为进一步探究电穿孔理论机制,通过COMSOL建立单细胞电穿孔二维轴对称模型,该模型同时纳入表征微孔密度的电穿孔渐进方程和表征微孔动态演变过程的孔径变化方程,且模型的轴对称性使穿孔面积的计算更为准确,从而得到微孔的时空分布特性,...为进一步探究电穿孔理论机制,通过COMSOL建立单细胞电穿孔二维轴对称模型,该模型同时纳入表征微孔密度的电穿孔渐进方程和表征微孔动态演变过程的孔径变化方程,且模型的轴对称性使穿孔面积的计算更为准确,从而得到微孔的时空分布特性,并在此基础上探讨场强和脉宽对该特性的影响。结果表明:脉宽100μs、场强2 k V/cm的脉冲作用下,产生微孔7862个,穿孔面积达细胞表面积的6.3%,电穿孔各参量的时空分布规律与文献结果一致,从而可验证所建模型的有效性;在1~5 k V/cm范围内增大脉冲场强,微孔数与场强成正比,孔径则与场强成反比,孔面积与细胞面积之比从1.3%增至12.9%;对两组能量相同的纳秒脉冲和微秒脉冲进行比较,发现脉冲结束时前者产生的微孔数是后者的353.1倍,而在细胞膜上最靠近电极的点,后者的孔径是前者的19.3倍,说明纳秒脉冲有利于微孔数增加,而微秒脉冲有利于孔径扩大。仿真结果表明,微孔特性决定电穿孔的发生和发展过程,微孔特性的精确计算是阐释电穿孔效应的关键所在。展开更多
Three thermodynamical equations, for unitary two-phase fluid inclusions have been deduced. (1) The thermodynamical equation for mutual transformation between gas and liquid phases in fluid inclusions. The transformati...Three thermodynamical equations, for unitary two-phase fluid inclusions have been deduced. (1) The thermodynamical equation for mutual transformation between gas and liquid phases in fluid inclusions. The transformation direction from one phase to the other can be known in terms of the density and filling degree of gas and liquid. (2) The thermodynamical equation for pressure effect on temperature after homogenization of fluid inclusions. The coefficient of P-T variation is directly proportional to the fining degree of gas phase and inversely to the density of gas phase and liquid phase. Equations for homogenization, decrepitation and formation temperatures of fluid inclusions can be inferred from. this equation. (3) The thermodynomical equation for decrepitation temperatures of fluid inclusions. Many factors have effects on the decrepitation temperatures of fluid inclusions.Decrepitation temperature cannot be considered in any case as formation temperature.Thermal and vapor halos produced by decrepitation of minerals of the same kind and the same period from the same locality are worthy of consideration.展开更多
文摘为进一步探究电穿孔理论机制,通过COMSOL建立单细胞电穿孔二维轴对称模型,该模型同时纳入表征微孔密度的电穿孔渐进方程和表征微孔动态演变过程的孔径变化方程,且模型的轴对称性使穿孔面积的计算更为准确,从而得到微孔的时空分布特性,并在此基础上探讨场强和脉宽对该特性的影响。结果表明:脉宽100μs、场强2 k V/cm的脉冲作用下,产生微孔7862个,穿孔面积达细胞表面积的6.3%,电穿孔各参量的时空分布规律与文献结果一致,从而可验证所建模型的有效性;在1~5 k V/cm范围内增大脉冲场强,微孔数与场强成正比,孔径则与场强成反比,孔面积与细胞面积之比从1.3%增至12.9%;对两组能量相同的纳秒脉冲和微秒脉冲进行比较,发现脉冲结束时前者产生的微孔数是后者的353.1倍,而在细胞膜上最靠近电极的点,后者的孔径是前者的19.3倍,说明纳秒脉冲有利于微孔数增加,而微秒脉冲有利于孔径扩大。仿真结果表明,微孔特性决定电穿孔的发生和发展过程,微孔特性的精确计算是阐释电穿孔效应的关键所在。
文摘Three thermodynamical equations, for unitary two-phase fluid inclusions have been deduced. (1) The thermodynamical equation for mutual transformation between gas and liquid phases in fluid inclusions. The transformation direction from one phase to the other can be known in terms of the density and filling degree of gas and liquid. (2) The thermodynamical equation for pressure effect on temperature after homogenization of fluid inclusions. The coefficient of P-T variation is directly proportional to the fining degree of gas phase and inversely to the density of gas phase and liquid phase. Equations for homogenization, decrepitation and formation temperatures of fluid inclusions can be inferred from. this equation. (3) The thermodynomical equation for decrepitation temperatures of fluid inclusions. Many factors have effects on the decrepitation temperatures of fluid inclusions.Decrepitation temperature cannot be considered in any case as formation temperature.Thermal and vapor halos produced by decrepitation of minerals of the same kind and the same period from the same locality are worthy of consideration.
