Measurements of the membrane water permeability (Lp) and its temperature dependence (activation energy) in human fresh and failed-to-fertilize oocytes and mouse oocyte.

The volumetric response of oocytes during rapid alterations of the extracellular osmotic environment were recorded using video microscopy. From these observations, the kinetics of water loss for human and mouse oocytes were determined over the temperature range 37 to 10 degrees C, including 37, 30, 20, and 10 degrees C. The changes in diameter of oocytes were measured over a 5-min period and a computer model was used to derive values for membrane water permeability (Lp) and inactive volume (Vb) and to compare the experimental data to the predicted values. The results for the mouse oocyte Lp were comparable to values determined by other methods. However the human data, for both failed-to-fertilize and fresh oocytes, have a wide range of values with large standard deviations. The Lp values at the various temperatures were used to calculate the Arrhenius activation energy (Ea). An Ea value of 9.48 kcal/mol was found for the fresh mouse oocyte, whereas the activation energy for human oocytes was extremely low, 3.73 kcal/mol for fresh oocytes and 1.93 kcal/mol for failed-to-fertilize oocytes.     

Osmotic gradient-induced water permeation across the sarcolemma of rabbit ventricular myocytes

The mechanism of water permeation across the sarcolemma was characterized by examining the kinetics and temperature dependence of osmotic swelling and shrinkage of rabbit ventricular myocytes. The magnitude of swelling and the kinetics of swelling and shrinkage were temperature dependent, but the magnitude of shrinkage was very similar at 6 degrees, 22 degrees, and 37 degrees C. Membrane hydraulic conductivity, Lp, was approximately 1.2 x 10(-10) liter.N-1.s-1 at 22 degrees C, corresponding to an osmotic permeability coefficient, Pf, of 16 microns.s-1, and was independent of the direction of water flux, the magnitude of the imposed osmotic gradient (35-165 mosm/liter), and the initial cell volume. This value of Lp represents an upper limit because the membrane was assumed to be a smooth surface. Based on capacitive membrane area, Lp was 0.7 to 0.9 x 10(-10) liter.N-1.s-1. Nevertheless, estimates of Lp in ventricle are 15 to 25 times lower than those in human erythrocytes and are in the range of values reported for protein- free lipid bilayers and biological membranes without functioning water channels (aquaporin). Evaluation of the effect of unstirred layers showed that in the worst case they decrease Lp by < or = 2.3%. Analysis of the temperature dependence of Lp indicated that its apparent Arrhenius activation energy, Ea', was 11.7 +/- 0.9 kcal/mol between 6 degrees and 22 degrees C and 9.2 +/- 0.9 kcal/mol between 22 degrees and 37 degrees C. These values are significantly greater than that typically found for water flow through water-filled pores, approximately 4 kcal/mol, and are in the range reported for artificial and natural membranes without functioning water channels. Taken together, these data strongly argue that the vast majority of osmotic water flux in ventricular myocytes penetrates the lipid bilayer itself rather than passing through water-filled pores.     

Studies on membrane permeability of zebrafish (Danio rerio) oocytes in the presence of different cryoprotectants

Investigation into fish oocyte membrane permeability is essential for developing successful protocols for their cryopreservation. The aim of the present work was to study the permeability of the zebrafish (Danio rerio) oocyte membrane to water and cryoprotectants before cryopreservation protocol design. The study was conducted on stage III and stage V zebrafish oocytes. Volumetric changes of stage III oocytes in different concentrations of sucrose were measured after 20 min exposure at 22 degrees C and the osmotically inactive volume of the oocytes (Vb) was determined using the Boyle-van't Hoff relationship. Volumetric changes of oocytes during exposure to different cryoprotectant solutions were also measured. Oocytes were exposed to 2 M dimethyl sulphoxide (DMSO), propylene glycol (PG), and methanol for 40 min at 22 degrees C. Stage III oocytes were also exposed to 2 M DMSO at 0 degrees C. Oocyte images were captured on an Olympus BX51 cryomicroscope using Linkham software for image recording. Scion Image was used for image analysis and diameter measurement. The experimental data were fitted to a two-parameter model using Berkeley Madonna 8.0.1 software. Hydraulic conductivity (L(p)) and solute (cryoprotectant) permeability (Ps) were estimated using the model. The osmotically inactive volume of stage III zebrafish oocytes was found to be 69.5%. The mean values+/-SE of Lp were found to be 0.169+/-0.02 and 0.196+/-0.01 microm/min/atm in the presence of DMSO and PG, respectively, at 22 degrees C, assuming an internal isosmotic value for the oocyte of 272 mOsm. The Ps values were 0.000948+/-0.00015 and 0.000933+/-0.00005 cm/min for DMSO and PG, respectively. It was also shown that the membrane permeability of stage III oocytes decreased significantly with temperature. No significant changes in cell volume during methanol treatment were observed. Fish oocyte membrane permeability parameters are reported here for the first time. The Lp and Ps values obtained for stage III zebrafish oocytes are generally lower than those obtained from successfully cryopreserved mammalian oocytes and higher than those obtained with fish embryos and sea urchin eggs. It was not possible to estimate membrane permeability parameters for stage V oocytes using the methods employed in this study because stage V oocytes experienced the separation of outer oolemma membrane from inner vitelline during exposure to cryoprotectants.     

Measurement of the water permeability of single human granulocytes on a microscopic stopped-flow mixing system

The water permeability (Lp) of human granulocytes was measured for individual isolated cells with a novel, microscopic stopped-flow mixing system. Changes in volume were monitored as a cell was introduced suddenly into an osmotically active solution. Permeability values were determined as a function of solution osmolality from the volume versus time curves for mixing into both hypotonic and hypertonic solutions within the range of 145 to 833 mOsm. The calculated reference permeability at 25 degrees C was 1.15 micrometers/atm.min with an osmotic coefficient of 0.46 Osm/kg.     

Temperature-dependent osmotic behavior of germinal vesicle and metaphase II stage bovine oocytes in the presence of Me2SO in relationship to cryobiology

Plasma membrane permeability coefficients and their activation energies (Ea) for water (Lp) and dimethyl sulfoxide (PMe2SO) as well as the reflection coefficient (sigma) were determined for germinal vesicle (GV) and metaphase II (MII) bovine oocytes. A micropipette perfusion technique was used with a temperature controlled circulation chamber, which was adapted to a micromanipulator. Experiments were performed at five different temperatures (30, 20, 10, 4 and -3 degrees C). The Kedem and Katchalsky model was assumed and L(p), P(Me2SO) and sigma were estimated. Estimated permeability values from the experimental temperatures were then applied to Arrhenius plots In(Lp) or In(PMe2SO) vs 1/Temperature (K) to estimate the activation energies (Ea) for L(p)Me2SO and P(Me2SO). The estimated E(a) for L(p)Me2SO for GV and MII oocytes were 23.84 Kcal/mol and 8.46 Kcal/mol, respectively. The E(a) for P(Me2SO) were 21.0 Kcal/mol and 23.20 Kcal/mol, respectively. The correlation (r2) for these linear regression plots for GV oocytes were 0.83 and 0.95 for L(p)Me2SO and P(Me2SO), respectively. For MII oocytes, r2 values were 0.95 and 0.99 for L(p)Me2SO and P(Me2SO), respectively. There was a possible discontinuity detected in the Arrhenius plot for L(p)Me2SO for GV oocytes. A significant decrease of the reflection coefficient was observed at 10 degrees C compared to other experimental temperatures. These data provide a fundamental basis that should be taken into account for low temperature preservation of bovine oocytes in the presence of Me2SO.     

Effects of temperature on water diffusion in human erythrocytes and ghosts--nuclear magnetic resonance studies

The temperature-dependence of water diffusion across human erythrocyte membrane was studied on isolated erythrocytes and resealed ghosts by a doping nuclear magnetic resonance technique. The conclusions are the following: (1) The storage of suspended erythrocytes at 2 degrees C up to 24 h or at 37 degrees C for 30 min did not change the water exchange time significantly, even if Mn2+ was present in the medium. This indicates that no significant penetration of Mn2+ is taking place under such conditions. (2) In case of cells previously incubated at 37 degrees C for longer than 30 min with concentrations of p-chloromercuribenzene sulfonate (PCMBS) greater than 0.5 mM, the water-exchange time gradually decreased if the cells were stored in the presence of Mn2+ for more than 10 min at 37 degrees C. (3) When the Arrhenius plot of the water-exchange time was calculated on the basis of measurements performed in such a way as to avoid a prolonged exposure of erythrocytes to Mn2+ no discontinuity occurred, regardless of the treatment with PCMBS. (4) No significant differences between erythrocytes and resealed ghosts regarding their permeability and the activation energy of water diffusion (Ea,d) were noticed. The mean value of Ea,d obtained on erythrocytes from 35 donors was 24.5 kJ/mol. (5) The value of Ea,d increased after treatment with PCMBS, in parallel with the percentage inhibition of water diffusion. A mean value of 41.3 kJ/mol was obtained for Ea,d of erythrocytes incubated with 1 mM PCMBS for 60 min at 37 degrees C and 28.3 kJ/mol for ghosts incubated with 0.1 mM PCMBS for 15 min, the values of inhibition being 46% and 21% respectively.     

High channel-mediated water permeability in rabbit erythrocytes: characterization in native cells and expression in Xenopus oocytes.

Erythrocytes from several mammalian species contain mercurial-sensitive water transporters. By a stopped-flow light scattering technique, osmotic water permeability (Pf) was exceptionally high in rabbit erythrocytes (0.053 +/- 0.002 cm/s) and reversibly inhibited by 98% by p-(chloromercuri)benzenesulfonate (pCMBS). The activation energy (Ea) was 4.6 kcal/mol (15-37 degrees C). pCMBS inhibition was half-maximal at 0.1 mM (60-min incubation); at 1 mM pCMBS, half-maximal inhibition occurred in 8 min. Pf was also inhibited by HgCl2 and pCMB with greater than 90% inhibition in 5 min. There was no inhibition by high concentrations of phloretin, DNDS, cytochalasin B, amiloride, ouabain, furosemide, and several proteases. In defolliculated Xenopus oocytes microinjected with 50 nL of water or unfractionated mRNA (1 mg/mL) from rabbit reticulocytes, oocyte Pf assayed at 10 degrees C after 72-h incubation increased from (4 +/- 1) X 10(-4) cm/s (water injected) to (18 +/- 2) X 10(-4) cm/s (mRNA injected). Pf increased linearly with [mRNA] (0-75 ng/oocyte) and was inhibited slowly and reversibly by pCMBS and immediately by HgCl2 but not by cytochalasin B, phloretin, or DNDS. Ea was 9.6 kcal/mol (water injected) and 2.6 kcal/mol (mRNA injected). These results demonstrate that rabbit erythrocytes have the highest Pf and the greatest percentage inhibition of Pf by mercurials of any mammalian erythrocyte studied. The characteristics of the expressed and native water channels were similar, suggesting that the erythrocyte water channel is a membrane protein suitable for expression cloning.     

Effects of temperature on the transport of nucleosides in guinea pig erythrocytes

The initial rate of [14C]uridine transport by guinea pig erythrocytes was investigated at different temperatures. At 37, 22, and 10 degrees C the concentration dependence of uridine zero-trans influx and equilibrium exchange influx was resolved into two components; (a) a saturable component which followed simple Michaelis-Menten kinetics and which was inhibited by nitrobenzylthioinosine, and (b) a linear component of low magnitude and insensitive to nitrobenzylthioinosine inhibition. The maximum velocity, Vmax, of zero-trans uridine influx for the saturable transport system was 70-fold higher at 37 than 10 degrees C (1.24, 0.20, and 0.018 mmol/L of cells per hour at 37, 22, and 10 degrees C, respectively). Similarly, the apparent affinity, Km, for zero-trans influx decreased as the temperature was lowered (0.27, 0.066, and 0.038 mM at 37, 22, and 10 degrees C, respectively). In contrast, uridine equilibrium exchange influx was less temperature dependent (Vmax, 2.80, 0.89, and 0.14 mmol/L of cells per hour; apparent Km 0.61, 0.36, and 0.24 mM at 37, 22, and 10 degrees C, respectively). These results demonstrate that the mobility of the empty carrier is impaired to a greater extent than the mobility of the loaded carrier temperature decreased. However, the kinetic constants for zero-trans uridine influx and efflux at 37 degrees C were similar, indicating that the nucleoside transporter exhibited directional symmetry at 37 degrees C. Arrhenius plots of the maximum velocity for equilibrium exchange and zero-trans uridine influx were discontinuous above 25 degrees C, but between 20 and 5 degrees C the plots were linear (Ea = 22 and 30 kcal/mol for equilibrium exchange and zero-trans influx, respectively.     

Effect of temperature on kinetics and differential mobility of empty and loaded nucleoside transporter of human erythrocytes

The transmembrane equilibration of [3H]uridine was measured in human erythrocytes as a function of temperature using rapid kinetic techniques. Arrhenius plots of the maximum velocity of equilibrium exchange were continuous between 5 and 30 degrees C (Ea = 17-20 kcal/mol), but the increase in velocity with increase in temperature leveled off above 30 degrees C. This leveling off did not reflect heat inactivation of the carrier since transport activity was stable for 3 h at 37 degrees C. Transmembrane equilibration of uridine in equilibrium exchange and zero-trans modes at 5, 15, 25, and 35 degrees C conformed to appropriate integrated rate equations derived for the simple transporter. The nucleoside transporter exhibited directional symmetry, but the loaded carrier moved on the average 5 times more rapidly than the empty carrier at 15, 25, and 35 degrees C, but 25-40 times faster at 5 degrees C. This marked shift in differential mobility of loaded and empty carrier between 15 and 5 degrees C was entirely attributable to an impairment of mobility of empty carrier. The Michaelis-Menten constant for equilibrium exchange increased about 3-fold with increase in temperature between 5 and 35 degrees C. The van't Hoff plot of the values was approximately linear and yielded an estimate of the enthalpy of carrier:substrate dissociation of 7.8 kcal/mol.     

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.     

Assessment of canine oocyte viability after transportation and storage under different conditions

To improve assisted reproductive technologies in the domestic dog, different transport treatments were evaluated for their ability to maintain viability of canine oocytes, as assessed by esterase activity 8h after storage or after 48 h of in vitro maturation (IVM) culture. In Experiment 1, ovaries were transported within reproductive tracts or were excised and stored at either 20 or 37 degrees C in phosphate buffered saline. Oocytes collected from reproductive tracts transported at 37 degrees C had the greatest viability after storage (P<0.05). However, after IVM there were no significant differences among any of the four storage conditions in oocyte viability or meiotic resumption (P=0.05). In Experiment 2, isolated oocytes were transported in either TCM-199 with Hank's salts and Hepes buffer or in TL-Hepes at either 20 or 37 degrees C, or in maturation medium equilibrated with 5% CO(2) at 37 degrees C. In Experiment 2, oocytes transported in Hepes buffered media at 37 degrees C had greater viability rates after storage than did those transported in these same media at 20 degrees C or in sodium bicarbonate buffered medium at 37 degrees C (P<0.001). After IVM, oocytes transported in the 37 degrees C treatment groups had greater viability rates than did those transported at 20 degrees C (P<0.01). Overall, isolated oocytes transported at 37 degrees C had greater rates of meiotic resumption than did those transported at 20 degrees C (P<0.05). Taken together, these data indicate that canine oocytes exhibited sensitivity to lesser temperatures and maintained greater rates of viability during transport at 37 degrees C. Isolated oocytes maintained greater viability than oocytes transported in situ. Hepes buffered media increased viability rates for isolated oocytes transported at 37 degrees C compared to a similar medium buffered with sodium bicarbonate.     

Light-induced transpiration alters cell water relations in figleaf gourd (Cucurbita ficifolia) seedlings exposed to low root temperatures

Water relation parameters including elastic modulus (epsilon), half-times of water exchange (T(w)(1/2)), hydraulic conductivity and turgor pressure (P) were measured in individual root cortical and cotyledon midrib cells in intact figleaf gourd (Cucurbita ficifolia) seedlings, using a cell pressure probe. Transpiration rates (E) of cotyledons were also measured using a steady-state porometer. The seedlings were exposed to low ambient (approximately 10 micromol m(-2) s(-1)) or high supplemental irradiance (approximately 300 micromol m(-2) s(-1) PPF density) at low (8 degrees C) or warm (22 degrees C) root temperatures. When exposed to low irradiance, all the water relation parameters of cortical cells remained similar at both root temperatures. The exposure of cotyledons to supplemental light at warm root temperatures, however, resulted in a two- to three-fold increase in T(w)(1/2) values accompanied with the reduced hydraulic conductivity in both root cortical (Lp) and cotyledon midrib cells (Lp(c)). Low root temperature (LRT) further reduced Lp(c) and E, whether it was measured under low or high irradiance levels. The reductions of Lp as the result of respective light and LRT treatments were prevented by the application of 1 microM ABA. Midrib cells required higher concentrations of ABA (2 microM) in order to prevent the reduction in Lp(c). When the exposure of cotyledons to light was accompanied by LRT, however, ABA proved ineffective in reversing the inhibition of Lp. LRT combined with high irradiance triggered a drastic 10-fold reduction in water permeability of cortical and midrib cells and increased epsilon and T(w)(1/2) values. Measurement of E indicated that the increased water demand by the transpiring plants was fulfilled by an increase in the apoplastic pathway as principal water flow route. The importance of water transport regulation by transpiration affecting the hydraulic conductivity of the roots is discussed.     

Effect of atrial natriuretic factor on the water permeability of endothelial cells.

Atrial natriuretic factor increases the water permeability of the whole endothelium. This study investigates how it would affect the transcellular osmotic water permeability of bovine artery endothelial cells. The cyclic-GMP production by the isolated cells was maximal for 10(-6)M atrial natriuretic factor within 30 minutes at 37 degrees C. The cyclic-GMP protein kinase cell concentration was 1.87 +/- 0.15 ng/mg protein. The control apparent water permeability of the cells measured by light scattering was 195 +/- 11 microns/sec (n = 5). Membrane folding revealed by light and scanning electron microscopy indicated that their true water permeability values would be close to 20-40 microns/sec, similar to the values for lipid membranes. The energy activation calculated from the temperature dependence of water permeability between 15 degrees C and 37 degrees C was 9.3 kcal/mol. This value suggests water movement through the lipid bilayer and not through water channels. Atrial natriuretic factor 10(-6)M did not significantly increase the water permeability of the cells. Hence, atrial natriuretic factor-stimulated increase in water permeability of the endothelium is more related to changes in paracellular water pathways than in transcellular water flux.     

Kinetics of water loss and the likelihood of intracellular freezing in mouse ova. Influence of the method of calculating the temperature dependence of water permeability

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 is the temperature dependence of the water permeability, Lp (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 of Lp on temperature. This paper compares the kinetics of water loss based on that extrapolation with that based on an Arrhenius relation between Lp and temperature, and finds substantial differences below -20 to -25 degrees C. Since the ice-nucleation temperature of mouse ova in the cryoprotectants DMSO and glycerol is usually below -30 degrees 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 degrees 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.     

Spindle dynamics in living mouse oocytes during meiotic maturation, ageing, cooling and overheating: a study by polarized light microscopy

A liquid crystal polarized light microscope (LC PolScope) was used to examine spindle dynamics in living mouse oocytes. Immature oocytes were cultured for 0-48 h and spindles were imaged with the PolScope at various time points of culture. Oocytes at metaphase I (M-I) and metaphase II (M-II) were also exposed to shifts of temperature from 25 to 41 degrees C to examine the effects of fluctuations of temperature on spindle dynamics. After examination with the PolScope, some oocytes were fixed and examined by immunocytochemical staining and confocal microscopy. After culturing for 6 h, 76% and 2% of the oocytes reached M-I and M-II stages and all oocytes had birefringent spindles. When the oocytes were cultured for 14-16 h, 88% and 6% of oocytes were at M-II and M-I stages respectively and all oocytes had birefringent spindles. However, when the oocytes were cultured for 22-48 h, the proportions of oocytes with birefringent spindles decreased as culture time was increased. Exposure of oocytes to 25 degrees C induced spindle disassembly within 10-20 min in both M-I and M-II oocytes. Most (93-100%) oocytes reassembled spindles after warming at 37 degrees C. Furthermore, exposure of oocytes at M-I stage but not at M-II stage, to 30 degrees C also induced significant microtubule disassembly. However, exposure of oocytes to 38-41 degrees C did not obviously change the quantity of microtubules in the spindles, which was measured by retardance. This study indicates that the PolScope can be used to examine spindle dynamics in living oocytes, and it has the advantage over the routine fluorescence microscope in that images can be obtained in the same individual oocyte and the quantity of microtubules can be measured by retardance in living oocytes. These results also indicate that the M-II spindle in mouse oocytes is sensitive to oocyte ageing and cooling, but not heating, and M-I spindle is more sensitive to temperature decline than M-II spindle.     

A simplified procedure to determine the optimal rate of freezing biological systems

The effect of several cell-level parameters on the predicted optimal cooling rate B(opt) of an arbitrary biological system has been studied using a well-defined water transport model. An extensive investigation of the water transport model revealed three key cell level parameters: reference permeability of the membrane to water L(pg), apparent activation energy E(Lp), and the ratio of the available surface area for water transport to the initial volume of intracellular water (SA/WV). We defined B(opt) as the "highest" cooling rate at which a predefined percent of the initial water volume is trapped inside the cell (values ranging from 5% to 80%) at a predefined end temperature (values ranging from -5 degrees C to -40 degrees C). Irrespective of the choice of the percent of initial water volume trapped and the end temperature, an exact and linear relationship exists between L(pg), SA/WV, and B(opt0. However, a nonlinear and inverse relationship is found between E(Lp) and B(opt). Remarkably, for a variety of biological systems a comparison of the published experimentally determined values of B(opt) agreed quite closely with numerically predicted B(opt) values when the model assumed 5% of initial water is trapped inside the cell at a temperature of -15 degrees C. This close agreement between the experimental and model predicted optimal cooling rates is used to develop a generic optimal cooling rate chart and a generic optimal cooling rate equation that greatly simplifies the prediction of the optimal rate of freezing of biological systems.     

High microvascular endothelial water permeability in mouse lung measured by a pleural surface fluorescence method.

Transport of water between the capillary and airspace compartments in lung encounters serial barriers: the alveolar epithelium, interstitium, and capillary endothelium. We previously reported a pleural surface fluorescence method to measure net capillary-to-airspace water transport. To measure the osmotic water permeability across the microvascular endothelial barrier in intact lung, the airspace was filled with a water-immiscible fluorocarbon. The capillaries were perfused via the pulmonary artery with solutions of specified osmolalites containing a high-molecular-weight fluorescent dextran. An increase in perfusate osmolality produced a prompt decrease in surface fluorescence due to dye dilution in the capillaries, followed by a slower return to initial fluorescence as capillary and lung interstitial osmolality equilibrate. A mathematical model was developed to determine the osmotic water permeability coefficient (Pf) of lung microvessels from the time course of pleural surface fluorescence. As predicted, the magnitude of the prompt change in surface fluorescence increased with decreased pulmonary artery perfusion rate and increased osmotic gradient size. With raffinose used to induce the osmotic gradient, Pf was 0.03 cm/s at 23 degrees C and was reduced 54% by 0.5 mM HgCl2. Temperature dependence measurements gave an Arrhenius activation energy (Ea) of 5.4 kcal/mol (12-37 degrees C). The apparent Pf induced by the smaller osmolytes mannitol and glycine was 0.021 and 0.011 cm/s (23 degrees C). Immunoblot analysis showed approximately 1.4 x 10(12) aquaporin-1 water channels/cm2 of capillary surface, which accounted quantitatively for the high Pf. These results establish a novel method for measuring osmotically driven water permeability across microvessels in intact lung. The high Pf, low Ea, and mercurial inhibition indicate the involvement of molecular water channels in water transport across the lung endothelium.     

Measurement and simulation of water and methanol transport in algal cells

BACKGROUND: Experimental data and a complementary biophysical model are presented to describe the dynamic response of a unicellular microalga to osmotic processes encountered during cryopreservation. METHOD OF APPROACH: Chlorococcum texanum (C. texanum) were mounted on a cryoperfusion microscope stage and exposed sequentially to various solutions of sucrose and methanol. Transient volumetric excursions were determined by capturing images of cells in real time and utilizing image analysis software to calculate cell volumes. A biophysical model was applied to the data via inverse analysis in order to determine the plasma membrane permeability to water and to methanol. The data were also used to determine the elastic modulus of the cell wall and its effect on cell volume. A three-parameter (hydraulic conductivity (Lp), solute permeability; (omega), and reflection coefficient, (sigma)) membrane transport model was fit to data obtained during methanol perfusion to obtain constitutive property values. These results were compared with the property values obtained for a two coefficient (Lp and omega) model. RESULTS: The three-parameter model gave a value for sigma not consistent with practical physical interpretation. Thus, the two-coefficient model is the preferred approach for describing simultaneous water and methanol transport. The rate of both water and methanol transport were strongly dependent on temperature over the measured temperature range (25 degrees C to -5 degrees C) and cells were appreciably more permeable to methanol than to water at all measured temperatures. CONCLUSION: These results may explain in part why methanol is an effective cryoprotective agent for microalgae.     

Membrane transport properties of equine and macaque ovarian tissues frozen in mixtures of dimethylsulfoxide and ethylene glycol

The rate at which equine and macaque ovarian tissue sections are first cooled from +25 degrees C to +4 degrees C has a significant effect on the measured water transport when the tissues are subsequently frozen in 0.85 M solutions of glycerol, dimethylsulfoxide (DMSO), or ethylene glycol (EG). To determine whether the response of ovarian tissues is altered if they are suspended in mixtures of cryoprotective agents (CPAs), rather than in solutions of a single CPA, we have now measured the subzero water transport from ovarian tissues that were suspended in mixtures of DMSO and EG. Sections of freshly collected equine and macaque ovaries were suspended either in a mixture of 0.9 M EG plus 0.7 M DMSO (equivalent to a mixture of approximately 5% vv of EG and DMSO) or in a 1.6M solution of only DMSO or only EG. The tissue sections were cooled from +25 degrees C to +4 degrees C and then frozen to subzero temperatures at 5 degrees C/min. As the tissues were being frozen, a shape-independent differential scanning calorimeter technique was used to measure water loss from the tissues and, consequently, the best fit membrane permeability parameters (L(pg) and E(Lp)) of ovarian tissues during freezing. In the mixture of DMSO+EG, the respective values of L(pg) and E(Lp) for equine tissue first cooled at 40 degrees C/min between +25 degrees C and +4 degrees C before being frozen were 0.15 microm/min atm and 7.6 kcal/mole. The corresponding L(pg) and E(Lp) values for equine tissue suspended in 1.6M DMSO were 0.12 microm/min atm and 27.2 kcal/mole; in 1.6M EG, the values were 0.06 microm/min atm and 21.9 kcal/mole, respectively. For macaque ovarian tissues suspended in the mixture of DMSO+EG, the respective values of L(pg) and E(Lp) were 0.26 microm/min atm and 26.2 kcal/mole. Similarly, the corresponding L(Lg) and E(Lp) values for macaque tissue suspended in 1.6M DMSO were 0.22 microm/min atm and 31.4 kcal/mole; in 1.6 M EG, the values were 0.20 microm/min atm and 27.9 kcal/mole. The parameters for both equine and macaque tissue samples suspended in the DMSO+EG mixture and first cooled at 0.5 degrees C/min between +25 degrees C and +4 degrees C were very similar to the corresponding values for samples cooled at 40 degrees C/min. In contrast, the membrane parameters of equine and macaque samples first cooled at 0.5 degrees C/min in single-component solutions were significantly different from the corresponding values for samples cooled at 40 degrees C/min. These results show that the membrane properties of ovarian cells from two species are different, and that the membrane properties are significantly affected both by the solution in which the tissue is suspended and by the rate at which the tissue is cooled from +25 degrees C to +4 degrees C before being frozen. These observations suggest that these variables ought to be considered in the derivation of methods to cryopreserve ovarian tissues.     

In vitro transformation of apoA-I-containing lipoprotein subpopulations: role of lecithin:cholesterol acyltransferase and apoB-containing lipoproteins

Two populations of apoA-I-containing lipoproteins are found in plasma: particles with apoA-II [Lp(AI w AII)] and particles without apoA-II [Lp(AI w/o AII)]. Both are heterogeneous in size. However, their size subpopulation distributions differ considerably between healthy subjects and patients with coronary artery diseases. The metabolic basis for such alterations was studied by determining the role of lecithin:cholesterol acyltransferase (LCAT) and apoB-containing lipoproteins (LpB) in the size subpopulation distributions of Lp(AI w AII) and Lp(AI w/o AII). ApoB-free and LCAT-free plasmas, prepared by affinity chromatography, and whole plasma were incubated at 4 degrees C and 37 degrees C for 24 hr. After incubation, Lp(AI w AII) and Lp(AI w/o AII) were isolated by anti-A-II and anti-A-I immunosorbents. Their size subpopulation distributions were studied by nondenaturing gradient polyacrylamide gel electrophoresis. At 4 degrees C most Lp(AI w AII) particles were in the range of 7.0-9.2 nm Stokes diameter. Incubation of plasma at 37 degrees C resulted in an overall enlargement of particles up to 11.2 nm and larger. These particles were enriched with cholesteryl ester and triglyceride and depleted of phospholipids and free cholesterol. Removal of LpB or LCAT from plasma prior to incubation greatly reduced their enlargement. At 4 degrees C, Lp(AI w/o AII) contained mostly particles of 8.5 and 10.1 nm. Incubation at 37 degrees C abolished both subpopulations with the formation of a new subpopulation of 9.2 nm. This transformation was identical in apoB-free plasma but was not seen in LCAT-free plasma. Our study shows that transformation of Lp(AI w AII) requires both LCAT and LpB. However, LpB is not necessary for the transformation of Lp(AI w/o AII) in vitro. The relevance of these in vitro studies to in vivo lipoprotein metabolism was demonstrated in a subject with hepatic triglyceride lipase deficiency.