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The rate of efflux of trapped 5/6-carboxyfluorescein from sealed lipid vesicles showed a marked dependence on (a) temperature, (b) phospholipid acyl chain composition, and (c) the nature of co-trapped counterions. When the dye was salted with sodium, at pH greater than 7, the rate of dye permeation showed a discrete maximum at the melting point of the lipid bilayer (Tc); in the case of membranes composed of dipalmitoylphosphatidylcholine, this discontinuity extended over a very broad temperature range, being detectable at least 10 degrees C above and below Tc. The peak in dye permeation rate was superimposed on a permeation profile that showed a simple exponential relationship to temperature. Studies with a homologous series of saturated lecithin bilayers revealed a consistent pattern of behavior: a logarithmic dependence of dye permeation rate on temperature with a superimposed discontinuity at Tc. For thin membranes (12-14-carbon acyl chains), the discontinuity was severe, exerting an influence over a very broad temperature range and leading to extremely high overall dye leakage rates. As the acyl chains were lengthened, the discontinuity became less pronounced, almost disappearing at a chain length of 20 carbons. In sharp contrast to these results, dye salted with N-methylglucamine [or with tris(hydroxymethyl)aminomethane] showed no efflux maximum at Tc, and base-line leakage rates were generally slower. When dye was salted with ammonium, efflux was too rapid to monitor, even at temperatures well below Tc. The results indicate that the rate of release of electrically charged dyes, such as 5/6-carboxyfluorescein, from sealed lipid vesicles can be tightly coupled to the counterion leakage rate and hence can provide an accurate and convenient assay of relative ion flux across phospholipid bilayers.

Simple phospholipid bilayers show a high level of permeability to protons; in spite of this fact, large proton gradients existing across such bilayers may decay very slowly. In sealed systems, the free movement of protons across a membrane barrier is severely restricted by the coincident development of a proton diffusion potential. Using the fluorescent weak acid N-[5-(dimethylamino)naphth-1-ylsulfonyl]glycine strongly buffered systems movement of the small number of protons giving rise to this electrical potential is insufficient to perturb the proton concentration gradient; significant flux of protons (and hence significant collapse of the concentration gradient) can only occur if protons traverse the membrane as part of an electroneutral complex or if there is a balancing flow of appropriate counterions. In both instances, proton flux is obligatorily coupled to the translocation of species other than protons. In weakly buffered systems, the small initial uncoupled electrogenic flux of protons may significantly alter the concentration gradient. This initial rapid gradient collapse caused by uncoupled electrogenic proton movements is then superimposed upon the residual collapse attributable to tightly coupled proton flux. The initial uncoupled electrogenic proton flux shows a temperature dependence very similar to that demonstrated for water permeation across simple lipid bilayers; upon cooling, there is a sharp decrease in flux at the temperature coinciding with the main gel-liquid-crystalline phase transition of the lipid. The coupled proton flux shows a markedly different temperature dependence with no dramatic change in rate at the phase transition temperature and strong similarity to the behavior previously seen with solutes known to be permeating as electrically neutral compounds.(ABSTRACT TRUNCATED AT 250 WORDS)

There are distinct differences in the molecular packing of phospholipid molecules in the inner and outer membrane monolayers of small lipid vesicles; a small radius of curvature imparts an asymmetry to the interface between these two monolayers. I have used an amphiphilic fluorescent probe, N-[5-(dimethylamino)naphthalenyl-1-sulfonyl]glycine (dansylglycine), to determine if this asymmetry in molecular packing leads to the existence of different environments for fluorescent probes resident in the membrane. Dansylglycine is highly sensitive to the dielectric constant of its environment, and the fluorescence signal from membrane-bound dye is distinct from that in the aqueous medium. When dansylglycine is first mixed with vesicles, it rapidly partitions into the outer monolayer; the subsequent movement of dye into the inner monolayer is much slower. Because of the time lag between the initial partitioning and the subsequent translocation, it is possible to measure the emission spectrum from membrane-bound dye before and after translocation, thus distinguishing the two potential environments for dansylglycine molecules. In the outer membrane monolayer of small dipalmitoylphosphatidylcholine vesicles, dye fluorescence emission is maximal at 530 nm, corresponding to a dielectric constant of 7 for the medium surrounding the fluorophore. For dye in the inner monolayer, emission is maximal at 519 nm, corresponding to a dielectric constant of 4.7. The results suggest that water molecules are excluded more efficiently from the dye binding sites of the inner membrane monolayer than they are from those of the outer monolayer.(ABSTRACT TRUNCATED AT 250 WORDS)

The amphiphilic fluorescent dye N-[(5-dimethylamino)naphth-1-ylsulfonyl]glycine (dansylglycine) can be used to monitor the magnitude and stability of transmembrane proton gradients. Although freely soluble in aqueous media, the dye readily adsorbs to the surfaces of lipid vesicles. Because membrane-bound dye fluoresces at a higher frequency, and with greater efficiency, than dye in aqueous solution, it is easy to isolate the fluorescence emission from those dye molecules adsorbed to the lipid surface. When dansylglycine is mixed with phospholipid vesicles, the dye molecules attain a partition equilibrium between buffer and the outer, proximal surface of the vesicles. This is a rapid, diffusion-limited process that is indicated by a fast phase of fluorescence intensity increase monitored at 510 nm. In a second step, the inner, distal surface of each vesicle becomes populated with dye, a process that involves permeation through the lipid bilayer and that is generally much slower than the original adsorption step. Dansylglycine is a weak acid that permeates as an electrically neutral species; the flux of dye across the bilayer is thus strongly dependent on the degree of protonation of the dye's carboxylate moiety. When the external pH is lower than that of the vesicle lumen, the inward flux of dye is greater than that in the opposite direction, and dye accumulates in the lumen. This leads to a local elevation of dansylglycine concentration in the inner membrane monolayer, which in turn results in an elevated fluorescence intensity proportional to the membrane pH gradient.