The effect of follicular wave on fertility characteristics in beef cattle.

The objectives of this experiment were to determine the effects of follicular wave (first or second) on diameter of the dominant follicle, concentrations of progesterone and estradiol and the hepatic enzymes that inactivate them, thickness of the endometrium, and pregnancy rates to AI. Beef heifers ( = 101) and cows ( = 106) were randomly assigned to 1 of 2 treatments: insemination to the first follicular wave (FFW) or insemination to the second follicular wave (SFW). Estrous cycles of females were synchronized to ensure appropriate timing for the treatments. The MIXED procedure of SAS was used for analysis. A similar proportion of females in each treatment responded to presynchronization; however, females in the FFW group ovulated in response to the first injection of GnRH of the CO-Synch protocol more frequently. Only females ( = 94) that properly responded to ovulation synchronization were included in further analyses. Cows in the FFW group tended ( 0.06) to have larger ovulatory follicles 36 h post-PGF of the CO-Synch protocol compared to cows in the SFW group (14.22 ± 0.42 and 11.83 ± 0.49, respectively), whereas heifers were similar between treatment groups. Three d prior to AI, circulating concentrations of progesterone were lesser ( 0.01) in females in the FFW (3.63 ± 0.80 ng/mL) than in the SFW (7.12 ± 0.83 ng/mL), whereas concentrations of estradiol tended ( 0.08) to be greater in those in the FFW (82.72 ± 6.48 pg/mL) than in the SFW (65.55 ± 6.74 pg/mL). Concentrations of cytochrome P450 1A in the liver were lesser ( 0.01) in females in the FFW than those in the SFW (0.68 ± 0.08 vs. 0.96 ± 0.06, respectively). Endometrial thicknesses were similar between treatments but were thicker ( < 0.0001) in cows (9.73 ± 0.24 mm) than heifers (7.22 ± 0.26 mm). When considering all females or only those that were properly presynchronized, pregnancy rates were similar between treatments. However, when evaluating females that ovulated to the assigned follicular wave, there was a treatment by parity interaction ( = 0.04) with heifers in the FFW having a lesser pregnancy rate (25.9%) than heifers in the SFW (72.0%) while cows in both treatment groups were intermediate (45.4% in FFW and 50.0% in SFW). The differences in concentrations of steroids between treatment groups may affect fertility of heifers; however, additional research is necessary.

Role of membrane proteins and lipids in water diffusion across red cell membranes.

When human red cells are treated with the mercurial sulfhydryl reagent, p-chloromercuribenzene sulfonate, osmotic water permeability is suppressed and only diffusional water permeability remains (Macey, R.I. and Farmer, R.E.L. (1970) Biochim. Biophys. Acta 211, 104-106). It has been suggested that the route for the remaining water permeation is by diffusion through the membrane lipids. However, after making allowance for the relative lipid area of the membrane, the water diffusion coefficient through lipid bilayers which contain cholesterol is too small by a factor of two or more. We have measured the permeability coefficient of normal human red cells by proton T1 NMR and obtained a value of 4.0 X 10(-3) cm X s-1, in good agreement with published values. In order to study permeation-through red cell lipids we have perturbed extracted red cell lipids with the lipophilic anesthetic, halothane, and found that halothane increases water permeability. The same concentration of halothane has no effect on the water permeability of human red cells, after maximal pCMBS inhibition. In order to compare halothane mobility in extracted red cell membrane lipids with that in red cell ghost membranes, we have studied halothane quenching of N-phenyl-1-naphthylamine by equilibrium fluorescence and fluorescence lifetime methods. Since halothane mobility is similar in these two preparations, we have concluded that the primary route of water diffusion in pCMBS-treated red cells is not through membrane lipids, but rather through a membrane protein channel.

Specific interaction of the water transport inhibitor, pCMBS, with band 3 in red blood cell membranes.

The human red cell anion transport protein, band 3, contains six pCMBS (p-chloromercuribenzene sulfonate) reactive SH groups, five of which react with N-ethylmaleimide. We have carried out equilibrium binding experiments using N-ethylmaleimide-treated red cell ghosts and found that the sulfhydryl reactive water transport inhibitor, pCMBS, inhibits the binding to band 3 of the specific anion exchange inhibitor DBDS (4,4'-dibenzoamido-2,2'-disulfonic stilbene) in a non-competitive manner. Stopped-flow kinetic studies, in which DBDS is mixed with ghosts in the presence of pCMBS, show that pCMBS slows the DBDS induced conformational change in band 3. A non-competitive reaction scheme has been developed which incorporates the quantitative results of equilibrium and kinetic studies. The pCMBS effect on DBDS binding and kinetics is reversed with 5 mM cysteine suggesting a sulfhydryl bond is involved in pCMBS binding to band 3. These data suggest that pCMBS has a specific binding site on band 3, consistent with the hypothesis that band 3 mediates red cell water transport.

Interaction of phloretin with the anion transport protein of the red blood cell membrane.

Phloretin is an inhibitor of anion exchange and glucose and urea transport in human red cells. Equilibrium binding the kinetic studies indicate that phloretin binds to band 3, a major integral protein of the red cell membrane. Equilibrium phloretin binding has been found to be competitive with the binding of the anion transport inhibitor, 4,4'-dibenzamido-2,2'-disulfonic stilbene (DBDS), which binds specifically to band 3. The apparent binding (dissociation) constant of phloretin to red cell ghost band 3 in 28.5 mM citrate buffer, pH 7.4, 25 degree C, determined from equilibrium binding competition, is 1.8 +/- 0.1 microM. Stopped-flow kinetic studies show that phloretin decreases the rate of DBDS binding to band 3 in a purely competitive manner, with an apparent phloretin constant of 1.6 +/- 0.4 microM. The pH dependence of equilibrium binding studies show that it is the charged, anionic form of phloretin that competes with DBDS binding, with an apparent phloretin inhibition constant of 1.4 microM. The phloretin binding and inhibition constants determined by equilibrium binding, kinetic and pH studies are all similar to the inhibition constant of phloretin for anion exchange. These studies suggest that phloretin inhibits anion exchange in red cells by a specific interaction between phloretin and band 3.

Target analysis studies of red cell water and urea transport.

Radiation inactivation was used to determine the nature and molecular weight of water and urea transporters in the human red cell. Red cells were frozen to -50 degrees C in a cryoprotectant solution, irradiated with 1.5 MeV electrons, thawed, washed and assayed for osmotic water and urea permeability by stopped-flow light scattering. The freezing and thawing process did not affect the rates of water or urea transport or the inhibitory potency of p-chloromercuribenzenesulfonate (pCMBS) on water transport and of phloretin on urea transport. Red cell urea transport inactivated with radiation (0-4 Mrad) with a single target size of 469 +/- 36 kDa. 40 microM phloretin inhibited urea flux by approx. 50% at each radiation dose, indicating that urea transporters surviving radiation were inhibitable. Water transport did not inactivate with radiation; however, the inhibitory potency of 2.5 mM pCMBS decreased from 86 +/- 1% to 4 +/- 9% over a 0-2 Mrad dose range. These studies suggest that red cell water transport either required one or more low-molecular-weight proteins, or is lipid-mediated, and that the pCMBS-binding site which regulates water flow inactivates with radiation. These results also suggest that red cell urea transport is mediated by a specific, high-molecular-weight protein. These results do not support the hypothesis that a band 3 dimer (190 kDa) mediates red cell osmotic water and urea transport.

Anion transport inhibitor binding to band 3 in red blood cell membranes.

The inhibitor of anion exchange 4,4'-dibenzoamido-2,2'-disulfonic stilbene (DBDS) binds to band 3, the anion transport protein in human red cell ghost membranes, and undergoes a large increase in fluorescence intensity when bound to band 3. Equilibrium binding studies performed in the absence of transportable anions show that DBDS binds to both a class of high-affinity (65 nM) and low-affinity (820 nM) sites with stoichiometry equivalent to 1.6 nmol/mg ghost protein for each site, which is consistent with one DBDS site on each band 3 monomer. The kinetics of DBDS binding were studied both by stopped-flow and temperature-jump experiments. The stopped-flow data indicate that DBDS binding to the apparent high-affinity site involves association with a low-affinity site (3 microM) followed by a slow (4 s-1) conformational change that locks the DBDS molecule in place. A detailed, quantitative fit of the temperature-jump data to several binding mechanisms supports a sequential-binding model, in which a first DBDS molecule binds to one monomer and induces a conformational change. A second DBDS molecule then binds to the second monomer. If the two monomers are assumed to be initially identical, thermodynamic characterization of the binding sites shows that the conformational change induces an interaction between the two monomers that modifies the characteristics of the second DBDS binding site.

Proton (or hydroxide) fluxes and the biphasic osmotic response of human red blood cells.

Upon exposure of human red blood cells to hypertonic sucrose, the fluorescence of the potentiometric indicator 3,3'-dipropylthiadicarbocyanine iodide, denoted diS-C3(5), displays a biphasic time course indicating the rapid development of an inside-positive transmembrane voltage, followed by a slow DIDS (4,4'-diisothiocyano-2,2'-disulfonic acid stilbene)-sensitive decline of the voltage. In addition to monitoring membrane potential, proton (or hydroxide) fluxes were measured by a pH stat method, cell volume was monitored by light scattering, and cell electrolytes were measured directly when red cells were shrunken either with hypertonic NaCl or sucrose. Shrinkage by sucrose induced an initial proton efflux (or OH- influx) of 5.5 mu eq/g Hb.min and a Cl shift of 21-31 mu eq/g Hb in 15 min. Upon shrinkage with hypertonic NaCl, the cells are initially close to Donnan equilibrium and exhibit no detectable shift of Cl or protons. Experiments with the carbonic anhydrase inhibitor ethoxzolamide demonstrate that for red cell suspensions exposed to air and shrunken with sucrose, proton fluxes mediated by the Jacobs-Stewart cycle contribute to dissipation of the increased outward Cl concentration gradient. With maximally inhibitory concentrations of ethoxzolamide, a residual proton efflux of 2 mu eq/g Hb.min is insensitive to manipulation of the membrane potential with valinomycin, but is completely inhibited by DIDS. The ethoxzolamide-insensitive apparent proton efflux may be driven against the electrochemical gradient, and is thus consistent with HCl cotransport (or Cl/OH exchange). The data are consistent with predictions of equations describing nonideal osmotic and ionic equilibria of human red blood cells. Thus osmotic equilibration after shrinkage of human red blood cells by hypertonic sucrose occurs in two time-resolved steps: rapid equilibration of water followed by slower equilibration of chloride and protons (or hydroxide). Under our experimental conditions, about two-thirds of the osmotically induced apparent proton efflux is mediated by the Jacobs-Stewart cycle, with the remainder being consistent with mediation via DIDS-sensitive HCl cotransport (or Cl/OH exchange).

Phospholipase activation, free fatty acids and the proton permeability of a biological membrane.

The rate of collapse of a proton gradient across the apical membrane of rat kidney proximal tubule increases upon treatment with calcium, mercuric chloride and mellitin, substances which activate phospholipase A2. Treatment with phospholipase A2 or oleic acid also enhances the rate of proton gradient dissipation. Membrane water permeability is not affected. This phenomenon may have implications in pathological states arising from ischemia or toxic exposure.

Temperature dependence of anion transport inhibitor binding to human red cell membranes.

The binding characteristics of the inhibitor of anion transport in human red cells, 4,4'-dibenzamido-2,2'-disulfonic stilbene (DBDS), to the anion transport protein of red cell ghost membranes in buffer containing 150 mM NaCl have been measured over the temperature range 0-30 degrees C by equilibrium and stopped-flow fluorescence methods. The equilibrium dissociation constant Keq, increased with temperature. No evidence of a 'break' in the ln(Keq) vs. 1/T plot was found. The standard dissociation enthalpy and entropy changes calculated from the temperature dependence are 9.1 +/- 0.9 kcal/mol and 3.2 +/- 0.3 e.u., respectively. Stopped-flow kinetic studies resolve the overall binding into two steps: a bimolecular association of DBDS with the anion transport protein, followed by a unimolecular rearrangement of the DBDS-protein complex. The rate constants for the individual steps in the binding mechanism can be determined from an analysis of the concentration dependence of the binding time course. Arrhenius plots of the rate constants showed no evidence of a break. Activation energies for the individual steps in the binding mechanism are 11.6 +/- 0.9 kcal/mol (bimolecular, forward step), 17 +/- 2 kcal/mol (bimolecular, reverse step), 6.4 +/- 2.3 kcal/mol (unimolecular, forward step), and 10.6 +/- 1.9 kcal/mol (unimolecular, reverse step). Our results indicate that there is an appreciable enthalpic energy barrier for the bimolecular association of DBDS with the transport protein, and appreciable enthalpic and entropic barriers for the unimolecular rearrangement of the DBDS-protein complex.

Mechanism of acridine orange interaction with phospholipids and proteins in renal microvillus vesicles.

The mechanism of interaction of acridine orange (AO), a fluorescent, weak base, with rabbit kidney brush border membrane vesicles (BBMV) has been studied by absorption, and steady-state and time-resolved fluorescence spectroscopy. Equilibrium binding experiments indicate that AO binds to an apparent single class of sites on BBMV with a dissociation constant of 90 microM and site stoichiometry of 810 nmol/mg protein. The absorption spectra AO indicate that BBMV induces aggregation of AO; experiments with lipid vesicles show that the aggregation requires BBMV membrane proteins. Fluorescence stopped-flow experiments in which 0.15 mg/ml BBMV is mixed with increasing concentrations of AO result in a time course of fluorescence enhancement for [AO] less than 1.5 microM, and of fluorescence quenching for [AO] greater than 1.5 microM. Similar stopped-flow experiments with phosphatidylcholine lipid vesicles result only in a fluorescence enhancement time course. These results indicate the presence of two parallel pathways for AO binding to BBMV: one for AO binding to BBMV lipid, the other for AO binding to BBMV protein. Nanosecond lifetime measurements and fluorescence titration experiments confirm the presence of two environments for AO in BBMV. Fluorescence stopped-flow experiments indicate that AO responds to the imposition of an outwardly directed proton gradient by a rapid (less than 0.5 s) decrease in fluorescence, corresponding to re-equilibration of AO into the acidic intravesicular compartment, followed by an increase in fluorescence, corresponding to proton flux across the membrane. These findings have been incorporated into a stepwise mechanism for AO interaction with BBMV which have direct implications for the use of AO as a pH indicator in biological systems.

Chloride-bicarbonate exchange through the human red cell ghost membrane monitored by the fluorescent probe 6-methoxy-N-(3-sulfopropyl)quinolinium.

The exchange of chloride and bicarbonate across the human red cell membrane has been characterized by quenching of an intracellular fluorophore, 6-methoxy-N-(3-sulfopropyl)quinolinium (SPQ). In 20 mM Hepes, pH 7.4, and varying concentrations of chloride and bicarbonate with total anion concentration of 150 mM, SPQ is quenched dynamically by chloride with an apparent Stern-Volmer quenching constant 0.071 +/- 0.016 mM-1 at 25 degrees C. Hepes alone quenched SPQ fluorescence with a quenching constant of 0.030 +/- 0.003 mM-1. Stopped-flow kinetic experiments give fluorescence time courses that, when corrected for Stern-Volmer quenching, are first order. Disulfonic stilbenes (inhibitors of anion exchange) decrease the rate of fluorescence equilibration. Transport of bicarbonate via hydration-dehydration of CO2 does not contribute to the observed kinetics. The chloride-bicarbonate exchange rate is independent of the anion concentration gradient, but increases at 25 degrees C from 1 to 4 s-1 as equilibrium chloride concentration increases from 20 to 130 mM (with concomitant decrease in bicarbonate concentration from 130 to 20 mM). The data indicate that the translocation rate of the chloride-loaded transport protein is greater than that of bicarbonate-loaded transport protein and that bicarbonate has a higher affinity for the transport protein than chloride. Our results validate the use of SPQ to measure quantitatively chloride-bicarbonate exchange in red cell ghosts. The methods we describe should be applicable to other systems exhibiting chloride-bicarbonate exchange.

Effect of unstirred layers on binding and reaction kinetics at a membrane surface.

The effects of solution unstirred layers on the time course of chemical reactions and transport processes at a membrane surface are determined. A set of equations which describes non-steady-state diffusion through an unstirred layer coupled with chemical reaction at a membrane surface or transport through a membrane is developed. A numerical solution to the equations is obtained by uncoupling diffusive and chemical processes in an iterative manner. The diffusive process is solved by the Crank-Nicolson method; the chemical process is solved by integrating the differential equations describing the kinetics. Diffusive processes in one dimension, in three dimensions, and in the presence of an arbitrary potential near the membrane surface are solved. General characteristics of the calculated reaction time course are discussed using surface binding and membrane transport examples. Small, neglected, unstirred layers are shown to sometimes yield erroneous values of rate parameters for a surface reaction and to simulate competitive reaction kinetics. Experimental approaches for measuring unstirred layer thickness are reviewed.

Pyrene eximer mapping in cultured fibroblasts by ratio imaging and time-resolved microscopy.

The kinetics of pyrene eximer formation provide a measure of lateral diffusibility in bilayer membranes. Swiss 3T3 fibroblasts were labeled with pyrene, pyrenedecanoic acid (PDA) and 1,3-bis(1 pyrene) propane (BPP) by incubation in the presence of Pluronic F127. Single-cell emission spectra obtained by epifluorescence microscopy (excitation 350 nm) with photodiode array detection showed monomer (380-420 nm) and eximer (475 nm) peaks. The eximer-to-monomer fluorescence ratio (E/M) increased with increasing temperature and loading time. Time-resolved microscopy studies of fibroblasts labeled with PDA for 15 min gave monomer and eximer lifetimes of 101 and 78 ns, respectively, with a monomer-to-eximer conversion rate of 0.02 ns-1. E/M ratio images were obtained with a microchannel plate intensifier and CCD camera at 350-nm excitation and 405 +/- 5 nm (monomer) and greater than 470-nm (eximer) emission wavelengths. E/M ratios of PDA showed spatial variation across the cell with highest ratios at the peripheral plasma membrane. These results establish the methodology to label cells with pyrene eximer-forming probes and to image eximer distributions in membranes of intact cultured cells. Eximer-to-monomer fluorescence ratios are sensitive to maneuvers that alter the membrane physical state and should be of utility in examining the cellular regulation of membrane fluidity.

Mapping of fluorescence anisotropy in living cells by ratio imaging. Application to cytoplasmic viscosity.

Steady-state and time-resolved fluorescence properties of probes incorporated into living cells give information about the microenvironment near the probe. We have extended studies of spatially averaged fluorescence anisotropy (r) by using an epifluorescence microscope, equipped with excitation and emission polarizers and an image analysis system, to map r of nonoriented fluorophores incorporated into cultured cells. With this imaging system, r for reflected light or glycogen scattering solutions was greater than 0.98. Measurement of r over the range 0.01-0.35 for fluorophores in bulk solution and in thin capillary tubes placed side-by-side gave values equivalent to r measured by cuvette fluorometry. Cytoplasmic viscosity (eta) in Madin-Darby canine kidney (MDCK) cells and Swiss 3T3 fibroblasts was examined from anisotropy images and time-resolved fluorescence decay of the cytoplasmic probes 2,7-bis-carboxyethyl-5 (and 6)-carboxy-fluorescein (BCECF) and indo-1. Nanosecond lifetimes and anisotropy decay were measured using a pulsed light source and gated detector interfaced to the epifluorescence microscope. Anisotropy images of BCECF in MDCK cells revealed two distinct regions of r: one from the cytoplasm (r = 0.144 +/- 0.008) and a second appearing at late times from the interstitial region (r = 0.08 +/- 0.03), representing BCECF trapped beneath the tight junctions. Anisotropy values, taken together with intracellular life-times and the calibration between r and eta/tau f for water/glycerol mixtures, gave eta values of 10-13 cP at 23 degrees C. These values assume little fluorophore binding to intracellular components and are therefore upper limits to cytoplasmic viscosity. These data establish a new methodology to map anisotropy in intact cells to examine the role of fluidity in cellular physiology.

Binding of chloride and a disulfonic stilbene transport inhibitor to red cell band 3.

The effect of chloride on 4,4'-dibenzamido-2,2'-disulfonic stilbene (DBDS) binding to band 3 in unsealed red cell ghost membranes was studied in buffer [NaCl (0 to 500 mM) + Na citrate] at constant ionic strength (160 or 600 mM), pH 7.4, 25 degrees C. In the presence of chloride, DBDS binds to a single class of sites on band 3. At 160 mM ionic strength, the dissociation constant of DBDS increases linearly with chloride concentration in the range [Cl] = 10 to 120 mM; at 600 mM ionic strength, the DBDS dissociation constant saturates hyperbolically with half-saturating [Cl] = 450 mM. The observed rate of DBDS binding to ghost membranes, as measured by fluorescence stopped-flow kinetic experiments, increases with chloride concentration at both 160 and 600 mM ionic strength. The equilibrium and kinetic results have been incorporated into the following model of the DBDS-band 3 interaction: (formula; see text) The equilibrium and rate constants of the model at 600 mM ionic strength are K1 = 0.67 +/- 0.16 microM, k2 = 1.6 +/- 0.7 sec-1, k-2 = 0.17 +/- 0.09 sec-1, K'1 = 6.3 +/- 1.7 microM, k'2 = 9 +/- 4 sec-1 and k'-2 = 7 +/- 3 sec-1. The apparent dissociation constants of chloride from band 3, KCl, are 40 +/- 4 mM (160 mM ionic strength) and 11 +/- 3 mM (600 mM ionic strength). Our results indicate that chloride and DBDS have distinct, interacting binding sites on band 3.

Osmotic properties of human red cells.

When an osmotic pressure gradient is applied to human red cells, the volume changes anomalously, as if there were a significant fraction of "nonosmotic water" which could not serve as solvent for the cell solutes, a finding which has been discussed widely in the literature. In 1968, Gary-Bobo and Solomon (J. Gen. Physiol. 52:825) concluded that the anomalies could not be entirely explained by the colligative properties of hemoglobin (Hb) and proposed that there was an additional concentration dependence of the Hb charge (ZHb). A number of investigators, particularly Freedman and Hoffman (1979, J. Gen. Physiol. 74:157) have been unable to confirm Gary-Bobo and Solomon's experimental evidence for this concentration dependence of ZHb and we now report that we are also unable to repeat the earlier experiments. Nonetheless, there still remains a significant anomaly which amounts to 12.5 +/- 0.8% of the total isosmotic cell water (P much less than 0.0005, t test), even after taking account of the concentration dependence of the Hb osmotic coefficient and all the other known physical chemical constraints, ideal and nonideal. It is suggested that the anomalies at high Hb concentration in shrunken cells may arise from the ionic strength dependence of the Hb osmotic coefficient. In swollen red cells at low ionic strength, solute binding to membrane and intracellular proteins is increased and it is suggested that this factor may account, in part, for the anomalous behavior of these cells.

Translational diffusion coefficient and partition coefficient of a spin-labeled solute in lecithin bilayer membranes.

The translational diffusion coefficient and the partition coefficient of a spin-labeled solute, di-t-butyl nitroxide, in an aqueous suspension of dipalmitoyl lecithin vesicles have been studied by electron spin resonance spectroscopy. When the lecithin is cooled through its phase transition temperature near 41 degrees C, some solute is "frozen out" of the bilayer, and the standard partial molar enthalpy and entropy of partition go more positive by a factor of 8 and 6, respectively. However, the apparent diffusion constant in the lecithin phase is only slightly smaller than that in water, both above and below the transition temperature. The fraction of bilayer volume within which solute is distributed may increase with temperature, contributing to the positive enthalpy of partition. Comparison of time constants suggests that there is a permeability barrier to this solute in the periphery of the bilayer.

Cell membrane fluidity in the intact kidney proximal tubule measured by orientation-independent fluorescence anisotropy imaging.

Membrane fluidity was measured in the isolated perfused proximal tubule from rabbit kidney. The apical and basolateral plasma membranes of tubule cells were stained separately with the fluidity-sensitive fluorophore trimethylammonium-diphenyl-hexatriene (TMA-DPH) by luminal or bath perfusion. Fluorescence anisotropy (r) of TMA-DPH was mapped with spatial resolution using an epifluorescence microscope (excitation 380 nm, emission greater than 410 nm) equipped with rotatable polarizers and a quantitative imaging system. To measure r without the confounding effects of fluorophore orientation, images were recorded with emission polarizer parallel and perpendicular to a continuum of orientations of the excitation polarizer. The theoretical basis of this approach was developed and its limitations were evaluated by mathematical modeling. The tubule inner surface (brush border) was brightly stained when the lumen was perfused with 1 microM TMA-DPH for 5 min; apical membrane r was 0.281 +/- 0.006 (23 degrees C). Staining of the tubule basolateral membrane by addition of TMA-DPH to the bath gave a significantly lower r of 0.242 +/- 0.010 (P less than 0.005); there was no staining of the brush border membrane. To interpret anisotropy images quantitatively, effects of tubule geometry, TMA-DPH lifetime, fluorescence anisotropy decay, and objective-depolarization were evaluated. Steady-state and time-resolved r and lifetimes in the intact tubule, measured by a nanosecond pulsed microscopy method, were compared with results in isolated apical and basolateral membrane vesicles from rabbit proximal tubule measured by cuvette fluorometry; r was 0.281 (apical membrane) and 0.276 (basolateral membrane) (23 degrees C). These results establish a methodology to quantitate membrane fluidity in the intact proximal tubule, and demonstrate a significantly higher fluidity in the basolateral membrane than in the apical membrane.

Fluorescence depolarization of cis- and trans-parinaric acids in artificial and red cell membranes resolved by a double hindered rotational model.

Although steady-state anisotropy measurements of phase-sensitive probes provide a qualitative description of the phase behavior of biomembranes, there is little information about the physical state of lipid domains. We have developed a ground-state double hindered rotator model (DHR) for fluorescence anisotropy decay, in which probes possess separate rotational correlation times and r infinity in each phase. To validate the model, multifrequency differential phase angles (delta) and modulation amplitudes (lambda) were measured in a two-compartment cuvette with combinations of POPOP, TMA-DPH, and DPH in isotropic solvents and in DPPC liposomes. Rotational parameters obtained by fitting the DHR model were similar to those of a single hindered rotator model fitted to data obtained separately for each probe. As predicted by the model, negative delta and decreasing lambda with increasing modulation frequency were obtained when fluorophores in isotropic solvents were paired with fluorophores in DPPC liposomes. The rotational parameters of the phase-sensitive fluorophores cis-parinaric (cPnA) and trans-parinaric (tPnA) acid in DPPC/DMPC (1:0, 0:1, and 1:1) liposomes were determined at 15-40 degrees C. Two lifetimes (1 and 3 ns) were obtained above the phase transition temperature (Tc); greater than 95% of the fluorescence intensity was described by two lifetimes (3-9 and 12-32 ns) below Tc. Negative delta values were obtained when solid-phase lipid was present. r infinity varied from 0.26-0.32 below to 0.11-0.14 above Tc; at intermediate T, where two phases coexists, r infinity values were approximately 0.23 and approximately 0.31. These data indicate very hindered PnA rotation in solid-phase lipid.(ABSTRACT TRUNCATED AT 250 WORDS)