The effects of membrane lipid order and cholesterol on the internal and external cationic sites of the Na+−K+ pump in erythrocytes

Cholesterol depletion alters the apparent affinity of the internal cationic sites and the maximal translocation rate but not the affinity of the external cationic sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump in human erythrocytes. To test whether these effects were mediated by a direct cholesterol-internal site interaction or by a change in membrane lipid order, the effects of five fluidizing amphiphiles (chlorpromazine, imipramine, benzyl alcohol, sodium oleate and sodium benzenesulphonate) on the kinetic parameters of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump were determined. The cholesterol removal and all the agents used induced dose-response decreases in membrane lipid order as measured by fluorescence polarization or ESR. Positive and neutral amphiphiles mimicked the effects of cholesterol removal on the affinity of the internal sites of the pump and to a lesser extent on the maximal translocation rate. Anionic amphiphiles had no effect on internal sites, probably because they distributed preferentially within the outer leaflet on the membrane. These results indicate that cholesterol controls the affinity of the internal sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump by altering the membrane lipid order. In contrast, neither cholesterol depletion nor the agents used altered the affinity of the external sites of the $\text{Na}{}^{\mathrm{+}}\text{?K}{}^{\mathrm{+}}$ pump. This difference in sensitivity to membrane lipid order suggests that internal and external cationic sites, although borne by the same protein, are in different lipid environments.     

Local measurement of lateral motion in erythrocyte membranes by photobleaching technique

The lateral diffusion coefficients ($\text{D}$) of the molecular fluorescence probe 3,3′-dioctadecylindocarbocyanine iodide (DII) in the membrane of discoid erythrocyte ghosts has been measured with the photobleaching technique between 7°C and 40°C. A fluorescence microscope which allows bleaching experiments within small local fields (approx. 1 μm²) at high magnification (X1600) has been used for these measurements. The diffusion coefficient increases from $\text{D = 9 · 10}{}^{\mathrm{?10}}\text{cm}{}^2\text{/s}$ to $\text{D = 7.5 · 10}{}^{\mathrm{?9}}\text{cm}{}^2\text{/s}$ from 7 to 40°C. An increase in membrane fluidity between 12°C and 17°C indicates a conformational change of the lipid bilayer moiety in this temperature region. The diffusion coefficient measured in the regions between the spicules of echinocytes is appreciably smaller than in the untransformed discoid ghosts. In the myelin tubes originating from cells, the lateral diffusion is somewhat larger (about a factor of 2) than in the non-transformed ghosts. With the fluorescence probe technique the rate of growth of myelin tubes of 0.3 μm diameter has been estimated.     

Incorporation into lipid bilayer membranes of a photo-sensitive pigment from the honeybee compound eye

An increase of electrical conductance up to a factor $\text{10}{}^2\text{-5·10}{}^2$ was obtained by adding, in the dark, the honeybee photopigment to a positively charged lipid bilayer. The increase in conductance was made slower by illuminating the system during the incorporation of the protein into the membrane and it was negligible when the photopigment was bleached before the incorporation. The interaction of the photopigment with the membrane is tentatively interpreted in terms of formation of channels.     

Effect of angiotensin II on artificial lipid membranes

(5-Isoleucine)-angiotensin II applied to black lipid membranes produced current fluctuations varying between $\text{Δ>G = 5 · 10}{}^{\mathrm{?11}}\text{Ω}{}^{\mathrm{?}}$ and 3.5 · 10^?10 Ω^?1. These fluctuations depend on the voltage and the hydrostatic pressure. The membrane resistance is lowered by $\text{Δ>R = 6.1 · 10}{}^7\text{Ω · cm}{}^2$. With (5-isoleucine, 8-leucine)-angiotensin II the jumps are of a single amplitude ($\text{Δ>G = 2 · 10}{}^{\mathrm{?10}}\text{Ω}{}^{\mathrm{?1}}$). In both cases water and ions are transported across the membrane.     

Effects of insulin on the lipid structure of liver plasma membrane measured with fluorescence and ESR spectroscopic methods

Insulin increased the lipid order of rat and mouse liver plasma membrane domains sampled by the hydrophobic fluorescent probe 1,6-diphenyl-1,3,5-hexatriene in a concentration-dependent saturable manner. The ordering is half maximal at $\text{5.1 · 10}{}^{\mathrm{?11}}\text{M}$ and fully saturated at $\text{1.7 · 10}{}^{\mathrm{?10}}\text{M}$ insulin. Membranes prepared from obese hyperglycemic (ob / ob) mice demonstrated a right-shift in the dose-dependent ordering induced by insulin, such that ordering was half maximal at $\text{1.2 · 10}{}^{\mathrm{?10}}\text{M}$ and fully saturated at $\text{2.0 · 10}{}^{\mathrm{?10}}\text{M}$. Insulin also increased the order of rat liver plasma membranes labeled with the cis- and trans-parinaric acid methyl esters. The ordering caused by insulin as detected with cis methyl parinarate was complete within approx. 15 min. after hormone addition at 37°C, and the ordering was approximately double that observed with the trans isomer. Additional ESR experiments demonstrated that the addition of insulin increased the outer hyperfine splittings of spectra recorded from membranes labeled with the steroid-like spin labels, nitroxide cholestane and nitroxide androstane, but not the fatty acid spin probe, 5-nitroxide stearate. Studies utilizing model membrane systems strongly suggest that the 5-nitroxide stearate samples a cholesterol-poor domain of the membrane, while the steroid-like probes preferentially sample cholesterol-rich regions of the membrane. Finally, insulin-induced membrane ordering was dose-dependently inhibited by cytochalasin B in the range 1–50 μM. From these results, we conclude that (1) the ordering effect of insulin addition to isolated liver plasma membrane fractions occurs within the physiological range of hormone concentration, and the dose-response is right-shifted in membranes from ‘insulin resistant’ animals; (2) the relative responses of the fluorescent and spin probes suggest that the effects of insulin are confined to specific domains within the membrane matrix; and (3) the direct effects of insulin on the membranes may involve protein components having cytochalasin B binding sites.     

Kinetics of phospholipid exchange between bilayer membranes

In an accompanying publication by Duckwitz-Peterlein, Eilenberger and Overath ((1977) Biochim. Biophys. Acta 469, 311–325) it is shown that the exchange of lipid molecules between negatively charged vesicles consisting of total phospholipid extracts from Escherichia coli occurs by the transfer of single lipid monomers or small micelles through the water. Here a kinetic interpretation is presented in terms of a rate constant, $\text{k}{}_{\mathrm{?}}$, for the escape of lipid molecules from the vesicle bilayer into the water. The evaluated rate constants are $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>P</mtext>}}\text{= (0.86 ± 0.05) · 10}{}^{\mathrm{?5}}\text{s}{}^{\mathrm{?1}}$ and $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>E</mtext>}}\text{= (1.09 ± 0.13) · 10}{}^{\mathrm{?6}}\text{s}{}^{\mathrm{?1}}$ for phospholipid molecules with $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ and $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, respectively, as the predominant acyl chain component. The rate constants are discussed in terms of the acyl chain and polar head group composition of the lipids.     

Voltage-induced conductance in human erythrocyte membranes

Isotonic suspensions of erythrocytes were exposed to intense electric fields for a duration in microseconds. Time-dependent increase in the conductivity of the suspension was observed under fields greater than a threshold of about 1.5 kV/cm. The threshold was independent of the ionic strength of the medium, and changed little with temperature or with the rise time of the applied field. Under fields greater than 3 kV/cm, the time course of the conductivity increase consisted of a rapid (approx. 1 μs) and a slow (approx. 100 μs) phases. The increase is attributed primarily to large membrane conductance induced by the applied field. The membrane conductance is in the order of $\text{10 Ω}{}^{\mathrm{?1}}\text{/}\text{cm}{}^2$ in the rapid phase and $\text{10}{}^2\text{Ω}{}^{\mathrm{?1}}\text{/}\text{cm}{}^2$ in the slow phase. Comparison with previous results indicates that this induced membrane conductance corresponds to the formation of aqueous pores in the cell membrane. After the applied field was removed, the conductivity of the suspension returned nearly to its initial value, indicating that the induced membrane conductance is strongly dependent on the membrane potential. The conductivity then increased again in the time range of 10 s. This is attributed to the diffusional efflux of intracellular ions through the voltage-induced pores. From the rate of the efflux, number of the pores/cell is estimated to be in the order of 10². Final stage of the conductivity change was a slow decrease, corresponding to the colloid osmotic swelling of the perforated cells.     

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.     

The non-covalent binding of benzo[a]pyrene and its hydroxylated metabolites to intracellular proteins and lipid bilayers

The non-covalent interactions of benzo[a]pyrene (BP) and several of its hydroxylated metabolites with ligandin, aminoazodye-binding protein A (Z-protein, fatty acid binding protein) and lecithin bilayers have been studied by equilibrium dialysis, an adsorption technique and fluorescence spectroscopy. Binding affinities expressed as $\text{v}\text{/c}$ (where $\text{v}$ = moles of BP or BP metabolite bound per mole of protein or lipid and c = unbound concentration), were measured at concentrations sufficiently low that there was no self-association of the unbound compounds as judged by their fluorescence characteristics. 3-Hydroxybenzo[a]pyrene (BP-3-phenol), 4,5-dihydro-4,5-dihydroxybenzo[a]pyrene (BP-4,5-dihydrodiol) and 7,8-dihydro-7,8-dihydroxybenzo[a]pyrene (BP-7,8-dihydrodiol) bind more strongly ($\text{v}\text{/c = 10}{}^5\text{?5 · 10}{}^5\text{l}\text{·}\text{mol}{}^{\mathrm{?1}}$) to all three binders than does BP itself ($\text{v}\text{/c = 10}{}^4\text{?7 · 10}{}^4\text{l}\text{·}\text{mol}{}^{\mathrm{?1}}$). 9,10-Dihydro-9,10-dihydroxybenzo[a]pyrene (BP-9,10-dihydrodiol) binds to ligandin with an affinity similar to those of the other BP metabolites studied here, but binds much less strongly to both protein A and lecithin ($\text{v}\text{/c = 10}{}^4$ and 3 · 10⁴ l · mol^?1, respectively). The low affinity of BP-9,10-dihydrodiol for lecithin would account for earlier findings that on incubation of BP with isolated rat hepatocytes, this metabolite egressed from the cells to the extracellular medium much more readily than either BP-4,5-dihydrodiol or BP-7,8-dihydrodiol.Calculations based on these results suggest that within hepatocytes BP and its metabolites, including BP-9,10-dihydrodiol, will be found almost exclusively associated (>98%) with lipid membranes.     

Histamine,theophylline and tryptamine transport through lipid bilayer membranes

Diffusion of histamine, theophylline and tryptamine through planar lipid bilayer membranes was studied as a function of pH. Membranes were made of egg phosphatidylcholine plus cholesterol (1 : 1 mol ratio) in tetradecane. Tracer fluxes and electrical conductances were used to estimate the permeabilities to nonionic and ionic species. Only the nonionic forms crossed the membrane at a significant rate. The membrane permeabilities to the nonionic species were: histamine, $\text{3.5 · 10}{}^{\mathrm{?5}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; theophylline, $\text{2.9 · 10}{}^{\mathrm{?4}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; and tryptamine, $\text{1.8 · 10}{}^{\mathrm{?1}}\text{cm}\text{· s}{}^{\mathrm{?1}}$. Chemical reactions in the unstirred layers are important in the transport of tryptamine and theophylline, but not histamine. For example, as pH decreased from 10.0 to 7.5 the ratio of nonionic (B) to ionic (BH⁺) tryptamine decreased by 300-fold, but the total tryptamine permeability decreased only 3-fold. The relative insensitivity of the total tryptamine permeability to the ratio, [B]/[BH⁺], is due to the rapid interconversion of B and BH⁺ in the instirred layers. Our model describing diffusion and reaction in the unstirred layers can explain some ‘anomalous’ relationships between pH and weak acid/base transport through lipid bilayer and biological membranes.     

Structure and action of heteronemertine polypeptide toxins Binding of cerebratulus lacteus toxin B-IV to axon membrane vesicles

The binding of the crustacean selective protein neurotoxin, toxin B-IV, from the nemertine Cerebratulus lacteus to lobster axonal vesicles has been studied. A highly radioactive, pharmacologically active derivative of toxin B-IV has been prepared by reaction with Bolton-Hunter reagent. Saturation binding and competition of ¹²⁵I-labeled toxin B-IV by native toxin B-IV have shown specific binding of ¹²⁵I-labeled toxin B-IV to a single class of binding sites with a dissociation constant of 5–20 nM and a binding site capacity, corrected for vesicle sidedness, of 6–9 pmol per mg membrane protein. This compares to a value of 3.8 pmol [³H]saxitoxin bound per mg in the same tissue. Analysis of the kinetics of toxin B-IV association ($\text{k}{}_{\mathrm{+1}}\text{=7.3·10}{}^5\text{M}{}^{\mathrm{?1}}\text{·s}{}^{\mathrm{?1}}$) and dissociation ($\text{k}{}_{\mathrm{?\; 1}}\text{=2·10}{}^{\mathrm{?3}}\text{s}{}^{\mathrm{?1}}$) shows a nearly identical $\text{K}{}_{\mathrm{<mtext>d</mtext>}}$ of about 3 nM. There is no competition of toxin B-IV binding by purified toxin from Leiurus quinquestriatus venom while Centruroides sculpturatus Ewing toxin I appears to cause a small enhancement of toxin B-IV binding.     

Weak acid-induced release of liposome-encapsulated carboxyfluorescein

Leakage of the entrapped anionic fluorophore carboxyfluorescein was used as a measure of the permeability of liposomes to several different acids. Carboxyfluorescein leakage increased with increasing buffer concentration at a given pH and depended on its chemical nature: apolar weak acids such as acetic or pyruvic acids induced fast leakage at relatively high pH (4 to 5), while glycine, aspartic, citric and hydrochloric acids induced leakage only at lower pH. Fluorescence leakage measurements reflected the acidification of the liposomes' aqueous spaces, which was primarily caused by the diffusion of undissociated acid molecules across the lipid bilayer. A simple mathematical model in accord with this hypothesis and assuming that carboxyfluorescein leakage was directly related to the proportion of its neutral lactone form, described satisfactorily the carboxyfluorescein leakage kinetics and allowed rough estimation of permeability coefficients for carboxyfluorescein (neutral lactone form; 9 · 10^?9 cm · s^?1), acetic acid ($\text{>1 · 10}{}^{\mathrm{?7}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$) and glycine (cation: 6 · 10^?9 cm · s^?1). These results are consistent with low effective proton permeability of liposomes ($\text{<5 · 10}{}^{\mathrm{?12}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$) and with the permeability coefficient of HCl (3 · 10^?3 cm · s^?1) reported by Nozaki and Tanford ((1981) Proc. Natl. Acad. Sci. U.S.A. 78, 4324–4328). Diffusion of weak acid molecules across lipid membranes has implications for drug encapsulation and delivery, and may be of biological significance.     

Calcium ion-flux across phosphatidylcholine membranes mediated by ionophore A23187

The antibiotic A23187 carries Ca²⁺ across Müller-Rudin membranes made from $\text{1,2-}\text{dierucoyl}\text{-sn-}\text{glycero}\text{-3-}\text{phosphocholine}$ and $\text{n-}\text{decane}$. The conductance of the membranes is not increased by the Ca²⁺-transport. The flux depends linearly on Ca²⁺ concentration and ionophore concentration (above pH 6). It increases with increasing pH, approximately by a factor of 4–5 between pH 6 and pH 8. Maximal Ca²⁺-fluxes of about $\text{10}{}^{\mathrm{?10}}\text{mol}\text{·}\text{cm}{}^{\mathrm{?2}}\text{·}\text{s}{}^{\mathrm{?1}}$ were found. A counter transport of H⁺ could not be detected.The complex formation between A23187 and Ca²⁺ in egg phosphatidylcholine vesicles was studied spectroscopically. The results are consistent with the formation of a 2 : 1 complex. Optical absorption measurements on single phosphatidylcholine membranes were used to calculate the concentration of membrane-bound ionophore A23187.     

Carnitine uptake into human heart cells in culture

The uptake of radiolabeled carnitine and butyrobetaine has been studied in human heart cells (CCL 27). The uptake of carnitine is 3–10-fold higher in heart cells than in fibroblasts ($\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}$). The uptake of carnitine increases with temperature coefficient $\text{K}{}_{\mathrm{<mtext>T</mtext>}}$ of 1.6 in the interval 10–20° C and with a negligible uptake at 4 and 10° C. The uptake of carnitine follows Michaelis-Menten kinetics with a $\text{K}{}_{\mathrm{<mtext>M</mtext>}}$ of $\text{4.8 ± 2.2 μ}\text{M}$ and $\text{V = 8.7 ± 3.2}\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}\text{·}\text{h}{}^{\mathrm{?1}}$. Carnitine uptake is suppressed 90% by NaF (24 mM). Butyrobetaine is taken up into heart cells to the same extent as carnitine with a $\text{K}{}_{\mathrm{<mtext>M</mtext>}}$ of 5.7–17.3 μM and $\text{V = 8.7–9.3}\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}\text{·}\text{h}{}^{\mathrm{?1}}$. Butyrobetaine inhibits competitively the uptake of carnitine and carnitine inhibits the uptake of butyrobetaine to the same extent. No conversion of radiolabeled butyrobetaine to carnitine, or carnitine to methyl choline was observed intra- or extracellulary during incubation. These data are compatible with a selective transport mechanism for carnitine which is also responsible for the uptake of butyrobetaine.     

Structural and dynamical studies of mixed chlorophyll/ phosphatidylcholine bilayers via x-ray diffraction,absorption polarization spectroscopy and nuclear magnetic resonance

The structure and dynamics of phosphatidylcholine bilayers containing chlorophyll were studied by X-ray diffraction and absorption polarization spectroscopy in the form of hydrated orientated multilayers below the thermal phase transition of the lipid chains and by nuclear magnetic resonance in the form of single-wall vesicles above the thermal transition. Our results show that (a) chlorophyll is incorporated into the phosphatidylcholine bilayers with its porphyrin ring located anisotropically in the polar headgroup layer of the membrane and with its phytol chain penetrating in a relatively extended form between the phosphatidylcholine fatty acid chains in the hydrocarbon core of the mixed bilayer membrane and (b) the intramolecular anisotropic rotational dynamics of the host phosphatidylcholine molecules are significantly perturbed upon chlorophyll incorporation into the bilayer at all levels of the phosphatidylcholine structure. These dynamics for the host phosphatidtlcholine fatty acid chains are qualitatively different from that of the incorporated chlorophyll phytol chains on a $\text{10}{}^{\mathrm{?9}}\text{? 10}{}^{\mathrm{?10}}\text{s}$ time scale in the ideally mixed two-component bilayer.     

Dopamine-stimulated cyclic AMP and binding of [3H]dopamine in acini from dog pancreas

Dispersed acini from dog pancreas were used to examine the ability of dopamine to increase cyclic AMP cellular content and the binding of [³H]dopamine. Cyclic AMP accumulation caused by dopamine was detected at 1·10^?8 M and was half-maximal at $\text{7.9±3.4·10}{}^{\mathrm{?7}}\text{M}$. The increase at 1·10^?5 M, (7.5-fold) was equal to the half-maximal increase caused by secretin at 1·10^?9 M. Haloperidol, a dopaminergic receptor antagonist inhibited cyclic AMP accumulation caused by dopamine. The IC₅₀ value for haloperidol, calculated from the inhibition of cyclic AMP increase caused by 1·10^?5 M dopamine was $\text{2.3±0.9·10}{}^{\mathrm{?6}}\text{M}$. Haloperidol did not alter basal or secretin-stimulated cyclic AMP content. [³H]Dopamine binding was studied on the same batch of cells as cyclic AMP accumulation. At 37°C, it was rapid, reversible, saturable and stereospecific. The $\text{K}{}_{\mathrm{<mtext>d</mtext>}}$ value for high affinity binding sites was $\text{0.43±0.1·10}{}^{\mathrm{?7}}\text{M}$ and $\text{4.7±1.6·10}{}^{\mathrm{?7}}\text{M}$ for low affinity binding sites. The concentration of drugs necessary to inhibit specific binding of dopamine by 50% was $\text{1.2±0.4·10}{}^{\mathrm{/t-7}}\text{M}$ noradrenaline, 2·10^/t-7 M epinine, $\text{4.1±1.8·10}{}^{\mathrm{/t-6}}\text{M}$ fluphenazine, $\text{8.0±1.6·10}{}^{\mathrm{/t-6}}\text{M}$ haloperidol, $\text{4.2±1.2·10}{}^{\mathrm{?6}}\text{M}$cis-flupenthixol, $\text{2.7±0.4·10}{}^{\mathrm{?5}}\text{M}$trans-flupenthixol, $\text{>1·10}{}^{\mathrm{?5}}\text{M}$ apomorphine, sulpiride, naloxone and isoproterenol.     

Interaction of human fibrinogen with divalent metal chlorides

Precipitation of human fibrinogen in 0.15 m NaCl occurred at pH 7.4 (Tris-HCl buffer) when ZnCl₂, CuCl₂, NiCl₂, or CoCl₂ were added beyond their respective critical concentrations. The critical concentrations were about $\text{4 × 10}{}^{\mathrm{?5}}\text{m}\text{ZnCl}{}_2\text{, 6 × 10}{}^{\mathrm{?5}}\text{m}\text{CuCl}{}_2\text{, 3 × 10}{}^{\mathrm{?4}}\text{m}\text{NiCl}{}_2\text{and}\text{1 × 10}{}^{\mathrm{?3}}\text{m}\text{CoCl}{}_2$. At pH 5.8 2-(N-morpholino)-ethane sulphonic acid buffer, the critical concentrations were found only for CuCl₂ and ZnCl₂, and were about $\text{3 × 10}{}^{\mathrm{?5}}\text{and}\text{3 × 10}{}^{\mathrm{?4}}\text{m}$, respectively. CaCl₂ and MgCl₂ were not effective up to $\text{1 × 10}{}^{\mathrm{?2}}\text{and}\text{2 × 10}{}^{\mathrm{?2}}\text{m}$ at pH 7.4 and 5.8, respectively. At pH 7.4, precipitation was better in 0.015 m NaCl than in 0.15 m NaCl for both CuCl₂ and ZnCl₂. Little or no conformational change was indicated on binding Cu²⁺ ions. The fluorescence of tryptophan was quenched only by CuCl₂, while other metal ions (ZnCl₂, NiCl₂, CoCl₂ and CaCl₂) were ineffective as quenchers.     

The use of 13C spin relaxation to investigate molecular motion in liquid tristearin

Longitudinal and transverse ¹³C spin relaxation times have been used to investigate the molecular motion of tristearin over a range of temperatures in the melt. Overall molecular rotational diffusion rates have been obtained as well as the diffusion rates about successive bonds in the stearoyl chains. The data can be explained using an anisotropic rotor model in which the fast and slow molecular diffusion rates are $\text{? 8 x 10}{}^9\text{sec}{}^{\mathrm{?1}}\text{and}\text{0.018 (2) x 10}{}^9\text{sec}{}^{\mathrm{?1}}$ respectively The alignment of the fast diffusion axis is close to the long chain axis of the ‘tuning fork’ model and the existence of such a configuration in the melt is supported by the observation of different relaxation times for the two chemically equivalent primary glyceryl carbons.The low flexibility gradient and high end group mobility of the acyl chain found at low temperatures in the melt is similar to that observed in lipid vesicle studies and suggest that the chains are aligned parallel. A break down of this short range order is apparent above 150°C.