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.     

Membrane leakage of solutes after thermal shock or freezing

Washed human erythrocytes were cooled at different rates from +37 °C to 0 °C in hypertonic solutions of either NaCl (1.2 m) or of a mixture of sucrose (40% $\text{w}\text{v}$) with NaCl (2.53% $\text{w}\text{v}$). Thermal shock hemolysis was measured and the surviving cells were examined for their mass and cell water content and also for net movements of sodium, potassium, and ¹⁴C-sucrose. The results were compared with those obtained from cells in sucrose (40% $\text{w}\text{v}$) initially, cooled at different rates to ?196 °C and rapidly thawed.The cells cooled to 0 °C in NaCl (1.2 m) showed maximal hemolysis at the fastest cooling rate studied (39 °C/min). In addition in the surviving cells this cooling rate induced the greatest uptake of ¹⁴C-sucrose and increase in cell water and cell mass and also entry of sodium and loss of cell potassium. A different dependence on cooling rate was seen with the cells cooled from +37 °C to 0 °C in sucrose (40% $\text{w}\text{v}$) with NaCl (2.53% $\text{w}\text{v}$). In this solution, survival decreased both at slow and fast cooling rates correlating with the greatest uptake of cell sucrose and increase in cell water. There was extensive loss of cell potassium and uptake of sodium at all cooling rates, the cation concentrations across the cell membrane approaching unity.The cells frozen to ?196 °C at different cooling rates in sucrose (40% $\text{w}\text{v}$) initially, also showed sucrose and water entry on thawing together with a loss of cell potassium and an uptake of cell sodium. More sucrose entered the cells cooled slowly (1.8 ° C/min) than those cooled rapidly (318 ° C/min).These results show that cooling to 0 °C in hypertonic solutions (thermal shock) and freezing to ?196 °C both induce membrane leaks to sucrose as well as to sodium and potassium. These leaks are not induced by the hypertonic solutions themselves but are due to the effects of the added stress of the temperature reduction on the membranes modified by the hypertonic solutions. The effects of cooling rate are explicable in terms of the different times of exposure to the hypertonic solutions. These results indicate that the damage observed after thermal shock or slow freezing is of a similar nature.     

Intracellular freezing: effect of extracellular supercooling.

Human erythrocytes were frozen on the stage of a cryomicroscope at accurately controlled constant-cooling rates with varying degrees of extracellular supercooling. The formation of intracellular ice was detected by direct observation of the frozen cells through the microscope. A significant coupling effect was determined between the minimum cooling rate necessary to produce intracellular freezing and the extent of supercooling. Increased degrees of extracellular supercooling reduced the range of cooling rates for which water would freeze within the cell. Specific data points were obtained at ΔT_SC = 0, ?5, and ?12 °C for which the corresponding transition cooling rates were respectively ?845, ?800, and ?11 °C/min.An explanation for the occurrence of this phenomenon is presented based on the physiochemical processes that govern the freezing of a cell suspension.     

Kinetics of water loss and the likelihood of intracellular freezing in mouse ova

To avoid intracellular freezing and its usually lethal consequences, cells must lose their freezable water before reaching their ice-nucleation temperature. One major factor determining the rate of water loss in the temperature dependence of the water permeability,L _p (hydraulic conductivity). Because of the paucity of water permeability measurements at subzero temperatures, that temperature dependence has usually been extrapolated from above-zero measurements. The extrapolation has often been based on an exponential dependence ofL _p on temperature. This paper compares the kinetics of water loss based on that extrapolation with that based on an Arrhenius relation betweenL _p and temperature, and finds substantial differences below ?20 to ?25°C. Since the ice-nucleation temperature of mouse ova in the cryoprotectants DMSO and glycerol is usually below ?30°C, the Arrhenius form of the water-loss equation was used to compute the extent of supercooling in ova cooled at rates between 1 and 8°C/min and the consequent likelihood of intracellular freezing. The predicted likelihood agrees well with that previously observed. The water-loss equation was also used to compute the volumes of ova as a function of cooling rate and temperature. The computed cell volumes agree qualitatively with previously observed volumes, but differ quantitatively.     

Viability and Morphology of rat heart cells after freezing and thawing of the whole heart

Intact adult rat hearts were cooled in the presence of 10% DMSO according to an external cooling program which approximated the optimal external three-step cooling program for the isolated adult heart cells: 20 min at ?20 °C, 0.2 °C/min from ?20 to ?25, ?30, or ?50 °C, and rapid cooling to ?196 °C. Following rapid thawing, cells were isolated after perfusion with a 0.1% collagenase solution. Only cells which originated from the free wall of the right ventricle could be isolated, even after cooling to ?20 °C. Most cells from hearts cooled to ?196 °C did not survive. When the third cooling step was omitted and the end temperature of the second cooling step was ?30 °C, 38% of the cells excluded trypan blue, 29% were morphologically intact, and 30% showed spontaneous contractions after thawing, expressed as percentages of the control, A much lower survival was found after cooling to ?50 °C.Histological and electron microscopical study of the heart immediately after thawing revealed no differences between hearts cooled to ?20, ?30, or ?196 °C. Also no marked differences were observed between the morphological integrity after freezing and thawing of the atrium, the left and right ventricle walls, and the ventricular septum. The survival data suggest the presence of nonmorphologically detectable alterations in cells frozen to ?196 °C, compared to cells frozen to ?30 °C. The morphological investigations indicate no essential differences in resistance of atrial and ventricular cells to the freezing process.Experiments involving neonatal rat hearts cooled to ?196 °C, according to the method which gave optimal preservation of the isolated cells, revealed that after thawing cells are present from which growing and contracting cultures can be derived. It appears that cells in the neonatal rat heart are more resistant to freezing to ?196 °C than cells in the adult rat heart.     

Cold tolerance and dehydration in Enchytraeidae from Svalbard

When cooled in contact with moisture, eight species of arctic Enchytraeidae from Svalbard were killed by freezing within minutes or hours at −3 and −5 °C; an exception was Enchytraeus kincaidi which survived for up to 2 days. When the temperature approached 0 °C the enchytraeids apparently tried to escape from the moist soil. The supercooling capacity of the enchytraeids was relatively low, with mean supercooling points of −5 to −8 °C. In contrast, specimens of several species were extracted from soil cores that had been frozen in their intact state at −15 °C for up to 71 days. Compared to freezing in a moist environment, higher survival rates were obtained during cooling at freezing temperatures in dry soil. Survival was recorded in species kept at −3 °C for up to 35 days, and in some species kept at −6 °C for up to 17 days. Slow warming greatly increased survival rates at −6 °C . The results strongly suggest that arctic enchytraeids avoid freezing by dehydration at subzero temperatures. In agreement with this, weight losses of up to ca. 42% of fresh weight were recorded in Mesenchytraeus spp. and of up to 55% in Enchytraeus kincaidi at water vapour pressures above ice at −3 to −6 °C. All specimens survived dehydration under these conditions. Accepted: 12 December 1997     

Optimal conditions for the preservation of mouse lymph node cells in liquid nitrogen using cooling rate techniques

The factors that affect the survival of mouse lymphocytes throughout a procedure for storage at ?196 °C have been studied both for the improvement of recovery and the possible extension to the mouse system of cell selection by freezing. After thawing, the survival of cells cooled at different rates in dimethyl sulphoxide (DMSO, 5 or 10%, $\text{v}\text{v}$) was assessed from the [³H]thymidine incorporation in response to phytohaemagglutinin and concanavalin A. Before freezing the protection against freezing damage increased with time (up to 20 min) in DMSO (5%, $\text{v}\text{v}$) at 0 °C. Superimposed upon this effect was toxicity due to the DMSO. During freezing and thawing the cooling rate giving optimal survival was 8 to 15 °C/min for cells in DMSO (5%) and 1 to 3 °C/min for DMSO (10%). Omission of foetal calf serum was detrimental. Rapid thawing (>2.5 °C/min) was superior to slow thawing. After thawing dilution at 25 or 37 °C greatly improved cell survival compared with 0 °C; at 25 °C survival was optimal (75%) at a moderate dilution rate of 2.5 min for a 10-fold dilution in FCS (10%, $\text{v}\text{v}$) followed by gentle centrifugation (50g).Dilution damage during both thawing and post-thaw dilution may be due to osmotic swelling as DMSO and normally excluded solutes leave the cell. The susceptibility of the cell membrane to dilution damage may also be increased during freezing. The need to thaw rapidly and dilute at 25 °C after thawing is probably due to a decrease in dilution stress at higher temperatures. Optimisation of dilution procedures both maximised recovery and also widened the range of cooling rates over which the cells were recovered. These conditions increase the possibility of obtaining good recovery of a mixed cell population using a single cooling procedure. Alternatively, if cell types have different optimal cooling rates, stressful dilution may allow their selection from mixed cell populations.     

Intracellular ice formation in yeast cells vs. cooling rate: Predictions from modeling vs. experimental observations by differential scanning calorimetry

To survive freezing, cells must not undergo internal ice formation during cooling. One vital factor is the cooling rate. The faster cells are cooled, the more their contents supercool, and at some subzero temperature that supercooled cytoplasm will freeze. The question is at what temperature? The relation between cooling rate and cell supercooling can be computed. Two important parameters are the water permeability (Lp) and its temperature dependence. To avoid intracellular ice formation (IIF), the supercooling must be eliminated by dehydration before the cell cools to its ice nucleation temperature. With an observed nucleation temperature of −25 °C, the modeling predicts that IIF should not occur in yeast cooled at <20 °C/min and it should occur with near certainty in cells cooled at ?30 °C/min. Experiments with differential scanning calorimetry (DSC) confirmed these predictions closely. The premise with the DSC is that if there is no IIF, one should see only a single exotherm representing the freezing of the external water. If IIF occurs, one should see a second, lower temperature exotherm. A further test of whether this second exotherm is IIF is whether it disappears on repeated freezing. IIF disrupts the plasma membrane; consequently, in a subsequent freeze cycle, the cell can no longer supercool and will not exhibit a second exotherm. This proved to be the case at cooling rates >20 °C/min.     

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.     

Cold tolerance of a New Zealand alpine cockroach, Celatoblatta quinquemaculata (Dictyoptera, Blattidae)

Abstract. Ecophysiological features, including survival and recovery from freezing and determination of the freezable water content, are reported for a cold-adapted cockroach Celatoblatta quinquemaculata Johns 1966 (Dictyoptera, Blattidae) inhabiting alpine communities at altitudes greater than 1300 m a.s.l. in mountains of Central Otago, New Zealand. Nymphs ranged from 15 to 51 mg live weight of which 67% was water. Cockroaches had a mean supercooling point temperature of ?5.4 ± 0.1°C; with recovery from freezing close to this temperature being rapid, but no recovery was observed when frozen at ?9 to ?10°C. The duration of exposure to freezing conditions and the time allowed for recovery (24–96 h) both influenced individual recovery and subsequent survival. Comparison of supercooling point data and survival shows that this species possesses a few degrees of freeze tolerance, and individuals have been found frozen in the field when subzero temperatures occur. Differential scanning calorimetry showed ≈ 74% of body water froze during cooling and between 24 and 27% of total body water was osmotically inactive (unfreezable under the experimental conditions). Carbohydrates, other than glucose at 7.5μg/mg fresh weight, were in low concentrations in the body fluids, suggesting little cryoprotection. No thermal hysteresis from antifreeze protein activity was detected in haemolymph samples using calorimetric techniques. It is suggested that slow environmental cooling rates, together with high individual supercooling points, confer a small amount of freezing tolerance on this species enabling it to survive low winter temperatures. This has allowed it to colonize and maintain populations in alpine habitats > 1300 m a.s.1. in New Zealand.     

Intracellular freezing of glycerolized red cells.

The response of glycerolized human red blood cells to freezing has been evaluated in terms of the thermodynamic state of the frozen intracellular medium. The physiochemical conditions requisite for intracellular freezing, characterized by the cooling rate and the degree of extracellular supercooling, are altered appreciably by the prefreezing addition of glycerol to the cells.Fresh human erythrocytes were suspended in an isotonic glycerol solution yielding a final cryophylactic concentration of either 1.5 or 3.0 m. Subsequently the cell suspension was frozen on a special low temperature stage, mounted on a light microscope, at controlled constant cooling rates with varying degrees of extracellular supercooling (ΔT_sc). The formation of a pure intracellular ice phase was detected by direct observation of the cells.The addition of glycerol produced several significant variations in the freezing characteristics of the blood. As in unmodified cells, the incidence of intracellular freezing increased with the magnitudes of both the cooling rate and the extracellular supercooling. However, the glycerolized cells exhibited a much greater tendency to supercool prior to the initial nucleation of ice. Values of ΔT_sc > ?20 °C were readily obtained. Also, the transition from 0 to 100% occurrence of intracellular ice covered a cooling rate spectrum in excess of 300 to 600 °K/min, as compared with 10 °C/min for unmodified cells. Thus, the incidence of intracellular ice formation was significantly increased in glycerolized cells.     

Effect of cholesterol-loaded cyclodextrins on bull and goat sperm processed with fast or slow cryopreservation protocols

Cholesterol-loaded cyclodextrins (CLC) added to the sperm before cryopreservation enhance sperm quality after freeze-thawing in several cold shock-sensitive species, including cattle and goats. However, all studies conducted to date have used conventional protocols, in which sperm are cooled slowly to 5°C before freezing. As cholesterol plays a significant role in sperm cold shock resistance, it is possible that CLC-treated sperm can withstand cooling damage when the sperm are not cooled slowly to 5°C before freezing. In this study, we determined whether CLC-treated goat (1 mg CLC/120×10⁶ sperm) and bull (2 mg CLC/120×10⁶ sperm) sperm quality, after thawing, was different for sperm frozen using conventional protocols (including a slow cooling phase to 5ºC) and protocols in which the sperm were frozen from room temperature, without cooling the sperm slowly to 5°C before freezing. CLC-treated sperm exhibited higher percentages of plasma membrane-intact sperm than control sperm when cryopreserved using conventional protocols. In addition, CLC treatment enhanced both sperm motility and plasma membrane integrity when sperm were frozen directly from room temperature. However, this treatment did not fully prevent the damage of the sperm after cooling rapidly and subsequent freezing, as the sperm quality was lower than that presented by the samples frozen using the conventional protocol. The results are promising, but studies to optimize the protocols for freezing sperm directly from room temperature need to be conducted, as well as studies to determine how cryopreserving sperm in this manner affects other sperm functions.     

Comparison of the cold hardiness of two larval Lepidoptera (Noctuidae)

Abstract Diapause larvae of the European corn borer (Ostrinia nubilalis (Hubn.)) and the related Mediterranean noctuid Sesamia cretica Led. possess sufficient supercooling ability to avoid freezing over their normal environmental temperature ranges. In progressive chilling experiments (10 days acclimation at each 5° step in the temperature range from 15 to ?5°C), mean supercooling points (measured at a cooling rate of 0.1°C min^?1) were lowered from ?20.4°C at 15°C to ?24.0°C at 5°C (lower lethal temperatures: c.?28°C) in O.nubilalis, compared with ?15.0 to ?17.2°C (lower lethal temperatures: ?15 to ?17°C respectively) in S.cretica. Concentrations of glycerol and trehalose determined by gas chromatography of whole body extracts were consistently higher in the former than in the latter species at both 15 and 5°C, and may be responsible for the deeper supercooling in O.nubilalis larvae. Acclimation to 5°C increased glycerol levels in O. nubilalis extracts compared with 15°C, and this was enhanced in larvae exposed for a further 10 days at each of 0 and ?5°C (glycerol being 438μmol ml^?1 body water). Haemolymph glycerol concentrations showed a similar pattern to whole body extracts in this species. Fat body glycogen was reduced during low temperature acclimation in both species. Body water contents did not change with acclimation in O.nubilalis, whilst S.cretica, containing significantly more water, lost c.7% during acclimation from 15 to 5°C. Haemolymph osmolalities increased during acclimation, especially in Ostrinia larvae, probably as a result of the accumulation of cryoprotectants. The majority of O.nubilalis larvae survived freezing under the conditions of the cooling experiments, whilst larvae of S.cretica did not, thereby confirming an element of freezing tolerance in the former.     

A microprocessor-controlled rate controller for use in cryopreservation

The design and operation of a microprocessor-controlled rate controller incorporated into a constant-rate cooling system used in the cryopreservation of cells is described. The controller differs from those currently available in that the actual temperature of the cell suspension being cooled is compared with a preselected ramp of the microprocessor. Differences between the two determine the opening of solenoid valves that permit entry of liquid N₂ vapors into the freezing chamber. The heat of fusion, which is released as extracellular ice crystallizes, automates the opening of additional solenoid valves. The rapid entry of N₂ vapors into the chamber cools the cell suspension, therefore restoring the programmed cooling rate. The functional recovery of murine splenic lymphocytes cooled at ?1.0 °C/min using this system exceeds the recoveries given in most other reports.     

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.     

Field ecology of freezing: Linking microhabitat use with freezing tolerance in Litoria ewingii

A small number of vertebrate species, including some frogs, are freezing tolerant and survive ice forming in their bodies under ecologically relevant conditions. Habitat use information is critical for interpreting laboratory studies of freezing tolerance, but there is often little known about the winter habitat and behaviours of the species under study. This work describes microhabitats used by the freezing‐tolerant frog Litoria ewingii Duméril and Bibron 1841 and their temperature characteristics. In winter, L. ewingii used microhabitats with wood, located further away from water than in summer. Microhabitat temperature records showed that frog microhabitats regularly fell below the temperature at which frog body fluids freeze (?1°C), and cooled substantially more slowly than did the air temperature. Temperatures were highly variable between microhabitats, seasons and years, with a minimum of ?2.4°C and a maximum cooling rate of 0.77°C h^?1. Frozen frogs were observed to recover in the field, demonstrating freezing tolerance. Both the characteristics of microhabitats and their selection are important in ensuring freezing survival.     

Cryoprotectant removal temperature as a factor in the survival of frozen rice and sugarcane cells

Removal of cryoprotective additives through use of a room temperature (22 °C) washing step, instead of 0 °C, was found to improve the recovery of sugarcane suspension culture and rice callus tissues. Cultured cells were cryoprotected by gradual addition of a mixture of polyethylene glycol, glucose, and DMSO (PGD) to a final concentration of 10%-8%-10%, w/v, respectively, added at either 0 or 22 °C. After a programmed slow freezing of the cells, they were thawed rapidly and the cryoprotectants were gradually diluted and washed out using a 22 or 0 °C washing medium. Viability of suspension cultured sugarcane cells protected with PGD was greatly diminished when a cold washing solution was used, whether the cells had been frozen (?23 °C) or not. Two mutant lines of rice callus when frozen to ?196 °C in PGD and thawed showed less growth than unfrozen cells, but their growth was improved by washing the thawed cells with a 22 °C solution. With all cultures tested, the addition of PGD at 0 °C and post-thaw washing out at 22 °C gave improved survival. Particularly with the rice lines, optimizing the addition and washing procedures allowed culture survival of liquid nitrogen freezing not otherwise attained.     

Differing actions of penetrating and nonpenetrating cryoprotective agents.

A two-step freezing technique has been used to examine the role of cryoprotective agents during cooling. Chinese hamster fibroblasts were cooled to various subzero holding temperatures and subsequently thawed or cooled to ?196 °C before thawing. Cells were suspended in various concentrations of dimethylsulfoxide (DMSO) or hydroxyethyl starch (HES) before freezing. The results indicated differing protective actions of DMSO and HES. These differences were verified using glycerol as either a penetrating or a nonpenetrating agent.The results are consistent with the concepts that cryoprotection is based on the avoidance or minimization of intracellular freezing and the minimization of damage to the cell from the environment of concentrated solutes during cooling, and that the colligative action of both penetrating and nonpenetrating agents allows the cells to survive the conditions for a reduction of cell water content during cooling thereby reducing the amount of intracellular freezing. The results indicate that penetrating and nonpenetrating agents accomplish this in different ways. Penetrating agents create the environment for a reduction of cell water content at temperatures sufficiently low to reduce the damaging effect of the concentrated solutes on the cells. Nonpenetrating agents osmotically “squeeze” water from the cells primarily during the initial phases of freezing at temperatures between ?10 and ?20 °C when these additives become concentrated in the extracellular regions.     

Increased cold hardiness in eggs of Arcynopteryx compacta (Plecoptera) by dehydration

Eggs of the stonefly, Arcynopteryx compacta, that overwinter in the alpine region of Norwegian mountains, increase their cold-hardiness by dehydration. Eggs enclosed in ice at −22°C survive the loss of about two-thirds of their total water content by shrinkage due to passive diffusion of body water along the concentration gradient. Fully hydrated eggs are killed by freezing at their supercooling point of −26°C, and by direct cooling to −30°C. Dehydrated eggs have a mean supercooling point of −31°C, and survive exposure at −27 and −29°C in ice. Judged from their melting points the eggs do not accumulate low-molecular-weight cryoprotective substances. The difference between freezing and melting points corresponds to a thermal hysteresis of up to 1.8°C. The presence of thermal hysteresis antifreezes may stabilize their supercooled state when enclosed by ice during overwintering. The eggs enter diapause in the autumn, and diapause completion is enhanced both by temperature and time during enclosure in ice.     

Freezing and desiccation tolerance of imbibed canola seed

Depending on the environmental conditions, imbibed seeds survive subzero temperatures either by supercooling or by tolerating freezing-induced desiccation. We investigated what the predominant survival mechanism is in freezing canola ( Brassica napus cv. Quest) and concluded that it depends on the cooling rate. Seeds cooled at 3°C h⁻¹ or faster supercooled, whereas seeds cooled over a 4-day period to −12°C and then cooled at 3°C h⁻¹ to−40°C did not display low temperature exotherms. Both differential thermal analysis and nuclear magnetic resonance (NMR) spectroscopy confirmed that imbibed canola seeds undergo freezing-induced desiccation at slow cooling rates. The freezing tolerance of imbibed canola seed (LT₅₀) was determined by slowly cooling to −12°C for 48 h, followed with cooling at 3°C h⁻¹ to −40°C, or by holding at a constant −6°C (LD₅₀). For both tests, the loss in freezing tolerance of imbibed seeds was a function of time and temperature of imbibition. Freezing tolerance was rapidly lost after radicle emergence. Seeds imbibed in 100 μ M abscisic acid (ABA), particularly at 2°C, lost freezing tolerance at a slower rate compared with water-imbibed seeds. Seeds imbibed in water either at 23°C for 16 h, or 8°C for 6 days, or 2°C for 6 days were not germinable after storage at −6°C for 10 days. Seeds imbibed in ABA at 23°C for 24 h, or 8°C for 8 days, or 2°C for 15 days were highly germinable after 40 days at a constant −6°C. Desiccation injury induced at a high temperature (60°C), as with injury induced by freezing, was found to be a function of imbibition temperature and time.