Study on the Compatibility of C<sub>6</sub>F<sub>12</sub>O Gas Mixture with EPDM

Objective SF<sub>6</sub> is widely used in electrically insulated equipment due to its excellent insulating properties. However, its global warming potential is 23 500 times greater than that of CO<sub>2</sub>, with an atmospheric lifespan of up to 3200 years. As the severity of global warming intensifies, finding a new environmentally friendly insulating gas to reduce the using of SF<sub>6</sub> has become a hot research topic in recent years. C<sub>6</sub>F<sub>12</sub>O has both environmental benign characteristics and insulating properties, which has attracted the attention of scholars. However, the liquefaction temperature of pure C<sub>6</sub>F<sub>12</sub>O gas is 49 ℃ at atmospheric pressure, which is difficult to use as an insulating medium in practical engineering scenarios. It must be mixed with low-boiling point buffer gases, including CO<sub>2</sub> and N<sub>2</sub>. It has been shown that a gas mixture comprising 4% C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>, when pressurized above 0.14 MPa, can be used as an insulating gas in 10 kV switchgear. For new eco-friendly insulation gas, its compatibility with the internal sealing materials of the equipment is also need to be considered.Method The experimental study on the compatibility between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> gas mixture and the sealing rubber EPDM was carried out by building a thermally accelerated compatibility experimental platform in this paper. The effect of trace O<sub>2</sub> on the compatibility of C<sub>6</sub>F<sub>12</sub>O gas mixture and EPDM was investigated by adding a small amount of O<sub>2</sub> into the gas mixture. The changes in the surface morphology, the elements of rubber samples, the gas mixture components, and the mechanical properties were analyzed before and after the experiments. The interaction between C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> gas mixture and rubber was also calculated based on the MD theory.Results and Discussions The results from scanning electron microscopy showed that the scaly structures appeared on the surface of EPDM when mixed with C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> at 110 °C. A flocculent structure appeared when EPDM was mixed with C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> at only 90 °C. This observation suggested that the inclusion of O<sub>2</sub> promotes the interaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> gas mixture and EPDM, which in turn leads to the corrosion of EPDM. The results of X-ray photoelectron spectroscopy showed that a decrease in the carbon content alongside increases in oxygen and fluorine within the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixed EPDM with increasing temperature. This trend indicated that C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> reacts with EPDM. In group of C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub>, the changes were more significant, which indicate that O<sub>2</sub> promoted the reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and EPDM. Post-experimental analyses identified new spectral peaks at 284.5 eV, 285.8 eV and 289.2 eV, corresponding to C—C, C—H and —COO— ester bonds, respectively. Three characteristic peaks of elemental F were detected on the EPDM surface for metal fluoride at 683 eV, organofluoride at 684.5 eV, and —CF<sub>2</sub>CH<sub>2</sub>— at 687 eV. The intensity of C characteristic peak was significantly lower, while the intensity of O and F were higher in the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> gas mixture after testing. These findings indicated that O<sub>2</sub> actively participates in the reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and the EPDM, fostering an intensified interaction. The results of tensile properties showed that the mechanical properties of EPDM decreased significantly with increasing temperature. The mechanical property of EPDM in C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> atmosphere was slightly worse than those of the original samples. The mechanical property of EPDM under C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> was worse than that of C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>. The reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and EPDM was more intensive after adding O<sub>2</sub>, leading to a significant decrease in the mechanical properties of EPDM. At the end of the experiment, a small amount of the resultant gas was collected and subjected to Gas chromatography–mass spectrometry for further analysis. The small amount of H<sub>2</sub>O remaining inside the gas tank was involved in the decomposition reaction of the C<sub>6</sub>F<sub>12</sub>O gas mixture. Throughout the reaction, <inline-formula><tex-math id="Z-20240912144036">${\rm H}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144036.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144036.png"/></alternatives></inline-formula> and <inline-formula><tex-math id="Z-20240912144046">${\rm OH}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144046.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144046.png"/></alternatives></inline-formula> were generated from the decomposition of H<sub>2</sub>O, which can interact with particles such as <inline-formula><tex-math id="Z-20240912144102">${\rm CF}_3^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144102.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144102.png"/></alternatives></inline-formula>, <inline-formula><tex-math id="Z-20240912144122">${\rm C_{3}F}_7^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144122.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144122.png"/></alternatives></inline-formula>, and <inline-formula><tex-math id="Z-20240912144203">${\rm F}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144203.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144203.png"/></alternatives></inline-formula> produced by C<sub>6</sub>F<sub>12</sub>O to produce decomposition products such as C<sub>3</sub>F<sub>6</sub> and C<sub>3</sub>F<sub>7</sub>H. Meanwhile, the reaction rate of the C<sub>6</sub>F<sub>12</sub>O gas mixture with EPDM and the concentration of C<sub>3</sub>F<sub>6</sub> and C<sub>3</sub>F<sub>7</sub>H were increased by both the increasing temperature and O<sub>2</sub> introduction. The diffusion coefficient <italic>D</italic> indicates that the diffusion speed of gas molecules in EPDM can reflect the physicochemical relationship between the gas and the solid material. The diffusion coefficients of both C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> in EPDM increased with rising temperatures. At 110 °C, the diffusion coefficients of C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> were increased by 1.71 and 2.49 times, respectively, following O<sub>2</sub> addition. It indicates that the internal energies of gas molecules were increased by adding O<sub>2</sub>, and the C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> gas molecules could be easier to diffuse on the EPDM surface and interact with EPDM. The Flory–Huggins interaction parameter (<inline-formula><tex-math id="Z-20240912143141">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143141.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143141.png"/></alternatives></inline-formula>) quantifies alterations in molecular interaction energy during miscibility and aids in determining the solubility of binary mixtures. A value of <inline-formula><tex-math id="Z-20240912143235">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143235.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143235.png"/></alternatives></inline-formula> tending towards 0 indicates good compatibility between the mixed systems. Meanwhile, the parameter (<inline-formula><tex-math id="Z-20240912143253">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143253.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143253.png"/></alternatives></inline-formula>) tends to be linear with the mixing energy (Δ<italic>E</italic><sub>mix</sub>). Both <inline-formula><tex-math id="Z-20240912143312">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143312.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143312.png"/></alternatives></inline-formula> and Δ<italic>E</italic><sub>mix</sub> values of the EPDM mixing system decreased with increasing temperature. The <inline-formula><tex-math id="Z-20240912143325">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143325.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.

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SHILAP Revista de lepidopterología
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2024-09-01
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High voltage insulation and dielectric phenomena
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article

Study on the Compatibility of C6F12O Gas Mixture with EPDM

SHILAP Revista de lepidopterología
High voltage insulation and dielectric phenomena
article

Study on the Compatibility of C6F12O Gas Mixture with EPDM

article en

Abstract

Objective SF<sub>6</sub> is widely used in electrically insulated equipment due to its excellent insulating properties. However, its global warming potential is 23 500 times greater than that of CO<sub>2</sub>, with an atmospheric lifespan of up to 3200 years. As the severity of global warming intensifies, finding a new environmentally friendly insulating gas to reduce the using of SF<sub>6</sub> has become a hot research topic in recent years. C<sub>6</sub>F<sub>12</sub>O has both environmental benign characteristics and insulating properties, which has attracted the attention of scholars. However, the liquefaction temperature of pure C<sub>6</sub>F<sub>12</sub>O gas is 49 ℃ at atmospheric pressure, which is difficult to use as an insulating medium in practical engineering scenarios. It must be mixed with low-boiling point buffer gases, including CO<sub>2</sub> and N<sub>2</sub>. It has been shown that a gas mixture comprising 4% C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>, when pressurized above 0.14 MPa, can be used as an insulating gas in 10 kV switchgear. For new eco-friendly insulation gas, its compatibility with the internal sealing materials of the equipment is also need to be considered.Method The experimental study on the compatibility between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> gas mixture and the sealing rubber EPDM was carried out by building a thermally accelerated compatibility experimental platform in this paper. The effect of trace O<sub>2</sub> on the compatibility of C<sub>6</sub>F<sub>12</sub>O gas mixture and EPDM was investigated by adding a small amount of O<sub>2</sub> into the gas mixture. The changes in the surface morphology, the elements of rubber samples, the gas mixture components, and the mechanical properties were analyzed before and after the experiments. The interaction between C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> gas mixture and rubber was also calculated based on the MD theory.Results and Discussions The results from scanning electron microscopy showed that the scaly structures appeared on the surface of EPDM when mixed with C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> at 110 °C. A flocculent structure appeared when EPDM was mixed with C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> at only 90 °C. This observation suggested that the inclusion of O<sub>2</sub> promotes the interaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> gas mixture and EPDM, which in turn leads to the corrosion of EPDM. The results of X-ray photoelectron spectroscopy showed that a decrease in the carbon content alongside increases in oxygen and fluorine within the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixed EPDM with increasing temperature. This trend indicated that C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> reacts with EPDM. In group of C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub>, the changes were more significant, which indicate that O<sub>2</sub> promoted the reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and EPDM. Post-experimental analyses identified new spectral peaks at 284.5 eV, 285.8 eV and 289.2 eV, corresponding to C—C, C—H and —COO— ester bonds, respectively. Three characteristic peaks of elemental F were detected on the EPDM surface for metal fluoride at 683 eV, organofluoride at 684.5 eV, and —CF<sub>2</sub>CH<sub>2</sub>— at 687 eV. The intensity of C characteristic peak was significantly lower, while the intensity of O and F were higher in the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> gas mixture after testing. These findings indicated that O<sub>2</sub> actively participates in the reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and the EPDM, fostering an intensified interaction. The results of tensile properties showed that the mechanical properties of EPDM decreased significantly with increasing temperature. The mechanical property of EPDM in C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> atmosphere was slightly worse than those of the original samples. The mechanical property of EPDM under C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>/O<sub>2</sub> was worse than that of C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub>. The reaction between the C<sub>6</sub>F<sub>12</sub>O/CO<sub>2</sub> mixture and EPDM was more intensive after adding O<sub>2</sub>, leading to a significant decrease in the mechanical properties of EPDM. At the end of the experiment, a small amount of the resultant gas was collected and subjected to Gas chromatography–mass spectrometry for further analysis. The small amount of H<sub>2</sub>O remaining inside the gas tank was involved in the decomposition reaction of the C<sub>6</sub>F<sub>12</sub>O gas mixture. Throughout the reaction, <inline-formula><tex-math id="Z-20240912144036">${\rm H}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144036.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144036.png"/></alternatives></inline-formula> and <inline-formula><tex-math id="Z-20240912144046">${\rm OH}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144046.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144046.png"/></alternatives></inline-formula> were generated from the decomposition of H<sub>2</sub>O, which can interact with particles such as <inline-formula><tex-math id="Z-20240912144102">${\rm CF}_3^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144102.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144102.png"/></alternatives></inline-formula>, <inline-formula><tex-math id="Z-20240912144122">${\rm C_{3}F}_7^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144122.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144122.png"/></alternatives></inline-formula>, and <inline-formula><tex-math id="Z-20240912144203">${\rm F}^{\,\cdot} $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144203.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912144203.png"/></alternatives></inline-formula> produced by C<sub>6</sub>F<sub>12</sub>O to produce decomposition products such as C<sub>3</sub>F<sub>6</sub> and C<sub>3</sub>F<sub>7</sub>H. Meanwhile, the reaction rate of the C<sub>6</sub>F<sub>12</sub>O gas mixture with EPDM and the concentration of C<sub>3</sub>F<sub>6</sub> and C<sub>3</sub>F<sub>7</sub>H were increased by both the increasing temperature and O<sub>2</sub> introduction. The diffusion coefficient <italic>D</italic> indicates that the diffusion speed of gas molecules in EPDM can reflect the physicochemical relationship between the gas and the solid material. The diffusion coefficients of both C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> in EPDM increased with rising temperatures. At 110 °C, the diffusion coefficients of C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> were increased by 1.71 and 2.49 times, respectively, following O<sub>2</sub> addition. It indicates that the internal energies of gas molecules were increased by adding O<sub>2</sub>, and the C<sub>6</sub>F<sub>12</sub>O and CO<sub>2</sub> gas molecules could be easier to diffuse on the EPDM surface and interact with EPDM. The Flory–Huggins interaction parameter (<inline-formula><tex-math id="Z-20240912143141">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143141.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143141.png"/></alternatives></inline-formula>) quantifies alterations in molecular interaction energy during miscibility and aids in determining the solubility of binary mixtures. A value of <inline-formula><tex-math id="Z-20240912143235">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143235.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143235.png"/></alternatives></inline-formula> tending towards 0 indicates good compatibility between the mixed systems. Meanwhile, the parameter (<inline-formula><tex-math id="Z-20240912143253">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143253.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143253.png"/></alternatives></inline-formula>) tends to be linear with the mixing energy (Δ<italic>E</italic><sub>mix</sub>). Both <inline-formula><tex-math id="Z-20240912143312">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143312.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143312.png"/></alternatives></inline-formula> and Δ<italic>E</italic><sub>mix</sub> values of the EPDM mixing system decreased with increasing temperature. The <inline-formula><tex-math id="Z-20240912143325">$\chi $</tex-math><alternatives><graphic specific-use="online" xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="202300004_Z-20240912143325.jpg"/><graphic specific-use="print" xmlns:xlink="http://www.

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High voltage insulation and dielectric phenomena
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