The reduced nicotinamide adenine dinucleotide “oxidase” of Acholeplasma laidlawii membranes

An NADH dehydrogenase possessing a specific activity 3–5 times that of membrane-bound enzyme was obtained by extraction of Acholeplasma laidlawii membranes with 9.0 % ethanol at 43 °C. This dehydrogenase contained only trace amounts of iron (suggesting an uncoupled respiration), a flavin ratio of 1 : 2 FAD to FMN, and 30–40 % lipid. Its resistance to sedimentation is probably due to the high flotation density of the lipids. It efficiently utilized ferricyanide, menadione and dichlorophenol indophenol as electron acceptors, but not O₂, ubiquinone $\text{Q}{}_{10}$ or cytochrome $\text{c}$. Lineweaver-Burk plots of the dehydrogenase were altered to linear functions upon extraction with 9.0 % ethanol. A secondary site of ferricyanide reduction could not be explained by the presence of cytochromes, which these membranes lack. In comparison to other respiratory chain-linked NADH dehydrogenases in cytochrome-containing respiratory chains, this dehydrogenase was characterized by similar $\text{K}{}_{\mathrm{<mtext>m</mtext>}}\text{'}\text{s}$ with ferricyanide, dichlorophenol indophenol, menadione as electron acceptors, but considerably smaller $\text{V'}\text{s}$ with ferricyanide, dichlorophenol indophenol, menadione as electron acceptors, and smaller specific activities. It was not stimulated or reactivated by the addition of FAD, FMN, Mg²⁺, cysteine or membrane lipids, and was less sensitive to respiratory inhibitors than unextracted enzyme. The ineffectiveness of ADP stimulation on O₂ uptake, the insensitivity to oligomycin and the very low iron content of A. laidlawii membranes were considered in relation to conservation of energy by these cells. Some kinetic properties of the dehydrogenation, the uniquely high glycolipid content and apparently uncoupled respiration at Site I were noteworthy characteristics of this NADH dehydrogenase from the truncated respiratory chain of A. laidlawii.     

Transport kinetics of dipicrylamine through lipid bilayer membranes. Effects of membrane structure

Charge-pulse current-relaxation studies have been performed with lipid bilayer membranes in the presence of the hydrophobic ion dipicrylamine. From the analysis of the relaxation times and amplitudes the translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ of dipicrylamine as well as the partition coefficient β between membrane surface and water could be evaluated. In a first series of experiments membranes made from monoolein or dioleoylphosphatidylcholine in a number of different $\text{n-}\text{alkane}$ solvents were studied, as well as virtually solvent-free bilayer membranes made from monolayers. The thickness $\text{d}$ of the hydrocarbon layer of these membranes varied between 5.0 and 2.5 nm. While β was almost insensitive to variations in $\text{d}$, a strong decrease of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ with increasing membrane thickness was found; the observed dependence of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ on $\text{d}$ approximately agreed with the theoretically expected influence of membrane thickness on the height of the dielectric barrier. No specific differences between Mueller-Rudin films and solvent-free (Montal-Mueller) membranes other than differences in thickness were found. In a further series of experiments the chemical structure of the lipid was systematically varied (number and position of double bonds in the hydrocarbon chain, nature of the polar head group). The translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ was much larger in phosphatidylethanolamine membranes than in phosphatidylcholine membranes. A strong increase of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ was found when the number of double bonds in the hydrocarbon chain was increased from one to three. These changes were discussed in terms of membrane fluidity and dielectric barrier height. Much higher values of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ were observed in lipids with ester linkage between hydrocarbon chain and glycerol backbone, as compared with the corresponding ether analogs. This finding is qualitatively consistent with determinations of dipolar potentials in monolayers of ester and ether lipids. When cholesterol is added to phosphatidylcholine membranes, the translocation rate constant $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ increases up to five-fold, while the partition coefficient β remains virtually constant. The variation of $\text{k}{}_{\mathrm{<mtext>i</mtext>}}$ in this case can be largely accounted for by a decrease in membrane thickness and a concomitant reduction in dielectric barrier height. In membranes made from the negatively charged lipid phosphatidylserine the partition coefficient of dipicrylamine strongly increased with ionic strength, as expected from the Gouy-Chapman theory of the surface potential.     

Asymmetric binding of cytochrome b5 to the membrane of human erythrocyte ghosts

The intact, amphipatic form of cytochrome $\text{b}{}_5$ could bind to unsealed ghosts, but not to resealed ghosts, suggesting that the cytochrome could bind only to the inner (cytoplasmic) surface of the ghost membrane. This was further confirmed by the finding that the cytochrome could bind to closed, inside-out vesicles prepared from the ghosts. This asymmetric binding was not due to the exclusive localization of sialic acid and sugar chains on the outer surface of the ghosts membrane, because the cytochrome could not bind to ghosts even after enzymatic removal of these components. Although liposomes consisting of phosphatidylcholine or both phosphatidylcholine and sphingomyelin could effectively bind the cytochrome, this binding capacity was progressively decreased as increasing amount of cholesterol was included in the composition of phosphatidylcholine liposomes. Removal of cholesterol from resealed ghosts by incubation with egg phosphatidylcholine liposomes resulted in the binding of cytochrome $\text{b}{}_5$ to the outer surface of the treated ghosts. The possibility is discussed that the asymmetric binding is due to preferential localization of cholesterol in the outer leaflet of the lipid bilayer that constitutes the ghost membrane.     

Biochemical adaptation of mitochondria,muscle, and whole-animal respiration to endurance training

The experimental intervention of exercise training has been used to study mitochondrial biosynthesis, and the physiologic integration of subcellular, cellular, and whole-animal energetics. Gross mitochondrial composition was unchanged in rat muscle by a 10-week program of endurance treadmill running. The mitochondrial concentration of iron-sulfur clusters, cytochromes, flavoprotein, dehydrogenases, oxidases, and membrane protein and lipid, as well as the ratios of each component to the others, maintained constant proportions. The mitochondrial content of muscle, however, increased by approximately 100% as did absolute tissue oxidative capacity. The soluble portions of mitochondria maintained a constant total protein content and mass, relative to the membrane fraction, despite adaptive changes in the specific activities of some citric acid-cycle enzymes. Mitochondria from endurance-trained muscles generated normal transmembrane potentials, ADP/O ratios, and respiratory control ratios. Muscle oxidase activity was highly correlated (r = 0.92) with endurance capacity, which increased 403%. Whole-animal maximal O₂ consumption (), however, increased only 14% and was a relatively poor predictor of endurance. Thus, mitochondrial factors, rather than , must play an important role in dictating the limits of endurance activity. Conversely, was strongly related to the maximal intensity of work which could be attained aerobically (r = 0.82). Comparison of O₂ consumption at the mitochondrial, muscle, and whole-animal levels revealed that maximal muscle oxidase activity was not an absolute limitation to : It is concluded that other factors intervene to control the percentage of muscle O₂ consumption capacity which may be utilized during exercise.     

Microcalorimetric studies of the interactions between cytochromes c and c1 and of their interactions with phospholipids

Thermotropic properties of purified cytochrome $\text{c}{}_1$ and cytochrome $\text{c}$ have been studied by differential scanning calorimetry under various conditions. Both cytochromes exhibit a single endothermodenaturation peak in the differential scanning calorimetric thermogram. Thermodenaturation temperatures are ionic strength, pH, and redox state dependent. The ferrocytochromes are more stable toward thermodenaturation than the ferricytochromes. The enthalpy changes of thermodenaturation of ferro- and ferricytochrome $\text{c}{}_1$ are markedly dependent on the ionic strength of the solution. The effect of the ionic strength of solution on the enthalpy change of thermodenaturation of cytochrome $\text{c}$ is rather insignificant. The formation of a complex between cytochromes $\text{c}$ and $\text{c}{}_1$ at lower ionic strength causes a significant destabilization of the former and a slight stabilization of the latter. The destabilization of cytochrome $\text{c}$ upon mixing with cytochrome $\text{c}{}_1$ was also observed at high ionic strength, under which conditions no stable complex was detected by physical separation. This suggests formation of a transient complex between these two cytochromes. When cytochrome $\text{c}$ was complexed with phospholipids, no change in the thermodenaturation temperature was observed, but a great increase in the enthalpy change of thermodenaturation resulted.     

The binding of cytochrome b5 to plasma membranes of rat liver. Its implication for membrane specificity and biogenesis

The in vitro incorporation of cytochrome $\text{b}{}_5$ into purified plasma membranes was investigated by biochemical and immunological methods. Plasma membrane preparations incorporated three times less cytochrome $\text{b}{}_5$ than did microsomal preparations; 60% of this cytochrome $\text{b}{}_5$ could not be reduced by the NADH-cytochrome $\text{b}{}_5$ reductase and was considered as being bound to the plasma membrane. The morphological observations made after the immunochemical labeling of cytochrome $\text{b}{}_5$ clearly showed a good but asymmetrical distribution of the ferritin labeling: only the inner face of the plasma membrane incorporated cytochrome $\text{b}{}_5$. These results are discussed with respect to theories which concern the subcellular membrane relationships in the cell.     

Effect of fatty acids on plasma membrane lipid dynamics and cation permeability in neuroblastoma cells

In this study the effects of experimental modifications of plasma membrane lipid lateral mobility on the electrical membrane properties and cation transport of mouse neuroblastoma cells, clone Neuro-2A, have been studied. Short-term supplementation of a chemically defined growth medium with oleic acid or linoleic acid resulted in an increase in the lateral mobility of lipids as inferred from fluorescence recovery after photobleaching of the lipid probe 3,3′-dioctadecylindocarbocyanide iodide. These changes were accompanied by a marked depolarization of the membrane potential from ?51 mV to ?36 mV, 1.5 h after addition, followed by a slow repolarization. Tracer flux studies, using ⁸⁶Rb⁺ as a radioactive tracer for K⁺, demonstrated that the depolarization was not caused by changes in (Na⁺ + K⁺)-ATPase-mediated K⁺ influx or in the transmembrane K⁺ gradient. The permeability ratio ($\text{P}{}_{\mathrm{<mtext>Na</mtext>}}\text{P}{}_{\mathrm{<mtext>K</mtext>}}$), determined from electrophysiological measurements, however, increased from 0.10 to 0.27 upon supplementation with oleic acid or linoleic acid. This transient rise of $\text{P}{}_{\mathrm{<mtext>Na</mtext>}}\text{P}{}_{\mathrm{<mtext>K</mtext>}}$ was shown by ²⁴Na⁺ and ⁸⁶Rb⁺ flux measurements to be due to both an increase of the Na⁺ permeability and a decrease of the K⁺ permeability. None of these effects occurred upon supplementation of the growth medium with stearic acid.     

Lipid structural order parameters (reciprocal of fluidity) in biomembranes derived from steady-state fluorescence polarization measurements

This paper presents an interpretation of fluorescence polarization measurements in lipid membranes which are labelled with the apolar probe 1,6-diphenyl-1,3,5-hexatriene. The steady-state fluorescence anisotropy, $\text{r}{}_{\mathrm{<mtext>S</mtext>}}$, is resolved into a fast decaying or kinetic component, $\text{r}{}_{\mathrm{<mtext>f</mtext>}}$, and an infinitely slow decaying or static component, $\text{r}{}_{\mathrm{\infty }}$. The latter contribution, which predominates in biological membranes, is exclusively determined by the degree of molecular packing (order) in the apolar regions of the membrane; $\text{r}{}_{\mathrm{\infty }}$ is proportional to the square of the lipid order parameter. An empirical relation between $\text{r}{}_{\mathrm{<mtext>S</mtext>}}$ and $\text{r}{}_{\mathrm{\infty }}$ is presented, which is in agreement with a prediction based on a theory of rotational dynamics in liquid crystals. This relation enabled us to estimate a lipid structural order parameter directly from simple steady-state fluorescence polarization measurements in a variety of isolated biological membranes. It is shown that major factors determining the order parameter in biomembranes are the temperature, the cholesterol and sphingomyelin content and (in a few systems) the membrane intrinsic proteins.     

Binding of bovine cytochrome b5 to phosphatidycholine liposomes Characterization of the reconstituted lipid-protein vesicles

Cytochrome $\text{b}{}_5$ was extracted and purified from beef liver by a detergent method (cytochrome $\text{d-b}{}_5$). The hydrophilic moiety which carries the heme group (cytochrome $\text{t-b}{}_5$) was prepared by trypsin action upon pure cytochrome $\text{d-b}{}_5$.Single-shelled lecithin liposomes form complexes with cytochromes $\text{d-b}{}_5$ up to a molar ratio of one protein for 35 phospholipids. The lipid-protein complexes were isolated by gel filtration on Sepharose 4B. They are hollow vesicles in which [³H]-glucose can be trapped. Their diameter is greater than that of the initial liposomes.Cytochrome $\text{t-b}{}_5$ does not interact with the vesicles. These results show that the hydrophobic tail is necessary for the binding and that the hydrophilic part of the protein is located on the outer face of the vesicles. This asymmetry is also proved by the action of reducing agents.Experiments with saturated phosphatidylcholines show that the protein interacts with the lipids both below the transition temperature $\text{T}{}_{\mathrm{M}}$. i.e. when the aliphatic chains are in a crystalline state, and above $\text{T}{}_{\mathrm{M}}$, when the alipathic chain are in a fluid state.¹H NMR spectra show that even at the maximum cytochrome $\text{d-b}{}_5$ concentration the presence of the proteins does not markedly change the dynamics to the phospholipid molecules. An asymmetric single-shelled vesicle structure is proposed for the complex.     

Transversal mobility in bilayer membrane vesicles: Use of pyrene lecithin as optical probe

Pyrene lecithin, a new excimer-forming lipid molecule, has been synthesized to examine the transversal mobility of probe molecules in lecithin bilayer vesicles. The rate of the lipid exchange is obtained by following the excimer yield as a function of time after mixing of fluorescence doped and undoped vesicles. A rapid exchange ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 11}\text{s}$) is followed by a slow transfer ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 8}\text{h}$). Above the lipid phase transition the fast transfer can be attributed to an exchange of lipid molecules from the outer layer of one vesicle to the outer layer of another one. The slow exchange is interpreted in terms of the ‘flip-flop’ process between the two layers of a single bilayer vesicle.Using pyrene and pyrene decanoic acid as probe molecules only the fast transfer through the water phase is observed ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 4}\text{s}$ for pyrene and $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 7}\text{s}$ for pyrene decanoic acid). This indicates that molecules like fatty acids or apolar membrane constituents must equilibrate very rapidly in a single bilayer vesicle.The water solubility or the critical micelle concentration of the probe molecules is determined and related to the transfer rates. An exchange process through the water phase via a monomeric state can be excluded.     

Induction of a relatively fast transbilayer movement of phosphatidylcholine in vesicles. A 13C NMR study

[$\text{N-}{}^{13}\text{CH}{}_3$] Phosphatidylcholines are introduced into the outer monolayer of phosphatidylcholine vesicles with the phosphatidylcholine exchange protein from bovine liver. The transbilayer distribution of the [$\text{N-}{}^{13}\text{CH}{}_3$] phosphatidylcholine is measured with ¹³C NMR. The transbilayer movements of $\text{[N-}{}^{13}\text{CH}{}_3\text{]-}\text{dioleoyl}$ phosphatidylcholine and [$\text{N-}{}^{13}\text{CH}{}_3$] dimyristoyl phosphatidylcholine at 30°C in vesicles composed of these phosphatidylcholines are extremely slow processes with estimated half-times of days. [$\text{N-}{}^{13}\text{CH}{}_3$] Dioleoyl phosphatidylcholine introduced into dimyristoyl phosphatidylcholine vesicles migrates from the outer to the inner monolayer with a half-time of less than 12 h. The data suggest that differential changes in the lateral packing of the two monolayers might be a driving force for transbilayer transport of phospholipids.     

Properties of bilayer membranes in the presence of dipicrylamine. A comparative study by optical absorption and electrical relaxation measurements

In order to test the question if a pool of lipophilic ions may exist in black lipid membranes which cannot be detected by electrical relaxation measurements we have performed simultaneously measurements of the optical absorption of a lipophilic ion. The absorbance of membrane-bound dipicrylamine at 410 nm was measured with a sensitive spectrophotometer which can detect absorbance changes $\text{? 4 · 10}{}^{\mathrm{?5}}$. A minimal concentration of about 6 · 10¹¹ dipicrylamine ions per cm² of the membrane could be detected with this instrument. The dipicrylamine concentration in the membrane obtained with the optical method $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ is compared with the concentrations $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ obtained from simultaneous electrical relaxation measurements. $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ and $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$ agreed at low dipicrylamine concentrations (10^?8–10^?7 M in the aqueous phase) and showed saturation at higher concentrations (up to 5 · 10^?6 M). In the saturation range $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>opt</mtext>}}$ was maximally four times higher than $\text{N}{}_{\mathrm{<mtext>t</mtext>}}{}^{\mathrm{<mtext>el</mtext>}}$. The significance of this difference is discussed together with general aspects of the saturation phenomenon.     

Pulse radiolysis at planar lipid membranes doped with ion carriers or pore formers

The effect of 14 MeV electrons on ion transport through planar lipid membranes was investigated. The membranes were formed in the presence of well defined ion carriers or pore forming substances. In the presence of the ion carriers valinomycin or nonactin or in the presence of the pore formers nystatin or amphotericin B, irradiation produced a transient increase of the membrane conductance followed by a long lasting decrease. The effects are interpreted on the basis of a time-dependent chemical modification of the membrane structure caused by exposure to high energy radiation. The pore former gramicidin A shows an exponential inactivation with increasing dose. At pH 3 and in the presence of oxygen the pore is highly sensitive to radiation ($\text{D}{}_{37}\text{≈ 10}\text{Gy}$) whereas at pH 9.5 a considerably lower radiation sensitivity ($\text{D}{}_{37}\text{≈ 1000}\text{Gy}$), was found. In the absence of oxygen, gramicidin A is virtually insensitive to irradiation. This is considered an evidence that the inactivation of this ion channel is primarily caused by the perhydroxyl radical HO₂.     

Chloroplast membrane damage during freezing: the lipid phase

In order to study the effect of freeze damage to chloroplast membranes microviscosity of spinach thylakoids was probed by stearic acid spin labels. Changes in ESR parameters have been determined either as a function of temperature or during freezing at ?15 °C as a function of time. An empirical parameter $\text{h}{}_{\mathrm{+}}\text{h}{}_0$ (ratio of height of a low field line component h₊ over height of the central line h₀) proved to be very sensitive to minute changes in membrane structure.In cryoprotected chloroplast membranes Arrhenius plot breaks indicative of phase changes are observed at +15 and ?10 °C. Breaks in the Arrhenius plots were not observed in vesicles prepared from chloroplast lipids by sonication. Instead, a melting zone was indicated below ?30 °C.Freeze damage of thylakoids during storage at ?15 °C is reflected in an increase of $\text{h}{}_{\mathrm{+}}\text{h}{}_0$ and a decrease in central line width W₀. At +20 °C, differences between the ESR parameters of active as compared to freeze-damaged membranes could be detected, if the osmolarity of the suspending medium exceeded 200 mosm. The observed changes in line shapes are interpreted as an increase in mobility and/or orientation of the lipids following the swelling of thylakoids. They do not indicate a disorganization of the lipid phase. Sedimentation experiments indicated that the freeze-damaged swollen membranes still exhibited osmotic responses. It is suggested that freezing which is known to dissociate proteins from the membranes altered the charge distribution of the membranes leading first to membrane swelling and finally, by the opening of hydrophilic channels, to membrane collapse.     

Electrophoretic measurements about the relation between transition voltage and ζ-potential of biological membranes

The effects of inorganic cations, $\text{n-}\text{hexanol}$, saccharose and ²H₂O on the electrophoretic mobility and ζ-potential of membrane vesicles from nerve myelin were measured and the results compared with the corresponding effects of the same reagents on the transition voltage, $\text{V}{}_{\mathrm{<mtext>Tr</mtext>}}$, of the nerve axon membrane. Different cation concentrations and ²H₂O affect both potentials, the ζ-potential and $\text{V}{}_{\mathrm{<mtext>Tr</mtext>}}$, in a parallel way. Saccharose and $\text{n-}\text{hexanol}$, however, shift $\text{V}{}_{\mathrm{<mtext>Tr</mtext>}}$ but leave the electrophoretic mobility of the myelin vesicles unchanged. These results suggest that $\text{V}{}_{\mathrm{<mtext>Tr</mtext>}}$ shifts are not necessarily linked to changes in the membrane surface charge density but may also be caused by an interaction between the reagent and non-polar groups of the membrane interior.     

Involvement of the proton electrochemical gradient in genetic transformation in Escherichia coli

Plasmid pIY2 DNA which encodes for ampicillin-resistance was used to study the energetics of Ca⁺⁺-induced transformation in Escherichia coli. When cells are exposed to DNA in the presence of carbonylcyanide-m-chlorophenylhydrazone or 2,4-dinitrophenol, two protonophores that collapse the proton electrochemical gradient across the cell membrane ($\text{Δ}\text{μ}{}_{\mathrm{H}}\text{+}$), transformation to ampicillin-resistance is drastically reduced with little or no effect on viability. Furthermore, when the components of $\text{Δ}\text{μ}{}_{\mathrm{H}}\text{+}$ are altered by varying ambient pH or by performing transformation in the presence of valinomycin or nigericin, the efficiency of transformation is directly correlated with the magnitude of the membrane potential and changes in the pH gradient have no significant effect. It is concluded that $\text{Δ}\text{μ}{}_{\mathrm{H}}\text{+}$, more specifically the membrane potential, plays a critical role in Ca⁺⁺-induced transformation.     

Possible effects of the detachment of stromal lamellae from granal stacks on salt-induced changes in spillover. A study by sonication of chloroplasts

Salt-induced chlorophyll fluorescence and spillover changes in control and briefly sonicated chloroplasts have been studied under conditions where Photosystem II traps are closed. In a low-salt medium containing 10 mM KCl, control envelope-free chloroplasts exhibited good spillover, as measured by low chlorophyll fluorescence yield at room temperature, a high ratio of the fluorescence peaks $\text{F}{}_{735}\text{F}{}_{685}$ at 77 K, and increased Photosystem I activity in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea and Photosystem II light. In contrast, when stacked chloroplasts were briefly sonicated and subsequently diluted into a low-salt medium, a high fluorescence yield at room temperature and a low ratio of $\text{F}{}_{735}\text{F}{}_{685}$ at 77 K persisted. When unstacked chloroplasts were sonicated and then diluted into a high-salt medium, the room temperature fluorescence yield remained low. The results are interpreted in terms of a model relating the changes in chlorophyll fluoresecence with the lateral diffusion of Photosystem I and Photosystem II chlorophyll-protein complexes in the plane of the thylakoid membrane creating randomized or segregated domains, depending on the degree of electrostatic screening of surface charges (Barber, J. (1980) FEBS Lett. 188, 1–10). It is argued that brief sonication of stacked chloroplasts separates stromal membranes from granal stacks, thus limiting the inter-mixing of the photosystems via lateral diffusion even when the ionic composition of the medium is varied. Consequently energy transfer from Photosystem II to Photosystem I is relatively poor and chlorophyll fluorescence from Photosystem II is enhanced. The loss of the salt effect on sonicated unstacked membranes can also be accommodated by the model. In this case it seems that the generation of small membrane fragments does not allow the normal salt-induced phase separation of the pigment-protein complexes to occur.     

Proton nuclear magnetic resonance studies of the manganese (II) binding site of concanavalin A. Effect of saccharides on the solvent relaxation rates

The longitudinal relaxation rate ($\text{1}\text{T}{}_{\mathrm{<mtext>1</mtext><mtext>p</mtext>}}$) of water protons was studied in solutions of Mn(II)-concanavalin A at a number of frequencies. These relaxation rates were lowered in the presence of a variety of saccharides which have affinities for concanavalin A which range over two orders of magnitude. A good correlation was found in which saccharides which bind tightly have the greatest effect and saccharides which bind weakly or not at all have little effect on the $\text{1}\text{T}{}_{\mathrm{<mtext>1</mtext><mtext>p</mtext>}}$ values. The temperature dependence of the proton relaxation rates showed that the lowering of these rates in the presence of saccharides was most likely due to a change in the exchange rate of solvent interacting with protein-bound Mn(II), $\text{1}\text{T}{}_{\mathrm{<mtext>m</mtext>}}$.An analysis of the temperature and frequency dependence of the $\text{1}\text{T}{}_{\mathrm{<mtext>1</mtext><mtext>p</mtext>}}$ and $\text{1}\text{T}{}_{\mathrm{<mtext>2</mtext><mtext>p</mtext>}}$ (transverse) solvent proton relaxation rates resulted in evaluation of a number of parameters for solvent water molecules interacting in the first coordination sphere of Mn(II) bound to concanavalin A. The ratio of the number of water molecules (q) to the Mn(II)-proton distance (r) obtained from a computer fit of the data over a limited temperature range is in accord with the findings of Koenig et al. ((1973) Proc. Nat. Acad. Sci.70, 475) and Meirovitch and Kalb ((1973) Biochim. Biophys. Acta303, 258). However, our studies of $\text{1}\text{T}{}_{\mathrm{<mtext>1</mtext><mtext>p</mtext>}}$ and $\text{1}\text{T}{}_{\mathrm{<mtext>2</mtext><mtext>p</mtext>}}$ of water over a more extensive temperature range are best fit with the following conclusions: at low temperatures (<20 °C), the data are consistent with an outer-sphere relaxation process. At higher temperatures (> 30 °C), the water molecule in the inner coordination sphere of the bound Mn(II) begins exchanging more rapidly and contributes to the relaxation processes ($\text{1}\text{T}{}_{\mathrm{<mtext>1</mtext><mtext>p</mtext>}}$ and $\text{1}\text{T}{}_{\mathrm{<mtext>2</mtext><mtext>p</mtext>}}$). The relaxation time of protons in the inner coordination shell, T_1M, contributes over the entire temperature range and produces a frequency dependence in the relaxivity data from 6 to 100 MH_z since the contributions to the correlation times are in the range 10^?9-10^?8 sec.