Thermal stability of myosin rod from various species

The radius of gyration and fraction helix as a function of temperature have been determined for myosin rod from four different species: rabbit, frog, scallop, and antarctic fish. Measurements from sodium dodecyl sulfate gel electrophoresis indicate that all particles have the same molecular weight (approximately 130K). All fragments are nearly 100% alpha-helical at low temperatures (0-5 degrees C). The melting profiles for each are qualitatively similar in shape, but their midpoints are shifted along the temperature axis in the following order: antarctic fish (Tm = 33 degrees C), scallop (Tm = 39 degrees C), frog (Tm = 45 degrees C), and rabbit (Tm = 49 degrees C). Corresponding radius of gyration vs temperature profiles for each species are shifted to lower temperatures (approximately 5-8 degrees C) with respect to the optical rotation melting curves. From plots of radius of gyration vs fraction helix, we find a marked drop in the radius of gyration (from 43 to approximately 34 nm) with less than a 5% decrease in fraction helix for rabbit, frog, and antarctic fish rods, whereas the radius of gyration of scallop rod never exceeds 34 nm. Results indicate hinging of the myosin rod of each species. The thermal stabilities of the myosin rods shift in parallel with the working temperature of their respective muscles.     

A synchrotron X-ray scattering characterization of purified tubulin and of its expansion induced by mild detergent binding

This report presents a synchrotron radiation X-ray scattering characterization of calf brain tubulin purified by the modified Weisenberg procedure. The results show that under nonassembly conditions (i.e., in 10 mM sodium phosphate and 0.1 mM GTP, pH 7, buffer) these preparations consist of a uniform population of molecules with a radius of gyration of 3.1 +/- 0.1 nm, which can be interpreted as arising from the native alpha-beta heterodimer. The uniformity in the population persists even at unusually high concentrations of protein. Binding of colchicine or substitution of GTP by GDP does not induce, within the statistical accuracy and resolution range of our measurements, any significant structural modification in soluble tubulin. In assembly buffer [i.e., 10 mM sodium phosphate, 6 mM magnesium chloride, 1 mM [ethylenebis(oxyethylenenitrilo)]tetraacetic acid, 1 mM GTP, and 3.4 M glycerol, pH 6.5], these preparations readily assemble into microtubules upon increasing the temperature from 4 to 37 degrees C. Binding of nondenaturing amphiphiles to soluble tubulin provides a simplified model for tubulin-membrane interactions. The X-ray scattering data show that the radius of gyration of tubulin progressively increases upon binding of the mild detergent sodium deoxycholate, reaching a maximum value of 4.3 +/- 0.1 nm at detergent saturation. The relative increase in the radius of gyration coincides within experimental error with the previously determined relative increase in the frictional coefficient [Andreu, J.M., & Mu?oz, J.A. (1986) Biochemistry 25, 5220-5230]. Analysis of these observations suggests that the effect of detergent binding is to induce an isotropic swelling of the protein structure.     

Substrate binding closes the cleft between the domains of yeast phosphoglycerate kinase.

Using small angle x-ray scattering from solutions of yeast phosphoglycerate kinase, we have measured the radius of gyration of the enzyme both in the presence and in the abscence of ligands. We find that the radius of gyration decreases by 1.09 +/- 0.34 A upon binding both substrates MgATP and 3-phosphoglycerate to form the ternary complex. Smaller decreases, at the limit of the precision of the measurement, were found for the separate binding of MgATP (0.30 +/- 0.50 A). Using computer modeling, it has been estimated that a substrate-induced cleft closure in phosphoglycerate kinase resulting from one lobe rotating 8-14 degrees relative to the other lobe lobe is consistent with this observed change in radius of gyration. We suggest, therefore, that the conformational change that results in the smaller radius of gyration for the ternary complex is a hinge motion of the two lobes which produces a closing of the cleft between the two lobes. The apparent similarity of the ligand-induced change in phosphoglycerate kinase to the cleft closure in hexokinase suggests that this kind of conformational change may prove to be a rather general kinase phenomenon (Bennett, W.S., and Steitz T.A. (1978) Proc. Natl. Acad. Sci. U.S.A. 75, 4848-4852; Anderson, C.M., Zucker, F.H., and Steitz, T.A. (1979) Science 204, 375-380).     

On the conformation of serine-specific transfer RNA. Studies by small-angle X-ray scattering and ultraviolet absorption of the molecule in solution.

The scattered X-ray intensities from dilute solutions of tRNASer (yeast) in 0.1 M Soerensen buffer at pH 7.0 were measured at 25 degrees C. The radius of gyration, molecular weight and volume were determined. A model equivalent in scattering is given. The change of the conformation of tRNASer by heating was followed by small-angle X-ray measurements and ultraviolet absorption in a temperature range 20-70 degrees C. The molecule begins to unfold at about 40 degrees C and 70 degrees C has a random coil conformation. Addition of magnesium stabilizes the tRNASer molecule. The reversibility of the melting process was also studied by both methods. An interesting effect was found by ultraviolet absorption: by heating the tRNASer solutions to 55 degrees C and 60 degrees C and subsequently slowly cooling, the melting curves lie at higher absorption values than the corresponding cooling curves. The small-angle data and optical properties of tRNASer are compared with those of tRNAPhe which has already been thoroughly investigated.     

Hinging of rabbit myosin rod

The question of hinging in myosin rod from rabbit skeletal muscle has been reexamined. Elastic light scattering and optical rotation have been used to measure the radius of gyration and fraction helix, respectively, as a function of temperature for myosin rod, light meromyosin (LMM), and long subfragment 2 (long S-2). The radius of gyration vs temperature profile of myosin rod is shifted with respect to the optical rotation melting curve by about -5 degrees C. Similar studies on both LMM and long S-2 show virtually superimposable profiles. To correlate changes in the secondary structure with the overall conformation, plots of radius of gyration vs fraction helix are presented for each myosin subfragment. Myosin rod exhibits a marked decrease in the radius of gyration from 43 nm to approximately 35 nm, while the fraction helix remains at nearly 100%. LMM and long S-2 did not show this behavior. Rather, a decrease in the radius of gyration of these fragments occurred with comparable changes in fraction helix. These results are interpreted in terms of hinging of the myosin rod within the LMM/S-2 junction.     

Synchrotron radiation small angle scattering studies of thermal stability of xylanase XYNII from Trichoderma longibrachiatum

Xylanase XYNII from Trichoderma longibrachiatum is a small protein of the molecular weight 21 kDa, belonging to the family 11 of glycosyl hydrolases, which catalyses hydrolysis of xylan. This article reports thermal stability study of xylanase XYN II conformation in the temperature range 15-65 degrees C by the small angle synchrotron radiation scattering. The study has been performed at different pH conditions: at pH 4.0 (below the physiological optimum of the enzyme activity) at pH 5.8 close to the optimum for enzymatic activity and at pH 8.0. The radius of gyration and the pair distance distribution function p(r) have been analyzed to characterize the changes of the enzyme conformation on heating. In the environment of the pH close to that of the optimum for the enzymatic activity, xylanase shows the greatest thermal stability and undergoes denaturation only above 55 degrees C. In the acidic and basic environments, the enzyme stability is much lower and denaturation begins at 45 degrees C. On the basis of the SAXS data, the shape of the xylanase molecule in solution in different temperatures has been reconstructed using ab initio method and program DAMMIN. The shape of the xylanase molecule at room temperature is similar to the right hand, which is typically observed for xylanase crystal structure. In higher temperatures (close to the enzyme activity optimum), the conformation of the right hand is loosened and half opened.     

Temperature induced denaturation of collagen in acidic solution

The denaturation of collagen solution in acetic acid has been investigated by using ultra-sensitive differential scanning calorimetry (US-DSC), circular dichroism (CD), and laser light scattering (LLS). US-DSC measurements reveal that the collagen exhibits a bimodal transition, i.e., there exists a shoulder transition before the major transition. Such a shoulder transition can recover from a cooling when the collagen is heated to a temperature below 35 degrees C. However, when the heating temperature is above 37 degrees C, both the shoulder and major transitions are irreversible. CD measurements demonstrate the content of triple helix slowly decreases with temperature at a temperature below 35 degrees C, but it drastically decreases at a higher temperature. Our experiments suggest that the shoulder transition and major transition arise from the defibrillation and denaturation of collagen, respectively. LLS measurements show the average hydrodynamic radius R(h), radius of gyration R(g)of the collagen gradually decrease before a sharp decrease at a higher temperature. Meanwhile, the ratio R(g)/R(h) gradually increases at a temperature below approximately 34 degrees C and drastically increases in the range 34-40 degrees C, further indicating the defibrillation of collagen before the denaturation.     

Viscoelastic and light scattering studies on thermally induced sol to gel phase transition in fish myosin solutions

Viscoelastic (VE) and dynamic light scattering (DLS) analyses of fish (white croaker) myosin solutions were performed at myosin concentrations of 30 mg/mL for VE and 0.1 mg/mL for DLS at 0.6M KCl and pH 7.0 to clarify thermally induced gelation. The hydrodynamic radius R(h) considerably decreased around 30-35 degrees C. The shear modulus G was constant below 25 degrees C and increased by incubating the sample at 30 degrees C. G further increased as the temperature of the incubated sample decreased. The curves of G vs T for different time courses showed a sharp peak around 35 degrees C and a moderate peak around 60 degrees C in the heating process, while a stepwise increase in G was observed around 30 degrees C in the cooling process when the temperature was elevated to not more than 60 degrees C. No distinct stepwise change was observed once the temperature of the sample exceeded 60 degrees C. The absolute value of G strongly depended on the maximum elevated temperature and the incubation time at that temperature. The corresponding behavior of the viscosity eta was observed for each time course. Based on these results, the mechanism of thermally induced gelation of myosin solutions is discussed in view of S-S bridge formation in the head and tail portions and unwinding/rewinding of coiled-coil alpha-helices in the tail portion.     

Patterns of community change among ammonia oxidizers in meadow soils upon long-term incubation at different temperatures

The effect of temperature on the community structure of ammonia-oxidizing bacteria was investigated in three different meadow soils. Two of the soils (OMS and GMS) were acidic (pH 5.0 to 5.8) and from sites in Germany with low annual mean temperature (about 10 degrees C), while KMS soil was slightly alkaline (pH 7.9) and from a site in Israel with a high annual mean temperature (about 22 degrees C). The soils were fertilized and incubated for up to 20 weeks in a moist state and as a buffered (pH 7) slurry amended with urea at different incubation temperatures (4 to 37 degrees C). OMS soil was also incubated with less fertilizer than the other soils. The community structure of ammonia oxidizers was analyzed before and after incubation by denaturing gradient gel electrophoresis (DGGE) of the amoA gene, which codes for the alpha subunit of ammonia monooxygenase. All amoA gene sequences found belonged to the genus Nitrosospira. The analysis showed community change due to temperature both in moist soil and in the soil slurry. Two patterns of community change were observed. One pattern was a change between the different Nitrosospira clusters, which was observed in moist soil and slurry incubations of GMS and OMS. Nitrosospira AmoA cluster 1 was mainly detected below 30 degrees C, while Nitrosospira cluster 4 was predominant at 25 degrees C. Nitrosospira clusters 3a, 3b, and 9 dominated at 30 degrees C. The second pattern, observed in KMS, showed a community shift predominantly within a single Nitrosospira cluster. The sequences of the individual DGGE bands that exhibited different trends with temperature belonged almost exclusively to Nitrosospira cluster 3a. We conclude that ammonia oxidizer populations are influenced by temperature. In addition, we confirmed previous observations that N fertilizer also influences the community structure of ammonia oxidizers. Thus, Nitrosospira cluster 1 was absent in OMS soil treated with less fertilizer, while Nitrosospira cluster 9 was only found in the sample given less fertilizer.     

The conformation of polyriboadenylic acid at low temperature and neutral pH. A single-stranded rodlike structure.

The conformation of single-stranded polyrA in aqueous solution has been measured at temperatures down to ?12°C. The radius of gyration of low-molecular-weight polyrA varies very little with temperature in this range. By studying the dependence of radius of gyration on temperature for several polyrA fractions, we show that the dependence of the radius upon chain length is consistent with formation of a single-stranded rodlike structure at low temperature. The structure has an approximate length of 3.2 Å/nucleotide.     

Laser light-scattering characterization of mitochondrial complex III-Triton X-100-phospholipid mixed micelles

Bovine-heart mitochondrial complex III was purified in the presence of Triton X-100, and the size and shape of the resulting protein-surfactant-phospholipid mixed micelles were investigated by laser light-scattering. The protein appears to be present in the form of a dimer, irrespective of temperature (between 25 and 40 degrees C) and protein concentration (between 0.5 and 5 mg/ml). The molecular weight of the micelle increases with temperature from 600 000 (25 degrees C) to 692 000 (40 degrees C). The variation of the solvent second virial coefficient in this temperature range suggests that, with increasing temperature, some of the free surfactant molecules become integrated in the mixed micelles. The average quadratic radius of gyration of these is of 42 +/- 5 nm, corresponding in our case to an ellipsoidal shape.     

Thermally induced conformation change of succinoglycan in aqueous sodium chloride

Static and dynamic light scattering, viscosity, and optical rotation measurements have been made at eight different temperatures between 25 and 75 degrees C on two succinoglycan samples (sodium salt) with weight-average molecular weights M(w) of 7.14 x 10(5) and 3.54 x 10(5) (at 25 degrees C) in 0.01 M aqueous NaCl to investigate the thermally induced order-disorder conformation change of the polysaccharide. Additionally, viscometry and polarimetry have been performed for a sodium salt sample (M(w) = 4.55 x 10(5) at 25 degrees C) whose M(w), z-average radius of gyration (z)(1/2), and hydrodynamic radius R(H) in the aqueous salt had been determined previously. As the temperature increases, M(w), (z)(1/2), R(H), and the intrinsic viscosity for every sample sharply decrease around 55 degrees C where the specific rotation at 300 nm sigmoidally increases. In particular, M(w) at 25 degrees C (i.e., in the ordered helical state) is twice as large as that at 75 degrees C (i.e., in the disordered state). These findings substantiate that the ordered structure is composed of two chains and hence is a double helix. Data analysis shows that this helix at 25 degrees C is characterized by an unperturbed wormlike chain with a helix pitch of about 2 nm (per repeating unit) and a persistence length of about 50 nm and that upon heating, it dissociates directly (i.e., in all-or-none fashion) to disordered chains of a similar contour length but with a much smaller persistence length of about 10 nm. The temperature dependence of the light scattering second viral coefficient is discussed in relation to the association of disordered chains in the cooling process.     

Asymmetrical-flow field-flow fractionation with on-line multiangle light scattering detection. 1. Application to wormlike chain analysis of weakly stiff polymer chains

Four samples of hyaluronan in the sodium form, ranging in weight-average molecular weight, M(w), from 6.67 x 10(5) to 4.23 x 10(6) were investigated by asymmetrical-flow field-flow fractionation coupled to multiangle light scattering (FlFFF-MALS) in 0.2 M aqueous NaCl at 25 degrees C. M(w) and z-average radii of gyration, R(G)(z)(), obtained via FlFFF-MALS showed a good agreement with the results obtained by conventional static light scattering. Furthermore, the molecular weight dependence of the radius of gyration for sodium hyaluronan obtained via FlFFF-MALS was analyzed on the basis of the Kratky-Porod model for unperturbed wormlike chains combined with the Yamakawa theory for radius expansion factor, and a sufficiently good agreement was observed between the theoretical prediction and experimental data. These results show the potential usage of FlFFF-MALS regarding size separation and molecular characterization even for weakly stiff chains.     

SEC-MALS characterization of microbial polyhydroxyalkanoates

Characterization of poly-3-hydroxybutyric acid (PHB) and poly-3-hydroxybutyric-co-valeric acid (PHBV, 13% valerate) in chloroform was performed using size exclusion chromatography coupled to a multi-angle light scattering detector (SEC-MALS). Absolute molar mass averages, molar mass distribution, and the radius of gyration were determined. Three sample preparation methods were examined: dissolution in chloroform (1) at room temperature, (2) at 60 degrees C, and (3) after thermal pretreatment of samples (annealing at 180 degrees C with subsequent quenching in liquid nitrogen). Dissolution at 60 degrees C and dissolution of thermally pretreated samples gave molecularly dissolved PHB and PHBV. At 60 degrees C using acid free chloroform, there was no indication of degradation for up to 120 min dissolution time, whereas thermal degradation of polymers did take place during annealing at 180 degrees C. The degradation rate constants for number and weight average degree of polymerization at 180 degrees C were slightly higher for PHB (5.19 x 10(-5) min(-1), 4.95 x 10(-5) min(-1)) than for PHBV (4.99 x 10(-5) min(-1), 4.54 x 10(-5) min(-1)). The dependence of the radii of gyration on molar mass showed that both polymers form random coils in chloroform. The relationship between the absolute molar masses and relative SEC results was determined. DSC and NMR characterization also gave evidence of the progress of degradation.     

Studies of alpha- and betaL-crystallin complex formation in solution at 60 degrees C

Studies of molecular mechanisms of chaperone-like activity of alpha-crystallin became an active field of research over last years. However, fine interactions between alpha-crystallin and the damaged protein and their complex organization remain largely uncovered. Complexation between alpha- and betaL-crystallins was studied with thermal denaturation of betaL-crystallin at 60 degrees C using small-angle X-ray scattering (SAXS), light scattering, gel-permeation chromatography and electrophoresis. A mixed solution of alpha- and betaL-crystallins in concentrations about 10 mg/ml incubated at 60 degrees C was found to contain their soluble complexes with mean radius of gyration approximately 14 nm, mean molecular weight approximately 4000 kDA and maximal size approximately 40 nm. In pure betaL-crystallin solution, complexes were not observed at 60 degrees C. In SAXS studies, transitions in the alpha-crystallin quaternary structure at 60 degrees C were shown to occur and result in a double increase of the molecular weight. It suggests that during the temperature-induced denaturation of betaL-crystallin it binds with modified alpha-crystallin or, alternatively, alpha-betaL-crystallin complexation and alpha-crystallin modifications are concurrent. Estimates of the alpha-betaL-crystallin dimensions and relative contents of alpha- and betaL-crystallins in the complex suggest that several alpha-crystallin molecules are involved in complex formation.     

Resonance energy transfer study of membrane-bound aggregates of the sarcoplasmic reticulum calcium ATPase

The aggregation of the membrane-bound calcium ATPase from sarcoplasmic reticulum has been studied by resonance energy transfer. The temperature dependence of resonance energy transfer from a fluorescent membrane lipid donor to an acceptor covalently linked to the Ca2+ ATPase was observed for the native sarcoplasmic reticulum vesicles and for purified protein reconstituted into phospholipid vesicles. The efficiency of energy transfer in these systems increases as the size of protein aggregates decrease. This is due to the increased exposure of the protein in the lipid domain that results in the shortening of distances between donors and acceptors. The degree of aggregation was observed to decrease with increasing temperature. Aggregates rea h a limiting size at low temperature (5 degrees C) but not a high temperatures (45 degrees C). For the reconstituted system, the aggregate size showed a continuous, smooth decrease with increasing temperature. Sarcoplasmic reticulum vesicles showed a decrease in aggregation except for a region from 20 to 30 degrees C in which no change occurred. Arrhenius plots of the calcium transport activities for both systems do not reflect these differences, but instead show similar discontinuities and activation energies. A theoretical model is used to analyze the resonance energy transfer results for the reconstituted vesicles. The average radius of the ATPase aggregate is obtained from this analysis. The limiting, low temperature value of the aggregate radius is consistent with the formation of a tetramer. This structure breaks down to smaller, functional units at higher temperatures.     

α-Helical burst on the folding pathway of FHA domains from Rad53 and Ki67

We investigated refolding processes of β-sheeted protein FHA domains (FHA1 domain of Rad53 and Ki67 FHA domain) by cryo-stopped-flow (SF) method combined with far-ultraviolet (far-UV) circular dichroism (CD, the average secondary structure content) and small angle X-ray scattering (SAXS, measuring the radius of gyration). In case of FHA1 domain of Rad53, no detectable time course was observed except the initial burst on its refolding process at 4 °C, suggesting that the FHA1 domain of Rad53 was already refolded to its native state within the dead time of the SF apparatus and the rate of the refolding is too fast to be observed at this temperature. In contrast, there was an observable α-helical burst at −15 °C and −20 °C in the presence of 45% ethylene glycol (EGOH) by CD-SF. Besides, the radius of gyration (Rg) of the burst phase intermediate at −20 °C shows the intermediate is already compact, and the compaction process was accompanied with the decrease of α-helical content at the same temperature.     

Structural characterization of lactate dehydrogenase dissociation under high pressure studied by synchrotron high-pressure small-angle X-ray scattering.

The effect of high pressure on lactate dehydrogenase (LDH) was studied using small-angle X-ray scattering (SAXS). The SAXS results are interpreted in terms of the dissociation and association of LDH within a compression and decompression cycle and its temperature dependence. LDH consists of four identical subunits. At 120 MPa and 25 degrees C, 50% of the LDH dissociates into subunits, while at 10 degrees C, this occurs at 78 MPa. The hysteresis in the dissociation and association under pressure was confirmed in terms of the radius of gyration and was seen to be more conspicuous at low temperature. Forward scattering, I(0)/C, which is proportional to molecular weight, showed that LDH dissociated into dimer (not monomer) subunits under pressure. The application of high pressure to dissociated dimers induced irreversible aggregation. This result is in sharp contrast with the result of fluorescence spectroscopy suggesting a dissociated monomer [King, L., and Weber, G. (1986) Biochemistry 25, 3637-3640]. As for structural change after reassociation, there was little structural difference between native and drifted LDH. The difference was smaller than the structure change by ligand binding. At 200 MPa, the presence of five scattering peaks in the medium-angle region indicates that the dissociated dimer does not have a molten globule-like structure but a core structure. We propose a model of the dissociated dimer, based on the SAXS profile, in which the volume is reduced without disrupting the core structure.     

Conformation of hyaluronate in neutral and alkaline solutions

Increasing the pH of a neutral salt solution of sodium hyaluronate to 12.5 produces a rapid drop in viscosity which is reversible upon restoring the pH to neutrality. Light scattering data showing a decrease in radius of gyration with no change in molecular weight and negative results with chondroitin and other acidic glycosaminoglycans suggest that the conformational change is specific for hyaluronate molecules.     

Conformation of hyaluronate in neutral and alkaline solutions.

Increasing the pH of a neutral salt solution of sodium hyaluronate to 12.5 produces a rapid drop in viscosity which is reversible upon restoring the pH to neutrality. Light scattering data showing a decrease in radius of gyration with no change in molecular weight and negative results with chondroitin and other acidic glycosaminoglycans suggest that the conformational change is specific for hyaluronate molecules.