Irimajiri A, Asami K, Ichinowatari T, Kinoshita Y
Biochim Biophys Acta. 1987 Jan 26;896(2):203-13. doi: 10.1016/0005-2736(87)90181-7.
Frequency dependence of relative permittivity (dielectric constant) and conductivity, or the 'dielectric dispersion', of cultured cells (RBL-1 line) in suspension was measured using a fast impedance analyzer system capable of scanning 92 frequency points over a 10 kHz-500 MHz range within 80 s. Examination of the resulting dispersion curves of an improved reliability revealed that the dispersions consisted of at least two separate components. The low-frequency component (dispersion 1) had a permittivity increment (delta epsilon) of 10(3)-10(4) and a characteristic frequency (fc) at several hundred kHz; for the high-frequency component (dispersion 2), delta epsilon was smaller by a factor of 10(2) and fc = 10-30 MHz. Increments delta epsilon for both components increased with the volume fraction of cell suspension, while fc did not change appreciably as long as the conductivity of suspending medium was fixed. By fitting a model for shelled spheres (the 'single-shell' model) to the data of dispersion 1, the dielectric capacity of the plasma membrane phase (Cm) was estimated to be approx. 1.4 microF/cm2 for the cells in an isotonic medium. However, simulation by this particular shell model failed to reproduce the entire dispersion profile leaving a sizable discrepancy between theory and experiment especially at frequencies above 1 MHz where dispersion 2 took place. This discrepancy could not be filled up even by taking into consideration either the effect of cell size distribution actually determined or that of possible heterogeneity in the intracellular conductivity. The present data strongly indicate the need for a more penetrating model that effectively accounts for the behavior of dispersion 2.
使用一种能够在80秒内在10kHz - 500MHz范围内扫描92个频率点的快速阻抗分析仪系统,测量了悬浮培养细胞(RBL - 1系)的相对介电常数(介电常数)和电导率的频率依赖性,即“介电色散”。对所得色散曲线进行改进可靠性的检查发现,色散至少由两个独立的成分组成。低频成分(色散1)的介电常数增量(δε)为10³ - 10⁴,特征频率(fc)在几百kHz;对于高频成分(色散2),δε小10²倍,fc = 10 - 30MHz。两个成分的δε增量都随细胞悬浮液的体积分数增加,而只要悬浮介质的电导率固定,fc就没有明显变化。通过将带壳球体模型(“单壳”模型)拟合到色散1的数据中,对于等渗介质中的细胞,估计质膜相的介电容量(Cm)约为1.4μF/cm²。然而,用这个特定的壳模型进行模拟未能再现整个色散曲线,在理论与实验之间留下了相当大的差异,特别是在发生色散2的高于1MHz的频率处。即使考虑实际确定的细胞大小分布的影响或细胞内电导率可能的不均匀性,这种差异也无法弥补。目前的数据强烈表明需要一个更具穿透力的模型来有效解释色散2的行为。