TBI with lung dose reduction does not improve hematopoietic cell homing to BM during allogeneic transplantation.

To determine the effects of TBI dose, fractionation and lung shielding on hematopoietic stem cell homing to the BM, BM cells were extracted from tibiae and femurs of B6-green fluorescent protein (GFP) mice and transplanted into B6 mice. Recipient mice had either: (i) no radiation, (ii) single-dose TBI at 13.6 Gy, (iii) single-dose TBI at 13.6 Gy with reduced lung exposure to 0.4 Gy by shielding, (iv) split-dose TBI at 12 Gy to twice per day over 4 days or (v) split-dose TBI at 12 Gy to twice per day over 4 days with reduced lung exposure to 0.36 Gy by shielding. The last radiation exposure preceded tail vein injection by 4-6 h. Mice were killed after 18 h. The homing of GFP-positive, lineage-negative cells was not significantly improved in any irradiated group compared with control. The homing of GFP-positive, lineage-negative, Kit-positive cells was significantly worse in all irradiated groups. TBI does not improve the homing of lineage-negative donor BM cells to the recipient marrow. The homing of lineage-negative, Kit-positive donor BM cells was significantly worse following TBI, with or without lung dose reduction.

Modulation of angiogenesis by dithiolethione-modified NSAIDs and valproic acid.

BACKGROUND AND PURPOSE: Angiogenesis involves multiple signaling pathways that must be considered when developing agents to modulate pathological angiogenesis. Because both cyclooxygenase inhibitors and dithioles have demonstrated anti-angiogenic properties, we investigated the activities of a new class of anti-inflammatory drugs containing dithiolethione moieties (S-NSAIDs) and S-valproate. EXPERIMENTAL APPROACH: Anti-angiogenic activities of S-NSAIDS, S-valproate, and the respective parent compounds were assessed using umbilical vein endothelial cells, muscle and tumor tissue explant angiogenesis assays, and developmental angiogenesis in Fli:EGFP transgenic zebrafish embryos. KEY RESULTS: Dithiolethione derivatives of diclofenac, valproate, and sulindac inhibited endothelial cell proliferation and induced Ser(78) phosphorylation of hsp27, a known molecular target of anti-angiogenic signaling. The parent drugs lacked this activity, but dithiolethiones were active at comparable concentrations. Although dithiolethiones can potentially release hydrogen sulphide, NaSH did not reproduce some activities of the S-NSAIDs, indicating that the dithioles regulate angiogenesis through mechanisms other than release of H(2)S. In contrast to the parent drugs, S-NSAIDs, S-valproate, NaSH, and dithiolethiones were potent inhibitors of angiogenic responses in muscle and HT29 tumor explants assessed by 3-dimensional collagen matrix assays. Dithiolethiones and valproic acid were also potent inhibitors of developmental angiogenesis in zebrafish embryos, but the S-NSAIDs, remarkably, lacked this activity. CONCLUSIONS AND IMPLICATION: S-NSAIDs and S-valproate have potent anti-angiogenic activities mediated by their dithiole moieties. The novel properties of S-NSAIDs and S-valproate to inhibit pathological versus developmental angiogenesis suggest that these agents may have a role in cancer treatment.

Hemolymph osmolality and cation concentrations in Litopenaeus vannamei during exposure to artificial sea salt or a mixed-ion solution: relationship to potassium flux.

Interest in culturing the Pacific white shrimp Litopenaeus vannamei in low-salinity and brackish-well waters has led to questions about the ability of this species to osmo- and ionoregulate in environments containing low concentrations of ions and in environments with ionic ratios that differ from those found in sea water. After seven days, hemolymph osmolality and potassium, sodium and calcium values were all significantly affected by salinity (as artificial sea salt) with values decreasing with decreasing salinity. These decreases were small, however, relative to decreases in salinity, indicating iono- and osmoregulation with adjustment for gradients. The hemolymph osmolality and sodium and calcium concentrations in shrimp exposed to either 2 g/L artificial sea salt or 2 g/L mixed-ion solution (a mixture of sodium, potassium, calcium, and magnesium chlorides that approximate the concentrations and ratios of these cations found in 2 g/L dilute seawater) did not differ significantly. However, hemolymph potassium levels were significantly lower in shrimp held in the mixed-ion environment. Potassium influx rates were similar in shrimp held in either artificial sea salt or mixed ions. The results of this study indicate that salinity affects hemolymph-cation concentrations and osmolality. Further, differential potassium-influx rates do not appear to be the basis for low hemolymph potassium levels observed in shrimp held in mixed-ion environments.

Membrane skeleton involvement in cell fusion kinetics: a parameter that correlates with erythrocyte osmotic fragility.

Spectrin levels in erythrocytes have been related to several biomechanical and biophysical membrane properties essential to the survival and function of the cell. Populations of erythrocytes display a natural and finite range of sensitivities to osmotic shock that has been directly correlated, in studies from other laboratories, to the presence of spectrin. We used a procedure to isolate subpopulations of 1) the osmotically most sensitive and 2) the osmotically most resistant erythrocyte membranes in an attempt to select for membranes enriched and depleted in spectrin (and/or a related component). The mechanical function of the spectrin-based membrane skeleton was further explored in these two subpopulations by searching for any effect on the time-dependent increase in fusion zone diameter in pairs of electrofused erythrocyte ghosts as a model for cell fusion. The results clearly show that the diameter expansions in fusions of membranes from osmotically resistant erythrocytes are faster in the early stage (up to 9 to 10 s after fusion) but do not thereafter expand as far as in fusions of membranes from osmotically sensitive membranes.

A mechanical cycling phenomenon in electrofused eryhrocytes.

We have characterized a reciprocating mechanical oscillation that can easily be detected in a large fraction of electrofused erythrocytes. Under our conditions, up to about 30% of all electrofusion products (e.g. doublet, triplet, and higher) show at least one cycle and up to 10% show only two cycles. A much smaller fraction (about 1-2%) show 5-10 or more cycles before stopping. In fused doublets the oscillation appears as a roughly linear and slow expansion of the diameter of the 'hourglass constriction' or fusion zone which proceeds simultaneously with a slow contraction of the pole-to-pole length. At what appears to be a threshold, the fusion zone diameter shrinks simultaneously with an expansion in the pole-to-pole length. This takes place rapidly (within a few video frames). The change in length is about 10% and is easily observable by video light microscopy. The periodicity is variable (5-60 s) and subsequent periods often decrease substantially in length. For the range studied, the characteristics of the reciprocation do not appear to be dependent on the strength of the electric field pulse. To our knowledge this phenomenon was originally discovered, but not characterized, in another laboratory. Using our protocol, cells were observed to undergo fusion from as soon as 6, to as late as 84 s after the fusogenic electric pulse was applied.

Membrane skeleton restraint of surface shape change during fusion of erythrocyte membranes: evidence from use of osmotic and dielectrophoretic microforces as probes.

The role of the spectrin-based membrane skeleton in cell fusion was studied by following the condition-dependent diameter versus time expansion signature of the fusion zone in electrofused pairs of erythrocyte ghost membranes. Previous work showed that the presence of the dielectrophoresis-inducing alternating electric field, which is used to bring membranes into contact through pearl chain formation, had a detectable promoting effect on fusion zone expansion. Two new dielectrophoresis protocols were used in the present work to utilize this externally generated and controllable microforce field to probe the forces intrinsic to the system that drives the expansion of the fusion zone. First, fusion zones expanded to a greater diameter in a strong AC field compared to a weak AC field, and they expanded to a greater diameter if erythrocyte ghosts received a prior heat treatment (42 degrees C, 20 min). Furthermore, flat diaphragm fusion zones broke down into open lumen fusion zones sooner (i.e., had shorter lifetimes) when they were expanding more quickly. Second, changing the AC field strength at specific times during the fusion zone expansion led to an immediate visco-elastic response. However, shifting the AC field strength to zero after 5 s of fusion zone expansion resulted in a subsequent decrease in the average fusion zone diameter. This suggests not only that the spectrin-based membrane skeleton actually tends to prevent the rounding up process but that it may be capable of generating an antirounding force, which has broad implications for the role of the membrane skeleton in cell fusion. These results are consistent with the hypothesis that flat diaphragm fusion zones induced in heat-treated membranes were very easily stretched and that membrane-based forces that control or drive the expansion process must originate from membrane area that is outside rather than inside the fusion zone. Lastly, when an outward-directed osmotic pressure-based microforce was present at the time that erythrocyte ghosts were fused, the fusion zone diameter underwent a greater expansion in the 0-1 s interval after fusion. This suggests that an osmotic pressure-based microforce can be used to experimentally calibrate the dielectrophoretic force.

Dielectrophoretic forces and potentials induced on pairs of cells in an electric field.

A combined numerical/experimental study is reported of the membrane potentials and dielectrophoretically induced forces between cells, membrane pressures, and velocity of attraction of cells under the influence of an electric field. This study was designed to explore electrical and mechanical effects produced by a field on cells in close proximity or undergoing electrically induced fusion. Laplace's equation for pairs of membrane-covered spheres in close proximity was solved numerically by the boundary element method, and the electrically induced forces on the cells and between cells were obtained by evaluating the Maxwell stress tensor. The velocity of approach of erythrocyte ghosts or fused ghosts in a 60-Hz field of 6 V/mm was measured experimentally, and the data were interpreted by using Batchelor's theory for hydrodynamic interaction of hard spheres. The numerical results show clearly the origin of the dielectrophoretic pressures and forces in fused and unfused cells and the effects of a nearby cell on the induced membrane potentials. The experimental results agree well with predictions based on the simple electrical model of the cell. The analysis shows the strong effect of hydrodynamic interactions between the cells in determining their velocity of approach.

Surface shape change during fusion of erythrocyte membranes is sensitive to membrane skeleton agents.

We previously reported that the induction of membrane fusion between pairs of erythrocyte ghosts is accompanied by the formation of a multipore fusion zone that undergoes an area expansion with condition-dependent characteristics. These characteristics allowed us to hypothesize substantial, if not major, involvement of the spectrin-based membrane skeleton in controlling this expansion. It was also found that the fusion zone, which first appears in phase optics as a flat diaphragm, has a lifetime that is also highly condition-dependent. We report here that 2,3-diphosphoglycerate, wheat germ agglutinin, diamide, and N-ethylmaleimide, all known to have binding sites primarily on skeleton components (including spectrin), have condition-dependent effects on specific components of the fusion zone diameter versus time expansion curve and the flat diaphragm lifetime. We also report a pH/ionic strength condition that causes a dramatic stabilization of flat diaphragms in a manner consistent with the known pH/ionic strength dependence of the spectrin calorimetric transition, thus further supporting the hypothesis of spectrin involvement. Our data suggest that the influence of the membrane skeleton on cell fusion is to restrain the rounding up that takes place after membrane fusion and that it may have variable, rather than fixed, mechanical properties. Data show that WGA, a known ligand for sialic acid, and DPG, a known metabolite, influences the flat diaphragm stability and late period expansion rates, raising the possibility that some of these mechanical properties are biologically regulated.

Distinct mechanical relaxation components in pairs of erythrocyte ghosts undergoing fusion.

It was previously reported (Chernomordik and Sowers, 1991) that erythrocyte ghosts which were exposed to a 42 degrees C, 10-min heat treatment would, upon electrofusion, produce over 15-20 s a fusion product with an "open lumen" (i.e., the fusion product became converted to one large sphere), while electrofusion of ghost membranes not so exposed would lead to chains of polyghosts. In phase optics the chains of polyghosts showed a "flat diaphragm" at virtually every ghost-ghost junction (i.e., the ghosts do not appear to be fused even though fluorescent-labeled lipid analogs can laterally diffuse from a labeled ghost to an adjacent unlabeled ghost). In the present study we found that the diameter increase in open lumen- and flat diaphragm-producing fusion processes both had a rapid but short early phase (0-5 s after fusion) which was exponential or nearly so and a slow but long late phase (5-120 s after fusion) which was essentially linear. Heat treatments at 39 or 42 degrees C caused a minor acceleration in only the late phase, while temperatures of 45 or 50 degrees C caused an immediate and dramatic acceleration in the rate of diameter increase (spheres in 1-2 s). Ghost membranes in the presence of glycerol at 20% (v/v) did not form open lumens when exposed to the 42 degrees C (but not the > or = 45 degrees C) heat treatment. This suggested that the heat treatment was denaturing a critical protein. Both of these observations are consistent with the involvement of the spectrin network since it is the only protein in the erythrocyte membrane which is known (Brandts et al., 1977) to have a calorimetric transition over the same temperature range used in our heat treatments. The diameter versus time curves were sensitive to: (i) the residual effects of the fusogenic electric pulse only up to about 1 s after the pulse, (ii) the strength of the dielectrophoretic field after the pulse, but not before the pulse,(iii) the ambient temperature during the measurement.

Kinetics and mechanism of cell membrane electrofusion.

A new quantitative approach to study cell membrane electrofusion has been developed. Erythrocyte ghosts were brought into close contact using dielectrophoresis and then treated with one square or even exponentially decaying fusogenic pulse. Individual fusion events were followed by lateral diffusion of the fluorescent lipid analogue 1,1'-dihexadecyl-3,3,3',3'-tetramethylindocarbocyanine perchlorate (Dil) from originally labeled to unlabeled adjacent ghosts. It was found that ghost fusion can be described as a first-order rate process with corresponding rate constants; a true fusion rate constant, k(f), for the square waveform pulse and an effective fusion rate constant, k(ef), for the exponential pulse. Compared with the fusion yield, the fusion rate constants are more fundamental characteristics of the fusion process and have implications for its mechanisms. Values of k(f) for rabbit and human erythrocyte ghosts were obtained at different electric field strength and temperatures. Arrhenius k(f) plots revealed that the activation energy of ghost electrofusion is in the range of 6-10 kT. Measurements were also made with the rabbit erythrocyte ghosts exposed to 42 degrees C for 10 min (to disrupt the spectrin network) or 0.1-1.0 mM uranyl acetate (to stabilize the bilayer lipid matrix of membranes). A correlation between the dependence of the fusion and previously published pore-formation rate constants for all experimental conditions suggests that the cell membrane electrofusion process involve pores formed during reversible electrical breakdown. A statistical analysis of fusion products (a) further supports the idea that electrofusion is a stochastic process and (b) shows that the probability of ghost electrofusion is independent of the presence of Dil as a label as well as the number of fused ghosts.

Evidence that the spectrin network and a nonosmotic force control the fusion product morphology in electrofused erythrocyte ghosts.

The conversion of the membrane area in the "contact zones" shared by erythrocyte ghosts held in contact by dielectrophoresis into a fusion product by electrofusion was studied by both light and electron microscopy. Fusion products fell into two categories: (a) those with a freely expanding open lumen which ended in the "giant cell morphology" and with considerable internal vesicle membrane fragments, and (b) linear chains of polyghosts with long term stability but having planar diaphragms at the ghost-ghost junctions. Thin section electron microscopy showed each of these planar diaphragms to be a double membrane septum multiply-perforated with fusion pores. Heat and low ionic strength treatments known to denature or detach spectrin caused the stable planar diaphragms to dissolve, thereby quickly converting the polyghost chains to the giant cell morphology, thereby suggesting that spectrin restricts fusion zone diameter expansion if it is intact. Other indications suggest that the expansion of the open lumens appears to take place as a result of one or more membrane-specific forces with a nonosmotic origin but this tendency to expansion can be overcome if the spectrin network on only one side of a contact zone is intact.

A delay in membrane fusion: lag times observed by fluorescence microscopy of individual fusion events induced by an electric field pulse.

Low light level video microscopy of the fusion of DiI- (1,1'-dihexadecyl-3,3,3',3'-tetramethylindocarbocyanine perchlorate) labeled rabbit erythrocyte ghosts with unlabeled rabbit erythrocyte ghosts, held in stable apposition by dielectrophoresis in sodium phosphate buffers, showed reproducible time intervals (delays) between the application of a single fusogenic electric pulse and the earliest detection of fluorescence in the unlabeled adjacent membranes. The delay increased over the range 0.3-4 s with a decrease in (i) the electric field strength of the fusion-inducing pulse from 1000 to 250 V/mm, (ii) the decay half-time of the fusogenic pulse in the range 1.8-0.073 ms, and (iii) the dielectrophoretic force which brings the membranes into close apposition. A change in the buffer viscosity from 1.8 to 10 mP.s caused the delay to increase from 0.36 to 3.7 s (in glycerol solutions) or to 5.2 s (in sucrose solutions). The delay decreased 2-3 times with an increase in temperature from 21 to 37 degrees C. It did not differ significantly for "white" ghosts [0.013 mM hemoglobin (Hb)] or "red" ghosts (0.15 mM Hb) or buffer strength over the range 5-60 mM (sodium phosphate, pH 8.5). The calculated activation energy, 17 kcal/mol, does not depend on the field strength. The yield of fused cells was high when the delay was short. The delay in electrofusion resembles the delays in pH-dependent fusion of vesicular stomatitis viruses with erythrocyte ghosts [Clague, M. J., Schoch, C., Zech, L., & Blumenthal, R. (1990) Biochemistry 29, 1303-1308] and of fibroblasts expressing influenza hemagglutinin and red blood cells [Morris, S. J., Sarkar, D.P., White, J. M., & Blumenthal, R. (1989) J. Biol. Chem. 264, 3972-3978].(ABSTRACT TRUNCATED AT 250 WORDS)

Low concentrations of macromolecular solutes significantly affect electrofusion yield in erythrocyte ghosts.

Electrofusion yields in rabbit erythrocyte ghosts containing various amounts of hemoglobin, bovine serum albumin, or dextran at low concentrations were measured as a function of pulse field strength and pulse decay half-time. The presence of any of the macromolecules in low concentrations caused fusion yields to be significantly higher than when the ghosts were white (i.e., containing only buffer). The fusion yield enhancement was also critically dependent on the parameters of the electric field pulse. The fusion yield was also significantly affected by small changes in the concentration of hemoglobin when it was present outside the ghost membranes in the suspension buffer.

Attraction, deformation and contact of membranes induced by low frequency electric fields.

The force of attraction between erythrocyte ghosts induced by low frequency electric fields (60 Hz) was measured as a function of the intermembrane separation. It varied from 10(-14) N for separation of the order of the cell diameter to 10(-12) N for close approach and contact in 20 mM sodium phosphate buffers (conductivity 260 mS/m, pH 8.5). For large separations the interaction force followed a dependence on separation as predicted for dipole-dipole interactions. For small separation an empirical formula was obtained. The membranes deformed at close approach (less than 1 microns) before making contact. The contact area increased with time until reaching the final equilibrium state. The ghosts separated reversibly after switching off the electric field. The membrane tension induced by the ghost interaction at contact was estimated to be of the order of 0.1 mN/m. These first quantitative measurements of the force/separation dependence for intermembrane interactions induced by low frequency electric fields indicate that attractive forces, membrane deformation and contact area of cells depend strongly on intermembrane separation and field strength. The quantitative relationship between them are important for measuring membrane surface and mechanical properties, intermembrane forces and understanding mechanisms of membrane adhesion, instability and fusion in electric fields and in general.

Membrane electroporation--fast molecular exchange by electroosmosis.

Human and rabbit erythrocyte ghosts loaded with FITC-dextran (mol. mass = 10 kDa) and NBD-glucosamine (mol. mass = 342 Da) in buffers of different ionic strength and composition were subjected to electric pulses (intensity 0.7 kV/mm and decay half-time 1 ms) at 7-10 degrees C and 20-24 degrees C. The transfer of the fluorescent dyes from the interior of the ghosts through the electropores was observed by low light level video microscopy. The pulses caused the fluorescence to appear outside the membranes as a transient cylindrical cloud directed toward the negative electrode during the first video frame (17 ms). It was similar in both rabbit and human erythrocyte ghosts and at both temperatures but differs for the two dyes, the fluorescence cylinder is long and tall for the FITC-dextran and relatively short and thick for the NBD-glucosamine. The molecular exchange was 2-3 orders of magnitude faster within the first 17 ms after the pulse than the diffusional exchange. It decreased with increasing ionic strength. Formulae for the transfer of molecules by electroosmotic flow through the pores are in agreement with these observations. They allow estimation of the total area of pores with radii larger than that of the fluorescent dye during the pulse. The major conclusion is that electroosmosis is the dominating mechanism of molecular exchange in electroporation of erythrocyte ghosts.

Evidence that electrofusion yield is controlled by biologically relevant membrane factors.

Rabbit + rabbit and human + human combinations of erythrocyte ghost membranes were fused under the same conditions with an electric pulse. Storage at 4 degrees C of ghost membranes from both rabbit and human erythrocytes showed no change with time but storage of the erythrocytes for various periods before ghost preparation showed consistent storage-dependent changes in fusion yield.

Electrofusion of dissimilar membrane fusion partners depends on additive contributions from each of the two different membranes.

Rabbit erythrocyte ghost (REG) membranes and human erythrocyte ghosts (HEG) were aligned into contact by dielectrophoresis and fused with an electric pulse in REG + REG, HEG + HEG, and REG + HEG combinations. REG + HEG fusion yields were approximately midway between fusion yields for REG + REG and HEG + HEG over a wide range of pulse characteristics.

Fusion events and nonfusion contents mixing events induced in erythrocyte ghosts by an electric pulse.

The mechanism of membrane fusion was studied by using human erythrocyte ghosts held in close contact by alternating current-induced dielectrophoresis and inducing fusion with a single electric field pulse. Individual fusion events were followed visually using either 1,1'-dihexadecyl-3,3,3',3'-tetramethylindo carbocyanine perchlorate as a membrane-mixing label or 10-kD fluorescein isothiocyanate-dextran as a contents-mixing label. However, over a range of variables, the number of contents-mixing events usually considerably exceeded the number of membrane-mixing events, although the discrepancy was less at higher ionic strength. However, when the dielectrophoretic force holding the membranes in contact was turned off after the pulse, Brownian motion caused some of the groups of ghosts in which contents mixing occurred to eventually separate from one another, showing that they could not represent fusion events. Separate experiments showed, conversely, that fusion did occur in the groups that did not separate after the dielectrophoresis was turned off.