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.     

Phase transition characteristics of diphosphatidylglycerol (cardiolipin) and stereoisomeric phosphatidyldiacylglycerol bilayers: Mono- and divalent metal ion effects

Synthesis and phase transition characteristics of aqueous dispersions of the homologous (12 : 0, 14 : 0, 16 : 0) diphosphatidylglycerols (cardiolipins) and phosphatidyldiacylglycerols are reported. Electron microscopy of the negatively stained aqueous dispersions reveals a characteristic lamellar structure suggesting that these phospholipid molecules are organized as bilayers in the aqueous dispersions. The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>m</mtext>}}$) and the enthalpy of transition ($\text{ΔH}$) increase monotonically with chain length in the cardiolipin and phosphatidyldiacylglycerol series; $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ for phosphatidyldiacylglycerol is higher than that for cardiolipin of the same chain-length. The transition temperatures for the enantiomeric $\text{sn-3,3-}\text{and}\text{sn-1,1-}\text{phosphatidyldiacylglycerol}$ and for the diastereomeric, $\text{meso}\text{-sn-1,3-}\text{phosphatidyldiacylglycerol}$ are approximately the same. The molar enthalpy for the transition of cardiolipin-NH₄⁺ bilayers is approximately twice the value for the phosphatidylcholines of the same chain length, i.e., the molar enthalpy per acyl chain is approximately the same in the two systems. The transition temperatures for metal ion salts of C_{1 6}-cardiolipin exhibit a biphasic dependence upon the unhydrated ionic radii, i.e. the highest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Ca²⁺- cardiolipin and decreases for the salts of ions with smaller and larger ionic radii than that of Ca²⁺. The lowest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Rb⁺-cardiolipin. Monovalent metal salts of cardiolipin exhibit two phase transitions. This effect may result from different conformational packing of the four acyl chains due to differences in metal-phosphate binding.     

Asymmetric antagonistic effects of an inhalation anesthetic and high pressure on the phase transition temperature of dipalmitoyl phosphatidic acid bilayers

The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>t</mtext>}}$) of dipalmitoyl phosphatidic acid multilamellar liposomes is depressed 10°C by the inhalation anesthetic methoxyflurane at a concentration of 100 mmol/mol lipid. Application of 100 atm of helium pressure to pure phosphatidic acid liposomes increased $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C. However, application of 100 atm helium pressure to dipalmitoyl phosphatidic acid lipsomes containing 100 mmol methoxyflurane/mol lipid almost completely antagonized the effect of the anesthetic. A nonlinear pressure effect is observed. In a previous study, a concentration of 60 mmol methoxyflurane/mol dipalmitoyl phosphatidylcholine depressed $\text{T}{}_{\mathrm{<mtext>t</mtext>}}$ only 1.5°C, exhibiting a linear pressure effect. The completely different behavior in the charged membrane is best explained by extrusion of the anesthetic from the lipid phase.     

Role of the plasma membrane in the mechanism of cholesterol efflux from cells

In order to investigate the role of the plasma membrane in determining the kinetics of removal of cholesterol from cells, the efflux of [³H]cholesterol from intact cells and plasma membrane vesicles has been compared. The release of cholesterol from cultures of Fu₅AH rat hepatoma and WIRL-3C rat liver cells to complexes of egg phosphatidylcholine (1 mg / ml) and human high-density apolipoprotein is first order with respect to concentration of cholesterol in the cells, with half-times ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$) for at least one-third of the cell cholesterol of 3.2 ± 0.6 and 14.3 ± 1.5 h, respectively. Plasma membrane vesicles (0.5–5.0 μm diameter) were produced from both cell lines by incubating the cells with 50 mM formaldehyde and 2 mM dithiothreitol for 90 min. The efflux of cholesterol from the isolated vesicles follows the same kinetics as the intact, parent cells: the $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for plasma membrane vesicles of Fu₅AH and WIRL cells are 3.9 ± 0.5 and 11.2 ± 0.7 h, respectively. These $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values reflect the rate-limiting step in the cholesterol efflux process, which is the desorption of cholesterol molecules from the plasma membrane into the extracellular aqueous phase. The fact that intact cells and isolated plasma membranes release cholesterol at the same rate indicates that variations in the plasma membrane structure account for differences in the kinetics of cholesterol release from different cell types. In order to investigate the role of plasma membrane lipids, the kinetics of cholesterol desorption from small unilamellar vesicles prepared from the total lipid isolated from plasma membrane vesicles of Fu₅AH and WIRL cells were measured. Half-times of cholesterol release from plasma membrane lipid vesicles of Fu₅AH and WIRL cells were the same, with values of 3.1 ± 0.1 and 2.9 ± 0.2 h, respectively. Since bilayers formed from isolated plasma membrane lipids do not reproduce the kinetics of cholesterol efflux observed with the intact plasma membranes, it is likely that the local domain structure, as influenced by membrane proteins, is responsible for the differences in $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ values for cholesterol efflux from these cell lines.     

Raman spectroscopic study of an interdigitated lipid bilayer. Dipalmitoylphosphatidylcholine dispersed in glycerol

Dipalmitoylphosphatidylcholine (DPPC) dispersed in perdeuterated glycerol was investigated in order to determine the effects on the Raman spectra of hydrocarbon chain interdigitation in gel-phase lipid bilayers. Interdigitated DPPC bilayers formed from glycerol dispersions in the gel phase showed a decrease in the peak height intensity $\text{I}{}_{2850}\text{/I}{}_{2880}$ ratio, for the symmetric and asymmetric methylene CH stretching modes, respectively, as compared to non-interdigitated DPPC/water gel-phase dispersions. The decrease in this spectral ratio is interpreted as an increase in chain-chain lateral interactions. Spectra recorded in the 700–740 cm^?1 CN stretching mode region, the 1000–1200 cm^?1 CC stretching mode region and the 1700–1800 cm^? CO stretching mode region were identical for both the interdigitated and non-interdigitated hydrocarbon chain systems. At low temperatures the Raman peak height intensity ratios $\text{I}{}_{2935}\text{/I}{}_{2880}$ were identical for the DPPC/glycerol and DPPC/water dispersions, indicating that this specific index for monitoring bilayer behavior is insensitive to acyl chain interdigitation. The increase, however, in the change of this index at the gel-liquid crystalline phase transition temperature for the DPPC/glycerol dispersions implies a larger entropy of transition in comparison to the non-interdigitated DPPC/water bilayer system.     

Membrane lipid dynamics and enzymic activity in bovine adrenal cortex microsomes

The lipid dynamics of the adrenocortical microsomal membranes was studied by monitoring the fluorescence anisotropy and excited state lifetime of a set of anthroyloxy fatty acid probes (2-, 7-, 9- and 12-(9-anthroyloxy)-stearic acid (AP) and 16-(9-anthroyloxy)palmitic acid (AS). It was found that a decreasing polarity gradient from the aqueous membrane interface to the membrane interior, was present. This gradient was not modified by the proteins, as evidenced by comparison of complete membranes and derived liposomes, suggesting that the anthroyloxy probes were not in close contact with the proteins. An important change of the value of the mean rotational relaxation time as a function of the position of the anthroyl ring along the acyl chain was evidenced. In the complete membranes, a relatively more fluid medium was evidenced in the C₁₆ as compared to the C₂ region, while the rotational motion appeared to be the most hindered at the C₇–C₉ level. In the derived liposomes, a similar trend was observed but the mobility was higher at all levels. The decrease of the mean rotational relaxation time was more important for 12-AS and 16-AP. Temperature dependence of the mean rotational relaxation time of 2-AS, 12-AS and 16-AP in the complete membranes revealed the existence of a lipid reorganization occurring around 27°C and concerning mainly the C₁₆ region. The extent to which the acyl chain reacted to this perturbation at the C₁₂ level depended on pH. The presence of proteins increased the apparent magnitude of this reorganization and also modified the critical temperature from approx. 23°C in the derived liposomes to approx. 27°C in the complete membranes. Thermal dependence of the maximum velocity of the $\text{3-}\text{oxosteroid}\text{Δ}{}^5\text{?Δ}{}^4\text{-}\text{isomerase}$, the second enzyme in the enzymatic sequence, responsible for the biosynthesis of the $\text{3-}\text{oxo}\text{-Δ}{}^4\text{-}\text{steroids}$ in the adrenal cortex microsomes, was studied. The activation energy of the catalyzed reaction was found to be low and constant ($\text{2–5}\text{kcal}\text{·}\text{mol}{}^{\mathrm{?1}}$) in the temperature range 16–40°C at pH 7.5, 8.5 and 9, corresponding to the minimum, intermediate and maximum rate, respectively. A drastic increase of the activation energy ($\text{20}\text{kcal}\text{·}\text{mol}{}^{\mathrm{?1}}$) was observed at temperature below 16°C at pH 7.5. A correlated change of the $\text{p}\text{K}{}_{\mathrm{<mtext>ES</mtext>}}{}^{\mathrm{<mtext>app</mtext>}}$ as function of temperature was detected; at 36°C $\text{p}\text{K}{}_{\mathrm{<mtext>ES</mtext>}}{}^{\mathrm{<mtext>app</mtext>}}\text{= 8.3}$ while at 13°C the value shifted to 8.7. The pH range of the group ionization was narrower at 13°C. In contrast with the behaviour of the $\text{3β-}\text{hydroxy}\text{-Δ}{}^5\text{-}\text{steroid dehydrogenase}$, the $\text{3-}\text{oxosteroid}\text{Δ}{}^5\text{?Δ}{}^4\text{-}\text{isomerase}$ was apparently unaffected by the lipid reorganization at 27°C. It is suggested that this enzyme possesses a different and more fluid lipid environment than the bulk lipids.     

Protein-catalyzed phospholipid exchange in bilayer vesicles determined by flow cytometry and electron microscopy

The protein-induced lipid transfer between phosphatidylcholine vesicles was investigated. Measurements of the degree of polarization at single vesicles were made by flow cytometry using diphenylhexatriene as the optical probe. Vesicles differing in phase transition temperature could be distinguished by their degree of polarization at a temperature where one population was in the fluid ($\text{T > T}{}_{\mathrm{<mtext>t</mtext>}}$) and the other one in the quasi-crystalline ($\text{T < T}{}_{\mathrm{<mtext>t</mtext>}}$) state. Besides vesicles containing exchanged lipids we also observed fractions of unaffected vesicles. The lipid exchange was visualized directly by freeze-fracture electron microscopy. The characteristic ‘ripple’ structure of phosphatidylcholine vesicles disappeared upon exchange with lipid in the fluid state.     

Major intrinsic polypeptide of lens membrane: Biochemical and immunological characterization of the major cyanogen bromide fragment

A protein of $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 has been shown to be the major component of eye-lens junctions, which are similar but not identical to the gap junctions of liver and other tissues. Cyanogen bromide cleavage of the $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 polypeptide from bovine lenses yields a major fragment of $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 15 000 (fragment 1). However, if the junctions are first treated with trypsin or carboxypeptidase Y, cyanogen bromide treatment yields a fragment of reduced molecular weight. Since protease treatment has been shown to cleave residues almost exclusively from the carboxy-terminal end of the $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 polypeptide, it follows that fragment 1 represents the carboxy-terminal half of this molecule, part of which is exposed to proteolytic attack outside the membrane. This latter result is corroborated by the fact that antisera which recognize both the $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 polypeptide and fragment 1 fail to do so after preadsorption with intact membranes. In addition, comparative amino acid and partial sequence analyses of the $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 polypeptide and fragment 1 indicate that fragment 1 is more hydrophilic in character, suggesting that much of the amino-terminal half of the $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 26 000 polypeptide is buried within the lipid bilayer.     

Phospholipid exchange between bilayer membranes

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 Å) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, the other type $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ as predominant acyl chain component. The vesicles show order?disorder transitions at transition temperatures, $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 42°}\text{C}$ and $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 29°}\text{C}$, respectively. A mixture of these vesicles is incubated at 45° C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$-containing lipid molecules appear more rapidly in the $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

Asymmetric or symmetric? Cytosolic modulation of human erythrocyte hexose transfer

(1) The Michaelis-Menten parameters for hexose transfer in erythroctes, erythrocyte ghosts and inside-out vesicles at 20°C were determined using the light scattering method of Sen and Widdas ((1962) J. Physiol. 160, 392–403). (2) The external $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for infinite-cis exit of d-glucose in cells and ghosts is $\text{3.6 ± 0.5}\text{mM}$. (3) Dilution of cellular solute (up to × 90 dilution) by lysing and resealing cells in varying volumes of lysate is without effect on the $\text{V}{}_{\mathrm{<mtext>m</mtext>}}$ for net d-glucose exit. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for net exit, however, falls from $\text{32.4 ± 3.7}\text{mM}$ in intact cells to $\text{12.9 ± 2.3}\text{mM}$ in ghosts. This effect is reversible. (4) Infinite-cis net d-glucose uptake measurements in cells and ghosts reveal the presence of a low $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$, high affinity internal site of $\text{5.9 ± 0.8}\text{mM}$. The $\text{V}{}_{\mathrm{<mtext>m</mtext>}}$ for net glucose entry increases from $\text{23.2 ± 3.7}\text{mmol/l per min}$ in intact cells to $\text{55.4 ± 6.3}\text{mmol/l per min}$ in ghosts. (5) The external $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for infinite-cisd-glucose exit in inside-out vesicles is $\text{6.8 ± 2.7}\text{mM}$. The kinetics of zero-transd-glucose exit from inside-out vesicles are changed markedly when cellular solute (obtained by lysis of intact cells) is applied to either surface of inside-out vesicles. When solute is present externally, the $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ and $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ for zero-trans exit are decreased by up to 10-fold. When solute is present at the interior of inside-out vesicles, $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ for zero-trans exit is reduced; $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for exit is unaffected. In the nominal absence of cell solute, transfer is symmetric in inside-out vesicles. The orientation of transporter in the bilayer is unaffected by the vesiculation procedure. (6) External application of cellular solute to ghosts reduces $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ for d-glucose exit but is without effect on the external $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for infinite-cis exit. (7) The inhibitory potency of cell lysate on hexose transfer is lost following dialysis indicating that the factors responsible for transfer modulation are low molecular weight species. (8) We consider the hexose transfer in human erythrocytes is intrinsically symmetric and that asymmetry of transfer is conferred by interaction of the system with low molecular weight cytosolic factors.     

Fractionation by velocity sedimentation of Torpedo nicotinic post-synaptic membranes

Velocity sedimentation on sucrose gradients containing Torpedo physiological saline has been utilized to fractionate Torpedo (Torpedo californica and T. nobiliana) post-synaptic membranes isolated initially on the basis of their density by equilibrium centrifugation. Membranes are separated into two populations: (1) those retained within the gradient (referred to as gradient pool); and (2) membranes sedimenting rapidly through the gradient (referred to as f 22, fraction 22 of the gradient). Comparison of their polypeptide compositions by sodium dodecyl sulfate/polyacrylamide gel electrophoresis indicates that the gradient pool consists of highly purified nicotinic post-synaptic membranes containing the peptides of the acetylcholine receptor and a peptide of $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 43 000, while f 22 contains the contaminating membranes present in the initial suspension as well as a small fraction of the nicotinic post-synaptic membranes. On the basis of the kinetics of efflux of ²²Na⁺ from the membrane fractions, it is concluded that the gradient pool contains most of the sealed vesicles with functional nicotinic receptors. The internal volume (μl/mg protein) of those membranes exceeds that of f 22 by a factor of 4, and greater than 85% of that internal volume is equilibrated by the nicotinic agonist carbamylcholine, while for f 22 only 40% is equilibrated. Thin-section electron microscopy has been used to estimate the distribution of vesicle sizes. The observed distribution for the gradient pool indicates that these vesicles are a size homogeneous population of diameter 0.3 μm, while f 22 contains a number of smaller and larger vesicles. Torpedo post-synaptic membranes have been treated with alkali to remove the non-receptor peptide of $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 43 000. After alkaline extraction, velocity sedimentation permits the isolation of a population of size-homogeneous and well-sealed vesicles containing only the peptides of the nicotinic receptor. It is concluded that upon homogenization, the innervated surface of the Torpedo electroplax tends to form vesicles of uniform size (0.3 μm) which can be readily isolated by velocity sedimentation and that the peptide of $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ 43 000 is not required for the maintenance of bilayer structure.     

Cooperative unit size in the gel-liquid crytalline phase transition of dipalmitoyl phosphatidylcholine-water multilayers: An estimate from raman spectroscopy

The temperature dependence of the Raman spectral transitions assigned to the acyl chain C-C stretching modes of dipalmitoyl phosphatidylcholine was determined for the gel, phase transition and liquid crystalline states of the lipid multilayers. The van't Hoff enthalpy differences $\text{ΔH}{}_{\mathrm{<mtext>VH</mtext>}}$ between trans and gauche rotational isomers were obtained from the Raman spectral data for the temperature region characteristics of each bilayer state. An average size for the cooperative unit undergoing the chain melting process during the phase transition was estimated from the ratio of the appropriate van't Hoff enthalpy to an adjusted calorimetric enthalpy.     

Identification and partial characterization of plasma membrane polypeptides of Trypanosoma brucei

A plasma membrane-enriched vesicle fraction has been prepared from Trypanosoma brucei by sonication and differential centrifugation on sucrose gradients. This fraction is enriched 5-fold in the plasma membrane marker enzymes adenyl cyclase (EC 4.6.1.1) and ouabain-inhibitable, ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}$)-dependent adenosine triphosphatase (EC 3.6.1.3). It is also enriched up to 14-fold in iodinated surface proteins, and up to 4-fold in [³H]mannose-labeled glycoproteins, of which the major variable surface coat glycoprotein is the main constituent. Proteins of the plasma membrane fraction and other subcellular fractions have been identified by electrophoretic analysis in sodium dodecyl sulfate-polyacrylamide gradient slab gels. Several high molecular weight surface glycopeptides have been selectively investigated and partially characterized by a combination of metabolic labeling with [³H]mannose, lactoperoxidase-catalyzed surface iodination, and affinity chromatography on Con A-Sepharose. In addition to the major variable surface coat glycoprotein (estimated $\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{= 58 000}$), there are several minor surface glycopeptides ($\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{= 76 000, 86 000}\text{and}\text{92 000–100 000}$) which are apparent extrinsic membrane components, and two surface glycopeptides ($\text{M}{}_{\mathrm{<mtext>r</mtext>}}\text{= 42 000}\text{and}\text{130 000}$) which are intrinsic membrane components.     

A restatement of melittin-induced effects on the thermotropism of zwitterionic phospholipids

Perturbations induced by melittin on the thermotropism of dimyristoyl-, dipalmitoyl-, distearoylphosphatidylcholine and natural sphingomyelin are investigated and rationalized from data obtained by fluorescence polarization, differential scanning calorimetry and Raman spectroscopy. Depending on the technique and / or experimental conditions used, the observed effects differ at the same lipid to protein molar ratio, due to partial binding of melittin. The binding is more efficient for tetrameric than for monomeric melittin, but in both cases its affinity is weaker for phosphatidylcholine dispersions in the gel phase than for sonicated vesicles. For temperatures $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$ efficient binding occurs whatever the initial state of the lipids is. One can summarize the effects induced by melittin on the transition temperature as follows: (i) No upward shift is observed on synthetic phosphatidylcholines when lipid degradation is avoided. This is achieved by using highly purified melittin, phospholipase inhibitors, and / or non-hydrolysable lipids. (ii) Melittin monomer does not change $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$. (iii) When melittin tetramer is stabilized, it decreases $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ by 10–15 deg. C. The transition broadens, and is finally abolished for $\text{R}{}_{\mathrm{<mtext>i</mtext>}}\text{? 2}$. Very similar results are found for natural sphingomyelin. Fluorescence polarization indicates similar changes in order and dynamics of the acyl chains for all lipid studied. For $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$, fluorescence and Raman show that melittin decreases the amount of CH₂ groups in ‘trans’ conformation and the intermolecular order of the chains. According to fluorescence data, there is an increase of the rigid-body orientational order at $\text{T ? T}{}_{\mathrm{<mtext>m</mtext>}}$, while from Raman the positional intermolecular order decreases without significant change in the CH₂ groups ‘trans’/‘gauche’ ratio.     

A chloride requirement for Na+-dependent amino-acid transport by brush border membrane vesicles isolated from the intestine of a mediterranean teleost (Boops salpa)

The uptake of d-glucose, 2-aminoisobutyric acid and glycine was studied with intestinal brush border membrane vesicles of a marine herbivorous fish: Boops salpa. The uptake of these three substances is stimulated by an Na⁺ electrochemical gradient ($\text{C}{}_{\mathrm{<mtext>out</mtext>}}\text{C}{}_{\mathrm{<mtext>in</mtext>}}$). For glucose, an increase of the electrical membrane potential generated by a concentration gradient of the liposoluble anion, SCN^?, increases the Na⁺-dependent transport. This responsiveness to the membrane potential was confirmed by valinomycin. Differently from glucose, uptake of glycine and 2-aminoisobutyric acid requires, besides the Na⁺ gradient, the presence of Cl^? on the external side of the vesicles. In the absence of Cl^?, amino acid uptake is not stimulated by the Na⁺ gradient and is not influenced by an electrical membrane potential generated by SCN^? gradient ($\text{C}{}_{\mathrm{<mtext>out</mtext>}}\text{>C}{}_{\mathrm{<mtext>in</mtext>}}$) or by a K⁺ diffusion potential ($\text{C}{}_{\mathrm{<mtext>in</mtext>}}\text{>C}{}_{\mathrm{<mtext>out</mtext>}}$). This Cl^? requirement differs from the Na⁺ requirement, since a Cl^? gradient ($\text{C}{}_{\mathrm{<mtext>out</mtext>}}\text{>C}{}_{\mathrm{<mtext>in</mtext>}}$) does not result in an accumulation of glycine or 2-aminoisobutyric acid similar to that produced by an Na⁺ gradient.     

Soluble and enzymatically stable (Na++K+)-ATPase from mammalian kidney consisting predominantly of protomer αβ-units: Preparation,assay and reconstitution of active Na+, K+transport

Soluble $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$ consisting predominantly of αβ-units with $\text{M}{}_{\mathrm{<mtext>r</mtext>}}$ below 170 000 was prepared by incubating pure membrane-bound $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$ (35–48 μmol P_i/min per mg protein) from the outer renal medulla with the non-ionic detergent dodecyloctaethyleneglycol monoether (C₁₂E₈). $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$ and potassium phosphatase remained fully active in the detergent solution at C₁₂E₈/protein ratios of 2.5–3, at which 50–70% of the membrane protein was solubilized. The soluble protomeric $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$ was reconstituted to Na⁺, K⁺ pumps in phospholipid vesicles by the freeze-thaw sonication procedure. Protein solubilization was complete at C₁₂E₈/protein ratios of 5–6, at the expense of partial inactivation, but $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$ and potassium phosphatase could be reactivated after binding of C₁₂E₈ to Bio-Beads SM2. At C₁₂E₈/protein ratios higher than 6 the activities were irreversibly lost. Inactivation could be explained by delipidation. It was not due to subunit dissociation since only small changes in sedimentation velocities were seen when the C₁₂E₈/protein ratio was increased from 2.9 to 46. As determined immediately after solubilization, $\text{S}{}_{\mathrm{<mtext>20,</mtext><mtext>w</mtext>}}$ was 7.4 S for the fully active $\text{(Na}{}^{\mathrm{+}}\text{+K}{}^{\mathrm{+}}\text{)-ATPase}$, 7.3 S for the partially active particle, and 6.5 S for the inactive particle at high C₁₂E₈/protein ratios. The maximum molecular masses determined by analytical ultracentrifugation were 141 000–170 000 dalton for these protein particles. Secondary aggregation occurred during column chromatography, with formation of enzymatically active $\text{(αβ)}{}_2\text{-}\text{dimers}$ or $\text{(αβ)}{}_3\text{-}\text{trimers}$ with $\text{S}{}_{\mathrm{<mtext>20,</mtext><mtext>w</mtext>}}\text{=10–12}$ S and apparent molecular masses in the range 273 000–386 000 daltons. This may reflect non-specific time-dependent aggregation of the detergent micelles.     

The affinity of bacterial polysaccharide-containing fractions for mammalian cell membranes and its relationship to immunopotentiating activity

The natural affinity of various bacterial glycopeptides and lipopolysaccharides for mammalian cell membranes was estimated quantitatively by comparison with the adsorption of lipopolysaccharide from Escherichia coli NCTC 8623 to erythrocytes, thymocytes, bone marrow cells, spleen cells, peritoneal lymphocytes and macrophages. Immunopotentiating activity was estimated by measuring the ability of the bacterial fractions to stimulate a humoral response to ovalbumin in HAM/1CR mice. When the affinity for mammalian cell membranes was compared with the stimulation of the antibody response, it was found that a negative correlation for peritoneal macrophages ($\text{r}{}_{\mathrm{<mtext>s</mtext>}}\text{=?0.94, P<0.0005}$) and a positive correlation for peritoneal lymphocytes ($\text{r}{}_{\mathrm{<mtext>s</mtext>}}\text{=+0.97,P<0.0005}$) and spleen cells ($\text{r}{}_{\mathrm{<mtext>s</mtext>}}\text{=+0.76,P<0.005}$) existed.