Equilibrium,quasi-equilibrium,and nonequilibrium freezing of mammalian embryos

The first successful freezing of early embryos to −196°C in 1972 required that they be cooled slowly at ∼1°C/min to about −70°C. Subsequent observations and physical/chemical analyses indicate that embryos cooled at that rate dehydrate sufficiently to maintain the chemical potential of their intracellular water close to that of the water in the partly frozen extracellular solution. Consequently, such slow freezing is referred to as equilibrium freezing. In 1972 and since, a number of investigators have studied the responses of embryos to departures from equilibrium freezing. When disequilibrium is achieved by the use of higher constant cooling rates to −70°C, the result is usually intracellular ice formation and embryo death. That result is quantitatively in accord with the predictions of the physical/chemical analysis of the kinetics of water loss as a function of cooling rate. However, other procedures involving rapid nonequilibrium cooling do not result in high mortality. One common element in these other nonequilibrium procedures is that, before the temperature has dropped to a level that permits intracellular ice formation, the embryo water content is reduced to the point at which the subsequent rapid nonequilibrium cooling results in either the formation of small innocuous intracellular ice crystals or the conversion of the intracellular solution into a glass. In both cases, high survival requires that subsequent warming be rapid, to prevent recrystallization or devitrification. The physical/ chemical analysis developed for initially nondehydrated cells appears generally applicable to these other nonequilibrium procedures as well.     

Nonequilibrium freezing of one-cell mouse embryos. Membrane integrity and developmental potential.

A thermodynamic model was used to evaluate and optimize a rapid three-step nonequilibrium freezing protocol for one-cell mouse embryos in the absence of cryoprotectants (CPAs) that avoided lethal intracellular ice formation (IIF). Biophysical parameters of one-cell mouse embryos were determined at subzero temperatures using cryomicroscopic investigations (i.e., the water permeability of the plasma membrane, its temperature dependence, and the parameters for heterogeneous IIF). The parameters were then incorporated into the thermodynamic model, which predicted the likelihood of IIF. Model predictions showed that IIF could be prevented at a cooling rate of 120 degrees C/min when a 5-min holding period was inserted at -10 degrees C to assure cellular dehydration. This predicted freezing protocol, which avoided IIF in the absence of CPAs, was two orders of magnitude faster than conventional embryo cryopreservation cooling rates of between 0.5 and 1 degree C/min. At slow cooling rates, embryos predominantly follow the equilibrium phase diagram and do not undergo IIF, but mechanisms other than IIF (e.g., high electrolyte concentrations, mechanical effects, and others) cause cellular damage. We tested the predictions of our thermodynamic model using a programmable freezer and confirmed the theoretical predictions. The membrane integrity of one-cell mouse embryos, as assessed by fluorescein diacetate retention, was approximately 80% after freezing down to -45 degrees C by the rapid nonequilibrium protocol derived from our model. The fact that embryos could be rapidly frozen in the absence of CPAs without damage to the plasma membrane as assessed by fluorescein diacetate retention is a new and exciting finding. Further refinements of this protocol is necessary to retain the developmental competence of the embryos.     

Depression of the ice-nucleation temperature of rapidly cooled mouse embryos by glycerol and dimethyl sulfoxide.

The temperature at which ice formation occurs in supercooled cytoplasm is an important element in predicting the likelihood of intracellular freezing of cells cooled by various procedures to subzero temperatures. We have confirmed and extended prior indications that permeating cryoprotective additives decrease the ice nucleation temperature of cells, and have determined some possible mechanisms for the decrease. Our experiments were carried out on eight-cell mouse embryos equilibrated with various concentrations (0-2.0 M) of dimethyl sulfoxide or glycerol and then cooled rapidly. Two methods were used to assess the nucleation temperature. The first, indirect, method was to determine the in vitro survival of the rapidly cooled embryos as a function of temperature. The temperatures over which an abrupt drop in survival occurs are generally diagnostic of the temperature range for intracellular freezing. The second, direct, method was to observe the microscopic appearance during rapid cooling and note the temperature at which nucleation occurred. Both methods showed that the nucleation temperature decreased from - 10 to - 15 degrees C in saline alone to between - 38 degrees and - 44 degrees C in 1.0-2.0 M glycerol and dimethyl sulfoxide. The latter two temperatures are close to the homogeneous nucleation temperatures of the solutions in the embryo cytoplasm, and suggest that embryos equilibrated in these solutions do not contain heterogeneous nucleating agents and are not accessible to any extracellular nucleating agents, such as extracellular ice. The much higher freezing temperatures of cells in saline or in low concentrations of additive indicate that they are being nucleated by heterogeneous agents or, more likely, by extracellular ice.     

Microscopic observation of intracellular ice formation in unfertilized mouse ova as a function of cooling rate

A physical-chemical analysis of water loss from cells at subzero temperatures had shown that the likelihood of intracellular ice formation increased with increasing cooling rate (22). We have now used a modified version of a unique conductioncooled cryomicroscope stage (8) to observe the freezing of unfertilized mouse ova suspended in dimethyl sulfoxide. Survival measurements showed that the respective survivals of ova were about 65, 56, and 0% when they were cooled at rates of 0.2 to 1.5, 2.5, and 5.4 °C/min. Direct microscopic observation of mouse ova during freezing showed that the respective fractions of cells that froze intracellularly were 13, 72, and 100% when they were cooled at rates of 1.3, 2.9, and 4.8 °C/min or faster. These values agree with those predicted from the physical-chemical analysis for cells the size of mouse ova. The microscopic observations have also shown that intracellular freezing generally occurred at about ?40 to ?45 °C. We had previously observed that mouse embryos must be cooled slowly to ?50 °C or below if they are to survive subsequent rapid cooling to ?196 °C. The observation of intracellular ice formation at ?45 °C supports the interpretation that at temperatures above ?50 °C the embryos still contain water capable of freezing intracellularly.     

Effect of warming rate on mouse embryos frozen and thawed in glycerol

Mouse embryos (8-cell) fully equilibrated in 1.5 M-glycerol were cooled slowly (0.5 degrees C/min) to temperatures between - 7.5 and - 80 degrees C before rapid cooling and storage in liquid nitrogen (-196 degrees C). Some embryos survived rapid warming (approximately 500 degrees C/min) irrespective of the temperature at which slow cooling was terminated. However, the highest levels of survival of rapidly warmed embryos were observed when slow cooling was terminated between -25 and -80 degrees C (74-86%). In contrast, high survival (75-86%) was obtained after slow warming (approximately 2 degrees C/min) only when slow cooling was continued to -55 degrees C or below before transfer into liquid N2. Injury to embryos cooled slowly to -30 degrees C and then rapidly to -196 degrees C occurred only when slow warming (approximately 2 degrees C/min) was continued to -60 degrees C or above. Parallel cryomicroscopical observations indicated that embryos became dehydrated during slow cooling to -30 degrees C and did not freeze intracellularly during subsequent rapid cooling (approximately 250 degrees C/min) to -150 degrees C. During slow warming (2 degrees C/min), however, intracellular ice appeared at a temperature between -70 and -65 degrees C and melted when warming was continued to -30 degrees C. Intracellular freezing was not observed during rapid warming (250 degrees C/min) or during slow warming when slow cooling had been continued to -65 degrees C. These results indicate that glycerol provides superior or equal protection when compared to dimethyl sulphoxide against the deleterious effects of freezing and thawing.     

Rapidly cooled horse spermatozoa: loss of viability is due to osmotic imbalance during thawing, not intracellular ice formation

The cellular damage that spermatozoa encounter at rapid rates of cooling has often been attributed to the formation of intracellular ice. However, no direct evidence of intracellular ice has been presented. An alternative mechanism has been proposed by Morris (2006) that cell damage is a result of an osmotic imbalance encountered during thawing. This paper examines whether intracellular ice forms during rapid cooling or if an alternative mechanism is present. Horse spermatozoa were cooled at a range of cooling rates from 0.3 to 3,000 degrees C/min in the presence of a cryoprotectant. The ultrastructure of the samples was examined by Cryo Scanning Electron Microscopy (CryoSEM) and freeze substitution, to determine whether intracellular ice formed and to examine alternative mechanisms of cell injury during rapid cooling. No intracellular ice formation was detected at any cooling rate. Differential scanning Calorimetry (DSC) was employed to examine the amount of ice formed at different rate of cooling. It is concluded that cell damage to horse spermatozoa, at cooling rates of up to 3,000 degrees C/min, is not caused by intracellular ice formation. Spermatozoa that have been cooled at high rates are subjected to an osmotic shock when they are thawed.     

Is intracellular ice formation the cause of death of mouse sperm frozen at high cooling rates?

Mouse spermatozoa in 18% raffinose and 3.8% Oxyrase in 0.25 x PBS exhibit high motilities when frozen to -70 degrees C at 20-130 degrees C/min and then rapidly warmed. However, survival is <10% when they are frozen at 260 or 530 degrees C/min, presumably because, at those high rates, intracellular water cannot leave rapidly enough to prevent extensive supercooling and this supercooling leads to nucleation and freezing in situ (intracellular ice formation [IIF]). The probability of IIF as a function of cooling rate can be computed by coupled differential equations that describe the extent of the loss of cell water during freezing and from knowledge of the temperature at which the supercooled protoplasm of the cell can nucleate. Calculation of the kinetics of dehydration requires values for the hydraulic conductivity (Lp) of the cell and for its activation energy (Ea). Using literature values for these parameters in mouse sperm, we calculated curves of water volume versus temperature for four cooling rates between 250 and 2000 degrees C/min. The intracellular nucleation temperature was inferred to be -20 degrees C or above based on the greatly reduced motilities of sperm that underwent rapid cooling to a minimum temperature of between -20 and -70 degrees C. Combining that information regarding nucleation temperature with the computed dehydration curves leads to the conclusion that intracellular freezing should occur only in cells that are cooled at 2000 degrees C/min and not in cells that are cooled at 250-1000 degrees C/min. The calculated rate of 2000 degrees C/min for IIF is approximately eightfold higher than the experimentally inferred value of 260 degrees C/min. Possible reasons for the discrepancy are discussed.     

Nucleation and growth of ice crystals inside cultured hepatocytes during freezing in the presence of dimethyl sulfoxide.

A three-part, coupled model of cell dehydration, nucleation, and crystal growth was used to study intracellular ice formation (IIF) in cultured hepatocytes frozen in the presence of dimethyl sulfoxide (DMSO). Heterogeneous nucleation temperatures were predicted as a function of DMSO concentration and were in good agreement with experimental data. Simulated freezing protocols correctly predicted and explained experimentally observed effects of cooling rate, warming rate, and storage temperature on hepatocyte function. For cells cooled to -40 degrees C, no IIF occurred for cooling rates less than 10 degrees C/min. IIF did occur at faster cooling rates, and the predicted volume of intracellular ice increased with increasing cooling rate. Cells cooled at 5 degrees C/min to -80 degrees C were shown to undergo nucleation at -46.8 degrees C, with the consequence that storage temperatures above this value resulted in high viability independent of warming rate, whereas colder storage temperatures resulted in cell injury for slow warming rates. Cell damage correlated positively with predicted intracellular ice volume, and an upper limit for the critical ice content was estimated to be 3.7% of the isotonic water content. The power of the model was limited by difficulties in estimating the cytosol viscosity and membrane permeability as functions of DMSO concentration at low temperatures.     

Cryomicroscopic observations of cattle embryos during freezing and thawing

A cryomicroscope was used to observe changes in the appearance of day 6 1 2 to 7 1 2 cattle embryos during cooling and warming in 1.4M glycerol/PBS. Embryos were cooled at various rates between 0.2 and 25 degrees C/min to temperatures between -25 and -60 degrees C and then cooled rapidly ( approximately 250 degrees C/min) to temperatures below -140 degrees C. The volume of the embryos calculated from the cross-sectional area during slow cooling decreased at -25 degrees C to about 50% of the isotonic volume. Fracture planes could be observed in the extracellular ice matrix surrounding the embryos after rapid cooling to approximately -140 degrees C. The fracture planes often touched the zona pellucida and sometimes caused cracks in the zona. Cracks in the zona pellucida were observed more often after rapid cooling from temperatures between -20 to -35 degrees C (9 13 ) than from temperatures between -36 to -60 degrees C (2 7 ). When embryos were warmed rapidly ( approximately 250 degrees C/min) from temperatures below -140 degrees C, no change was observed in the appearance of either the embryo or its surroundings except the melting of the extracellular ice. However, when embryos were warmed slowly (2 or 5 degrees C/min), a series of events was observed; first, at approximately -70 degrees C the cytoplasm and the extracellular space gradually darkened and reached maximum darkness at approximately -55 degrees C. Then, on continued slow warming, the dark material gradually disappeared and finally the large extracellular ice crystals melted.     

Effect of cooling rate and partial removal of yolk on the chilling injury in zebrafish (Danio rerio) embryos

High chilling sensitivity is one of the main obstacles to successful cryopreservation of zebrafish embryos. So far the nature of the chilling injury in fish embryos has not been clear. The aim of this study is to investigate the effect of cooling rate and partial removal of yolk on chilling injury in zebrafish embryos. Zebrafish embryos at 64-cell, 50%-epiboly, 6-somite and prim-6 stages were cooled to either 0 degrees C or -5 degrees C at three different cooling rates: slow (0.3 degrees C/min or 1 degree C/min), moderate (30 degrees C/min), and rapid (approximately 300 degrees C/min). After chilling, embryos were warmed in a 26 degrees C water bath, followed by 3-day culturing in EM at 26 +/- 1 degrees C for survival assessment. When embryos were cooled to 0 degrees C for up to 30 min, 64-cell embryos had higher survival after rapid cooling than when they were cooled at a slower rate. When 64-cell embryos were held at -5 degrees C for 1 min, their survival decreased greatly after both slow and rapid cooling. The effect of cooling rate on the survival of 50%-epiboly and 6-somite embryos was not significant after 1 h exposure at 0 degrees C and 1 min exposure at -5 degrees C. However, rapid cooling resulted in significantly lower embryo survival than a cooling rate of 30 degrees C/min or 1 degree C/min after 1 h exposure to 0 degrees C for prim-6 stage or 1 h exposure to -5 degrees C for all stages. Chilling injury in 64-cell embryos appears to be a consequence of exposure time at low temperatures rather than a consequence of rapid cooling. Results also indicate that chilling injury in later stage embryos (50%-epiboly, 6-somite and prim-6) is a consequence of the combination of rapid cooling and exposure time at low temperatures. Dechorionated prim-6 embryos were punctured and about half of yolk was removed. After 24 h culture at 26 +/- 1 degrees C after removal of yolk, the yolk-reduced embryos showed higher embryo survival than did control embryos after rapid cooling to -5 degrees C for 10 to 60 min. Results suggest that cold shock injury after rapid cooling can be mitigated after partial removal of yolk at the prim-6 stage. These findings help us to understand the nature of chilling sensitivity of fish embryos and to develop protocols for their cryopreservation.     

Survival of frozen mouse embryos after rapid thawing from -196 degrees C.

The effect of the rate of rewarming on the survival of 8-cell mouse embryos and blastocysts was examined. The samples were slowly cooled (0.3--0.6 degrees C/min) in 1.5 M-DMSO to temperatures between -10 and -80 degrees C before direct transfer to liquid nitrogen (-196 degrees C). Embryos survived rapid thawing (275--500 degrees C/min) only when slow cooling was terminated at relatively high subzero temperatures (-10 to -50 degrees C). The highest levels of survival in vitro of rapidly thawed 8-cell embryos were obtained after transfer to -196 degrees C from -35 and -40 degrees C (72 to 88%) and of rapidly thawed blastocysts after transfer from -25 to -50 degrees C (69 to 74%). By contrast, for embryos to survive slow thawing (8 to 20 degrees C/min) slow cooling to lower subzero temperatures (-60 degrees C and below) was required before transfer to -196 degrees C. The results indicate that embryos transferred to -196 degrees C from high subzero temperatures contain sufficient intracellular ice to damage them during slow warming but to permit survival after rapid warming. Survival of embryos after rapid dilution of DMSO at room temperature was similar to that after slow (stepwise) dilution at 0 degrees C. There was no difference between the viability of rapidly and slowly thawed embryos after transfer to pseudopregnant foster mothers. It is concluded that the behaviour of mammalian embryos subjected to the stresses of freezing and thawing is similar to that of other mammalian cells. A simpler and quicker method for the preservation of mouse embryos is described.     

Status of cryopreservation of embryos from domestic animals.

The discovery of glycerol as an effective cryoprotectant for spermatozoa led to research on cryopreservation of embryos. The first successful offspring from frozen-thawed embryos were reported in the mouse and later in other laboratory animals. Subsequently, these techniques were applied to domestic animals. Research in cryopreservation techniques have included studies concerning the type and concentration of cryoprotectant, cooling and freezing rates, seeding and plunging temperatures, thawing temperatures and rates, and methods of cryoprotectant removal. To date, successful results based on pregnancy rates have been obtained with cryopreserved cow, sheep, goat, and horse embryos but no success has been reported in swine. Post-thaw embryo survival has been shown to be dependent on the initial embryo quality, developmental stage, and species. The freezing techniques most frequently used in research and by commercial companies are identified as "equilibrium" cryopreservation. In this technique the embryos are placed in a concentrated glycerol solution (1.4 M in PBS supplemented with BSA) at room temperature and the glycerol is allowed to equilibrate for a 20-min period. During the cooling process the straws are seeded (-4 to -7 degrees C) and cooling is continued at a rate of 0.3 to 0.5 degree C/min to -30 degrees C when bovine embryos may be plunged into LN2. Sheep embryos are successfully frozen with ethylene glycol (1.5 M) or DMSO (1.5 M) rather than with glycerol. Horse embryos have been frozen in 0.5 rather than 0.25 cc straws but with cooling rates and seeding and plunging temperatures similar to those used with bovine embryos. Swine embryos have shown a high sensitivity to temperature and cryoprotectants probably due to their high lipid content and a temperature decrease to 15 or 10 degrees C causes a dramatic increase in the percentage of degenerated embryos. However, a recent study has shown that hatched pig blastocysts survived exposure below 15 degrees C. Recent research has shown that embryos may also be frozen by a "nonequilibrium" method. This rapid freezing by vitrification consists of dehydration of the embryo at room temperature by a very highly concentrated vitrification media (3.5 to 4.0 M) and a very rapid freeze that avoids the formation of ice allowing the solution to change from a liquid to a glassy state. Vitrification solutions consist of combinations of sucrose, glycerol, and propylene glycol. With this technique, 50% pregnancy rates have been reported with the bovine blastocyst.     

Protective effect of intracellular ice during freezing?

Injury results during freezing when cells are exposed to increasing concentrations of solutes or by the formation of intracellular ice. Methods to protect cells from the damaging effects of freezing have focused on the addition of cryoprotective chemicals and the determination of optimal cooling rates. Based on other studies of innocuous intracellular ice formation, this study investigates the potential for this ice to protect cells from injury during subsequent slow cooling. V-79W Chinese hamster fibroblasts and Madin-Darby Canine Kidney (MDCK) cells were cultured as single attached cells or confluent monolayers. The incidence of intracellular ice formation (IIF) in the cultures at the start of cooling was pre-determined using one of two different extracellular ice nucleation temperatures (-5 or -10 degrees C). Samples were then cooled at 1 degrees C/min to the experimental temperature (-5 to -40 degrees C) where samples were warmed rapidly and cell survival assessed using membrane integrity and metabolic activity. For single attached cells, the lower ice nucleation temperature, corresponding to increased incidence of IIF, resulted in decreased post-thaw cell recovery. In contrast, confluent monolayers in which IIF has been shown to be innocuous, show higher survival after cooling to temperatures as low as -40 degrees C, supporting the concept that intracellular ice confers cryoprotection by preventing cell dehydration during subsequent slow cooling.     

Mechanism of cryoprotection by extracellular polymeric solutes.

To elucidate the means by which polymer solutions protect cells from freezing injury, we cooled human monocytes to -80 degrees C or below in the presence of various polymers. Differential scanning calorimetric studies showed that those polymers which protect cells best have a limiting glass transition temperature (T'g) of approximately -20 degrees C; those with a T'g significantly higher or lower did not protect. Freeze-etch electron micrographs indicated that intracellular ice crystals had formed during this freezing procedure, but remained smaller than approximately 300 nm in the same proportion of cells as survived rapid thawing. We propose that cryoprotection of slowly frozen monocytes by polymers is a consequence of a T'g of -20 degrees C in the extracellular solution. In our hypothesis, the initial concentration and viscosity of protective polymer solutions reduce the extent and rate of cell water loss to extracellular ice and limit the injurious osmotic stress, which cells face during freezing at moderate rates to -20 degrees C. Below -20 degrees C, glass formation prevents further osmotic stress by isolating cells from extracellular ice crystals, virtually eliminating cell water loss at lower temperatures. On the other hand, the protective polymer solutions will allow some diffusion of water away from cells at temperatures above T'g. If conditions are correct, cells will concentrate the cytoplasm sufficiently during the initial cooling to T'g to avoid lethal intracellular freezing between T'g and the intracellular Tg, which has been depressed to low temperatures by that concentration. Thus, when polymers are used as cryoprotective agents, cell survival is contingent upon maintenance of osmotic stress within narrow limits.     

Stabilization of frozen Lactobacillus delbrueckii subsp. bulgaricus in glycerol suspensions: Freezing kinetics and storage temperature effects

The interactions between freezing kinetics and subsequent storage temperatures and their effects on the biological activity of lactic acid bacteria have not been examined in studies to date. This paper investigates the effects of three freezing protocols and two storage temperatures on the viability and acidification activity of Lactobacillus delbrueckii subsp. bulgaricus CFL1 in the presence of glycerol. Samples were examined at -196 degrees C and -20 degrees C by freeze fracture and freeze substitution electron microscopy. Differential scanning calorimetry was used to measure proportions of ice and glass transition temperatures for each freezing condition tested. Following storage at low temperatures (-196 degrees C and -80 degrees C), the viability and acidification activity of L. delbrueckii subsp. bulgaricus decreased after freezing and were strongly dependent on freezing kinetics. High cooling rates obtained by direct immersion in liquid nitrogen resulted in the minimum loss of acidification activity and viability. The amount of ice formed in the freeze-concentrated matrix was determined by the freezing protocol, but no intracellular ice was observed in cells suspended in glycerol at any cooling rate. For samples stored at -20 degrees C, the maximum loss of viability and acidification activity was observed with rapidly cooled cells. By scanning electron microscopy, these cells were not observed to contain intracellular ice, and they were observed to be plasmolyzed. It is suggested that the cell damage which occurs in rapidly cooled cells during storage at high subzero temperatures is caused by an osmotic imbalance during warming, not the formation of intracellular ice.     

Enhanced survival of yeast expressing an antifreeze gene analogue after freezing.

Yeast, like most organisms, survives poorly under freezing conditions. It has been proposed that after rapid cooling yeast suffers a loss in viability from the recrystallization of intracellular ice. Antifreeze proteins found in the blood of certain polar fishes have been shown to be potent inhibitors of ice recrystallization at very low concentrations. We have examined the feasibility of protecting rapidly cooled yeast cells from freezing damage by inhibiting the recrystallization of intracellular ice through in vivo expression of an antifreeze analogue gene. A chemically synthesized gene encoding a protein similar to but differing from the antifreeze proteins of the fish Pseudopleuronectes americanus (winter flounder) was genetically fused to the 3' end of a truncated staphylococcal Protein A gene. When the fused gene was expressed in the budding yeast Saccharomyces cerevisiae, its cells were shown to produce a new chimeric protein that inhibited the recrystallization of ice in vitro. Yeast cells expressing the chimeric antifreeze protein showed a twofold increase in survival after rapid freezing (95 degrees C/min to -196 degrees C) and moderate rates of warming (26 to 64 degrees C/min) compared to cells lacking the chimeric protein.     

Effect of silver iodide as an ice inducer on viability of frozen-thawed rabbit morulae

A new method was devised for inducing ice crystal formation in extracellular solution using silver iodide. A latent heat occurred immediately before temperature of sample reached -7 degrees C, when a column 70 mm high of 1.5M dimethyl sulfoxide (the freezing solution, FS) was aspirated into a plastic straw followed by 3 mm high of air and 10 mm high of 1% suspension of silver iodide in distilled water (1% AgI). To examine the effect of silver iodide as an inducer of ice crystal formation in extracellular solution on in vitro development of frozen-thawed rabbit morulae, the straws were filled by successive aspiration of the following fractions: 175 mul of FS containing the embryos, 7.5 mul of air, 25 mul of 1% AgI. The straws were cooled to -7 degrees C at 1 degrees C/min, and held at -7 degrees C for 10 min without initiating seeding; they were then cooled again to -30 degrees C at 1 degrees C/min and plunged into liquid nitrogen. After rapid thawing (>1000 degrees C/min), 100 of 109 (92%) embryos that were recovered developed into expanding blastocysts.     

Effect of cooling and warming rates during cryopreservation on survival of in vitro-produced bovine embryos

The effect of cooling and warming rates during cryopreservation on subsequent embryo survival was studied in 607 bovine morulae and 595 blastocysts produced by in vitro maturation, fertilization and culture (IVM/IVF/IVC). Morulae and blastocysts were prepared by co-culturing presumptive zygotes with bovine oviductal epithelial cells (BOEC) in serum-free TCM199 medium for 6 and 7 d, respectively. The embryos in 1.5 M ethylene glycol in plastic straws were seeded at -7 degrees C, cooled to -35 degrees C at each of 5 rates (0.3 degrees, 0.6 degrees , 0.9 degrees, 1.2 degrees, or 1.5 degrees C/min) and then immediately plunged into liquid nitrogen. The frozen embryos were warmed either rapidly in a 35 degrees C water bath (warming rate > 1,000 degrees C/min) or slowly in 25 degrees to 28 degrees C air (< 250 degrees C/mm). With rapid warming, 42.1% of the morulae that had been cooled at 0.3 degrees C/min developed into hatching blastocysts. The proportions of rapidly wanned morulae that hatched decreased with increasing cooling rates (30.4, 19.0, 15.8 and 8.9% at 0.6 degrees , 0.9 degrees, 1.2 degrees and 1.5 degrees C/min, respectively). With slow warming 25.9% of the morulae that had been cooled at 0.3 degrees C/min developed into hatching blastocysts, while <10% of the morulae that had been cooled faster developed. The hatching rate of blastocysts cooled at 0.3 degrees C/min and warmed rapidly (96.3%) was higher than those cooled at 06 degrees and 0.9 degrees C/min (82.7 and 84.6%, respectively), and was also significantly higher than those warmed slowly after cooling at 0.3 degrees, 0.6 degrees or 0.9 degrees C/min (69.1, 56.6 and 51.8%, respectively). Cooling blastocysts at 1.2 degrees or 1.5 degrees C/min resulted in lowered hatching rates either with rapid (71.2 or 66 0%) or slow warming (38.2 or 38.9%). These results indicate that the survival of in vitro-produced bovine morulae and blastocysts is improved by very slow cooling during 2-step freezing, nevertheless, slow warming appears to cause injuries to morulae and blastocysts even after very slow cooling.     

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.     

Quantitative study of the importance of water permeability in plant cold hardiness

The rate of ice formation was measured for Hedera helix L. cv. Thorndale (English ivy) bark exposed to -10 C. The cooling rate of bark exposed to -10 C was 31 C per minute. The water efflux rate required for ice formation to occur extracellularly was calculated from the rate of ice formation and the average cell diameter. The water potential difference driving the efflux of water to sites of extracellular ice was calculated from the sample temperature, osmotic water potential, and fraction of water frozen at a given freezing temperature. From the water efflux rate and water potential difference, the resistance of the barrier controlling movement of intracellular water to sites of extracellular ice was calculated. Comparison of the resistance of this barrier to water movement with the resistance of the cell membrane revealed that the membrane represented only 0.5% of the barrier resistance. Thus, membrane resistance can have little influence on the rate of water efflux and ice formation when bark is cooled at a rate of 31 C per minute. If ice formation occurred at the same rate in ivy bark as it occurred in a 10 mm MnCl(2) solution, the membrane resistance would still have represented only 1% of the resistance of the barrier to ice formation. Therefore, at a cooling rate of 31 C/minute, heat removal plays a large part in determining the rate of ice formation. At slower cooling rates experienced under natural freezing conditions the ability to remove heat would play an even larger role. It is concluded that under natural freezing conditions membrane resistance does not limit water efflux.