1 Department of Obstetrics, Gynecology and Reproductive Biology, Brigham and Women's Hospital, Harvard Medical School, 75 Francis Street, Boston, MA 02115, 2 Center for Engineering in Medicine and Surgical Services, Massachusetts General Hospital, Harvard Medical School, 51 Blossom Street, Boston, MA 02114 and 3 Department of Cell Biology, Harvard Medical School, 240 Longwood Avenue, Boston, MA, USA
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Abstract |
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Key words: cryobiology/freezing/human/intracellular ice formation/oocyte
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Introduction |
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Good fertilization and cleavage rates (Al-Hasani et al., 1987; Chen, 1988
; Gook et al., 1994
, 1995
; Toth et al., 1994
; Kazem, 1995
) as well as a few pregnancies (Van Uem et al., 1987
; Chen, 1988
; Tucker et al., 1996
; Porcu et al., 1997
) have been reported using human oocytes that survived cryopreservation. Although post-thaw survival rates ranging from 20 to 80% have been achieved, these freezing protocols have not been robust enough to translate into a reproducible, clinically useful technique. Pre-freezing events, such as oocyte exposure to cryoprotectant solutions and simple cooling, have been shown to be relatively innocuous, and do not inhibit fertilization and development (Hunter et al., 1991
; Bernard et al., 1992
; Gook et al., 1995
). Thus, the step that limits the efficiency of this multi-step process seems to be confined to the freeze and thaw procedure.
Hitherto, attempts to improve the freeze and thaw process in human oocytes have used protocols empirically derived from animal models. An alternative approach relies on studying the biophysical characteristics of oocytes under sub-zero conditions by observing water transport and intracellular ice formation (IIF) using a cryomicroscope. These biophysical characteristics are then used in a theoretical model to derive an optimized freezing protocol (Karlsson et al., 1996). The currently accepted theory states that the avoidance of large and numerous intracellular ice crystals is a necessary, but not sufficient, condition for a cell to survive freezing (Mazur, 1984
). One strategy to prevent IIF after extracellular ice seeding is to provide time for the cell to dehydrate before reaching the lower temperatures at which ice nucleation occurs. Typically, dehydration of oocytes occurs during a slow (<2°C/min) freezing, with the diffusion of intracellular water to the hyperosmotic extracellular media generated by the incorporation of pure water in the growing crystals. However, slowly cooled cells suffer damage due to long exposure to high electrolyte concentrations, excessive cell dehydration, mechanical effects of the external ice, and a combination thereof. Thus the cooling rates should be fast enough to minimize the long exposure of oocytes to deleterious freezing conditions, but slow enough to avoid the damaging effect of IIF. To design a freezing protocol, the biophysical parameters governing not only water transport across the oolemma but also ice nucleation need to be determined. To date, the parameters for water transport are known for bovine (Myers et al., 1987
) and mouse oocytes at supra-zero (Leibo, 1980
) and sub-zero temperatures (Toner et al., 1990a
). Ice nucleation parameters are known for both mouse oocyte (Toner et al., 1990b
; Karlsson et al., 1996
) and macaque (Younis et al., 1996
) oocytes. Some water transport parameters have been determined in human oocytes (Hunter et al., 1992
), but not those concerned with ice nucleation parameters.
In this paper, we show that the median temperature at which IIF occurs in human oocytes is not depressed to a significant level by the addition of several cryoprotectants. This unexpected finding indicates that IIF occurs more readily in human oocytes. We also report that the extracellular ice seeding temperature significantly affects IIF in human oocytes. The data are used to suggest modifications of a current method of freezing human oocytes to increase the post-thaw survival rate.
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Materials and methods |
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Human oocytes
The following categories of human oocytes were used for this study.
Fresh oocytes with a germinal vesicle
These were retrieved from patients scheduled for intracytoplasmic sperm injection (ICSI) who had their oocytes evaluated for maturity prior to injection. The cumulus mass was completely removed 4 h after the retrieval with a small bore glass pipette following a 30 s exposure to 80IU/ml hyaluronidase (H3506; Sigma) in HEPES-buffered HTF (9963; Irvine Scientific). The immature eggs with a germinal vesicle were selected for the study.
Oocytes after exposure to spermatozoa
Oocytecumulus complexes were inseminated 46 h after retrieval using 1 500 000 spermatozoa/ml. The spermatozoa were processed with a Percoll column (Punjabi et al., 1990). Fertilization was assessed at 1419 h post insemination. Two categories of these oocytes were selected for study.
Failed-to-fertilize.
Unfertilized oocytes were evaluated for maturity and classified as metaphase I (MI) and metaphase II (MII) oocytes, based on the presence or absence of a polar body. Eggs were used within 2430 h of the retrieval. Because of their scarce number, unfertilized oocytes with a germinal vesicle were not used for this study.
Polyspermic embryo.
Fertilized oocytes with an abnormal number of pronuclei were used while still in the uncleaved stage. Eggs were used 2430 h after retrieval.
Mouse eggs
The procedure for the collection of mouse oocytes has been described previously (Jackson and Keissling, 1989). Four to six week old BDF mice were obtained from the Jackson Laboratories (Bar Harbor, ME, USA). Female mice were induced to superovulate by intraperitoneal (i.p.) injection of 5IU of pregnant mare serum gonadotrophin (Sigma, G-4877), followed 48 h later by an i.p. injection of 5IU of HCG (Sigma, CG-5). Twelve to 15 h later, metaphase II oocytes were collected and used for experiments.
Cryoprotectant solutions
The following saline solutions were used in this work: Dulbecco's phosphate-buffered solution (DPBS) (4501300EC; Gibco) and PB1 (DPBS + glucose) (4501300eb; Gibco). Both solutions were supplemented with penicillin G (0.095 g/l) and streptomycin (0.05 g/l). All freezing solutions were prepared using PB1. The following cryoprotectant solutions were prepared: (i) 1.5 M propylene glycol (P1009; Sigma) in PB1 (PG), (ii) 1.5 M dimethyl sulphoxide (5879; Sigma) in PB1 (DMSO), and (iii) 1.5 M ethylene glycol (E-9129; Sigma) in PB1 (EG). For the oocyte cryopreservation experiments, PG, DMSO, and EG were supplemented with 20% SSS in order to minimize oocyte loss due to sticking in the straws. For the cryomicroscopy experiments, the freezing solutions were used without adding SSS, since oocytes were not recovered after a cryomicroscopy experiment. Only 1.5 M cryoprotectant solutions were used, except when a stepwise addition of 0.5 M and 1.0 M solutions of PG was needed. For the removal of cryoprotectant solutions from oocytes, 1.08 M sucrose (S0389; Sigma) in PB1 supplemented with 20% SSS was used for both conventional and modified cryopreservation protocols.
Oocyte cryomicroscopy
The occurrence of IIF in oocytes, in the presence and absence of a cryoprotectant, was observed using the cryomicroscopy system described by Cosman et al. (1989). Our equipment employed a programmable thermal microscope stage (Thermascope; Interface Technique, Cambridge, MA, USA) connected to a video microscopy system. Depending on availability, two to 15 human oocytes were equilibrated in the cryoprotectant solutions for 20 min and then placed in a 50 µl drop on the cryomicroscope stage under a coverslip sealed with silicone grease. The initiation of the sample freezing was achieved by slightly supercooling the solution to 6.5°C and manually triggering seeding extracellular ice by contacting the edge of the sample with a chilled forceps. Controlled cooling at a rate of 120°C/min to 60°C was initiated as soon as the growing ice front had engulfed all oocytes in the field of view. Oocytes were not held at the extracellular ice seeding temperature because the thin layer of 50 µl solution had a thickness of ~50100 µm which allows immediate latent heat dissipation. A rapid cooling rate of 120°C/min was chosen to minimize water efflux, thus reducing the effect of water transport on ice nucleation. Under bright-field illumination, IIF was manifested by a sudden darkening of the cytoplasm believed to be caused by the light scattering due to microscopic ice crystals and/or bubbles in the oocyte. The temperature at which IIF occurred in each oocyte was determined by reviewing the video recordings of each freezing experiment. The observed IIF temperature for each individual oocyte was corrected for the thermal gradient across the stage by subtracting the corresponding temperature of the ice front during the thaw, and adding the melting point of the solution (Toner et al., 1990b). In subsequent experiments, the effect of varying the cooling rates and extracellular ice seeding temperatures on IIF was also determined. Cooling rates of 0.2°C/min and 10°C/min were used to investigate the role of dehydration on IIF. Also, at a cooling rate of 0.2°C/min, the extracellular ice seeding temperature was modified by supercooling the solution to 4.5, 5.5, 6.0, 6.5 and 8°C before contacting the edge of the sample with a chilled forceps. The incidence of IIF for each experimental setting was recorded.
Oocyte cryopreservation
These experiments were designed to test the modified freezing protocol associated with a minimal incidence of IIF by assessing the viability of frozenthawed oocytes. Control experiments were conducted using the one step method for human embryo cryopreservation derived from a bovine embryo freezing protocol (Leibo 1984) and then modified (Nowrouzi et al., 1991
) for human use.
The conventional cryopreservation protocol
A Biocool freezer (FTS System, Stone Bridge, NY, USA) was used, with a reagent grade alcohol at 95% (Thomas Scientific, 4916-E52) and a TPC-44.E programmable controller set for the following protocol: starting temperatures -6°C and -8°C, ramp rate -0.2°C/min, holding temperature -40°C, holding time 15-30 min. In preparation for the freezing protocol, the oocytes were transferred to a PB1 solution for 10 min followed by PG equilibrated at room temperature for a maximum of 20 min. The 0.25 ml straws (IMV, France, A101) were loaded as follows: 10 mm of PG, 10 mm of air, 10 mm of PG containing the oocytes, 10 mm of air, 65 mm of sucrose solution, 10mm of air. The air was drawn up until the first PG column moistened the PVA powder between the two plugs and no more air could be drawn in. Both ends of the straw were sealed by heat and the plugged end was fitted with a 0.5 ml straw (IMV, A102) to be used as a handle. The straws were maintained in a horizontal position until they were briefly plunged into the alcohol bath at -6°C and -8°C. The top of the sucrose column and the bottom of the PG column not containing the oocytes were then seeded using a chilled forceps. All the straws were placed perpendicularly in a freezing basket (IMV, M001) suspended in the 95% alcohol bath and held for 15 min at the extracellular ice seeding temperature. After confirming that the straws were frozen, the ramp was activated as described above. At the end of the 15 min holding time at -40°C, the straws were quickly transferred to a liquid nitrogen canister, and then moved to a storage tank for 17 days.
For thawing, the straw was removed from the liquid nitrogen tank and laid at room temperature for 2 min with both ends supported by a slant rack. If, after wiping with a Kim wipe, condensation formed, an additional 30 s was allowed. After taking the handle off, and holding the unplugged end, the straw was shaken a few times like a thermometer until there was only one air space at this end. The straw was then placed, plugged end down, in 15 ml centrifuge tube containing Milli-Q water in a 37°C water bath for 3 min. The straw was then turned over, plugged end up, and placed in a 15ml centrifuge tube containing Milli-Q water at room temperature for 1 min. The straw was emptied on a dry dish under direct vision using a dissecting microscope. The oocytes were washed twice in PB1 at room temperature and allowed to equilibrate for 10 min before transfer to a culture dish in the conditions described above.
The modified cryopreservation protocol
To induce seeding of extracellular ice at -4.5°C, the following modifications were introduced to the conventional protocol described above. The Biocool unit was programmed as follows: segment 1: start temperature -3.5°C, ramp -0.2°C/min, holding temperature -15°C, holding time 0 min; segment 2: ramp -1°C/min, holding temperature -40°C, holding time 1530 min. The IMV straws were loaded as follows: 10 mm of PG, 10 mm of air, 20 mm of PG containing the oocytes, 10 mm of air, 55 mm of sucrose and 10 mm of air. The unplugged end was fitted with the 0.5 ml IMV straw. The straws were held perpendicularly, plugged end up, until all the oocytes migrated to the lower meniscus of the 20mm PG column. Their exact position was checked under a dissecting microscope. Meanwhile, the freezing programme was activated from the starting temperature of -3.5°C, then put on hold to maintain the alcohol bath temperature at -4°C. The straw was inverted, and briefly dipped in the alcohol bath for 1015 s at a 45° angle. All the temperatures were measured at the tip of a temperature probe located at the level of the 20 mm PG column. The lower meniscus of the 20 mm PG column was seeded in a location opposite to the oocytes, and replaced promptly in the alcohol bath in the slanted position. Simultaneously, the freezing ramp was reactivated to reach -4.5°C. This temperature was held for 20 min. After checking for seeding of the sucrose column without removing the straw from the alcohol bath, we proceeded with the protocol as above.
Attention to the following details was important to ensure adequate extracellular ice seeding. Because seeding of extracellular ice in an adjacent column at higher temperatures did not ensure proper ice formation in the cryoprotectant column containing the oocytes, the latter was seeded directly. Consequently, and to prevent accidental exposure of the eggs to ice seeding, the size of the cryoprotectant column containing the oocytes was doubled to 20 mm. The oocytes were also moved as far as possible from the seeding area by placing the straw perpendicularly, and their location was verified at the opposite meniscus prior to seeding of extracellular ice. The straw was placed in a 45° slanted position in the alcohol bath to allow the oocytes to move slowly toward the frozen area. In a perpendicular position, the oocytes reached the bottom of the PG column in 25 min, as opposed to 1015 min in the slanted position. This timing was critical. It allowed new ice to grow upward from the frozen region and trap the oocytes migrating downward in hyperosmolar channels located between the growing ice crystals.
Evaluation of oocyte survival
Oocyte survival was assessed at 2 and 24 h post-thaw. Signs of oocyte damage included zonal fracture, discoloured ooplasm, pyknosis and cytoplasmic disruption. A very good correlation was previously reported between delayed (24 h) morphological assessment, and vital staining when demonstrating viability of frozenthawed human oocytes (Pensis et al., 1989).
Biometrical methods
Box plots
The distributions of the temperature of IIF under various experimental conditions were plotted as proportional notched box plots to show the 10th, 25th, 50th (median), 75th, 90th percentiles (Kafadar, 1985). Observations that fall outside the 10th and 90th percentile were considered outliers. The width of the box is proportional to the number of observations. The notches were constructed using the formula 1.57x(75th percentile 25th percentile)/n. If the notches do not overlap, the medians are considered significantly different at a significance level of P = 0.05. The box plots were computed using the Number Cruncher Statistical System 97 (NCSS, Kaysville, UT, USA).
Contingency tables
The data in Tables I and II are presented as doubly ordered rxc contingency tables. The homogeneities of the row (seeding temperatures) distributions were tested using the one-sided exact JonckheereTerpstra test of significance (Pirie, 1983
). The value of P and its 99% confidence limits were computed by the Monte Carlo method using the StatXact 3 for Windows computer package (Cytel Software Corporation, Cambridge, MA, USA).
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Two of the sets of data in Tables I and II were also examined by fitting linear logistical regression equations of the form:
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where y = logit p = ln (p/(1 p)), p is the proportion responding, T is the extracellular ice seeding temperature, b0 is the intercept, and b1 is the slope of the regression. All computations were done using the LogXact for Windows computer package (Cytel).
Model threshold distributions
Consider a population of n oocytes. Hypothetically each oocyte will form intracellular ice as a result of extracellular ice seeding at some threshold temperature (TII). Likewise the oocyte will suffer irreversible damage and die as the result of seeding at some threshold temperature (TID). These two temperatures are not necessarily the same, although they may be highly correlated. In both cases frequency distributions [f(TID), f(TII)] of threshold values can be used to model the population of oocytes. The corresponding cumulative distributions of survivors (F(TID)) and oocytes in which intracellular ice forms (F(TII)) are given by:
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Specifically, we will assume that the two frequency distributions can be modelled by the logistic distribution, which is very close to the normal distribution and has properties that make it relatively simple to use (Malik, 1985). Finney (Finney 1947
) has described a comparable use of the logistic distribution, including the computations involved, in a discussion of tolerance distributions which arise in the field of biological assay. He showed that the logistic distribution can be estimated by substituting equation (1) in the equation:
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Thus the values of b0 and b1 obtained by fitting (1) to the data in Tables I and II have been substituted in (3) to estimate the two frequency distributions of the threshold temperatures that cause irreversible damage [f(TID)] and IIF [f(TII)]. The corresponding cumulative distributions can be computed by transforming the fitted linear equations from the logit response scale to the proportion response scale using the inverse of equation (1):
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Results
Preliminary observations
Preliminary experiments with human oocytes showed significant differences in the median temperature of IIF (TMED) in fresh oocytes with a germinal vesicle, unfertilized MI or MII oocytes and polyspermic oocytes (Figure 1). The differences were considered marginal and sufficiently small to justify pooling the data from all types of human oocytes when analysing all subsequent experiments.
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Uptake of cryoprotectant (PG)
Given the larger size of human oocytes, the equilibration of PG with human oocytes was evaluated from their volumetric behaviour in PG, as assessed by measuring the oocyte projected area and converting it to volume by assuming spherical geometry. Specifically, five human oocytes were placed in 1.5 M PG. They shrank rapidly within 30 s and then, relatively slowly, returned to their near-original volume in ~6 min (data not shown). This is the classical physiological response of a cell exposed to a permeable solute, and clearly demonstrates that human oocytes were nearly equilibrated with 1.5 M PG during our cryomicroscopy experiments.
Cytoplasmic damage due to osmotic shock
To rule out the possibility that osmotic damage to human oocytes during one-step addition of 1.5 M PG was causing elevated IIF temperatures, 33 human oocytes were first exposed sequentially to 0.5 M, 1.0 M and 1.5 M PG for 5 min each and then frozen at a rate of 120°C/min in 1.5 M PG. The TMED was -12.7°C, very similar to our previous estimate of -13.5°C. Furthermore, gross membrane damage after prolonged exposure (90 min) of five human oocytes to PG could not be demonstrated in the form of superficial blebs.
Rate of freezing
Forty-seven human oocytes in PG were frozen at a rate of -10°C/min. Although the TMED decreased to -17.7°C, potentially accounting for minimal water diffusion, it remained well above nucleation temperatures of mouse oocytes (below -30°C).
Oocyte culture
Since human oocytes were cultured for ~24 h prior to the cryomicroscopy experiments, the effect of culture on mouse oocyte IIF was also investigated. Twelve mouse oocytes cultured for 24 h were frozen in PG at 120°C/min. The observed TMED of -28.8°C was similar to the TMED determined in fresh mouse oocytes of -32.1°C.
Effect of seeding temperature on IIF
Groups of human oocytes were frozen on the cryomicroscope at a rate of -0.2°C/min, until the temperature was -40°C. The groups were seeded at -8.0, -6.5, -6.0, -5.5 and -4.5°C. The numbers of oocytes undergoing IIF were determined at the end of each run. The pooled results are shown in Table I. The exact Jonckheere-Terpstra test of significance shows that there are very significant differences between the effects of seeding temperature on the incidence of IIF (P < 0.001). The probability of IIF progessively falls as the seeding temperature is increased above 6.5°C. A linear logistic regression was fitted to the data (Table I
, Figure 5
), and its estimated slope was found to be significantly negative. The very significant deviance, however, indicates that the model is a poor fit to the data. Further analysis of the residuals showed that this lack of fit is mainly due to a small group of eight oocytes all of which developed intracellular ice after seeding at -6.5°C. When this group was omitted from the regression analysis the deviance became non-significant although the estimated slope was only slightly changed. Thus the sigmoid regression line shown in Figure 5
was computed, retaining the group with apparently extreme responses.
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Discussion
Cryomicroscopy has been used to determine the characteristics of IIF in human oocytes with and without several penetrating cryoprotectants. The results demonstrated that although the IIF temperature of human oocytes was not depressed by the addition of several cryoprotectants, a modified freeze and thaw protocol for human oocytes with high survival rates could still be designed.
Choosing an optimal seeding temperature
The ascending and descending sigmoid regression lines shown in Figure 5 are independent estimates of the cumulative proportions of oocytes undergoing IIF and oocytes surviving after extracellular ice seeding in a temperature range of -8°C and -4.5°C. Both sets of oocytes were frozen in the presence of PG. The curves are almost inversely symmetrical, and intersect at a point whose abscissa corresponds to a seeding temperature of 6.7°C. This relationship is similar to the high correlation observed between the incidence of IIF and cell survival on cooling rates (Toner et al., 1993
). Fifty-three per cent of the oocytes are expected to form intracellular ice and survive respectively when seeded at this temperature. The estimated frequency distribution of the threshold seeding temperatures at which individual oocytes form intracellular ice [f(TII)] is shown in Figure 6
. Similarly the estimated frequency distribution of the threshold seeding temperatures when individual oocytes suffer irreversible damage [f(TID)] is also shown in Figure 6
. A prominent feature of both distributions is the variability of the two parameters over a wide range of extracellular ice seeding temperatures. A few oocytes are very sensitive to the extracellular ice seeding temperatures and undergo IIF. As a result, these sensitive oocytes suffer irreversible damage at relatively high extracellular ice seeding temperatures (about -4.5°C). Alternatively, a few oocytes are very insensitive to the extracellular ice seeding temperature and do not undergo IIF. These oocytes suffer irreversible damage at only relatively low extracellular ice seeding temperatures (below -8°C). From a practical point of view, these results show that the initiation of the freezing protocol by seeding the extracellular ice at -8°C results in the loss of many human oocytes. On the other hand, seeding extracellular ice at -6°C will result in a significantly higher proportion of oocytes surviving. Nevertheless, particularly sensitive oocytes will still be lost. We thus propose that when human oocytes are frozen, the extracellular ice seeding temperature should be raised to a window between -4°C and -4.5°C to minimize the occurrence of IIF and save the more sensitive oocytes (Figure 6
). The effects of seeding temperature on the survival of human and mouse oocytes are noticeably different. The cumulative incidence of survival of mouse embryos decreases steeply only when the seeding temperature is lowered below -7°C (Whittingham, 1977
) or -8°C (Miyamoto, 1981
). Thus, the acceptable window for extracellular ice seeding in the mouse is somewhat wider (34°C) than that in the human, allowing much more flexibility in the choice of seeding temperatures.
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Quantitative differences between species in the effects of cryoprotectants
When human oocytes were frozen at -120°C/min in the presence of cryoprotectant, the TMED was only slightly depressed (~6.5°C) (Figure 1). The fall in the IIF temperature was far less than that which occurs in mouse oocytes (~23°C; Table I
) (Karlsson et al., 1996
). The reason for these differences may be related to the 3-fold difference in volume between the small mouse oocyte and the large human oocyte. Consistent with this possibility, a comparable relatively small depression of IIF (~4°C) produced by glycerol was observed in the large cow oocyte (Myers et al., 1987
). In contrast the published literature on the nucleation temperature of ice in water droplets of diameters comparable to those of mouse and human oocytes (80129 µm) does not support this explanation, because of a very weak measured dependence of nucleation on droplet volume. However, it is important to note that these water droplet studies are performed under either homogeneous or relatively ineffective heterogeneous nucleation conditions at temperatures below -30°C [review: Hobbs (1974)]. On the other hand, human oocytes underwent IIF at much higher temperatures, indicating a very effective heterogeneous catalysis of IIF. In fact, a model based on the modified classical nucleation theory predicts that the likelihood of IIF in mouse oocytes is a strong function of the surface area of the cell (thus, cell volume) under consideration (Toner, 1993
). Other cell-specific factors may also be involved since the depression of the temperature for IIF produced by DMSO in several cell types from different species was not correlated with volume (Hubel et al., 1991
). Further detailed studies are required to explain the observed interspecies differences.
The large difference between human and mouse oocytes in the range of temperatures when IIF occurs should arouse caution in extrapolating protocols optimized in the mouse for use in the human. In a typical freezing protocol with a freezing rate of <2°C/min, most mouse oocytes will loose 90% of their water before reaching the critical ice nucleation temperature zone between -30°C and -40°C, and will thus avoid lethal IIF (Mazur, 1977). In the human oocyte, we have shown that lowering the rate of freezing to -0.2°C/min is not successful in preventing IIF, presumably because the cell has not dehydrated sufficiently when it enters the critical IIF temperature zone. The insufficient dehydration is probably related to the remarkably higher ice nucleation temperatures observed in the human oocytes. More specifically, extracellular ice seeding at -6°C and -8°C, customary in most freezing protocols, triggers IIF in a significant number of human oocytes during the holding period (Table I
). Our results have shown that the undesirable IIF can be prevented by increasing the temperature of extracellular ice seeding as close as possible to the melting point of the solution, which in our case was -4.5°C. Presumably the higher extracellular ice seeding temperature allows the human oocyte to dehydrate extensively prior to reaching the critical temperature zone of IIF, thereby preventing the occurrence of IIF. In our protocol, a freezing rate of -0.2°C/min down to -15°C was empirically adopted to guarantee near equilibrium conditions between cytoplasmic and extracellular water as the oocyte approaches the IIF temperature range so as to ensure maximal dehydration. Thereafter, the freezing rate was increased to -1°C/min to reduce the exposure time to the potentially damaging extracellular electrolyte and solute concentrations which develop during freezing (Karlsson et al., 1996
). Although this modified two-step cooling protocol changed both the extracellular seeding temperature and the cooling rate compared to the conventional protocol, the total duration of the protocol between the seeding of the extracellular ice and the plunge temperature into liquid nitrogen at -40°C is similar for all protocols (~80 min). The rationale for constant protocol duration is the strong association observed between protocol duration and mouse oocyte viability in our earlier studies (Figure 5
of Karlsson et al., 1996
). Since these settings were arbitrarily determined, this protocol could be further optimized by using the theoretical model described elsewhere (Toner et al., 1991
; Karlsson et al., 1996
).
Seeding temperatures and IIF in other cells
The effects of extracellular ice seeding temperature and cooling rate on IIF has been theoretically investigated with several mammalian cells, including red blood cells (Diller, 1975), granulocytes (Schwartz and Diller, 1984
), hepatocytes (Toner et al., 1992
) and mouse oocytes (Toner et al., 1993
). All of these studies clearly indicate strong dependence of IIF behaviour of mammalian cells on the extracellular ice seeding temperatures. Typically, for faster cooling rates, the cumulative frequency of IIF increases for a given extracellular ice seeding temperature because less time is available for the cells to dehydrate at faster cooling rates. These studies underscore the important role of the extracellular ice seeding temperature on the fate of cells with respect to undergoing IIF. In the case of human oocytes, minimal depression of IIF in the presence of cryoprotectants requires using both a very slow cooling rate and a high extracellular ice seeding temperature to afford enough cellular dehydration to minimize (or prevent) IIF.
Are spare human oocytes useful in research?
There should always be concern about whether reliable conclusions can be reached when spare human oocytes and embryos are used for research (see Winston et al., 1993). Two observations suggest that the cell membranes of the failed-fertilized and polyspermic oocytes we have used retained their semipermeable properties which play a key role in the formation of intracellular ice. Firstly, the TMED of spare human oocytes frozen with no cryoprotectant -8.5°C, (Figure 1
) is only 4°C above the TMED observed when freshly isolated mouse oocytes were frozen without cryoprotectant. Secondly, there is a close inverse symmetry of the cumulative distributions of IIF and survivors when spare human oocytes are frozen (Figure 5
).
To conclude, we found that human oocytes display minimal or no depression of ice nucleation temperatures irrespective of the cryoprotectant used, and thus human oocytes are potentially more prone to lethal IIF during a freezethaw cycle. Increasing the seeding temperature was found to provide a narrow window for human oocytes to dehydrate without incurring IIF. Modification of a freezing protocol accordingly was associated with excellent survival rates of human oocytes. These conclusions might be extrapolated to the cryopreservation of fresh mature human oocytes and to human pronucleate embryos.
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Acknowledgments |
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Notes |
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5 To whom correspondence should be addressed
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References |
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Submitted on July 17, 1998; accepted on January 29, 1999.