Extracellular freezing in leaves of freezing-sensitive species

Low-temperature scanning-electron microscopy was used to study the freezing of leaves of five species that have no resistance to freezing: bean (Phaseolus vulgaris L.), tobacco (Nicotiana tabacum L.), tomato (Lycopersicon esculentum L.), cucumber (Cucumis sativus L.), and corn (Zea mays L.). In the leaves of the four dicotyledonous species, ice was extracellular and the cells of all tissues were collapsed. In contrast, in maize leaves ice was extracellular in the mesophyll, and these cells were collapsed, but the epidermal and bundle-sheath cells apparently retained their original shapes and volume. It is concluded that the leaves of the freezing-sensitive dicotyledonous species tested were killed by cellular dehydration induced by extracellular freezing, and not by intracellular freezing. Freezing injury in maize leaves apparently resulted from a combination of freezing-induced cellular dehydration of some cells and intracellular ice formation in epidermal and bundle-sheath cells.     

Relation of ice formation to ultrastructural cryoinjury and cryoprotection of rough endoplasmic reticulum

Ultrastructural observations on the frozen state of pancreatic acinar cells were correlated with results of parallel studies before freezing and after thawing, as to cryoinjury and cryoprotection.Data support an hypothesis of freezing injury based upon intracellular ice and solution effects during rapid and slow freezing, respectively. The basis for superiority of extracellular over intracellular glycerol in cryoprotection was demonstrated in terms of these factors.Evidence is offered to explain the ultrastructural cryoinjury and cryoprotection of rough endoplasmic reticulum (RER) seen after thawing, relative to the combined effects of freezing rate and glycerol. Slow freezing, in combination with the presence of extracellular glycerol, provided sufficient dehydration to almost completely suppress intracellular ice formation, yielding minimal ultrastructural alteration of RER. Greatest cryoinjury, expressed as extensive conversion of RER into sphere-like vesicles, was induced by the extensive intracellular ice formation which accompanied rapid freezing. A mechanism is suggested to explain physical damage of RER by intracellular ice.     

A theoretical model of intracellular devitrification

Devitrification of the intracellular solution can cause significant damage during warming of cells cryopreserved by freezing or vitrification. Whereas previous theoretical investigations of devitrification have not considered the effect of cell dehydration on intracellular ice formation, a new model which couples membrane-limited water transport equations, classical nucleation theory, and diffusion-limited crystal growth theory is presented. The model was used to explore the role of cell dehydration in devitrification of human keratinocytes frozen in the presence of glycerol. Numerical simulations demonstrated that water transport during cooling affects subsequent intracellular ice formation during warming, correctly predicting observations that critical warming rate increases with increasing cooling rate. However, for cells with a membrane transport activation energy less than approximately 50 kJ/mol, devitrification was also affected by cell dehydration during warming, leading to a reversal of the relationship between cooling rate and critical warming rate. Thus, for low warming rates (less than 10 degrees C/min for keratinocytes), the size and total volume fraction of intracellular ice crystals forming during warming decreased with decreasing warming rate, and the critical warming rate decreased with increasing cooling rate. The effects of water transport on the kinetics of intracellular nucleation and crystal growth were elucidated by comparison of simulations of cell warming with simulations of devitrification in H(2)O-NaCl-glycerol droplets of constant size and composition. These studies showed that the rate of intracellular nucleation was less sensitive to cell dehydration than was the crystal growth rate. The theoretical methods presented may be of use for the design and optimization of freeze-thaw protocols.     

Investigating cryoinjury using simulations and experiments: 2. TF-1 cells during graded freezing (interrupted slow cooling without hold time)

Cryopreservation plays a key role in the long-term storage of native and engineered cells and tissues for research and clinical applications. The survival of cells and tissues after freezing and thawing depends on the ability of the cells to withstand a variety of stresses imposed by the cryopreservation protocol. A better understanding of the nature and kinetics of cellular responses to temperature-induced conditions is required to minimize cryoinjury. An interrupted freezing procedure that allows dissection of cryoinjury was used to investigate the progressive damage that occurs to cells during cryopreservation using slow cooling. Simulations of cellular osmotic responses were used to provide interpretation linking states of the cell with events during the freezing procedure. Simulations of graded freezing (interrupted slow cooling without hold time) were correlated with cell recovery results of TF-1 cells. Calculated intracellular supercooling and osmolality, were used as indicators of the probability of cryoinjury due to intracellular ice formation and solution effects, providing direct links of cellular conditions to events in the freezing process. Using simulations, this study demonstrated that both intracellular supercooling and osmolality are necessary to explain graded freezing results.     

Intracellular ice formation and growth in MCF-7 cancer cells

Direct cell injury in cryosurgery is highly related to intracellular ice formation (IIF) during tissue freezing and thawing. Mechanistic understanding of IIF in tumor cells is critical to the development of tumor cryo-ablation protocol. In aid of a high speed CMOS camera system, the events of IIF in MCF-7 cells have been studied using cryomicroscopy. Images of ‘darkening’ type IIF and recrystallization are compared between cells frozen with and without ice seeding. It is found that ice seeding has significant impact on the occurrence and growth of intracellular ice. Without ice seeding, IIF is observed to occur over a very small range of temperature (∼1 °C). The crystal dendrites are indistinguishable, which is independent of the cooling rate. Ice crystal grows much faster and covers the whole intracellular space in comparison to that with ice seeding, which ice stops growing near the cellular nucleus. Recrystallization is observed at the temperature from −13 °C to −9 °C during thawing. On the contrary, IIF occurs from −7 °C to −20 °C with ice seeding at a high subzero temperature (i.e., −2.5 °C). The morphology of intracellular ice frozen is greatly affected by the cooling rate, and no ‘darkening’ type ice formed inside cells during thawing. In addition, the intracellular ice formation is directional, which starts from the plasma membrane and grows toward the cellular nucleus with or without ice seeding. These results can be used to explain some findings of tumor cryosurgery in vivo, especially the causes of insufficient killing of tumor cells in the peripheral area near vessels.     

Hemolysis in several animal species after rapid freezing of blood

The effect of various freezing rates on the extent of hemolysis in human, bovine and ovine erythrocytes, which are known to have different cell volumes, water contents and permeabilities, was investigated. Blood in stainless steel capillary tubes was frozen at various rates by abrupt immersion of the capillaries into cooling baths at temperatures ranging from ?20° to ?130°C. Minimum lysis values were obtained at freezing temperatures of ?40°, ?50° and ?70°C with, respectively, human, bovine and ovine blood. The smallest, highly permeable sheep erythrocytes were the least damaged at the highest freezing rates; the largest human cells with the highest water content, suffered the greatest damage; intermediate values were obtained with ox blood. At the lower freezing rates, the largest, human cells were the least damaged; the highest hemolysis values were obtained with the smallest, highly permeable sheep erythrocytes; ox blood again gave intermediate values. These results are in agreement with current views that, (1) very rapid freezing results in the formation of damaging intracellular ice; (2) injury associated with slow freezing is related to the extent of dehydration or to the increase in electrolyte concentration which accompanies ice formation; (3) minimum hemolysis is obtained under those freezing conditions in which osmotic dehydration has been sufficient to prevent the formation of intracellular ice, but has left enough water in the cells to prevent the damaging effects of dehydration and high electrolyte concentrations.     

Ice crystals formed in tissue during cryosurgery. II. Electron microscopy

Tissues frozen by means of a cryosurgical probe have been examined by electron microscopy following techniques designed to preserve the ice crystal spaces.Ice crystals appeared similar whether tissues were quenched or not following cryosurgery and the various techniques of dehydration resulted in similar ice crystal architecture.Ice crystal spaces in the area deep to the freezing probe were intracellular both in epithelium and muscle although in the muscle zone some fibers contained large and others small crystal spaces. It is suggested that this might be due to variations in the local blood supply.At the periphery of the frozen area ice crystals were usually extracellular producing gross distortion of the cells which, however, retained intracellular structural integrity. These results are consistent with the belief of many workers that intracellular ice is lethal while extracellular ice is not, but no evidence of penetration of cell membrane by ice crystals was seen.     

Effects of freezing on membranes and proteins in LNCaP prostate tumor cells

Fourier transform infrared spectroscopy (FTIR) and cryomicroscopy were used to define the process of cellular injury during freezing in LNCaP prostate tumor cells, at the molecular level. Cell pellets were monitored during cooling at 2 degrees C/min while the ice nucleation temperature was varied between -3 and -10 degrees C. We show that the cells tend to dehydrate precipitously after nucleation unless intracellular ice formation occurs. The predicted incidence of intracellular ice formation rapidly increases at ice nucleation temperatures below -4 degrees C and cell survival exhibits an optimum at a nucleation temperature of -6 degrees C. The ice nucleation temperature was found to have a great effect on the membrane phase behavior of the cells. The onset of the liquid crystalline to gel phase transition coincided with the ice nucleation temperature. In addition, nucleation at -3 degrees C resulted in a much more co-operative phase transition and a concomitantly lower residual conformational disorder of the membranes in the frozen state compared to samples that nucleated at -10 degrees C. These observations were explained by the effect of the nucleation temperature on the extent of cellular dehydration and intracellular ice formation. Amide-III band analysis revealed that proteins are relatively stable during freezing and that heat-induced protein denaturation coincides with an abrupt decrease in alpha-helical structures and a concomitant increase in beta-sheet structures starting at an onset temperature of approximately 48 degrees C.     

An Improved Model for Nucleation-Limited Ice Formation in Living Cells during Freezing

Ice formation in living cells is a lethal event during freezing and its characterization is important to the development of optimal protocols for not only cryopreservation but also cryotherapy applications. Although the model for probability of ice formation (PIF) in cells developed by Toner et al. has been widely used to predict nucleation-limited intracellular ice formation (IIF), our data of freezing Hela cells suggest that this model could give misleading prediction of PIF when the maximum PIF in cells during freezing is less than 1 (PIF ranges from 0 to 1). We introduce a new model to overcome this problem by incorporating a critical cell volume to modify the Toner''s original model. We further reveal that this critical cell volume is dependent on the mechanisms of ice nucleation in cells during freezing, i.e., surface-catalyzed nucleation (SCN) and volume-catalyzed nucleation (VCN). Taken together, the improved PIF model may be valuable for better understanding of the mechanisms of ice nucleation in cells during freezing and more accurate prediction of PIF for cryopreservation and cryotherapy applications.     

Experimental study of intracellular ice growth in human umbilical vein endothelial cells

Study of the intracellular ice formation (IIF) and growth is essential to the mechanistic understanding of cellular damage through freezing. In the aid of high speed and high resolution cryo-imaging technology, the transient intracellular ice formation and growth processes of the attached human umbilical vein endothelial cells (HUVEC) were successfully captured during freezing. It was found that the intracellular ice nucleation site was on the cell membrane closer to the nucleus. The ice growth was directional and toward the nucleus, which covered the whole nucleus before growing into the cytoplasm. The crystal growth rate in the nucleus was much larger than that in the cytoplasm, and its morphology was influenced by the cooling rate. During the thawing process, small crystals fused into larger ones inside the nucleus. Moreover, the cumulative fraction of the HUVEC with IIF was mainly dependent on the cooling rate not the confluence of the cells attached.     

Plant Freezing and Damage

Imaging methods are giving new insights into plant freezingand the consequent damage that affects survival and distributionof both wild and crop plants. Ice can enter plants through stomataand hydathodes. Intrinsic nucleation of freezing can also occur.The initial growth of ice through the plant can be as rapidas 40 mm s^-1, although barriers can limit this growth. Onlya small fraction of plant water is changed to ice in this firstfreezing event. Nevertheless, this first rapid growth of iceis of key importance because it can initiate further, potentiallylethal, freezing at any site that it reaches. Some organs andtissues avoid freezing by supercooling. However, supercooledparts of buds can dehydrate progressively, indicating that avoidanceof freezing-induced dehydration by deep supercooling is onlypartial. Extracellular ice forms in freezing-intolerant as wellas freezing-tolerant species and causes cellular dehydration.The single most important cause of freezing-damage is when thisdehydration exceeds what cells can tolerate. In freezing-adaptedspecies, lethal freezing-induced dehydration causes damage tocell membranes. In specific cases, other factors may also causedamage, examples being cell death when limits to deep supercoolingare exceeded, and death of shoots when freezing-induced embolismsin xylem vessels persist. Extracellular masses of ice can damagethe structure of organs but this may be tolerated, as in extra-organfreezing of buds. Experiments to genetically engineer expressionof fish antifreeze proteins have not improved freezing toleranceof sensitive species. A better strategy may be to confer toleranceof cellular dehydration.Copyright 2001 Annals of Botany Company Freezing, dehydration, infrared video thermography, low temperature scanning electron microscopy, NMR micro-imaging     

Mechanisms of intracellular ice formation.

The phenomenon of intracellular freezing in cells was investigated by designing experiments with cultured mouse fibroblasts on a cryomicroscope to critically assess the current hypotheses describing the genesis of intracellular ice: (a) intracellular freezing is a result of critical undercooling; (b) the cytoplasm is nucleated through aqueous pores in the plasma membrane; and (c) intracellular freezing is a result of membrane damage caused by electrical transients at the ice interface. The experimental data did not support any of these theories, but was consistent with the hypothesis that the plasma membrane is damaged at a critical gradient in osmotic pressure across the membrane, and intracellular freezing occurs as a result of this damage. An implication of this hypothesis is that mathematical models can be used to design protocols to avoid damaging gradients in osmotic pressure, allowing new approaches to the preservation of cells, tissues, and organs by rapid cooling.     

Microscopic and Calorimetric Assessment of Freezing Processes in Uterine Fibroid Tumor Tissue

The use of cryosurgery in the treatment of uterine fibroids is emerging as a possible treatment modality. The two known mechanisms of direct cell injury during the tissue freezing process are linked to intracellular ice formation and cellular dehydration. These processes have not been quantified within uterine fibroid tumor tissue. This study reports the use of a combination of freeze-substitution microscopy and differential scanning calorimetry (DSC) to quantify freeze-induced dehydration within uterine fibroid tumor tissue. Stereological analysis of histological tumor sections was used to obtain the initial cellular volume (V(o)) or the Krogh model dimensions (deltaX, the distance between the microvascular channels = 15.5 microm, r(vo), the initial radius of the extracellular space = 4.8 micro m, and L, the axial length of the Krogh cylinder = 19.1 microm), the interstitial volume ( approximately 23%), and the vascular volume ( approximately 7%) of the fibroid tumor tissue. A Boyle-van't Hoff plot was then constructed by examining freeze-substituted micrographs of "equilibrium"-cooled tissue slices to obtain the osmotically inactive cell volume, V(b) = 0.47V(o). The high interstitial volume precludes the use of freeze-substitution microscopy data to quantify freeze-induced dehydration. Therefore, a DSC technique, which does not suffer from this artifact, was used to obtain the water transport data. A model of water transport was fit to the calorimetric data at 5 and 20 degrees C/min to obtain the "combined best fit" membrane permeability parameters of the embedded fibroid tumor cells, assuming either a Krogh cylinder geometry, L(pg) = 0.92 x 10(-13) m(3)/Ns (0.55 microm/min atm) and E(Lp) = 129.3 kJ/mol (30.9 kcal/mol), or a spherical cell geometry (cell diameter = 18.3 microm), L(pg) = 0.45 x 10(-13) m(3)/Ns (0.27 microm/min atm) and E(Lp) = 110.5 kJ/mol (26.4 kcal/mol). In addition, numerical simulations were performed to generate conservative estimates, in the absence of ice nucleation between -5 and -30 degrees C, of intracellular ice volume in the tumor tissue at various cooling rates typical of those experienced during cryosurgery (< or =100 degrees C/min). With this assumption, the Krogh model simulations showed that the fibroid tumor tissue cells cooled at rates < or = 50 degrees C/min are essentially dehydrated; however, at rates >50 degrees C/min the amount of water trapped within the tissue cells increases rapidly with increasing cooling rate, suggesting the formation of intracellular ice.     

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.     

Ultrastructure before freezing,while frozen,and after thawing in assessing cryoinjury of mouse epididymal spermatozoa

Tails of mouse epididymides were treated as follows: control, unfrozen with and without cryoprotective agents (CPA); frozen (to below ?80 °C), slowly (8 °C/min), and rapidly (18 °C/sec), with and without CPA. Intracellular and/or extracellular location of CPA, at least glycerol, was influenced, respectively, by high (22 °C) or low (0 °C) exposure temperature. Standard procedures in electron microscopy were employed and the frozen state preserved by freeze-substitution. Motility before freezing and after thawing was the criterion of cryosurvival.Results showed no evidence of deleterious ultrastructural effects of freezing at rates compared, or of benefits of CPA, regardless of their cellular location. Differences were noted, however, in the appearance of spermatozoa in the frozen state, as a function of the rate of freezing but not as a function of the presence, absence, or location of either glycerol of DMSO. Rapidly frozen cells showed intracellular ice formation in the acrosome, neck, midpiece, and tail regions; there was no intranuclear ice, and extracellular ice artifacts were small. Slowly frozen cells showed large extracellular ice artifacts with evidence of shrinkage distortion due to the dehydration induced by extracellular ice. No spermatozoa survived any of the freezing treatments, showing the lethal effect of both extracellular ice during slow freezing and of intracellular and/or extracellular ice during rapid freezing.     

Do physical forces contribute to cryodamage?

To achieve the ultimate goal of both cryosurgery and cryopreservation, a thorough understanding of the processes responsible for cell and tissue damage is desired. The general belief is that cells are damaged primarily due to osmotic effects at slow cooling rates and intracellular ice formation at high cooling rates, together termed the “two factor theory.” The present study deals with a third, largely ignored component—mechanical damage. Using pooled bull sperm cells as a model and directional freezing in large volumes, samples were frozen in the presence or absence of glass balls of three different diameters: 70–110, 250–500, and 1,000–1,250 µm, as a means of altering the surface area with which the cells come in contact. Post‐thaw evaluation included motility at 0 h and after 3 h at 37°C, viability, acrosome integrity, and hypoosmotic swelling test. Interactions among glass balls, sperm cells, and ice crystals were observed by directional freezing cryomicroscopy. Intra‐container pressure in relation to volume was also evaluated. The series of studies presented here indicate that the higher the surface area with which the cells come in contact, the greater the damage, possibly because the cells are squeezed between the ice crystals and the surface. We further demonstrate that with a decrease in volume, and thus increase in surface area‐to‐volume ratio, the intra‐container pressure during freezing increases. It is suggested that large volume freezing, given that heat dissipation is solved, will inflict less cryodamage to the cells than the current practice of small volume freezing. Biotechnol. Bioeng. 2009; 104: 719–728 © 2009 Wiley Periodicals, Inc.     

Effects of freezing on membranes and proteins in LNCaP prostate tumor cells

Fourier transform infrared spectroscopy (FTIR) and cryomicroscopy were used to define the process of cellular injury during freezing in LNCaP prostate tumor cells, at the molecular level. Cell pellets were monitored during cooling at 2 °C/min while the ice nucleation temperature was varied between − 3 and − 10 °C. We show that the cells tend to dehydrate precipitously after nucleation unless intracellular ice formation occurs. The predicted incidence of intracellular ice formation rapidly increases at ice nucleation temperatures below − 4 °C and cell survival exhibits an optimum at a nucleation temperature of − 6 °C. The ice nucleation temperature was found to have a great effect on the membrane phase behavior of the cells. The onset of the liquid crystalline to gel phase transition coincided with the ice nucleation temperature. In addition, nucleation at − 3 °C resulted in a much more co-operative phase transition and a concomitantly lower residual conformational disorder of the membranes in the frozen state compared to samples that nucleated at − 10 °C. These observations were explained by the effect of the nucleation temperature on the extent of cellular dehydration and intracellular ice formation. Amide-III band analysis revealed that proteins are relatively stable during freezing and that heat-induced protein denaturation coincides with an abrupt decrease in α-helical structures and a concomitant increase in β-sheet structures starting at an onset temperature of approximately 48 °C.     

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.     

Membrane permeability parameters for freezing of stallion sperm as determined by Fourier transform infrared spectroscopy

Cellular membranes are one of the primary sites of injury during freezing and thawing for cryopreservation of cells. Fourier transform infrared spectroscopy (FTIR) was used to monitor membrane phase behavior and ice formation during freezing of stallion sperm. At high subzero ice nucleation temperatures which result in cellular dehydration, membranes undergo a profound transition to a highly ordered gel phase. By contrast, low subzero nucleation temperatures, that are likely to result in intracellular ice formation, leave membrane lipids in a relatively hydrated fluid state. The extent of freezing-induced membrane dehydration was found to be dependent on the ice nucleation temperature, and showed Arrhenius behavior. The presence of glycerol did not prevent the freezing-induced membrane phase transition, but membrane dehydration occurred more gradual and over a wider temperature range. We describe a method to determine membrane hydraulic permeability parameters (E_Lp, Lpg) at subzero temperatures from membrane phase behavior data. In order to do this, it was assumed that the measured freezing-induced shift in wavenumber position of the symmetric CH₂ stretching band arising from the lipid acyl chains is proportional to cellular dehydration. Membrane permeability parameters were also determined by analyzing the H₂O-bending and -libration combination band, which yielded higher values for both E_Lp and Lpg as compared to lipid band analysis. These differences likely reflect differences between transport of free and membrane-bound water. FTIR allows for direct assessment of membrane properties at subzero temperatures in intact cells. The derived biophysical membrane parameters are dependent on intrinsic cell properties as well as freezing extender composition.     

Membrane hydration correlates to cellular biophysics during freezing in mammalian cells

Cell survival during freezing applications in biomedicine is highly correlated to the temperature history and its dependent cellular biophysical events of dehydration and intracellular ice formation (IIF). Although cell membranes are known to play a significant role in cell injury, a clear correlation between the membrane state and the surrounding intracellular and extracellular water is still lacking. We previously showed that lipid hydration in LNCaP tumor cells is related to cellular dehydration. The goal of this study is to build upon this work by correlating both the phase state of the membrane and the surrounding water to cellular biophysical events in three different mammalian cell types: human prostate tumor cells (LNCaP), human dermal fibroblasts (HDF), and porcine smooth muscle cells (SMC) using Fourier Transform Infrared spectroscopy (FTIR). Variable cooling rates were achieved by controlling the degree of supercooling prior to ice nucleation (− 3 °C and − 10 °C) while the sample was cooled at a set rate of 2 °C/min. Membranes displayed a highly cooperative phase transition under dehydrating conditions (i.e. NT = − 3 °C), which was not observed under IIF conditions (NT = − 10 °C). Spectral analysis showed a consistently greater amount of ice formation during dehydrating vs. IIF conditions in all cell types. This is hypothesized to be due to the extreme loss of membrane hydration in dehydrating cells that is manifested as excess water available for phase change. Interestingly, changes in residual membrane conformational disorder correlate strongly with cellular volumetric decreases as assessed by cryomicroscopy. A strong correlation was also found between the activation energies for freezing induced lyotropic membrane phase change determined using FTIR and the water transport measured by cryomicroscopy. Reduced lipid hydration under dehydration freezing conditions is suggested as one of the likely causes of what has been termed as “solution effects” injury in cryobiology.