Clustering of membrane proteins is a dynamic process which can regulate cellular function and signaling. The size of receptor and other membrane protein clusters can in principle be measured in terms of their rotational diffusion. However, in practice, measuring rotation of membrane proteins of live cells has been difficult, largely because of the difficulty of rigidly attaching reporter groups to the molecules of interest. Here we show that polarized photobleaching recovery can detect rotation of membrane proteins genetically tagged with yellow fluorescent protein, YFP. MHC class I molecules were engineered with a rigid, in-sequence, YFP tag followed at the C-terminus by a pair of crosslinkable domains. When crosslinker was added we could detect changes in rotational anisotropy decay consistent with clustering of the MHC molecules. This result points the way to use of engineered fluorescent fusion proteins to measure rotational diffusion in native cell membranes.     

Rotational mobility of Sendai virus glycoproteins in membranes of fused human erythrocytes and in the envelopes of cell-bound virions

The rotational mobility of Sendai virus envelope glycoproteins (F, the fusion protein, and HN, the hemagglutinin/neuraminidase) was determined by using erythrosin (ER)-labeled monovalent Fab' antibody fragments directed specifically against either F or HN. By use of time-resolved phosphorescence anisotropy, the rotational mobility of Er-Fab'-viral glycoprotein complexes was studied both in the envelopes of unfused virions bound to erythrocyte ghosts and in the target cell membrane after fusion had occurred. The rotational correlation times (phi) of Er-Fab'-labeled F and HN were rather similar in the envelopes of bound unfused virions, but highly different in membranes of fused cells. The different phi values indicate that F and HN diffuse separately in the target cell membrane and for the major part are not complexed together. The temperature dependence of the phi values of the Er-Fab'-viral glycoprotein complexes revealed a breakpoint at 22 degrees C for the F protein both in bound virions and in the membranes of fused cells, and for the HN proteins in the envelopes of bound virions. In all these cases, the phi values increased between 4 and 22 degrees C, demonstrating a reduction in the rate of rotational diffusion. Further elevation of the temperature reversed the direction of the change in phi. This phenomenon may reflect a temperature-dependent microaggregation of F and HN saturating at ca. 22 degrees C and presumably related to the fusion mechanism since the breakpoint temperature correlates closely with the threshold temperature for virus-cell and cell-cell fusion.(ABSTRACT TRUNCATED AT 250 WORDS)     

Drug-induction decreases the mobility of cytochrome P-450 in rat liver microsomes: protein rotation study

Effect of drug-induction on the rotation of cytochrome P-450 and on lipid fluidity in rat liver microsomes was examined. Rotational diffusion of cytochrome P-450 was examined by observing the decay of absorption anisotropy, r(t), after photolysis of the heme.CO complex by a vertically polarized laser flash. Analysis of r(t) was based on a "rotation-about-membrane normal" model. Microsomal lipid fluidity was measured by observing fluorescence anisotropy of DPH incorporated in the lipid bilayer. The absorption anisotropy decayed within 2 ms to a time-independent value. Rotational diffusion of cytochrome P-450 was dependent on the drug-induction with PB, MC, and PCB when compared with non-induced CON-microsomes. The observed values for the normalized time-independent anisotropy r(infinity)/r(0) are r(infinity)/r(0) = 0.41 (CON-microsomes), 0.54 (PB-microsomes), 0.52 (MC-microsomes), and 0.57 (PCB-microsomes). The average rotational relaxation time phi = 580-690 microseconds was almost unchanged over all microsomes presently examined. A significantly high value of r(infinity)/r(0) = 0.41-0.57 implies the co-existence of mobile and immobile populations of cytochrome P-450. Based on the assumption that the heme tilts about 55 degrees from the membrane plane for all species of P-450s besides P-450PB, 59% (CON-microsomes), 46% (PB-microsomes), 48% (MC-microsomes), and 43% (PCB-microsomes), respectively, of the cytochrome P-450 in microsomes is calculated to be mobile. Upon drug-induction the microsomal membrane was fluidized to some extent as judged by the steady-state fluorescence anisotropy of 0.156 for CON-microsomes and 0.139-0.148 for drug-induced microsomes.(ABSTRACT TRUNCATED AT 250 WORDS)     

Rheology of biofilms formed at the surface of NF membranes in a drinking water production unit

In this study, the mechanical properties of biofilms formed at the surface of nano-filtration (NF) membranes from a drinking water plant were analysed. Confocal laser scanning microscopy observations revealed that the NF biofilms formed a dense and heterogeneous structure at the membrane surface, with a mean thickness of 32.5 +/- 17.7 mum. The biofilms were scraped from the membrane surface and analysed in rotation and oscillation experiments with a RheoStress 150 rotating disk rheometer. During rotation analyses, a viscosity decrease with speed of shearing characteristic of rheofluidification was observed (eta = 300 Pa s for y = 0.3 s(-1)). In the oscillation analyses with a sweeping of frequency (1-100 Hz), elasticity (G') ranged from 3000 to 3500 Pa and viscosity (G') from 800 to 1200 Pa. Creep curves obtained with an application of a shear stress of 30 Pa were viscoelastic in nature. The G(0) and eta values were, respectively, 1.4 +/- 0.3 x 10(3) Pa and 3.3 +/- 0.65 x 10(6) Pa s. The relationship between the characteristics of NF biofilms and the flow conditions encountered during NF is discussed.     

Interactions of triply phosphorylated human beta-casein: monomer characterization and hydrodynamic studies of self-association

The triply phosphorylated form of human beta-casein comprises about 15% of that fraction and is thus a significant component about midway between the two extremes of zero and five phosphoryls. Its partial specific volume, v, of 0.74 +/- 0.01 and absorbancy, E1% 1 cm, 280 nm, of 6.2 +/- 0.2 are almost identical to the other human beta-caseins. Equilibrium dialysis gave an average of 3.1 +/- 0.4 major Ca2+ binding sites at 37 degrees C with Kdiss = 8.6 x 10(-4) M. Sedimentation and viscosity at low temperatures or in 3.3 M urea suggested a prolate ellipsoidal monomer with 1.4 g H2O/g protein, 10 nm in length and 1.4 nm in width. The concentrated charge of the phosphoryls may be near one end of the ellipsoid, allowing the molecules to align with the flow in the viscometer at low concentration but, due to intermolecular electrostatic interactions, not when concentration is high. This would provide a reason for the heretofore unexplained curvature in the plots of reduced viscosity, eta red, vs beta-casein protein concentration. Self-association increased with temperature. At 37 degrees C in low salt buffer, s20,W was 16 S, which increased to about 33 S as ionic strength, I, was increased to 0.2 and above. At the same time, eta red in low salt buffer decreased from about 22 ml/g at 4 degrees C to a constant value of about 5 ml/g above 23 degrees C. A similar value for eta red at 37 degrees C, which was almost independent of protein concentration, was obtained at I greater than 0.25, giving an extrapolated intrinsic viscosity value of [eta] = 4.0 ml/g. Using this value and assuming a spherical aggregate, calculations suggest a radius of 9 nm with about 48 monomers and 0.86 g H2O/g protein.