Band 3 peptides block the adherence of sickle cells to endothelial cells in vitro.

Malaria-parasitized erythrocytes have increased endothelial adherence due to exposure of previously buried intramembranous sites of band 3. Because sickle erythrocytes also show increased adhesiveness and because the membrane portion of band 3 is aggregated in both types of cells, we examined the role of band 3 in sickle cell adhesiveness. Synthetic peptides derived from the second and third exofacial, interhelical regions of band 3 completely inhibited the abnormal adherence of sickle cells to an endothelial monolayer in a static assay. This effect was observed independently of plasma factors, required micromolar levels of peptide, was sequence-specific, and was found with both L- and D-isomers. The active peptides also inhibited the increased adherence induced by low-dose calcium loading of normal red blood cells. Finally, a monoclonal antibody against an active peptide specifically immunostained a fraction of sickle cells. These findings implicate a role for band 3 in at least one type of sickle cell adhesiveness via the exposure of normally cryptic membrane sites.

Distance between Cys-201 in erythrocyte band 3 and the bilayer measured by single-photon radioluminescence.

Single-photon radioluminescence (SPR), the excitation of fluorophores by short-range beta-decay electrons, was developed for the measurement of submicroscopic distances. The cytoplasmic domain of band 3 (cdb3) is the primary, multisite anchorage for the erythrocyte skeleton. To begin to define the membrane arrangement of the highly asymmetrical cdb3 structure, the distance from the bilayer of Cys-201 next to the "hinge" of cdb3 was measured by both SPR and resonance energy transfer (RET). cdb3 was labeled at Cys-201 with fluorescein maleimide. For SPR measurements, the bilayer was labeled with [3H]oleic acid. The corrected cdb3-specific SPR signal was 98 +/- 2 cps microCi-1 [mumol band 3]-1. From this and the signal from a parallel sample in which 3H2O was substituted for [3H]oleic acid to create uniform geometry between 3H and the fluorophores, a Cys-201-to-bilayer separation of 39 +/- 7 A was calculated. Confirmatory distances of 40 and 43 A were obtained by RET between fluorescein on Cys-201 and eosin and rhodamine B lipid probes, respectively. This distance indicates that Cys-201 lies near band 3's vertical axis of symmetry and that the subdomain of cdb3 between the hinge and the membrane is not significantly extended. In addition, these results validate SPR as a measure of molecular distances in biological systems.

Membrane-based, dry-reagent prothrombin time tests.

The authors describe a prototype membrane-based, dry-reagent prothrombin time assay for whole blood. This system uses an asymmetric polysulfone membrane to separate plasma from red blood cells, and works with samples as small as 10 microliters. The membrane contains calcium and thromboplastin, and permits the reactions of the complete extrinsic pathway to occur with minimal distortion from membrane surface interactions. Thrombin generation is monitored optically using a rhodamine-110-based fluorescent thrombin substrate. Fluorescence kinetics are analyzed to produce a prothrombin-time--equivalent parameter that can be converted to an international normalized ratio (INR) value. The system provides results that correlate well with conventional liquid phase prothrombin time assays (R2 = 0.96).

Anisotropy decay measurement of segmental dynamics of the anion binding domain in erythrocyte band 3.

Time-resolved anisotropy was utilized to detect nanosecond segmental motions of the band 3 intramembrane domain. Band 3 at lysine 430 was fluorescently labeled in ghost membranes by fluorescein or eosin maleimide treatment of intact human erythrocytes followed by hypotonic lysis. Single lifetimes for fluorescein (3.8-4.1 ns) and eosin (3.2-3.4 ns) were observed. Phase-modulation measurement of anisotropy decay indicated a segmental motion model, r(t) = exp(-t/tau 1c)[r infinity + (ro-r infinity) exp(-t/tau 2c)], defined by rotational correlation times corresponding to band 3 segmental motion (tau 1c, 30-70 ns) and rapid fluorescein motion in its binding pocket (tau 2c, 200-400 ps), and a residual anisotropy (r infinity, 0.23-0.28) describing hindered fluorescein motion. In PBS at pH 7.4, tau 1c, tau 2c, and r infinity were 44 ns, 307 ps, and 0.24, respectively, predicting a steady-state anisotropy of 0.24, in agreement with the measured value of 0.23. Factors that might influence band 3 structure/dynamics were examined. Whereas pH (range 5-10) had little effect on r(t), [NaCl] addition (0-150 mM) remarkably decreased tau 1c from 68 to 44 ns. The decrease in tau 1c correlated with solution ionic strength, and did not depend on osmolality (studied by mannitol addition), or specific anion interactions (comparing Cl, Br, F, SO4, citrate). The ionic strength effect was not observed in fluorescein-labeled carbonic anhydrase and trypsin-cleaved band 3, suggesting a specific effect on intact band 3. Anisotropy decay was relatively insensitive to external lectin or internal 2,3-DPG binding, but was sensitive to temperature, membrane fluidity, urea denaturation, fluid-phase viscosity, and aldehyde fixation.(ABSTRACT TRUNCATED AT 250 WORDS)

Detection of water proximity to tryptophan residues in proteins by single photon radioluminescence.

We recently developed a single photon radioluminescence (SPR) technique to measure submicroscopic distances in biological samples [Bicknese et al., and Shahrokh et al., Biophys. J., 63 (1992) 1256-1279]. SPR arises from the excitation of a fluorophore by the energy deposited from a slowing beta decay electron. The purpose of this study was to detect 3H2O molecules near tryptophan residues in proteins by tryptophan SPR. To detect small SPR signals, a sample compartment with reflective ellipsoidal optics was constructed, and amplified signals from a cooled photomultiplier were resolved by pulse-height analysis. A Monte Carlo calculation was carried out to quantify the relationship between SPR signal and 3H2O-tryptophan proximity. Measurements of tryptophan SPR were made on aqueous tryptophan; dissolved melittin (containing a single tryptophan); native and denatured aldolase; dissolved aldolase, monellin, and human serum albumin; and the integral membrane proteins CHIP28 (containing a putative aqueous pore) and MIP26 using 3H2O or the aqueous-phase probe 3H-3-O-methylglucose (OMG). After subtraction of a Bremsstrahlung background signal, the SPR signal from aqueous tryptophan (cps.microCi-1 mumol-1 +/- SE) was 8.6 +/- 0.2 with 3H2O and 7.8 +/- 0.3 with 3HOMG (n = 8). With 3H2O as donor, the SPR signal (cps.microCi-1 mumol-1) was 9.0 +/- 0.3 for monomeric melittin in low salt (trytophan exposed) and 4.6 +/- 0.8 (n = 9) for tetrameric melittin in high salt (tryptophans buried away from aqueous solution). The ratio of SPR signal obtained for aldolase under denaturing conditions of 8 M urea (fluorophores exposed) versus non-denaturing buffer (fluorophores buried) was 1.53 +/- 0.07 (n = 6). Ratios of SPR signals normalized to fluorescence intensities for monellin, aldolase, and human serum albumin, relative to that for d-tryptophan, were 1.42, 1.09, and 1.04, indicating that the cross-section for excitation of fluorophores in proteins is greater than that for tryptophan in solution. For the CHIP28 and MIP26 proteins in membranes, the ratio of SPR signal obtained with 3H2O versus 3HOMG was 1.35 +/- 0.13 (CHIP28, n = 5) and 0.99 +/- 0.02 (MIP26). These data are consistent with the existence of an aqueous channel through CHIP28 that excludes small solutes. We conclude that tryptophan radioluminescence in proteins is measurable and provides unique information about the presence of local aqueous compartments.

Calculation of resonance energy transfer in crowded biological membranes.

Analytical and numerical models were developed to describe fluorescence resonance energy transfer (RET) in crowded biological membranes. It was assumed that fluorescent donors were linked to membrane proteins and that acceptors were linked to membrane lipids. No restrictions were placed on the location of the donor within the protein or the partitioning of acceptors between the two leaflets of the bilayer; however, acceptors were excluded from the area occupied by proteins. Analytical equations were derived that give the average quantum yield of a donor at low protein concentrations. Monte Carlo simulations were used to generate protein and lipid distributions that were linked numerically with RET equations to determine the average quantum yield and the distribution of donor fluorescence lifetimes at high protein concentrations, up to 50% area fraction. The Monte Carlo results show such crowding always reduces the quantum yield, probably because crowding increases acceptor concentrations near donor-bearing proteins; the magnitude of the reduction increases monotonically with protein concentration. The Monte Carlo results also show that the distribution of fluorescence lifetimes can differ markedly, even for systems possessing the same average lifetime. The dependence of energy transfer on acceptor concentration, protein radius, donor position within the protein, and the fraction of acceptors in each leaflet was also examined. The model and results are directly applicable to the analysis of RET data obtained from biological membranes; their application should result in a more complete and accurate determination of the structures of membrane components.

Characterization of apocytochrome C binding to human erythrocytes.

The binding of 125I-labeled apocytochrome c to human erythrocytes was determined for free apocytochrome c concentrations at 10(-10)-10(-6) M. At about 2 x 10(-9) M, maximum cell association of apocytochrome c occurs at 50 mM NaCl and at 22 degrees C. Intact erythrocytes at 22 degrees C have three classes of apocytochrome c binding sites: one high-affinity noncooperative site (n1 = 728 per cell, Kd1 = 1.5 x 10(-9) M) and two positively cooperative sites (n2 = 3.7 x 10(4) per cell, Kd2 = 1.2 x 10(-7) M, alpha 2 = 2.0, and n3 = 2.5 x 10(5) per cell, Kd3 = 7.1 x 10(-7) M, alpha 3 = 12). Erythrocytes at 37 degrees C, and erythrocyte ghosts at 22 degrees C, also have three classes of apocytochrome c binding sites, and most sites are positively cooperative.

Segmental dynamics of the cytoplasmic domain of erythrocyte band 3 determined by time-resolved fluorescence anisotropy: sensitivity to pH and ligand binding.

Interactions between the erythrocyte membrane and its skeleton are mediated primarily by binding of cytoskeletal components to a conformationally sensitive structure, the cytoplasmic domain of band 3 (cdb3). To examine the nanosecond segmental motions of cdb3, band 3 was labeled selectively by fluorescein maleimide at Cys-201 near the proposed hinge in cdb3 about which pH-dependent conformational changes occur. Time-resolved anisotropy of labeled cdb3 in isolated form and in stripped erythrocyte membranes was measured by parallel-acquisition frequency-domain microfluorimetry. Samples had a single-component fluorescein lifetime of approximately 4 ns. Multifrequency phase and modulation data (5-200 MHz) fitted well to a segmental motion model containing two correlation times (tau 1c and tau 2c) and two limiting anisotropies (r1infinity and r2infinity). Measurements in protease-cleaved and denatured samples indicated that tau 1c (100-150 ps) corresponded to rapid rotation of bound fluorescein and tau 2c (2-5 ns) corresponded to segmental motion of cdb3. Both motions were hindered as quantified by nonzero r1infinity and r2infinity. The strong pH dependence of segmental motion correlated with that of cdb3 conformation measured by intrinsic tryptophan fluorescence. Significant changes in cdb3 segmental motion occurred upon interactions with the small ligands 2,3-bisphosphoglycerate and calcium and several glycolytic enzymes known to bind to the N terminus of band 3. These time-resolved fluorescence measurements of the nanosecond segmental dynamics of a labeled membrane protein provide evidence for the sensitivity of cdb3 conformation to ligand binding and suggest long-range structural communication through cdb3.

Cytoplasmic viscosity near the cell plasma membrane: measurement by evanescent field frequency-domain microfluorimetry.

The purpose of this study was to determine whether the unique physical milieu just beneath the cell plasma membrane influences the rheology of fluid-phase cytoplasm. Cytoplasmic viscosity was evaluated from the picosecond rotation of the small fluorophore 2',7'-bis-(2-carboxyethyl)-5-carboxyfluorescein (BCECF) by parallel-acquisition Fourier transform microfluorimetry (Fushimi and Verkman, 1991). Information about viscosity within < 200 nm of cell plasma membranes was obtained by selective excitation of fluorophores in an evanescent field created by total internal reflection (TIR) of impulse-modulated s-plane-polarized laser illumination (488 nm) at a glass-aqueous interface. Measurements of fluorescence lifetime and time-resolved anisotropy were carried out in solutions containing fluorescein or BCECF at known viscosities, and monolayers of BCECF-labeled Swiss 3T3 fibroblasts and Madin-Darby canine kidney (MDCK) cells. Specific concerns associated with time-resolved fluorescence measurements in the evanescent field were examined theoretically and/or experimentally, including variations in lifetime due to fluorophore proximity to the interface, and the use of the s and p polarized excitation. In fluorescein solutions excited with s-plane polarized light, there was a 5-10% decrease in fluorescein lifetime with TIR compared to trans (subcritical) illumination, but no change in rotational correlation time (approximately 98 ps/cP). Intracellular BCECF had a single lifetime of 3.7 +/- 0.1 ns near the cell plasma membrane. Apparent fluid-phase viscosity near the cell plasma membrane was 1.1 +/- 0.2 cP (fibroblast) and 1.0 +/- 0.2 cP (MDCK), not significantly different from the viscosity measured in bulk cytoplasm far from the plasma membrane. The results establish the methodology for time-resolved microfluorimetric measurement of polarization in the evanescent field and demonstrate that the cell plasma membrane has little effect on the fluid-phase viscosity of adjacent cytoplasm.

Defining the architecture of the red blood cell membrane: newer biophysical approaches.

For many years the red cell membrane has served as an extraordinarily valuable model for membrane structure and function. During the past 2 decades, the biochemical concept of the membrane skeleton was established, and, with the help of electron microscopy, a partial depiction of this structure evolved. Newer biophysical approaches designed to measure distances between various components of membrane skeleton as well as distances between the membrane skeleton and the overlying bilayer should now help to define this structure more realistically. Fluorescence resonance energy transfer, single photon radioluminescence, and total internal reflectance are three biophysical techniques that will enable us to measure such distances over a substantial range, which extends from a few Angstroms to approximately 2 microns. The ability to make such measurements in intact cells and in fully hydrated, undenatured membrane preparations should add a new dimension to our understanding of the structure of the red cell membrane.

Hereditary hemolytic disease with increased red blood cell phosphatidylcholine and dehydration: one, two, or many disorders?

We have compared characteristics of red cells from patients who were originally diagnosed as having two different disorders, high phosphatidyl choline hemolytic anemia (HPCHA) and hereditary xerocytosis (HX). Both types of cells had reduced intracellular potassium, with attendant cell dehydration and an increase in the relative amount of membrane phosphatidyl choline. Neither these observations nor a review of previous studies of HX and HPCHA revealed any means of distinguishing between the two disorders. Measurements of chloride-dependent potassium transport revealed flux characteristics in both HX and HPCHA red cells that were different from those in simultaneously run control samples. HX and HPCHA red cells did not show the same kinds of deviations from the normal pattern. However, extensive characterization of transport behavior under a variety of controlled conditions will be required to determine whether these differences represent intrinsic differences in chloride-dependent transport properties. It appears likely that HX and HPCHA both represent a spectrum of disorders resulting from a variety of defects that produce the same general pattern of abnormalities in cation content and membrane phospholipid composition.

Single photon radioluminescence. I. Theory and spectroscopic properties.

The excitation of a fluorescent molecule by a beta-decay electron (radioluminescence) depends upon the electron energy, the distance between radioactive 'donor' and fluorescent 'acceptor', and the excitation characteristics and solvent environment of the fluorophore. The theory for calculation of single photon radioluminescence (SPR) signals is developed here; in the accompanying paper, measurement methods and biological applications are presented. To calculate the three-dimensional spatial profile for electron energy deposition in an aqueous environment, a Monte Carlo calculation was performed incorporating theories of electron energy distributions, energy loss due to interactions with matter, and deflections in electron motion due to collisions. For low energy beta emitters, 50% of energy deposition occurs within 0.63 micron (3H, 18.5 keV), 22 microns (14C, 156 keV), 25 microns (35S, 167 keV), and 260 microns (36Cl, 712 keV) of the radioisotope. In close proximity to the beta emitter (100 nm, 3H; 10 microns, 14C) the probability for fluorophore excitation is approximately proportional to the inverse square of the distance between the beta emitter and fluorophore. To investigate the other factors that determine the probability for fluorophore excitation, SPR measurements were carried out in solutions containing 3H and a series of fluorophores in different solvents. In water, the probability of fluorescence excitation was nearly proportional to the integrated absorbance over a > 1,000-fold variation in absorbances. The probability of fluorescence excitation was enhanced up to 2,600-fold when the fluorophore was in a "scintillant" aromatic or hydrocarbon solvent. SPR emission spectra were similar to fluorescence emission spectra obtained with photon excitation. The single photon signal due to Bremsstrahlung increased with wavelength in agreement with theory. The distance dependence for the SPR signal predicted by the model was in good agreement with measurements in which a 14C donor was separated by known thicknesses of water from a fluorescently-coated coverglass. Quantitative predictions for radioluminescence signal as a function of donor-acceptor distance were developed for specific radioisotope-fluorophore geometries in biological samples.

Single photon radioluminescence. II. Signal detection and biological applications.

A quantitative theory for excitation of fluorescent molecules by beta decay electrons is reported in the accompanying manuscript; experimental detection methods and biological applications are reported here. The single photon signals produced by an excited fluorophore (single photon radioluminescence, SPR) provide quantitative information about the distance between radioisotope and fluorophore. Instrumentation was constructed for SPR signal detection. Photons produced in a 0.5-ml sample volume were detected by a cooled photomultiplier and photon counting electronics. To minimize electronic noise and drift for detection of very small SPR signals, a mechanical light chopper was used for gated-signal detection, and a pulse height analyzer for noise rejection. SPR signals of approximately 1 cps were reproducibly measurable. The influence of inner filter effect, sample turbidity, and fluorophore environment (lipid, protein, and carbohydrate) on SPR signals were evaluated experimentally. SPR was then applied to measure lipid exchange kinetics, ligand binding, and membrane transport, and to determine an intermolecular distance in an intact membrane. (a. Lipid exchange kinetics.) Transfer of 12-anthroyloxystearic acid (12-AS) from sonicated lipid vesicles and micelles to vesicles containing 3H-cholesterol was measured from the time course of increasing SPR signal. At 22 degrees C, the half-times for 12-AS transfer from vesicles and micelles were 3.3 and 1.1 min, respectively. (b. Ligand binding.) Binding of 3H-oleic acid to albumin in solution, and 3H-2,2'-dihydro-4,4'-diisothiocyanodisulfonic stilbene (3H-H2DIDS) to band 3 on the erythrocyte membranes were detected by the radioluminescence of the intrinsic tryptophans. The SPR signal from 5 microCi 3H-oleic acid bound to 0.3 mM albumin decreased from 13 +/- 2 cps to 3 +/- 2 cps upon addition of nonradioactive oleic acid, giving 2.7 high affinity oleic acid binding sites per albumin. The SPR signal from 1 microCi 3H-H2DIDS bound selectively to erythrocyte band 3 in erythrocyte ghosts (1.5 mg protein/ml) was 2.2 +/- 0.8 cps. (c. Membrane transport). Dilution of J774 macrophages loaded with 3H-3-O-methylglucose and BCECF gave a decreasing SPR signal with a half-time of 81 s due to methylglucose efflux; the SPR measurement of the efflux rate was in agreement with a conventional tracer efflux rate determination by filtration. 20 microM cytochalasin B inhibited efflux by 97%. (d. Distance determination.) The SPR signal from erythrocyte membranes labeled with 27 microCi 3H-oleic acid and 10 microM of fluorescein-labeled wheat germ agglutinin was 5.7 +/- 0.5 cps, giving an average glycocalyx-to-bilayer distance of 5 nm. The results establish methods for experimental detection of SPR signals and demonstrate the applications of radioluminescence to the measurement of lipid exchange kinetics, ligand binding, membrane transport, and submicroscopic distances in intact membranes in real time.

A novel photoactivatable cross-linker for the functionally-directed region-specific fluorescent labeling of proteins.

A cleavable cross-linking reagent, sulfosuccinimidyl-2(7-azido-4-methylcoumarin-3-acetamido)-ethyl-1,3'- dithiopropionate (SAED), was synthesized for the selective transfer of a coumarin fluorophore from a 'donor' protein to a position near the binding site of an interacting 'target' protein. SAED contains a terminal N-sulfosuccinimidyl ester for conjugation to the donor, a terminal photoactivatable azido-coumarin species for cross-linking with the interacting target, and a central disulfide spacer for the release of the labeled target after cleavage. To evaluate the effectiveness of this labeling reagent, soybean trypsin inhibitor (STI) was derivatized (approximately 0.5 mol/mol) with SAED and then photolyzed in the presence of trypsin. A single fluorescent cross-linked species (6-7 mol% of total STI) was observed by SDS/PAGE and, after reductive cleavage, was shown to be a 1:1 STI-trypsin complex. This complex was not detected without photolysis or with an inactivated cross-linker. Importantly, complex formation was inhibited by an excess of unmodified STI and prevented by substitution of a non-interacting protein for trypsin. Cleavage of the cross-linked complex revealed that the trypsin, but not the STI, was fluorescent; the uncomplexed trypsin fraction remained unlabeled. These results demonstrated the specificity of the labeling of trypsin by fluorescent-transfer cross-linking with SAED. An efficiency of about 15% for this cross-linking mediated labeling of trypsin was calculated. The short cross-linking span of SAED (less than or equal to 1.8 nm) strictly limited the labeling to the vicinity of the contact region of trypsin with STI. Thus, this novel cross-linker permits the region-specific targeting of a fluorophore near a functionally important binding site.

Conformational changes in the foot protein of the sarcoplasmic reticulum assessed by site-directed fluorescent labeling.

Ca2+ release from sarcoplasmic reticulum during excitation--contraction coupling is likely to be mediated by conformational changes in the foot protein moiety of the triadic vesicles. As a preparative step toward the studies of dynamic conformational changes in the foot protein moiety, we have developed a new method that permits specific labeling of the foot protein moiety of the isolated membranes with a fluorophore. A novel fluorescent cleavable photoaffinity cross-linking reagent, sulfosuccinimidyl 3-((2-(7-azido-4-methylcoumarin-3-acetamido)ethyl)dithio)propionate (SAED), was conjugated with site-directing carriers, polylysine (Ca(2+)-release inducer) and neomycin (Ca(2+)-release blocker). The conjugates were allowed to bind to polylysine- and neomycin-binding sites of the heavy fraction of SR (HSR). After photolysis, the cross-linked reagent was cleaved by reduction and the fluorescently labeled HSR was separated from the carriers by centrifugation. These procedures led to specific incorporation of the methylcoumarin acetate (MCA) into the foot protein. Polylysine and neomycin bound to different sites of the foot protein, since neomycin, at release-blocking concentrations, did not interfere with polylysine binding. The fluorescence intensity of the foot protein labeled with the carrier, neomycin, showed biphasic changes as a function of ryanodine concentration (increasing up to 1 microM ryanodine and decreasing above it), while with the carrier polylysine, ryanodine induced no change in fluorescence intensity. In contrast, the fluorescence intensity of the foot protein labeled with each of the two carriers, neomycin and polylysine, showed almost identical calcium dependence (first increasing from 0.1 microM to about 3.0 microM calcium concentration, and then decreasing at higher calcium concentrations).(ABSTRACT TRUNCATED AT 250 WORDS)

Distance between skeletal protein 4.1 and the erythrocyte membrane bilayer measured by resonance energy transfer.

To assess the molecular architecture of the human erythrocyte skeletal protein 4.1:bilayer interface, the distance between a donor sulfhydryl-specific fluorescent probe attached to a region near the glycophorin-binding domain of protein 4.1 and an acceptor lipophilic probe in the exposed leaflet of inside-out vesicles (IOVs) was measured by fluorescence resonance energy transfer. To prevent aggregation and loss of function, protein 4.1 was labeled in situ on the surface of IOVs, purified, and rebound onto fresh IOVs. The labeled protein 4.1 was similar to the native protein in its gel electrophoretic pattern and its binding affinity to stripped-IOVs (Kd 35 +/- 4 nM). Energy transfer was assessed using two donor-acceptor pairs, 5-[2-[(iodoacetyl)amino]ethyl] aminonaphthalene-1-sulfonic acid and 3,3'-ditetradecyloxacarbocyanine perchlorate, or 5-iodoacetamidofluorescein and tetramethylrhodamine phosphatidylethanolamine. Using both donor fluorescence intensity and lifetime quenching measurements, an average distance of 75 +/- 5 A between the probe on the protein and the surface of IOVs was found. In parallel fluorescence resonance energy transfer studies with protein 4.1 and liposomes with a phospholipid composition similar to the inner leaflet of the red cell membrane, a closer distance was found (49 +/- 5 A). Two control experiments validated energy transfer: (a) the spectrum of a mixture of IOVs separately labeled with donor and acceptor was different from the spectrum of the doubly labeled IOVs at identical donor and acceptor concentrations; and (b) no energy transfer was observed following detergent disruption of the geometric relationship between donor and acceptor. Taken together, these observations suggest that membrane-bound protein 4.1 is elongated and that the labeled site is located at a position deep in the 30-kDa N-terminal glycophorin-binding domain of the protein. The data are also consistent with the view that the cytoplasmic tail of glycophorin is interposed between protein 4.1 and the lipids. These experiments represent the first measurement of a distance between a skeletal protein and the lipid bilayer.

Measurement and analysis of triplet-state lifetimes by multifrequency cross-correlation phase and modulation phosphorimetry.

In this paper we describe a novel approach to study the triplet-state lifetimes by a conventional multifrequency cross-correlation phase and modulation apparatus. The analysis of phase and modulation data of eosin-labeled band 3 erythrocyte ghosts revealed the existence of two phosphorescence lifetime values of 2700 and 750 microseconds, with a fractional contribution of 78 and 22%, respectively, which are in good agreement with those reported in the literature. Differential polarization phase analysis, which facilitates the study of the rotational properties of band 3, provided data in good agreement with those reported in the literature. The method proposed in this paper to study the radiative emission from the triplet state may represent a convenient alternative to the pulse laser flash technique.

Effect of L-carnitine and acetyl-L-carnitine on the human erythrocyte membrane stability and deformability.

In this study we examined the effect of carnitine and acetylcarnitine on the human erythrocyte membrane stability and membrane deformability. Since erythrocyte membranes are impermeable to these compounds, we resealed erythrocyte ghosts in the presence of different concentrations of carnitine or acetylcarnitine. Resealed ghosts can be adequately studied in their cellular deformability and membrane stability properties by means of ektacytometry. Both carnitine and acetylcarnitine alter the membrane stability but not membrane deformability of the red cell membrane. Resealed ghosts containing 20, 50, 150, and 300 microM carnitine had 1.1, 1.6, 0.9, and 0.7 times the normal stability. While resealed ghosts containing 20, 50, 150, and 300 microM acetylcarnitine had 1.1, 1.5, 1.3, and 1.2 times the normal stability. Such changes were found to be reversible. We also conducted SDS PAGE of cytoskeletal membrane proteins from membrane fragments and residual membranes produced during membrane stability analysis, and unsheared resealed membranes in those samples where we observed an increase or a decrease of membrane stability. No changes in the cytoskeletal membrane proteins were noticed, even when the samples, prior SDS PAGE analysis, were treated with or without dithiothreitol. In addition, fluorescence steady state anisotropy of DPH in the erythrocyte membrane treated with carnitine or acetylcarnitine shows no modification of the lipid order parameter. Our results would suggest that both carnitine and its acetyl-ester, at physiological concentrations, may increase membrane stability in mature erythrocytes, most likely via a specific interaction with one or more cytoskeletal proteins, and that this effect would manifest when the erythrocytes are subjected to high shear stress.