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体外龟小脑分子层和颗粒层中表观组织电导率的起源及电流源密度分析的解释

Origin of the apparent tissue conductivity in the molecular and granular layers of the in vitro turtle cerebellum and the interpretation of current source-density analysis.

作者信息

Okada Y C, Huang J C, Rice M E, Tranchina D, Nicholson C

机构信息

Magnetophysiology Laboratory, Veterans Affairs Medical Center, Albuquerque, 87108.

出版信息

J Neurophysiol. 1994 Aug;72(2):742-53. doi: 10.1152/jn.1994.72.2.742.

Abstract
  1. We determined the origin of the apparent tissue conductivity (sigma 2) of the turtle cerebellum in vitro. 2. Application of a current with a known current density (J) along the longitudinal axis of a conductivity cell produced an electric field in the cerebellum suspended in the cell. The measured electric field (E) perpendicular to the cerebellar surface indicated a significant inhomogeneity in sigma a (= J/E) with a major discontinuity between the molecular layer (0.25 +/- 0.05 S/m, mean +/- SD) and granular layers (0.15 +/- 0.03 S/m) (n = 39). 3. This inhomogeneity was more pronounced after anoxic depolarization. The value of sigma a decreased to 0.11 +/- 0.03 and 0.040 +/- 0.008 S/m in the molecular and granular layers, respectively. The ratio of sigma a S in the two layers increased from 1.67 in the normoxic condition to 2.75 after anoxic depolarization. 4. This difference in sigma a across the two layers was present within the range of frequencies (DC to 10 kHz) studied where the phase of sigma a was small (less than +/- 2 degrees) and therefore sigma a was ohmic. 5. The inhomogeneity in sigma a was in part due to an inhomogeneity in the extracellular conductivity (sigma e) as determined from the extracellular diffusion of ionophoresed tetramethylammonium. Like sigma a, the value of sigma e was also higher in the molecular layer (0.165 S/m) than in the granular layer (0.097 S/m). The inhomogeneity in sigma e was due to a smaller tortuosity and a larger extracellular volume fraction in the molecular layer compared with the granular layer. 6. sigma a was, however, consistently higher, by approximately 50%, than sigma e. A core conductor model of the cerebellum indicated that these discrepancies between sigma a and sigma e were attributable to additional conductivity produced by a passage of the longitudinal applied current through the intracellular space of Purkinje cells and ependymal glial cells, with the glial compartment playing the dominant role. Cells with a long process and a short space constant such as the ependymal glia evidently enhance the effective "extracellular" conductivity by serving as intracellular conduits for the applied current. The result implies that the effective sigma e may be larger than sigma e for neuronally generated currents in the turtle cerebellum because the space constant for Purkinje cells is several times greater than that for the ependymal glia and consequently Purkinje cell-generated currents travel over a long distance relative to the space constant of glial cells.(ABSTRACT TRUNCATED AT 400 WORDS)
摘要
  1. 我们在体外确定了龟小脑表观组织电导率(σ2)的来源。2. 沿电导率细胞纵轴施加具有已知电流密度(J)的电流,在悬浮于细胞中的小脑中产生电场。垂直于小脑表面测得的电场(E)表明,σa(=J/E)存在显著的不均匀性,分子层(0.25±0.05 S/m,平均值±标准差)和颗粒层(0.15±0.03 S/m)之间存在主要的不连续性(n = 39)。3. 这种不均匀性在缺氧去极化后更为明显。分子层和颗粒层中σa的值分别降至0.11±0.03和0.040±0.008 S/m。两层中σa的比值从常氧条件下的1.67增加到缺氧去极化后的2.75。4. 在研究的频率范围(直流到10 kHz)内,两层之间的σa差异存在,其中σa的相位很小(小于±2度),因此σa是欧姆性的。5. σa的不均匀性部分归因于细胞外电导率(σe)的不均匀性,这是通过离子载体四甲基铵的细胞外扩散确定的。与σa一样,分子层中σe的值(0.165 S/m)也高于颗粒层(0.097 S/m)。σe的不均匀性是由于分子层与颗粒层相比曲折度较小且细胞外体积分数较大。6. 然而,σa始终比σe高约50%。小脑的核心导体模型表明,σa和σe之间的这些差异归因于纵向施加的电流通过浦肯野细胞和室管膜胶质细胞的细胞内空间产生的额外电导率,其中胶质区室起主导作用。具有长突起和短空间常数的细胞,如室管膜胶质细胞,显然通过作为施加电流的细胞内管道来提高有效的“细胞外”电导率。结果表明,对于龟小脑中神经元产生的电流,有效的σe可能大于σe,因为浦肯野细胞的空间常数比室管膜胶质细胞的空间常数大几倍,因此浦肯野细胞产生的电流相对于胶质细胞的空间常数传播的距离更长。(摘要截断于400字)

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