Relationship between intracellular ice formation in oocytes of the mouse and Xenopus and the physical state of the external medium--a revisit

We have previously reported that intracellular ice formation (IIF) in mouse oocytes suspended in glycerol/PBS solutions or ethylene glycol (EG)/PBS solutions and rapidly cooled to −50 °C or below occurs at temperatures where a critical fraction of the external water remains unfrozen [P. Mazur, S. Seki, I.L. Pinn, F.W. Kleinhans, K. Edashige, Extra- and intracellular ice formation in mouse oocytes, Cryobiology 51 (2005) 29-53; P. Mazur, I.L. Pinn, F.W. Kleinhans, The temperature of intracellular ice formation in mouse oocytes vs. the unfrozen fraction at that temperature, Cryobiology 54 (2007) 223-233]. For mouse oocytes in PBS or glycerol/PBS that fraction is 0.06; for oocytes in EG that fraction was calculated to be 0.13, more than double. The fractions unfrozen are computed from ternary phase diagrams. In the previous publication, we used the EG data of Woods et al. [E.J. Woods, M.A.J. Zieger, D.Y. Gao, J.K. Critser, Equations for obtaining melting points for the ternary system ethylene glycol/sodium chloride/Water and their application to cryopreservation., Cryobiology 38 (1999) 403-407]. Since then, we have determined that ternary phase diagrams for EG/NaCl/water synthesized by summing binary phase data for EG/water NaCl/water gives substantially different curves, which seem more realistic [F.W. Kleinhans, P. Mazur, Comparison of actual vs. synthesized ternary phase diagrams for solutes of cryobiological interest, Cryobiology 54 (2007) 212-222]. Unfrozen fractions at the temperatures of IIF computed from these synthesized phase diagrams are about half of those calculated from the Woods et al. data, and are in close agreement with the computations for glycerol; i.e., IIF occurs when about 92-94% of the external water is frozen. A parallel paper was published by Guenther et al. [J.F. Guenther, S. Seki, F.W. Kleinhans, K. Edashige, D.M. Roberts, P. Mazur, Extra-and intra-cellular ice formation in Stage I and II Xenopus laevis oocytes, Cryobiology 52 (2006) 401-416] on IIF in oocytes of the frog Xenopus. It too examined whether the temperatures of IIF were related to the unfrozen fractions at those temperatures. It also used the Woods et al. ternary phase data to calculate the unfrozen fractions for EG solutions. As reported here, once again the values of these unfrozen fractions are substantially different from those calculated using synthesized phase diagrams. With the latter, the unfrozen fractions at IIF become very similar for EG and glycerol.     

Extra- and intracellular ice formation in mouse oocytes

The occurrence of intracellular ice formation (IIF) during freezing, or the lack there of, is the single most important factor determining whether or not cells survive cryopreservation. One important determinant of IIF is the temperature at which a supercooled cell nucleates. To avoid intracellular ice formation, the cell must be cooled slowly enough so that osmotic dehydration eliminates nearly all cell supercooling before reaching that temperature. This report is concerned with factors that determine the nucleation temperature in mouse oocytes. Chief among these is the concentration of cryoprotective additive (here, glycerol or ethylene glycol). The temperature for IIF decreases from -14 degrees C in buffered isotonic saline (PBS) to -41 degrees C in 1M glycerol/PBS and 1.5M ethylene glycol/PBS. The latter rapidly permeates the oocyte; the former does not. The initial extracellular freezing at -3.9 to -7.8 degrees C, depending on the CPA concentration, deforms the cell. In PBS that deformation often leads to IIF; in CPA it does not. The oocytes are surrounded by a zona pellucida. That structure appears to impede the growth of external ice through it, but not to block it. In most cases, IIF is characterized by an abrupt blackening or flashing during cooling. But in some cases, especially with dezonated oocytes, a pale brown veil abruptly forms during cooling followed by slower blackening during warming. Above -30 degrees C, flashing occurs in a fraction of a second. Below -30 degrees C, it commonly occurs much more slowly. We have observed instances where flashing is accompanied by the abrupt ejection of cytoplasm. During freezing, cells lie in unfrozen channels between the growing external ice. From phase diagram data, we have computed the fraction of water and solution that remains unfrozen at the observed flash temperatures and the concentrations of salt and CPA in those channels. The results are somewhat ambiguous as to which of these characteristics best correlates with IIF.     

Extra- and intra-cellular ice formation in Stage I and II Xenopus laevis oocytes

We are currently investigating factors that influence intracellular ice formation (IIF) in mouse oocytes and oocytes of the frog Xenopus. A major reason for choosing these two species is that while their eggs normally do not possess aquaporin channels in their plasma membranes, these channels can be made to express. We wish to see whether IIF is affected by the presence of these channels. The present Xenopus study deals with control eggs not expressing aquaporins. The main factor studied has been the effect of a cryoprotective agent [ethylene glycol (EG) or glycerol] and its concentration. The general procedure was to (a) cool the oocytes on a cryostage to slightly below the temperatures at which extracellular ice formation occurs, (b) warm them to just below the melting point, and (c) then re-cool them to -50 degrees C at 10 degrees C/min. In the majority of cases, IIF occurs well into step (c), but a sizeable minority undergo IIF in steps (a) or (b). The former group we refer to as low-temperature flashers; the latter as high-temperature flashers. IIF is manifested as abrupt blackening of the egg, which we refer to as "flashing." Observations on the Linkam cryostage are restricted to Stage I and II oocytes, which have diameters of 200 300 microm. In the absence of a cryoprotective agent, that is in frog Ringers, the mean flash temperature for the low-temperature freezers is -11.4 degrees C, although a sizeable percentage flash at temperatures much closer to that of the EIF (-3.9 degrees C). When EG is present, the flash temperature for the low-temperatures freezers drops significantly to approximately -20 degrees C for EG concentrations ranging from 0.5 to 1.5 M. The presence of 1.5 M glycerol also substantially reduces the IIF temperature of the low-temperature freezers; namely, to -29 degrees C, but 0.5 and 1 M glycerol exert little or no effect. The IIF temperatures observed using the Linkam cryostage agree well with those estimated by calorimetry [F.W. Kleinhans, J.F. Guenther, D.M. Roberts, P. Mazur, Analysis of intracellular ice nucleation in Xenopus oocytes by differential scanning calorimetry, Cryobiology 52 (2006) 128-138]. The IIF temperatures in Xenopus are substantially higher than those observed in mouse oocytes [P. Mazur, S. Seki, I.L. Pinn, F.W. Kleinhans, K. Edashige, Extra- and intracellular ice formation in mouse oocytes, Cryobiology 51 (2005) 29-53]. Perhaps that is a reflection of their much larger size.     

Effects of hold time after extracellular ice formation on intracellular freezing of mouse oocytes

MII mouse oocytes in 1 and 1.5M ethylene glycol(EG)/phosphate buffered saline have been subjected to rapid freezing at 50 degrees C/min to -70 degrees C. When this rapid freezing is preceded by a variable hold time of 0-3 min after the initial extracellular ice formation (EIF), the duration of the hold time has a substantial effect on the temperature at which the oocytes subsequently undergo intracellular ice formation (IIF). For example, in 1M EG, the IIF temperatures are -23.7 and -39.2 degrees C with 0 and 2 min hold times; in 1.5M EG, the corresponding IIF temperatures are -29.1 and -40.8 degrees C.     

Relative contributions of the fraction of unfrozen water and of salt concentration to the survival of slowly frozen human erythrocytes.

As suspensions of cells freeze, the electrolytes and other solutes in the external solution concentrate progressively, and the cells undergo osmotic dehydration if cooling is slow. The progressive concentration of solute comes about as increasing amounts of pure ice precipitate out of solution and cause the liquid-filled channels in which the cells are sequestered to dwindle in size. The consensus has been that slow freezing injury is related to the composition of the solution in these channels and not to the amount of residual liquid. The purpose of the research reported here was to test this assumption on human erythrocytes. Ordinarily, solute concentration and the amount of liquid in the unfrozen channels are inversely coupled. To vary them independently, one must vary the initial solute concentration. Two solutes were used here: NaCl and the permeating protective additive glycerol. To vary the total initial solute concentration while holding the mass ratio of glycerol to NaCl constant, we had to allow the NaCl tonicity to depart from isotonic. Specifically, human red cells were suspended in solutions with weight ratios of glycerol to NaCl of either 5.42 or 11.26, where the concentrations of NaCl were 0.6, 0.75, 1.0, 2.0, 3.0, or 4.0 times isotonic. Samples were then frozen to various subzero temperatures, which were chosen to produce various molalities of NaCl (0.24-3.30) while holding the fraction of unfrozen water constant, or conversely to produce various unfrozen fractions (0.03-0.5) while holding the molality of salt constant. (Not all combinations of these values were possible). The following general findings emerged: (a) few cells survived the freezing of greater than 90% of the extracellular water regardless of the salt concentration in the residual unfrozen portion. (b) When the fraction of frozen water was less than 75% the majority of the cells survived even when the salt concentration in the unfrozen portion exceeded 2 molal. (c) Salt concentration affected survival significantly only when the frozen fraction lay between 75 and 90%. To find a major effect on survival of the fraction of water that remains unfrozen was unexpected. It may require major modifications in how cryobiologists view solution-effect injury and its prevention.     

Cryomicroscopic analysis of intracellular ice formation during freezing of mouse oocytes without cryoadditives

Kinetics of intracellular ice formation (IIF) under various freezing conditions was investigated for mouse oocytes at metaphase II obtained from B6D2F1 mice. A new cryostage with improved optical performance and "isothermal" temperature field was used for nucleation experiments. The maximum thermal gradient across the window was less than 0.1 degrees C/10 mm at sample temperatures near 0 degrees C. The dependence of IIF on the initial concentration of the suspending medium was found to be pronounced. The mean IIF temperatures were found to be -9.56, -12.49, -17.63, -22.20 degrees C for freezing at 120 degrees C/min in 200, 285, 510, and 735 mosm phosphate-buffered saline, respectively. For concentrations higher than 735 mosm, the kinetics of IIF showed a break point at approximately -31 degrees C. Below -31 degrees C, all the remaining unfrozen oocytes underwent IIF almost immediately over a temperature range of less than 3 degrees C. This dramatic shift in the kinetics of IIF suggests that there were two distinct mechanisms responsible for IIF during freezing. The effect of the cooling rate on the kinetics of IIF was also investigated in isotonic PBS. At 1 degrees C/min none of the oocytes contained ice, whereas, at 5 degrees C/min all the oocytes contained ice. The mean IIF temperatures for cooling rates between 1 and 120 degrees C/min were almost constant with an average of -12.82 +/- 0.6 degrees C (SEM). In addition, constant temperature experiments were conducted in isotonic PBS. The percentages of oocytes with IIF were 0, 50, 60, and 95% for -3.8, -6.4, -7.72, and -8.85 degrees C. In undercooling experiments, IIF was not observed until approximately -20 degrees C (at which temperature the whole suspension was frozen spontaneously), suggesting the involvement of the external ice in the initiation of IIF between approximately -5 and -31 degrees C during freezing of oocytes.     

Analysis of intracellular ice nucleation in Xenopus oocytes by differential scanning calorimetry

Intracellular ice formation (IIF) plays a central role in cell damage during cryopreservation. We are investigating the factors which trigger IIF in Xenopus oocytes, with and without aquaporin water channels. Here, we report differential scanning calorimeter studies of Xenopus control oocytes which do not express aquaporins. Stage I to VI oocytes (which increase progressively in size) were investigated with emphasis on stage I and II because they are translucent and can also be studied under the cryomicroscope. Measurements were made in 1, 1.5, and 2M ethylene glycol (EG) in frog Ringers plus SnoMax. A multistep freezing protocol was used in which the samples were cooled until extracellular ice formation (EIF) occurred, partially remelted, slowly recooled through the EIF temperature, and then rapidly (10 degrees C/min) cooled. EIF in the 1, 1.5, and 2M EG occurred at -6.4, -7.8, and -8.9 degrees C, respectively. Freezing exotherms of individual stage I-VI oocytes were readily visible. A general trend was observed in which the IIF temperature of the early stage oocytes (I-III) was well below T(EIF) while the later stages (IV-VI) froze at temperatures much closer to T(EIF). Thus, in 1.5M EG, T(IIF) was -21.1, -25, and -26.6 degrees C in stages I-III, but was -17 and -8.5 degrees C for stage IV and V-VI. Concurrently, the percentage of oocytes in which IIF was observed fell dramatically from a high of 40 to 72% in early stages (I-III) to a low of only 7% in stage V-VI because, particularly in the later stages, IIF was hidden in the EIF exotherm. We conclude that early stage oocytes are a good model system in which to investigate modulators of IIF, but that late stage oocytes are damaged during EIF and infrequently supercool.     

Cell inactivation and membrane damage after long-term treatments at sub-zero temperature in the supercooled and frozen states

The survival of cells subjected to cooling at sub-zero temperature is of paramount concern in cryobiology. The susceptibility of cells to cryopreservation processes, especially freeze-thawing, stimulated considerable interest in better understanding the mechanisms leading to cell injury and inactivation. In this study, we assessed the viability of cells subjected to cold stress, through long-term supercooling experiments, versus freeze-thawing stress. The viability of Escherichia coli, Saccharomyces cerevisiae, and leukemia cells were assessed over time. Supercooled conditions were maintained for 71 days at -10 degrees C, and for 4 h at -15 degrees C, and -20 degrees C, without additives or emulsification. Results showed that cells could be inactivated by the only action of sub-zero temperature, that is, without any water crystallization. The loss of cell viability upon exposure to sub-zero temperatures is suggested to be caused by exposure to cold shock which induced membrane damage. During holding time in the supercooled state, elevated membrane permeability results in uncontrolled mass transfer to and from the cell maintained at cold conditions and thus leads to a loss of viability. With water crystallization, cells shrink suddenly and thus are exposed to cold osmotic shock, which is suggested to induce abrupt loss of cell viability. During holding time in the frozen state, cells remain suspended in the residual unfrozen fraction of the liquid and are exposed to cold stress that would cause membrane damage and loss of viability over time. However, the severity of such a stress seems to be moderated by the cell type and the increased solute concentration in the unfrozen fraction of the cell suspension.     

On the mechanism of injury to slowly frozen erythrocytes.

When cells are frozen slowly in aqueous suspensions, the solutes in the suspending solution concentrate as the amount of ice increases; the cells undergo osmotic dehydration and are sequestered in ever-narrowing liquid-filled channels. Cryoprotective solutes, such as glycerol, reduce the amount of ice that forms at any specified subzero temperature, thereby controlling the buildup in concentration of those other solutes present, as well as increasing the volume of the channels that remain to accommodate the cells. It has generally been thought that freezing injury is mediated by the increase in electrolyte concentration in the milieu surrounding the cells, rather than reduction of temperature or any direct action of ice. In this study we have frozen human erythrocytes in isotonic solutions of sodium chloride and glycerol and have demonstrated a correlation between the extent of damage at specific subzero temperatures, and that caused by the action at 0 degrees C of solutions having the same composition as those produced by freezing. The cell lysis observed increased directly with glycerol concentration, both in the freezing experiments and when the cells were exposed to corresponding solutions at 0 degrees C, showing that the concentration of sodium chloride alone is not sufficient to account quantitatively for the damage observed. We then studied the effect of freezing in anisotonic solutions to break the fixed relationship between solute concentration and the volume of the unfrozen fraction, as described by Mazur, P., W. F. Rall, and N. Rigopoulos (1981. Biophys. J. 653-675). We confirmed their experimental findings, but we explain them differently. We ascribe the apparently dominant effect of the unfrozen fraction to the fact that the cells were frozen in, and returned to, anisotonic solutions in which their volume was either less than, or greater than, their physiological volume. When similar cell suspensions were subjected to a similar cycle of increase and then decrease in solution strength, but in the absence of ice (at 20 degrees C), a similar pattern of hemolysis was observed. We conclude that freezing injury to human erythrocytes is due solely to changes that occur in the composition of their surrounding milieu, and is most probably mediated by a temporary leak in the plasma membrane that occurs during the thawing (reexpansion) phase.     

Roles of unfrozen fraction, salt concentration, and changes in cell volume in the survival of frozen human erythrocytes

The cause of slow freezing injury and the basis of the protection by solutes like glycerol are subjects of debate. During slow freezing, cells are sequestered in unfrozen channels between ice crystals that grow by removing pure water from the channels. As a consequence, the solute concentration in the channels rises and the volume of liquid in the channels progressively decreases. The rise in solute concentration, in turn, causes the cells to progressively shrink osmotically. Until recently cryobiologists have ascribed slow freezing injury to either the rise in solute (electrolyte) concentrations in the channels or to the consequent cell shrinkage, rather than to the decrease in the of the channels. Although ordinarily reciprocally coupled, it is possible to separate the composition of the channels from their size, or more precisely from the magnitude of the unfrozen fraction, by suspending cells in NaCl/cryoprotectant solutions in which the mole ratio of the two is held constant, but the molality of the NaCl is allowed to vary below and above isotonic. When human red cells are frozen in such solutions to temperatures that produce given NaCl concentrations (ms), but varying unfrozen fractions (U), survival at low U is found to be strongly dependent on U but independent of ms. At higher values of U, survival becomes inversely dependent on both ms and U. Although cell volume during freezing is independent of the NaCl tonicity in the solution, the cells in the several solutions differ in volume both prior to the onset of freezing and after the completion of thawing. We have now examined and compared the effect of returning the thawed cells to isotonic solutions and isotonic volume or nearly so, and find that there is little change in survival after exposure to low U, but that survival after exposure to high U values exhibits substantially increased sensitivity to ms, a sensitivity that is probably a manifestation of posthypertonic hemolysis. Low values of U were in general attained by the use of solutions with low tonicities of NaCl, and as a consequence cells frozen to low U values had larger volumes prior to freezing than cells frozen to higher U values. The significance of this confounding is discussed.     

Intracellular ice formation in mouse oocytes subjected to interrupted rapid cooling

The formation of ice crystals within cells (IIF) is lethal. The classical approach to avoiding it is to cool cells slowly enough so that nearly all their supercooled freezable water leaves the cell osmotically before they have cooled to a temperature that permits IIF. An alternative approach is to cool the cell rapidly to just above its ice nucleation temperature, and hold it there long enough to permit dehydration. Then, the cell is cooled rapidly to -70 degrees C or below. This approach, often called interrupted rapid cooling, is the subject of this paper. Mouse oocytes were suspended in 1.5M ethylene glycol (EG)/PBS, rapidly cooled (50 degrees C/min) to -25 degrees C and held for 5, 10, 20, 30, or 40 min before being rapidly cooled (50 degrees C/min) to -70 degrees C. In cells held for 5 min, IIF (flashing) occurred abruptly during the second rapid cool. As the holding period was increased to 10 and 20 min, fewer cells flashed during the cooling and more turned black during warming. Finally, when the oocytes were held 30 or 40 min, relatively few flashed during either cooling or warming. Immediately upon thawing, these oocytes were highly shrunken and crenated. However, upon warming to 20 degrees C, they regained most of their normal volume, shape, and appearance. These oocytes have intact cell membranes, and we refer to them as survivors. We conclude that 30 min at -25 degrees C removes nearly all intracellular freezable water, the consequence of which is that IIF occurs neither during the subsequent rapid cooling to -70 degrees C nor during warming.     

Sugars exert a major influence on the vitrification properties of ethylene glycol-based solutions and have low toxicity to embryos and oocytes

A systematic approach was taken to assess the vitrification properties of ethylene glycol-based solutions supplemented with carbohydrates. Solutions were prepared by weight (gravimetrically) using ethylene glycol as the cryoprotectant, 0.9% NaCl in water, and six different sugars: d-glucose, d(-)-fructose, d-sorbitol, sucrose, d(+)-trehalose, and raffinose. Sugars were added on a molal basis (0. 1, 0.5, and 1 m). Characteristics of the solutions were measured during warming by differential scanning calorimetry using a cooling rate of 100 degrees C/min and a warming rate of 10 degrees C/min. In the absence of carbohydrates a 59 wt% EG-saline solution formed a stable glass. When EG was replaced by an equimolal concentration of glucose, fructose, or sorbitol (monosaccharides) at 0.1, 0.5, or 1.0 m there was no change in the total solute concentration at which vitrification occurred, but the glass transition (Tg) occurred at a higher temperature than in EG-saline alone. When EG was replaced by an equimolal concentration of sucrose or trehalose (disaccharides) both the Tg and the lowest total solute concentration required for vitrification became progressively higher as the molecular weight, or the ratio of sugar to EG in the solutions, increased. At the highest tested disaccharide concentration (1 m) vitrification was achieved at a total solute concentration of 65 wt% (sucrose) and 67 wt% (trehalose). The polysaccharide raffinose significantly modified the vitrification properties of ethylene glycol solutions. When 0.5 or 0.1 m raffinose replaced EG on an equimolal basis the glass transition point was raised more than with either the monosaccharides or the disaccharides. Raffinose allowed vitrification at a total solute concentration of 67 wt% (0.5 m) and 63 wt% (0.1 m). The maturation of immature mouse oocytes, and the development of embryos in media containing 5-7 mM of any sugar was comparable to controls, indicating that they are not toxic. Exposure of freshly collected GV or MII oocytes to sugar concentrations between 0.5 and 1.0 M, for up to 10 min had no significant effect on the proportion which subsequently formed two cells. We conclude that added sugars do contribute to a solutions overall vitrification properties, and their properties should be taken into consideration when vitrification solutions are being designed or modified.     

Effect of warming rate on the survival of vitrified mouse oocytes and on the recrystallization of intracellular ice

Successful cryopreservation demands there be little or no intracellular ice. One procedure is classical slow equilibrium freezing, and it has been successful in many cases. However, for some important cell types, including some mammalian oocytes, it has not. For the latter, there are increasing attempts to cryopreserve them by vitrification. However, even if intracellular ice formation (IIF) is prevented during cooling, it can still occur during the warming of a vitrified sample. Here, we examine two aspects of this occurrence in mouse oocytes. One took place in oocytes that were partly dehydrated by an initial hold for 12 min at -25 degrees C. They were then cooled rapidly to -70 degrees C and warmed slowly, or they were warmed rapidly to intermediate temperatures and held. These oocytes underwent no IIF during cooling but blackened from IIF during warming. The blackening rate increased about 5-fold for each five-degree rise in temperature. Upon thawing, they were dead. The second aspect involved oocytes that had been vitrified by cooling to -196 degrees C while suspended in a concentrated solution of cryoprotectants and warmed at rates ranging from 140 degrees C/min to 3300 degrees C/min. Survivals after warming at 140 degrees C/min and 250 degrees C/min were low (<30%). Survivals after warming at > or =2200 degrees C/min were high (80%). When warmed slowly, they were killed, apparently by the recrystallization of previously formed small internal ice crystals. The similarities and differences in the consequences of the two types of freezing are discussed.     

Relative influence of unfrozen fraction and salt concentration on the survival of slowly frozen eight-cell mouse embryos

This laboratory has previously reported that the survival of frozen-thawed human erythrocytes is determined more by the fraction of the extracellular solution that remains unfrozen than by the salt concentration in that fraction, especially when the cells are frozen at low hematocrit. To determine the extent to which these findings are applicable to nucleated mammalian cells, we have studied the survival of some 3300 mouse embryos as a function of the unfrozen fraction and the concentration of salt in that unfrozen fraction. Also varied in the study was the weight percentage ratio of glycerol to salt. The concentration of embryos in these experiments (i.e., the cytocrit) was so low that embryo-embryo contacts should have been rare during the freezing. As in the case of the red cells at low hematocrit, we find that the survival of slowly frozen eight-cell embryos is not affected by the high concentrations of salt produced by freezing, at least up to 3.3 molal NaCl, and therefore is not affected by the extent to which the cells shrink below their isotonic volume, nor in general is survival influenced by the temperature at which given salt concentrations and unfrozen fractions are attained or by the glycerol concentration at those temperatures. On the other hand, the attainment of low values of the unfrozen fraction (U) is damaging, but the damage appears in part to be due to the fact that low values of U had to be achieved by placing embryos in solutions hypotonic with respect to NaCl, which caused their volume to be greater than isotonic prior to freezing.     

Influence of cell concentration on the contribution of unfrozen fraction and salt concentration to the survival of slowly frozen human erythrocytes

We have shown previously that the survival of human red blood cells during slow freezing at 2% hematocrit is dependent more on the magnitude of the unfrozen fraction than on the salt concentration in that unfrozen fraction. In parallel, first Nei and more recently Pegg and colleagues have shown that survival is affected by the hematocrit of the suspension. Freezing at hematocrits above 30% becomes increasingly damaging. The present studies were designed to see whether there is a link between the two phenomena. Cells were suspended at nominal hematocrits of 0.4, 2, 8, 40, or 60% in five test solutions of glycerol-NaCl. The test solutions were of such composition that when frozen to a specified temperature, the magnitude of the unfrozen fraction differed but the NaCl concentration (ms) remained constant. At low hematocrits (0.4 to 8%), red cell survival was dependent predominantly on the unfrozen fraction and was relatively independent of the salt concentration in that fraction. This we term the "rheological" effect because injury appears to be related to interaction with the ice walls and perhaps is due to shearing forces or cell deformation. But at high hematocrits (40 or 60%), cell survival became dependent on both the unfrozen fraction and the salt concentration in that fraction. When freezing occurs at high hematocrits, increasing numbers of cells are presumably brought into contact with their neighbors. Furthermore, they are increasingly shrunken cells, for the progressive removal of liquid water, which is responsible for the crowding, also causes a rise in ms and the consequent osmotic shrinkage of cells. Our data suggest that at unfrozen fractions above those producing injurious rheological forces, the tight packing of less shrunken cells (i.e., high hematocrit, low ms) and the extensive shrinking of loosely packed cells (high ms, low hematocrit) are both quite innocuous. Injury becomes substantial only when extensively shrunken cells are brought into close contact (i.e., high ms, high hematocrit). At high hematocrit the cells occupy a substantial fraction of the unfrozen space, and the water that they lose during slow freezing adds substantially to the volume of extracellular ice. Accordingly, we defined other measures of unfrozen fraction that include these perturbations. However, we found that the conclusions on the relation between survival, unfrozen fraction, and hematocrit were not affected by the method of expressing the unfrozen fraction. Freezing at high hematocrit to high ms and low values of unfrozen fraction is one way to produce contact between shrunken cells at low temperatures.(ABSTRACT TRUNCATED AT 400 WORDS)     

Performance of a kinetic model for intracellular ice formation based on the extent of supercooling.

Cryomicroscopy was used to study the incidence of intracellular ice formation (IIF) in protoplasts isolated from rye (Secale cereale) leaves during subfreezing isothermal periods and in in vitro mature bovine oocytes during cooling at constant rates. IIF in protoplasts occurred at random times during isothermal periods, and the kinetics of IIF were faster as isothermal temperature decreased. Mean IIF times decreased from approximately 1700 s at -4.0 degrees C to less than 1 s at -18.5 degrees C. Total incidence of IIF after 200 s increased from 4% at -4.0 degrees C to near 100% at -15.5 degrees C. IIF behavior in protoplasts was qualitatively similar to that for Drosophila melanogaster embryos over the same temperature ranges (Myers et al., Cryobiology 26, 472-484, 1989), but the kinetics of IIF were about five times faster in protoplasts. IIF observations in linear cooling of bovine oocytes indicated a median IIF temperature of -11 degrees C at 16 degrees C/min and total incidences of 97%, 50%, and 19% at 16, 8, and 4 degrees C/min, respectively. A stochastic model of IIF was developed which preserved certain features of an earlier model (Pitt et al. Cryobiology 28, 72-86, 1991), namely Weibull behavior in IIF temperatures during rapid linear cooling, but with a departure from the concept of a supercooling tolerance. Instead, the new model uses the osmotic state of the cell, represented by the extent of supercooling, as the independent variable governing the kinetics of IIF. Two kinetic parameters are needed for the model: a scale factor tau 0 dictating the sensitivity to supercooling, and an exponent rho dictating the strength of time dependency. The model was fit to the data presented in this study as well as those from Myers et al. and Pitt et al. for D. melanogaster embryos with and without cryoprotectant, and from Toner et al. (Cryobiology 28, 55-71, 1991) for mouse oocytes. In protoplasts, D. melanogaster embryos, and mouse oocytes, the parameters were estimated from IIF times in the early stages of isothermal periods, while the osmotic state of the cell was relatively constant. In bovine oocytes, the parameters were estimated from linear cooling data. Without further calibration, the model was used to predict total IIF incidence under different cooling regimes. For protoplasts, D. melanogaster embryos, and bovine oocytes, the model's predictions were quite accurate compared to the actual data. In mouse oocytes, adjustment of the hydraulic permeability coefficient (Lp) at 0 degree C was required to yield realistic behavior.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effect of cryoprotectants and their concentration on in vitro development of vitrified-warmed immature oocytes in buffalo (Bubalus bubalis)

Experiments were conducted to study the effect of cryoprotectants, dimethyl sulfoxide (DMSO), ethylene glycol (EG), 1,2-propanediol (PROH), and glycerol at different concentrations (3.5, 4, 5, 6, and 7 M each with 0.5 M sucrose and 0.4% BSA in DPBS) on survival, in vitro maturation, in vitro fertilization, and post-fertilization development of vitrified-thawed immature buffalo oocytes. The COCs were harvested from the ovaries by aspirating the visible follicles. The recovery of post-thaw morphologically normal oocytes was lower in 3.5 and 4 M DMSO, EG, and PROH compared to 5, 6, and 7 M. In all the concentrations of glycerol, an overall lower numbers of oocytes recovered were normal compared to other cryoprotectants. Less number of oocytes reached metaphase-II (M-II) stage from the oocytes cryopreserved in any of the concentrations of DMSO, EG, PROH, and glycerol compared to fresh oocytes. Among the vitrified groups, highest maturation was obtained in 7 M solutions of all the cryoprotectants. The cleavage rates of oocytes vitrified in different concentrations of DMSO, EG, PROH, and glycerol were lower than that of the fresh oocytes. The cleavage rates were higher in oocytes cryopreserved in 6 and 7 M DMSO, EG, PROH, and glycerol compared with oocytes cryopreserved in other concentrations. However, the percentage of morula and blastocyst formation from the cleaved embryos did not vary in fresh oocytes and vitrified oocytes. In conclusion, this report describes the first successful production of buffalo blastocysts from immature oocytes cryopreserved by vitrification.     

Temperature dependence of the survival of human erythrocytes frozen slowly in various concentrations of glycerol.

One widely accepted explanation of injury from slow freezing is that damage results when the concentration of electrolyte reaches a critical level in partly frozen solutions during freezing. We have conducted experiments on human red cells to further test this hypothesis. Cells were suspended in phosphate-buffered saline containing 0-3 M glycerol, held for 30 min at 20 degrees C to permit solute permeation, and frozen at 0.5 or 1.7 degrees C/min to various temperatures between -2 and -100 degrees C. Upon reaching the desired minimum temperature, the samples were warmed at rates ranging from 1 to 550 degrees C/min and the percent hemolysis was determined. The results for a cooling rate of 1.7 degrees C/min indicate the following: (a) Between 0.5 and 1.85 M glycerol, the temperature yielding 50% hemolysis (LT50) drops slowly from -18 to -35 degrees C. (b) The LT50's over this range of concentrations are relatively independent of warming rate. (c) With glycerol concentrations of 1.95 and 2.0 M, the LT50 drops abruptly to -60 degrees C and to below -100 degrees C, respectively, and becomes dependent on warming rate. The LT50 is lower with slow warming at 1 degree C/min than with rapid. With still higher concentrations (2.5 and 3.0 M), there is no LT50, i.e., more than 50% of the cells survive freezing to-100 degrees C. Results for cooling at 0.5 degrees C/min in 2 M glycerol were similar except that the LT50s were some 10-20 degrees C higher. A companion paper (Rall et al., Biophys. J. 23:101-120, 1978) examines the relation between survival and the concentrations of salts produced during freezing.     

Toxicity and protective efficiency of cryoprotectants to flounder (Paralichthys olivaceus) embryos

With the purpose of finding an ideal cryoprotectant or combination of cryoprotectants in a suitable concentration for flounder (Paralichthys olivaceus) embryo cryopreservation, we tested the toxicities, at culture temperature (16 degrees C), of five most commonly used cryoprotectants-dimethyl sulfoxide (Me2SO), glycerol, methanol (MeOH), 1,2-propylene glycol (PG) and ethylene glycol (EG). In addition, cryoprotective efficiency to flounder embryos of individual and combined cryoprotectants were tested at -15 degrees C for 60 min. Five different concentrations of each of the five cryoprotectants and 20 different combinations of these cryoprotectants were tested for their protective efficiency. The results showed that the toxicity to flounder embryos of the five cryoprotectants are in the following sequence: PG < MeOH < Me2SO < glycerol < EG (P < 0.05); whereas the protective efficiency of each cryoprotectant, at -15 degrees C for a period of 60 min, are in the following sequence: PG > Me2SO approximately MeOH approximately glycerol > EG (greater symbols mean P < 0.05, and approximate symbols mean P > 0.05). Methanol combined with any one of the other cryoprotectants gave the best protection, while ethylene glycol combined with any one of the other cryoprotectants gave the poorest protection at -15 degrees C. Toxicity effect was concentration dependent with the lowest concentration being the least toxic for all five cryoprotectants at 16 degrees C. For PG, MeOH and glycerol, 20% solutions gave the best protection at -15 degrees C; whereas a 15% solution of Me2SO, and a 10% solution of EG, gave the best protection at -15 degrees C.     

Starfish oocytes form intracellular ice at unusually high temperatures

Starfish oocytes, eggs, and embryos are popular models for studying meiotic maturation, fertilization, and embryonic development. Their large (170- to 200-microm) oocytes are obtainable in copious amounts and are amenable to manipulations that mammalian oocytes are not. The most formidable obstacle to working with marine oocytes is their seasonal availability, yet a successful means of preserving them for use during the nonreproductive season has not been reported. The aim of this study was to investigate the response of starfish oocytes to freezing with rapid and slow cooling rates under a variety of conditions to develop a cryopreservation protocol for these cells. Cryomicroscopic observation revealed that starfish oocytes in isotonic medium undergo intracellular ice formation (IIF) at very high subzero temperatures, such that the mean difference between the temperature of extracellular ice formation (T(EIF)) and IIF (TI(IF)) was less than 3 degrees C and the average T(IIF) was approximately between -4 and -6 degrees C. Neither partial cellular dehydration nor addition of the cryopreservative dimethyl sulfoxide significantly depressed the T(IIF). Under some conditions, we observed ice nucleation at multiple locations within the cytoplasm, suggesting that several factors contribute to the unusually high T(IIF) during controlled-rate freezing and thus vitrification may be a more suitable method for cryopreserving these cells.