Brigham Young University BYU ScholarsArchive All Theses and Dissertations 2006-11-30 The Influence of Membrane Lipid Order on Cell Shape and Microvesiculation in Human Erythrocytes Laurie Jackson Gonzalez Brigham Young University - Provo Follow this and additional works at: http://scholarsarchive.byu.edu/etd Part of the Cell and Developmental Biology Commons, and the Physiology Commons BYU ScholarsArchive Citation Gonzalez, Laurie Jackson, "The Influence of Membrane Lipid Order on Cell Shape and Microvesiculation in Human Erythrocytes" (2006). All Theses and Dissertations. Paper 1058. This Thesis is brought to you for free and open access by BYU ScholarsArchive. It has been accepted for inclusion in All Theses and Dissertations by an authorized administrator of BYU ScholarsArchive. For more information, please contact [email protected]. THE INFLUENCE OF MEMBRANE LIPID ORDER ON CELL SHAPE AND MICROVESICULATION IN HUMAN ERYTHROCYTES by Laurie J. Gonzalez A thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of Master of Science Department of Physiology and Developmental Biology Brigham Young University December 2006 BRIGHAM YOUNG UNIVERSITY GRADUATE COMMITTEE APPROVAL of a thesis submitted by Laurie J. Gonzalez This thesis has been read by each member of the following graduate committee and by majority vote has been found to be satisfactory. ______________________________ Date ____________________________________ John D. Bell, Chair ______________________________ Date ____________________________________ William S. Bradshaw ______________________________ Date ____________________________________ Allan M. Judd BRIGHAM YOUNG UNIVERSITY As chair of the candidate’s graduate committee, I have read the thesis of Laurie J. Gonzalez in its final form and have found that (1) its format, citations, and bibliographical style are consistent and acceptable and fulfill university and department style requirements; (2) its illustrative materials including figures, tables, and charts are in place; and (3) the final manuscript is satisfactory to the graduate committee and is ready for submission to the university library. __________________________ Date __________________________________________ John D. Bell Chair, Graduate Committee Accepted for the Department __________________________________________ James P. Porter Chair. Physiology and Developmental Biology Accepted for the College __________________________________________ Alan R. Harker Associate Dean, College of Biology and Agriculture ABSTRACT THE INFLUENCE OF MEMBRANE LIPID ORDER ON CELL SHAPE AND MICROVESICULATION IN HUMAN ERYTHROCYTES Laurie J. Gonzalez Department of Physiology and Developmental Biology Master of Science Exposure of human erythrocytes to elevated intracellular calcium causes alterations in cell shape and stimulates shedding of the cell membrane in the form of microvesicles. We hypothesized that both the shape transition and microvesiculation are influenced by microscopic membrane physical properties such as lipid order. To test this hypothesis, membrane properties were manipulated by varying the experimental temperature, membrane cholesterol content, and the internal ionic environment. Changes in membrane order were assessed using steady-state fluorescence spectroscopy with an environment-sensitive probe, laurdan. Our observations led us to the following conclusions: 1) the modest temperature dependence of membrane structure observed with laurdan is shifted to lower temperatures and becomes more cooperative upon removal of membrane cholesterol, 2) the calcium-induced shape change observed in erythrocytes requires a decrease in membrane order, 3) the influence of membrane order is not limited to shape transitions induced only by calcium, and 4) decreased order is also a permissive factor for microvesicle shedding. Our data suggest that while the mechansims that regulate the shape transition and the release of microvesicles are different, they both require a state of membrane disorder. ACKNOWLEDGMENTS Gratitude is expressed to Dr. John Bell for his role as an excellent mentor and advisor. Not only did he provide me with the opportunity to have a fine graduate experience, but through his leadership this project was also the means of training many undergraduate scientists, including: Jeremy Fairbourn, Taylor Brueseke, Mai Vu, Quinn Bahm, Erin Olson, Rachel Bailey, Chisako McLemore, and Brian Thurber. I appreciate their assistance in completing the experiments described in this paper. Thanks to Samantha Smith for her input on the Laurdan experiments. I am deeply grateful to my family for their encouragment and hospitality, and above all to my husband, Casey, for his support and patience while I completed this work. TABLE OF CONTENTS 1. INTRODUCTION…………………………………………………………..1 2. MATERIALS AND METHODS…………………………………………...3 3. RESULTS…………………………………………………………………...8 4. FIGURES AND FIGURE LEGENDS……………………………………..14 5. DISCUSSION……………………………………………………………....27 6. LITERATURE REVIEW…………………………………………………..35 7. REFERENCES…..………………………………………………………….50 vii INTRODUCTION Human erythrocytes are characterized by their resting discoid shape and deformability, which allows them to pass through tiny capillaries to facilitate gas exchange. Physical and chemical properties of the plasma membrane contribute to these characteristics. The membrane consists of 52% protein, 40% lipid, and 8% carbohydrate (Nakao, 2002). Intrinsic proteins of the membrane serve as a connection to an underlying cytoskeleton and include band 3 (AE1), glycophorin C and transport adenosine triphosphatases. The cytoskeleton is located just below the membrane and is composed of spectrin fibers arranged in a hexagonal array, along with actin, protein 4.1, adducin, ankyrin, p55, tropomyosin, tropomodulin, calmodulin and various others. The primary lipid components of the membrane are phospholipids and approximately equimolar cholesterol arranged in a bilayer (Lange et al., 1980). In erythrocytes, the understanding of an asymmetrical arrangement of phospholipids between the two leaflets of the bilayer has been well established. Most of the cholinecontaining lipids are found in the outer leaflet, while the majority of phosphatidylserine (PS), phosphatidylethanolamine (PE), and phosphatidylinositol (PI) are in the inner leaflet (Zachowski, 1993). Carbohydrates are localized on the external face of the membrane covalently bound to lipids and proteins designated as glycolipids and glycoproteins. The individual behavior and interactions of the lipids and proteins in the membrane contribute to its ability to deform. In addition to typical circulation stresses, the cell shape is sensitive to the well-being of the cell and as erythrocytes become aged or damaged, the shape changes. Furthermore, under these conditions the cells also exhibit 1 microvesicle release, or “blebbing” of the plasma membrane. These changes are similar to what happens during platelet activation, and in other cell types during apoptosis and necrosis (Chukhlovin, 1996). Experimentally, the shape change and concomittant microvesicle release can be induced by lowering intracellular ATP or elevating intracellular calcium. Moreover, increased cytoplasmic calcium causes other physical changes to the membrane including increased exposure of PS in the outer leaflet (flip-flop), susceptibility of the membrane to hydrolysis via secretory phospholipase A2, and increased ordering of membrane lipids (Henseleit et al., 1990; Smith et al., 2001; Vest et al., 2004). Efforts have been made to understand more specifically the effects of calcium on erythrocyte shape change and microvesicle release (Allan and Thomas, 1981; Bucki et al., 1998; Comfurious et al., 1990; Gedde et al., 1997; Greenwalt, 2006; Greco et al., 2006; Liu et al., 2005; Muller et al., 1981; Pasquet et al., 1998; Wolfs et al., 2003). What remains to be elucidated, however, is an explanation of the potential relationship between these phenomena and membrane fluidity. In order to accomplish this purpose, we have manipulated membrane properties by varying the experimental temperature, membrane cholesterol content, and the internal ionic environment of erythrocytes. We then assessed the effects of these manipulations on the release of microvesicles and an erythrocyte shape transition initiated by treatment with the ionophore, ionomycin. Membrane cholesterol was removed from the erythrocytes with the cholesterolbinding agent methyl-ß-cyclodextrin (MBCD). Cyclodextrins have been used in pharmacology research for years in delivery of lipophilic drugs and have recently become important in membrane studies mainly because they have been shown to selectively 2 extract membrane cholesterol in multiple cell types, including erythrocytes (Klein et al., 1995; Lange et al., 2002; Ohtani et al., 1989; Wolkers et al., 2002; Yancey et al., 1996). Ohtani et al. showed that MBCD neither bonds to nor incorporates into the membrane (1989). MBCD acts at the membrane surface extracting cholesterol into a central, nonpolar cavity of cyclic oligomers of glucopyranoside (Pitha et al., 1988). Membrane order was assessed by steady-state fluorescence spectroscopy with an environment-sensitive probe, laurdan. Laurdan is sensitive to the presence and mobility of water molecules within the bilayer, yielding information on membrane order and fluidity (Parasassi et al., 1991, 1993, 1997). It has been used previously to study effects of temperature and divalent cations on membrane lipid order in erythrocytes (Best et al., 2002; Smith et al., 2001; Vest et al., 2004). Harris et al. used laurdan fluorescence to study the effects of membrane cholesterol concentration on fluidity in artificial membranes (2002). Subsequently, we used this data to aid in our interpretation of the measurements of microvesicle shedding and shape change with cholesterol-depleted cells. MATERIALS AND METHODS Materials - Erythrocytes were obtained from healthy individuals undergoing routine physicals at Brigham Young University McDonald Health Center. The samples were fresh or stored up to 2 days at 4 °C in EDTA vacutainers from which patient identification was removed. Control experiments comparing fresh blood with stored samples demonstrated that the storage conditions did not influence the results (Smith et al., 2001). Erythrocytes were isolated by centrifugation, plasma and buffy coat removed, 3 washed, centrifuged a second time, and resuspended to the original hematocrit in a lowcalcium, low-magnesium cell medium (LCCM) (NaCl = 134 mM, KCl = 6.2 mM, Hepes = 18.0 mM, glucose = 13.6 mM, pH 7.4, 37 °C). Cell preparations for experiments using indo-1 used MBSS as a cell medium (NaCl = 134 mM, KCl = 6.2 mM, CaCl2 = 1.6 mM, MgCl2 = 1.2 mM, Hepes = 18.0 mM, and glucose = 13.6 mM, pH 7.4, 37 °C). Laurdan (6-dodecanoyl-2-dimethylaminonapthalene), indo-1 (acetoxymethyl ester form), and the Amplex Red Cholesterol Assay Kit were purchased from Invitrogen (Carlsbad, CA). Ionomycin was purchased from Calbiochem (La Jolla, CA) and MBCD from Sigma-Aldrich (St. Louis, MO). All other reagents are from standard sources. Laurdan (250 µM), ionomycin (120 µM) and indo-1 (2.5 µM) were dissolved in dimethylsulfoxide (DMSO). MBCD (0.1 mM, 0.3 mM, 1.0 mM) was dissolved in LCCM. BaCl2, CaCl2, CoCl2, MgCl2, MnCl2, NiSO4, and Sr(NO3)2 were dissolved at 1.0 M stock concentrations in deionized water and then used at appropriate concentrations. Control experiments indicate that the addition of these ions to LCCM at the concentration used in this study (0.6 mM) does not significantly alter pH (Vest et al., 2004). Fluorescence spectroscopy - Steady-state fluorescence was monitored for fluorescent probes laurdan and indo-1 using photon-counting spectrofluorometers (Fluoromax and Fluoromax-3 from Jobin Yvon, Edison, NJ, and PC1 from ISS, Champaign, IL). All three instruments maintain sample homogeneity by continuous gentle stirring with a magnetic stir bar. Control experiments (not shown) show that stir bar speed had no effect on light scatter noise. Sample temperature was controlled and maintained using circulating water baths and equilibrated for at least 5 minutes to achieve 4 temperature stability. In both Fluoromax instruments, simultaneous assessment of fluorescence intensity at multiple excitation and emission wavelengths was obtained by rapid sluing of monochromator mirrors using control software provided with the instrument. Band pass was set at 4 nm for both monochromators. In all instruments, erythrocyte preparations were suspended in 2 ml of MBSS or LCCM in a quartz fluorometer sample cell to a final density of about 3 - 4 x 106 cells/ ml. Rayleigh light scattering - Light scattering was assessed in samples of erythrocytes prepared as described for fluorescence spectroscopy. No fluorescent probes were included in the experiments and monochromator settings were set to 500 nm excitation and 510 nm emission. Intracellular calcium influx - Intracellular calcium concentrations at 25 °C, 37 °C and 45 °C were assessed using indo-1 as described previously (Wilson et al., 2004). Erythrocyte samples were prepared as described above using MBSS and further diluted to a density of 1.5 - 2 x 106 cells/ ml. Indo-1 (final concentration = 2.5 µM) was added and incubated for 60 minutes at 37 °C in a shaking water bath. Cells were washed, resuspended in MBSS, and placed in cuvette (final volume = 2 ml). Fluorescence was continually monitored with excitation set at 350 nm and emission at 405 to 480 nm. A baseline was established for 3 minutes, followed by the addition of ionomycin (final concentration = 0.3 µM) and then a continuation of the time course for 13 additional minutes. Laurdan generalized polarization (GP) - Erythrocytes were prepared with LCCM as described above for fluorescence experiments. Samples were incubated with varying concentrations of MBCD (0.1 mM, 0.3 mM, or 1.0 mM) or a deionized water control for 5 30 minutes. After washing and resuspending cells to original concentrations, CaCl2 (final concentration = 0.6 mM) and laurdan (final concentration = 2.5 µM) were added to bring the total volume to 2 ml and placed in a quartz cuvette. In order to allow the laurdan to fully equilibrate into the membrane, samples were processed through a successive temperature series (25 °C, 30 °C, 35 °C, 40 °C, and 45 °C) recording the emission spectrum (excitation at 350 nm and emission from 360 to 600 nm) for each temperature to monitor incorporation. Incorporation did not change during the third series, so in the fourth series data were collected for the desired temperatures. Results were quantified by calculating the generalized polarization (GP) of laurdan at 435 nm and 500 nm as described by Parasassi et al. (1991). Quantification of cholesterol extraction - Washed erythrocytes were suspended in MBSS to a final volume of 1 ml and incubated in the presence or absence of varying concentrations (0.1 mM, 0.3 mM or 1.0 mM) of MBCD for 30 minutes at 37 °C. Cells were washed and separated by centrifugation (13,500 rpm for 120 seconds) in a microcentrifuge. The supernatant was removed and cholesterol was extracted from it by adding 900 ml chloroform, vortexing, removing organic layer and drying under a nitrogen stream. Cell pellets were frozen in liquid nitrogen to lyse the cells. Samples were quickly thawed, and lipids were extracted with chloroform and methanol using the method of Bligh and Dyer (1959). In brief, 150 µl of chilled MBSS was added to suspend the pellet followed by 125 µl chloroform and 250 µl methanol. After vortexing the tubes for 10 seconds, 125 µl of deionized water was added. The samples were vortexed and centrifuged for 30 seconds at 13,500 rpm. The residual organic layer was separated and 6 dried under a nitrogen stream. Samples were stored at –20 °C until utilized for the cholesterol assay. Reagents and basic protocol for quantification of cell and supernatant cholesterol were from the Amplex Red Cholesterol Assay Kit (Invitrogen). Stock solutions of reagents were prepared and stored at -20 °C. Briefly, 50 µl of distilled water and 50 µl of amplex red working solution was added to the dried supernatant and cell samples. Samples were incubated for 30 minutes at 37 °C in a shaking water bath, after which 50 µl was removed and added to deionized water in a quartz cuvette (final volume = 2 ml). Fluorescence emission spectrum were collected using excitation at 560 nm and emission from 570 to 700 nm and values for experimental samples were compared to a standard curve to determine concentrations. Microscopy - Erythrocytes were suspended in 2 ml LCCM in a 24-well plate dish at a final density of 3 - 4 x106 cells/ ml and placed in a shaking water bath and warmed to the determined temperature. After temperature equilibration, divalent ions (BaCl2, CaCl2, CoCl2, MgCl2, MnCl2, NiSO4) were added to different wells at a final concentration of 0.6 mM and allowed to mix for 5 minutes. Ionomycin (final concentration = 0.3 µM) was added and after 10 minutes, the plate was removed from the bath and photomicrographs collected on a Canon IX70 inverted light microscope. Data were collected for individual well plates at 25 °C, 30 °C, 33 °C, 37 °C, 40 °C and 45 °C. Photomicrographs of cholesterol-depleted cells were also collected at the same temperatures. LCCM-prepared erythrocytes were incubated with varying concentrations of MBCD (0.1 mM, 0.3 mM, or 1.0 mM) at 37 °C for 30 minutes. After incubation, the temperature of bath was changed to the desired experimental temperature. After reaching the set point, CaCl2 was added 7 (final concentration = 0.6 mM), followed 5 minutes later by ionomycin (final concentration = 0.3 µM). After a 10 minute incubation, the plate was removed for image collection. RESULTS At 45 °C, the addition of ionomycin to human erythrocytes at in the presence of calcium caused an increase in the intensity of light scattered by the sample concurrent with a decrease in the signal noise (Figure 1). Previous studies have demonstrated that the elevated scattering intensity results from an increase in the number of particles available to reflect light due to microvesicle shedding (Smith et al., 2001). Furthermore, changes in light-scatter noise apparently report the transition in cell shape from discocyte to a smaller rounded shape called spherocyte (Hoffman, 1987; Smith et al., 2001). As discocytes, erythrocytes aggregate as rouleaux in circulation (Derganc et al., 2003). These large structures reflect light irregularly as they move in a stirred suspension. As the shape changes, the rouleaux break apart, and the noise decreases as the suspension becomes more homogenous in terms of particle size. Figure 2 displays visual confirmation of the shape changes associated with the light scattering data. Figure 1 also shows that these changes in light scattering depended on the experimental temperature. They were clearly evident at 45 °C, reminiscent of similar effects observed previously at 37 °C (Vest et al., 2004). Conversely, neither the increase in intensity nor the reduction in signal noise was observed at 25 °C. Photomicrographs of treated cells at 25 °C do, however, show some changes. However, these alterations in shape represent an early transition to irregular discocytes and early echinocytes compared 8 to the advanced spherocytes and spheroechinocytes seen at 45 °C. While not quantitative, the images provide a more complete understanding of what is happening to the cell during these changes. In order to establish that the observed temperature dependence was not due to the ability of ionomycin to transport ions from the extracellular environment, we used the fluorescent probe indo-1 to report relative internal calcium ion concentration at 25 °C, 37 °C, and 45 °C. As illustrated in Figure 3, there was no statistical difference among the treatments. Although calcium flux was slower at 25 °C than at higher temperatures, there was no statistical difference in the end point level of calcium achieved after 600 seconds. This result was further validated by examining longer time courses (3000 seconds, data not shown). The temperature effect suggests the possibility that membrane physical properties are relevant to the processes involved in microvesicle release and the transition in cell shape. Although microvesicle shedding stimulated by calcium influx requires specific proteins such as calcium-dependent enzymes and ion channels (Allan and Thomas, 1981; Smith et al., 2001), recent evidence suggests that the effect of calcium on cell shape may involve direct interactions of the ion with the inner face of the cell membrane (Vest et al., 2004). Specifically, it was found that while calcium uptake causes shedding at 37 °C, a broader range of ions are capable of initiating the shape transition. Introduction of cobalt, nickel or manganese ions (but not strontium, magnesium, or barium) into erythocytes produces effects on cell shape similar to those caused by calcium (Vest et al., 2004). If the hypothetical link between membrane structure and the shape transition suggested by 9 Figure 1 is real, it should be manifest for each of the ions capable of causing that transition. Accordingly, the experiments in Figure 1 were repeated using erythrocytes treated with other divalent cations: manganese, cobalt, nickel, magnesium and barium (Figure 4). As expected, the level of signal noise diminished at 45 °C upon addition of ionomycin in each case except for magnesium and barium (data for barium not shown). Only manganese showed any evidence for microvesicle release at 45 °C. As observed with calcium, no changes were apparent with any ion for either parameter at 25 °C. Once again, the photomicrographs offer additional insight. Manganese, cobalt and even magnesium show early changes in the cell shape at 25 °C (Figure 5). As indicated in the figure, cells treated with magnesium at 25 °C are irregular and may be due to a nonspecific effect; repetition would be required to confirm this. At 45 °C, magnesium had no effect, but the effect of other ions on cell shape is advanced compared to the changes seen at 25 °C in agreement with the light scattering data. Figures 6 & 7 show summaries of light scattering data obtained from multiple samples like those shown in Figure 4. Figure 6 shows the effect of both low and high temperature on light scatter intensity (MV release) in the presence of calcium, manganese, cobalt, or nickel. At low temperatures, no ion caused a significant change. On the contrary, at 45 °C calcium treatment produced a large increase in intensity while cobalt resulted in a minor decrease. Magnesium and barium were also assayed and had no effect at either temperature, consistent with recent studies (Vest et al., 2004). Figure 7 illustrates the temperature effect on signal noise. In general, the average trend at 25 °C was toward a decrease in noise. However, this trend was sufficiently consistent to be 10 statistically significant only in the case of manganese. None of the groups were distinguishable from each other by analysis of variance. The trend towards a decrease in noise supports the early changes seen in the photomicrographs (Figures 2 & 5). In contrast, at 45 °C all ions caused a reproducible diminution in noise, manganese being the most obvious. To further explore possible relationships between membrane physical properties and calcium stimulation of the shape transition and microvesicle release, we repeated the experiments of Figure 1 at many temperatures and compared the results to measurements of laurdan fluorescence (Figure 9). Figure 8A represents the temperature dependence of the change in average signal noise following 600 seconds of incubation with ionomycin. In the range of 20 to 27 °C the change in noise increased steadily with temperature. Between 27 and 43 °C, the effect of temperature was more modest. The slope became more steep again from 43 to 48 °C. The change in light scatter intensity (Figure 8B) followed a similar trend, although the details were somewhat different. The intensity change rose very little from 20 to 30 °C, followed by a steep increase to 33 °C, a shallow rise until 37 °C, and finally a sharp increase to 48 °C. Figure 8C illustrates the effect of temperature on membrane order detected by the fluorescent probe laurdan. Laurdan is a fluorescent probe sensitive to the presence and mobility of water molecules trapped within the lipid bilayer (Parasassi et al., 1991, 1993, 1997) and has been shown to detect lipid order in the membrane (Harris et al., 2002). These data were analyzed by calculating GP, a quantitative method of evaluating shifts in laurdan spectra due to the solvent relaxation effect (Parnassi et al., 1991). Decreased GP values indicate increased solvent relaxation due to an increase in membrane water 11 content. As the temperature increased, the GP value decreased, indicating decreased membrane order. These results were consistent with previous observations made in our laboratory (Best et al., 2002). If the changes observed in shape transition and microvesicle shedding are dependent on membrane physical properties, then altering membrane cholesterol content should affect the results in a predictable manner. Figure 9 shows 5 panels, the upper 4 each representing samples treated with different concentrations of MBCD, followed by a summary of superimposed data (for clarity of presentation, only means are shown). Panel A is the same data illustrated in Figure 8C. As the concentration of MBCD increased, the GP value decreased concurrent with a shift in the curve toward lower temperatures suggesting a reduction in membrane lipid order. In cells with no MBCD, a mild transition towards decreased order occurred between 35 to 40 °C. By comparison, the cells treated with 1.0 mM MBCD saw a more dramatic transition toward decreased order between 25 to 30 °C, showing reduced cholesterol allowed the transition to occur at a lower temperature than in the control cells. Data in Figure 10 justify normalizing the GP values for the initial value at 25 °C, showing that the GP at the starting temperature of 25 °C is not significantly different for any given concentration of MBCD. While the absolute value of GP is not distinguishable from sample to sample because of donor effect, we wanted to know if the shape of the temperature curve was altered by MBCD concentration. A two-way analysis of variance was performed for the normalized data to see whether the temperature or the MBCD concentration had a significant effect on the results (p < 0.0001 for both). The interaction between the two variables was not significant (p = .99). 12 Visual inspection of the data in Figure 11 shows that removal of membrane cholesterol resulted in greater differences in light scatter intensity before and after the addition of ionomycin for both 0.3 mM and 1.0 mM MBCD. The data at 0.1 mM MBCD do not appear very different from those obtained for the control condition. A two-way analysis of variance showed that both MBCD and temperature had a significant effect on the results (p < 0.001 for both), and that the interaction between the two was also significant (p = 0.012), n = 3-4. The interaction between temperature and MBCD concentration is not unexpected, given that the data for both variables follow the same trend towards an increase of light scatter. Figure 12 shows the effect of cholesterol depletion on the shape transition. Photos and analysis of the light scattering of cells treated with 1.0 mM MBCD illustrate that the shape change occurred prior to ionomycin treatment; cells were almost all spherocytes regardless of whether they were treated without calcium, calcium only, calcium + ionomycin, or ionomycin only. This effect was similar for all temperatures. The results at 0.1 mM and 0.3 mM MBCD (not shown) also show changes in cell shape prior to ionomycin treatment, though not as dramatic as the 1.0 mM treatment. This further suggests that the shape transition was already occurring prior to the addition of ionomycin. Figure 13 illustrates the effectiveness of MBCD in removing cellular cholesterol by comparing the amount of cholesterol in the supernatant and the cell pellet after the 30 minute incubation. Treatment with 1.0 mM MBCD removed 69% ± 9% of cellular cholesterol compared to 6% ± 5% for cells treated without MBCD. 13 FIGURES AND FIGURE LEGENDS 600000 45C 500000 400000 300000 25C 200000 100000 0 600 800 1000 1200 Time (s) FIGURE 1. Light scattering by erythrocytes treated with calcium and ionomycin at 25 °C and 45 °C. Samples were treated with calcium as described in Materials and Methods. Ionomycin was added at the arrow. Fluorescence intensity is meaured as counts per second (“cps”). 14 calcium only calcium + ionomycin 25 °C ~100% discocytes ~50% discocytes, 50% early echinocytes earlyspherocytes 45 °C ~100% discocytes ~25% echinocytes, 75% spherocytes FIGURE 2. Photomicrographs of erythrocytes treated with calcium and ionomycin at 25 °C and 45 °C. Images are portions of field, while notes are approximations determined by visual inspection of entire field. 15 0.3 0.2 0.1 0.0 25C 37C 45C Temperature (°C) FIGURE 3. Effects of temperature on transport of internal erythrocyte calcium concentration by ionophore. Data were obtained using indo-1 to indicate change in internal calcium concentration (see Materials and Methods). Raw intensities were normalized using the indo-1 excitation/emission ratio to show net relative changes in calcium concentration. The treatment groups are not significantly different by analysis of variance (p = 0.71, n = 2-3). Data are expressed as mean ± SEM. 16 60000 60000 Manganese Cobalt 50000 50000 45C 40000 45C 40000 30000 20000 200 60000 30000 25C 20000 400 600 800 300000 Nickel 250000 50000 400 600 800 1000 Magnesium 200000 45C 40000 150000 100000 30000 20000 200 25C 10000 200 1000 600 800 25C 50000 25C 400 45C different samples 25C 0 1000 600 800 1000 1200 time (s) FIGURE 4. Light scattering by erythrocytes treated with divalent cations and ionomycin at 25 °C and 45 °C. Samples were treated with divalent cations as described in Materials and Methods. Ionomycin was added at the arrow. 17 45 °C ~20% discocyte, 80% early echinocyte or beyond Mixed group, abundant spherocytes ~100% discocytes ~50% discocyte, 50% echinocyte ~50% discocyte, 50% early echinocyte ~50% discocyte, 50% echinocyte Magnesium Cobalt Nickel Manganese 25 °C ~50% discocyte, 50% echinocyte or beyond (strange shape, may be artifact) ~100% discocytes FIGURE 5. Photomicrographs of erythrocytes treated with various divalent cations and ionomycin at 25 °C and 45 °C. Images are portions of field, while notes are approximations determined by visual inspection of entire field. 18 1.5 A 1.0 0.5 0.0 -0.5 Ca Mn Co Ni 1.5 B 1.0 0.5 0.0 -0.5 Ca Mn Co Ni FIGURE 6. Change in intensity of scattered light after the addition of ionomycin at 25 ºC and 45 ºC for selected cations. Data (mean ± SEM) express the difference in the average intensity before the addition of ionomycin compared to that measured 600 s later (normalized to intitial average intensity). Panel A, microvesicle release at 25 ºC. Means are significantly different from each other using ANOVA (p = 0.015). The results for each group (cation) were indistinguishable from zero based upon one sample t-tests (Ca2+, p = 0.20, n = 4; Mn2+, p = 0.08, n = 5; Co2+, p = 0.07, n = 5; Ni2+, p = 0.26, n = 5). Panel B, microvesicle release at 45 ºC. Means are significantly different from each other using ANOVA (p = 0.0001). Individual differences measured with the one sample t-test show that Ca2+and Co2+ are different from 0 (p = 0.0001, n = 6; p = 0.0011, n = 5 respectively) while Mn2+ and Ni2+ are not (p = 0.35, n = 5; p = 0.10, n = 4, respectively). 19 0.00 -0.25 -0.50 -0.75 A Ca Mn Co Ni 0.00 -0.25 -0.50 -0.75 B Ca Mn Co Ni FIGURE 7. Change in noise of light scattering after the addition of ionomycin at 25 ºC and 45 ºC for selected cations. Data (mean ± SEM) express the difference in the average standard deviation (SD) before the additon of ionomycin compared to that measured 600 s later (normalized to intital average SD). Panel A, erythrocyte shape change (Ca2+, n = 4; Mn2+, n = 5; Co2+, n = 5; Ni2+, n = 5) at 25 ºC. Means are not significantly different from each other using ANOVA (p = 0.87). Only Mn2+ was significantly different from 0 based upon a one sample t-test (p = 0.02), (Ca2+, p = 0.67; Co2+, p = 0.16; Ni2+, p = 0.16). Panel B, erythrocyte shape change at 45 ºC. Means are significantly different from each other using ANOVA (p = 0.04). Individual differences measured with the one sample t-test show that all ions are different from 0 (Ca2+, p = 0.0003, n = 6; Mn2+, p = 0.0003, n = 5; Co2+, p = 0.03, n = 4; Ni2+, p = 0.01, n = 4). 20 14000 11000 A 8000 5000 2000 -1000 20 30 40 50 Temperature (°C) 1.00 0.75 B 0.50 0.25 0.00 20 30 40 50 Temperature (°C) 1.1 1.0 0.9 0.8 0.7 20 C 30 40 50 Temperature (°C) FIGURE 8. The effect of temperature on fluorescence intensity, noise and membrane order. Panel A, raw light scattering data (like those seen in Fig. 1) were analyzed using nonlinear regression. Pre-ionomycin and pre-ionomycin + 600 s standard deviations were calcuated from the residuals and averaged. The data show the difference between the two and are expressed as mean ± SEM (n = 3-15). Panel B, the same data as Panel A were analyzed in a similar method, only here showing the difference between the minimum post-ionomycin intensity and minimum + 240 s. Panel C, GP was calculated as described in Materials and Methods and normalized for the value at 25 °C. Error bars represent mean ± SEM (n = 9 for each temperature). Lines drawn in all panels have no theoretical significance. 21 1.1 1.1 A 1.0 0.9 0.9 0.8 0.8 0.7 B 1.0 0.7 0 mM MBCD 0.6 0.6 1.1 1.1 C 1.0 0.9 0.1 mM MBCD D 1.0 0.9 0.8 0.7 0.8 0.6 0.5 0.4 0.7 0.3mM MBCD 20 25 30 35 40 45 0.6 50 1.0 mM MBCD 20 25 30 35 40 45 50 Temperature (°C) 1.1 E 1.0 0.9 O MBCD 0.1 MBCD 0.3 MBCD 1.0 MBCD 0.8 0.7 0.6 0.5 0.4 20 Summary 25 30 35 40 45 50 Temperature (°C) FIGURE 9. Effect of cholesterol depletion on laurdan GP. Erythrocyte samples were prepared with MBCD to remove cholesterol as described in Materials and Methods. GP was calculated as described in Materials and Methods and normalized for the value at 25 °C. Panel A, n = 9; Panel B, n = 10; Panel C, n = 10; Panel D, n = 9 for each temperature. Data are expressed as mean ± SEM. Panel E illustrates the same data expressed in the individual panels but without error bars and curves were generated by nonlinear regression using an arbitrary function. 22 0.6 0.4 0.2 0.0 FIGURE 10. Relationship between laurdan GP at initial temperature of 25 °C and MBCD concentration. GP values shown are the original un-normalized data from the 25 °C data point for each group in Fig. 9. Data were compared using ANOVA. The initial GP values for the treated cells are not significantly different from each other (p = .36, n = 5-8). Data are expressed as mean ± SEM. 23 1.25 0.1 mM MBCD 1.00 0.75 0.50 0.25 0.00 -0.25 -0.50 -0.75 20 25 30 35 40 45 50 Temperature (°C) 1.25 0.3 mM MBCD 1.00 0.75 0.50 0.25 0.00 -0.25 -0.50 -0.75 20 30 40 50 Temperature (°C) 1.25 1.0 mM MBCD 1.00 0.75 0.50 0.25 0.00 -0.25 -0.50 -0.75 20 30 40 50 Temperature (°C) FIGURE 11. Relationship between temperature and light scattering displacement using cholesterol-depleted erythrocytes. Raw light scattering data (like those seen in Fig. 1) were analyzed using nonlinear regression and the average intensity pre-ionomycin and pre-ionomycin + 600 s were calculated. These data show the difference between the two and are expressed as mean ± SEM (n = 3-15). Data are normalized for the yintercept. Control data (no MBCD) are shown as black boxes in each panel. 24 calcium only calcium + ionomycin no drug ~100% discocytes ~5% discocytes, 95% echinocytes or beyond ~5% echinocytes, 95% spherocytes ~100% spherocytes 1.0 mM MBCD FIGURE 12. Photomicrographs of erythrocytes treated with and without MBCD in the presence of calcium ± ionomycin at 37 °C. 25 A 100 B 75 50 25 0 0.00 0.25 0.50 0.75 1.00 [MBCD] (mM) FIGURE 13. Cholesterol content of MBCD treated erythrocytes. Cells and supernatant were assayed to measure cholesterol content using cholesterol oxidase/Amplex Red assay as described in methods. Panel A shows a theoretical graph of relative MBCD and cholesterol concentrations assuming the MBCD was able to remove all the cellular cholesterol. Panel B shows cholesterol concentrations in cell pellet and supernatant treated with various concentrations of MBCD (no MBCD, 0.1 mM, 0.3 mM and 1.0 mM), n = 4 for all conditions. Data are expressed as mean ± SEM. 26 DISCUSSION Our purpose in this work was to characterize the shape transition and microvesiculation of ionophore-treated erythrocytes in terms of microscopic membrane physical properties such as lipid order. We reasoned that manipulation of these physical properties by altering cholesterol content and the experimental temperature would affect these processes in ways that can be interpreted using known lipid phase behavior obtained from artificial bilayers (Harris et al., 2002). Our observations led us to the following conclusions: 1) the modest temperature dependence of membrane structure observed with laurdan is shifted to lower temperatures and becomes more cooperative upon removal of membrane cholesterol, 2) the calcium-induced shape change observed in erythrocytes requires a decrease in membrane order, 3) the influence of membrane order is not limited to shape transitions induced only by calcium, and 4) decreased order is also a permissive factor for microvesicle shedding. 1) Erythrocyte membranes display significant temperature dependence of several membrane properties including membrane capacitance, K+-permeability inducement via amphotericin-B derivatives, deformability, transmembrane potential, membrane order and susceptibility to PLA2 (Bao, 1992; Best et al., 2002; Galla, 1980; Glaser, 1992; Wietserbin, 1990; Williamson et al., 1975). Figure 9 shows a clear temperature dependence of laurdan GP in human erythrocytes. As the temperature increases, the GP decreases reflecting a more disordered membrane. This data are consistent with reports from artificial membranes (Sheffield et al., 1995) as well as erythrocytes (Best et al., 2002; Moore et al., 1999; Wolkers et al., 2002). Furthermore, the temperature dependence of control cells (no MBCD) demonstrates a mildly cooperative phase 27 transition between 35 to 40 °C. Using FTIR to measure fluidity, Wolkers et al. also noted low-cooperativity phase transitions at 14 °C and 34 °C in non-depleted erythrocytes (2002), while Moore et al. saw only a monotonic increase in temperature-dependent fluidity (1999). The cells treated with 1.0 mM MBCD (Figure 9) saw a more drastic transition toward decreased order between 25 to 30 °C. That the removal of cholesterol increases the cooperativity of the transition is not surprising. One of the roles of cholesterol in the membrane is to function as a fluidity buffer, fluidizing the bilayer in the gel state and adding stability in the fluid phase by reducing lateral mobility of phospholipids. These data agree with studies performed in artificial membranes (Harris et al., 2002; Silvius, 1992; 1996). Harris et al. demonstrate how incorporation of exogenous cholesterol into artificial membranes attenuates the temperature dependent decrease in membrane order above the the phase transition of approximately 40 °C (2002). The fluidity buffer concept has been further corroborated in biological systems. FTIR studies in cholesterol-depleted membranes show evidence that cholesterol modulates membrane fluidity by decreasing the lipid order at low temperatures and increasing the lipid order at high temperatures (Moore et al., 1999; Wolkers et al., 2002). Our data support the concept that at higher temperatures cholesterol rigidifies the membrane. However, at lower temperatures our temperature range does not discriminate; or in other words, the variation in laurdan GP between donors is as great or greater than the variation between MBCD treatments (Figure 10). 2) While it is well known that increased intracellular calcium causes a reversible shape transition in erythocytes from discocyte to echinocyte or crenated sphere (Smith et 28 al., 2002; Smith et al., 1981; Vest et al., 2004), the mechanisms responsible for the change are not well understood. We conclude that one of the requirements for the calcium-induced shape transition is a decrease in membrane order. The shape transition is clearly temperature dependent in both light scattering data and photomicrographs (Figures 1, 2, 7, & 8) . The results at higher temperatures are reminiscent of similar effects observed previously at 37 °C (Vest et al., 2004). An alternative explanation for the data in the figures cited above, that the temperature dependence of the shape transition is due to the ability of ionomycin to transport calcium, is refuted in Figure 3. While the kinetics of the reaction may lag somewhat at lower temperatures, when allowed to equilibrate as described in Materials and Methods, the overall calcium influx is the same. Therefore, any explanation of observed changes due to efficacy of ionomycin transport may be abandoned. We reasoned that if membrane order was necessary for the shape transition to occur, removing cholesterol from the erythrocytes would affect the shape transition in a manner similar to temperature. However, considering the amount of cholesterol we removed in treatment with MBCD we cannot rule out the possibility that the effects of cholesterol depletion may be due partly or completely to changes in membrane surface area (Shattil, 1975). 3) By utilizing other divalent cations in our experiments, we were able to distinguish between calcium-specific effects and general effects of cations on the shape transition. While not all cations caused a change in shape, manganese, cobalt, and nickel were able to cause a shape change that exhibited a similar temperature dependence to that induced by calcium (Figures 4 & 5). Therefore, we build on the observations that Vest et 29 al. (2004) made at 37 ºC by concluding that the temperature dependence that permits the shape change is not calcium-specific. Interestingly, Vest et al. (2004) also reported that the presence of cobalt, nickel or manganese elicited the highest responses to ionomycininduced membrane ordering when compared to the alkaline earth metals. There was a high correlation seen between maximal response and ionic radius or electronegativity. Thus, the unique characteristics of each ion could contribute to their ability to bind to the membrane and cause the variations in effect that we observe with the selected ions. The effect of various ions on the shape transition raises interesting questions. On the one hand, we show that a shape transition is most likely to occur when the membrane order is decreased. On the other hand, all of the ions that stimulate the transition in shape also cause an increase in membrane order (Vest et al., 2004). So how does a decrease in membrane order permit the shape transition? There are three possible explanations. 1) The shape transition may require the actual conversion of a disordered to an ordered membrane in order to change. 2) We may assume that the transition itself causes major disruptions in the protein scaffolding network and the membrane enough to cause ordering of the membrane through altered lipid-protein interactions. 3) The ordering of the membrane may be a parallel event that is unrelated to the shape transition. While our data can not distinguish among these three possibilities, limited evidence suggests that that the first explanation is preferred. An interesting concept introduced by Glaser and Leitmannova in 1975 called the “rigidity-pattern hypothesis” proposes a model of shape transformation based upon lateral inhomogeneities in the erythrocyte membrane. They suggest that shape dynamics of erythrocytes must be considered in the context of occurrence of microphases and local lipid domains (see 30 Literature Review for more detail). Furthermore, studies with two-photon microscopy that looked at the spatial distribution of order across the membrane demonstrate that the effect of calcium on membrane order is markedly different from ordering caused by decreasing temperature. Lowering the temperature increases order in a general, homogeneous fashion while increased internal calcium (or other ions) expanded regions or more ordered domains. This suggests the possiblity, since ionomycin causes ordering heterogenously on top of a fluid background, that the ordering caused by the introduction of the cations may directly influence the shape transition. 4) The connection of membrane physical properties with microvesicle release is not well-established. Our data illustrate that calcium-induced microvesicle release shows a clear temperature dependence (Figures 1, 6, & 8B). In addition, removal of membrane cholesterol created an environment more willing to release microvesicles (Figure 11). These observations strongly suggest that decreased membrane order is an important component of the mechanism that regulates microvesicle shedding. To address the possibility of a non-specific artifact of MBCD, we included a control experiment in which we pre-loaded the MBCD molecules with erythrocyte cholesterol, and then assessed its effect on calcium-induced microvesicle release (data not shown). The pre-loaded MBCD treatment showed an significant attenuation of microvesicle shedding when compared to 1.0 mM MBCD treated cells, illustrating that MBCD alone is not responsible for the shedding. Care should be noted that cells treated with 1.0 mM MBCD are considered fragile and have, at time, undergone hemolysis at high temperatures. 31 An alternate interpretation of the data that reflect temperature dependence of microvesicle release and shape change is that changes in activation energy of enzymatically driven processes or other protein lipid interactions may play a role. However, the fact that MBCD treatment yielded similar results as temperature manipulation in the case of microvesicle release suggests that changes in membrane properties are a more likely explanation than activation energies, although we cannot rule out that some of the temperature dependence may be due to enzymatic function. Clearly, proteins have been implicated in the mechanisms that regulate microvesicle release. Interactions between calcium and specific proteins such as calpain, the Gardos channel and scramblase are well documented as being linked to the phenomenon (Allan and Thomas, 1981; Smith et al., 2001). However, the data presented herein show that the physical properties of membrane lipids are also involved. For example, Best et al. (2002) notes that the “flip-flop” which causes the asymmetrical distribution of lipids (involving scramblase) is not temperature sensitive. This reinforces the idea that the effects we are observing are also membrane-dependent, rather than exclusively protein-mediated. In contrast to the results regarding the shape transition, we show in Figure 6 that only calcium was able to produce a robust microvesicle response at 45 ºC (manganese did cause an effect, however the reaction was greatly reduced compared to calcium). This is in agreement with the observations made by Vest et al., 2004. While the shape transition from discocyte to echinocyte is often accompanied by the release of microvesicles, the ion specificity of the response suggests that the mechanisms of the two events are different. 32 How would the order of the lipid bilayer affect the ability of the membrane to produce vesicles? Membrane domains of varying fluidity, i.e. lipid rafts, may provide insight to the relationship. A study by Salzer et al. concludes that lipid rafts are involved in the vesiculation process because the calcium-induced microvesicles contain high amounts of lipids and proteins from rafts, specifically cholesterol, gangliosides, somatin, flotillin, and AchE. They suggest that elevated calcium induces segregation of different rafts selectively and that membrane fusion proteins such as synexin may also play a role (2003). This idea is further supported by two-photon data that suggest that the plasma membranes of ionophore-treated erythrocytes also exhibit an increase in liquid-ordered domains (Vest et al., 2006). Whether MBCD removes cholesterol selectively within domains or generally throughout the cell is not well established (Hoessli et al., 1998; Steck et al., 2002; Rothblat et al., 1999). The data presented in this paper offer new insight as to the reason that the cholesterol:phospholipid ratio (normally approximately 0.8 mol/mol of phospholipid, (Lange et al., 1980)) in erythrocyte membranes is tightly regulated. When the membrane cholesterol pool is depleted, cells undergo a change in the average order of the membrane that makes them susceptible to vesiculation and possibly a shape change. At physiological temperature, the cholesterol:phospholipid ratio provides just enough rigidity to give the cell strength and stability in its discoid shape, yet allows the cell to be fluid enough to be flexible while moving through the microcirculation. Moreover, by illustrating the requirement of a disordered membrane for the cell to shed microvesicles, and changes in shape, we provide compelling evidence that membrane order is a critical 33 component of the mechanisms that regulate both of these processes in human erythrocytes. 34 LITERATURE REVIEW Regulation of Erythrocyte Shape “…a classic problem in cell biology” The normal resting shape of the erythocyte is a flattened, biconcave disk called a discocyte (or normocyte) 8 µm in diameter and possesses a unique ability to deform enough to pass through capillaries as small as 2 µm wide. In vitro, various treatments are known to change the normal resting shape reversibly into other shapes such as echinocytes (spiculated cells), stomatocytes (cup-shaped cells) and spherocytes (small, round cells). Standardized classification of the morphological details of these shapes and their various stages was established in work by M. Bessis after the introduction of the scanning electron microscope (1972). For example, a type II echinocyte maintains a disk-like appearance with cellular projections that vary in length while the type III looks more like a spherical erythrocyte with numerous spicules. While the morphological details have been well characterized, to this day the mechanisms responsible for the transformation of discocyte to echinocyte, or discocyte to stomatocyte are less understood. This remains a “classic problem in cell biology” (Mukhopadhyay et al., 2002) and is the first of eight questions posed by Joseph Hoffman for red blood cell physiologists to ponder in this millenium (2001). Implications from clinical studies Hereditary disorders of the erythrocyte membrane can offer important clues to the mechanisms of shape regulation. Hereditary spherocytosis, hereditary elliptocytosis, hereditary pyropoikilocytosis, and hereditary stomatocytosis comprise an important 35 group of hemolytic anemias that can be diagnosed by looking at the various shapes present in blood smears. Some disorders are linked to deficiencies in or inactive cytoskeletal proteins such as hereditary spherocytosis and elliptocytosis (Liu et al., 1990; Mohandas et al., 1992). Sickle-cell anemia (HbS) is caused by the auto-oxidation of membrane proteins such as band 3, which disrupts the assembly of the cytoskeleton leading to sickling (Platt and Falcone, 1995). Other types of anemias may have a variety of causes that are less understood or unknown, such as the molecular basis for hereditary stomatocytosis. For more information regarding these hemolytic anemias, refer to a recent review on the subject (Gallagher, 2005). More generally, pathologies such as vascular disease, diabetes (type II), childhood leukemia, and liver disease have been shown to alter the morphology of red blood cells (Perotta et al., 2001; Turchetti et al., 1997). Administration of certain drugs, such as cyclosporine or lidocaine, can cause morphological changes (Nishiguchi et al., 1989; Ohsako, et al. 1998). Erythrocytes from patients with chronic obstructive pulmonary disease, Down syndrome, and those who have suffered an acute myocardial infarction all show evidence of decreased fluidity of red blood cell membranes (Przybylska et al., 2000; Saldhana et al., 1999; Santini et al., 1997). While review of these pathologies is helpful in determining various protein and membrane components that may be responsible for altering cell shape and membrane properties, it is important to note that the mechanisms may be different than the experimentally-induced, reversible changes in shape on which this report focuses. Perturbations that can cause shape changes Normal, healthy erythrocytes can undergo shape transformations in vitro to 36 echinocytes or stomatocytes (or the final stage for both, spherocyte) upon addition or variation in: electrolyte concentrations (Deutike, 1968; Herrman et al., 1985; Rasia, 1998) including calcium (which will be addressed in more detail at the end of this section), pH (Gedde et al.,1997; Libera et al., 1997; Rasia, 1998), ATP concentration (Gov and Safran, 2005; Nakao et al., 1960, Weed et al.,1969), amphiphilic compounds such as lipids, fatty acids, various drugs, etc. (Chen et al., 2003; Deutike, 1968; Iglic et al., 1998; Isomaa et al., 1997; Sheetz and Singer 1974,) and the rearrangement of asymmetrically organized membrane lipids (reviewed by Zachowski, 1993). A relationship exists between erythrocyte shape and the transmembrane electric potential; consequently, the effect of pH and and other compounds can also be attributed to the transmembrane potential (Bifano et al., 1984; Glaser, 1992, 1998). See citations for an interesting debate on this topic. The effect of elevated intracellular calcium on the shape of erythrocytes It is well known that increased intracellular calcium causes a reversible shape transition in erythrocytes from discocyte to echinocyte or crenated sphere (Smith et al., 2001; Smith et al., 1981;Vest et al., 2004). In normal erythrocytes, the concentration of calcium is kept at levels below 1.0 mM (via a calcium-ATPase pump and calmodulin), however these levels can be increased due to ATP depletion (inhibition of outward calcium pumping) or introduction of calcium via ionophore (Wiley and McCullough, 1982). Elevated intracellular calcium with ionophore causes rapid echinocytosis, decreased potassium levels, dehydration and volume decrease (Dreher et al., 1980; Gedde, 1997; Kirkpatrick et al., 1975). This is commonly known as the Gardos effect. 37 Chukhlovin carefully reviewed the connection between echinocytosis and apoptosis, saying “the transition of the normal discocyte to echinocyte is often induced by the same factors that cause apoptosis of blood cells (i.e. ionizing radiation and other ROIinducing agents, exogenous oxidants, in vitro aging conditions, cytosolic calcium increase, etc. (1996).” He also cited three mechanisms that may explain the calciuminduced changes in shape. Briefly, 1) altered transverse asymmetry of membrane phospholipids caused by the inhibition of aminophospholipid translocase, 2) activation of PKC, disruption of the bonds between proteins 4.1 and band 3 and 3) decrease in phosphotidylinositol bi and monophosphates which also cause alterations in membrane cytoskeleton contacts (1996). These proposals all implicate protein-dependent regulation of cell shape. Moreover, it is known that the membrane structure and stability of the cell is especially sensitive to the interaction of calcium and proteins. In the presence of calcium levels higher than 0.1 mM, the calcium-calmodulin complex reduces the affinity of protein 4.1 to the spectrin-actin region of the cytoskeleton, weakening the system (Takakuwa and Mohandas, 1998). However, similar concentrations of calcium also reduce the affinity of protein 4.1 to the cytoplasmic domain of band 3, and increases the binding of band 3 to ankyrin (Takakuwa, 2000). Liu et al. suggest the opposing effects of these events can regulate membrane structure and stability through an unknown mechanism (2003). Furthermore, using atomic force microscopy, Liu et al. showed that extra calcium binding on the cytoplasmic surface of the membrane increases cytoskeleton rigidity and prevented spectrin aggregation (2005). 38 Alternatively, Sikorski et al. emphasizes that protein 4.1 and spectrin are capable of binding to the lipid portion of the membranes, not only to other proteins (2000). The interaction of protein 4.1 with PS-containing membranes was inhibited by calcium (Sato and Ohnishi, 1983). Sikorski et al. postulate whether lipid binding can substitute for the regulatory processes involved with protein 4.1, i.e. phosphorylation and calciumcalmodulin binding (2000). Other studies with artificial membranes (Binder et al., 2001; Binder and Zschornig, 2002; Hauser, 1991) and erythrocytes (Vest et al., 2004) claim that divalent cations can alter cell membrane physical properties by interacting directly with the bilayer, instead of through protein-mediated regulation. Bilayer Couple Theory In 1974, Sheetz and Singer proposed the bilayer couple theory that explains shape change based upon the relative surface area of the outer membrane leaflet compared to the inner leaflet, and that the bending elasticity of the membrane is caused by the area elasticity of the two lipid layers and their fixed distance. For example, a positivelycharged amphiphile added to the membrane will penetrate and remain in the relatively negative inner leaflet. Consequently, the surface area of the inner layer expands slightly while the outer layer remains the same, causing the membrane to form cup-shaped cavities (stomatocytosis) to accommodate the extra area. Alternatively, a factor which leads to the expansion of the outer leaflet forms convex structures like the spicules of the echinocyte (also called crenate cells). Although many studies support the bilayer couple theory (Chen et al., 2003; Farge and Devaux, 1992; Lange and Steck, 1982; Sheetz and Singer, 1974; Tachev et al., 2004), many phenomena argue against the bilayer theory being the only valid hypothesis explaining the change in shape. 39 Protein Scaffolding The protein scaffolding theory maintains that is it the organization of the intrinsic and cytoskeletal proteins that largely determine cell shape, and the asymmetrical distribution of the bilayer may be a result, but not a cause, of a shape transition (see review by Nakao, 2002). For example, the amphipathic molecule 2,4-dinotrophenol (DNP); a cup-former, and chlorpromazine; a crenator, are still able to induce shape changes in ghosts that demonstrate a large hole (hence, a discontinuous membrane) in the lipid layer at 4 °C (Lieber, 1982). Furthermore, after the cytoskeleton was destroyed using proteinases, the amphipaths were unable to cause morphological changes (Jinbu, 1982). Anderson and Lovrien fixed the cytoskeletal proteins of intact cells with wheat germ agglutination antibodies, and found that the cell shape remained unchanged upon addition of ionophore and calcium (1981). The bilayer hypothesis and studies that support protein regulation of shape are not mutually exclusive, and a complete description of the mechanism most likely requires elements of both ideas. As mentioned previously, Sikorski et al. reviewed the interaction of membrane skeletal proteins with membrane lipid domain and pointed out a variety of cases where structural proteins such as spectrin and protein 4.1 can bind directly to the lipid layer instead of other membrane proteins to provide a “scaffolding” (2000). These lipid-protein interactions may prove to be a connection between the two theories. Band 3 conformation hypothesis Band 3 (Anion exchanger 1, AE1) was one of the first erythrocyte membrane proteins to be characterized, mainly because of its abundance (1.2 x 106 copies per cell, representing 10% of the surface area and 25% of total membrane protein) (Fairbanks et 40 al., 1971). It has been the subject of many reviews in its role in maintaining cell homeostasis and regulating cell shape (Inaba et al., 1996; Jay and Cantley, 1986; Tanner 1993). However, it was Wong who proposed a specific mechanism of eythrocyte shape control in which Band 3 plays a central role and claims that it explains several observations related to human erythrocyte shape (Wong, 2006 – see article for history of other Wong papers). Briefly, transport of an anion changes the conformation of the transmembrane domain of Band 3, which in turn changes the conformation of the cytoplasmic domain, as both are flexibly linked. Decrease and increase of the outward/inward band 3 ratio folds and unfolds spectrin. The conformational change in spectrin contracts and relaxes the cytoskeleton to promote echinocytosis and stomatocytosis, respectively. Alternatively, Gimsa and Reid (1995) proposed the Band 3 conformation-controlled bilayer couple hypothesis, which maintains that the change of the ratio of inward and outward binding sites in turn significantly alters the membrane monolayer area ratio, the external orientation increasing the area of the outer leaflet. Rigidity-pattern hypothesis Glaser and Leitmannova (1975) proposed a model of shape transformation based upon lateral inhomogeneities in the erythrocyte membrane called the rigidity-pattern hypothesis. It considers a changing pattern of membrane areas with different bending properties. The size of the areas may be governed by the metabolic state of the cell, and the location by the bending of the membrane. For example, rigid areas may be extruded from strongly bent regions into flat areas of the membrane. Glaser further postulates that it is likely that membrane composition in strongly bent regions differs from that of other 41 areas (1992). For support, Glaser cites Bessis and Prenant (1972) for establishing that a membrane “memory” exists: spicules from echinocytes occur in the same places after reversing and restarting the process. Thus, the shape dynamics of erythrocytes must be considered in the context of the occurrence of microphases and local lipid domains. Cell volume can change shape Hereditary stomatocytosis is a group of disorders associated with abnormalities in cation permeability that lead to changes in cell volume, whether increased (hydrocytosis) or decreased (xerocytosis). Hydrocytosis is characterized by significant stomatocytosis, severe hemolysis, and macrocytosis, along with elevated cytosolic sodium concentration, reduced potassium, and increased total cation content…predictably elevating cell water content. Interestingly, xerocytosis is characterized by echinocytes and variable numbers of stomatocytes and is linked to hyperkalemia (see review by Gallagher, 2005). Relationship between domains, order and shape A few papers have given some insight to the general principles associated with how physical properties of the bilayer may be involved in the erythrocyte shape transition. Typical stomatocyte ⇔ discocyte ⇔ echinocyte shape changes based on the bilayer couple hypothesis have been used to study the transmembrane motion of lipids, as pointed out by Zachowski in a comprehensive review of the subject (1993). He also notes that the two leaflets of the bilayer have different physical properties due to the degree of saturation in the fatty acid chains of resident phospholipids, i.e. lower local microviscosity and faster lateral diffusion in the inner leaflet. Fisher (1993) claims that monolayer bending must be taken into consideration to accurately describe shape changes. 42 A possible connection between order, shape, and membrane proteins exists due to the fact that spectrin can partially penetrate the lipid bilayer. Data show that the removal of spectrin induced an increase in the spin-labeled order parameter and a decrease when it was reassociated (Sikorski et al., 1987). Similar results were achieved when the fluorescent probe, diphenylhexatriene, was used to measure fluidity (Michalak et al., 1993). In an effort to understand the existence of lipid domains in the erythrocyte membrane, Moore et al. published a series of papers based upon a novel FTIR method to study the conformational order and likelihood of membrane domain formation of specific phospholipids (1996, 1997, 1999). They used acyl chain perdeuterated lipid species that acted as “reporter molecules,” providing structural, phase transition, and miscibility info similar to their proteated counterparts based upon a well-established correlation between the methylene stretching frequencies and acyl chain conformational order. Briefly, they concluded that 1) echinocytic erythrocytes have domains of PC and PE in the outer leaflet of the bilayer. The phase transitions were broadened in erythrocytes compared to pure lipids, indicating a relatively small domain size or mixing of other components into the domain. 2) The order of lipids that commonly reside in the inner leaflet (PE and PS) is altered when they are forced to reside in the outer layer. PE appears to be a mostly pure lipid domain (cooperative transition) and PS shows no cooperative change but has higher conformational order than when it is located in the inner leaflet. 3) The observed phase behavior of incorporated species appears to be a strong function of cell morphology. When erythrocytes were incubated with 1:1 mixtures of PS-d54/PC or PS/PC-d54 (d54 indicating perdeuteration, or the reporter lipid), the lipids partioned into their 43 expected monolayers while maintaining the discocytic shape of the cell. In these cases, no phase transitions were observed and order was measured as an intermediate between common gel or liquid crystal values. Therefore, the existence of domains as suggested by the behavior of incorporated lipids as described in 1 and 2 is dependent on echinocytic morphology and further speculated to be located in the protrusions of the spicules. Influence of temperature on shape change Erythrocytes observed at high temperatures (50 to 55 °C) turn to spherocytes, and exhibit budding and fragmentation that has been linked to denaturation of the cytoskeletal protein, spectrin (reviewed by Williamson et al., 1975). Alternatively, cells stored at low temperatures develop echinocytosis over time. This has been linked to metabolic changes due to storage, not temperature per se (Nakao et al., 1960). Regulation of Erythrocyte Vesiculation Physiological Importance of Microvesicles Virtually all cells shed microvesicles (MVs), however erythrocytes have proven a good model to study the phenomenon because of their simplicity. Microvesiculation is the loss of membrane from the tips of the spicules of echinocytes and occurs in vivo as well as during storage (Laczko et al., 1985). In vivo, MVs are removed from circulation by the reticuloendothelial system. MVs shed by platelets have clinical importance because of their ability to promote coagulation and platelet adhesion to the subendothelium (see review by Heemskerk et al, 2002). In erythrocytes, the release of membrane probably alleviates some of the osmotic effects due to calcium-stimulated potassium efflux through the Gardos channel. It has also been proposed that the vesicles 44 provide a defense mechansim for erythrocytes from attack by complement (Iida et al., 1991). Further suggestion of a protective role comes from a study in which poly (ethylene-glycol) cholesterol induces echinocytosis and is located in the tips of the spicules, as though the cell is trying to sequester the exogenous compound (Baba et al., 2004). Along with membrane blebbing and PS exposure, MV release is an external indicator of apoptosis (Chukhlovin, 1993). Calcium-induced microvesiculation Like the shape transition, the MVs that are released from the spicules of the echinocyte have been well-characterized by their size and composition (Salzer et al., 2001; 2002). Microvesicles can be produced by elevated calcium concentrations, depleted ATP levels, or the addition of various amphipathic molecules (Allan and Thomas, 1981; Hagelberg and Allan, 1990; Kralj-Iglic et al., 2000; Smith et al., 2001; Vest et al., 2006). Between 1975 and 1980, a series of papers published by D. Allan and colleagues were the first to study MV release in detail, focusing on the effect of elevated calcium introduced by ionophore. They characterized the composition of vesicles as depleted in PC, and cytoskeletal proteins spectrin, actin, and glycophorin while retaining band 3 and acetylcholinesterase (see review by Greenwalt, 2005). High calcium concentrations lead to alterations in the membrane protein patterns, namely protein aggregation and cytoskeletal rearrangement due to proteolysis of protein 4.1 by calpain (Croall et al., 1986). Calcium also causes the breakdown of phosphatidylinositol 4-phosphate and phosphatidylinositol 4,5-bisphosphate with a simultaneous increase in 1,2-diacylglycerol and phosphatidic acid (Allan and Michell, 1975). Calcium activates scramblase and inhibits aminophospholipid translocase which 45 results in a distortion of phospholipid organization, especially PS exposure on the extracellular surface, over the two leaflets of the bilayer (Comfurious et al, 1990). Moreover, calcium stimulates the Gardos channel and the concomitant potassium efflux exerts osmotic effects which may result in loss of cell water and cell shrinkage due to blebbing (Maher and Kuchel, 2003). Recently, the GTPase Rap2 was shown to be selectively enriched in microvesicles stimulated by calcium influx (Greco et al., 2006). Of all the morphological or biochemical changes that calcium causes, it appears that the activity of calpain, scramblase, and potassium efflux are required for cells to release vesicles (Smith et al., 2001). Bilayer and microvesicle release Beyond the proteins that have been implicated as responsible for microvesicle release, there exists evidence that the influence of the bilayer also plays a role. One of which is the ability of amphipathic molecules to cause MV release (as stated above). In addition, Salzer et al. concludes that lipid rafts are involved in the vesiculation process by showing calcium-induced vesicles that are high in lipids and proteins from rafts, specifically cholesterol and gangliosides, somatin, flotillin, AchE, etc. They suggest that elevated calcium induces segregation of different rafts selectively and that membrane fusion proteins such as synexin may also play a role (2003). Role of cholesterol in the erythrocyte membrane Cholesterol and membrane microscopic physical properties Artificial membranes consisting of one species of phospholipid are characterized by a phase transition temperature (Tm) from the gel to liquid-crystalline state. In contrast, 46 biological membranes exhibit a more complex thermal phase behavior because of the mixture of phospholipids, sterols, and proteins with preferential interactions between them. For example, one of the roles of cholesterol in the membrane is a fluidity buffer, fluidizing the bilayer in the gel state and adding stability in the fluid phase by reducing lateral mobility in between phospholipids (Wolkers et al., 2002). This effect can be seen in a study of DPPC vesicles performed recently in our laboratory that show how incorporation of exogenous cholesterol attenuates the temperature dependent decrease in membrane order in a dose-dependent manner above the the phase transition of approximately 40 °C (Harris et al., 2002). This data is in agreement with other studies in artificial membranes (Silvius, 1992; Silvius et al., 1996). The fluidity buffer concept has been further corroborated in biological systems. In 2002, Wolkers et al. performed FTIR studies that show evidence that cholesterol modulates the membrane fluidity by decreasing the lipid order at low temperatures and by increasing the lipid order at high temperatures. His group also noted distinct phase transition temperatures of 14 °C and 34 °C in erythrocytes, which is surprising given that the normally high concentrations of cholesterol in the membrane usually mask distinct phase transitions (Moore et al. saw only monotonic increases in fluidity in erythrocytes (1999)). Spatial removal of cholesterol Whether cholesterol removal via MBCD occurs generally or selectively from lateral domains or leaflets is not well understood. Cholesterol interacts preferentially with sphingomyelin, creating a fluidity intermediate called the liquid ordered phase in microdomains commonly known as lipid rafts (Ipsen, 1987). Rothblat et. al. observed 47 biexponential kinetics of cholesterol efflux, a fast pool (t1/2= 19 to 23 seconds) and a slow pool (t1/2= 15 to 30 minutes) using both model membranes and a variety of cell lines (not erythrocytes) (1999). Ilangumaran and Hoessli observered three different kinetic pools for cholesterol in lymphocyte membranes that received the following assignments: the fluid phase (fastest), the liquid ordered phase of the microdomains (intermediate), and a transition zone (slowest) in between that is postulated to exist to provide “a smooth transition in the energy states between the two phases” (1998). This indicates that MBCD selectively removes cholesterol from outside the sphingolipid microdomains. In contrast, Steck et. al. (2002) showed in erythrocytes that all cholesterol efflux followed first order kinetics with a t1/2 < 1 second. While their data do not show evidence of different kinetic pools, they do find that the transbilayer diffusion of cholesterol is fast compared to the kinetics of extraction. They interpret this result to indicate that MBCD removes cholesterol from both the inner and outer leaflet of the bilayer. Cholesterol in lipid rafts Much of the research regarding lipid rafts has been in artificial membranes, however biological rafts have been implicated in a number of important cellular signaling events, including apoptosis (Scheel-Toellner et al., 2002). Leidy et al. (2002) reviewed the relationship between cholesterol and lipid raft aggregation and/or function and shares the following relevant information. Erythrocyte membranes contain a high concentration of cholesterol, hence, there is only a mildly cooperative phase transition at high temperatures because cholesterol interacts with sphingomyelin within domains but also partitions into the fluid phase. Lower concentrations of cholesterol would favor increased domain formation (as seen in platelets & other cell types). In addition, the fact 48 that exogenous cholesterol can alter the phase boundaries in artificial cells suggests that cholesterol is active at the domain boundary. There are established interactions between cholesterol content and protein function in lipid domains (Hao et al., 2001; Hoessli et al., 1998; Samuel et al., 2001; Westover et al., 2003). This must be taken into account in the discussion of the effect of cholesterol depletion on events such as shape change and MV release. However, the significance of interference from protein-based signaling pathways is limited by the use of erythrocytes as a model. 49 REFERENCES 1. Allan, D. and Michell, RH. (1979) The relationship between Ca2+-mediated polyphosphoinositide phosphodiesterase activity, 1, 2-diacylglycerol accumulation, and microvesiculation in erythrocytes, Prog. Clin. Biol. Res. 30: 523-9. 2. Allan, D. and Thomas, P. (1981). Ca2+-induced biochemical changes in human erythrocytes and their relation to microvesiculation, Biochem. J. 198(3):433-40. 3. Anderson, R.A. and Lovrien, R. 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Physiology and Developmental Biology, Brigham Young University Thesis: “The influence of membrane order on cell shape and microvesiculation in human erythrocytes” GPA: 3.8 2001 B.S. Zoology with Honors, Brigham Young University Honors Thesis: “The effect of elevated intracellular calcium on membrane fluidity in human erythrocytes : a fluorescent probe study” GPA: 3.5 Technical Experience • Graduate Research Assistant, Biophysics Lab, BYU • Graduate Research Assistant, Reproductive Endocrinology Lab, BYU • Laboratory Technician, Huntsman Cancer Institute, SLC, Utah Teaching Experience • Instructor, Introduction to the Human Body and Cell Biology, Linn-Benton Community College, Albany, Oregon, 2004-2005 • Teaching Assistant at BYU, Biopsychology, 2003; Biology 100, 2002-2003; Human Anatomy and Physiology, 1995-1996 • Spanish Teacher, Missionary Training Center, BYU, 1999-2000 Posters • • • • Biophysics Society Annual Meeting, 2006, Salt Lake City, UT Society for Neuroscience Annual Meeting, 2003, New Orleans, LA 5th International Symposium of the Role of Soy in Treating Chronic Disease, Orlando, FL Experimental Biology Annual Meeting, 2003, San Diego, CA Publications Vest RS, Gonzales LJ, Permann SA, Spencer E, Hansen LD, Judd AM, Bell, JD. 2004. Divalent cations increase lipid order in erythrocytes and susceptibility to secretory phopholipase A2. Biophysics Journal 86(4):2251-60. Smith SK, Farnbach AR, Harris, FM, Hawes AC, Jackson LR, Judd AM, Vest RS, Sanchez S, Bell JD. 2001. Mechanisms by which intracellular calcium induces susceptibility to secretory phospholipase A2 in human erythrocytes. Journal of Biological Chemistry 276 (25): 22732-41. Skills Fluent in spoken and written Spanish; public speaking; computer software (proficiency in all Microsoft Office, Corel and Adobe programs with emphasis in creating multi-media presentations); statistical analysis (Prism Graphpad, Minitab, S-Plus, SAS); laboratory skills: in-situ hybridization, immunohistochemistry, fluorescence spectroscopy and microscopy. Personal Enjoy photography, cooking, alpine skiing, triathlons, playing and coaching women’s lacrosse 59
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