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.

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.

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).

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.

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.

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.

Resonance Raman spectroscopy of chemically modified hemoglobins.

Hemoglobin obtained from out-dated human blood was stripped of 2,3-diphosphoglycerate and modified with the crosslinking agents glyoxalic acid, 1,2-cyclohexadione, or fumarate to stabilize the tetramer. The resulting hemoglobins, which show alterations in their oxygen transport capability, have been studied in their oxy, deoxy and fluoro-met forms using resonance Raman spectroscopy with Soret excitation. The resonance Raman spectra of oxy-hemoglobins cross linked with glyoxalic acid and 1,2-cyclohexadione show that these cross linking agents force the heme into a high spin structure. The resonance Raman spectra of the fluoro-met hemoglobins, however, indicate that the same cross linking agents force the heme into a lower spin structure. Absorption spectroscopy and molecular orbital considerations suggest that protein constraints at the sixth ligand of the heme can account for the change in spin state in the glyoxalic acid and 1,2-cyclohexadione cross linked hemoglobins.

Fluorescence measurement of chloride transport in monolayer cultured cells. Mechanisms of chloride transport in fibroblasts.

The methodology has been developed to measure Cl activity and transport in cultured cells grown on a monolayer using the entrapped Cl-sensitive fluorophore 6-methoxy-N-[3-sulfopropyl] quinolinium (SPQ). The method was applied to a renal epithelial cell line, LLC-PKI, and a nonepithelial cell line, Swiss 3T3 fibroblasts. SPQ was nontoxic to cells when present for greater than h in the culture media. To load with SPQ (5 mM), cells were made transiently permeable by exposure to hypotonic buffer (150 mOsm, 4 min). Intracellular fluorescence was monitored continuously by epifluorescence microscopy using low illumination intensity at 360 +/- 5 nm excitation wavelength and photomultiplier detection at greater than 410 nm. Over 60 min at 37 degrees C, there was no photobleaching and less than 10% leakage of SPQ out of cells; intracellular SPQ fluorescence was uniform. SPQ fluorescence was calibrated against intracellular [Cl] using high K solutions containing the ionophores nigericin and tributyltin. The Stern-Volmer constant (Kq) for quenching of intracellular SPQ by Cl was 13 M-1 for fibroblasts and LLC-PKl cells. In the absence of Cl, SPQ lifetime was 26 ns in aqueous solution and 3.7 +/- 0.6 ns in cells, showing that the lower Kq in cells than in free solution (Kq = 118 M-1) was due to SPQ quenching by intracellular anions. To examine Cl transport mechanisms, the time course of intracellular [Cl] was measured in response to rapid Cl addition and removal in the presence of ion or pH gradients. In fibroblasts, three distinct Cl transporting systems were identified: a stilbeneinhibitable Cl/HCO3 exchanger, a furosemide-sensitive Na/K/2Cl cotransporter, and a Ca-regulated Cl conductance. These results establish a direct optical method to measure intracellular [Cl] continuously in cultured cells.

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.

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)

Rhodamine 123 as a probe of in vitro toxicity in MDCK cells.

The effect of mercuric chloride on Madin-Darby Canine Kidney (MDCK) cells grown in culture was assayed by the mitochondrial-specific fluorescent probe, rhodamine 123. Treatment of cells with mercuric chloride resulted in a dissipation of rhodamine fluorescence from the mitochondria into the cytoplasm, followed by a release into the medium bathing the cells. Toxicity was assayed either by determining the proportion of cells with delocalized rhodamine fluorescence, or by measuring the rhodamine released from or retained in the cells. Quantifying the release or retention of rhodamine 123 is semi-automated and represents a highly sensitive method of using a vital fluorescent dye for in vitro toxicity analysis.

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.

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.

Quenching of red cell tryptophan fluorescence by mercurial compounds.

Intrinsic tryptophan fluorescence in red cell ghost membranes labeled with N-ethylmaleimide (N-EM) is quenched in a dose-dependent manner by the organic mercurial p-chloromercuribenzene sulfonate (p-CMBS). Fluorescence lifetime analysis shows that quenching occurs by a static mechanism. Binding of p-CMBS occurs by a rapid (less than 5 s) biomolecular association (dissociation constant K1 = 1.8 mM) followed by a slower unimolecular transition with forward rate constant k2 = 0.015 s-1 and reverse rate constant k-2 = 0.0054 s-1. Analysis of the temperature dependence of k2 gives delta H = 6.5 kcal/mol and delta S = -21 eu. The mercurial compounds p-chloromercuribenzoic acid, p-aminophenylmercuric acetate, and mercuric chloride quench red cell tryptophan fluorescence by the same mechanism as p-CMBS does; the measured k2 value was the same for each compound, whereas K1 varied. p-CMBS also quenches the tryptophan fluorescence in vesicles reconstituted with purified band 3, the red cell anion exchange protein, in a manner similar to that in ghost membranes. These experiments define a mercurial binding site on band 3 in ghosts treated with N-EM and establish the binding mechanism to this site. The characteristics of this p-CMBS binding site on band 3 differ significantly from those of the p-CMBS binding site involved in red cell water and urea transport inhibition.

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.

Radiation inactivation studies of renal brush border water and urea transport.

Radiation inactivation was used to determine the nature and molecular weight of water and urea transport pathways in brush border membrane vesicles (BBMV) isolated from rabbit renal cortex. BBMV were frozen to -50 degrees C, irradiated with 1.5 MeV electrons, thawed, and assayed for transport or enzyme activity. The freezing process had no effect on enzyme or transport kinetics. BBMV alkaline phosphatase activity gave linear ln(activity) vs. radiation dose plots with a target size of 68 +/- 3 kDa, similar to previously reported values. Water and solute transport were measured using the stopped-flow light-scattering technique. The rates of acetamide and osmotic water transport did not depend on radiation dose (0-7 Mrad), suggesting that transport of these substances does not require a protein carrier. In contrast, urea and thiourea transport gave linear ln(activity) vs. dose curves with a target size of 125-150 kDa; 400 mM urea inhibited thiourea flux by -50% at 0 and 4.7 Mrad, showing that radiation does not affect inhibitor binding to surviving transporters. These studies suggest that BBMV urea transport requires a membrane protein, whereas osmotic water transport does not.

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.

n-Alkanols and halothane inhibit red cell anion transport and increase band 3 conformational change rate.

The effects of halothane and n-alkanols on band 3, the anion-exchange protein of the red cell membrane, have been characterized by radioactive sulfate exchange and equilibrium and kinetic binding of a fluorescent anion transport inhibitor, 4,4'-dibenzamido-2,2'-stilbenedisulfonic acid (DBDS), with fluorescence and stopped-flow techniques. Ethanol, butanol, hexanol, heptanol, octanol, and decanol inhibit radioactive sulfate efflux from red blood cells in a dose-dependent manner with an average Hill coefficient of 1.3 +/- 0.1. Over a 10(4)-fold range of buffer concentrations, the calculated membrane alkanol concentrations at which anion transport rates are reduced by 50% are 100-200 mM. At 100-300 mM membrane concentrations, halothane and the n-alkanols increase the apparent rate of DBDS binding to band 3 2-3-fold. Analysis of kinetic and equilibrium DBDS binding data shows that these drugs increase the rate of the DBDS-induced conformational change in the DBDS-band 3 complex. Equilibrium DBDS binding studies reveal differences between the actions of short-chain alkanols (ethanol and butanol) and those of long-chain alkanols (hexanol and longer). Short-chain alkanols reduce the equilibrium affinity of DBDS for band 3, while long-chain alkanols have no effect on equilibrium DBDS binding. The results for halothane and long-chain alkanols suggest a nonspecific, lipid-mediated mechanism of anesthetic action, which may be coupled to protein inactivation by an increase in the rate of protein conformational changes resulting in nonfunctional states. The results for short-chain alkanols indicate that they have the same nonspecific actions as the long-chain alkanols but also have specific effects on the stilbene binding site of band 3.

Water and urea transport in renal microvillus membrane vesicles.

Light scattering was used to measure the water and urea permeability of brush border membrane vesicles (BBMV) isolated from rabbit renal cortex. In stop-flow experiments, exposure of BBMV to a 200 mM inwardly directed mannitol gradient gave a monophasic time course of decreasing BBMV volume corresponding to an osmotic water permeability (Pf) of 1.1 +/- 0.1 X 10(-2) cm/s at 37 degrees C. The temperature dependence of Pf was biphasic with delta H = 2 kcal/mol for T less than 33 degrees C and delta H = 14 kcal/mol for T greater than 33 degrees C. A 200 mM inwardly directed urea gradient gave a biphasic time course of BBMV volume due to rapid water efflux (approximately 50 ms) followed by slower urea influx (1-5 s) with urea permeability (Purea) of 2.4 +/- 0.2 X 10(-6) cm/s. Preincubation of BBMV with increasing [urea] reversibly inhibited both urea flux (Kd = 1,200 mM) and thiourea flux (Kd = 370 mM) according to a single-site inhibition model, suggesting a saturable urea carrier. Comparison of BBMV Pf and Purea with proximal tubule transepithelial water and urea transport rates suggests that the permeability of the tubular apical membrane (BBMV) is high enough to support a transcellular route for both osmotic water and urea transport.