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Electrophoretic and hydrodynamic properties of duplex ribonucleic acid molecules transcribed in vitro: evidence that A-tracts do not generate curvature in RNA.

We have developed a T7 RNA polymerase based transcription system for the production of fully complementary RNA molecules (i.e., molecules capable of forming blunt-ended duplex species) as the direct products of transcription, thus rendering unnecessary the enzymatic removal of single-stranded ends. A combined gel electrophoretic and hydrodynamic analysis of a 180 bp double-stranded (ds) RNA molecule containing four A5-tracts in approximate phase coherence with the helix repeat provides no indication that the helix axis is curved, in sharp contrast to DNA molecules containing phased A-tracts. The electrophoretic behavior of dsRNA molecules reveals that their mobilities in nondenaturing acrylamide gels are approximately 10-20% lower than the corresponding mobilities of duplex DNA, in accord with earlier observations in the literature. Furthermore, the relative mobilities are only slightly modulated by gel concentration, the concentration of monovalent salt, or the presence of spermidine and/or Mg2+. The reduced mobilities are not caused by increased contour length, since direct hydrodynamic measurements using transient electric birefringence indicate that the average helix rise, h, of the dsRNA molecules examined in the current study is 2.8 +/- 0.1 A/bp. The reduced electrophoretic mobilities, extrapolated to zero acrylamide concentration, are consistent with the lower residual charge predicted for dsRNA by counterion condensation theory. Finally, birefringence measurements indicate that dsRNA is only marginally stiffer than DNA, with a persistence length of ca. 500-700 A.

Base Sequence↗

Hydrodynamic properties of the gonadotropin receptor from a murine Leydig tumor cell line are altered by desensitization.

The murine Leydig tumor cell line 1 (MLTC-1) contains gonadotropin receptors (GR) that are coupled to adenylate cyclase through the stimulatory guanine nucleotide binding protein (Gs). The binding of human choriogonadotropin (hCG) causes MLTC-1 cells to accumulate cAMP. With time, the ability of MLTC-1 cells to respond to hCG is attenuated by a process called desensitization. The hydrodynamic properties of GR from control and desensitized MLTC-1 cells were studied. Sucrose density gradient sedimentation in H2O and D2O and gel filtration chromatography were used to estimate the Stokes radius (a), partial specific volume (vc), sedimentation coefficient (S20,w), and molecular weight (Mr) of the detergent-solubilized hormone-receptor complex (hCG-GR). [125I]hCG was bound to MLTC-1 cells under conditions that allow (37 degrees C) or prevent (0 degree C) desensitization, and hCG-GR was solubilized in Triton X-100. In the absence of desensitization, control hCG-GR had a Mr of 213,000 (a = 6.2; vc = 0.76; S20,w = 7.3), whereas desensitized hCG-GR had a Mr of 158,000 (a = 6.1; Vc = 0.71; S20,w = 6.6). Deglycosylated hCG (DG-hCG) is an antagonist that binds to GR with high affinity but fails to stimulate adenylate cyclase or cause desensitization. [125I]DG-hCG was bound to MLTC-1 cells and DG-hCG-GR solubilized in Triton X-100. The hydrodynamic properties of DG-hCG-GR (Mr 213,000; a = 5.8; Vc = 0.77; S20;w = 7.6) were the same as that for control hCG-GR. There was no evidence for the association of adenylate cyclase or Gs with GR in Triton X-100 solubilized preparations.(ABSTRACT TRUNCATED AT 250 WORDS)

Adenylyl Cyclases↗

Conformation of myosin in dilute solution as estimated from hydrodynamic properties.

On the basis of the current knowledge of the structure and dimensions of myosin and its parts, we analyze available data on hydrodynamic properties (translational diffusion, rotational diffusion, and intrinsic viscosity) for comparison with values calculated for models with varying geometry. Special attention is paid to detecting flexibility effects in those properties. After obtaining a plausible model for subfragment S-1, we concentrate on the conformation of the rodlike parts of myosin. Although uncertainties in the experimental values do not allow a rigorous, quantitative analysis, we show how hydrodynamic data provide evidence for the flexibility of the rod at the joint of subfragment S-2 and light meromyosin.

Chemical Phenomena↗

Conformation of Escherichia coli ribosomal protein L7/L12 in solution: hydrodynamic, spectroscopic, and conformation prediction studies.

The conformation of Escherichia coli ribosomal protein L7/L12 in solution has been studied using spectroscopic and hydrodynamic methods. Circular dichroism studies in the near-ultraviolet region reveal two bands at 262 and 268 nm originating from the tertiary conformational environment of the phenylalanyl residues. Additional characterization of the phenylalanine environment includes an intrinsic fluorescence emission spectrum arising from the phenylalanine fluorophores. Computer analysis of the far-ultraviolet circular dichroism spectrum suggests that L7/L12 contains as much as approximately 76% alpha helix. Hydrodynamic properties of L7/L12, measured with the purpose of providing relevant shape information, include the frictional coefficient ratio (1.84 +/- 0.03) and intrinsic viscosity (28 +/- 0.4 mL/g). The experimentally determined frictional coefficient (6.15 +/- 0.15 X 10(-8) has been compared with theoretical calculations of the same value employing two independent methods and assuming various dimensions for the L7/L12 dimer. Combining the experimental results from this work with those available from the literature, and using conformation predictive methods of Chou & Fasman [P. Y. Chou & G. D. Fasman (1974) Biochemistry 13, 211-222, 222-245] and of Maxfield & Scheraga (F. R. Maxfield & H. A. Scheraga (1976) Biochemistry 15, 5138-5153), several possible molecular models of the L7/L12 dimer have been constructed and critically examined. A model which is consistent with all of the available data is proposed.

Cell Fractionation↗

The shape of myosin subfragment-1. A equivalent oblate ellipsoid model based on hydrodynamic properties.

The molecular weights of the two heads of myosin subfragment-1, S-1(A1) and S-1(A2), based on sedimentation equilibrium are 120 000 and 110 000. Hydrodynamically, the two heads are indistinguishable, with intrinsic viscosity, [eta], of 0.064-0.065 dL/g and sedimentation coefficient, s(0)20,w, of 5.8 S. Together with the rotational correlation time taken from the literature (235 ns), all three hydrodynamic properties can be better fitted with an equivalent oblate ellipsoid of revolution than a prolate model. The width of the equatorial axis of the ellipsoid is about 135 A (the axial ratio is about 6). Probably, the S-1(A1) and S-1(A2) molecules have a half-doughnutlike or a flattened pearlike shape rather than an elongated one.

Animals↗

Hydrodynamic properties and quaternary structure of the 90 kDa heat-shock protein: effects of divalent cations.

The 90 kDa heat-shock protein (Hsp90) is one of the major stress proteins whose overall structure remains unknown. In this study, we investigated the influence of divalent cations Mg(2+) and Ca(2+) on the hydrodynamic properties and quaternary structure of Hsp90. Using analytical ultracentrifugation, size-exclusion chromatography, and polyacrylamide gel electrophoresis, we showed that native Hsp90 was mostly dimeric. The Hsp90 dimer had a sedimentation coefficient, s(w,20) degrees, of 6.10 +/- 0.03 S, which slightly deviated from the hydrodynamics of a globular protein. Using chemical cross-linking and analytical ultracentrifugation, we showed that Mg(2+) and Ca(2+) induced a tertiary conformational change of Hsp90, leading to a self-association process. In the presence of divalent cations, Hsp90 existed as a mixture of monomers, dimers, and tetramers at equilibrium. Finally, to identify Hsp90 domains involved in this divalent cation-dependent self-association, we studied the oligomerization state of the N-terminal (positions 1-221) of Hsp90, the influence of an N-terminal specific ligand, geldanamycin (GA), and the effect of C-terminal truncation on the ability of Hsp90 to oligomerize in the presence of divalent cations. We previously showed that GA inhibits Hsp90 heat-induced oligomerization [Garnier, C., Protasevich, I., Gilli, R., Tsvetkov, P., Lobachov, V., Peyrot, V., Briand, C., and Makarov, A. (1998) Biochem. Biophys. Res. Commun. 249, 197-201], but now we observed that GA does not influence divalent cation-dependent oligomerization of Hsp90, suggesting another mechanism. This mechanism involved the C-terminal part of the protein since C-terminally truncated Hsp90 did not oligomerize in the presence of divalent cations.

Animals↗

Structural dynamics of the alpha-neurotoxin-acetylcholine-binding protein complex: hydrodynamic and fluorescence anisotropy decay analyses.

The three-fingered alpha-neurotoxins have played a pivotal role in elucidating the structure and function of the muscle-type and neuronal alpha7 nicotinic acetylcholine receptors (nAChRs). To advance our understanding of the alpha-neurotoxin-nAChR interaction, we examined the flexibility of alpha-neurotoxin bound to the acetylcholine-binding protein (AChBP), which shares structural similarity and sequence identities with the extracellular domain of nAChRs. Because the crystal structure of five alpha-cobratoxin molecules bound to AChBP shows the toxins projecting radially like propeller "blades" from the perimeter of the donut-shaped AChBP, the toxin molecules should increase the frictional resistance and thereby alter the hydrodynamic properties of the complex. alpha-Bungarotoxin binding had little effect on the frictional coefficients of AChBP measured by analytical ultracentrifugation, suggesting that the bound toxins are flexible. To support this conclusion, we measured the anisotropy decay of four site-specifically labeled alpha-cobratoxins (conjugated at positions Lys(23), Lys(35), Lys(49), and Lys(69)) bound to AChBP and free in solution and compared their anisotropy decay properties with fluorescently labeled cysteine mutants of AChBP. The results indicated that the core of the toxin molecule is relatively flexible when bound to AChBP. When hydrodynamic and anisotropy decay analyses are taken together, they establish that only one face of the second loop of the alpha-neurotoxin is immobilized significantly by its binding. The results indicate that bound alpha-neurotoxin is not rigidly oriented on the surface of AChBP but rather exhibits segmental motion by virtue of flexibility in its fingerlike structure.

Animals↗

Organization of human interferon gamma-heparin complexes from solution properties and hydrodynamics.

Heparan sulfate (HS) recognizes a variety of proteins, one of which is the pleiotropic cytokine IFN-gamma, and as such modulates many biological processes. IFN-gamma is a homodimer with a well-defined core and two flexible C-termini that constitute HS binding domains. We show here using molecular modeling that an extended IFN-gamma structure overlaps a HS fragment of 16 disaccharides (16 nm). Since a 21-24-disaccharide HS fragment was experimentally defined as the minimum size that interacts with IFN-gamma [Lortat-Jacob, H., Turnbull, J. E., and Grimaud, J. A. (1995) Biochem. J. 310 (Part 2), 497-505], this raises the question of the complexe organization. We combine analytical ultracentrifugation, size exclusion chromatography, and hydrodynamic bead modeling to characterize the complexes formed in solution with heparin oligosaccharides. For oligosaccharides of 14 and 20 nm, two types of complexes are formed with one IFN-gamma and one or two heparin molecules. Complexes consisting of two IFN-gamma and one or two heparin molecules are present for a fragment of 25 nm and aggregates for a fragment of 35 nm. The complexes are rather compact and can be formed without major conformational changes of the partners. The complex pattern of interaction is related to the size of the partners and their multiple binding possibilities. These various possibilities suggest networks of interactions at the crowded surface of the cells. Hydrodynamic methods used here proved to be very efficient tools for describing protein-HS complexes that, due to the intrinsic heterogeneity and flexibility of the partners, are otherwise very difficult to analyze.

Chromatography, Gel↗

Subunit composition of the peripherin/rds-rom-1 disk rim complex from rod photoreceptors: hydrodynamic evidence for a tetrameric quaternary structure.

Peripherin/rds and rom-1 are homologous integral membrane protein subunits found as an oligomeric complex at the rim regions of rod and cone photoreceptor outer segment disks. These proteins are essential for the morphogenesis of normal outer segments and have been linked to a variety of human retinal degenerative diseases. Previous studies have suggested that disulfide-linked homodimers of peripherin/rds and rom-1 can associate noncovalently to form higher order structures. We have characterized the hydrodynamic properties of Triton X-100 solubilized peripherin/rds-rom-1 complexes from bovine ROS membranes by gel exclusion chromatography on Sepharose C1-6B and velocity sedimentation through H2O- and D2O-based sucrose gradients. A single hydrodynamic species is observed which has a Stokes radius of 6.2 nm, a sedimentation coefficient (S20,w) of 5.8 S, and a partial specific volume of 0.83 mL/g. From these data the molecular mass of the detergent-peripherin/rds-rom-1 complex is calculated to be 240 kDa. The protein component of this complex is estimated to be 135 kDa, providing direct evidence that the solubilized peripherin/rds-rom-1 complex is a tetramer. The abundance of this complex as measured by competitive ELISA and immunoaffinity purification is approximately 4% of total bovine ROS membrane protein and indicates that peripherin/rds-rom-1 tetramers are present at a relatively high average surface density (ca. 4100/ microns m2) at the rim surfaces of rod outer segment disks.

Animals↗

The hydrodynamics of a Graesser ("raining bucket") contactor with a reverse micellar phase.

A variety of contactor types have been assessed for the liquid-liquid extraction of proteins using reversed micelles; however, many of these contactors suffer from drawbacks such as emulsion formation and poor mass transfer performance. In this study, a small (1.25 L) Graesser "raining bucket" contactor was assessed for use with this system since it has the potential to ameliorate many of these problems. The aim of the work was to evaluate the hydrodynamics of the contactor in order to use this information for future work on mass transfer performance. Hydrodynamic characteristics such as the axial mixing coefficient were determined by residence time distribution studies using a tracer injection method. The effect of rotor speed and flow rate of each phase on axial mixing was investigated, and as a result of its unusual structure, i.e., falling/rising sheet, the interfacial mass transfer area in the Graesser was determined by image analysis. It was found that rotor speed had more influence on the axial mixing coefficient in the aqueous phase than in the reverse micellar phase. The axial mixing coefficient in each phase increased by increasing the flow rate of the same phase. The images obtained in a dropping cell showed that under the conditions of this study (3 rpm, 22 degrees C), the bucket pours one phase through the other in the form of a curtain or sheet. A new image technique was developed to determine the interfacial area of both phases, and it was found that the specific area was 8.6 m(2)/m(3), which was higher than in a spray column but considerably lower than in a RDC or a Graesser run at high rotational speed (50 rpm) without the addition of a surfactant.

Equipment Design↗

Combined effect of hydrodynamic and interfacial flow parameters on lysozyme deactivation in a stirred tank bioreactor.

The dynamic environment within a bioreactor and in the purification equipment is known to affect the activity and yield of enzyme production. The present research focuses on the effect of hydrodynamic flow parameters (average energy dissipation rate, maximum energy dissipation rate, average shear rate, and average normal stress) and the interfacial flow parameters (specific interfacial area and mass transfer coefficient) on the activity of lysozyme. Flow parameters were estimated using CFD simulation based on the k-epsilon approach. Enzyme deactivation was investigated in 0.1, 0.3, 0.57, and 1 m i.d. vessels. Enzyme solution was subjected to hydrodynamic stress using various types of impellers and impeller combinations over a wide range of power consumption (0.03 < P(G)/V < 7, kW/m3). The effects of tank diameter, impeller diameter, blade width, blade angle, and the number of blades on the extent of deactivation were investigated. At equal value of P(G)/V, epsilon(max), and gamma(avg), the extent of deactivation was dramatically different for different impeller types. The extent of deactivation was found to correlate well with the average turbulent normal stress and the mass transfer coefficient.

Bioreactors↗

Efficient, accurate calculation of rotational diffusion and NMR relaxation of globular proteins from atomic-level structures and approximate hydrodynamic calculations.

The calculation of the rotational diffusion tensor and NMR relaxation times of quasi-rigid macromolecular structures with atomic detail can be made by means of bead/shell models. The computing time required for calculation of these properties for a single structure using rigorous hydrodynamic methods requires a moderate computing time. In possible applications of the methodology in which such a calculation had to be repeated for many structures, a faster method would be welcome. We have studied the effect of introducing a simplifying approximation in the treatment of hydrodynamic interaction, comparing the rigorous and approximate results for a set of 30 globular proteins. When the NMR relaxation times are combined in some relative form, the rigorous and approximate results are practically coincident. For absolute quantities, such as the correlation time, we find that the bias introduced by the approximation can be closely predicted and corrected. The differences between the results of the approximate-corrected and rigorous procedures are not greater than usual experimental errors, and the typical computing time is reduced from 5 min to 1 s.

Nitrogen Isotopes↗

Hydrodynamics of nearly smooth granular gases.

Hydrodynamic equations of motion for a monodisperse collection of nearly smooth homogeneous spheres have been derived from the corresponding Boltzmann equation, using a Chapman-Enskog expansion around the elastic smooth spheres limit. Because in the smooth limit the rotational degrees of freedom are uncoupled from the translational ones, it turns out that the required hydrodynamic fields include (in addition to the standard density, velocity, and translational granular temperature fields) the (infinite) set of number densities, n(s,r, t), corresponding to the continuum of values of the angular velocities. The Chapman-Enskog expansion was carried out to high (up to 10th) order in a Sonine polynomial expansion by using a novel computer-aided method. One of the consequences of these equations is that the asymptotic spin distribution in the homogeneous cooling state for nearly smooth, nearly elastic spheres, is highly non-Maxwellian. The simple sheared flow possesses a highly non-Maxwellian distribution as well. In the case of wall-bounded shear, it is shown that the angular velocity injected at the boundaries has a finite penetration length.

Journal Article↗

A self-consistent field quantum hydrodynamic approach for molecular clusters.

We present a novel self-consistent orbital-free method useful for quantum clusters. The method uses a hydrodynamical approach based on the de Broglie-Bohm description of quantum mechanics to satisfy an orbital-free density functional-like Euler-Lagrange equation for the ground state of the system. In addition, we use an information theoretical approach to obtain the optimal density function derived from a series of statistical sample points in terms of density approximates. These are then used to calculate an approximation to the quantum force in the hydrodynamic description. As a demonstration of the utility and flexibility of the approach, we compute the lowest-energy structures for small rare-glass clusters of argon and neon with 4, 5, 13, and 19 atoms. Extension to more complex systems is straightforward.

Journal Article↗

Thin film drainage: hydrodynamic and disjoining pressures determined from experimental measurements of the shape of a fluid drop approaching a solid wall.

Accurate measurements of the shape of a mercury drop separated from a smooth flat solid surface by a thin aqueous film reported recently by Connor and Horn (Faraday Discuss. 2003, 123, 193-206) have been analyzed to calculate the excess pressure in the film. The analysis is based on calculating the local curvature of the mercury/aqueous interface, and relating it via the Young-Laplace equation to the pressure drop across the interface, which is the difference between the aqueous film pressure and the known internal pressure of the mercury drop. For drop shapes measured under quiescent conditions, the only contribution to film pressure is the disjoining pressure arising from double-layer forces acting between the mercury and mica surfaces. Under dynamic conditions, hydrodynamic pressure is also present, and this is calculated by subtracting the disjoining pressure from the total film pressure. The data, which were measured to investigate the thin film drainage during approach of a fluid drop to a solid wall, show a classical dimpling of the mercury drop when it approaches the mica surface. Four data sets are available, corresponding to different magnitudes and signs of disjoining pressure, obtained by controlling the surface potential of the mercury. The analysis shows that total film pressure does not vary greatly during the evolution of the dimple formed during the thin film drainage process, nor between the different data sets. The hydrodynamic pressure appears to adjust to the different disjoining pressures in such a way that the total film pressure is maintained approximately constant within the dimpled region.

Journal Article↗

Unwinding and hydrodynamic flow linear dichroism characteristics of supercoiled DNA covalently modified with two isomeric methylchrysene diol epoxides of different biological activities.

Adducts derived from the covalent binding of two positional monomethyl-substituted isomers of a bay region chrysene diol epoxide to supercoiled pIBI30 DNA (2926 base pairs/genome) were prepared, and their characteristics were investigated by a combination of gel electrophoresis and flow linear dichroism techniques. The 5- and 6-methyl derivatives of trans-1,2-dihydroxy-anti-3,4-epoxy-1,2,3,4-tetrahydrochrysene [(+)-5- and (+)-6-MeCDE, respectively], both with 1R,2S,3S,4R stereochemistry, are characterized by significant differences in their biological activities [Melikian et al. (1988) Cancer Res. 48, 1781-1787]. When covalently bound to plasmid DNA, these two molecules give rise to striking differences in the gel electrophoretic and flow hydrodynamic characteristics of the modified supercoiled DNA. The hydrodynamic flow linear dichroism of linearized DNA molecules (obtained by EcoRI enzyme digestion of covalently closed supercoiled pIBI30 DNA), modified covalently with the highly tumorigenic and mutagenic (+)-5-MeCDE derivative, indicates that flexible joints, bends, or kinks are formed at the site of binding of (+)-5-MeCDE. Slab gel data, as well as ethidium bromide-titration tube agarose gel electrophoresis data, indicate that the formation of (+)-5-MeCDE-DNA lesions causes the removal of superhelical turns with an unwinding angle of 13 +/- 3 degrees per covalently bound polycyclic aromatic residue. In contrast, the biological inactive (+)-6-MeCDE does not significantly alter the characteristics of supercoiled DNA, the unwinding angle is only 2.7 +/- 1 degrees, and the changes in persistence lengths detected by the flow linear dichroism technique are significantly smaller than in the case of (+)-5-MeCDE-DNA adducts.(ABSTRACT TRUNCATED AT 250 WORDS)

Chemical Phenomena↗

Hydrodynamic model of heat stroke.

This work presents an hydrodynamical model of heat stroke, which is a physiopathological state of stress, due to an exposure of animals to an ambient temperature of approximatively 40 degrees C during two hours. The evolution of body temperature during this stress process is characterised by three phases. A first phase of increase is followed by a plateau which occurs before a second phase of increase which can be lethal. The model is based on the analogy of a boat progressively caught in a whirlpool. The evolution of the degree of freedom lost by the boat is mathematically analysed and this study leads to the same three phases. The theoretical curves calculated during this study are well in agreement with the experimental curves obtained with animals. This analogy is compared to a previous one which has been made during another experiment with animals constrained by chemical intoxications. It seems that stress can be considered as a vital vorticity and that hydrodynamic models are powerful tools in understanding this physiopathological state.

Animal Testing Alternatives↗

Evidence against a hydrodynamic function for fish schools.

THERE are numerous explanations for the formation of fish schools(1,2), one of the most popular being that the members gain hydrodynamic advantage over solitary individuals(3-6). The model proposed by Weihs(5,6) for the first time makes precise predictions about school structure which can be verified. We report here the first empirical test of this model, and demonstrate that three species of schooling fish do not swim in appropriate positions to gain hydrodynamic advantage.

Journal Article↗