The inhibition of erythrocyte glyceraldehyde-3-phosphate dehydrogenase. In situ PMR studies

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 (t 1/2) 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 micron 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 t 1/2 values for plasma membrane vesicles of Fu5AH and WIRL cells are 3.9 +/- 0.5 and 11.2 +/- 0.7 h, respectively. These t 1/2 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 rates 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 t 1/2 values for cholesterol efflux from these cell lines.     

The characterization of energized and partially de-energized (respiration-independent) β-galactoside transport into escherichia coli

Unidirectional fluxes of [¹⁴C]lactose by whole cells of Escherichia coli under highly energized and partially de-energized (in the presence of CN^?) conditions are analyzed kinetically.When the cells are energized, the value for $\text{V}$ influx is $\text{0.45 ± 0.01}\text{mM}$ internal concentration increment/s and $\text{K}{}_{\mathrm{t}}$ is $\text{0.26 ± 0.03}\text{mM}$. At an external concentration of 0.61 mM the steady-state internal concentration is 0.25 M, reached after about 1h. The maximum steady-state concentration ratio is $\text{2 · 10}{}^3$.The efflux process under these conditions is non-saturable, being linearly dependent upon internal concentration over the range 25–250 mM with a first-order rate constant of $\text{8.8 ± 0.2 · 10}{}^{\mathrm{?4}}\text{s}{}^{\mathrm{?1}}$.The transport in the presence of CN^? is active, with a maximum concentration ratio (internal concentration/external concentration) of 104, and the uptake is mimicked by anoxia (< 70 ppm O₂).The effects of CN^? are to lower the $\text{V}$ for influx and to change the efflux from a non-saturable to a saturable process with a value for $\text{K}{}_{\mathrm{t}}$ (60 mM) intermediate between that for energized efflux ($\text{> 250}\text{mM}$) and influxe (0.3–0.6 mM), the latter value not changing appreciably. Partial de-energization thus affects both the influx and efflux processes.     

Effect of metabolic acidosis on phosphate transport by the renal brush-border membrane

Metabolic acidosis produces a phosphaturia which is independent of parathyroid hormone or dietary phosphorus intake. To study the underlying mechanism, inorganic phosphate (P_i) and glucose transport were studied in brush-border membrane vesicles prepared from the renal cortex of parathyroidectomized rats gavaged for three days with either 7.5 ml of 1.6% NaCl (control) or 1.5% NH₄Cl (acidosis). At killing, blood pH and plasma bicarbonate were $\text{7.36 ± 0.01}$ and $\text{21.8 ± 0.8}\text{mequiv./l}$, respectively, in control and $\text{7.12 ± 0.03}$ ($\text{P < 0.01}$) and $\text{11.1 ± 1.2}$ ($\text{P < 0.01}$) in acidotic rats. Serum P_i was similar in both groups, while 24 h urine P_i excretion was higher in the acidotic group ($\text{P < 0.01}$). Peak sodium-dependent uptake of P_i, measured after 1.5 min of incubation, was higher in controls than acidotic rats ($\text{4442 ± 464}$ vs. $\text{2412 ± 259}\text{pmol/mg}$ protein, $\text{P < 0.01}$), whereas peak glucose uptake at 1.5 min was not significantly different between the groups. Equilibrium values for P_i and glucose uptake were similar in the two groups. $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for P_i uptake in the control and acidotic animals were not different, 0.036 and 0.040 mM, respectively. By contrast, $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ was higher in controls than in the acidotic group, 3.13 vs. 1.15 nmol/mg protein per 15 s. These results suggest that metabolic acidosis directly inhibits P_i uptake by the brush border of the proximal tubule by decreasing the availability of P_i carriers of the renal brush-border membrane.     

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.     

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.     

Stimulation of respiration-linked proton efflux in Escherichia coli by carbonylcyanide-p-trifluoromethoxyphenylhydrazone (FCCP).

The proton efflux from intact, anaerobic $\text{Escherichia}\text{coli}$ cells following a small oxygen pulse is both slow ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>M</mtext><mtext>2</mtext>}}\text{～-10s}$) and inefficient ($\text{H}{}^{\mathrm{+}}\text{O}\text{～-0.5}$. Very low levels (<80 nM) of the proton ionophore carbonylcyanide-$\text{p}$-trifluoromethoxyphenylhydrazone (FCCP), which have no detectable effect upon active transport, cause a 3–5 fold stimulation in the extent of proton efflux without affecting the efflux rate. At slightly higher concentrations of FCCP (80 nM to 0.5 μM), a sharp inhibition of this increased proton efflux occurs, with the $\text{H}{}^{\mathrm{+}}\text{O}$ ratio obtained in the presence of 0.5 μM FCCP approximately equal to that obtained in the absence of FCCP. Still higher concentrations of FCCP (> 1 μM), which inhibit active transport, cause a further gradual decrease in the $\text{H}{}^{\mathrm{+}}\text{O}$ ratio. The unusual increase in the apparent efficiency of H⁺ efflux by <80 nM FCCP is not accompanied by an increase in the rate of membrane deenergization following an O₂ pulse, although such an increase is seen with the higher (uncoupling) FCCP concentrations.     

Cytochrome b5/cytochrome b5 reductase interaction in microsomes: kinetics at subzero temperature.

The cytochrome $\text{b}{}_5\text{b}{}_5$ reductase system solubilized from microsomes exhibits monophasic reduction kinetics over the temperature range 15 ° to ?25 °C in aqueous/ethylene glycol co-solvent, whereas in intact microsomes, the process becomes increasingly heterogeneous below 0 °C, reflecting heterogeneities in membrane structure observable as distributions in reaction rates and activation energies.     

Cyclic AMP transport in human erythrocyte ghosts

10^?5 M cyclic AMP has high permeability in human erythrocyte ghosts ($\text{p = 0.061 · 10}{}^{\mathrm{?6}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$). Saturation of influx and efflux occurs. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>oi</mtext>}}\text{= 4.43}\text{mM}$. $\text{V}{}_{\mathrm{zt}}{}^{\mathrm{oi}}\text{= 259.6 μ}\text{M · min}{}^{\mathrm{?1}}$. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 0.475 μ}\text{M}$. $\text{V}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 28.3 μ}\text{M · min}{}^{\mathrm{?1}}$ at 30°C. Equilibrium exchange entry of cyclic AMP has similar kinetics to zero trans influx, though the system does show counterflow. Cythochalasin B is an apparent competitive inhibitor of cyclic AMP exit. ($\text{K}{}_{\mathrm{<mtext>i</mtext>}}\text{= 3.9 · 10}{}^{\mathrm{?7}}\text{M}$).Control experiments indicated that cyclic AMP remains intact during incubation with red blood cell ghosts and is contained within the intravesicular space during the transport experiments.     

Determination of the kinetic constants of fructose transport and phosphorylation in the perfused rat liver

The kinetics of fructose uptake was determined in perfused rat liver during steady-state fructose elimination. On the basis of the corresponding values of fructose concentration in the affluent and in the effluent medium, and the fructose and ATP concentration in biopsies, the kinetics of membrane transport and intracellular phosphorylation in the intact organ was calculated according to a model system. Carrier-mediated fructose transport has a high $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ (67 mM) and $\text{V}$ (30 μmoles · min^?1 ·g^?1). The calculated kinetic constants of the intracellular phosphorylation were compared with values obtained with an acid-treated rat liver high speed supernatant (values given in parentheses). $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ with fructose 1.0 mM (0.7 mM), $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ with ATP 0.54 mM (0.37 mM), $\text{V}$ 10.3 μmoles · min^?1 · g^?1 (10.1 μmoles · min^?1 · g^?1, calculated on the basis of the highest measured rate of fructose uptake correcting the ATP concentration to saturating values). The kinetics of fructose uptake reveals that at Physiological fructose concentrations the membrane transport limits the rate of fructose uptake, thus protecting the liver from severe depletion of adenine nucleotides.     

The effect of prostaglandins E1 and E2 on the human erythrocyte as monitored by spin labels

The effects of the prostaglandins PGE₁ and PGE₂ on the deformability of the human erythrocyte were studied using spin-labeled erythrocytes. Two magnetic resonance parameters were measured: (1) The orientation relaxation time, $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, for the erythrocyte, and (2) the order parameter, S, for a fatty acid spin label bound to the membrane. Prostaglandins PGE₁ and PGE₂ exhibited opposite effects on both $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ and S. PGE₂ made the cell less deformable (increases of $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ and S) and PGE₁ made the erythrocyte more deformable (decrease of $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ and S).     

Identification of Ca2+-pump-related phosphoprotein in plasma membrane vesicles of Ehrlich ascites carcinoma cells

Plasma membrane vesicles of Ehrlich ascites carcinoma cells have been isolated to a high degree of purity. In the presence of Mg²⁺, the plasma membrane preparation exhibits a Ca²⁺-dependent ATPase activity of 2 μmol P_i per h per mg protein. It is suggested that this $\text{(}\text{Ca}{}^{\mathrm{2+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{)-}\text{ATPase}$ activity is related to the measured Ca²⁺ transport which was characterized by $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ values for ATP and Ca²⁺ of $\text{44 ± 9 μ}\text{M}$ and $\text{0.25 ± 0.10 μ}\text{M}$, respectively. Phosphorylation of plasma membranes with [γ-³²P]ATP and analysis of the radioactive species by polyacrylamide gel electrophoresis revealed a Ca²⁺-dependent hydroxylamine-sensitive phosphoprotein with a molecular mass of 135 kDa. Molecular mass and other data differentiate this phosphoprotein from the catalytic subunit of $\text{(}\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ and from the catalytic subunit of $\text{(}\text{Ca}{}^{\mathrm{2+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{)-}\text{ATPase}$ of endoplasmic reticulum. It is suggested that the 135 kDa phosphoprotein represents the phosphorylated catalytic subunit of the $\text{(}\text{Ca}{}^{\mathrm{2+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{)-}\text{ATPase}$ of the plasma membrane of Ehrlich ascites carcinoma cells. This finding is discussed in relation to previous attempts to identify a Ca²⁺-pump in plasma membranes isolated from nucleated cells.     

Phospholipid methylation of kidney cortex brush border membranes. Effect on fluidity and transport

Exposure of intact brush border membrane vesicles of hog kidney cortex to cholesterol oxidase resulted in 24% oxidation of membrane cholesterol compared with more than 95% oxidation of cholesterol in lipids isolated from membranes, showing that cholesterol is asymmetrically distributed in membranes. Phospholipase C, hydrolyzed 76% of phosphatidylcholine and 10–12% phosphatidylethanolamine while phosphatidylserine was not hydrolyzed, thus indicating that majority of phosphatidylcholine is present on the outer surface of these vesicles while phosphatidylethanolamine and phosphatidylserine are present on the inner surface. Methylation of phospholipids in brush border membrane with $\text{S-}\text{adenosyl}\text{-[methyl-}{}^3\text{H}\text{]}\text{methionine}$ resulted in the formation of $\text{phosphatidyl}\text{-N-}\text{monomethylethanolamine}$, $\text{phosphatidyl}\text{-N,N-}\text{dimethylethanolamine}$ and phosphatidylcholine from endogenous phosphatidylethanolamine. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for $\text{S-}\text{adenosylmethionine}$ was 1·10^?4 M with an optimum pH 9.0 for the formation of all three methyl derivatives. Mg²⁺ was without any effect between pH 5 to 10. Addition of exogenous mono- and dimethylphosphatidylethanolamine derivatives enhanced methyl group incorporation by 4–5-fold as compared to the addition of phosphatidylethanolamine. The conversion of endogenous phosphatidylethanolamine to $\text{phosphatidyl}\text{-N-}\text{monomethylethanolamine}$ or addition of exogenous phosphatidylmonomethylethanolamine to brush border membrane did not result in a change in bulk membrane fluidity as determined by fluorescence polarization of diphenylhexatriene. Methylation of phosphatidylethanolamine in brush border membrane did not affect the Na⁺-dependent uptake of either d-glucose or phosphate, although the accessibility of cholesterol in membrane to cholesterol oxidase was diminished by 21%, presumably due to altered flip-flop movement of cholesterol in the membrane.     

Oxidative phosphorylation by membrane vesicles from Bacillus alcalophilus

ADP and P_i-loaded membrane vesicles from l-malate-grown Bacillus alcalophilus synthesized ATP upon energization with $\text{ascorbate}\text{N,N,N′,N′-}\text{tetramethyl}\text{-p-}\text{phenylenediamine}$. ATP synthesis occurred over a range of external pH from 6.0 to 11.0, under conditions in which the total protonmotive force was as low as ?30 mV. The phosphate potentials (ΔG_p) were calculated to be 11 and 12 kcal/mol at pH 10.5 and 9.0, respectively, whereas the values in vesicles at these two pH values were quite different (?40 ± 20 mV at pH 10.5 and ?125 ± 20 mV at pH 9.0). ATP synthesis was inhibited by KCN, gramicidin, and by N,N′-dicyclohexylcarbodiimide. Inward translocation of protons, concomitant with ATP synthesis, was demonstrated using direct pH monitoring and fluorescence methods. No dependence upon the presence of Na⁺ or K⁺ was found. Thus, ATP synthesis in B. alcalophilus appears to involve a proton-translocating ATPase which functions at low .     

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.     

New experimental approach to the estimation of rate of electron transfer from the primary to secondary acceptors in the photosynthetic electron transport chain of purple bacteria

A method for calculating the rate constant ($\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$) for the oxidation of the primary electron acceptor (A₁) by the secondary one (A₂) in the photosynthetic electron transport chain of purple bacteria is proposed.The method is based on the analysis of the dark recovery kinetics of reaction centre bacteriochlorophyll (P) following its oxidation by a short single laser pulse at a high oxidation-reduction potential of the medium. It is shown that in Ectothiorhodospira shaposhnikovii there is little difference in the value of $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ obtained by this method from that measured by the method of Parson ((1969) Biochim. Biophys. Acta 189, 384–396), namely: $\text{(4.5±1.4) · 10}{}^3\text{s}{}^{\mathrm{?1}}$ and $\text{(6.9±1.2) · 10}{}^3\text{s}{}^{\mathrm{?1}}$, respectively.The proposed method has also been used for the estimation of the $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ value in chromatophores of Rhodospirillum rubrum deprived of constitutive electron donors which are capable of reducing P⁺ at a rate exceeding this for the transfer of electron from A₁ to A₂. The method of Parson cannot be used in this case. The value of $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ has been found to be $\text{(2.7±0.8) · 10}{}^3\text{s}{}^{\mathrm{?1}}$.The activation energies for the A₁ to A₂ electron transfer have also been determined. They are 12.4 kcal/mol and 9.9 kcal/mol for E. shaposhnikovii and R. rubrum, respectively.     

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.     

Differential polarized phase fluorometric studies of phospholipid bilayers under high hydrostatic pressure

Differential polarized phase fluorometry was used to quantify the rotational rate ($\text{R}$) and limiting anisotropy ($\text{r}{}_{\mathrm{\infty }}$) of the membrane probe diphenylhexatriene (DPH) in solvents and lipid vesicles exposed to hydrostatic pressures ranging from 1 bar to 2 kbar. These measurements reveal the effect of pressure on the phase-transition temperatures of the phosphatidylcholine vesicles, and the effects of pressure on order parameter of the acyl side-chain region of the membranes, the latter as indicated by $\text{r}{}_{\mathrm{\infty }}$. In addition to the well-known elevation of the transition temperature ($\text{T}{}_{\mathrm{<mtext>c</mtext>}}$) with pressure, our results demonstrate that increased pressure restores the order of the bilayers to that representative of temperatures below the transition temperature. We also found that solvents which allowed free isotropic rotation of DPH at 1 bar no longer allowed free rotation when sufficiently compressed; moreover, the apparent DPH rotational rate increased with $\text{r}{}_{\mathrm{\infty }}$. Pressure studies using both DPH and the charged DPH analogue, trimethylammonium DPH (TMA-DPH) indicated that the $\text{T}{}_{\mathrm{<mtext>c</mtext>}}$ of dipalmitoylphosphatidylcholine vesicles increased 23 K/kbar and an apparent volume change of 0.036 ml/mol lipid at the phase transition. Assuming, as has been proposed, that TMA-DPH is localized near the glycerol backbone region of the bilayers, these results indicate a similar temperature- and pressure-dependent phase transition in this region and the acyl side-chain region of the membrane.     

The polymorphic phase behaviour and miscibility properties of synthetic phosphatidylethanolamines

(1) The polymorphic phase behaviour of aqueous dispersions of various synthetic phosphatidylethanolamines, both singly and in mixtures, has been investigated by ³¹P-NMR. (2) $\text{14:0}\text{14:0}$ PE remains in the lamellar phase up to 90°C. $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibits a lamellar to hexagonal (H_II) transition between 60°C and 63°C. For $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE, the lamellar to hexagonal (H_II) transition occurs between 7 and 12°C, whereas for $\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}$ PE, the hexagonal (H_II) phase is the preferred structure above ?15°C. (3) Mixtures of $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibit near-ideal miscibility behaviour. For mixtures of $\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}\text{18:1}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{14:0}\text{14:0}$ PE there is evidence of fluid-solid immiscibility at temperatures below the gel-liquid crystalline transition temperature of the $\text{14:0}\text{14:0}$ PE component. Mixtures of $\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}\text{18:2}{}_{\mathrm{<mtext>c</mtext>}}$ PE and $\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}\text{18:1}{}_{\mathrm{<mtext>t</mtext>}}$ PE exhibit complex phase behaviour involving limited fluid-solid immiscibility at low temperatures and formation of a phase allowing isotropic motional averaging at higher temperatures. (4) ³¹P-NMR provides a graphic method for investigating the miscibility properties of mixed PE systems.