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[基于椭球壳模型的完整大鼠晶状体理论阻抗分析]

[Theoretical impedance analysis of the intact rat lens with an ellipsoidal shells model].

作者信息

Watanabe M, Matsuoka R, Seike K, Mokudai Y, Ueno H

机构信息

Department of Ophthalmology, Kochi Medical School, Japan.

出版信息

Nippon Ganka Gakkai Zasshi. 1998 Sep;102(9):555-60.

PMID:9785851
Abstract

We measured a.c. admittances for isolated rat lenses over a wide frequency range of 100 Hz to 500 MHz. In order to evade electrode polarization at low frequencies, we examined extracted lenses by direct semi-squeezing with Pt black-coated platinum electrodes. This gave rise to a 10(6) increment in permittivity at low frequencies, and two distinct dielectric dispersions were exhibited; dispersion 1 with a characteristic frequency (fc) of 2 kHz, and dispersion 2 with an fc of 2 MHz. In terms of loss tangent function, the two dispersions clearly dominated as two peaks. By curve fitting analysis with an allocated ellipsoidal-shells model based on ultrastructural features of the lens with a lens equivalent circuit, dispersion 1 was assigned to the equatorial cortex where regularly arranged lens fibers ran parallel to the applied electric field, and dispersion 2 to the nucleus of complicated fibers, combined with the polar cortex where lens fibers ran perpendicular to the electric field. Our results suggested that both lens dispersions were beta-dispersions attributable to bio-membranes.

摘要

我们在100 Hz至500 MHz的宽频率范围内测量了离体大鼠晶状体的交流导纳。为了避免低频下的电极极化,我们通过用涂有铂黑的铂电极直接半挤压来检查摘除的晶状体。这导致低频下介电常数增加了10^6,并且呈现出两种不同的介电色散;色散1的特征频率(fc)为2 kHz,色散2的fc为2 MHz。就损耗角正切函数而言,这两种色散明显作为两个峰值占主导地位。通过基于晶状体超微结构特征并结合晶状体等效电路的分配椭球壳模型进行曲线拟合分析,色散1被归因于赤道皮质,其中规则排列的晶状体纤维与施加的电场平行,色散2被归因于复杂纤维的核,以及晶状体纤维与电场垂直的极皮质。我们的结果表明,两种晶状体色散均为归因于生物膜的β色散。

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