Saulis G
Department of Biology, Vytautas Magnus University, Kaunas, Lithuania.
Biophys J. 1997 Sep;73(3):1299-309. doi: 10.1016/S0006-3495(97)78163-3.
The process of pore disappearance after cell electroporation is analyzed theoretically. On the basis of the kinetic model, in which the formation and annihilation of a metastable hydrophilic pore are considered as random one-step processes, a distribution function of cell resealing times, Fr(t), is derived. Two cases are studied: 1) the rate of pore resealing, k(r), is significantly greater than the rate of pore formation, k(f); and 2) the rate of pore formation, k(f), is comparable with k(r). It is determined that the shape of the distribution function depends on the initial number of pores in a cell, n(i). If in the absence of an external electric field the rate of pore formation, k(f), is significantly less than the rate of pore resealing, k(r) (case 1), pores disappear completely, whereas when k(f) approximately k(r) (case 2), the cell achieves a steady state in which the number of pores is equal to k(f)/k(r). In case 1, when n(i) = 1, the distribution function Fr(t) is exponential. The developed theory is compared with experimental data available in the literature. Increasing the time of incubation at elevated temperature increases the fraction of resealed cells. This indicates that the time necessary for the resealing varies from cell to cell. Although the shape of experimental relationships depends on the electroporation conditions they can be described by theoretical curves quite well. Thus it can be concluded that the disappearance of pores in the cell membrane after electroporation is a random process. It is shown that from the comparison of presented theory with experiments, the following parameters can be estimated: the average number of pores, n(i), that appeared in a cell during an electric pulse; the rate of pore disappearance, k(r); the ratio k(f)/k(r); and the energy barrier to pore disappearance deltaWr(0). Estimated numerical values of the parameters show that increasing the amplitude of an electric pulse increases either the apparent number of pores created during the pulse (the rate of pore resealing remains the same) or the rate of pore resealing (the average number of pores remains the same).
从理论上分析了细胞电穿孔后孔消失的过程。基于动力学模型,其中亚稳态亲水孔的形成和湮灭被视为随机的一步过程,推导了细胞重新封闭时间的分布函数(F_r(t))。研究了两种情况:1)孔重新封闭的速率(k(r))显著大于孔形成的速率(k(f));2)孔形成的速率(k(f))与(k(r))相当。结果表明,分布函数的形状取决于细胞中初始孔的数量(n(i))。如果在没有外部电场的情况下,孔形成的速率(k(f))显著小于孔重新封闭的速率(k(r))(情况1),孔会完全消失,而当(k(f))近似于(k(r))(情况2)时,细胞达到稳态,其中孔的数量等于(k(f)/k(r))。在情况1中,当(n(i)=1)时,分布函数(F_r(t))是指数形式的。将所发展的理论与文献中的实验数据进行了比较。在升高的温度下延长孵育时间会增加重新封闭细胞的比例。这表明重新封闭所需的时间因细胞而异。尽管实验关系的形状取决于电穿孔条件,但它们可以被理论曲线很好地描述。因此可以得出结论,电穿孔后细胞膜中孔的消失是一个随机过程。结果表明,通过将所提出的理论与实验进行比较,可以估计以下参数:在电脉冲期间细胞中出现的孔的平均数量(n(i));孔消失的速率(k(r));(k(f)/k(r))的比值;以及孔消失的能垒(\Delta W_r(0))。参数的估计数值表明,增加电脉冲的幅度会增加脉冲期间产生的表观孔的数量(孔重新封闭的速率保持不变)或孔重新封闭的速率(孔的平均数量保持不变)。