RESUMEN
This study addresses the general mechanisms whereby the major cytoplasmic proteins from the adult bovine lens contribute both to transparency and maintenance of the refractive index gradient across the lens. Colloid osmotic properties and quaternary structure were measured for alpha- and beta-crystallins isolated from the steer lens, including low-molecular-weight crystallins from the cortex (alpha Le and beta L) and nucleus (alpha Ln) and high-molecular-weight crystallins from the nucleus (alpha H and beta H). In electron microscopic images of rotary-shadowed preparations alpha Le appears as spherical particles 16 nm in diameter, alpha Ln appeared as individual spheres or small aggregates of spherical subunits, alpha H contained large irregular aggregates as large as 180 nm, and both beta L and beta H appeared as elliptical particles of 7-9 nm diameter. Secondary osmometry showed that for all these crystallins colloid osmotic pressure increased monotonically in a non-linear fashion with protein concentration. For the alpha-crystallins, osmotic pressure rose more steeply with concentration for alpha Le than for either alpha Ln or alpha H, so that at 0.3 g ml-1 at 0.1 M ionic strength, the colloid osmotic pressure of alpha Le, alpha Ln and alpha H were approximately 2.6 x 10(5) dyn cm-2, 1.6 x 10(5) dyn cm-2 and 1.0 x 10(5) dyn cm-2, respectively. In a similar manner, osmotic pressure rose more steeply with concentration of beta L than for beta H, so that at 0.3 g ml-1 at 0.1 M ionic strength the colloid osmotic pressures of beta L and beta H were 2.6 x 10(5) dyn cm-2 and 1.1 x 10(5) dyn cm-2, respectively. The osmotic pressure of alpha Le dropped as ionic strength was increased from 0.02 to 0.4 M. For beta L and beta H, osmotic pressure dropped as ionic strength was increased from 0.02 to 0.1 M but was nearly the same at 0.1 M and 0.4 M ionic strength. The data for steer alpha Ln and beta H were similar to previous reports for calf cortical alpha L and beta-crystallins, respectively. The osmotic pressure isotherms for alpha Le, beta L and that previously reported for steer cortical extract were nearly identical, whereas the nuclear crystallins (alpha Ln, alpha H or beta H) generated slightly higher pressures than those previously reported for steer nuclear crystallin extracts. In all cases, osmotic pressure rose more steeply with concentration for the cortical crystallins than for the nuclear crystallins.(ABSTRACT TRUNCATED AT 400 WORDS)
Asunto(s)
Cristalinas/química , Animales , Bovinos , Cristalinas/ultraestructura , Corteza del Cristalino/química , Núcleo del Cristalino/química , Masculino , Microscopía Electrónica , Modelos Químicos , Peso Molecular , Concentración Osmolar , Presión Osmótica , Conformación Proteica , RefractometríaRESUMEN
We report the magnetic field dependence of 1/T1 of solvent water protons and deuterons (nuclear magnetic relaxation dispersion, or NMRD, profiles) for solutions of steer lens beta L-crystallin. Such data allow the study of intermolecular protein interactions over a wide concentration range, here 1-34% vol/vol, by providing a measure of the rotational relaxation time of solute macromolecules. We conclude that, for approximately less than 5% protein, the solute particles are noncompact, with a rotationally averaged volume approximately three times that of a compact 60-kD sphere. (Earlier results for alpha-crystallin, approximately 1,000 kD, from optical and osmotic measurements (Vérétout and Tardieu, 1989. J. Mol. Biol. 205:713-728), show a similar, approximately twofold, effect). At intermediate concentrations, to approximately 20% protein, there is evidence for limited association or oligomerization, as found for the structurally related gamma II-crystallin (Koenig et al. 1990. Biophys. J. 57:461-469), to a limiting size about two-thirds that of alpha-crystallin. The difference in NMRD behavior of the three classes of crystallins is consonant with their differing osmotic properties (Vérétout and Tardieu. J. Mol. Biol. 1989, 205:713-728; Kenworthy, McIntosh, and Magid. Biophys. J. 1992. 61:A477; Tardieu et al. 1992. Eur. Biophys. J. 21:1-12). We indicate how the unusual structures and interactions of these three classes of proteins can be combined to optimize transparency and minimize colloid osmotic difficulties in eye lens.
Asunto(s)
Cristalinas/química , Animales , Fenómenos Biofísicos , Biofisica , Bovinos , Coloides/química , Deuterio , Técnicas In Vitro , Sustancias Macromoleculares , Espectroscopía de Resonancia Magnética , Masculino , Estructura Molecular , Peso Molecular , Ósmosis , Protones , Soluciones , TemperaturaRESUMEN
The osmotic behavior of soluble cortical and nuclear steer lens crystallins was characterized by secondary osmometry for several ionic strength and pH conditions. Osmotic pressure versus protein concentration relationships were measured for pressures up to 1.15 x 10(6) dyn cm-2. At low concentrations (< 0.2 g ml-1), the osmotic pressure increased linearly with pressure, whereas for concentrations above 0.2 g ml-1, the pressure rose more sharply, giving progressively larger changes in osmotic pressure with increasing crystallin concentration. At a given ionic strength and applied osmotic pressure, the nuclear proteins attained a higher protein concentration than did the cortical proteins. For example, at the highest osmotic pressure of 1.15 x 10(6) dyn cm-2 at pH 7.6 and 0.1 M ionic strength, the observed protein concentrations were 0.43 g ml-1 for the cortical proteins and 0.52 g ml-1 for the nuclear proteins. For both cortical and nuclear steer crystallins, the pressure rose more steeply with concentration than do pressures for calf crystallins described in the literature. The impact of these developmental differences in osmotic pressure on lens transparency is discussed. Both the nuclear and cortical crystallins exhibited ionic strength-dependent shifts in their pressure-concentration behavior. At 0.02 M ionic strength, higher pressures were observed, whereas at 0.4 M ionic strength lower pressures were observed for a given protein concentration. The crystallins were also found to equilibrate to different protein concentrations at a constant osmotic pressure and 0.1 M ionic strength over a pH range of 4-9, with a maximum concentration around pH 5 for the cortical crystallins and pH 6 for the nuclear crystallins. Thus, the adult bovine cortical and nuclear soluble lens extracts are different in their osmotic properties, reflecting underlying differences in protein composition. The results of the ionic strength and pH experiments suggest that hard-sphere, electrostatic, and Donnan forces contribute to the total colloid osmotic pressure of the lens crystallins. However, near physiologic pH and ionic strength the charges of the proteins are screened to the extent that the colloid osmotic pressure exhibits only minor changes for large changes in ionic conditions. The differences in the osmotic behavior of the cortical and nuclear proteins are consistent with a model where regional variations in the colloid osmotic properties of the proteins across the lens help support the radial refractive index gradient that is present in vertebrate lenses. The importance of a radial concentration gradient of metabolites is also discussed.
Asunto(s)
Cristalinas/química , Envejecimiento/fisiología , Animales , Bovinos , Concentración de Iones de Hidrógeno , Corteza del Cristalino/fisiología , Núcleo del Cristalino/fisiología , Concentración Osmolar , Presión Osmótica , RefractometríaRESUMEN
The effects of the cholesterol analog 5 alpha-cholestan-3 beta-ol-6-one (6-ketocholestanol) on bilayer structure, bilayer cohesive properties, and interbilayer repulsive pressures have been studied by a combination of x-ray diffraction, pipette aspiration, and dipole potential experiments. It is found that 6-ketocholestanol, which has a similar structure to cholesterol except with a keto moiety at the 6 position of the B ring, has quite different effects than cholesterol on bilayer organization and cohesive properties. Unlike cholesterol, 6-ketocholestanol does not appreciably modify the thickness of liquid-crystalline egg phosphatidylcholine (EPC) bilayers, and causes a much smaller increase in bilayer compressibility modulus than does cholesterol. These data imply that 6-ketocholestanol has both its hydroxyl and keto moieties situated near the water-hydrocarbon interface, thus making its orientation in the bilayer different from cholesterol's. The addition of equimolar 6-ketocholestanol into EPC bilayers increases the magnitude, but not the decay length, of the exponentially decaying repulsive hydration pressure between adjacent bilayers. Incorporation of equimolar 6-ketocholestanol into EPC monolayers increases the dipole potential by approximately 300 mV. These data are consistent with our previous observation that the magnitude of the hydration pressure is proportional to the square of the dipole potential. These results mean that 6-ketocholestanol, despite its location in the bilayer hydrocarbon region, approximately 10 A from the physical edge of the bilayer, modifies the organization of interlamellar water. We argue that the incorporation of 6-ketocholestanol into EPC bilayers increases the hydration pressure, at least in part, by increasing the electric field strength in the polar head group region.
Asunto(s)
Cetocolesteroles , Membrana Dobles de Lípidos , Fosfatidilcolinas/química , Matemática , Potenciales de la Membrana , Modelos Teóricos , Conformación Molecular , Difracción de Rayos XRESUMEN
We monitored the mass thickness of egg yolk phosphatidylcholine multilayers at several temperatures during electron irradiation. The rate of irradiation-induced mass loss was reduced substantially when this specimen was cooled to liquid nitrogen temperature from room temperature. Additional cooling to liquid helium temperature caused an additional reduction of mass-loss rate. The characteristic doses D(1/e), which are the slopes of the logarithm of the differential mass thickness against dose, were approximately 7 x 10(3) e/nm2 at 290 K, 8 x 10(4) e/nm2 at 130 K, and 1.4 x 10(5) e/nm2 at less than 10 K. The fractions of the original mass thickness that remained after arbitrarily high doses were about 69% at 290 K, 72% at 130 K, and 77% at less than 10 K.
Asunto(s)
Microscopía Electrónica/normas , Fosfatidilcolinas/efectos de la radiación , Animales , Yema de Huevo , Electrones , Fosfatidilcolinas/química , TemperaturaRESUMEN
Pressure vs. distance relationships have been obtained for phosphatidylglycerol bilayers, in both charged and uncharged states. Water was removed from the lipid multilayers by the application of osmotic pressures in the range of 0-2.7 x 10(9) dyn/cm2, and the distance between adjacent bilayers was obtained from Fourier analysis of lamellar x-ray diffraction data. For phosphatidylglycerol bilayers made electrically neutral either by lowering the pH or by adding equimolar concentrations of the positively charged lipid stearylamine, the pressure-distance data could be fit with a single exponential. The measured decay lengths were 1.1 A at low pH and 1.5 A with stearylamine, which are similar to decay lengths of the hydration pressure found for gel phases of other neutral bilayers. In addition, the magnitude of this repulsive pressure was proportional to the square of the Volta potential (equivalent to the dipole potential for electrically neutral bilayers) measured in monolayers in equilibrium with bilayers, in agreement with results previously found for the hydration pressure between phosphatidylcholine bilayers. For charged phosphatidylglycerol bilayers, the pressure-distance relation had two distinct regions. For bilayer separations greater than 10 A, the pressure-distance data had an exponential decay length (11 A) and a magnitude consistent with that expected for electrostatic repulsion from double-layer theory. For bilayer separations of 2-10 A, the pressure decayed much more rapidly with increasing bilayer separation (decay length less than 1 A). We interpret these data at low bilayer separations in terms of a combination of hydration repulsion and steric hindrance between the lipid head groups and the sodium ions trapped between apposing bilayers.
Asunto(s)
Membrana Dobles de Lípidos , Fosfatidilgliceroles , Aminas , Matemática , Modelos Teóricos , Conformación Molecular , Presión Osmótica , TermodinámicaRESUMEN
Well-ordered multilamellar arrays of liquid-crystalline phosphatidylcholine and equimolar phosphatidylcholine-cholesterol bilayers have been formed in the nonaqueous solvents formamide and 1,3-propanediol. The organization of these bilayers and the interactions between apposing bilayer surfaces have been investigated by X-ray diffraction analysis of liposomes compressed by applied osmotic pressures up to 6 X 10(7) dyn/cm2 (60 atm). The structure of egg phosphatidylcholine (EPC) bilayers in these solvents is quite different than in water, with the bilayer thickness being largest in water, 3 A narrower in formamide, and 6 A narrower in 1,3-propanediol. The incorporation of equimolar cholesterol increases the thickness of EPC bilayers immersed in each solvent, by over 10 A in the case of 1,3-propanediol. The osmotic pressures of various concentrations of the neutral polymer poly(vinylpyrrolidone) dissolved in formamide or 1,3-propanediol have been measured with a custom-built membrane osmometer. These measurements are used to obtain the distance dependence of the repulsive solvation pressure between apposing bilayer surfaces. For each solvent, the solvation pressure decreases exponentially with distance between bilayer surfaces. However, for both EPC and EPC-cholesterol bilayers, the decay length and magnitude of this repulsive pressure strongly depend on the solvent. The decay length for EPC bilayers in water, formamide, and 1,3-propanediol is found to be 1.7, 2.4, and 2.6 A, respectively, whereas the decay length for equimolar EPC-cholesterol bilayers in water, formamide, and 1,3-propanediol is found to be 2.1, 2.9, and 3.1 A, respectively. These data indicate that the decay length is inversely proportional to the cube root of the number of solvent molecules per unit volume.(ABSTRACT TRUNCATED AT 250 WORDS)
Asunto(s)
Membrana Dobles de Lípidos , Fosfatidilcolinas , Solventes , Colesterol , Electrones , Formamidas , Presión Osmótica , Glicoles de Propileno , Difracción de Rayos X/métodosRESUMEN
The muscle isozyme of adenylosuccinate synthetase (AdSS), an enzyme of the purine nucleotide cycle, has previously been shown to bind to purified F-actin in buffers of low ionic strength and pH (Ogawa et al. Eur. J. Biochem. 85: 331-338, 1978). We have extended these observations by measuring the association of both crude and purified AdSS with the contractile proteins of muscle in buffers of physiological ionic strength and pH. Under these conditions, the enzyme binds to F-actin, actin-tropomyosin complexes, reconstructed thin filaments, and myofibrils but not to myosin. The apparent dissociation constant of 1.2 microM and binding maximum of 2.6 nmol enzyme/mg myofibrils indicate that binding of AdSS to myofibrils can be physiologically significant. The results suggest that AdSS in muscle may be associated with the thin filament of myofibrils.
Asunto(s)
Adenilosuccinato Sintasa/metabolismo , Proteínas Contráctiles/metabolismo , Isoenzimas/metabolismo , Ligasas/metabolismo , Músculos/enzimología , Miofibrillas/enzimología , Actinas/metabolismo , Animales , Concentración de Iones de Hidrógeno , Miosinas/metabolismo , Concentración Osmolar , Conejos , Tropomiosina/metabolismoRESUMEN
Pressure versus distance relations have been obtained for solid (gel) and neat (liquid-crystalline) phase uncharged lipid bilayers by the use of x-ray diffraction analysis of osmotically stressed monoglyceride aqueous dispersions and multilayers. For solid phase monoelaidin bilayers, the interbilayer repulsive pressure decays exponentially from a bilayer separation of approximately 7 A at an applied pressure of 3 x 10(7) dyn/cm2 to a separation of approximately 11 A at zero applied pressure, where an excess water phase forms. The decay length is approximately 1.3 A, which is similar to the value previously measured for gel phase phosphatidylcholine bilayers. This implies that the decay length of the hydration pressure does not depend critically on the presence of zwitterionic head groups in the bilayer surface. For liquid-crystalline monocaprylin, the repulsive pressure versus distance curve has two distinct regions. In the first region, for bilayer separations of approximately 3-8 A and applied pressures of 3 x 10(8) to 4 x 10(6) dyn/cm2, the pressure decays exponentially with a decay length of approximately 1.3 A. In the second region, for bilayer separations of approximately 8-22 A and applied pressures of 4 x 10(6) to 1 x 10(5) dyn/cm2, the pressure decays much more gradually and is inversely proportional to the cube of the distance between bilayers. These data imply that two repulsive pressures operate between liquid-crystalline monocaprylin bilayers, the hydration pressure, which dominates at small (3-8 A) bilayer separations, and the fluctuation pressure, which dominates at larger bilayer separations (greater than 8 A) and strongly influences the hydration properties of the liquid-crystalline bilayers. Thus, due primarily to thermally induced fluctuations, monocaprylin bilayers imbibe considerably more water than do monoelaidin bilayers. For both monoelaidin andmonocaprylin, the measured magnitude of the hydration pressure is found to be proportional to the square of the dipole potential.
Asunto(s)
Glicéridos , Membrana Dobles de Lípidos , Matemática , Modelos Teóricos , Presión OsmóticaRESUMEN
Pressure versus distance relationships have been obtained for egg phosphatidylcholine bilayers containing a range of cholesterol concentrations. Water was removed from between adjacent bilayers by the application of osmotic pressures in the range of 0.4-2600 atm (4 x 10(5)-2.6 x 10(9) dyn/cm2), and the distance between adjacent bilayers was obtained by Fourier analysis of X-ray diffraction data. For applied pressures up to about 50 atm and bilayer surface separations of 15-5 A, the incorporation of up to equimolar cholesterol has little influence on plots of pressure versus bilayer separation. However, for the higher applied pressures, cholesterol reduces the interbilayer separation distance by an amount that depends on the cholesterol concentration in the bilayer. For example, the incorporation of equimolar cholesterol reduces the distance between bilayers by as much as 6 A at an applied pressure of 2600 atm. At this applied pressure, electron density profiles show that the high-density head-group peaks from apposing bilayers have merged. This indicates that equimolar concentrations of cholesterol spread the lipid molecules apart in the plane of the bilayer enough to allow the phosphatidylcholine head groups from apposing bilayers to interpenetrate as the bilayers are squeezed together. All of these X-ray and pressure-distance data indicate that, by reducing the volume fraction of phospholipid head groups, cholesterol markedly reduces the steric repulsion between apposing bilayers but has a much smaller effect on the sum of the longer ranged repulsive hydration and fluctuation pressures. Increasing concentrations of cholesterol monotonically increase the dipole potential of egg phosphatidylcholine monolayers, from 415 mV with no cholesterol to 493 mV with equimolar cholesterol.(ABSTRACT TRUNCATED AT 250 WORDS)
Asunto(s)
Colesterol , Membrana Dobles de Lípidos , Fosfatidilcolinas , Presión Osmótica , Difracción de Rayos XRESUMEN
The change in pressure needed to bring egg phosphatidylcholine bilayers into contact from their equilibrium separation in excess water has been determined as a function of both distance between the bilayers and water content. A distinct upward break in the pressure-distance relation appears at an interbilayer separation of about 5 A, whereas no such deviation is present in the pressure-water content relation. Thus, this break is not a property of the dehydration process per se, but instead is attributed to steric repulsion between the mobile lipid head groups that extend 2-3 A into the fluid space between bilayers. That is, electron density profiles of these bilayers indicate that the observed break in the pressure-spacing relation occurs at a bilayer separation where extended head groups from apposing bilayers come into steric hindrance. The pressure-spacing data are used to separate steric pressure from the repulsive hydration pressure, as well as to quantitate the range and magnitude of the steric interaction. An appreciable fraction of the measured steric energy can be ascribed to a decrease in configurational entropy due to restricted head-group motion as adjacent bilayers come together.