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Biomedical subjects

S W Hui

Publications and source records attributed to S W Hui.

At least 55 records · Page 3Linked to original sources
PubMed1994

Electrofusion of cell-size liposomes.

Cell size liposomes of egg phosphatidylcholine (PC), trans-acylated egg phosphatidylethanolamine (PE), bovine brain phosphatidylserine (PS) and egg phosphatidylglycerol, suspended in 2.5% of polyethylene glycol (M(r) 8000), Ficoll (M(r) 400,000) or Dextran (M(r) 71,200) were aligned by dielectrophoresis and fused by applying a 1.7 kV/cm pulse of varying duration. Because the internal and external media of liposome suspension can be controlled, and the surface charge is known, the results can be described mathematically. The fusion yields (FY) at different pulse length were measured by microscopy. The FY curves were sigmoidal, with a common minimally required pulse length of 19 microseconds, and shifted to longer pulse length with increasing external media conductivity or vesicle surface charge. The types of polymer in solutions had little effect. The minimal required pulse length was interpreted to be the minimum rise time for the smallest vesicle capable of reaching the bilayer breakdown potential induced by the pulse, and the sigmoidal shape FY curves represented the cumulative vesicle size distribution curve. The shifting of FY curves upon changing media conductivity or vesicle surface charge were quantitatively accounted for by the balance of pulse-induced dipole-dipole attraction and electrostatic repulsion. Deviation from sigmoidal shape FY curves in the cases of charged liposomes was explained by increasing electrostatic repulsion due to vesicle deformation under pulse-induced dipole pressure. The data confirm the hypothesis that membrane potential breakdown is a pre-requisite or minimum requirement for electrofusion, and support our earlier proposition that pulse-induced dipole force plays an important role in the electrofusion process, and that electrostatic repulsion posts additional barrier to electrofusion.

Animals↗
PubMed1994

Dielectrophoresis of cell-size liposomes.

The dielectrophoresis (DEP) behavior of cell size liposomes were studied in the frequency range from 20 kHz to 3 MHz. Liposomes in the size of about 10 microns in diameter were made from egg phosphatidylcholine (PC), egg phosphatidylethanolamine (PE), egg phosphatidylglycerol (PG) and brain phosphatidylserine (PS). These liposomes, having an internal conductivity of 58 microS/cm, were suspended in either PEG or Ficoll solutions of conductivities 9 and 20 microS/cm, respectively. The liposomes were induced to form pearl chains in an electric field gradient in specially designed chambers with either coaxial or flat electrodes. Liposome rotation and convection (mixed positive and negative dielectrophoresis) were observed just beyond the experimental frequency range, within which positive dielectrophoresis leading to pearl chain formation were found. The threshold voltages that caused pearl chain formation were recorded within the experimental frequency range. The threshold voltages remained more or less constant within the positive DEP frequency range, and increased at both ends of the range. Charged liposomes (PS, PG) were found to have lower threshold than uncharged ones (PC, PE). Theoretical DEP spectra were calculated using a model proposed by Kaler and Jones ((1990) Biophys. J. 57, 173-182), for uncharged liposomes. The surface current effect in charged liposomes was accounted for, using an approximation proposed by Schwartz ((1962) J. Phys. Chem. 66, 2636-42). The experimental data agreed with theoretical prediction in general. The higher cutoff frequencies observed experimentally were thought to represent a slight lowering of internal conductivity due to leakage. The higher than predicted ratio between threshold voltages of charged and uncharged liposomes was interpreted to be due to the slight difference in size of these two types of liposomes. The agreement between theory and experiment showed that the available theory was adequate, and that liposomes provide a good model to study the nature of dielectrophoretic forces.

Electric Conductivity↗
PubMed1994

Molecular organization in phospholipid monolayer domains by correlative fluorescence microscopy and electron diffraction.

Lipid monolayer is a half leaflet model for lipid bilayer, which forms the basis of biological membranes. Within a certain range of surface area per molecular of phospholipid monolayers at the air-water interface, where the compressibility was nearly infinite, two phases with different molecular packings were observable by fluorescence microscopy. Mixed-phase monolayers of L-1,2-dipalmitoyl-N-monomethyl-3-phosphatidylethanolamine [DP(Me)PE] or L-1,2-dipalmitoyl-N-dimethyl-3-phosphatidyl-ethanolamine [DP(Me)2PE] were deposited on marker grids coated with Formvar films. The molecular organization in the dark and bright fluorescent areas on the grids was investigated by low dose, selected area electron diffraction. Sharp reflection arcs, at a spacing of 4.2A and arranged in a hexagon pattern, were detected from dark domains of both lipids. A diffuse reflection ring at a spacing of 4.6A was derived from the bright background areas. Diffraction patterns were obtained from neighboring areas along selected dark domains of both lipids. The orientations of diffraction patterns from areas along smooth and curving boundaries of DP(Me)2PE domains were found to turn with the boundaries. In the branching domains of DP(Me)PE, the orientations of diffraction patterns indicated that the branches were formed by twinning. Electron diffraction thus provides an unique way to sample the local molecular packing order and orientation within individual domains in phospholipid monolayers.

Microscopy, Fluorescence↗
PubMed1994

Electrically induced fusion of mammalian cells in the presence of polyethylene glycol.

Chinese Hamster Ovary (CHO) cells were fused by subjecting cell suspensions to an exponentially decaying electric pulse in the presence of polyethylene glycol (PEG), Dextran or Ficoll. PEG (MW 1,000, 3,350, 8,000, 10,000 and 18,500), Dextran (MW 71,200) and Ficoll (MW 400,000) were added to the pulsing medium. A single exponential electric pulse with peak field strength of 4 kV/cm, and a half-time of 0.72 msec was used. The combination of two techniques, PEG-induced fusion and electrofusion, resulted in highly efficient fusion of CHO cells. Fusion yields (FY) at different concentrations of these polymers were measured using phase-contrast microscopy. FY was highly dependent on the concentration of PEG in media, while the presence of Dextran and Ficoll had no influence on fusion yield. PEG with MW 8,000 was found to be the most effective in causing cell aggregation, and to give the highest FY (40%). An optimal concentration for fusion was found for PEG of each molecular weight. Diluting cells suspended in higher concentrations of PEG to these optimal concentrations after the pulse application regained the optimal FY. It was concluded that PEG-induced prepulse aggregation and moderate cell swelling immediately after the pulse were important factors in achieving high fusion yields.

Animals↗
PubMed1994

Studies of cell pellets: I. Electrical properties and porosity.

Cell pellets formed by centrifugation provided a good system to study the osmotic behavior, electroporation, and interaction between cells. Rabbit erythrocyte pellets were used in this study because they were simpler than nucleated cells to model analytically. Structurally, cell pellets possessed properties of porous solid bodies and gels. Electrically, cell pellets were shown to behave as a parallel set of resistance, Rp, and capacitance, Cp. Information on pellet structures was obtained from electric measurements. The pellet resistance reflected the intercellular conductivity (porosity and gap conductivity), whereas the pellet capacitance depended mostly on membrane capacitance. The pellet resistance was more sensitive to experimental conditions. The intercellular gap distance can be derived from pellet porosity measurements, providing the cell volume and surface area were known. Rp increased and relaxed exponentially with time when centrifugation started and stopped; the cycles were reversible. When supernatants were exchanged with solutions containing hypotonic electrolytes or macromolecules (such as PEG) after the pellets were formed, complicated responses to different colloidal osmotic effects were observed. A transient decrease followed by a large increase of Rp was observed after the application of a porating electric pulse, as expected from a momentary membrane breakdown, followed by a limited colloidal-osmotic swelling of pelleted cells. The equilibrium values of Rp, Cp, pellet porosity, and intercellular distances were measured and calculated as functions of cell number, centrifugation force, and ionic strength of the exchanged supernatant. Thus, the structure and properties of cell pellets can be completely characterized by electrical measurements.

Animals↗
PubMed1994

Studies of cell pellets: II. Osmotic properties, electroporation, and related phenomena: membrane interactions.

Using the relations between pellet structure and electric properties derived from the preceding paper, the responses of rabbit erythrocyte pellets to osmotic or colloidal-osmotic effects from exchanged supernatants and from electroporation were investigated. Changing the ionic strength of the supernatant, or replacing it with dextran or poly(ethylene glycol) solutions, caused changes of Rp according to the osmotic behavior of the pellet. Rp was high and ohmic before electroporation, but dropped abruptly in the first few microseconds once the transmembrane voltage exceeded the membrane breakdown potential. After the initial drop, Rp increased as a result of the reduction of intercellular space. Rp increased regardless of whether the pellets were formed before or immediately after the pulse, indicating that porated cells experienced a slow colloidal-osmotic swelling. The intercellular or intermembrane distances between cells in a pellet, as a function of osmotic, colloidal-osmotic, and centrifugal pressures used to compress rabbit erythrocyte pellets, were deduced from the Rp measurement. This offered a unique opportunity to measure the intermembrane repulsive force in a disordered system including living cells. Electrohemolysis of pelleted cells was reduced because of limited swelling by the compactness of the pellet. Electrofusion was observed when the applied voltage per pellet membrane exceeded the breakdown voltage. The fusion yield was independent of pulse length greater than 10 microseconds, because after the breakdown of membrane resistance, voltage drop across the pellet became insignificant. Replacing the supernatant with poly(ethylene glycol) or dextran solutions, or coating pellets with unporated cell layers reduced the colloidal-osmotic swelling and hemolysis, but also reduced the electrofusion yield. These manipulations can be explored to increase electroloading and electrofusion efficiencies.

Animals↗
PubMed1994

Characterization of PEG-mediated electrofusion of human erythrocytes.

Polyethylene glycol (PEG) and electrofusion were applied together in a simple and highly efficient cell fusion method. PEG (8000 M(r)) was used to bring human erythrocytes into contact, and a single 4.4 kV/cm, 80 microseconds duration pulse was applied to cell suspensions. The fusion yield (FY) is PEG concentration-dependent. A maximum FY (50%) was found at about 10% PEG. Higher PEG concentrations (> 10%) suppressed FY caused by colloid osmotic shrinkage. Morphological changes, such as colloidal osmotic swelling and shrinking, and the expanding and contraction of fusion lumen, when suspension media were changed from PBS to isotonic 15% dextran solutions, was examined by microscopy. FY was found to depend on both simple osmotic and colloidal-osmotic swelling. From the swelling behavior, we propose two types of electropores: the pre-fusion sites between cell pairs, and electropores on each individual cell connecting intracellular and extracellular space. The latter type is responsible for the colloidal osmotic swelling and shrinking of cell which, together with simple osmotic swelling, is responsible for expanding the pre-fusion sites into fusion lumens. Resealing of electropores resulted in reducing FY, but the FY can be restored by simple osmotic shock. Apparently, PEG plays two opposite roles in this fusion method; one is to promote pre-pulse and post-pulse cell-cell contact, protecting pre-fusion sites, and the other suppresses FY by colloid osmotic shrinkage of cells after pulsing, especially when high PEG concentration is used. 10% PEG 8000 represents the optimal combination of these properties.

Biophysical Phenomena↗
PubMed1993

Merocyanine interaction with phosphatidylcholine bilayers.

Merocyanine (MC 540) is a fluorescent probe whose optical properties depend on the environmental polarity. In the presence of lipid bilayers, MC 540 binds to the membrane surface while simultaneously changing its fluorescence properties. Previous studies have shown that the fluorescence of merocyanine depends upon the lipid packing in the membrane. We measured the partitioning of MC 540 and its fluorescence properties in the presence of phosphatidylcholine membranes. We found that the fluorescence of MC 540 shows, as expected, a major change around the main phase transition of phosphatidylcholine membranes. However, instead of a step-like increase of fluorescence, the maximum at phase transition was observed. We were able to explain our data by combining two effects; dependence of MC 540 fluorescence on temperature and lipid fluidity. In addition, we established that the increase of the fluorescence intensity in the presence of lipid bilayers in the fluid state is due to the elevated partitioning of the probe into the lipid phase. The partition of MC 540 into the fluid membrane does not depends on the dye concentration in the aqueous phase. When lipid was in the gel phase the partitioning of the dye increased with its bulk concentration, whereas the fluorescence intensity remained unchanged. We conclude, therefore, that MC 540 forms nonfluorescent complexes when in the gel lipid membrane.

Chemical Phenomena↗
PubMed1993

Dehydration-induced lamellar-to-hexagonal-II phase transitions in DOPE/DOPC mixtures.

Plasma membranes of protoplasts isolated from non-acclimated rye plants undergo a transition from the bilayer to the inverted hexagonal (HII) phase during freeze-induced dehydration at -10 degrees C. It has been suggested (Bryant, G. and Wolfe, J. (1989) Eur. Biophys. J. 16, 369-372) that the differential hydration of various membrane components may induce fluid-fluid demixing of highly hydrated (e.g., PC) from poorly hydrated (PE) components during dehydration. This could yield a PE-enriched domain more prone to form the HII phase. We have examined the lyotropic phase behavior of mixtures of DOPE and DOPC at 20 degrees C by freeze-fracture electron microscopy, differential scanning calorimetry, and X-ray diffraction. HII phase formation was favored by higher proportions of DOPE and lower water contents. Mixtures of 1:1 and 1:3 DOPE/DOPC had a hydration-dependent appearance of two L alpha phases at water contents just above those at which the HII phase occurred. The hydration-dependence of the lamellar repeat spacings suggested that the DOPE-enriched domains preferentially underwent the L alpha-to-HII phase transition. Mixtures of 3:1 DOPE/DOPC did not separate into two L alpha phases during dehydration. These data suggest that the differential hydration characteristics of various membrane components may induce their lateral fluid-fluid demixing during dehydration.

Chemical Phenomena↗
PubMed1993

Dithionite penetration through phospholipid bilayers as a measure of defects in lipid molecular packing.

The permeability of dithionite through bilayers was utilized to probe the structural defects in the bilayers of these lipids through their respective gel-fluid and bilayer-hexagonal phase transitions. The water soluble dithionite ion penetrates intact bilayers very slowly. The rate of irreversible quenching of the fluorescence of NBD-PE labelled liposomes may thus be used as an indicator of the permeability of this ion through bilayers. The quenching rate has a fast and a slow component, the fast one corresponds to the quenching of fluorophores immediately accessible to the quencher, i.e. those on the outer surface of liposomes. The slower component represents the average rate of penetration of the quencher through the bilayer, to quench those fluorophores at the inner shells of the multilamellar vesicles. Both rates may be approximated by a single exponential function. The slow exponent is simply related to the permeability. The permeability of DMPC as a function of temperature shows a peak at the gel-fluid phase transition at 24 degrees C, but returns to about the pre-transition value at temperatures above the phase transition. The permeability of egg PE shows a hump at 45 degrees C before the hexagonal phase transition at 65 degrees C is reached and becomes infinite at the hexagonal phase transition as all fluorophores are immediately accessible to the quencher. We believe that the permeability measured by this method relates more to the molecular packing defects which maximizes at the gel-fluid phase transition temperatures just below the bilayer-hexagonal phase transition, rather than the general packing order which simply changes with structural phases.

Cell Membrane Permeability↗
PubMed1993

Electron diffraction studies of molecular ordering and orientation in phospholipid monolayer domains.

The molecular order and orientation of phase separated domains in monolayers of DP(Me)PE and DP(Me)2PE were determined by electron diffraction. Dark and bright fluorescent domains at the air-water interface were observed by fluorescence microscopy. The monolayers were transferred to Formvar coated electron microscope grids for electron diffraction studies. The positions of domains on the marker grids were recorded in fluorescence micrographs, which were used as guide maps to locate these domains in the electron microscope. Selected area electron diffraction patterns were obtained from predetermined areas within and outside the dark domains. Sharp hexagonal diffraction patterns were recorded from dark domains, and diffuse diffraction rings from bright areas in between dark domains. The diffraction results indicated that the dark domains and bright areas were comprised of lipid molecules in solid and fluid states, respectively. The orientation of diffraction patterns from adjacent locations within a dark domains changed gradually, indicating a continuous bending of the molecular packing lattice vector within these domains. Orientation directors in U-shaped DP(Me)2PE domains followed the turn of the arm; no vortex nor branching was indicated by electron diffraction. Directors branching from the "stem" of highly invaginated DP(Me)PE domains usually occurred at twinning angles of n pi/3 from the stem director, which would minimize packing defects in the development of thinner branches. Electron diffraction from local areas of individual domains proved that dark fluorescent domains were solid ones, and that pseudo-long range order existed in these solid domains.

Biophysical Phenomena↗
PubMed1992

Relationship between membrane lipid mobility and spectrin distribution in lymphocytes.

We have previously established that T and B lymphocytes in situ are remarkably heterogeneous with respect to the cytoskeletal protein spectrin. Since in erythrocytes spectrin is known to play an important role in the regulation of membrane fluidity, lipid organization and lateral mobility of membrane proteins, we have sought to determine if the heterogeneous patterns of spectrin distribution that we have observed are related to possible differences in membrane lipid organization in these various subsets. To this end, we have utilized a fluorescent pyrene-labelled phospholipid as a probe of the lipid lateral mobility and have examined two related T cell systems maintained in vitro, DO.11.10 cells and a spontaneously arising variant, DO.11.10V. In these (and other cloned in vitro systems) we have previously observed that the cells homogeneously express one of the kinds of spectrin distribution patterns observed in situ. Thus the uniformity of staining of these systems permits us to address whether the various patterns of spectrin distribution may be predictive of differences in membrane lipid properties. Here we show that in cells in which there is little or nor spectrin at the plasma membrane (DO.11.10) that the lipids in the plasma membrane are considerably less mobile than in its related variant in which spectrin is diffusely distributed within the cell and at the plasma membrane. From this and previous results, we conclude that differences in the distribution of the cytoskeletal protein spectrin among lymphocytes may be a useful parameter in helping to predict the status of membrane lipid organization.

Cell Line↗
PubMed1992

Merocyanine 540 as a probe to monitor the molecular packing of phosphatidylcholine: a monolayer epifluorescence microscopy and spectroscopy study.

The characteristics of the fluorescent dye, merocyanine 540 (MC-540), incorporated in monolayers of 1,2-dipalmitoyl-phosphatidylcholine (DPPC), and 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) were studied in different states of molecular packing. Conditions for phase separation in these monolayers were defined by their pressure/area (pi-A) isotherms. Within the liquid expanded (LE) and the liquid condensed (LC) coexisting phases of DPPC monolayers, low light level epifluorescence microscopy revealed 'dark' discoid domains embedded in a 'bright' matrix. Under the same conditions, and at temperatures as low as 12 degrees C, the pi-A isotherms of POPC demonstrate the existence of a single phase, and no fluorescent domains were observed. Fluorescence spectra of MC-540 labelled monolayers, recorded in different structural states, reveal three distinct emission peaks: a 572 nm peak, present for monolayer packing conditions at low surface pressures; a 585 nm peak, similar to that obtained from dye molecules in fluid phase lipid bilayers, and observed here within the respective area/molecule ranges of 54-62 A2 and 62-69 A2 for monolayers of DPPC and POPC with diminishing intensity at increasing surface pressure; and finally, a peak at 560 nm, which predominates in densely packed POPC monolayers. Our results are interpreted on the basis of dye partitioning between monolayer and subphase, and different orientations of the dye with respect to the monolayer in various structural states. The usefulness of MC-540 to differentiate lipid packing in cell membranes is discussed.

Antiviral Agents↗
PubMed1992

On the mechanism of inhibition of viral and vesicle membrane fusion by carbobenzoxy-D-phenylalanyl-L-phenylalanylglycine.

The mechanism by which the hydrophobic peptide Z-D-Phe-L-PheGly inhibits membrane fusion was investigated. Differential scanning calorimetry, 2H nuclear magnetic resonance (NMR), and 13C NMR of phosphatidylcholine bilayers in the presence of Z-D-Phe-L-PheGly indicate that this hydrophobic peptide penetrates the phospholipid bilayer but does not strongly perturb the properties of phosphatidylcholine bilayers with a large effective radius of curvature. However, Z-D-Phe-L-PheGly does affect the properties of highly curved phosphatidylcholine bilayers. Small, sonicated vesicles (SUV) of dipalmitoylphosphatidylcholine (DPPC) were made in the presence and absence of Z-D-Phe-L-PheGly. At pH 4.5, the presence of Z-D-Phe-L-PheGly inhibited the formation of SUV. At pH 6.7 and 7.4, SUV could form. Once sonication ceased and the vesicles were incubated at 23 degrees C, modest growth in vesicle size occurred for pure DPPC SUV. Rapid change to large sheetlike structures occurred in the presence of Z-D-Phe-L-PheGly. Z-D-Phe-L-PheGly appeared to favor the formation of phospholipid structures with large radii of curvature. In these experiments, Z-D-Phe-L-PheGly had access to both sides of the bilayer. If Z-D-Phe-L-PheGly was added to preformed DPPC SUV (and thus present initially only in the outer leaflet of the vesicle bilayer) and incubated at 23 degrees C, only modest growth in vesicle size was observed with little difference from control values at short to intermediate incubation times.(ABSTRACT TRUNCATED AT 250 WORDS)

1,2-Dipalmitoylphosphatidylcholine↗
PubMed1992

Methylation effects on the microdomain structures of phosphatidylethanolamine monolayers.

Increasing methylation of the headgroup in DPPE results in an increase of minimum area per molecule in highly compressed monolayers at the air-water interface. The shape of solid domains, as observed by epifluorescence microscopy, also exhibits marked changes upon increasing headgroup methylation. Branching domains are observed in DPPE and DP(Me)PE, whereas U-shaped or round domains are observed in DP(Me)2PE and DPPC under our experimental conditions. The domain shape is determined more by the headgroup methylatin than by the corresponding shift in critical temperatures, as shown by the study of PCs of different acyl chain moieties. In mixed lipid monolayers, PC (phosphatidylcholine) and PE (phosphatidylethanolamine) do not mix ideally, as indicated by the non-linear variation of the average area per molecule with composition, and by distinct domain shapes in LE/LC (liquid expanded/liquid condensed) coexisting phases representing PE-enriched or PC-enriched domains in those mixed monolayers.

1,2-Dipalmitoylphosphatidylcholine↗
PubMed1992

Formation of a new stable phase of phosphatidylglycerols.

Dilauroyl and dimyristoylphosphatidylglycerol (DMPG) form a more stable gel state when aqueous suspensions are incubated several days at low temperature (0-2 degrees C), pH 7.4 with 0.15 M NaCl. This gel state is characterized by a higher transition temperature and a higher transition enthalpy. The geometry of this gel state is distinguishable from the metastable gel state that forms rapidly upon hydration on the basis of its x-ray diffraction pattern. Infrared spectra in the CH2 scissoring region indicate that the stable gel phase of DMPG is also characterized by reduced reorientational fluctuations of acyl chains and increased interchain interactions. Analysis of vibrational bands due to ester carbonyl groups of DMPG suggests that the transition to a new gel phase is initiated by changes in the interfacial and/or headgroup region of the bilayer, most likely via formation of interlipid hydrogen bonds. The melting of the stable gel phase of DMPG is accompanied by a gross morphological change resulting in vesiculation.

Calorimetry, Differential Scanning↗