Immobilized lipase Candida sp. 99-125 catalyzed methanolysis of glycerol trioleate: solvent effect

The immobilized lipase Candida sp. 99-125 catalyzed methanolysis of glycerol trioleate was studied in twelve different solvents in order to deduce the solvent effect through an attempt to correlate the highest yield with such solvent properties as hydrophobicity (log P), dielectric constant (epsilon), and Hildebrand solubility parameter (delta). The results showed that the conversion of glycerol trioleate and yield of oleic acid methyl ester were quite dependent on the solvent. The catalyst lipase in various solvents also needed different optimum amount of water to keep its maximum activity, and generally this lipase in more hydrophobic solvents required more water. The correlation between the highest yield and log P value was found to be reasonable except deviation of data points of certain solvents, while no obvious correlation existed between the other two parameters, dielectric constant (epsilon) and Hildebrand solubility parameter (delta), and the enzyme activity. The study revealed that more hydrophobic solvents such as n-hexane or cyclohexane were more suitable solvents for Candida sp. 99-125 catalyzed transesterification of glycerol trioleate to oleic acid methyl ester.     

The molecular mechanism of action of the proton ionophore FCCP (carbonylcyanide p-trifluoromethoxyphenylhydrazone).

We propose a simple model that accounts for the ability of the weak acid FCCP (Carbonylcyanide-p-trifluoromethoxyphenylhydrazone) to both transport protons across phospholipid bilayer membranes and uncouple oxidation from phosphorylation in mitochondria. Four parameters are required to characterize this model: the rate constant for the movement of A- across the membrane, kA, the rate constant for the movement of HA across the membrane, kHA, the adsorption coefficient of A- onto the membrane-solution interface, beta A, and the surface pK. These four parameters were determined from kinetic measurements on planar bilayer membranes using the charge-pulse and voltage-clamp techniques. We confirmed the adequacy of the model by determining each of these parameters independently, utilizing equilibrium dialysis, zeta potential, membrane potential, spectrophotometric, and conductance measurements. For a phosphatidylethanolamine bilayer the values of the parameters are kHA = 10(4)S-1, beta A = 3 10(-3) cm, and 6.0 less than pK less than 6.4. As predicted theoretically, the value of KA depends on both the applied voltage, V, and dielectric constant of the membrane, epsilon r; when V approaches zero and the membrane contains chlorodecane (epsilon r congruent to 2.7) kA = 700 s-1. If oxidation is coupled to phosphorylation by means of a delta microH+, and V er congruent to 2.7 for the inner membrane of the mitochondrion, the model predicts that FCCP should exert maximal uncoupling activity at a pH congruent to pK. This prediction agrees with the published experimental results.     

Passive electrical properties of the membrane and cytoplasm of cultured rat basophil leukemia cells. II. Effects of osmotic perturbation

The effects of osmotic perturbation on the dielectric behavior of cultured rat basophilic leukemia (RBL-1) cells were examined. Cells exposed to osmolalities (pi) of 145-650 mosmolal showed dielectric dispersions of the following characteristics: Permittivity increment delta epsilon(= epsilon l - epsilon h where epsilon l and epsilon h refer to the low- and high-frequency limit values) for a fixed volume concentration increased with pi; gross permittivity behavior was apparently of a typical Cole-Cole type; however, frequency dependence of conductivity was undulant and could be simulated by a superposition of two separate Cole-Cole type dispersions; separation of these subdispersions along the frequency axis was an increasing function of pi, and so was conductivity increment in the high-frequency region. As examined by light microscopy, the cells were spherical in spite of imposed anisotonic stresses and behaved as osmometers at 200-410 mosmolal. When normalized by dividing by number (not volume) concentration, delta epsilon remained relatively constant irrespective of pi. Apparent membrane capacities (Cm), analyzed by applying a single-shell model, increased systematically from a hypotonic value of approx. 1 microF/cm2 up to 5 microF/cm2 at 650 mosmolal. This increase was interpreted as due to increased cellular 'surface/volume' ratios that were confirmed by scanning electron microscopy. Cole-Cole's beta parameter, which culminated around 0.9 for isotonic cells and declined to approx. 0.8 for anisotonic cells, did not parallel the broadening of cell volume distribution but appeared to reflect changes in the intracellular conductivity caused by the anisotonic challenge. The results indicate that the dispersion method can probe changes in surface morphology as well as subcellular organelles' constitution of living cells.     

Evaluation of the intramolecular stacking of the fluorosulfonylbenzoyl derivatives of 1,N6-ethenoadenosine, adenosine, and guanosine

The differences in conformation in solution of fluorosulfonylbenzoyl nucleosides were analyzed by fluorescence and proton nuclear magnetic resonance spectroscopy. The quantum yield of 5'-p-fluorosulfonylbenzoyl-1,N6-ethenoadenosine (5'-FSB epsilon A) in aqueous solution is low (? = 0.01) as compared to that of its parent nucleoside, ethenoadenosine (? = 0.54), and increases approximately 5-fold when measured in a series of solvents of decreasing dielectric constant. The quantum yield of 5'-p-sulfonylbenzoyl-1,N6-ethenoadenosine covalently bound to glutamate dehydrogenase and pyruvate kinase is also 0.01, suggesting that the analogue may exist in the same conformation when enzyme-bound as when free in solution. In D2O, the resonances of the purine ring protons on 5'-FSB epsilon A, 5'-p-fluorosulfonylbenzoyl adenosine (5'-FSBA), and 5'-p-fluorosulfonylbenzoyl guanosine (5'-FSBG) are shifted upfield by about 0.1-0.3 ppm relative to the corresponding protons of their parent nucleosides. The calculated difference in chemical shift (delta delta) decreases as the dielectric constant of the solvent decreases. The delta delta decreases with increasing temperature. These data indicate that 5'-FSB epsilon A, 5'-FSBA, and 5'-FSBG exist in aqueous solution in a conformation in which the purine ring is intramolecularly stacked with the benzoyl moiety. From the magnitude of change in delta delta for 5'-FSB epsilon A, 5'-FSBA, and 5'-FSBG as a function of solvent, it appears that the three analogues differ in their sensitivity to disruption of stacking. The solution conformation of these three fluorosulfonylbenzoyl nucleoside analogues may be an important determinant of their reaction with various enzymes and may explain differences among the analogues in their reaction with a single enzyme.     

Impulse photoconductance of solutions of chlorophyll and its analogs. IV. Absolute quantum yield of ion radical formation during photooxidation of chlorophyll a by n-benzoquinone

The values of absolute quantum yield phi of the formation of free ion-radicals during the illumination of alkohol solutions of chlorophyll alpha (Chl) and rho-benzoquinone (Q) at room temperature were obtained by the method of impulse photoconductance. With an increase of the dielectric constant epsilon of the solvent from approximately 6 to approximately 25 phi increases by two orders ( approximately 10(-3)--approximately 10(-1). That obtained relationship phi (epsilon) is explained by epsilon effect on the efficiency of dissociation of "solvent-shared" ion-radical pair Chls+. Os-. The comparison of experimental data and theoretically expected ones allowed the estimation of some parameters to be obtained which characterize the ion-radical pair: interionic distance (10 A), the dissociation velocity constant ( approximately 10(5)--10(8) s-1), the velocity constant of reverse electron transfer (10(8) s-1), the life time approximately 10(-8) s).     

Passive electrical properties of the membrane and cytoplasm of cultured rat basophil leukemia cells. I. Dielectric behavior of cell suspensions in 0.01-500 MHz and its simulation with a single-shell model

Frequency dependence of relative permittivity (dielectric constant) and conductivity, or the 'dielectric dispersion', of cultured cells (RBL-1 line) in suspension was measured using a fast impedance analyzer system capable of scanning 92 frequency points over a 10 kHz-500 MHz range within 80 s. Examination of the resulting dispersion curves of an improved reliability revealed that the dispersions consisted of at least two separate components. The low-frequency component (dispersion 1) had a permittivity increment (delta epsilon) of 10(3)-10(4) and a characteristic frequency (fc) at several hundred kHz; for the high-frequency component (dispersion 2), delta epsilon was smaller by a factor of 10(2) and fc = 10-30 MHz. Increments delta epsilon for both components increased with the volume fraction of cell suspension, while fc did not change appreciably as long as the conductivity of suspending medium was fixed. By fitting a model for shelled spheres (the 'single-shell' model) to the data of dispersion 1, the dielectric capacity of the plasma membrane phase (Cm) was estimated to be approx. 1.4 microF/cm2 for the cells in an isotonic medium. However, simulation by this particular shell model failed to reproduce the entire dispersion profile leaving a sizable discrepancy between theory and experiment especially at frequencies above 1 MHz where dispersion 2 took place. This discrepancy could not be filled up even by taking into consideration either the effect of cell size distribution actually determined or that of possible heterogeneity in the intracellular conductivity. The present data strongly indicate the need for a more penetrating model that effectively accounts for the behavior of dispersion 2.     

Theoretical calculation of the dielectric constant of a bilayer membrane.

The dielectric constant (epsilon) and refractive index (n) of a bilayer lipid membrane is determined from the known values of the polarizabilities of the carbon-carbon and carbon-hydrogen bonds. It is assumed that the hydrocarbon chains are hexagonally arranged in an all-trans conformation perpendicular to the plane of the membrane. The only variable in the calculation is the average separation between the chains and the theory relates epsilon to this separation. The calculation and results differ significantly from those presented in a 1968 publication by Ohki. It is shown that a thin membrane is not homogeneously polarized by the applied field. This effect is analysed and the dependence of epsilon on the membrane thickness is determined. The theoretical results are in good quantitative agreement with experimental measurements on bulk paraffins and on oriented multilayers of saturated fatty acids. The most important conclusion is that the dielectric constant for an applied field perpendicular to the membrane (which is the appropriate value for capacitance measurements) differs by only a few percent from the value for the macroscopic (bulk) liquid hydrocarbon. Thus the dielectric constant of a bilayer membrane can be approximated by the value for the appropriate bulk hydrocarbon.     

Characterization of the ethenoadenosine diphosphate binding site of myosin subfragment 1. Energetics of the equilibrium between two states of nucleotide.S1 and vanadate-induced global conformation changes detected by energy transfer

The fluorescence decay of 1,N6-ethenoadenosine diphosphate (epsilon ADP) bound to myosin subfragment 1 (S1) was studied as a function of temperature. The decay was biexponential, and the two lifetimes were quenched relative to the single lifetime of free epsilon ADP. The temperature dependence of the fractional intensities of the decay components showed two states of the S1.epsilon ADP complex. At pH 7.5 in 30 mM TES, 60 mM KCl, and 3 mM MgCl2, the equilibrium constant for the conversion of the low-temperature state (S1L.epsilon ADP) to the high-temperature state (S1H.epsilon ADP) was 40 at physiological temperatures, and delta H degrees = 13 kcal.mol-1 and delta S degrees = 49 cal.deg-1.mol-1. At 10 degrees C the equilibrium constant of S1 for epsilon ADP was 5, indicating that S1H.epsilon ADP was the dominant state, and that for the vanadate complex epsilon ADP.Vi was 0.7, suggesting that in S1.epsilon ADP.Vi the dominant state of the S1-nucleotide complex was converted from S1H.epsilon ADP to S1L.epsilon ADP. The single rotational correlation time of bound epsilon ADP at 10 degrees C decreased from 107 ns in S1.epsilon ADP to 74 ns in S1+.epsilon ADP.Vi. Conversion of the binary complex to the ternary vanadate complex resulted in a 3-A decrease in the energy transfer distance between bound epsilon ADP and N-[4-(dimethylamino)-3,5-dinitrophenyl]maleimide attached to SH1 and a decrease of the average distance between bound epsilon ADP and bound Co2+ from 12.6 to 8.3 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

A distinct contribution of the delta subunit to acetylcholine receptor channel activation revealed by mutations of the M2 segment.

Acetylcholine receptor (AChR) channels with proline (P) mutations in the putative pore-forming domain (at the 12' position of the M2 segment) were examined at the single-channel level. For all subunits (alpha, beta, epsilon, and delta), a 12'P mutation increased the open channel lifetime >5-fold. To facilitate the estimation of binding and gating rate constants, subunits with 12'P mutations were co-expressed with alpha subunits having a binding site mutation that slows channel opening (alphaD200N). In these AChRs, a 12'P mutation in epsilon or beta slowed the closing rate constant approximately 6-fold but had no effect on either the channel opening rate constant or the equilibrium dissociation constant for ACh (Kd). In contrast, a 12'P mutation in delta slowed the channel closing rate constant only approximately 2-fold and significantly increased both the channel opening rate constant and the Kd. Pairwise expression of 12'P subunits indicates that mutations in epsilon and beta act nearly independently, but one in delta reduces the effect of a homologous mutation in epsilon or beta. The results suggest that a 12'P mutation in epsilon and beta has mainly local effects, whereas one in delta has both local and distributed effects that influence both agonist binding and channel gating.     

Comparison of calculation and experiment implicates significant electrostatic contributions to the binding stability of barnase and barstar

The contributions of electrostatic interactions to the binding stability of barnase and barstar were studied by the Poisson-Boltzmann model with three different protocols: a), the dielectric boundary specified as the van der Waals (vdW) surface of the protein along with a protein dielectric constant (epsilon (p)) of 4; b), the dielectric boundary specified as the molecular (i.e., solvent-exclusion (SE)) surface along with epsilon (p) = 4; and c), "SE + epsilon (p) = 20." The "vdW + epsilon (p) = 4" and "SE + epsilon (p) = 20" protocols predicted an overall electrostatic stabilization whereas the "SE + epsilon (p) = 4" protocol predicted an overall electrostatic destabilization. The "vdW + epsilon (p) = 4" protocol was most consistent with experiment. It quantitatively reproduced the observed effects of 17 mutations neutralizing charged residues lining the binding interface and the measured coupling energies of six charge pairs across the interface and reasonably rationalized the experimental ionic strength and pH dependences of the binding constant. In contrast, the "SE + epsilon (p) = 4" protocol predicted significantly larger coupling energies of charge pairs whereas the "SE + epsilon (p) = 20" protocol did not predict any pH dependence. This study calls for further scrutiny of the different Poisson-Boltzmann protocols and demonstrates potential danger in drawing conclusions on electrostatic contributions based on a particular calculation protocol.     

Density functional theory calculations on the dielectric constant dependence of the oxidation potential of chlorophyll: implication for the high potential of P680 in photosystem II

The primary donor chlorophyll (Chl) of photosystem II (PSII), P680, has an extremely high oxidation redox potential (E(ox)) of approximately 1.2 V, which is essential for photosynthetic water oxidation. The mechanism for achieving a high potential such as that of P680 has been one of the central questions in photosynthesis research. Here, we have examined the dielectric constant (epsilon) dependence of the E(ox) of monomer Chl using density functional theory calculations with the polarizable continuum model. The calculated E(ox) of a model Chl compound exhibited a sharp increase with a decrease in epsilon in the relatively low epsilon region (epsilon < 5). In contrast, in the higher-epsilon region, E(ox) was rather insensitive to epsilon and converged to a constant value at very high epsilon values. This tendency in the high-epsilon region explains the experimental E(ox) values of isolated Chl a that have been observed in a relatively narrow range of 0.74-0.93 V. The E(ox) of Chl in an ideal hydrophobic protein was estimated to be approximately 1.4 V at an epsilon value of 2. This value indicates that Chl in a hydrophobic environment originally has a high E(ox) that is sufficient for oxidizing water (E(ox) = 0.88 V at pH 6). On the basis of the reported X-ray crystallographic structures, the protein environment of P680 in PSII was estimated to be more hydrophobic than that of the primary donors in bacterial reaction centers. It is therefore suggested that the low-dielectric environment around P680 is one of the major factors in its very high E(ox), and thus, introducing nonpolar amino acids into the binding pocket of P680 was an important process in the evolution of PSII.     

Distinctive activities of DNA polymerases during human DNA replication

The contributions of human DNA polymerases (pols) alpha, delta and epsilon during S-phase progression were studied in order to elaborate how these enzymes co-ordinate their functions during nuclear DNA replication. Pol delta was three to four times more intensely UV cross-linked to nascent DNA in late compared with early S phase, whereas the cross-linking of pols alpha and epsilon remained nearly constant throughout the S phase. Consistently, the chromatin-bound fraction of pol delta, unlike pols alpha and epsilon, increased in the late S phase. Moreover, pol delta neutralizing antibodies inhibited replicative DNA synthesis most efficiently in late S-phase nuclei, whereas antibodies against pol epsilon were most potent in early S phase. Ultrastructural localization of the pols by immuno-electron microscopy revealed pol epsilon to localize predominantly to ring-shaped clusters at electron-dense regions of the nucleus, whereas pol delta was mainly dispersed on fibrous structures. Pol alpha and proliferating cell nuclear antigen displayed partial colocalization with pol delta and epsilon, despite the very limited colocalization of the latter two pols. These data are consistent with models where pols delta and epsilon pursue their functions at least partly independently during DNA replication.     

The effect of protein relaxation on charge-charge interactions and dielectric constants of proteins.

The effect of the reorganization of the protein polar groups on charge-charge interaction and the corresponding effective dielectric constant (epsilon(eff)) is examined by the semimicroscopic version of the Protein Dipole Langevin Dipoles (PDLD/S) method within the framework of the Linear Response Approximation (LRA). This is done by evaluating the interactions between ionized residues in the reaction center of Rhodobacter sphaeroides, while taking into account the protein reorganization energy. It is found that an explicit consideration of the protein relaxation leads to a significant increase in epsilon(eff) and that semimicroscopic models that do not take this relaxation into account force one to use a large value for the so-called "protein dielectric constant," epsilon(p), of the Poisson-Boltzmann model or for the corresponding epsilon(in) in the PDLD/S model. An additional increase in epsilon(eff) is expected from the reorganization of ionized residues and from changes in the degree of water penetration. This finding provides further support for the idea that epsilon(in) (or epsilon(p)) represents contributions that are not considered explicitly. The present study also provides a systematic illustration of the nature of epsilon(eff), supporting our previously reported view that charge-charge interactions correspond to a large value of this "dielectric constant," even in protein interiors. It is also pointed out that epsilon(eff) for the interaction between ionizable groups in proteins is very different from the effective dielectric constant, epsilon'(eff), that determines the free energy of ion pairs in proteins (epsilon'(eff) reflects the effect of preoriented protein dipoles). Finally, the problems associated with the search for a general epsilon(in) are discussed. It is clarified that the epsilon(in) that reproduces the effect of protein relaxation on charge-charge interaction is not equal to the epsilon(in) that reproduces the corresponding effect upon formation of individual charges. This reflects fundamental inconsistencies in attempts to cast microscopic concepts in a macroscopic model. Thus one should either use a large epsilon(in) for charge-charge interactions and a small epsilon(in) for charge-dipole interactions or consider the protein relaxation microscopically.     

Electrostatic effects on the alpha-helix and beta-strand formation of BPTI(16-36) studied by Monte Carlo simulated annealing.

The electrostatic effects on the secondary structure forming tendencies of a peptide fragment with residues 16-36 of bovine pancreatic trypsin inhibitor, BPTI(16-36), are studied using Monte Carlo simulated annealing simulations. We consider three dielectric functions epsilon(r) of distance r: constant dielectric function (epsilon = 2; strong electrostatic interactions) and sigmoidal functions varying from epsilon(0) = 2 to epsilon(infinity) = 47 (intermediate) and to epsilon(infinity) = 78 (weak). Simulations with epsilon = 2 suggest that this peptide exhibits a significant propensity for beta-strand formations in accordance with a beta-sheet structure of the relevant segment in native BPTI. The tendency for alpha-helix formations becomes almost comparable with that of beta-strands in the simulation with epsilon(infinity) = 47, and there appears no appreciable conformational propensity for this case. Finally, the results with epsilon(infinity) = 78 generate low-energy conformations with conspicuous alpha-helices. These findings suggest the possibility that the change in electrostatic interactions can be the key factor for the conformational transitions of peptides between alpha-helix and beta-sheet that have recently been observed in experiments. These changes in electrostatic interactions can arise from those in various environmental factors such as conformations of the rest of the protein molecule and solvent conditions.     

Dielectric analysis of the rat thyroid gland by modeling the follicle as a key structure]

To correlate the dielectric behavior of the thyroid gland with its follicle structure, I examined the admittance properties of isolated rat thyroid hemilobes over the frequency range from 100 Hz up to 500 MHz. Rats were divided into three groups: control, thyroxine (T4) administered, and goitrogen (propylthiouracil, PTU) administered. In control glands, observed dielectric dispersions with a permittivity increment (delta epsilon) of 60,000 were of the beta-type having two separate characteristic frequencies (fc1 and fc2) around 12 kHz and 3 MHz. In T4- or PTU-treated thyroid, both delta epsilon and fc1 departed from those of control, resulting in the following sequences: For delta epsilon, T4 < control < PTU, and for fc1, PTU < control < T4. These contrasting results were then correlated with morphological features involved. Histomorphometry revealed apparent differences in follicular size distribution between the three groups of tissue. Based on a model analysis using curve fitting technique, I estimated the electrical conductivity of colloid to be about 2 mS/cm, a value 6-fold smaller than that of blood plasma. Another conclusion worthy of note is that the gross dielectric behavior of the thyroid gland can be interpreted only by taking the follicular structure into account.     

Assembly of DNA polymerase delta and epsilon holoenzymes depends on the geometry of the DNA template.

To study in details the assembly of DNA polymerases delta and epsilon holoenzymes a circular double-stranded DNA template containing a gap of 45 nucleotides was constructed. Both replication factor C and proliferating cell nuclear antigen were absolutely required and sufficient for assembly of DNA polymerase delta holoenzyme complex on DNA. On such a circular DNA substrate replication protein A (or E. coli single-strand DNA binding protein) was neither required for assembly of DNA polymerase delta holoenzyme complex nor for the gap-filling reaction. A circular structure of the DNA substrate was found to be absolutely critical for the ability of auxiliary proteins to interact with DNA polymerases. The linearization of the circular DNA template resulted in three dramatic effects: (i) DNA synthesis by DNA polymerase delta holoenzyme was abolished, (ii) the inhibition effect of replication factor C and proliferating cell nuclear antigen on DNA polymerase alpha was relieved and (iii) DNA polymerase epsilon could not form any longer a holoenzyme with replication factor C and proliferating cell nuclear antigen. The comparison of the effect of replication factor C and proliferating cell nuclear antigen on DNA polymerases alpha, delta and epsilon indicated that the auxiliary proteins appear to form a mobile clamp, which can easily slide along double-stranded DNA.     

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. I. Proton in the cavity.

Time resolved fluorimetry was employed to monitor the geminate recombination between proton and excited pyranine anion locked, together with less than 30 water molecules, inside the heme binding site of Apomyoglobin (sperm whale). The results were analyzed by a numerical reconstruction of the differential rate equation for time-dependent diffusion controlled reaction with radiating boundaries using N. Agmon's procedure (Huppert, Pines, and Agmon, 1990, J. Opt. Soc. Am. B., 7:1541-1550). The analysis of the curve provided the effective dielectric constant of the proton permeable space in the cavity and the diffusion coefficient of the proton. The electrostatic potential within the cavity was investigated by the equations given by Gilson et al. (1985, J. Mol. Biol., 183:503-516). According to this analysis the dielectric constant of the protein surrounding the site is epsilon prot < or = 6.5. The diffusion coefficient of the proton in the heme binding site of Apomyoglobin-pyranine complex is D = 4 x 10(-5) cm2/s. This value is approximately 50% of the diffusion coefficient of proton in water. The lower value indicates enhanced ordering of water in the cavity, a finding which is corroborated by a large negative enthropy of binding delta S0 = -46.6 cal.mole-1 deg-1. The capacity of a small cavity in a protein to retain a proton had been investigated through the mathematical reconstruction of the dynamics. It has been demonstrated that Coulombic attraction, as large as delta psi of energy coupling membrane, is insufficient to delay a free proton for a time frame comparable to the turnover time of protogenic sites.     

Purification of membrane attachment and inhibitory subunits of the proton translocating adenosine triphosphatase from Escherichia coli.

The portion of Escherichia coli adenosine triphosphatase (ATPase) which is peripheral to the membrane (ECFl) is composed of five separate polypeptides referred to as alpha, beta, gamma, delta, and epsilon. Treating purified ECFl with pyridine precipitated the three larger polypeptides (alpha, beta, and gamma), but the two smaller ones (delta and epsilon), which represent only about 10% of ECFl, remained in solution. After removing the pyridine, both delta and epsilon were active and both were obtained in essentially pure form after chromatography on a single molecular-seive column. epsilon strongly inhibited the ATPase activity of ECFl, indicating that epsilon has a regulatory role in the enzyme. epsilon inhibited ECFl missing delta, indicating that delta is not required for inhibition by epsilon. However, enzyme containing just the alpha and beta subunits, which was prepared by treating ECFl with a protease, was fully active hydrolytically but not at all sensitive to inhibition by epsilon. This result suggests that the gamma polypeptide is required for the inhibition of the ATPase by epsilon. delta restored the capacity of ECFl missing delta to recombine with ECFl-depleted membrane vesicles. The ECFl, which became attached to the vesicles by the added delta, was functional in energy transduction, as evidenced by the coupling of ATP hydrolysis to the transhydrogenase reaction in the vesicles. The rebinding of ECFl missing delta was directly proportional to the amount of delta added until all the ECFl receptors in the membranes were occupied. delta may be a stalk which connects the Fl headpiece to the membrane, since the attachment of ECFl to the membrane exhibited an absolute dependence on delta. Although delta is known to have an apparent molecular weight of about 20,000 by gel electrophoresis in the presence of sodium dodecyl sulfate, the active delta eluted from a molecular-seive column with an apparent molecular weight of about 35,000, suggesting that in the active form delta is a dimer or rather elongated in shape. The active epsilon subunit eluted from the same column with an apparent molecular weight of about 16,000.     

Study of the dielectric permeability in the superhigh frequency range of a degraded polyoxybutyrate biopolymer

The dielectric permeability of the degradable biopolymer polyhydroxybutyrate synthesized by hydrogen-oxidizing bacteria Alcaligenes eutrophus was investigated by the resonance method using original highly sensitive microstrip sensors. For the first time, a linear growth of dielectric permeability (delta epsilon/delta T = 7 x 10(-4) degree-1) due to the flexibility of the polymer chain in the temperature range from 10 to 70 degrees C was revealed. The energy of a bend of the nearest fragments was evaluated (E = 392 K), and its correspondence to the energies of bends of the alcyl groups of low-molecular substances like liquid crystals was established. It was shown that at low values of dielectric permeability in the high-frequency range (epsilon' = 2.25 +/- 0.02), which are stable, in a wide range of frequencies of the electromagnetic field (1 MHz - 1 Hz), polyoxybutyrate can be used in the microwave equipment.     

Evidence for the existence of protomers in the assembly of encephalomyocarditis virus.

Two capsid precursor subunits, which sediment on glycerol gradients at 13S and 14S, respectively, have been identified in cytoplasmic extracts of encephalomyocarditis virus-infected HeLa cells. The 13S subunit, which was detected after a 10-min pulse label with -3H-labeled amino acids, contained only capsid precursor chain A (mol wt 100,000). When the 10-min pulse label in such cells was chased for 20 min, the A-containing 13S subunit in the cytoplasmic extracts was replaced by a 14S subunit containing equimolar proportions of three chains: epsilon, gamma, and alpha. This (epsilon, gamma, alpha)-containing 14S subunit could be dissociated into 6S subunits with the same polypeptide composition. The sedimentation properties and the polypeptide stoichiometry of these three precursor subunits, when compared with those of the 13S, (beta, gamma, alpha)(5), and 5S, (beta, gamma, alpha), subunits derived by acid dissociation of purified virions, suggest the following structural assignments: 13S, (A)(5); 14S, (epsilon, gamma, alpha)(5), 6S, (epsilon, gamma, alpha). The molecular weights of the individually isolated capsid chains were determined by gel filtration in 6 M guanidine hydrochloride to be: epsilon, 36,000; alpha, 32,000; beta, 29,500; gamma, 26,500; and delta, 7,800. With the exception of the delta-chain, these values are in reasonable agreement with the values previously determined by electrophoresis on sodium dodecyl sulfatepolyacrylamide gels. These data support the hypothesis that picornavirus capsids are assembled from identical protomers according to the following scheme: (A) leads to (A)(5) leads to (epsilon, gamma, alpha)(5) leads to (delta, beta, gamma, alpha)60-n(epsilon, gamma, alpha)n where n is the number of immature protomers per virion.