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Dielectric behavior of the frog lens in the 100 Hz to 500 MHz range. Simulation with an allocated ellipsoidal-shells model.

机译:蛙镜在100 Hz至500 MHz范围内的介电性能。使用已分配的椭球壳模型进行仿真。

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摘要

In an attempt to correlate the passive electrical properties of the lens tissue with its structure, we measured ac admittances for isolated frog lenses, lens nuclei, and homogenate of cortical fiber cells, over the frequency range 10(2)-5.10(8) Hz. The whole lenses molded into discoid shape show a characteristic "two-step" dielectric dispersion with a huge permittivity increment of the order of 10(5) at 1 kHz. Of the two subdispersions disclosed, dispersion 1 has a permittivity increment (delta epsilon) of 2.10(5) with a characteristic frequency (fc) of 2 kHz, and dispersion 2 has a delta epsilon of 400 with an fc of 2 MHz. In terms of loss tangent, these dispersions are more clearly located as two separate peaks. Data are analyzed using an allocated ellipsoidal-shells model which has been developed by taking into account fiber orientation inside the lens tissue. Dispersion 1 is assigned to the equatorial cortex, where fiber cells run parallel to the applied electric field, and dispersion 2 to the nucleus with a complex fiber arrangement and also to the polar cortex, in which the fiber alignment is predominantly perpendicular. In addition, the model analysis reveals that, in the frog lens, the nucleus occupies approximately 30% in volume and that relative permittivity and conductivity for the cell interior are, respectively, 45 and 3 mS/cm for the cortical cells, and 28 and 0.3 mS/cm for the nuclear cells.
机译:为了使晶状体组织的无源电特性与其结构相关联,我们在10(2)-5.10(8)Hz的频率范围内测量了孤立的青蛙晶状体,晶状体核和皮质纤维细胞匀浆的ac导纳。 。模制成盘状形状的整个透镜显示出特征性的“两步”介电色散,在1 kHz时介电常数的巨大增量约为10(5)。在公开的两个子色散中,色散1具有2.10(5)的介电常数增量(δepsilon),特征频率(fc)为2 kHz,并且色散2具有400的δε,fc为2 MHz。就损耗角正切而言,这些色散更清楚地定位为两个单独的峰。使用分配的椭球壳模型分析数据,该模型是通过考虑晶状体组织内部的纤维取向而开发的。色散1分配给赤道皮质,其中纤维细胞与施加的电场平行,色散2分配给具有复杂纤维排列的核,也分配给极性皮质,其中纤维排列主要垂直。此外,模型分析表明,在青蛙晶状体中,核占据约30%的体积,并且细胞内部的相对介电常数和电导率分别为45和3 mS / cm(皮质细胞),以及28和28。核细胞为0.3 mS / cm。

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