Pressure in isochoric systems containing aqueous solutions at subzero Centigrade temperatures

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Abstract

Objective Preservation of biological materials at subzero Centigrade temperatures, cryopreservation, is important for the field of tissue engineering and organ transplantation. Our group is studying the use of isochoric (constant volume) systems of aqueous solution for cryopreservation. Previous studies measured the pressure-temperature relations in aqueous isochoric systems in the temperature range from 0C to – 20C. The goal of this study is to expand the pressure-temperature measurement beyond the range reported in previous publications. Materials and methods To expand the pressure-temperature measurements beyond the previous range, we have developed a new isochoric device capable of withstanding liquid nitrogen temperatures and pressures of up to 413 MPa. The device is instrumented with a pressure transducer than can monitor and record the pressures in the isochoric chamber in real time. Measurements were made in a temperature range from – 5C to liquid nitrogen temperatures for various solutions of pure water and Me2SO (a chemical additive used for protection of biological materials in a frozen state and for vitrification (glass formation) of biological matter). Undissolved gaseous are is carefully removed from the system. Results Temperature-pressure data from – 5C to liquid nitrogen temperature for pure water and other solutions are presented in this study. Following are examples of some, temperature-pressure values, that were measured in an isochoric system containing pure water: (- 20C, 187 MPa); (-25C, 216 MPa); (- 30C, 242.3 MPa); (-180C, 124 MPa). The data is consistent with the literature, which reports that the pressure and temperature at the triple point, between ice I, ice III and water is, - 21.993C and 209.9 MPa, respectively. It was surprising to find that the pressure in the isochoric system increases at temperatures below the triple point and remains high to liquid nitrogen temperatures. Measurements of pressure-temperature relations in solutions of pure water and Me2SO in different concentrations show that, for concentrations in which vitrification is predicted, no increase in pressure was measured during rapid cooling to liquid nitrogen temperatures. However, ice formation either during cooling or warming to and from liquid nitrogen temperatures produced an increase in pressure. Conclusions The data obtained in this study can be used to aid in the design of isochoric cryopreservation protocols. The results suggest that the pressure measurement is important in the design of “constant volume” systems and can provide a simple means to gain information on the occurrence of vitrification and devitrification during cryopreservation processes of aqueous solutions in an isochoric system.

Figures

  • Fig 1. Experimental system. A) a photograph of the isochoric chamber, B) Two isochoric devices in the cooling chamber of a Planer Kryo 10 series III controlled rate freezer.
  • Fig 2. Pressure as a function of time during cooling and warming. The experiments were performed by setting a constant temperature for periods of 30 minutes during cooling and warming. The constant temperatures and their corresponding steady state pressure (with the standard deviation) measured are listed on the figure. Supporting information contained in S1 File
  • Fig 3. Comparison of experimentally determined pressure and temperature data from this study, with data from other publications, overlaid on a phase diagram for pure water (with modification from [38].
  • Fig 4. Pressure as a function of time during cooling and warming. The experiments were performed by setting a constant temperature for periods of 30 minutes during cooling and warming. The constant temperatures and their corresponding steady state pressure (with the standard deviation) measured are listed on the figure. The arrow points to the spike in pressure during cooling to– 40˚C. Supporting information contained in S2 File
  • Fig 5. The data from Fig 5 displayed on a phase diagram. The data points–the open circles. The phase diagram outline is a modified version of the phase diagram in [38]
  • Fig 6. Thermal history during the third set of experiments. Supporting information contained in S3 File
  • Fig 7. Pressure as a function of time during the freezing and thawing of various solutions of water and Me2SO to and from liquid nitrogen temperatures. The three regions of temperature correspond to those marked in Fig 6. Supporting information contained in S4 File
  • Fig 8. Pressure as a function of time during the freezing and thawing of various solutions of water and Me2SO to and from liquid nitrogen temperatures. The temperature history is given in the Fig 6 and the three regions (A, B, and C) correspond to those marked in Fig 6. Supporting information contained in S5 File

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Ukpai, G., Năstase, G., Şerban, A., & Rubinsky, B. (2017). Pressure in isochoric systems containing aqueous solutions at subzero Centigrade temperatures. PLoS ONE, 12(8). https://doi.org/10.1371/journal.pone.0183353

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